Material response of metasurface integrated uncooled silicon germanium oxide SixGeyO1-x-y infrared microbolometers

This paper presents a study of metasurface integrated microbolometers. The semiconductor absorber is sandwiched between a metal Frequency-Selective Surface (FSS) and ground plane. When the semiconductor absorber is electrically isolated from the ground plane by a thin dielectric it can be used to measure the temperature of the pixel. The integration with the FSS removes the need for a Fabry-Perot cavity. The FSS allows control the attributes of radiation absorbed by the microbolometer on a pixel-by-pixel basis which provides the potential for spectral or polarimetric imaging. The FSS also affects he electrical performance of the semiconductor absorber and the thermal performance of the microbolometer. In addition, the complex permittivity of the semiconductor affects the optimal design of the FSS. The Si/Ge/O system is selected because it allows the properties of the absorber to be engineered (e.g., less oxygen gives lower absorptance and higher resistivity). This paper explores the absorber/FSS parameter space with an emphasis on the electrical and noise properties of the integrated system. Models are developed to explain results. Preliminary results show that the addition of the FSS improves TCR of the microbolometer by 10% while dramatically lowering its resistivity (factor of 5×). The resistivity reduction leads to a dramatic reduction of the noise power spectral density with the addition of FSS improving the measured 1/f noise by two orders of magnitude over an identical sample without the FSS. In addition, this paper will present the microbolometer figures of merits including voltage responsivity, detectivity, and thermal response time.

[1]  Chuang Qu,et al.  Design and analysis of frequency-selective surface enabled microbolometers , 2016, SPIE Defense + Security.

[2]  Qi Cheng,et al.  Silicon germanium oxide (SixGe1-xOy) infrared material for uncooled infrared detection , 2009, Defense + Commercial Sensing.

[3]  H. Sipola,et al.  An Ultra-Low Noise Superconducting Antenna-Coupled Microbolometer With a Room-Temperature Read-Out , 2006, IEEE Microwave and Wireless Components Letters.

[4]  Chuang Qu,et al.  Polycrystalline metasurface perfect absorbers fabricated using microsphere photolithography. , 2016, Optics letters.

[5]  C. Hewitt,et al.  Expanded applications for high performance VOx microbolometer FPAs , 2005, SPIE Defense + Commercial Sensing.

[6]  Tim Williams,et al.  Performance of a long-wave infrared hyperspectral imager using a Sagnac interferometer and an uncooled microbolometer array. , 2008, Applied optics.

[7]  Mahmoud Almasri,et al.  Noise Reduction of Amorphous SixGeyO1–x–y Thin Films for Uncooled Microbolometers by Si3N4 Passivation and Annealing in Vacuum , 2016, IEEE Sensors Journal.

[8]  Margaret Kohin,et al.  Commercialization of uncooled infrared technology , 2004, SPIE Optics + Photonics.

[9]  John F. Brady,et al.  Amorphous silicon based large format uncooled FPA microbolometer technology , 2008, SPIE Defense + Commercial Sensing.

[10]  Mahmoud Almasri,et al.  Self-supporting uncooled infrared microbolometers with low-thermal mass , 2001 .

[11]  A. Crastes,et al.  Uncooled microbolometer detector: Recent developments at Ulis , 2007 .

[12]  M. Almasri,et al.  Uncooled silicon germanium oxide (SixGeyO1-x-y) thin films for infrared detection , 2012, Defense + Commercial Sensing.

[13]  M. Almasri,et al.  Characterization of radio frequency sputtered SixGe1-xOy thin films for uncooled micro-bolometer , 2008, SPIE Defense + Commercial Sensing.

[14]  R. E. Hollingsworth,et al.  Amorphous silicon thin-films for uncooled infrared microbolometer sensors , 2010, Defense + Commercial Sensing.