Optica · 2023 · 15 citations · 69 references
Natural SciencesMaterials EngineeringMaterials ScienceElectronic MaterialsHeat TransferOptical MaterialsDetector TechnologyInfrared DetectorsInfrared InstrumentationLongwave RadiationThermal SensorsEvanescent WavesInfrared SensingInfrared SensorsThermal DetectorsThermal Infrared DetectorsThermal Infrared MaterialsThermal Infrared SensorsThermal Sensing
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 3.8×10 9 cmHz/W, which is the highest reported for any room temperature device operating in the long-wave infrared ( λ ∼8−12µm). 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 1.54×10 22 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, SiN x , 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 =633nm), chosen for its long-term compatibility with array reads using a single integrated transceiver.
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Infrared detectors: status and trends
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