Abstract:
An apparatus for providing pump light (50) of a first wavelength λ1 to a laser (32) that emits a second wavelength λ2 has first and second lasers (12a, b) of the wavelength λΐ to direct light along first and second axes (A,B) in a first direction. The first and second axes define a first plane PI. To form a composite light beam (50) of wavelength λ1, a filter apparatus (40) has a first filter (Fl) on a first surface (36) at an oblique angle to the first and second axes (A,B) and that transmits λΐ and reflects λ2. A second filter (F2) on a second surface (54) parallel to the first surface (36), reflects λΐ and transmits λ2. A third filter (F3) formed on the first surface (36) coplanar with the first filter (Fl) reflects λΐ and transmits λ2. The filter apparatus (40) re-aligns the first and second axes (A,B) along a second plane P2, orthogonal to P 1 and parallel to the first direction and prevents feedback from the pumped laser (32) to the first and second lasers (12a, b).
Abstract:
Methods of optimizing optical alignment in an optical package are provided. In one embodiment, the optical package includes a laser diode, a wavelength conversion device, coupling optics positioned along an optical path extending from the laser diode to the wavelength conversion device, and one or more adaptive actuators. The method involves adjusting the optical alignment of the wavelength conversion device in a non-adaptive degree of freedom by referring to a thermally-dependent output intensity profile of the laser diode and a thermally-dependent coupling efficiency profile of the optical package. The adjustment in the non-adaptive degree of freedom is quantified such that, over a given operating temperature range of the optical package, portions of the coupling efficiency profile characterized by relatively low coupling efficiency offset portions of the output intensity profile characterized by relatively high laser output intensity and portions of the coupling efficiency profile characterized by relatively high coupling efficiency offset portions of the output intensity profile characterized by relatively low laser output intensity. Additional embodiments are disclosed and claimed.
Abstract:
Methods of controlling semiconductor lasers (10) are provided where the semiconductor laser generates an output beam that is directed towards the input face of a wavelength conversion device (20). Particular aspects of the present invention relate to alignment and/or intentional misalignment of a beam spot (15) of an output beam on an input face of a wavelength conversion device (20). Additional embodiments are disclosed and claimed.
Abstract:
The present invention relates generally to semiconductor lasers and laser scanning systems and, more particularly, to schemes for controlling wavelength in semiconductor lasers. According to one embodiment of the present invention, a method of minimizing laser wavelength variations in a semiconductor laser is provided. According to the method, one or more of the laser drive currents is configured to comprise a drive portion and a wavelength recovery portion. The wavelength recovery portion of the drive current comprises a recovery amplitude IR that is distinct from the drive amplitude ID and a recovery duration t R that is less than the drive duration to. The recovery amplitude I R and duration t R are sufficient to recover carrier density distribution distorted by gain compression effects prior to recovery. Additional embodiments are disclosed and claimed.
Abstract translation:本发明一般涉及半导体激光器和激光扫描系统,更具体地,涉及用于控制半导体激光器中的波长的方案。 根据本发明的一个实施例,提供了一种使半导体激光器中的激光波长变化最小化的方法。 根据该方法,一个或多个激光驱动电流被配置为包括驱动部分和波长恢复部分。 驱动电流的波长恢复部分包括与驱动振幅ID不同的恢复幅度IR和小于驱动持续时间的恢复持续时间t R S。 恢复振幅I R和持续时间t R N足以恢复在恢复之前由增益压缩效应失真的载流子密度分布。 公开并要求保护附加实施例。
Abstract:
The present invention relates to methods for modulating a semiconductor laser and wavelength matching to a wavelength converter using monolithic micro-heaters integrated in the semiconductor laser. According to one embodiment of the present invention, a method of compensating for thermally induced patterning effects, e.g. wavelength drift, in a semiconductor laser is provided where the laser's heating element driving current I H is set to a relatively high magnitude when the laser's driving current I D is at a relatively low magnitude. The heating element driving current I H decreases from said relatively high magnitude to said relatively low magnitude at a time Δt prior to an increase in said laser driving current I D from said relatively low magnitude to said relatively high magnitude. The semiconductor laser may be a DBR laser diode comprising a wavelength selective region (12), a phase matching region (14), and a gain region (16), each region provided with a pair of heating element strips (62,64).
Abstract translation:本发明涉及使用集成在半导体激光器中的单块微型加热器来调制半导体激光器和波长转换器的波长匹配的方法。 根据本发明的一个实施例,一种补偿热诱导图案化效应的方法,例如, 提供了在半导体激光器中,当激光器的驱动电流I SUB相对于激光器的加热元件驱动电流I H H被设定为相对高的幅度时, 低幅度 在所述激光器驱动电流I SUB从所述激光器驱动电流I SUB增加之前的时间Δt,加热元件驱动电流I H H从所述相对高的幅度减小到所述相对低的幅度 相对较低的幅度到相对较高的幅度。 半导体激光器可以是包括波长选择区域(12),相位匹配区域(14)和增益区域(16)的DBR激光二极管,每个区域设置有一对加热元件条(62,64)。
Abstract:
A hyperspectral imaging system and method are described herein for providing a hyperspectral image of an area of a remote object (e.g., scene of interest). The hyperspectral imaging system includes at least one optic, a scannable slit mechanism, a spectrometer, a two-dimensional image sensor, and a controller. The scannable slit mechanism can be a micro-electromechanical system spatial light modulator (MEMS SLM), a diffractive Micro-Opto-Electro-Mechanical Systems (MOEMS) spatial light modulator (SLM), a digital light processing (DLP) system, a liquid crystal display, a rotating drum with at least one slit formed therein, or a rotating disk with at least one slit formed therein.
Abstract:
A method for operating a frequency converted light source includes sweeping a wavelength control signal of a semiconductor laser over an initial signal range and measuring an optical power of an output beam emitted from a wavelength conversion device coupled to the semiconductor laser. The wavelength control signal of the semiconductor laser may then be swept over at least one truncated signal range and the optical power of the resulting output beam is measured. The at least one truncated signal range may be centered on a point corresponding to a maximum power of the output beam of the sweep of the wavelength control signal over the preceding signal range. An operational signal range for the wavelength control signal is determined such that a midpoint of the operational signal range corresponds to the maximum optical power of the resulting output beam of the sweep over the preceding signal range. Closed-loop feedback control of the wavelength control signal in the operational signal range may then be initiated.
Abstract:
The present disclosure relates generally to semiconductor lasers and laser projection systems. According to one embodiment of the present disclosure, a method of operating a laser projection system is provided. According to the method, the laser projection system is utilized to display a sequence of pixelized image frames comprising an alternating sequence of relatively high intensity active projection periods Mod ON and relatively low intensity inactive projection periods Mod OFF . A complementary control signal transitions between an active state Q ON during the relatively high intensity active projection periods Mod ON and an inactive state Q OFF during the relatively low intensity inactive projection periods Mod OFF . The transition of the complementary control signal from the inactive state Q OFF to the active state Q ON is conditioned to anticipate initiation of relatively high intensity active projection periods ModON such that it is optimized upon initiation of the relatively high intensity active projection periods Mod ON . Additional embodiments are disclosed and claimed.
Abstract:
Methods of controlling semiconductor lasers are provided where the semiconductor laser generates a wavelength-modulated output beam λ MOD that is directed towards the input face of a wavelength conversion device. The intensity of a wavelength-converted output λ CONV of the device is monitored as the output beam of the laser is modulated and as the position of the modulated output beam λ MOD on the input face of the wavelength conversion device is varied. A maximum value of the monitored intensity is correlated with optimum coordinates representing the position of the modulated output beam λ MOD on the input face of the wavelength conversion device. The optical package is operated in the data projection mode by directing an intensity-modulated laser beam from the semiconductor laser to the wavelength conversion device using the optimum positional coordinates. Additional embodiments are disclosed and claimed. Laser controllers and projections systems are also provided.
Abstract:
Particular embodiments of the present invention relate generally to semiconductor lasers and laser scanning systems and, more particularly, to schemes for controlling semiconductor lasers. According to one embodiment of the present invention, a laser is configured for optical emission of encoded data. At least one parameter of the optical emission is a function of a drive current I GAIN injected into the gain section (16) of the semiconductor laser (10) and one or more additional drive currents I PHASE , I DBR. Mode selection in the semiconductor laser is altered by perturbing at least one of the additional drive currents I PHASE , I DBR witn a perturbation signal I PTRB to alter mode selection in the semiconductor laser (10) such that a plurality of different emission modes are selected in the semiconductor laser (10) over a target emission period. In this manner, patterned variations in the wavelength or intensity profile of the laser can be disrupted to disguise patterned flaws that would otherwise be readily noticeable in the output of the laser.