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Infrared Wavelength Converter for Imaging Applications Based On Quantum Well Devices

机译:基于量子阱器件的成像应用红外波长转换器

摘要

A mid-infrared (MIR) and/or far-infrared (FIR) to near-infrared (NIR) converter (10) for imaging applications is disclosed. The converter (10) makes use of the properties of Optical Readout Quantum Well Infrared Photodetectors (ORQWIP) (20), an NIR source (16), and a conventional near infrared detector device (24). In combination, an MIR or FIR light source (12) to be imaged is focused by lenses or mirrors (17) into a beam combiner (18) along with an NIR probe wave generated by the NIR source (16). The lower conduction level electrons (50a-50g) of the OR-QWIP (20) absorb MIR/FIR photons (60) and are excited to an upper conduction level (48) or free electron band (166) of the OR-QWIP (20) corresponding to the MIR/FIR wavelength (60), while valence band electrons (54a-54g) of the ORQWIP (20) absorb NIR photons (52) and are excited to the freed-up lower conduction level (46) corresponding to the NIR wavelength (52). The resulting change in transmittance of NIR radiation due to absorption is recorded by conventional near infrared detection equipment such as a standard digital camera (24). If multiple layers (202a-202d) of AlGaAs are alternated with multiple layers (200a-200c) of GaAs of the same thickness and composition, then identical quantum wells (203, 223) will result, all of which absorb a single MIR/FIR wavelength and a single NIR wavelength. If multiple layers (246a-246d) of AIGaAs are alternated with multiple layers (244a-244c) of GaAs of different thicknesses and/or composition, then quantum wells (249, 259) having different energy level differences will result, the multiple quantum wells (249, 259) absorbing multiple MIR/FIR wavelengths (256a-256c, 264a-264c) and multiple NIR wavelengths (258a-258c, 270a, 270c).
机译:公开了用于成像应用的中红外(MIR)和/或远红外(FIR)至近红外(NIR)转换器( 10 )。转换器( 10 )利用了光学读出量子阱红外光电探测器(ORQWIP)( 20 ),近红外光源( 16 )和常规的近红外检测器设备( 24 )。组合起来,将要成像的MIR或FIR光源( 12 )通过透镜或反射镜( 17 )聚焦到光束组合器( 18 >)以及由NIR源( 16 )生成的NIR探测波。 OR-QWIP的较低传导水平电子( 50 a - 50 g )( 20 )吸收MIR / FIR光子( 60 )并被激发到较高的传导水平( 48 )或自由电子带( 166 >)对应于MIR / FIR波长( 60 )的OR-QWIP( 20 ),而价带电子( 54 a - 54 g )的ORQWIP( 20 )吸收近红外光子( 52 )并被激发到与NIR波长( 52 )相对应的释放的较低传导水平( 46 )。由于吸收而导致的NIR辐射的透射率变化由传统的近红外检测设备(例如标准数码相机( 24 ))记录下来。如果AlGaAs的多层( 202 a - 202 d )与多层( 200 a - 200 c )具有相同厚度和组成的GaAs,然后具有相同的量子阱( 203、223 ),它们全部吸收单个MIR / FIR波长和单个NIR波长。如果AIGaAs的多层( 246 a - 246 d )与多层( 244 a - 244 c )具有不同厚度和/或组成的GaAs,然后是量子阱( 249、259) )具有不同的能级差,多个量子阱( 249、259 )吸收多个MIR / FIR波长( 256 a - 256 c ,264 a - 264 c < / I>)和多个NIR波长( 258 a - 258 c ,270 a ,270 c )。

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