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Небесная энциклопедия

Космические корабли и станции, автоматические КА и методы их проектирования, бортовые комплексы управления, системы и средства жизнеобеспечения, особенности технологии производства ракетно-космических систем

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Мониторинг СМИ

Мониторинг СМИ и социальных сетей. Сканирование интернета, новостных сайтов, специализированных контентных площадок на базе мессенджеров. Гибкие настройки фильтров и первоначальных источников.

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Форма поиска

Поддерживает ввод нескольких поисковых фраз (по одной на строку). При поиске обеспечивает поддержку морфологии русского и английского языка
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Применить Всего найдено 37881. Отображено 100.
05-01-2012 дата публикации

Minute particle analyzing device and method

Номер: US20120001090A1
Принадлежит: Icyt Mission Technology Inc, Sony Corp

A minute particle analyzing device includes: a light source; a first condenser lens for condensing light from the light source to a first end of a multimode optical fiber; a second condenser lens for condensing the light emerging from a second end of the multimode optical fiber to a minute particle; and a detector for detecting light generated from the minute particle by the application of the light from the light source.

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05-01-2012 дата публикации

High voltage switch with adjustable current

Номер: US20120002685A1
Принадлежит: Bergmann Messgeraete Entwicklung KG

The present disclosure relates to a high voltage switch which may comprise a chain of MOS field-effect transistors (MOSFETs). The current of the individual MOSFETS, and hence the chain, can be controlled by means of adding a current measuring resistance into the source path of the transistors and transmitting the voltage arising there via a capacitor to a gate connector of the transistors.

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20-11-2016 дата публикации

Лазер на парах металлов

Номер: RU0000166246U1

Лазер на парах металлов, содержащий газоразрядную трубку 1 с электродами 2 на каждом из ее торцевых концов и с навеской металлического стронция внутри нее, оптический резонатор, управляемый высоковольтный блок питания лазера импульсным электрическим током 3, электрически связанный своими выходами с электродами 2 газоразрядной трубки, блок управления 4, обеспечивающий управление величиной напряжения и частотой повторения электрических импульсов блока питания 3 и электронное вычислительное устройство 5, причем газоразрядная трубка расположена между зеркалами оптического резонатора таким образом, что зеркала оптически связаны друг с другом через внутренний объем газоразрядной трубки вдоль ее продольной оси; а упомянутый управляемый высоковольтный блок питания 3 своим входом электрически связан с выходом блока управления 4, отличающийся тем, что в нем установлен приемник радиосигналов 6, имеющий возможность принимать радиосигнал от передатчика радиосигналов и электрически связанный своим выходом с входом электронного вычислительного устройства 5, а выход электронного вычислительного устройства электрически связан с входом блока управления 4. РОССИЙСКАЯ ФЕДЕРАЦИЯ (19) RU (11) (51) МПК H01S 3/227 (13) 166 246 U1 (2006.01) ФЕДЕРАЛЬНАЯ СЛУЖБА ПО ИНТЕЛЛЕКТУАЛЬНОЙ СОБСТВЕННОСТИ (12) ТИТУЛЬНЫЙ (21)(22) Заявка: ЛИСТ ОПИСАНИЯ ПОЛЕЗНОЙ МОДЕЛИ К ПАТЕНТУ 2015140529/28, 23.09.2015 (24) Дата начала отсчета срока действия патента: 23.09.2015 (45) Опубликовано: 20.11.2016 Бюл. № 32 1 6 6 2 4 6 R U (57) Формула полезной модели Лазер на парах металлов, содержащий газоразрядную трубку 1 с электродами 2 на каждом из ее торцевых концов и с навеской металлического стронция внутри нее, оптический резонатор, управляемый высоковольтный блок питания лазера импульсным электрическим током 3, электрически связанный своими выходами с электродами 2 газоразрядной трубки, блок управления 4, обеспечивающий управление величиной напряжения и частотой повторения электрических импульсов блока питания 3 и ...

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03-05-2017 дата публикации

Твердотельный лазер

Номер: RU0000170707U1

Полезная модель относится к лазерной технике. Твердотельный лазер содержит корпус, активный элемент, лампу накачки и резонатор, состоящий из оптически связанных устройства для излома оси резонатора в оправе и концевого элемента в оправе, включающего выходное и глухое зеркала. Устройство для излома оси резонатора выполнено в виде трехгранной призмы БкР - 180°, концевой элемент выполнен в виде стеклянной подложки с нанесенными выходным и глухим зеркалами. Резонатор содержит электрооптический затвор и поляризатор, а оправа с концевым элементом и оправа с устройством для излома оси имеют плоскую опорную поверхность, опирающуюся на соответствующую торцевую грань корпуса. Корпус имеет две противоположные плоские боковые грани, параллельные оптической оси резонатора, причем в корпусе выполнена сквозная полость прямоугольной формы, проходящая через указанные противоположные плоские боковые грани. На боковых гранях корпуса напротив полости установлены две платформы, на первой платформе закреплен первый отражатель, а на второй платформе закреплен второй отражатель, лампа накачки, лазерный электрооптический затвор и поляризатор. Платформы установлены так, что закрепленные на них элементы обращены внутрь сквозной полости, при этом первый и второй отражатели, имеющие внутреннюю рабочую поверхность в виде части цилиндра с диффузно отражающим покрытием, совместно образуют цилиндрическую поверхность, охватывающую активный элемент и лампу накачки, при этом поляризатор и лазерный электрооптический затвор расположены между глухим зеркалом и трехгранной призмой БкР - 180°. Заявляемая полезная модель обеспечивает стабилизацию энергетических и пространственных параметров излучения в широком диапазоне температур окружающей среды и при воздействии ударов и вибрации в широком диапазоне частот и ускорений. 4 ил. РОССИЙСКАЯ ФЕДЕРАЦИЯ (19) RU (11) (13) 170 707 U1 (51) МПК H01S 3/02 (2006.01) H01S 3/115 (2006.01) ФЕДЕРАЛЬНАЯ СЛУЖБА ПО ИНТЕЛЛЕКТУАЛЬНОЙ СОБСТВЕННОСТИ (12) ФОРМУЛА ПОЛЕЗНОЙ МОДЕЛИ ...

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22-08-2018 дата публикации

Твердотельный моноимпульсный лазер

Номер: RU0000182530U1

Полезная модель относится к лазерной технике, а именно к импульсным твердотельным лазерам. Заявленный твердотельный моноимпульсный лазер содержит оптический источник накачки, два активных элемента с теплоотводами, расположенных параллельно источнику накачки симметрично относительно его оси, резонатор, образованный глухим и полупрозрачным зеркалами, и оборачивающую призму с нечетным числом отражений. Оборачивающая призма установлена так, что ее основание обращено к торцам активных элементов и ориентировано параллельно им. Оборачивающая призма в сечении, лежащем в плоскости, содержащей оптические оси активных элементов, выполнена в виде равнобедренной трапеции, причем у верхней грани оборачивающей призмы, противоположной основанию и параллельной ему, введен зеркальный отражатель, совместно с оборачивающей призмой образующий оборачивающую систему, а ширина основания трапеции а и высота h оборачивающей системы связаны соотношениемгдеα>α- угол между основанием оборачивающей призмы и ее боковой гранью;а - ширина основания оборачивающей призмы в плоскости, содержащей оси активных элементов;b - расстояние между оптическими осями активных элементов (база);=arcsin 1/n - угол полного внутреннего отражения;n - показатель преломления материала оборачивающей призмы;Δb - допуск на несоосность активных элементов относительно оптической оси резонатора. Технический результат - увеличение выходной энергии лазерного излучения, повышение однородности энергии в сечении лазерного пучка и обеспечение стабильности направления лазерного пучка в процессе работы лазера. 6 з.п. ф-лы, 3илл РОССИЙСКАЯ ФЕДЕРАЦИЯ (19) RU (11) (13) 182 530 U1 (51) МПК H01S 3/02 (2006.01) G01C 3/08 (2006.01) ФЕДЕРАЛЬНАЯ СЛУЖБА ПО ИНТЕЛЛЕКТУАЛЬНОЙ СОБСТВЕННОСТИ (12) ОПИСАНИЕ ПОЛЕЗНОЙ МОДЕЛИ К ПАТЕНТУ (52) СПК H01S 3/02 (2018.02); G01C 3/08 (2018.02) (21)(22) Заявка: 2017145023, 21.12.2017 (24) Дата начала отсчета срока действия патента: Дата регистрации: 22.08.2018 (45) Опубликовано: 22.08.2018 Бюл. № 24 1 8 2 5 3 ...

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22-08-2018 дата публикации

Твердотельный лазер

Номер: RU0000182531U1

Полезная модель относится к лазерной технике, а именно к импульсным твердотельным лазерам. Твердотельный лазер содержит резонатор, образованный глухим и полупрозрачным зеркалами, оптический источник накачки, два активных элемента с теплоотводами, расположенных параллельно источнику накачки симметрично относительно его оси, и оборачивающую призму, установленную так, что ее основание обращено к торцам активных элементов и ориентировано параллельно им, перекрывая проекции обоих торцов. Теплоотводы активных элементов образуют один общий теплоотвод, расположенный по одну сторону от активных элементов, введен второй источник накачки, причем один источник накачки установлен параллельно первому активному элементу, а второй источник накачки - параллельно второму активному элементу на минимальных расстояниях от них. Оборачивающая призма выполнена в виде призмы-крыши, ребро которой расположено между осями активных элементов перпендикулярно плоскости, в которой лежат эти оси, а глухое зеркало резонатора выполнено в виде призмы БР-180°, ребро которой повернуто на 90° относительно ребра оборачивающей призмы-крыши. Технический результат заключается в обеспечении возможности увеличения выходной энергии излучения, повышения однородности энергии в сечении лазерного пучка и в обеспечении стабильности направления лазерного пучка в процессе работы лазера. 3 з.п. ф-лы, 2 ил. РОССИЙСКАЯ ФЕДЕРАЦИЯ (19) RU (11) (13) 182 531 U1 (51) МПК H01S 3/08 (2006.01) ФЕДЕРАЛЬНАЯ СЛУЖБА ПО ИНТЕЛЛЕКТУАЛЬНОЙ СОБСТВЕННОСТИ (12) ОПИСАНИЕ ПОЛЕЗНОЙ МОДЕЛИ К ПАТЕНТУ (52) СПК H01S 3/08 (2018.05) (21)(22) Заявка: 2017145021, 21.12.2017 (24) Дата начала отсчета срока действия патента: Дата регистрации: 22.08.2018 (45) Опубликовано: 22.08.2018 Бюл. № 24 1 8 2 5 3 1 R U (54) ТВЕРДОТЕЛЬНЫЙ ЛАЗЕР (57) Реферат: Полезная модель относится к лазерной технике, а именно к импульсным твердотельным лазерам. Твердотельный лазер содержит резонатор, образованный глухим и полупрозрачным зеркалами, оптический источник накачки, ...

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22-08-2018 дата публикации

Двухканальный моноимпульсный лазер

Номер: RU0000182532U1

Полезная модель относится к лазерной технике, а именно к импульсным твердотельным лазерам. Заявленный двухканальный моноимпульсный лазер содержит оптический источник накачки, два активных элемента с теплоотводами, расположенных параллельно источнику накачки симметрично относительно его оси, резонатор, образованный глухим и полупрозрачным зеркалами, и оборачивающую призму. Причем оборачивающая призма установлена так, что ее основание обращено к торцам активных элементов и ориентировано параллельно им. Глухое зеркало резонатора выполнено в виде призмы полного внутреннего отражения. Оборачивающая призма в сечении, лежащем в плоскости, содержащей оптические оси активных элементов, выполнена в виде равнобедренной трапеции, причем, на верхнюю грань оборачивающей призмы, противоположную основанию и параллельную ему, установлена призма-крыша, гипотенузная грань которой параллельна верхней грани оборачивающей призмы. Ребро между катетными гранями призмы-крыши лежит в плоскости, содержащей оптические оси активных элементов, а ширина основания а оборачивающей призмы и суммарная высота h оборачивающей системы, состоящей из оборачивающей призмы с призмой-крышей, связаны соотношением где α>α пво - угол между основанием оборачивающей призмы и ее боковой гранью; а - ширина основания оборачивающей призмы в плоскости, содержащей оси активных элементов; b - расстояние между оптическими осями активных элементов (база); α пво =arcsin 1/n - угол полного внутреннего отражения; n - показатель преломления материала оборачивающей призмы и призмы-крыши; Δb - допуск на несоосность активных элементов относительно оптической оси резонатора. Технический результат - повышение выходной энергии лазера при улучшении однородности энергии в сечении лазерного пучка и устранении его отклонения в процессе работы лазера. 6з.п. ф-лы; 3 ил. РОССИЙСКАЯ ФЕДЕРАЦИЯ (19) RU (11) (13) 182 532 U1 (51) МПК H01S 3/02 (2006.01) G01C 3/08 (2006.01) ФЕДЕРАЛЬНАЯ СЛУЖБА ПО ИНТЕЛЛЕКТУАЛЬНОЙ СОБСТВЕННОСТИ (12) ОПИСАНИЕ ...

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19-01-2012 дата публикации

Size segregated aerosol mass concentration measurement with inlet conditioners and multiple detectors

Номер: US20120012744A1
Принадлежит: TSI Inc

A system for measuring size segregated mass concentration of an aerosol. The system includes an electromagnetic radiation source with beam-shaping optics for generation of a beam of electromagnetic radiation, an inlet sample conditioner with adjustable cut-size that selects particles of a specific size range, and an inlet nozzle for passage of an aerosol flow stream. The aerosol flow stream contains particles intersecting the beam of electromagnetic radiation to define an interrogation volume, and scatters the electromagnetic radiation from the interrogation volume. The system also includes a detector for detection of the scattered electromagnetic radiation an integrated signal conditioner coupled to the detector and generating a photometric output, and a processor coupled with the conditioner for conversion of the photometric output and cut-size to a size segregated mass distribution.

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26-01-2012 дата публикации

Determining the Degradation and/or Efficiency of Laser Modules

Номер: US20120020382A1
Принадлежит: Trumpf Laser Gmbh

A method for monitoring a laser system including a plurality of laser modules connected in series, there being connected in parallel to each laser module a bypass arrangement for bridging the corresponding laser module, includes determining a first laser power of the laser system with a plurality of laser modules operational; activating the bypass arrangement of at least one laser module so that at least one of the plurality of laser modules is bypassed; determining a second laser power of the laser system with the at least one of the plurality of laser modules bypassed; and monitoring the laser system based on a difference between the first and second laser power.

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02-02-2012 дата публикации

Fluorescence detection device and fluorescence detection method

Номер: US20120025098A1

When receiving fluorescence emitted by a measurement object irradiated with laser light emitted from a laser light source unit, a fluorescence detection device generates a modulation signal for modulating the intensity of the laser light and modulates the laser light using the modulation signal. The fluorescence detection device obtains a fluorescent signal of the fluorescence emitted by the measurement object irradiated with the laser light, and calculates, from the fluorescent signal, a fluorescence intensity and the phase delay of the fluorescence with respect to the modulation signal. At the time, the fluorescence detection device controls the operation amounts of the signal level of a DC component of the modulation signal and the gain of amplification just after the output of the fluorescent signal so that the value of a fluorescence intensity signal falls within a preset range. After the operation amounts are settled, the fluorescence detection device calculates the fluorescence intensity and then calculates the fluorescence relaxation time of the fluorescence emitted by the measurement object using the phase delay.

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02-02-2012 дата публикации

High power multi-chip pump modules with protection filter for 1060nm, and pump modules including the same

Номер: US20120027043A1
Автор: Bernhard Valk
Принадлежит: OCLARO TECHNOLOGY LTD

A multi-chip pump unit comprising a light source and a filter for directing light from the light source towards an optical fiber, wherein the filter exhibits one of either (i) relatively low transmissivity and high reflectivity at a wavelength of the light source, and relatively high transmissivity and low reflectivity at a wavelength greater than the wavelength of the light source; or (ii) relatively high transmissivity and low reflectivity at a wavelength of the light source, and relatively low transmissivity and high reflectivity at a wavelength greater than the wavelength of the light source.

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09-02-2012 дата публикации

Neon or iodine absorption enhanced hene ring laser gyroscope

Номер: US20120033225A1
Автор: Kenneth Salit, Mary Salit
Принадлежит: Honeywell International Inc

One embodiment of a ring laser gyroscope discussed herein includes a cavity containing a gain medium having a first linewidth, a first plurality of reflective surfaces coupled to the cavity, and at least one medium exciter operable to excite the gain medium. The first plurality of reflective surfaces includes at least first, second, and third reflective surfaces. The first, second, and third reflective surfaces are positioned to reflect light along a path defined in the cavity between the plurality of reflective surfaces. The excited gain medium induces first and second laser fields within the cavity. A portion of the cavity contains an absorption medium having a second linewidth that is narrower than the first linewidth of the gain medium. The absorption medium reduces the gain of the first and second laser fields at a first range of frequencies.

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09-02-2012 дата публикации

Single longitudinal mode fiber laser apparatus

Номер: US20120033688A1

The present invention provides a single frequency fiber laser apparatus. The fiber laser apparatus includes a Faraday rotator mirror. A piece of erbium doped fiber is inside the laser cavity. A wavelength selective coupler is connected to the erbium doped fiber. A pump source is coupled via the wavelength selective coupler. At least one sub-ring cavity component and/or an absorb component are inserted into the cavity for facilitating suppressing laser side modes to create a single longitudinal mode fiber laser. A partial reflectance fiber Bragg grating (FBG) is used as the front cavity end for this fiber laser.

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09-02-2012 дата публикации

Optical pumping of a solid-state gain-medium using a diode-laser bar stack with individually addressable bars

Номер: US20120033692A1
Принадлежит: Coherent Inc

A diode-laser bar stack includes a plurality of diode-laser bars having different temperature dependent peak-emission wavelengths. The stack is arranged such that the bars can be separately powered. This allows one or more of the bars to be “on” while others are “off”. A switching arrangement is described for selectively turning bars on or off, responsive to a signal representative of the temperature of the diode-laser bar stack, for providing a desired total emission spectrum.

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16-02-2012 дата публикации

Passively mode-locked picosecond laser device

Номер: US20120039345A1
Принадлежит: Beijing GK Laser Technology Co Ltd

A passively mode-locked picosecond laser device comprising a pump source, a laser crystal, a laser cavity, a mode-locked output structure is provided. In the device, the pump source is placed at the side of the incident end surface of the laser crystal; the laser cavity includes a plane reflective mirror and a first plano-concave mirror, the reflective mirror is placed opposite to the concave surface of the plano-concave mirror and located on the position of the focal radius of the plano-concave mirror. The normal direction of the reflective mirror and the axis of the plano-concave mirror form a small angle therebetween; the laser generated from the laser crystal oscillates in the laser cavity, and output through the mode-locked output structure. The device uses a stable cavity design of the equivalent confocal cavity, which can increase the optical path, reduce the repetition frequency, and significantly reduce the cavity length and volume.

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01-03-2012 дата публикации

Device for amplifying light impulses

Номер: US20120050843A1

The present invention relates to a device ( 12 ) and to a method for amplifying light impulses ( 13 ). The device comprises a stretcher ( 15 ) stretching the light impulses over time, at least one amplifier ( 16 ) amplifying the stretched light impulses, and a compressor ( 17 ) compressing the stretched and amplified light impulses, wherein the amplifier ( 16 ) applies a non-linear phase generated by self-phase modulation to the stretched light impulses. In order to provide a device and a method for amplifying light impulses, by means of which light impulses having higher light impulse quality and light impulse peak power can be generated, the invention proposes that means for spectrally shaping the light impulses are disposed ahead of the amplifier ( 16 ) in the beam path, wherein the means for spectrally shaping the light impulses bring about a spectral trimming of the light impulses.

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01-03-2012 дата публикации

Intra-cavity second harmonic generation (shg) laser device

Номер: US20120051375A1
Автор: Fedor Karpushko
Принадлежит: Fedor Karpushko

A laser device for intra-cavity frequency conversion, in particular, for the second harmonic generation, the device comprising a laser cavity, formed by the first and the second laser cavity end reflectors wherein the said laser cavity end reflectors are highly reflective for the radiation about the laser fundamental frequency and as such provide for a predetermined level of circulating inside the cavity fundamental frequency power; an active medium provided within the said laser cavity; at least one non-linear crystal, in particular, for the second harmonic generation provided within the same laser cavity; tuning means adapted for tuning at least one of laser cavity end reflectors; wherein at least one of the laser cavity end reflectors comprises an interferometric layout providing spectrally selective reflection for the radiation about the laser fundamental frequency with the value of reflectivity nearly to 100% within a spectral range close to the free spectrum range of the laser cavity and with a sufficiently lower reflectivity outside the above spectral range such that the laser cavity restricts the spectrum of the laser radiation to a single longitudinal mode.

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01-03-2012 дата публикации

Integrated optical fiber gyroscope chip based on surface plasmon polariton waveguide

Номер: US20120051691A1
Принадлежит: SOUTHEAST UNIVERSITY

An integrated optical fiber gyroscope chip based on surface Plasmon Polariton waveguide is an integrated optical fiber gyroscope chip in which optical signal is transmitted through the surface Plasmon Polariton waveguide and the polymer optical waveguide which are connected with each other, and it is used in the optical fiber gyroscope field. From the input end to the output end, the optical fiber gyroscope chip sequentially has: an input waveguide ( 1 ) and the third output waveguide ( 7 ), a directional coupler ( 2 ), a symmetrical triple waveguide splitter ( 3 ), the first output waveguide ( 61 ) and the second output waveguide ( 62 ), wherein the input waveguide ( 1 ), the first output waveguide ( 61 ), the second output waveguide ( 62 ) and the third output waveguide ( 7 ) are polymer optical waveguides, but the directional coupler ( 2 ) and the symmetrical triple waveguide splitter ( 3 ) are made from the surface Plasmon Polariton waveguide. The chip utilizes the transmission characteristics of the surface Plasmon Polariton waveguide to realize the single polarization of long-distance transmission of the optical signal, and directly modulates the surface Plasmon Polariton waveguide core layer, and removes influence of the leakage light to the precision of the fiber gyroscope through the specific structure.

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22-03-2012 дата публикации

Laser irradiation apparatus, laser irradiation method, fabrication method for thin film semiconductor device and fabrication method for display apparatus

Номер: US20120067856A1
Принадлежит: Sony Corp

A laser irradiation apparatus, including: an optical system configured to form laser light of a linear cross section to be irradiated on an irradiation object; and a cutting member having a light blocking portion configured to block the laser light formed in the linear cross section by the optical system to cut the laser light so as to have a predetermined length along a line longitudinal direction; the light blocking portion having a plurality of fins provided on the light blocking portion thereof so as to fetch and absorb the laser light.

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05-04-2012 дата публикации

Large diameter optical waveguide, grating and laser

Номер: US20120082175A1
Принадлежит: Individual

A large diameter optical waveguide, grating, and laser includes a waveguide having at least one core surrounded by a cladding, the core propagating light in substantially a few transverse spatial modes; and having an outer waveguide dimension of said waveguide being greater than about 0.3 mm. At least one Bragg grating may be impressed in the waveguide. The waveguide may be axially compressed which causes the length of the waveguide to decrease without buckling. The waveguide may be used for any application where a waveguide needs to be compression tuned. Also, the waveguide exhibits lower mode coupling from the core to the cladding and allows for higher optical power to be used when writing gratings without damaging the waveguide. The waveguide may resemble a short “block” or a longer “cane” type, depending on the application and dimensions used.

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19-04-2012 дата публикации

Intra-cavity optical parametric oscillator

Номер: US20120093179A1
Принадлежит: University of St Andrews

An optical parametric oscillator comprising: an optical cavity; a semiconductor gain-medium located within the optical cavity, such that together they form a semiconductor laser, and a nonlinear material located within the cavity such that the nonlinear material continuously generates down-converted idler- and signal-waves in response to a pump-wave continuously generated by the semiconductor gain-medium, wherein the pump wave is resonant within the optical cavity and one or other but not both of the down-converted waves is resonant within the pump wave cavity or a further optical cavity. Brewster plates ensure singly resonant optical parametric oscillators and a birefringent filer is used for frequency setting. Coupled cavities allow for setting the photon lifetime in the cavity that relaxation oscillations are prevented.

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31-05-2012 дата публикации

Particle counting method

Номер: US20120133936A1
Принадлежит: Rion Co Ltd

A particle counting method that can count the number of the particles precisely. The method discriminates a wave pattern of the scattered light from a normal particle (subject of the counting) and a wave pattern of the light scattered by the agitation such as a floating particle, a radiation or changes in the intensity of the light. In one embodiment, a method for counting particles is disclosed which irradiates a light to a sample gas, detects a scattered light from a particle included in the sample gas by a photoelectric conversion device, counts the number of the particles of every particle size division by the output voltage wave pattern of the photoelectric conversion device, calculate a time difference (Ta−T 1 ) from a point (T 1 ) being a peak of output voltage wave pattern and a point (Ta) being a falling detection threshold (A), when the time difference (Ta−T 1 ) is beyond counting cancellation time (B), the output voltage wave pattern is not counted as a particle.

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31-05-2012 дата публикации

Optical fiber delivery system for delivering optical short pulses and optical fiber delivery method

Номер: US20120134011A1
Принадлежит: Olympus Corp

The optical fiber delivery system for delivering optical short pulses includes: a chirped pulse source ( 10 ) for emitting an up-chirped optical short pulse having high peak power; optical waveguide unit ( 20 ) for delivering the optical short pulse emitted from the chirped pulse source ( 10 ); negative group-velocity dispersion generation unit ( 30 ) for providing negative group-velocity dispersion to the optical short pulse exited from the optical waveguide unit ( 20 ); and an optical fiber ( 40 ) for delivering the optical short pulse exited from the negative group-velocity dispersion generation unit ( 30 ), along a desired distance, in which the optical short pulse emitted from the chirped pulse source ( 10 ) is adapted to be exited, from the optical fiber ( 40 ), as a down-chirped optical short pulse that is substantially free of waveform distortion resulting from higher-order dispersion.

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28-06-2012 дата публикации

Active body

Номер: US20120160121A1
Принадлежит: RHEINMETALL WAFFE MUNITION GMBH

An active body ( 1 ) includes flares ( 2, 6, 7 ) arranged adjacent, above, or behind each other, wherein at least one hydrophobic separating layer ( 3, 5 ) is integrated between the flares, or flare disks ( 2, 6, 7 ), thereby preventing the flares ( 2, 6, 7 ) from attaching or sticking. In one embodiment, the hydrophobic separating layer ( 3 ) is applied to at least one side of the flares ( 2 ), preferably as a powder preferably consisting of microspheres, or the like. In another embodiment, a separating disk is disposed between the flares ( 6, 7 ) as the separating layer ( 5 ), which in addition is anti-cohesive and anti-adhesive.

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28-06-2012 дата публикации

Enclosure for controlling the environment of optical crystals

Номер: US20120160856A1
Автор: J. Joseph Armstrong
Принадлежит: KLA Tencor Technologies Corp

An enclosure that maintains the environment of one or more optical crystals and allows efficient frequency conversion for light at wavelengths at or below 400 nm with minimal stress being placed on the crystals in the presence of varying temperatures. Efficient conversion may include multiple crystals of the same or different materials. Multiple frequency conversion steps may also be employed within a single enclosure. Materials that have been processed specifically to provide increased lifetimes, stability, and damage thresholds over designs previously available are employed. The enclosure allows pre-exposure processing of the crystal(s) such as baking at high temperatures and allowing real time measurement of crystal properties.

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28-06-2012 дата публикации

Diamond heat sink in a laser

Номер: US20120163406A1
Автор: Robert Linares
Принадлежит: Apollo Diamond Inc

A laser has a laser material in thermal contact with a diamond, such that the diamond is operable to carry heat away from the laser material. In further embodiments, the diamond has a reduced nitrogen content, is a reduced carbon-13 content, is a monocrystalline or multilayer low-strain diamond, or has a thermal conductivity of greater than 2200 W/mK.

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05-07-2012 дата публикации

Remotely Induced Atmospheric Lasing

Номер: US20120170599A1
Принадлежит: US Department of Navy

A laser pulse from an ultrashort pulse laser (USPL) is fired into the atmosphere. The USPL pulse is configured to generate a plasma filament at a predefined target in the atmosphere, in which free, or “seed,” electrons are generated by multi-photon or tunneling ionization of the air molecules in the filament. A second pulse is fired into the atmosphere to form a heater beam that impinges on the plasma filament and thermalizes the seed electrons within the plasma filament, leading to the collisional excitation of the electrons in the filament. The excited electrons collisionally excite various electronic and vibrational states of the air molecules in the filament, causing population inversions and lasing, e.g., exciting the C 3 Π u →B 3 Π g (v=0→0) transition of the N 2 in the atmosphere to cause lasing at 337 nm.

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05-07-2012 дата публикации

Laparoscopic Laser Device and Method

Номер: US20120172856A1
Автор: Kester Nahen
Принадлежит: AMS Research LLC

Laser radiation delivered to a treatment area may be used with a smoke suppressing irrigant. A laparoscopic laser device may include an elongate body adapted for insertion into an insufflated bodily cavity. A laser energy delivery element, at the distal end of the elongate body, may be coupleable to a source of tissue-vaporization-capable laser energy and capable of delivering laser energy along a laser energy path extending away from the laser energy delivery element. A smoke-suppressing liquid may be directed generally along the laser energy path. A remote visualization device may be used to view along the laser energy path. The laser energy path can be shrouded with a circumferentially extending suction manifold so that liquid can be suctioned from the target site and away from the laser energy path. In some examples, the suction manifold is an axially extendable and contractible suction manifold.

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12-07-2012 дата публикации

Optical Pulse Compressor

Номер: US20120177332A1
Принадлежит: Canon Inc

Optical pulse compensator having a chirp unit including a normal dispersion fiber that provides a positive chirp to an input pulse and having a dispersion compensator including an anomalous fiber is provided. The nonlinear coefficient and the absolute value of the second-order group-velocity dispersion of the anomalous fiber that forms the dispersion compensator is set such that a soliton order becomes one or more, and the fiber length of the anomalous dispersion fiber is made to be equal to or smaller than a length required for optical soliton formation.

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09-08-2012 дата публикации

Optical parametric oscillator pumped by femtosecond thin-disk laser

Номер: US20120200912A1
Принадлежит: Coherent Inc

Pulses from a mode-locked Yb-doped laser are spectrally broadened, and temporally compressed, then frequency-doubled and used to pump an optical parametric oscillator (OPO). The OPO output is tunable over a wavelength range from about 600 nm to about 1100 nm.

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23-08-2012 дата публикации

driver for supplying modulated current to a laser

Номер: US20120213237A1
Автор: Iain Ross Mactaggart
Принадлежит: Tyco Electronics Corp

A driver device for a laser includes a control device configured to generate a control current, an NPN differential amplifier connected to the control device and configured to superimpose a modulation current onto the control current to generate a combined current, and a laser activation switch coupled to the output of the NPN differential amplifier, the laser activation switch operating the laser utilizing the combined current. Also described herein is a communication system including a driver device.

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30-08-2012 дата публикации

Fiber lasers for producing amplified laser pulses with reduced non-linearity

Номер: US20120217375A1
Автор: Anthony Hong Lin
Принадлежит: Individual

The present application discloses techniques and devices comprising fiber-based chirped fiber Bragg grating for compressing amplified laser pulses.

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20-09-2012 дата публикации

Wavelength conversion device, solid-state laser apparatus, and laser system

Номер: US20120236894A1
Принадлежит: GIGAPHOTON INC

A wavelength conversion device in this disclosure may include: a nonlinear crystal including a first surface; a first film to be joined to the first surface and including at least one layer; and a first prism to be joined to the first film.

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18-10-2012 дата публикации

Hybrid laser amplifier system including active taper

Номер: US20120262781A1
Принадлежит: NLight Photonics Corp

Hybrid laser systems include fiber amplifiers using tapered waveguides and solid-state amplifiers. Typically, such systems represent a technically simple and low cost approach to high peak power pulsed laser systems. The tapered waveguides generally are provided with an active dopant such as a rare earth element that is pumped with one or more semiconductor lasers. The active waveguide taper is selected to taper from a single or few mode section to a multimode section. A seed beam in a fundamental mode is provided to a section of the waveguide taper associated with a smaller optical mode, and an amplified beam exits the waveguide taper at a section associated with a larger optical mode. The waveguide taper permits amplification to higher peak power values than comparable small mode area fibers. The fiber amplified beam is then directed to a solid state amplifier, such as a thin disk or rod-type laser amplifier.

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25-10-2012 дата публикации

Optical Source with Remote Optical Head Outputting High Power Short Optical Pulses

Номер: US20120268808A1
Принадлежит: Fianium Ltd

An optical source can include a remote optical head for outputting high power short optical pulses. The optical source can include signal source operable to output short optical pulses; an optical pump light source; an optical head provided at a location remote from the location of the optical signal source; and an optical fibre amplifier having at least its optical output located within the optical head. The source can also include an optical signal delivery fibre arranged to deliver optical pulses from the optical signal source to the optical fibre amplifier and a pump light delivery fibre arranged to deliver optical pump light to the high power optical fibre amplifier. In use short optical pulses of a first optical power are delivered to the optical fibre amplifier and are amplified therein to a higher optical power for output from the optical head

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25-10-2012 дата публикации

High-precision synchronization of pulsed gas-discharge lasers

Номер: US20120269223A1
Принадлежит: Coherent GmbH

Two excimer lasers have individual pulsing circuits each including a storage capacitor which is charged and then discharged through a pulse transformer to generate an electrical pulse, which is delivered to the laser to generate a light pulse. The time between generation of the electrical pulse and creation of the light pulse is dependent on the charged voltage of the capacitor. The capacitors are charged while disconnected from each other. The generation of the electrical pulses is synchronized by connecting the capacitors together for a brief period after the capacitors are charged to equalize the charging voltages. The capacitors are disconnected from each other before they are discharged.

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01-11-2012 дата публикации

Titanium-doped amorphous aluminum nitride microlaser device and method for making and using same

Номер: US20120274944A1
Принадлежит: BALL STATE UNIVERSITY BOARD OF TRUSTEES

A microlaser system, including a microlaser, having an elongated generally cylindrical substrate, a thin dopant film encircling at least a portion of the substrate, and a pumping laser positioned to shine onto the thin film. The thin film is between about 2 and about 10 microns thick. When the pumping laser shines on the thin film, the thin film lases in whispering gallery mode. The dopant is preferably selected from the group including transition metals and rare-earth elements. In a most preferred embodiment, the thin film is titanium-doped amorphous aluminum nitride.

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01-11-2012 дата публикации

Method and apparatus for generation and amplification of light in a semi-guiding high aspect ratio core fiber

Номер: US20120275475A1
Принадлежит: Raytheon Co

A planar laser gain medium and laser system. The novel laser gain medium includes an active core having a high aspect ratio cross-section with a fast-axis dimension and a slow-axis dimension, signal claddings adapted to form reflective boundaries at fast-axis boundaries of the core, and a material adapted to minimize reflections at slow-axis boundaries of the core. In an illustrative embodiment, the laser gain medium is an optical fiber. The core and claddings form a waveguide adapted to control modes propagating in the fast-axis direction. When the laser gain medium is employed as a laser oscillator, a high reflectivity mirror and an outcoupler are positioned at opposite ends of the core to form a laser resonator adapted to control modes in the slow-axis direction.

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08-11-2012 дата публикации

Waveguide co2 laser with mutiply folded resonator

Номер: US20120281728A1
Принадлежит: Coherent Inc

A gas-discharge waveguide CO 2 laser has a Z-shaped folded waveguide formed by three ceramic tubes. Ends of the adjacent tubes are shaped and fitted together to form a common aperture. The tubes are held fitted together by spaced-apart parallel discharge electrodes. Four mirrors are arranged to form a laser-resonator having a longitudinal axis extending through the tubes.

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08-11-2012 дата публикации

White Blood Cell Analysis System and Method

Номер: US20120282598A1
Автор: Giacomo Vacca, Jiong Wu
Принадлежит: ABBOTT LABORATORIES

Systems and methods for analyzing blood samples, and more specifically for performing a white blood cell (WBC) differential analysis. The systems and methods screen WBCs by means of fluorescence staining and a fluorescence triggering strategy. As such, interference from unlysed red blood cells (RBCs) and fragments of lysed RBCs is substantially eliminated. The systems and methods also enable development of relatively milder WBC reagent(s), suitable for assays of samples containing fragile WBCs. In one embodiment, the systems and methods include: (a) staining a blood sample with an exclusive cell membrane permeable fluorescent dye, which corresponds in emission spectrum to an excitation source of a hematology instrument; (b) using a fluorescence trigger to screen the blood sample for WB Cs; and (c) using measurements of (1) axial light loss, (2) intermediate angle scatter, (3) 90° polarized side scatter, (4) 90° depolarized side scatter, and (5) fluorescence emission to perform a differentiation analysis.

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22-11-2012 дата публикации

Fluorescence detecting method, method for producing fluorescent beads, and fluorescent beads

Номер: US20120295278A1

Two or more kinds of fluorescent beads containing at least two kinds of basic fluorochromes different in fluorescence intensity, fluorescence wavelength, and fluorescence relaxation time from each other, wherein a content ratio between the at least two kinds of basic fluorochromes and absolute amounts of contents of the basic fluorochromes are set so as to be different between different kinds of fluorescent beads. The fluorescent beads are used in a flow cytometer for fluorescence detection. This makes it possible to identify a greater variety of beads than before with high accuracy in a single measurement.

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06-12-2012 дата публикации

Multiple Flow Channel Particle Analysis System

Номер: US20120307244A1
Принадлежит: Cytonome ST LLC

A microfluidic multiple channel particle analysis system ( 1 ) which allows particles ( 2 ) from a plurality of particle sources ( 3 ) to be independently simultaneously entrained in a corresponding plurality of fluid streams ( 4 ) for analysis and sorting into particle subpopulations ( 5 ) based upon one or more particle characteristics ( 6 ).

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06-12-2012 дата публикации

Pulsed light generation method

Номер: US20120307850A1
Принадлежит: Sumitomo Electric Industries Ltd

The present invention relates to a method of enabling generation of pulsed lights each having a narrow pulse width and high effective pulse energys. A pulse light source has a MOPA structure, and comprises a single semiconductor laser, a bandpass filter and an optical fiber amplifier. The single semiconductor laser outputs two or more pulsed lights separated by a predetermined interval, for each period given according to a predetermined repetition frequency. The bandpass filter attenuates one of the shorter wavelength side and the longer wavelength side, in the wavelength band of input pulsed lights.

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06-12-2012 дата публикации

Impedance-matching transformers for rf driven co2 gas discharge lasers

Номер: US20120307852A1
Принадлежит: Coherent Inc

In a CO 2 gas discharge laser energized by a radio frequency (RF) power source a transformer having selectively variable output impedance is used to match output impedance of the power source to the impedance of discharge electrodes of the laser. A similar transformer can be used to impose a selective variable phase-shift on the RF power from the source. The variable impedance transformer can also be used for impedance matching between amplifier stages in the power source.

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03-01-2013 дата публикации

Apparatus for adjusting polarization characteristics, and ultra-short ultra-high intensity pulse laser generator comprising same

Номер: US20130003763A1

The present invention relates to an apparatus for generating an ultra-short ultra-high intensity pulse laser, comprising: a pulse laser providing unit which generates an ultra-short ultra-high intensity pulse laser, stretches pulse width, then selects and provides only a pulse laser having a predetermined polarizing angle; a polarization characteristic adjusting unit which divides the pulse laser provided by the pulse laser providing unit into S-polarizing component light and P-polarizing component light, varies the phase difference and amplitude difference between the S-polarizing component light and the P-polarizing component light, and combines the two types of light to generate a pulse laser with varied polarization characteristics; and a pulse compression unit which compresses the pulse width of the pulse laser, the polarization characteristics of which are varied by the polarization characteristic adjusting unit, and outputs the pulse laser.

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03-01-2013 дата публикации

Molecular gas laser

Номер: US20130003772A1
Автор: Robert Neil Campbell
Принадлежит: Individual

The closed cycle solid state optically pumped gas hybrid (chemical recovery) system utilizes a laser diode excited solid state, fiber or bulk, laser as a pump for a molecular gas, or gas mix, medium. The existence of efficient high power laser diode excited solid state fiber or bulk lasers, output spectrally matched to suitable principle and excited level 1st and 2nd overtones of relevant gases, is the enabling system technology. The utilization of such in combination with suitable gases introduces a range of viable, in principle sourcing on laser diodes and thus effectively laser diode pumped, gas laser systems with access to the ˜3.5 μm to ˜5.2 μm and ˜9 μm to ˜11 μm spectral region. Continuous wave or pulsed operation, with significant energy capability courtesy of solid state storage, is admitted.

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24-01-2013 дата публикации

Fiber laser device

Номер: US20130022061A1
Автор: Kotaro SHIMOKOSHI
Принадлежит: Fujikura Ltd

A laser diode driving device ( 1 ) of the present invention includes: a variable DC power supply ( 3 ) for outputting a voltage for driving laser diodes (LD1 to LDn); a current driving element ( 4 ) for causing a current If to flow; a current control section ( 5 ) for controlling (i) turning on and off of the current driving element ( 4 ) and (ii) the amount of the current If; and a power supply control section ( 7 ) for controlling an output voltage of the variable DC power supply ( 3 ). The power supply control section ( 7 ) controls, on the basis of If-Vf characteristic data (D 2 ), voltage drop characteristic data (D 3 ), and Vds setting data (D 4 ) all stored in a memory section ( 8 ), the output voltage of the variable DC power supply ( 3 ) so that the current driving element ( 4 ) has a constant inter-terminal voltage regardless of the amount of the current If.

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14-02-2013 дата публикации

Pulse fiber laser device

Номер: US20130038924A1
Принадлежит: Hamamatsu Photonics KK

A pulse fiber laser device 1 has a Fabry-Perot type optical resonator, and is provided with an excitation light source 11 , an optical coupling unit 12 , an amplifying optical fiber 13 , a saturable absorber 14 , a gradient index lens 15 , an optical output unit 16 , a dispersion adjusting unit 17 , a mirror 21 and a mirror 22 . The saturable absorber 14 and the mirror 21 , integrated into one body, constitute a saturable absorber mirror 23 . The gradient index lens 15 converges the light output from an end face of an optical fiber 32 and outputs the light to the saturable absorber mirror 23 , and inputs the light reflected from the saturable absorber mirror 23 into the end face of the optical fiber 32 . Thus, there is provided a pulse fiber laser device that enables easy adjustment of the intensity of light incident on a saturable absorber and facilitates miniaturization.

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14-02-2013 дата публикации

Gas laser apparatus equipped with power calculation unit

Номер: US20130039377A1
Принадлежит: FANUC Corp

Disclosed is a gas laser apparatus having: a first estimation unit which calculates an estimate of input power to the laser power supply device by using the output current value and output voltage value of the DC power supply unit and also using the efficiency of conversion from input power to output power by the DC power supply unit; a second estimation unit which calculates an estimate of input power to the driving device by using the output current value of the driving device; and a power calculation unit which calculates the power consumption value of the gas laser apparatus, based on the estimate of the input power to the laser power supply device and the estimate of the input power to the driving device.

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07-03-2013 дата публикации

Systems and methods for resonator fiber optic gyroscope intensity modulation control

Номер: US20130057870A1
Принадлежит: Honeywell International Inc

Systems and methods for improved resonator fiber optic gyroscope intensity modulation control are provided. In one embodiment, a resonant fiber optic gyroscope (RFOG) having a residual intensity modulation (RIM) controller is provided. The controller includes an intensity modulator optically coupled to receive a light beam from a laser source modulated at a resonance detection modulation frequency, and an optical tap device optically coupled to the intensity modulator. The controller also includes a feedback servo coupled to the optical tap device and the intensity modulator, the demodulating feedback servo generating a sinusoidal feedback signal to the intensity modulator. The feedback servo adjusts an amplitude and phase of the sinusoidal feedback signal provided to intensity modulator based on a residual intensity modulation detected by the demodulating feedback servo.

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07-03-2013 дата публикации

Laser driver

Номер: US20130058368A1
Принадлежит: Texas Instruments Inc

An apparatus is provided. The apparatus includes a lasing element, a laser driver and logic. The laser driver is configured to drive the lasing element at multiple current levels, and the laser driver includes a switching network, multiple direct current (DC) loops, and an output circuit. The switching network receives a differential input signal, and each DC loop is coupled to the switching network. The output circuit is also coupled to the lasing element, and the logic is coupled to each of the DC current loops, where the logic selects one or more of the DC loops in each (of several) modes. Each mode generates one or more output lasing currents for the lasing element that corresponds to a one or more of the current levels in response to the differential input signal.

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14-03-2013 дата публикации

Fine particle measuring apparatus

Номер: US20130065269A1
Автор: Nao Nitta
Принадлежит: Sony Corp

A fine particle measuring apparatus is provided. The fine particle measuring apparatus includes a detection unit configured to detect light emitted from a fine particle and a processing unit having a memory device storing instructions which when executed by the processing unit, cause the processing unit to calculate a corrected intensity value of the detected light and generate spectrum data based on the corrected intensity value.

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21-03-2013 дата публикации

Method and apparatus for measuring optical properties of particles of a dispersion

Номер: US20130070243A1
Автор: Wolfgang Goehde
Принадлежит: Partec GmbH

Disclosed is apparatus for measuring optical properties of particles of a flowable dispersion using a measuring cuvette. The dispersion flows through the central inner chamber of the cuvette. Two laser light beams, which are offset 90 degrees to one another, illuminate the inner chamber of the cuvette, so as to illuminate a particle, regardless of its orientation, in a way that balances out form factor errors.

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21-03-2013 дата публикации

Optical system for signal amplification using a multimode fiber

Номер: US20130070330A1
Автор: Roland Ryf
Принадлежит: Alcatel Lucent USA Inc

An optical coupler for coupling optical-pump power into a multimode fiber configured to transport an optical space-division-multiplexed (SDM) signal, the coupling being performed in a manner that enables amplification of the SDM signal in the multimode fiber via a stimulated-emission process or a stimulated Raman-scattering process. The optical coupler can be a part of an optical transmitter configured for co-directional pumping, an optical receiver configured for contra-directional pumping, or a relay station disposed within an optical communication link and configured for either type of pumping. The optical coupler can advantageously be used, e.g., to offset the different degrees of attenuation to which the SDM-signal components corresponding to different guided modes of the multimode fiber are subjected to therein.

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21-03-2013 дата публикации

LASER APPARATUS AND METHOD OF CONTROLLING THE LASER APPARATUS

Номер: US20130070802A1
Автор: Ichihara Shigeru
Принадлежит: CANON KABUSHIKI KAISHA

Disclosed is a method of controlling a laser apparatus, which has a laser light irradiation unit, an excitation unit including a flash lamp, a laser light shielding unit, and a control unit configured to control light shielding by the light shielding unit and release of the light shielding and control setting conditions of the flash lamp. The control unit performs a process of blocking the laser light by the light shielding unit when irradiation of the laser light is stopped, then performs a process of controlling the setting condition so that consumption of the flash lamp is reduced, performs, when the irradiation is restarted, a process of controlling the setting conditions so that the laser light is stably irradiated, and then performs a process of releasing the light shielding. 1. A method of controlling a laser apparatus , which has an irradiation unit configured to irradiate a laser light to an irradiated object , an excitation unit configured to excite the irradiation unit by emission of a flash lamp , a light-shielding unit configured to block the laser light irradiated from the irradiation unit , and a control unit configured to control light shielding by the light-shielding unit and release of light shielding and control setting conditions associated with the emission of the flash lamp , the control unit performing a method comprising:performing a process of blocking the laser light by the light-shielding unit, when the irradiation with the laser light from the irradiation unit to the irradiated object is stopped;performing a consumption reduction start process of controlling the setting condition so that the consumption of the flash lamp is reduced;performing, when the irradiation with the laser light from the irradiation unit to the irradiated object is restarted, a consumption reduction stop process of controlling the setting condition so that the laser light is stably irradiated by the irradiation unit; andperforming a process of releasing the light ...

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04-04-2013 дата публикации

HIGH-EFFICIENCY METHOD AND DEVICE, TO PRODUCE COHERENT SMITH-PURCELL RADIATION

Номер: US20130083811A1

High-efficiency method and device, to produce coherent Smith-Purcell radiation. A conductive diffraction grating, delimited by two conductive walls, is used, and an electron beam is passed above the grating to generate the radiation. According to the invention, the speed of the electrons is sufficiently low in order that, in a diagram (wave number k, frequency f), the beam line (I) intersects a portion (V) of a branch of the dispersion relationship, located in the first Brillouin zone, and corresponding to the grating's fundamental mode, at a point (P) located outside the zone delimited by the light lines (III, IV), and the current density of the beam is sufficiently high to excite the grating's fundamental mode which is radiated towards the outside thereof. 1. A method for generating coherent Smith-Purcell radiation , in which:an electrically conductive diffraction grating which is delimited laterally by two electrically conductive walls is used, andan electron beam, having determined speed and current density, is passed above the diffraction grating, between the walls delimiting the latter, with a view to producing the coherent Smith-Purcell radiation by interaction of the electron beam with the diffraction grating,characterised in that:the speed of the electrons is sufficiently low in order that, in a dispersion diagram, where the frequency is expressed as a function of the wave number, for the grating-beam combination, a straight line called the beam line (I) and representing the electron beam, intersects a portion (V) of a branch of the three-dimensional dispersion relationship of the diffraction grating, located in the first Brillouin zone, and corresponding to the fundamental mode of the diffraction grating (II), at a point (P) located outside the zone delimited by straight lines called respectively the forward light line and backward light line (III, IV), andthe current density of the electron beam is sufficiently high to excite the fundamental mode of the ...

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04-04-2013 дата публикации

Narrow linewidth brillouin laser

Номер: US20130083813A1
Автор: Arthur H. Hartog
Принадлежит: Schlumberger Technology Corp

A Brillouin laser having a narrowed linewidth, reduced relative intensity noise, and increased output power includes a pump laser that provides pump energy to an optical fiber resonant cavity to stimulate Brillouin emission. The output of pump laser is stabilized and its linewidth is narrowed by locking the frequency and phase of the optical signal generated by the pump laser to a longitudinal mode of the optical fiber resonant cavity. In addition, the resonant cavity is temperature and/or strain-tuned so that the Brillouin gain is substantially centered on a longitudinal mode of the cavity, thereby ensuring that the Brillouin frequency shift is substantially equal to an integer number of the free spectral range of the cavity.

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11-04-2013 дата публикации

Systems And Methods For Amplifying Space-Multiplexed Optical Signals

Номер: US20130088771A1
Принадлежит:

In one embodiment, an optical system for amplifying space-multiplexed optical signals includes an input fiber that propagates multiple spatially-separated optical signals and a bulk amplifier formed of a doped material that receives the multiple spatially-separated optical signals and simultaneously amplifies those signals to generate multiple amplified signals. 1. An optical system for amplifying space-multiplexed optical signals , the system comprising:an input fiber that propagates multiple spatially-separated optical signals; anda bulk amplifier formed of a doped material that receives the multiple spatially-separated optical signals and simultaneously amplifies those signals to generate multiple amplified signals.2. The optical system of claim 1 , further comprising an output fiber that receives the multiple amplified signals from the amplifier.31. The system of claim 1 , wherein the input fiber is a multimode fiber claim 1 , multi-core fiber claim 1 , or a fiber bundle.43. The system of claim 1 , wherein the input fiber is a multi-core fiber having multiple cores and at least one of the cores supports multiple spatial modes.5. The system of claim 1 , wherein the bulk amplifier is made of phosphate glass.6. The system of claim 5 , wherein the phosphate glass is doped with erbium or erbium/ytterbium.7. The system of claim 6 , wherein a doping concentration of the phosphate glass is uniform.8. The system of claim 7 , wherein a doping concentration of the phosphate glass is non-uniform.9. The system of claim 1 , wherein the bulk amplifier is formed as a composite laser rod having a central doped core.10. The system of claim 9 , wherein the composite laser rod comprises multiple discrete segments.11. The system of claim 10 , wherein radiuses of the doped cores of some of the segments are different.12. The system of claim 1 , further comprising a lens positioned between the input fiber and the bulk amplifier.13. The system of claim 12 , further comprising an ...

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11-04-2013 дата публикации

SINGLE MODE PROPAGATION IN FIBERS AND RODS WITH LARGE LEAKAGE CHANNELS

Номер: US20130089113A1
Принадлежит: IMRA AMERICA, INC.

Various embodiments include large cores fibers that can propagate few modes or a single mode while introducing loss to higher order modes. Some of these fibers are holey fibers that comprising cladding features such as air-holes. Additional embodiments described herein include holey rods. The rods and fibers may be used in many optical systems including optical amplification systems, lasers, short pulse generators, Q-switched lasers, etc. and may be used for example for micromachining. 1. (canceled)2. An optical fiber configured to propagate at least one lower order mode having a wavelength , λ , said optical fiber comprising:a core region having a core width; anda cladding region surrounding said core region, said cladding region comprising a plurality of cladding features disposed in a matrix material, said plurality of cladding features having a maximum feature size, d, said plurality of cladding features separated by bridges having a maximum bridge width, a, said bridge comprising matrix material,wherein said core width is greater than about 25 micrometers,wherein said plurality of cladding features are arranged in no more than two layers around said core region, andwherein said maximum bridge width has a value that yields a ratio of a/λ that is at least about 5.3. The optical fiber of claim 2 , wherein said maximum bridge width claim 2 , a claim 2 , has a value that yields a ratio of a/λ that is less than about 100.4. The optical fiber of claim 2 , wherein said core width is less than about 300 micrometers.5. The optical fiber of claim 2 , wherein said maximum feature size claim 2 , d claim 2 , has a value that yields a ratio of d/λ that is in a range from about 5 to 100.6. The optical fiber of claim 2 , wherein said plurality of cladding features have an average center-to-center spacing claim 2 , Λ claim 2 , and wherein d/Λ is greater than about 0.4 and less than about 0.9.7. The optical fiber of claim 2 , wherein said plurality of cladding features are ...

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11-04-2013 дата публикации

LASER COMPRISING A LASER MEDIUM

Номер: US20130089119A1
Автор: Kopf Daniel
Принадлежит: HIGH Q LASER GMBH

A laser having a standing wave resonator including a first resonator section, which has at least a first end mirror and a second resonator section, which has at least a second end mirror. At least one of the optical elements of the first resonator section is embodied in focusing fashion. Accordingly, the beam axes of the laser beam which arrives upon respective tiltings of at least one of the optical elements in the second resonator section have at least one crossing point, which lies in the pump region of the laser medium or is at a distance from the pump region which amounts to less than the Rayleigh length. The radius (w) of the laser beam is less than five times the radius (w) of the laser beam in the pump region of the laser medium. 1. A laser comprising a laser medium , which is excited in a pump region , and a standing wave resonator , which includes optical elements , by which a laser beam , which has a beam axis and penetrates the laser medium , is guided and which comprise a first end mirror and a second end mirror , wherein the resonator comprises a first resonator section , which has at least the first end mirror , and a second resonator section , which has at least the second end mirror , wherein at least one of the optical elements of the first resonator section is a focusing optical element , by which the beam axes of the laser beam , which result upon respective tilts of at least one of the optical elements arranged in the second resonator section , have at least one intersection point , and wherein said intersection point or one of said intersection points of the beam axes of the laser beam lies in the pump region of the laser medium or has a distance from the pump region which is less than a Rayleigh length , which corresponds to a section of the laser beam which lies between the laser medium and a closest one of the focusing optical elements of the first resonator section , a radius (w) of the laser beam , at least over a section of the laser beam ...

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18-04-2013 дата публикации

LASER

Номер: US20130094533A1
Принадлежит: KONINKLIJKE PHILIPS ELECTRONICS N.V.

The invention relates to a laser () for emitting laser light in the visible spectral range. A rare earth doped anisotropic crystal () comprising a -transition is arranged within a laser resonator (), and a pumping light source () pumps the crystal () for generating laser light in the visible spectral range by using the -transition. The -transition of the rare earth doped anisotropic crystal comprises an absorption band extending over several nm. Thus, pump light having a wavelength within a relatively broad wavelength range can be used. This reduces the requirements with respect to the wavelength accuracy of the pumping light source and, thus, more pumping light sources of an amount of produced pumping light sources can be used for assembling the laser, thereby reducing the amount of rejects. 1. A laser for emitting laser light in the visible spectral range , the laser comprising:a laser resonator, characterized by{'b': 5', '4, 'i': d', 'f, 'a rare earth doped anisotropic crystal comprising a -transition, wherein the crystal is arranged within the laser resonator,'}{'b': 5', '4, 'i': d', 'f, 'a pumping light source for pumping the crystal by illuminating the crystal with pump light for generating laser light in the visible spectral range by using the -transition.'}2. The laser as defined in claim 1 , wherein the crystal and the pumping light source are adapted such that the generated laser light is within a green wavelength range.354df. The laser as defined in claim 1 , wherein the crystal is adapted to comprise a specific indicatrix axis claim 1 , wherein the sum of the cross section of the stimulated emission at a visible wavelength range on the -transition of a rare earth doping element with respect to the specific indicatrix axis and the cross section of the excited state absorption at the same visible wavelength range with respect to the same specific indicatrix axis is positive claim 1 , wherein the cross section of the stimulated emission is denoted with a ...

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25-04-2013 дата публикации

LASER APPARATUS, EXTREME ULTRAVIOLET LIGHT GENERATION SYSTEM, AND METHOD FOR GENERATING LASER BEAM

Номер: US20130099140A1
Принадлежит: Gigaphoton Inc.

A laser apparatus may include a seed laser device configured to output a pulse laser beam, a pulse energy adjusting unit configured to vary pulse energy of the pulse laser beam, at least one amplifier for amplifying the pulse laser beam, at least one power source for varying an excitation intensity in the at least one amplifier, and a controller configured to control the pulse energy adjusting unit on a pulse-to-pulse basis for the pulse laser beam passing therethrough and to control the at least one power source for a group of multiple pulses of the pulse laser beam. 1. A laser apparatus , comprising:a seed laser device configured to output a pulse laser beam;a pulse energy adjusting unit configured to vary pulse energy of the pulse laser beam;at least one amplifier for amplifying the pulse laser beam;at least one power source for varying an excitation intensity in the at least one amplifier; anda controller configured to control the pulse energy adjusting unit on a pulse-to-pulse basis for the pulse laser beam passing therethrough and to control the at least one power source for a group of multiple pulses of the pulse laser beam.2. The laser apparatus according to claim 1 , further comprising an energy monitor provided downstream from the at least one amplifier claim 1 , wherein the controller is configured to control the pulse energy adjusting unit on a pulse-to-pulse basis for the pulse laser beam based on a target value of the pulse energy received from an external device and a detected value by the energy monitor.3. The laser apparatus according to claim 1 , further comprising an energy monitor provided downstream from the at least one amplifier claim 1 , wherein the controller is configured to control the at least one power source for a group of multiple pulses of the pulse laser beam based on a target value of the pulse energy received from an external device and a detected value by the energy monitor.4. The laser apparatus according to claim 3 , wherein the ...

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25-04-2013 дата публикации

PUMP ABSORPTION AND EFFICIENCY FOR FIBER LASERS/AMPLIFIERS

Номер: US20130100972A1
Автор: Creeden Daniel J.

Techniques are disclosed for improving pump absorption and efficiency for fiber lasers and amplifiers, for instance. In some embodiments, the techniques are implemented by applying a partially reflective coating on a fiber end-face to double-pass any unabsorbed or otherwise excess pump light in the cladding of a fiber. While being reflective to pump wavelengths, the coating can be non-reflective at the lasing wavelength, so as to avoid unwanted feedback into the system. The benefits of this approach include that excess pump power can be effectively utilized to add more power to the laser output. In addition, the double-pass technique allows for the use of a shorter fiber length, which in turn allows for more compact system designs, saves on material costs, and facilitates manufacturability. 1. An optical fiber comprising:a fiber core;a first cladding surrounding the core;an outer cladding surrounding the first cladding, wherein the outer cladding has a lower index of refraction than the first cladding; anda partial reflector applied to a fiber-to-free-space interface associated with the fiber, wherein the partial reflector is reflective at pump light wavelengths and antireflective at core light wavelengths.2. The optical fiber of claim 1 , wherein the partial reflector is configured to double-pass any unabsorbed pump light back through the first cladding.3. The optical fiber of or claim 1 , wherein the length of the optical fiber is determined based on optimal double-pass absorption of pump light.4. The optical fiber of any of the preceding claims claim 1 , wherein the partial reflector is applied to a tip of the optical fiber.5. The optical fiber of any of the preceding claims claim 1 , wherein a tip of the optical fiber is coated by the partial reflector.6. The optical fiber of any of the preceding claims claim 1 , wherein the partial reflector is applied to a tip of the optical fiber using a fiber connector claim 1 , and connectorization adhesive does not strip ...

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25-04-2013 дата публикации

Controlling Temperature Differences in a Gas Laser

Номер: US20130100975A1
Автор: Borstel Michael von
Принадлежит: TRUMPF LASER- UND SYSTEMTECHNIK GMBH

A gas laser includes discharge tubes connected to together by corner housings, each corner housing including a first cooling channel configured to allow flow of a first coolant. A heat exchanger circuit includes a plurality of second cooling channels configured to allow flow of a second coolant. Each second cooling channel is operable to cool laser gas prior to the laser gas entering into one of the corner housings. The gas laser further includes a temperature control device, in which the temperature control device is selected from the group consisting of a laser gas cooling device, a coolant temperature control assembly, and combinations thereof. The temperature control device is operable to maintain a temperature difference of less than approximately 5 K between the first coolant flowing through the first cooling channel of the corner housing and the laser gas entering into the corner housing. 1. A gas laser comprising:a plurality of discharge tubes, the discharge tubes being connected to together by corner housings, each corner housing comprising a mirror element for guiding a laser beam and a first cooling channel configured to allow flow of a first coolant;a primary heat exchanger circuit comprising a plurality of second cooling channels configured to allow flow of a second coolant, wherein each second cooling channel is operable to cool laser gas prior to the laser gas entering into one of the corner housings; andat least one temperature control device being selected from the group consisting of a laser gas cooling device, a coolant temperature control assembly operable to generate a temperature difference between the first coolant flowing in the first cooling channel of the corner housing and the second coolant flowing in the second cooling channel of the primary heat exchanger circuit, and combinations thereof, wherein the at least one temperature control device is operable to maintain a temperature difference of less than approximately 5 K between the first ...

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02-05-2013 дата публикации

Biochip

Номер: US20130104632A1
Принадлежит: Wistron Corp

A biochip including a chip body, a first electrode and a second electrode is provided. The body has a first accommodating cavity, a second accommodating cavity and a micro-fluid channel. The micro-fluid channel is connected with the first accommodating cavity and the second accommodating cavity. The first electrode has a first end and a second end. The first end is used for contacting a first probe of a detection apparatus. The second end is positioned in the first accommodating cavity. The second electrode has a third end and a forth end. The third end is used for contacting a second probe of the detection apparatus. The forth end is positioned in the second accommodating cavity.

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02-05-2013 дата публикации

DIVERSIONARY DEVICE

Номер: US20130104766A1
Автор: THOMAS Duncan
Принадлежит: THOMAS LOWE DEFENCE

A diversionary device has a housing containing a pyrotechnic cartridge () with an ignitable fuse (). A firing arrangement includes an ignition cap () containing a primer charge (). Passageways () in the housing and ignition cap define a first flow path from the primer charge to a region of the housing in which the fuse () is located through which flash from the primer charge can flow to ignite the fuse (). A further flow path connects said region of the housing with the exterior of the housing to supply the fuse with oxygen for reliable burning. The device may be a multi-burst device containing a plurality of cartridges () and the first flow path may include a flash divider () for directing a proportion of the flash from a primer charge on to the fuse () of each cartridge. The housing may be separable to allow replacement of the cartridges (). 1. A diversionary device comprising a housing having an outer housing portion defining an internal cavity , at least one replaceable pyrotechnic cartridge mounted in the housing and at least partly located within the internal cavity , the cartridge having a first end containing an ignitable fuse , the housing defining a region in which the first end of the at least one cartridge is located , a firing arrangement mounted to the housing and including an ignition cap containing a primer charge , the housing and ignition cap defining a first flow path from the primer charge to the housing region to provide a fluid path through which a proportion of a flash of heat and pressure given off by a primer charge in the ignition cap when it is fired is can flow to ignite the fuse , in which a further flow path is provided to fluidly connect the housing region with the exterior of the housing.27.-. (canceled)8. A diversionary device as claimed in claim 1 , in which the outer housing portion includes a hollow side wall region closed at either end by means of an end closure to define the internal cavity claim 1 , at least one of the end ...

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09-05-2013 дата публикации

LARGE CORE AREA SINGLE MODE OPTICAL FIBER

Номер: US20130114129A1
Принадлежит: NKT Photonics A/S

A single-mode optical fiber for guiding an optical signal, wherein the core region is capable of guiding an optical signal in a fundamental core mode at an optical signal wavelength. A cladding region is arranged to surround the core region and includes an inner cladding region and an outer cladding region. The inner cladding region includes a background material and a plurality of inner cladding features arranged in the background material, wherein a plurality of the plurality of inner cladding features are of a first type of feature that includes an air hole surrounded by a high-index region comprising a high-index material that is larger than the refractive index of the inner cladding background material. 163-. (canceled)64. A single-mode optical fiber for guiding an optical signal , said optical fiber having a longitudinal , optical axis and a cross section perpendicular thereto , said optical fiber comprising:{'sub': c', '1, 'a core region being capable of guiding an optical signal in a fundamental core mode with an effective refractive index, n, at an optical signal wavelength, λ;'}{'sub': b', 'r', '1', 'c', '1, 'a cladding region surrounding the core region, the cladding region comprising an inner cladding region and an outer cladding region, said inner cladding region comprising a background material having a refractive index, n, and a plurality of inner cladding features arranged in said background material, wherein at least a plurality of said plurality of inner cladding features are of a first type of feature, said first type of feature comprising an air hole surrounded by a high-index region comprising a high-index material having a refractive index, n, that is larger than the refractive index of the inner cladding background material, said first type of feature supports an optical mode with an effective refractive index, n, which is lower than or equal to the effective refractive index of the fundamental core mode, n, at said optical signal wavelength, ...

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09-05-2013 дата публикации

METHOD AND DEVICE FOR OBTAINING AN OPTICAL DISCHARGE IN A GAS

Номер: US20130114637A1
Принадлежит:

The invention relates to the field of laser physics and laser technology and can be used in the development and creation of plasma-chemical systems based on lasers. 1. Method of obtaining an optical discharge in a gas consisting of optical breakdown of the gas to form a plasma region and maintain it in a laser beam during the duration of its action , characterized in that the breakdown of the gas to form a plasma region and its maintenance is carried out in the laser cavity.2. The method according to claim 1 , characterized in that the formation of a plasma region and its maintenance is carried out in an additional cavity of three-mirror laser cavity.3. The method according to claim 1 , characterized in that the formation of a plasma region and its maintenance is carried out in the focal region of a conical laser beam .4. The method according to wherein the formation of a plasma region and its maintenance is carried out in the focal region of a volumetric laser beam.5. Device to obtain an optical discharge in a gas containing a laser claim 1 , optically coupled to the focusing lens characterized in that it further comprises a laser claim 1 , optically coupled to the focusing lens system forming a ring beam in a reflective axicon and the conical mirror and rotating conical mirror claim 1 , the angle converging conical beam is 1800.6. Device to obtain an optical discharge in a gas containing a laser claim 1 , optically coupled to the focusing lens characterized in that it further comprises a laser claim 1 , which is a set of disk or diode laser segments located on the surface of a sphere centered at the point of intersection of the optical axis. The invention relates to the field of laser physics and laser technology and can be used in the development and creation of plasma-chemical systems based on lasers.There is a method [1] of obtaining an optical discharge in a gas consisting of optical breakdown of the gas to form a plasma region and maintain it in a laser beam ...

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16-05-2013 дата публикации

OPTICAL AMPLIFIERS

Номер: US20130120831A1
Принадлежит:

An optical amplifier system is provided which comprises first and second optical amplifiers () for amplifying optical signals in a fibre optic communications link and a common pump () for optically pumping both the first amplifier () and the second amplifier () to effect such amplification. There is also provided an optical switch () for providing an optical path between the pump and the first amplifier in a first switching state and an optical path between the pump and the second amplifier in a second switching state to enable pumping of the first and second amplifiers by the pump sequentially. Advantageously this arrangement provides high accuracy to the outputs () of the pump () and reduces low power pump noise. 1. An optical amplifier system comprising:(i) first and second optical amplifiers for amplifying optical signals in a fibre optic communications link,(ii) a common pump for optically pumping both the first amplifier and the second amplifier to effect such amplification, and(iii) switching means for providing an optical path between the pump and the first amplifier in a first switching state and an optical path between the pump and the second amplifier in a second switching state to enable optical pumping of the first and second amplifiers by the pump sequentially,wherein the switching means is adapted to independently vary the power supplied to one of the first and second amplifiers from 0% to maximum pump power.2. An optical amplifier system according to claim 1 , wherein the switching means includes an input coupled to the pump and outputs coupled to the first amplifier and the second amplifier.3. An optical amplifier system according to claim 1 , further comprising a grating coupled to an input or an output of the switching means so as to lock the optical path between the pump and the first amplifier in the first switching state and to lock the optical path between the pump and the second amplifier in the second switching state.4. (canceled)5. An ...

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16-05-2013 дата публикации

INFRARED LASER

Номер: US20130121353A1
Принадлежит:

Laser devices are presented in which a graphene saturable absorber and an optical amplifier are disposed in a resonant optical cavity with an optical or electrical pump providing energy to the optical amplifier. 1. A linear cavity laser device , comprising:a first mirror with a first surface;a second mirror with a second surface at least partially facing the first surface of the first mirror, the first and second mirrors defining a resonant optical cavity in which electromagnetic energy is amplified by stimulated emission of coherent radiation that is partially transmitted through the second mirror;a solid-state optically pumped optical gain medium disposed at least partially between the first and second surfaces;an optical pump providing light to the solid-state optically pumped optical gain medium; anda graphene saturable absorber disposed at least partially between the solid-state optically pumped optical gain medium and the first surface.2. The linear cavity laser device of claim 1 , wherein the solid-state optically pumped optical gain medium is a rare earth doped fiber amplifier operable at wavelengths of about 1.4 μm or more and about 3.0 μm or less.3. The linear cavity laser device of claim 1 , wherein the solid-state optically pumped optical gain medium is a solid state optically pumped infrared optical gain medium.4. The linear cavity laser device of claim 1 , wherein the solid-state optically pumped optical gain medium includes at least one II-VI family doped crystal.5. The linear cavity laser device of claim 1 , wherein the solid-state optically pumped optical gain medium includes at least one transition metal doped zinc chalcogenide.6. The linear cavity laser device of claim 1 , wherein the solid-state optically pumped optical gain medium includes at least one rare earth doped or transition metal doped laser ceramic.7. The linear cavity laser device of claim 1 , wherein the solid-state optically pumped optical gain medium includes at least one lead salt ...

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16-05-2013 дата публикации

Mode control waveguide-type laser device

Номер: US20130121355A1
Принадлежит: Mitsubishi Electric Corp

In a laser device, a control range of focal distance of a generated thermal lens is broadened and reliability is improved. A mode control waveguide-type laser device includes: a planar laser medium having a waveguide structure in a thickness direction of a cross section perpendicular to an optical axis, for generating gain with respect to laser light; a cladding bonded onto the laser medium; and a heat sink bonded onto the laser medium. The laser medium generates a lens effect, and the laser light oscillates in a waveguide mode in the thickness direction, and oscillates in a spatial mode due to the lens effect in a direction perpendicular to the optical axis and the thickness direction. The refractive index distribution within the laser medium is created by generating a temperature distribution in the laser medium depending on a junction area of the cladding and the heat sink.

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16-05-2013 дата публикации

Method of Forming a Single Common Laser Resonator Cavity and an Optically Segmented Composite Gain Medium

Номер: US20130121363A1
Автор: Goldberg Lew

A compact solid state laser that generates multiple wavelengths and multiple beams that are parallel, i.e., bore-sighted relative to each other, is disclosed. Each of the multiple laser beams can be at a different wavelength, pulse energy, pulse length, repetition rate and average power. Each of the laser beams can be turned on or off independently. The laser is comprised of an optically segmented gain section, common laser resonator with common surface segmented cavity mirrors, optically segmented pump laser, and different intra-cavity elements in each laser segment. 1. An optically segmented composite gain medium , each segment of the composite gain medium functioning as an optical waveguide for a respective pump light of a segmented laser diode pump array , said optically segmented composite gain medium comprising:a plurality of gain medium sections, each gain medium section being based on a selected gain material to function as an optical waveguide for the respective pump light; andseparation regions defined by a region separating adjacent regions of said plurality of gain medium sections for optical isolation based on a material of lower refractive index, the lower index material forming each separation region.2. The optically segmented composite gain medium recited in claim 1 , wherein a refractive index step between the respective adjacent gain material and the lower refractive index region causes all light below the critical angle to be reflected at the respective boundary claim 1 , allowing each gain medium section to function as an optical waveguide for the respective pump light claim 1 , pump light injected into each section being wave-guided along the respective section without coupling into adjoining gain sections.3. The optically segmented composite gain medium recited in claim 1 , wherein each section of gain medium is either a slab or a rod based on a selection of material chosen from a group consisting of Nd:YAG claim 1 , Yb:YAG claim 1 , Nd:YVO ...

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23-05-2013 дата публикации

Laser oscillation apparatus

Номер: US20130128906A1

Provided is a laser oscillation apparatus capable of stabilizing resonance even when finesse of an optical resonator is increased and generating stronger laser light than that of a traditional apparatus by accumulating laser light in the optical resonator. The laser oscillation apparatus includes a laser light source which generates laser light for excitation, a fiber amplifier which generates laser light with a desired wavelength when the laser light generated at the laser light source for excitation is supplied, an optical resonator, an optical isolator which is interposed between the optical resonator and the fiber amplifier and which guides the laser light from the fiber amplifier to one side of the optical resonator while blocking laser light in the opposite direction, a circulation optical path which accelerates resonance as introducing laser light emitted from the other side of the optical resonator and returning the laser light to the optical resonator via the fiber amplifier and the optical isolator, and a modulator which performs amplitude modulation on the laser light in the circulation optical path.

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23-05-2013 дата публикации

DIODE PUMPED SOLID STATE OPTO-MECHANICALLY OPTIMIZED GREEN LASER

Номер: US20130128908A1
Принадлежит: Laser Energetics Inc.

A unique physical design of 532 nm Diode Pumped Solid State (DPSS) laser elements to achieve independent crystal phasing (rotation), spacing and output coupler (OC) alignment in a robust small package is provided. 1. A laser apparatus comprising:a laser diode, an Nd:YVO4 crystal, a KTP crystal, and an output coupler, aligned in order in an assembly in an optical path;wherein the Nd:YVO4 crystal is held at a predetermined distance from the laser diode on an adjustable rotating mount, the predetermined distance maintained by a spacer, the adjustable rotating mount and spacer together forming an Nd:YVO4 assembly.2. The laser apparatus according to claim 1 , wherein the a collimating lens is placed between the laser diode and the Nd:YVO4 crystal.3. The laser apparatus according to claim 1 , wherein the laser diode incorporates a collimating lens.4. The laser apparatus according to claim 1 , wherein the Nd:YVO4 crystal is optimally rotated to a position to maximize output of the laser diode through the Nd:YVO4 crystal to produce 1064 nm radiation claim 1 , the position fixed by a plurality of adjustment screws attached to the adjustable rotating mount.5. The laser apparatus according to claim 4 , wherein the KTP crystal is held at a second predetermined distance from the Nd:YVO4 crystal on a second rotating mount claim 4 , the second predetermined distance maintained by a second spacer claim 4 , the second rotating mount and second spacer having a plurality of rods and nuts fastened thereto for adjusting the pitch and yaw of the KTP crystal.6. The laser apparatus according to claim 5 , further comprising the second spacer includes a plurality of spring loaded adjustment screws claim 5 , wherein the second predetermined distance of the second spacer is adjusted using the spring loaded adjustment screws.7. The laser apparatus according to claim 5 , wherein the output coupler is held by an output coupler assembly claim 5 , the output coupler assembly holding the output ...

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30-05-2013 дата публикации

TUNABLE MODE LOCKED LASER

Номер: US20130136147A1
Автор: Villeneuve Alain
Принадлежит:

A laser for emitting simultaneously a first and second laser lights having respectively first and second wavelength differing from each other. The laser comprises: an optical resonator defining a first optical path and a second optical path, the first laser light travelling along the first optical path and the second laser light travelling along the second optical path; a modulated gain element inserted in the optical resonator for amplifying the first and second laser lights as the first and second laser lights propagate in the optical resonator respectively along the first and second optical paths, the modulated gain element having a variable gain modulated with a modulation period, round trip times of the first and second laser lights along respectively the first and second optical paths being respective integer multiples of the modulation period; and an output port for releasing the first and sec and laser lights from the optical resonator. 1. A laser cavity for emitting simultaneously a first laser light having a first wavelength and a second laser light having a second wavelength using pump light emitted by a pump light source , said first and second wavelengths differing from each other , said laser cavity comprising:an optical resonator, said optical resonator defining a first optical path and a second optical path, said first laser light travelling along said first optical path and said second laser light travelling along said second optical path;a gain medium inserted in said optical resonator, said gain medium being responsive to said pump light for converting said pump light to said first and second laser lights;a pump light input port optically coupled to said gain medium for receiving said pump light and conveying said pump light to said gain medium;an optical intensity modulator inserted in said optical resonator for absorbing simultaneously a portion of both said first and second laser lights as said first and second laser lights propagate in said ...

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06-06-2013 дата публикации

FRAME ELEMENT OF A LASER GYROSCOPE COMPRISING A SUBSTRATE COMPRISING MOBILE IONS AND AN ELECTRODE

Номер: US20130141732A1
Принадлежит: THALES

The invention pertains to a frame element of a laser gyroscope comprising a substrate comprising mobile ions and an electrode fixed to the said substrate, comprising at least one electrically conducting element, connected electrically to the said electrode, and furnished with at least one distal part integrated into the said substrate and exhibiting at least one tip and/or at least one groove, forming at least one blind hole and/or at least one groove in the said substrate, of shape corresponding to that of the said distal part or parts, so as to obtain a tip effect. 1104. Frame element of a laser gyroscope comprising a substrate comprising mobile ions and an electrode fixed to the said substrate , wherein that it comprises at least one electrically conducting element () , connected electrically to the said electrode , and furnished with at least one distal part integrated into the said substrate and exhibiting at least one tip and/or at least one groove , forming at least one blind hole and/or at least one groove in the said substrate , of shape corresponding to that of the said distal part or parts , so as to obtain a tip effect.2. Frame element of a laser gyroscope according to claim 1 , in which at least one groove exhibits a radius of curvature of a value less than the square of the greatest length of the zone of the substrate to be protected claim 1 , divided by the minimum distance separating the said groove and the zone of the substrate to be protected.3. Frame element of a laser gyroscope according to claim 1 , in which at least one tip exhibits a radius of curvature of a value less than the square of the greatest length of the zone of the substrate to be protected claim 1 , divided by the minimum distance separating the said tip and the zone of the substrate to be protected.4. Frame element of a laser gyroscope according to claim 3 , in which at least one groove exhibits a radius of curvature of a value less than the square of the greatest length of the ...

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06-06-2013 дата публикации

PULSE COMPRESSION SYSTEMS AND METHODS

Номер: US20130142207A1
Автор: Sankar Pat
Принадлежит:

A non-linear FM pulse compression system includes a non-linear FM transmitter adapted to receive an input signal and transmit an output signal. The non-linear FM transmitter is adapted to modulate the frequency of the output signal by at least one of the following: increasing the frequency of the output signal as a logarithmic function of the frequency of samples in the input signal; modulating the frequency of the output signal in inversely proportional relationship to the frequency of samples in the input signal; and modulating the frequency of the output signal according to a random permutation of the frequency of the input signal. At least one antenna interfaces with the non-linear FM transmitter. A non-linear FM receiver interfacing with the at least one antenna. The non-linear FM receiver is adapted to auto-correlate the output signal with a return signal. 1. A free electron laser system , comprising:an undulator having a first series of magnets and a second series of magnets, the first and second series of magnets configured to be positioned substantially parallel to and spaced apart from each other, the first series comprising two or more adjacent magnets and the second series comprising two or more adjacent magnets, wherein adjacent magnets in the first series of magnets have north poles rotated approximately 90 degrees from each other and adjacent magnets in the second series of magnets have north poles rotated approximately 90 degrees from each other;a laser cavity defined between the first and second series of magnets; andan electron source configured to emit an electron beam through the laser cavity.2. The system of claim 1 , wherein the magnets are permanent magnets.3. The system of claim 1 , further comprising a full-silvered mirror and a half-silvered mirror at opposite ends of the laser cavity.4. The system of claim 1 , wherein the north poles are rotated about an axis perpendicular to the first and second series of magnets.5. The system of claim 4 ...

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06-06-2013 дата публикации

OPTICAL AMPLIFIER AND LASER INCORPORATING SUCH AN AMPLIFIER

Номер: US20130142208A1
Принадлежит: AMPLITUDE SYSTEMES

A high-gain optical amplifier for a wave to be amplified at a wavelength referred to as the emission wavelength, includes: optical pumping elements () producing a pump wave at a wavelength referred to as the pump wavelength; a solid amplifying medium () that is doped with active ions, the solid amplifying medium being capable of emitting laser radiation at the emission wavelength when the medium is pumped by the pumping elements; cooling elements () capable of cooling the solid amplifying medium to a temperature of no higher than 250 Kelvin; and optical multiplexing elements capable of coupling together the pump wave and the wave to be amplified in the amplifying medium. The amplifying medium has Stark sublevels contained within a spectral domain ranging over less than 200 cm(approximately 20 nm, when expressed in wavelength). A laser including a resonant optical cavity and an amplifier are also described. 1. A high-gain optical amplifier for a wave to be amplified at a wavelength referred to as the emission wavelength , comprising:{'b': '4', 'optical pumping means () producing a pump wave at a wavelength referred to as the pump wavelength;'}{'b': 1', '1, 'a solid amplifying medium () that is doped with active ions, said solid amplifying medium () being capable of emitting laser radiation at an emission wavelength when it is pumped by said pumping means;'}{'b': 2', '1, 'cooling means () capable of cooling said solid amplifying medium () to a temperature lower than or equal to 250 Kelvin;'}optical multiplexing means capable of coupling together the pump wave and the wave to be amplified in the amplifying medium,characterized in that:{'b': '1', 'sup': '−1', 'the solid amplifying medium () has Stark sublevels contained within a spectral domain ranging over less than 200 cm(about 20 nm when expressed in wavelength).'}2. The optical amplifier according to claim 1 , characterized in that the active ions are ytterbium ions.3. The optical amplifier according to claim 2 , ...

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13-06-2013 дата публикации

WAVELENGTH SWEEP CONTROL

Номер: US20130148190A1
Автор: Taverner Domino
Принадлежит: WEATHERFORD/LAMB, INC.

Methods and apparatus for the active control of a wavelength-swept light source used to interrogate optical elements having characteristic wavelengths distributed across a wavelength range are provided. 1. A method comprising:providing light, wherein a wavelength of the light is changed according to a sweep function;interrogating one or more optical elements with the wavelength-swept light to produce optical signals;filtering the optical signals, wherein a bandpass wavelength range is changed based on the sweep function to follow the changes in the light's wavelength; andreceiving the filtered optical signals for processing.2. The method of claim 1 , wherein the optical elements comprise transmissive optical elements.3. The method of claim 1 , wherein the sweep function comprises a constant sweep rate.4. The method of claim 3 , wherein the sweep rate is set to a trip frequency or a harmonic thereof claim 3 , wherein the trip frequency is equal to a speed of light in an optical waveguide for conveying the optical signals divided by a trip distance of the light from a light source to the furthest one of the optical elements and then to a receiver via the optical waveguide.5. The method of claim 1 , wherein filtering the optical signals comprises filtering out Rayleigh scattering and back-reflections from an optical waveguide conveying the optical signals.6. The method of claim 1 , further comprising delaying the sweep function before filtering claim 1 , such that the changing of the bandpass wavelength range is delayed from the changing of the light's wavelength.7. The method of claim 1 , wherein delaying the sweep function comprises delaying the sweep function by a trip distance of the light claim 1 , in an optical waveguide for conveying the optical signals claim 1 , from a light source to one of the optical elements and then to a receiver divided by a speed of light in the optical waveguide.8. The method of claim 1 , wherein filtering the optical signals comprises ...

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20-06-2013 дата публикации

Semiconductor Wavelength Converting Devices and Light Sources for Generating Infrared Rays

Номер: US20130156062A1
Принадлежит: NGK Insulators, Ltd.

It is provided a wavelength converting device oscillating an idler light having a wavelength of 5 to 10 μm from a pump light. The wavelength of the idler light is longer than that of the pump light. The wavelength converting device includes a wavelength converting layer of a semiconductor non-linear optical crystal and having a thickness of 50 μm or smaller. The wavelength converting layer includes a crystal orientation inversion structure wherein crystal orientation of the optical crystal is inverted at a predetermined period and at least one flat main face . The device further includes a Peltier device controlling a temperature of the wavelength converting layer and a clad portion joined with the flat main face of the wavelength converting layer and provided between the wavelength converting layer and the Peltier device The pump light, idler light and signal light satisfies a particular phase matching condition. 1. A wavelength converting device generating an idler light having a wavelength of 5 to 10 μm from a pump light , said wavelength of said idler light being longer than that of said pump light , said wavelength converting device comprising:a wavelength converting layer comprising a semiconductor non-linear optical crystal and having a thickness of 50 μm or smaller, said wavelength converting layer comprising at least one flat main face and a crystal orientation inversion structure wherein crystal orientation of said optical crystal is inverted at a predetermined period;a Peltier device controlling a temperature of said wavelength converting layer; anda clad portion joined with said flat main face of said wavelength converting layer and provided between said wavelength converting layer and said Peltier device; {'br': None, 'i': n p/λp', 'n s/λs', 'n i/λi, '()=()+()+(1/Λ) \u2003\u2003(1)'}, 'wherein said pump light, said idler light and said signal light satisfies a phase matching condition of the following formula (1), in the conditions that “np” represents ...

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27-06-2013 дата публикации

COHERENT LIGHT SOURCE APPARATUS AND PROJECTOR

Номер: US20130162955A1
Принадлежит: USHIO DENKI KABUSHIKI KAISHA

A coherent light source apparatus includes a coherent light source, a first optical system, a light deflection unit, a second optical system and a light mixing unit disposed in that order. The coherent light source forms a first light emission region, and light projected therefrom forms a second light emission region near the light deflection unit, which deflects light flux from the second light emission region. The second optical system forms a third light emission region which is conjugate to the second light emission region near an input end of the light mixing unit, which mixes angle and a position components of incident light. The light deflection unit is configured to continuously changing a direction in which the light flux is deflected, thereby reducing speckling in light emitted from the light mixing unit. 1. A coherent light source apparatus comprising:a first optical system, which comprises a first light emission region formed by a coherent light source, wherein light is projected from the first light emission region to form a second light emission region;a light deflection unit, that deflects light flux relating to formation of the second light emission region near the second light emission region;a second optical system, that is disposed downstream of the light deflection unit and forms a third light emission region that is conjugate to the second light emission region; anda light mixing unit that is disposed downstream of the second optical system, the light mixing unit mixes components of an angle and a position of an incident light, wherein an incident end of the light mixing unit is provided near the third light emission region,wherein the light deflection unit is configured to perform an operation for continuously changing a direction in which the light flux is deflected.2. The coherent light source apparatus according to claim 1 , wherein the light mixing unit is an optical guide that guides light waves while confining the light in a predetermined ...

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04-07-2013 дата публикации

LASER MACHINE AND CONTROLLING METHOD OF LASER MACHINE

Номер: US20130170514A1
Принадлежит: AMADA COMPANY, LIMITED

A laser machine includes a laser oscillator, a cooler for cooling the laser oscillator, and a control unit for controlling the laser oscillator and the cooler. The control unit includes a controller that stops base discharge of the laser oscillator at a time when a specified time has elapsed from a stop of laser light emission by the laser oscillator. According to the laser machine, since base discharge of the laser oscillator is stopped after the specified time has elapsed from the stop of laser light emission, wasteful energy (power) consumption of the laser oscillator in a standby state can be restricted. 1. A laser machine comprising:a laser oscillator;a cooler for cooling the laser oscillator; anda control unit for controlling the laser oscillator and the cooler, whereinthe control unit includes a controller that stops base discharge of the laser oscillator at a time when a specified time has elapsed from a stop of laser light emission by the laser oscillator.2. The laser machine according to claim 1 , whereinthe controller reduces a supplied amount of laser gas supplied to the laser oscillator at the time when or after the specified time has elapsed.3. The laser machine according to claim 1 , whereinthe controller expands temperature control range of a cooling medium of the cooler at the time when or after the specified time has elapsed.4. The laser machine according to claim 1 , further comprisinga switch that triggers the controller in a state of the stop of laser light emission by the laser oscillator.5. A controlling method of a laser machine that includes a laser oscillator claim 1 , the method comprising:stopping base discharge of the laser oscillator at a time when a first specified time has elapsed from a stop of laser light emission by the laser oscillator.6. The controlling method of a laser machine according to claim 5 , further comprisingreducing a supplied amount of laser gas supplied to the laser oscillator at a time when a second specified time ...

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18-07-2013 дата публикации

LASER PROCESSING APPARATUS

Номер: US20130182727A1
Принадлежит:

A laser marking apparatus is provided with a laser emission unit that emits laser beam and a laser radiation unit that is detachably connected to the laser emission unit. The laser radiation unit radiates the laser beam emitted from the laser emission unit toward an object to be processed. A projection, which projects rearward, is formed on a part of the laser radiation unit that is connected with the laser emission unit. A recess is provided in a part of the laser emission unit that is connected with the laser radiation unit. The projection can fit into the recess. The recess is opened forward, backward, to lateral sides, and downward. 110-. (canceled)11. A laser processing apparatus comprising:a laser oscillation portion;a laser emission unit including an emission optical system that emits a laser beam oscillated by the laser oscillation portion;a laser radiation unit that is detachably connected to the laser emission unit and has a radiation optical system for radiating the laser beam emitted from the laser emission unit to an object to be processed;a first connection portion provided in a part of the laser emission unit that is connected to the laser radiation unit;a second connection portion provided in a part of the laser radiation unit that is connected to the laser emission unit;a projection provided on a lower end portion of one of the first connection portion and the second connection portion, the projection protruding along an optical axis of the laser beam; anda recess provided on a lower end portion of the other one of the first connection portion and the second connection portion, whereinthe recess can fit the projection and slideably guide the projection along the optical axis, andthe recess is open in a direction facing at least the projection in an optical axis direction and downward in a direction intersecting the optical axis.12. The laser processing apparatus according to claim 11 , further comprising a main unit that has the laser oscillation ...

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18-07-2013 дата публикации

CONTINUOUS MASS FLOW GAS REPLENISHMENT FOR GAS LASING DEVICES

Номер: US20130182737A1
Принадлежит: IPG MICROSYSTEMS LLC

Continuous mass flow gas replenishment may be implemented in a gas lasing device, such as a gas laser or amplifier, by using a restrictive orifice to bleed one or more gases into a reservoir and/or discharge chamber of the gas laser or amplifier at a predefined mass flow rate. The mass flow rate is a function of the pressure drop across the restrictive orifice resulting from the pressure differential between the depleted gas and the source gas. Thus, gases may be added as needed such that the gas total pressure, as well as the constituent partial pressures, is maintained within a desired range throughout the laser or amplifier fill lifetime. The continuous mass flow gas replenishment may thus make up the lost partial pressure of reactive gases in gas lasing devices in a manner that is less complicated and is less expensive than other continuous flow methodologies. 1. A continuous mass flow gas replenishment system for a gas discharge laser or amplifier , the gas discharge laser or amplifier including a gas discharge chamber for containing a gas or a mixture of gases and a plurality of electrodes located in a discharge region of the discharge chamber , the system comprising:at least one gas source;at least one accumulator gas chamber configured to receive the gas from the gas source; andat least one restrictive orifice between the at least one accumulator gas chamber and the gas discharge chamber and configured to provide a mass flow rate into the gas discharge chamber as a function of a pressure drop across the restrictive orifice.2. The system of claim 1 , wherein the restrictive orifice is located in a metering device.3. The system of claim 2 , wherein the metering device is selected from a group consisting of an orifice plate claim 2 , a Venturi tube claim 2 , and a flow nozzle.4. The system of claim 2 , wherein the metering device operates on the Bernoulli principle.5. The system of claim 1 , further comprising at least one check valve located between the at ...

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25-07-2013 дата публикации

GAS LASER OSCILLATOR AND GAS EXCHANGE METHOD FOR GAS LASER OSCILLATOR

Номер: US20130186476A1
Принадлежит:

The sealed gas laser oscillator that includes the airtight vessel, the laser gas supply source that supplies a laser gas to the airtight vessel, and the vacuum pump that performs evacuation until a pressure of an inside of the airtight vessel reaches a target reached pressure every predetermined interval between laser gas exchanges and is connected to the airtight vessel, and that performs laser oscillation in a state where the airtight vessel is filled with the laser gas. The gas laser oscillator includes a unit that determines the target reached pressure on the basis of the interval between laser gas exchanges, a leakage rate of an impurity gas from the outside to the airtight vessel after evacuation, and an allowable impurity gas pressure at which the gas laser oscillator is capable of being operated.

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25-07-2013 дата публикации

SHORT PULSED IR FIBER LASER AT WAVELENGTH > 2 um

Номер: US20130188660A1
Принадлежит:

A method of generating ultrashort pulses with wavelengths greater than 2 μm comprising a short pulse diode laser or fiber laser operating at a wavelength of 1 μm or greater with a pulse width of 10 ps or greater, one or more amplification stages to increase the peak power of the pulsed source, a nonlinear fiber stage whereby the dispersion of the nonlinear fiber is anomalous at the pulsed source wavelength such that the fiber breaks up the pulse into a series of sub-ps pulse train through modulation instability which may be seeded by spontaneous noise which are then wavelength shifted in one or more stages by soliton self frequency shift in anomalous dispersion fiber or Raman in normal dispersion fiber and amplified in one or more stages to generate a high peak power ultrashort pulse (<1 ps) source at a wavelength of 2.4 μm or greater. 1. A method for generating ultrashort infrared pulses , comprising:using a laser to generate one or more pulses;amplifying the pulse in one or more amplification stages;pumping the amplified pulse into one or more nonlinear fibers whereby the fiber breaks up the pulse into a pulse train that is 1 ps or less;wavelength shifting the pulse train one or more times; andamplifying the wavelength shifted pulse train to a wavelength of 2.4 μm or greater.2. The method of claim 1 , wherein the laser generates a pulse with a wavelength of 1 μm or greater.3. The method of claim 1 , wherein the laser generates a pulse with a pulse width of 10 ps or greater.4. The method of claim 1 , wherein the wavelength shifting is done by soliton self frequency shift in anomalous dispersion fiber or Raman in normal dispersion fiber.5. The method of claim 1 , wherein the laser is a diode laser or a fiber laser.6. The method of claim 1 , wherein amplification is achieved with fiber amplifiers claim 1 , semiconductor optical amplifiers claim 1 , bulk nonlinear crystal optical parametric amplifiers claim 1 , or any combination thereof.7. The method of claim 1 , ...

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01-08-2013 дата публикации

High Power Single Mode Ytterbium Fiber Laser System with Single Mode Neodymium Fiber Pump Source

Номер: US20130195126A1
Принадлежит: IPG Photonics Corp

A high power fiber laser system emitting a substantially diffraction limited beam with a Gaussian intensity profile includes a single mode (“SM”) neodymium fiber pump source outputting a SM pump light; a seed laser operative to emit a SM signal light at a wavelength greater than that of the pump light; a SM DWM receiving and multiplexing the SM pump and signal lights. The disclosed system further includes a booster fiber amplifier which is configured with a frustoconically-shaped ytterbium (“Yb”) doped core receiving the pump and signal lights and configured with a small diameter input end which supports only a SM and a large diameter output end which is capable of supporting the SM and high order modes (:HOM”). The booster further has a cladding surrounding and coextending with the core, the core being configured for having intensity profiles of respective SMs of pump and signal lights overlap one another so that an overlap integral substantially equals to one (1) along an entire length of the core. The SM of the light signal extracts substantially the entire energy from the pump mode leaving the HOMs without amplification necessary to affect a quality of the diffraction limited beam of the system in a MW peak power range and hundreds of watt average power range.

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08-08-2013 дата публикации

GAS FILLED HOLLOW FIBER LASER

Номер: US20130202006A1
Принадлежит:

Apparatus, systems, and methods using an optically pumped gas filled hollow fiber laser can be implemented in a variety of applications. In various embodiments, operation of an optically pumped gas filled hollow fiber laser is based on population inversion in the gas. Additional apparatus, systems, and methods are disclosed. 1. An apparatus comprising:a hollow optical fiber;a gas filling the hollow optical fiber, the gas selected such that the hollow optical fiber filled with the gas is operable as a laser based on population inversion generated in the gas.2. The apparatus of claim 1 , wherein the hollow optical fiber comprises a hollow core photonic crystal fiber.3. The apparatus of claim 1 , wherein the gas includes one of acetylene (CH) claim 1 , hydrogen cyanide claim 1 , (HCN) claim 1 , carbon monoxide (CO) claim 1 , carbon dioxide (CO) claim 1 , hydrogen bromide (HBr) claim 1 , nitrous oxide (NO) claim 1 , hydrogen sulfide (HS) claim 1 , carbonyl sulfide (OCS) claim 1 , I claim 1 , DF claim 1 , HP claim 1 , IBr claim 1 , HCl claim 1 , HI claim 1 , or an isotopic equivalent thereof.3. The apparatus of claim 1 , wherein the apparatus includes a pump laser arranged to direct a pump laser signal into the hollow optical fiber claim 1 , the pump laser signal having a wavelength corresponding to absorption by the gas to attain the population inversion or having a wavelength shifted by a nonlinear optical process to become resonant with the gas during propagation through the fiber.54. The apparatus of claim claim 1 , therein the wavelength of the pump laser signal differs from a wavelength of a laser output from the hollow optical fiber by about a factor of two claim 1 , when pumped by the pump laser.64. The apparatus of claim claim 1 , wherein the wavelength of the pump laser signal can be converted through nonlinear optical processes while radiation propagates through the fiber.74. The apparatus of claim claim 1 , wherein the pump laser includes an optical ...

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15-08-2013 дата публикации

Flow Cytometry For High Throughput Screening

Номер: US20130210672A1
Принадлежит: STC UNM

The present invention, provides a flow cytometry apparatus for the detection of particles from a plurality of samples comprising: means for moving a plurality of samples comprising particles from a plurality of respective source wells into a fluid flow stream; means for introducing a separation gas between each of the plurality of samples in the fluid flow stream; and means for selectively analyzing each of the plurality of samples for the particles. The present invention also provides a flow cytometry method employing such an apparatus.

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22-08-2013 дата публикации

Spatially Correlated Light Collection from Multiple Sample Streams Excited with a Line Focused Light Source

Номер: US20130214176A1
Принадлежит: STC UNM

An affordable flow cytometry system with a significantly increased analytical rate, volumetric sample delivery and usable particle size including a light beam that interrogates multiple flow streams so as to provide excitation across all of the streams, and an optical objective configured to collect light from the sample streams and image the light onto an array detector.

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22-08-2013 дата публикации

Laser apparatus and laser materials processing apparatus provided with same

Номер: US20130215914A1
Автор: Hirofumi Imai, Koji Hirano
Принадлежит: Nippon Steel and Sumitomo Metal Corp

A laser apparatus of the present invention has a first laser oscillator that emits a first laser beam; a passive fiber that is a double-clad fiber that transmits the first laser beam through a core; and a second laser oscillator that emits a second laser beam that is coupled into inner cladding of the passive fiber. Additionally, a laser materials processing apparatus of the present invention is provided with the laser apparatus; and an irradiation optical system having a collimating lens and a condenser lens.

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22-08-2013 дата публикации

LASER ARRANGEMENT AND SYSTEM, AND A MEDICAL LASER TREATMENT SYSTEM THEREOF

Номер: US20130215920A1
Автор: CHOMSKY Doron, Medini Dror
Принадлежит: DENTARAY, Ltd.

A method for providing a laser beam and a laser arrangement that includes an elongated tube; an elongated discharge region within the elongated tube including a discharge medium to be excited to induce laser radiation; two DC discharge electrodes disposed at opposite ends of the elongated discharge region; two RF electrodes disposed at opposite elongated sides of the elongated discharge region; and/or a laser resonator having two opposite mirrors disposed at opposite ends of the elongated tube, the laser resonator is unstable in at least one lateral axis. The method includes applying a DC discharge between the DC electrodes, and applying a RF discharge transverse to the DC discharge between the RF electrodes. The DC and RF discharges may be provided by the DC and/or RF voltage suppliers provided according to embodiments of the present invention. 1. A laser arrangement comprising:an elongated tube;an elongated discharge region within said elongated tube including a discharge medium to be excited to induce laser radiation;DC discharge electrodes disposed at opposite ends of the elongated discharge region;RF electrodes disposed at opposite elongated sides of the elongated discharge region; anda laser resonator having two opposite mirrors disposed at opposite ends of said elongated tube, the laser resonator is unstable in at least one lateral axis.2. A laser arrangement according to claim 1 , comprising a DC voltage supplier to apply pulsed DC electric discharge on said DC electrodes.3. A laser arrangement according to claim 2 , wherein said DC voltage supplier comprises a DC source claim 2 , a pulse shaper to shape into pulses a DC signal provided by the DC source claim 2 , a high voltage transformer to provide a high output voltage for exciting the discharge medium and an output smoother.4. A laser arrangement according to claim 1 , wherein said laser resonator is a hybrid stable and unstable resonator claim 1 , the hybrid resonator comprising:an output mirror ...

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22-08-2013 дата публикации

NON-HERMETIC, MULTI-EMITTER LASER PUMP PACKAGES AND METHODS FOR FORMING THE SAME

Номер: US20130215924A1
Принадлежит:

According to one embodiment described herein, a method for assembling a multi-emitter laser pump package, includes providing a base substrate comprising a laser riser block. A chip-on-hybrid laser assembly is bonded to the laser riser block with a solder preform. A scalar module is bonded to the base substrate with an adhesive such that an output of the chip-on-hybrid laser assembly is optically coupled into an input of the scalar module. A sidewall ring is adhesively bonded to the base substrate with a non-hermetic adhesive, the sidewall ring comprising a fiber interconnect fitting and at least one electrical connector. A first end of a fiber interconnect is optically coupled to an output of the scalar module and a second end of the fiber interconnect is positioned in the fiber interconnect fitting of the sidewall ring. 1. A method for assembling a multi-emitter laser pump package , the method comprising:providing a base substrate comprising a laser riser block;bonding a chip-on-hybrid laser assembly to the laser riser block with a solder preform;bonding a scalar module to the base substrate with an adhesive such that an output of the chip-on-hybrid laser assembly is optically coupled into an input of the scalar module;adhesively bonding a sidewall ring to the base substrate with a non-hermetic adhesive, the sidewall ring comprising a fiber interconnect fitting and at least one electrical connector; andoptically coupling a first end of a fiber interconnect to an output of the scalar module and positioning a second end of the fiber interconnect in the fiber interconnect fitting of the sidewall ring.2. The method of claim 1 , further comprising adhesively bonding a lid to the sidewall ring with a non-hermetic adhesive.3. The method of claim 1 , wherein the fiber interconnect is non-hermetically sealed to the fiber interconnect fitting.4. The method of claim 1 , wherein:the base substrate comprises a fiber interconnect riser block; andthe method further comprises ...

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22-08-2013 дата публикации

Method of generating enhanced intra-resonator laser light, enhancement resonator and laser device

Номер: US20130215925A1

A method of generating intra-resonator laser light ( 1 ) comprises the steps of coupling input laser light ( 2 ), e.g. laser pulse or continuous-wave light, into an enhancement resonator ( 20 ), which comprises at least two curved resonator mirrors ( 21, 22, 23, 24 ) and which is free of a laser light amplifying medium, said at least two curved resonator mirrors ( 21, 22, 23, 24 ) being consecutively arranged and spanning at least one resonator path with a predetermined resonator length (Lres), wherein said at least two curved resonator mirrors ( 21, 22, 23, 24 ) providing at least two pairs of consecutive curved resonator mirrors which are serially coupled along said at least one resonator path, and coherent addition of the input laser light ( 2 ) in the enhancement resonator so that the intra-resonator laser light ( 1 ) is formed, wherein said at least two pairs of consecutive curved resonator mirrors each have a detuned concentric configuration, which deviates from a concentric configuration with regard to at least one of a distance between the curved mirrors. and an angle of incidence on the curved mirror surfaces. Furthermore, an enhancement resonator ( 20 ), in particular being configured for generating intra-resonator laser light ( 1 ), a laser device ( 100 ) including the enhancement resonator device ( 20 ) and applications of the enhancement resonator device ( 20 ) are described.

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29-08-2013 дата публикации

Microbubble optical resonator

Номер: US20130219970A1
Автор: Mikhail Sumetsky
Принадлежит: OFS FITEL LLC

An optical microresonator is configured as an optical microbubble formed along a section of an optical microcapillary. The curvature of the outer surface of the microbubble creates an optical resonator with a geometry that encourages the circulating WGMs to remain confined in the central region of the bubble, creating a high Q optical resonator. The resonator may be tuned by modifying the physical properties of the microbubble, allowing the resonator to be used as an optical filter. The resonator may also be used as a sensor or laser by introducing the material to be sensed (or the active laser material) into the microcapillary along which the microbubble is formed.

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29-08-2013 дата публикации

EXCITATION LIGHT DISTRIBUTION DEVICE, EXCITATION LIGHT DISTRIBUTION METHOD, OPTICAL AMPLIFICATION SYSTEM AND NODE DEVICE

Номер: US20130222890A1
Автор: Sakauchi Masahiro
Принадлежит: NEC Corporation

For the purpose of reducing the cost and power consumption of an optical amplification system provided with an optical amplifier, an excitation light distribution device of the present invention comprises an excitation light source output unit which outputs excitation light, an optical branching unit with variable branching ratio which branches and outputs the excitation light, and a control unit which, on the basis of information on an optical signal to be amplified by the excitation light outputted by the optical branching unit, controls at least either the branching ratio of the optical branching unit or the optical output power of the excitation light source output unit. 1. An excitation light distribution device comprising:an excitation light source output unit that outputs excitation light;an optical branching unit with variable branching ratio that branches and outputs said excitation light; anda control unit that controls, on the basis of information on an optical signal to be amplified by the excitation light outputted by said optical branching unit, at least either the branching ratio of said optical branching unit or the optical output power of said excitation light source output unit.2. The excitation light distribution device according to claim 1 , whereinsaid control unit controls at least either the branching ratio of said optical branching unit or the optical output power of said excitation light source output unit, on the basis of information on the number of optical signals to be amplified by the excitation light outputted by said optical branching unit and on optical paths on which said optical signals are transmitted.3. The excitation light distribution device according to claim 1 , wherein:said optical branching unit comprises an excitation light monitoring unit that monitors the power of said excitation light outputted from said optical branching unit and that outputs an excitation light monitoring signal corresponding to the intensity of said ...

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29-08-2013 дата публикации

Method for manufacturing a coupling arrangement, coupling arrangement and amplifier

Номер: US20130222891A1
Принадлежит: LZH Laser Zentrum Hannover eV

A single-mode fiber with certain parameters into the core of another fiber with different parameters; in particular single-mode guided light of a shorter wavelength is coupled into the core of a fiber which is a single-mode fiber at a longer wavelength but acts as multimode fiber for the shorter wavelength. Fabrication involves use of a model to determine a length of a pre-taper.

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29-08-2013 дата публикации

SPHERICAL LIQUID-CRYSTAL LASER

Номер: US20130223467A1
Автор: Humar Matjaz, Musevic Igor
Принадлежит: INSTITUT JOZEF STEFAN

The patent refers to one or more droplets of chiral liquid crystals used as point source(s) of laser light. The source is shaped as a droplet of chiral liquid crystals () and an active medium preferably dispersed in the liquid crystals. The source is spherical and with a size of preferably between a few nanometres and 100 micrometres. A droplet consists of chiral liquid crystals () that have selective reflection in the range of the active medium's emission and can be cholesteric liquid crystals, a mixture of nematic liquid crystals and a chiral dopant or any other chiral liquid-crystal phase, preferably the blue phase, the ferroelectric phase, the antiferroelectric phase, any of the ferrielectric phases or another chiral phase of a soft substance, that need not be chiral by itself. 1. A liquid-crystal laser formed of a droplet of liquid crystals , said droplet containing an active laser medium that , when stimulated with external light , emits laser light , wherein a refractive index of said droplet is modulated in a radial direction of the droplet forming optically different concentric layers , which act as a reflector for the laser light.2. The laser according to claim 1 , wherein the droplet is spherical and has a diameter of between a few nanometres and 100 micrometres.3. The laser according to claim 1 , wherein the droplet consists of chiral liquid crystals claim 1 , that have a selective reflection in the region of the active medium's emission.4. The laser according to claim 3 , wherein the chiral liquid crystals are cholesteric liquid crystals claim 3 , a mixture of nematic liquid crystals and a chiral dopant or any other chiral liquid-crystal phase claim 3 , preferably the blue phase claim 3 , the ferroelectric phase claim 3 , the antiferroelectric smectic phase claim 3 , any ferrielectric smectic phases claim 3 , another chiral phase of a soft substance or another chiral liquid-crystal phase made of non-chiral molecules claim 3 , such as for example bow- ...

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29-08-2013 дата публикации

EXCIMER LASER DEVICE

Номер: US20130223468A1
Принадлежит:

An excimer laser device capable of suppressing deterioration of optical elements provided in a laser chamber even if output energy per pulse is increased more than the conventional level, in which a width of a laser beam applied to the optical elements provided in the laser chamber is enlarged so as to reduce the energy density of the laser beam within such a range that a laser output of no less than a desired level is obtained. 112-. (canceled)13. An excimer laser device comprising:an oscillation stage laser configured to output a laser beam; andan amplification stage laser configured to output an amplified laser beam,the amplification stage laser comprising:a laser chamber;a rear-side mirror arranged so that the laser beam enters the rear-side mirror perpendicularly;an output-side mirror arranged parallel to the rear-side mirror; anda pair of discharge electrodes arranged in the chamber, the pair of discharge electrodes being arranged so that a longitudinal direction of the discharge electrode has a predetermined angle with respect to a laser beam direction.14. The excimer laser device according to claim 13 , wherein the predetermined angle is more than 0 mrad and equal to or less than 3 mrad.15. The excimer laser device according to claim 13 , wherein the amplification stage laser further comprises a beam expander including a transparent optical component of a wedge shape. This application is a divisional of U.S. application Ser. No. 13/048,159, filed Mar. 15, 2011, which is a divisional U.S. application Ser. No. 11/882,938, filed Aug. 7, 2007, the entireties of which are incorporated herein by reference.1. Field of the InventionThe present invention relates to a gas laser device, and in particular to a high output excimer laser device for exposure.2. Description of the Related ArtA demand for improving the resolution of exposure devices for semiconductor substrates has arisen along with the recent advancement of refinement and integration of semiconductor ...

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29-08-2013 дата публикации

APPARATUS FOR FEMTOSECOND LASER OPTICALLY PUMPED BY LASER DIODE PUMPING MODULE

Номер: US20130223470A1

There is disclosed an apparatus for femtosecond laser optically pumped by a laser diode pumping module that is able to mechanically couple optical mounts for mounting optical mounts to each other by using a bar with a low thermal expansion coefficient and to form a light pumping module distant from a laser platform or a case, to provide a stable mode locking for an ultrashort laser and to enhance a power stability and a beam stability. 1. An apparatus for femtosecond laser optically pumped by a laser diode pumping module comprising:a laser diode for pumping light;a half-wave plate for adjusting a polarizing direction of a light generated from the laser diode;a collimating lens and a focusing lens for enhancing mode coupling with respect to the light of the laser diode and for focusing the light on the laser material; anddichroic mirrors arranged in both sides of the laser material, respectively, to reflect a laser beam generated via the laser material and to transmit a pumping light generated from the laser diode,wherein the half-wave plate, the collimating lens, the focusing lens and the dichroic mirrors are integrally connected with each other via mechanical coupling to form a light pumping module, in a state of being distant from a laser platform.2. The apparatus for femtosecond laser optically pumped by the laser diode pumping module according to claim 1 , further comprising:a mount for mounting each of the half-wave plate, the collimating lens, the focusing lens and the dichroic mirrors thereon;at least one module coupling bar for coupling the mounts to each other, with passing through the mounts; anda module coupler arranged on the laser platform to fixedly support the module coupling bar.3. The apparatus for femtosecond laser optically pumped by the laser diode pumping module according to claim 1 , wherein the laser material is directly installed on the laser platform by a laser material mount.4. The apparatus for femtosecond laser optically pumped by the ...

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