TY - JOUR
T1 - Thermodynamically limited uncooled infrared detector using an ultra-low mass perforated subwavelength absorber
AU - Das, Avijit
AU - Mah, Merlin L.
AU - Hunt, John
AU - Talghader, Joseph J.
N1 - Publisher Copyright:
© 2023 OSA - The Optical Society. All rights reserved.
PY - 2023/8/20
Y1 - 2023/8/20
N2 - An uncooled detector has reached the thermodynamic temperature fluctuation limit, such that 98% of its total noise consisted of phonon and photon fluctuations of the detector body. The device has performed with a detectivity of 3.8 × 109 cm√Hz/W, which is the highest reported for any room temperature device operating in the long-wave infrared (λ ∼ 8−12 µm). The device has shown a noise-equivalent temperature difference of 4.5 mK and a time constant of 7.4 ms. The detector contains a subwavelength perforated absorber with an absorption-per-unit-thermal mass-per-area of 1.54 × 1022 kg−1 m−2, which is approximately 1.6–32.1 times greater than the state-of-the-art absorbers reported for any infrared application. The perforated absorber membrane is mostly open space, and the solid portion consists of Ti, SiNx, and Ni layers with an overall fill factor of ∼28%, where subwavelength interference, cavity coupling, and evanescent field absorption among units induce the high absorption-per-unit-thermal mass-per-area. Readout of the detector occurs via infrared-absorption-induced deformation using a Mach–Zehnder interferometry technique (at λ = 633 nm), chosen for its long-term compatibility with array reads using a single integrated transceiver.
AB - An uncooled detector has reached the thermodynamic temperature fluctuation limit, such that 98% of its total noise consisted of phonon and photon fluctuations of the detector body. The device has performed with a detectivity of 3.8 × 109 cm√Hz/W, which is the highest reported for any room temperature device operating in the long-wave infrared (λ ∼ 8−12 µm). The device has shown a noise-equivalent temperature difference of 4.5 mK and a time constant of 7.4 ms. The detector contains a subwavelength perforated absorber with an absorption-per-unit-thermal mass-per-area of 1.54 × 1022 kg−1 m−2, which is approximately 1.6–32.1 times greater than the state-of-the-art absorbers reported for any infrared application. The perforated absorber membrane is mostly open space, and the solid portion consists of Ti, SiNx, and Ni layers with an overall fill factor of ∼28%, where subwavelength interference, cavity coupling, and evanescent field absorption among units induce the high absorption-per-unit-thermal mass-per-area. Readout of the detector occurs via infrared-absorption-induced deformation using a Mach–Zehnder interferometry technique (at λ = 633 nm), chosen for its long-term compatibility with array reads using a single integrated transceiver.
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U2 - 10.1364/OPTICA.489761
DO - 10.1364/OPTICA.489761
M3 - Article
AN - SCOPUS:85166736948
SN - 2334-2536
VL - 10
SP - 1018
EP - 1028
JO - Optica
JF - Optica
IS - 8
ER -