4.5 Article Proceedings Paper

Terahertz Transition-Edge Sensor With Kinetic-Inductance Amplifier at 4.2 K

Journal

Publisher

IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/TTHZ.2018.2872413

Keywords

High-Q resonator; nonlinear kinetic inductance; superconducting nanowire; terahertz arrays; transition-edge sensor

Funding

  1. German Federal Ministry of Education and Research [05K16VKA]

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Different terrestrial terahertz applications would benefi from large-format arrays, operating in compact and inexpensive cryocoolers at liquid helium temperature with sensitivity, limited only by the 300-K background radiation. A voltage-biased transition-edge sensor (TES) as a THz detector can have sufficien sensitivity and has a number of advantages important for real applications: linearity of response, high dynamic range, and simple calibration. However, it requires a low-noise current readout. Usually, a current amplifie based on superconducting quantum-interference device (SQUID) is used for readout, but the scalability of this approach is limited due to the complexity of the operation and fabrication. Recently, it has been shown that instead of SQUID it is possible to use a current sensor, which is based on the nonlinearity of the kinetic inductance of a current-carrying superconducting stripe. Embedding the stripe into a microwave high-Q superconducting resonator allows for reaching sufficien current sensitivity. More important, it is possible with the resonator approach to scale up to large arrays using frequency-division multiplexing in GHz range. Here, we demonstrate the operation of a voltage-biased TES with a microwave kinetic-inductance current amplifie at 4.2 K. We measured the expected intrinsic noise-equivalent power similar to 5 x 10(-14) W/Hz(1/2) and confirme that a sufficien sensitivity of the readout can be reached in conjunction with a real TES operation. The construction of an array with the improved sensitivity similar to 10(-15) W/Hz(1/2) at 4.2 K could be realized using a combination of the new current amplifie and already existing TES detectors with improved thermal isolation.

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