会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 3. 发明申请
    • Interband Cascade Lasers
    • 带间级联激光器
    • US20120128018A1
    • 2012-05-24
    • US13023656
    • 2011-02-09
    • Igor VurgaftmanJerry R. MeyerChadwick L. CanedyWilliam W. BewleyJames R. LindleChul-soo KimMijin Kim
    • Igor VurgaftmanJerry R. MeyerChadwick L. CanedyWilliam W. BewleyJames R. LindleChul-soo KimMijin Kim
    • H01S5/343H01S5/34H01L29/66B82Y20/00
    • B82Y20/00H01S5/3401H01S5/3422H01S5/34306
    • A gain medium and an interband cascade laser, having the gain medium are presented. The gain medium can have one or both of the following features: (1) the thicknesses of the one or more hole quantum wells in the hole injector region are reduced commensurate with the thickness of the active hole quantum well in the active quantum well region, so as to place the valence band maximum in the hole injector region at least about 100 meV lower than the valence band maximum in the active hole quantum well; and (2) the thickness of the last well of the electron injector region is between 85 and 110% of the thickness of the first active electron quantum well in the active gain region of the next stage of the medium. A laser incorporating a gain medium in accordance with the present invention can emit in the mid-IR range from about 2.5 to 8 μm at high temperatures with room-temperature continuous wave operation to wavelengths of at least 4.6 μm, threshold current density of about 400 A/cm2 and threshold power density of about 900 W/cm2.
    • 提出了具有增益介质的增益介质和带间级联激光器。 增益介质可以具有以下特征中的一个或两个:(1)空穴注入器区域中的一个或多个空穴量子阱的厚度与有源量子阱区域中的有源孔量子阱的厚度相当, 使得空穴注入器区域中的价带最大值比活性孔量子阱中的价带最大值低至少100meV; 和(2)电子注入器区域的最后一个阱的厚度在介质的下一阶段的有源增益区域中的第一有源电子量子阱的厚度的85至110%之间。 包含根据本发明的增益介质的激光器可以在高温下在室温连续波操作中在约2.5至8μm的中红外范围内发射至少为4.6μm的波长,约400的阈值电流密度 A / cm 2和阈值功率密度约900W / cm2。
    • 5. 发明授权
    • Surface-emitting photonic crystal distributed feedback laser systems and methods
    • 表面发射光子晶体分布反馈激光系统及方法
    • US06826223B1
    • 2004-11-30
    • US10446259
    • 2003-05-28
    • Jerry MeyerIgor Vurgaftman
    • Jerry MeyerIgor Vurgaftman
    • H01S308
    • H01S5/18H01S5/0425H01S5/105H01S5/1203H01S5/1206H01S5/1231H01S2301/18
    • A surface-emitting photonic crystal distributed feedback laser apparatus configured to emit an optical beam of light. The apparatus includes a laser cavity bounded by top and bottom optical claddings, an active region configured to produce optical gain upon receiving optical or electrical pumping, a periodic two-dimensional grating having an order higher than the fundamental and configured to induce modulation of a modal refractive index, and lateral pumped gain area contained within an area covered by the grating, the lateral pumped gain area configured to produce gain in one or more lasing modes having a modal index modulated by the grating. The lateral pumped gain area has a substantially circular shape of diameter D, and wherein the pumped gain area is enclosed by an unpumped region contained within the area covered by the grating but not receiving the optical or electrical pumping.
    • 配置为发射光束的表面发射光子晶体分布反馈激光装置。 该装置包括由顶部和底部光学包层限定的激光腔,被配置为在接收光学或电学泵浦时产生光学增益的有源区域,周期性二维光栅,其具有高于基极的阶数并被配置为诱导模态的调制 折射率和包含在由光栅覆盖的区域内的横向泵浦增益区域,横向泵浦增益区域被配置为产生具有由光栅调制的模态指数的一个或多个激光模式的增益。 横向泵浦增益区域具有直径D的大致圆形形状,并且其中泵浦增益区域被包含在由光栅所覆盖的区域内的未抽空区域包围,但不接收光学或电气泵送。
    • 10. 发明授权
    • Photonic-crystal distributed-feedback and distributed bragg-reflector lasers
    • US06996152B2
    • 2006-02-07
    • US10385165
    • 2003-03-07
    • Igor VurgaftmanJerry Meyer
    • Igor VurgaftmanJerry Meyer
    • H01S3/08
    • B82Y10/00B82Y20/00H01S5/0267H01S5/0425H01S5/10H01S5/105H01S5/1071H01S5/1085H01S5/12H01S5/20
    • A photonic-crystal distributed-feedback laser includes a laser cavity with a waveguide structure that has a cavity length Lc and is bounded by two mirrors; an active region for producing optical gain upon receiving optical pumping or an input voltage; at least one layer having a periodic two-dimensional grating with modulation of a modal refractive index, the grating being defined on a rectangular lattice with a first period along a first axis of the grating and a second period along a second perpendicular axis of the grating, and wherein the grating produces three diffraction processes having coupling coefficients κ1′, κ2′, κ3′; and a lateral gain area contained within a second area patterned with the grating that has substantially a shape of a gain stripe with a width W, with the gain stripe tilted at a first tilt angle relative to the two mirrors. The rectangular lattice of the grating is tilted at a second tilt angle substantially the same as the first tilt angle with respect to the gain stripe, and the ratio of the first and second grating periods is equal to the tangent of the first tilt angle, with the first tilt angle being between about 16° and about 23°. The hexagonal lattice does not need to be tilted with respect to the two mirrors. The laser's output emerges along the normal to a facet irrespective of the operating laser wavelength, facilitating coupling the laser light into a fiber or other optical system while avoiding beam steering. The two-dimensional nature of the feedback in the laser provides for varying the wavelength through angle tuning. Wavelength tuning by changing the propagation direction (propagation angle) permits a straightforward selection of different wavelengths from photonic crystal devices monolithically fabricated on a single wafer. The fabrication procedure is straightforward since no ridges need to be defined. The single-mode spectral purity of the rectangular-lattice PCDFB is robust, owing to the near absence of side modes, and exhibits good beam quality.