TY - JOUR
T1 - Bias-selectable three-color short-, extended-short-, and mid-wavelength infrared photodetectors based on type-II InAs/GaSb/AlSb superlattices
AU - Haddadi, Abbas
AU - Razeghi, Manijeh
N1 - Publisher Copyright:
© 2017 Optical Society of America.
PY - 2017/11/1
Y1 - 2017/11/1
N2 - A bias-selectable, high operating temperature, three-color short-, extended-short-, and mid-wavelength infrared photodetector based on InAs/GaSb/AlSb type-II superlattices on GaSb substrate has been demonstrated. The short-, extended-short-, and mid-wavelength channels’ 50% cutoff wavelengths were 2.3, 2.9, and 4.4 μm, respectively, at 150 K. The mid-wavelength channel exhibited a saturated quantum efficiency of 34% at 4 μm under 200 mV bias voltage in a front-side illumination configuration and without any antireflection coating. At 200 mV, the device exhibited a dark current density of 8.7 × 10−5 A∕cm2 providing a specific detectivity of ∼2 × 1011 cm · Hz1∕2∕W at 150 K. The short-wavelength channel achieved a saturated quantum efficiency of 20% at 1.8 μm. At −10 mV, the device’s dark current density was 5.5 × 10−8 A∕cm2. At zero bias, its specific detectivity was 1 × 1011 cm · Hz1∕2∕W at 150 K. The extended short-wavelength channel achieved a saturated quantum efficiency of 22% at 2.75 μm. Under −2 V bias voltage, the device exhibited a dark current density of 1.8 × 10−6 A∕cm2 providing a specific detectivity of 6.3 × 1011 cm · Hz1∕2∕W at 150 K.
AB - A bias-selectable, high operating temperature, three-color short-, extended-short-, and mid-wavelength infrared photodetector based on InAs/GaSb/AlSb type-II superlattices on GaSb substrate has been demonstrated. The short-, extended-short-, and mid-wavelength channels’ 50% cutoff wavelengths were 2.3, 2.9, and 4.4 μm, respectively, at 150 K. The mid-wavelength channel exhibited a saturated quantum efficiency of 34% at 4 μm under 200 mV bias voltage in a front-side illumination configuration and without any antireflection coating. At 200 mV, the device exhibited a dark current density of 8.7 × 10−5 A∕cm2 providing a specific detectivity of ∼2 × 1011 cm · Hz1∕2∕W at 150 K. The short-wavelength channel achieved a saturated quantum efficiency of 20% at 1.8 μm. At −10 mV, the device’s dark current density was 5.5 × 10−8 A∕cm2. At zero bias, its specific detectivity was 1 × 1011 cm · Hz1∕2∕W at 150 K. The extended short-wavelength channel achieved a saturated quantum efficiency of 22% at 2.75 μm. Under −2 V bias voltage, the device exhibited a dark current density of 1.8 × 10−6 A∕cm2 providing a specific detectivity of 6.3 × 1011 cm · Hz1∕2∕W at 150 K.
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U2 - 10.1364/OL.42.004275
DO - 10.1364/OL.42.004275
M3 - Article
C2 - 29088141
AN - SCOPUS:85032800532
SN - 0146-9592
VL - 42
SP - 4275
EP - 4278
JO - Optics Letters
JF - Optics Letters
IS - 21
ER -