• Journal of Infrared and Millimeter Waves
  • Vol. 41, Issue 1, 2021417 (2022)
Qian SHI1、2、3, Shu-Kui ZHANG2、3、*, Jian-Lu WANG2、3、4、5、**, and Jun-Hao CHU3、4
Author Affiliations
  • 1Shanghai Institute Optics and Fine Mechanics,Chinese Academy of Sciences,Shanghai 201800,China
  • 2Hangzhou Institute for Advanced Study,University of Chinese Academy of Sciences,Hangzhou 310024,China
  • 3State Key Laboratory of Infrared Physics,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200083,China
  • 4Institute of Optoelectronics,Shanghai Frontier Base of Intelligent Optoelectronics and Perception,Fudan University,Shanghai 200433,China
  • 5Frontier Institute of Chip and System,Fudan University,Shanghai 200433,China
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    DOI: 10.11972/j.issn.1001-9014.2022.01.010 Cite this Article
    Qian SHI, Shu-Kui ZHANG, Jian-Lu WANG, Jun-Hao CHU. Progress on nBn infrared detectors[J]. Journal of Infrared and Millimeter Waves, 2022, 41(1): 2021417 Copy Citation Text show less
    History of the development of infrared detectors
    Fig. 1. History of the development of infrared detectors
    (a)Bandgap diagram of nBn barrier detector,(b)spatial makeups of the various current components and barrier blocking in nBn detector,(c)bandgap diagram of the p-n photodiode,(d)the schematic Arrhenius plot of the dark current in a p-n photodiode and nBn device and comparision with Rule 07 & Law 19
    Fig. 2. (a)Bandgap diagram of nBn barrier detector,(b)spatial makeups of the various current components and barrier blocking in nBn detector,(c)bandgap diagram of the p-n photodiode,(d)the schematic Arrhenius plot of the dark current in a p-n photodiode and nBn device and comparision with Rule 07 & Law 19
    (a)Conduction(filled)and valence(open)band offsets for the 12 binaries,(b)valence band offset as a function of lattice constant [52]
    Fig. 3. (a)Conduction(filled)and valence(open)band offsets for the 12 binaries,(b)valence band offset as a function of lattice constant 52
    (a)Arrhenius plot of dark current at different reverse bias values for a 300×300 μm nBn detector,(b)photoresponse spectra at 150 K(the calculated spectral response(solid line)and the measured spectral response at a reverse bias of -0.6 V(dotted line)),(c)image captured by a 320×256 nBn FPA detector(BF ROIC)operating at 150 K and f/3,(d)the device structure of InAsSb/AlAsSb nBn MWIR detector,(e)the stimulated energy band diagram under reverse bias conditions of InAsSb/AlAsSb nBn MWIR detector,(f)the dark current density vs bias voltage as a function of the temperature of the InAsSb/AlAsSb nBn MWIR detector[54,58,60]
    Fig. 4. (a)Arrhenius plot of dark current at different reverse bias values for a 300×300 μm nBn detector,(b)photoresponse spectra at 150 K(the calculated spectral response(solid line)and the measured spectral response at a reverse bias of -0.6 V(dotted line)),(c)image captured by a 320×256 nBn FPA detector(BF ROIC)operating at 150 K and f/3,(d)the device structure of InAsSb/AlAsSb nBn MWIR detector,(e)the stimulated energy band diagram under reverse bias conditions of InAsSb/AlAsSb nBn MWIR detector,(f)the dark current density vs bias voltage as a function of the temperature of the InAsSb/AlAsSb nBn MWIR detector545860
    Design of the InSb nBn barrier detector,(a)design of InSb nBn structure with InAlSb barrier layer including Al grading from 15% to 35%,(b)calculated energy band diagram at T = 110 K and V = 0 V of InSb/InAlSb/InSb nBn structure with 50 nm-thick InAlSb graded composition barrier layer,(c)Arrhenius plot of the dark current density collected at -50 mV where thermionic emission regime is identified,(d)J-V curves performed at 77 K of InSb-based nBn detector(solid line)and InSb PIN diode(dashed line),(e)J-V characteristics of nBn structure for different operating temperatures,from 105 K to 175 K,(f)Arrhenius behavior of three different types of InSb-based photodetectors[64,65,67]
    Fig. 5. Design of the InSb nBn barrier detector,(a)design of InSb nBn structure with InAlSb barrier layer including Al grading from 15% to 35%,(b)calculated energy band diagram at T = 110 K and V = 0 V of InSb/InAlSb/InSb nBn structure with 50 nm-thick InAlSb graded composition barrier layer,(c)Arrhenius plot of the dark current density collected at -50 mV where thermionic emission regime is identified,(d)J-V curves performed at 77 K of InSb-based nBn detector(solid line)and InSb PIN diode(dashed line),(e)J-V characteristics of nBn structure for different operating temperatures,from 105 K to 175 K,(f)Arrhenius behavior of three different types of InSb-based photodetectors646567
    (a)Alignment between mini-bands in the active and barrier layers of a T2SLs XBp device,superimposed on the band gaps of InAs,GaSb,and AlSb,(b)the schematic diagram of the SWIR nBn photodetector with the inset showing the superlattice band alignment of the H-structure electron barrier[71,72]
    Fig. 6. (a)Alignment between mini-bands in the active and barrier layers of a T2SLs XBp device,superimposed on the band gaps of InAs,GaSb,and AlSb,(b)the schematic diagram of the SWIR nBn photodetector with the inset showing the superlattice band alignment of the H-structure electron barrier7172
    Design of the HgCdTe nBn barrier detector,(a)the schematic illustration of the structure of the HgCdTe nBn photodetector device,(b)cross-sectional device diagram and structural parameters,(c)measured dark and unfiltered blackbody illuminated I-V characteristics of planar MWIR HgCdTe nBn device at 77 K[30,79]
    Fig. 7. Design of the HgCdTe nBn barrier detector,(a)the schematic illustration of the structure of the HgCdTe nBn photodetector device,(b)cross-sectional device diagram and structural parameters,(c)measured dark and unfiltered blackbody illuminated I-V characteristics of planar MWIR HgCdTe nBn device at 77 K3079
    Design of the two-dimensional materials nBn barrier detector,(a)the schematic diagram of the WS2 nBn vdW unipolar barrier photodetector,(b)simulated band diagrams of the device under different source-drain bias(Vds)conditions(WS2,h-BN,and PdSe2 flakes act as the absorber,barrier,and contact layer,respectively),(c)output characteristic curves of the nBn vdW unipolar barrier device under 520 nm laser illumination with increasing powers[94]
    Fig. 8. Design of the two-dimensional materials nBn barrier detector,(a)the schematic diagram of the WS2 nBn vdW unipolar barrier photodetector,(b)simulated band diagrams of the device under different source-drain bias(Vds)conditions(WS2,h-BN,and PdSe2 flakes act as the absorber,barrier,and contact layer,respectively),(c)output characteristic curves of the nBn vdW unipolar barrier device under 520 nm laser illumination with increasing powers94
    OrganizationMaterialStructureSize

    Pixel size

    (μm)

    Spectral range

    (μm)

    Temperature

    (K)

    NETD

    (mK)

    Northwestern UniversityInAs/AlSb/GaSbnBn1280×1024122.22150-
    T2SLpMp320×256274.915011
    JPLInAs/InAsSbBIRD640×512245.415018.7
    InAs/InAsSbBIRD640×5122412.56216.3
    SCDInAsSbnBn640×512153.6~4.2150<25
    InAsSbnBn1280×1024153.4~4.2150<25
    InAsSbnBn1280×102410-15030
    InAs/GaSb T2SLpBp640×512159.58015
    Wuhan GuideT2SLnpn320×256304.8/9.58020/25
    T2SLp×Ma320×256309.5-25
    T2SLp×Mn640×512159.5-25
    SITP

    InAs/GaSb

    T2SL

    npn640×512304.5/5.8--

    InAs/GaAsSb

    T2SL

    pB×Bn320×25630118021
    DAT-CONInSbXBn640×51215--23
    InSbXBn1280×102410--25
    Table 1. Development status of nBn infrared detectors[87-93]
    Qian SHI, Shu-Kui ZHANG, Jian-Lu WANG, Jun-Hao CHU. Progress on nBn infrared detectors[J]. Journal of Infrared and Millimeter Waves, 2022, 41(1): 2021417
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