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Physica C Superconductivity

Observation of 45GHz current waveforms using HTS sampler

Michitaka Maruyama, Hideo Suzuki, Tsunehiro Hato, H. Wakana, Ken‐ichi Nakayama, Yoshihiro Ishimaru, Osami Horibe, Seiji Adachi, Ai Kamitani, Kenji Suzuki, Yasuo Oshikubo, Y. Tarutani, K. Tanabe

Published Jul 20, 2005• 13 citations
Publisher
DOI
10.1016/j.physc.2005.02.128

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We are developing a system using a high-T/sub c/ superconductor (HTS) sampler for measuring a 40-Gbps digital signal waveform, which will be used in next generation ultra-high-speed communications. To measure a 40-Gbps digital signal, the sampler bandwidth needs to be more than 120 GHz. The HTS sampler has the potential to achieve this bandwidth. As a first step in developing this system, we have developed a prototype whose target bandwidth is 40 GHz. In the prototype system, the sampler chip is cooled down to 35 K by a single-stage Stirling cryocooler, and the digital signal is transmitted to the sampler chip via a 40-GHz bandwidth assembly line. This system is the first to integrate an HTS device, a cryocooler, and a high-frequency assemble line. A 5.9-Gbps digital waveform was reconstituted by the prototype system with the correct period.
A high-resolution Josephson sampler using a single fluxoid is fabricated. The sampling pulse generator comprised a two-junction interferometer (DC–SQUID) with a damping resistance resistively coupled to a single junction as the sampling gate to reduce a turn-on delay. An ultra-fast sampling pulse was generated at a vortex-to-vortex transition in this sampler. The fabricated sampler had less than a 5ps time resolution and about a 5 µA current sensitivity. The dynamic waveform associated with two kinds of transitions was observed by the use of this sampler: a vortex-to-vortex transition and a vortex-to-voltage transition. The results show that the pulse corresponding to a single fluxoid has a nearly constant pulse height that is independent of the bias current and that setting the bias current near the critical point results in the long rise time of a DC–SQUID.