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    • 3. 发明申请
    • EXCITED STATE QUANTUM CASCADE PHOTON SOURCE
    • 激光光源
    • US20080273565A1
    • 2008-11-06
    • US11744508
    • 2007-05-04
    • Claire F. GmachlKale J. Franz
    • Claire F. GmachlKale J. Franz
    • H01S5/34H01L33/00
    • H01S5/3402B82Y20/00H01S5/024H01S5/3415
    • A quantum cascade source, such as a QC laser, is provided comprising a plurality of repeat units each including an active region and an injector region. The active region includes at least two quantum wells that, in response to an applied electrical bias, provide a first, second, and third electron energy level, each resulting from a respective quantum well excited state. The first and second energy levels are configured so that an electron transition from the first energy level to the second energy level emits a photon of a selected wavelength. The second and third energy levels are configured so that an electron transition from the second energy level to the third energy level comprises a nonradiative transition to empty the second energy level sufficiently quickly to promote a population inversion between the first and second energy levels.
    • 提供了量子级联源,例如QC激光器,其包括多个重复单元,每个重复单元包括有源区和注入区。 有源区包括至少两个量子阱,其响应于施加的电偏压而提供第一,第二和第三电子能级,每个由相应的量子阱激发态产生。 第一和第二能级配置成使得从第一能级到第二能级的电子跃迁发射所选波长的光子。 第二和第三能级配置成使得从第二能量级到第三能级的电子跃迁包括非辐射过渡以足够快地清空第二能级,以促进第一和第二能量级之间的总体反转。
    • 4. 发明授权
    • Optical amplifier for quantum cascade laser
    • 用于量子级联激光器的光放大器
    • US06836499B2
    • 2004-12-28
    • US10155562
    • 2002-05-24
    • Federico CapassoAlfred Yi ChoClaire F. GmachlDeborah Lee SivcoMariano Troccoli
    • Federico CapassoAlfred Yi ChoClaire F. GmachlDeborah Lee SivcoMariano Troccoli
    • H01S500
    • B82Y20/00H01S5/026H01S5/1064H01S5/12H01S5/3402H01S5/50
    • Techniques for amplifying light produced by a quantum cascade laser are described. An assembly according to the present invention includes an optical amplifier having an optical input and an optical output. The optical output has an area significantly greater than that of the optical output and the geometry of the amplifier is such that the amplifier widens from the optical input to the optical output. The optical amplifier is formed of a layered waveguide structure which achieves quantum confinement of electrons and photons within the active region. A distributed feedback laser is suitably coupled to the optical amplifier at the optical input of the amplifier. The widening of the amplifier makes available a large number of electrons, so that the amplifier is able to produce many photons resulting from stimulated transitions caused by introduction of light to the optical input of the amplifier, even if the great majority of the transitions occur nonradiatively.
    • 描述用于放大由量子级联激光器产生的光的技术。 根据本发明的组件包括具有光输入和光输出的光放大器。 光输出具有明显大于光输出的面积,并且放大器的几何形状使得放大器从光输入增宽到光输出。 光放大器由层状波导结构形成,其在有源区内实现电子和光子的量子限制。 分布式反馈激光器适当地耦合到放大器的光输入处的光放大器。 放大器的加宽使得可以获得大量的电子,使得放大器能够产生由于通过向放大器的光输入引入光引起的受激变换而产生的许多光子,即使绝大多数的跃迁是非辐射的 。
    • 5. 发明授权
    • Engineering the gain/loss profile of intersubband optical devices having heterogeneous cascades
    • 设计具有异质级联的子带间光学器件的增益/损耗曲线
    • US06728282B2
    • 2004-04-27
    • US09883542
    • 2001-06-18
    • Federico CapassoAlfred Yi ChoRafaelle ColombelliClaire F. GmachlHock Min NgDeborah Lee Sivco
    • Federico CapassoAlfred Yi ChoRafaelle ColombelliClaire F. GmachlHock Min NgDeborah Lee Sivco
    • H01S500
    • B82Y20/00H01S5/3402H01S5/3422H01S5/4087H01S2301/18
    • An optical device includes a stack of at least two different intersubband (ISB) optical sub-devices in which the gain/loss profiles of the individual ISB sub-devices are mutually adapted, or engineered, so as to generate a predetermined overall function for the combination. We define this combination device as being heterogeneous since not all of the individual ISB sub-devices are identical to one another. Illustratively, the parameters of each individual ISB sub-device that might be subject to this engineering process include: the peak energy of the ISB optical transitions (emission or absorption) associated with each RT region, the position of each sub-device in the stack; the oscillator strengths of these ISB transitions; the energy bandwidth of each transition; and the total length of the RT and I/R regions of each ISB sub-device. In one embodiment, our approach may be used to engineer a gain profile that has peaks at a multiplicity of different wavelengths, thus realizing a multi-wavelength ISB optical source in which the applied electric field self-proportions itself so that each individual ISB sub-device experiences the appropriate field strength for its particular design. Alternatively, the gain profile may be engineered to be relatively flat over a predetermined wavelength range. In another embodiment, our approach may be used to generate a function that compensates for a characteristic of another device. For example, our heterogeneous ISB device may be engineered to have a gain profile that compensates for the loss profile of another device. Alternatively, the gain/loss profile may be engineered to produce a nonlinear refractive index profile in our device that compensates for that of another device (e.g., an optical fiber).
    • 光学装置包括至少两个不同的子带间(ISB)光学子装置的叠层,其中各个ISB子装置的增益/损耗曲线相互适应或设计,以便产生预定的整体功能 组合。 我们将此组合设备定义为异构,因为并非所有的单个ISB子设备都是相同的。 示例性地,可能受该工程过程影响的各个ISB子设备的参数包括:与每个RT区域相关联的ISB光学跃迁(发射或吸收)的峰值能量,堆叠中每个子设备的位置 ; 这些ISB转换的振荡器强度; 每个过渡的能量带宽; 以及每个ISB子设备的RT和I / R区域的总长度。 在一个实施例中,我们的方法可以用于设计在多个不同波长处具有峰值的增益分布,从而实现多波长ISB光源,其中所施加的电场自身比例,使得每个单独的ISB子载波, 设备体验其特定设计的适当场强。 或者,增益分布可以被设计为在预定波长范围上相对平坦。 在另一个实施例中,我们的方法可以用于产生补偿另一设备的特性的功能。 例如,我们的异构ISB设备可以被设计为具有补偿另一设备的丢失简档的增益简档。 或者,增益/损耗曲线可以被设计为在我们的装置中产生非线性折射率分布,其补偿另一装置(例如,光纤)的折射率分布。
    • 6. 发明授权
    • Semiconductor laser for operation in librational modes
    • 半导体激光器用于演示模式
    • US06333944B1
    • 2001-12-25
    • US09591716
    • 2000-06-12
    • Federico CapassoAlfred Yi ChoClaire F. GmachlDeborah Lee SivcoEvgueni E. NarimanovAlfred Douglas Stone
    • Federico CapassoAlfred Yi ChoClaire F. GmachlDeborah Lee SivcoEvgueni E. NarimanovAlfred Douglas Stone
    • H01S3083
    • H01S3/083
    • A solid state laser comprises a cavity resonator in the form of a generally cylindrical body and, located within the resonator, an active region which generates lasing light when suitably pumped. The resonator has a relatively high effective refractive index (n>2 and typically n>3) is sufficiently deformed from circularity so as to support at least one librational mode (e.g., a V-shaped or a bow-tie mode, the latter being presently preferred for generating relatively high power, directional outputs). Specifically described is a Group III-V compound semiconductor, quantum cascade (QC), micro-cylinder laser in which the resonator has a flattened quadrupolar deformation from circularity. This laser exhibits both a highly directional output emission and a three-order of magnitude increase in optical output power compared to conventional semiconductor micro-cylinder QC lasers having circularly symmetric resonators.
    • 固体激光器包括呈大致圆柱形体形式的空腔谐振器,并且位于谐振器内部的有源区域,其在适当泵浦时产生激光。 谐振器具有相对较高的有效折射率(n> 2且通常n> 3)从圆形度充分变形,以便支持至少一种示范模式(例如,V形或蝴蝶结模式,后者为 目前优选用于产生相对高功率的方向输出)。 具体描述的是其中谐振器具有从圆形度的扁平四极变形的III-V族化合物半导体,量子级联(QC),微圆柱激光器。 与具有圆形对称谐振器的常规半导体微型气缸QC激光器相比,该激光器表现出高度方向性的输出发射和光输出功率三位数的增加。