4.4 Article

Millimeter-Wave Response of All Metal-Organic Deposited YBCO Transition Edge Bolometer

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IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/TASC.2020.3033413

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Bolometer; detector; millimeter wave; superconducting devices; terahertz (THz); YBa2Cu3O7-x(YBCO)

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This study investigates the response of a monolithic high Tc transition-edge bolometer to approximately 3 mm wave radiation. The results indicate that the electrical conductivity of the YBCO film affects the absorption performance of the detector. The design of the meander line pattern on the bolometer structure allows for maximum absorption and responsivity when aligned with the polarized radiation source.
We report on the response of a monolithic high T-c transition-edge bolometer to about 3 mmWave for the first time. The detector structure consisting of 400-nm YBa2Cu3O7-x (YBCO) film on buffered yttria stabilized zirconia substrate without any coupled antenna, shows bolometric type responsivity to the 3-mmWave radiation at its transition temperature. The YBCO thin film and Ce0.9La0.1O2 buffer layer are both fabricated by the metal-organic deposition method. The meander line pattern of the bolometer is designed for obtaining maximum absorption and responsivity possible when the polarized radiation of the source is aligned with the pattern. Meander lines are 50 micrometers wide and 1.5-mm long. We have measured amplitude and phase of the response versus modulation frequency of the detector to the linearly polarized 95-GHz source, and the detector was biased at five distinct temperatures at the transition corresponding to five different electrical conductivities of the YBCO film. When the meander lines of the device are parallel to the incident beam polarization, the YBCO pattern is speculated to act as a dissipative antenna resulting in higher absorption leading to high magnitude of the response as observed. The results from the measured phase of the response versus modulation frequency are also in agreement with the discussed absorbed mechanism. The absorption of the YBCO pattern is also measured to depend on the electrical conductivity of the YBCO film and our results show that there is an optimum electrical conductivity for havingmaximum absorption for this detector. Simulation results for this structure confirm the experiments showing that at electrical conductivity value of 1.33 x 10(5) S/m we have the maximum absorption for our device. These observations promise design of versatileTHz andmillimeter-wave detectorswith potential for applications in medical and security imaging.

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