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 3.8×109cmHz/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 1.54×1022kg−1m−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.