TY - GEN
T1 - Uncooled nano-thermoelectric bolometers for infrared imaging and sensing
AU - Varpula, Aapo
AU - Murros, Anton
AU - Sovanto, Kuura
AU - Rantala, Arto
AU - Martins, David Gomes
AU - Tappura, Kirsi
AU - Tiira, Jonna
AU - Prunnila, Mika
N1 - Funding Information:
This work has been financially supported by Business Finland co-innovation project RaPtor (No. 6030/31/2018), European Union Future and Emerging Technologies (FET) Open under Horizon 2020 program (Grant Agreement No. 766853, project EFINED), and the Academy of Finland (Grant No. 342586). The work of Jonna Tiira was supported by Academy of Finland (Grant No. 324838). We acknowledge gratefully the technical assistance of Teija Häkkinen in device fabrication.
Publisher Copyright:
© 2023 SPIE.
PY - 2023/3/14
Y1 - 2023/3/14
N2 - The state-of-the-art quantum infrared photodetectors have high performance, but obtaining high sensitivity in mid- and long-wavelength infrared (MWIR and LWIR) requires cooling and exotic materials. Whereas thermal detectors offer lower cost without the need for cooling but are typically slower and less sensitive than cooled quantum infrared detectors. Nano-thermoelectrics and nanomembranes offer opportunities for enhancing the performance of uncooled MWIR and LWIR imaging and sensing. Similar to thermoelectric detectors, the infrared sensitive signal in those is generated by the thermoelectric effect, providing advantages over resistive bolometers, i.e. less noise sources and zero power consumption in the detector itself. We have recently demonstrated that nano-thermoelectrics provides a route towards high-sensitivity and cost-effective LWIR detection. When the thickness of the thermoelectric polysilicon membrane is reduced, increased phonon scattering leads to reduced thermal conductivity. This gives rise to the high thermoelectric figures of merit determining the detector sensitivity. The speed stems from the low-thermal-mass device design with an integrated metal nanomembrane absorber and the lack of separate support structures. We report integrated circuit concept for the readout of these detectors, and study how the absorber grid geometry determines the device performance. The fabricated devices have thermal time constants, responsivities and specific detectivities D* in the ranges of 190 – 208 µs, 334 – 494 V/W, and (7.9 – 8.7)·107 cmHz1/2/W, respectively. The differences in the device performance originate from the differences in the thermal mass, total resistance, and impedance matching of the absorber grid. By optimization, we expect that D* = 8.3·108 cmHz1/2/W can be reached.
AB - The state-of-the-art quantum infrared photodetectors have high performance, but obtaining high sensitivity in mid- and long-wavelength infrared (MWIR and LWIR) requires cooling and exotic materials. Whereas thermal detectors offer lower cost without the need for cooling but are typically slower and less sensitive than cooled quantum infrared detectors. Nano-thermoelectrics and nanomembranes offer opportunities for enhancing the performance of uncooled MWIR and LWIR imaging and sensing. Similar to thermoelectric detectors, the infrared sensitive signal in those is generated by the thermoelectric effect, providing advantages over resistive bolometers, i.e. less noise sources and zero power consumption in the detector itself. We have recently demonstrated that nano-thermoelectrics provides a route towards high-sensitivity and cost-effective LWIR detection. When the thickness of the thermoelectric polysilicon membrane is reduced, increased phonon scattering leads to reduced thermal conductivity. This gives rise to the high thermoelectric figures of merit determining the detector sensitivity. The speed stems from the low-thermal-mass device design with an integrated metal nanomembrane absorber and the lack of separate support structures. We report integrated circuit concept for the readout of these detectors, and study how the absorber grid geometry determines the device performance. The fabricated devices have thermal time constants, responsivities and specific detectivities D* in the ranges of 190 – 208 µs, 334 – 494 V/W, and (7.9 – 8.7)·107 cmHz1/2/W, respectively. The differences in the device performance originate from the differences in the thermal mass, total resistance, and impedance matching of the absorber grid. By optimization, we expect that D* = 8.3·108 cmHz1/2/W can be reached.
KW - Infrared detector
KW - long-wavelength infrared
KW - mid-wavelength infrared
KW - nano-thermoelectrics
KW - nanomembrane
KW - silicon
KW - thermoelectric bolometer
UR - http://www.scopus.com/inward/record.url?scp=85159779955&partnerID=8YFLogxK
U2 - 10.1117/12.2646314
DO - 10.1117/12.2646314
M3 - Conference article in proceedings
AN - SCOPUS:85159779955
T3 - Proceedings of SPIE - The International Society for Optical Engineering
BT - Optical Components and Materials XX
A2 - Jiang, Shibin
A2 - Digonnet, Michel J.
PB - International Society for Optics and Photonics SPIE
T2 - Optical Components and Materials XX, SPIE OPTO
Y2 - 30 January 2023 through 31 January 2023
ER -