Abstract

The sensitive detection of infrared (IR) radiation is a essential task in today’s modern world. The sensitivity of the state-of-the-art uncooled thermal infrared detectors is still several orders of magnitude above the fundamental photon noise limit. Thermal detectors based on temperature sensitive micro- and nanomechanical resonators are a promising approach to obtain improved thermal IR detectors. Here, we present an uncooled infrared detector based on a 1 mm×1 mm large nanoelectromechanical drum resonator made of 50 nm thick low-stress silicon nitride (SiN). The detector features a titanium nitride absorber with an absorptivity of ∼30% over the entire mid-IR range. The detector drum is driven at its resonance frequency by means of a phase-locked loop. Absorbed IR radiation results in an observable detuning of the drum’s oscillation frequency. We measured an Allan deviation of &sigma;<sub>A</sub> = 5.5 &times; 10<sup>−7</sup> at room temperature at a noise bandwidth of 25 Hz. With a responsivity of R = 343 W<sup>−1</sup> this results in a sensitivity defined as noise equivalent power (NEP) of NEP = 320 pW/rtHz for an IR beam at a wavelength of 9.5 µm. For this measurement, the IR beam focus spot diameter was equal to the drum size. The drum’s responsivity improves by a factor of ten for a focal spot size smaller than ∼ 100 &mu;m. For smaller spots the responsivity remains constant. Based on this analysis we predict a sensitivity of ∼ 30 pW/rtHz for an IR spot size smaller than 100 &mu;m. The detector can be improved further by e.g. optimizing the tensile pre-stress to a lower value or by improving the absorptivity.

Highlights

  • The sensitive detection of photons in the infrared regime of the electromagnetic spectrum is an essential task

  • The detector performance can be significantly improved by cryogenic cooling, as e.g. for liquid helium cooled bolometers

  • We have demonstrated the application of silicon nitride (SiN) drum resonators as uncooled nanoelectromechanical IR detector

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Summary

Introduction

The sensitive detection of photons in the infrared regime of the electromagnetic spectrum is an essential task Because of their low power, infrared (IR) photons can not be directly detected with a photon detector. As thermal detectors transduce the absorbed photons into heat, the power of absorbed infrared radiation is measured by the increase in temperature. Some of the common thermometer techniques are photoacoustic (Golay cell), thermoresistive (bolometer), pyroelectric, or thermoelectric (thermocouple). To this day, the sensitivity of state-of-the-art uncooled thermal infrared detectors is still several orders of magnitude above the fundamental photon noise limit.[1] The detector performance can be significantly improved by cryogenic cooling, as e.g. for liquid helium cooled bolometers. Due to their lower price, pyroelectric detectors are widely used and reach typical sensitivities of the order of 1 nW/rtHz

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