Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

International Journal of Infrared and Millimeter Waves

The development of an 850 GHz waveguide receiver using tuned sis junctions on 1µm Si3N4 membranes

J. Kooi, M. S. Chan, M. Bin, B. Bumble, Henry George LeDuc, C. K. Walker, Tom G. Phillips

Published Feb 1, 1995• 11 citations
Publisher
DOI
10.1007/bf02096322

Related papers

An 850 GHz Waveguide Receiver Using a Tuned Nb SIS Tunnel Junction Fabricated on a 1μm Si 3 N 4 Membrane

J. Kooi, Mansun Chan, Paul Schaffer⧧ +4 more

Softwaretechnik-Trends•Mar 1, 1996•2 citations

Fabrication and Characterization of a 600 GHz Resonant Distributed SIS Junction for Fixed-tuned Waveguide Receiver

T. Matsunaga, Edward Tong, Takashi Noguchi +1 more

•Jun 1, 2001•1 citation

180–425 GHz low noise SIS waveguide receivers employing tuned Nb/AIO x /Nb tunnel junctions

J. Kooi, M. Chan, B. Bumble +3 more

International Journal of Infrared and Millimeter Waves•May 1, 1994•20 citations

180-425 GHz Low Noise SIS Waveguide Receivers Employing Tuned Nb/AlOx/Tunnel Junctions

J. Kooi, Mansun Chan, Bruce Bumble +3 more

•May 1, 1994•0 citations

230 and 492 GHz low noise sis waveguide receivers employing tuned Nb/AlOx/Nb tunnel junctions

J. Kooi, M. Chan, B. Bumble +3 more

International Journal of Infrared and Millimeter Waves•Dec 1, 1995•41 citations

A 850-GHz waveguide receiver employing a niobium SIS junction fabricated on a 1-μm Si/sub 3/N/sub 4/ membrane

J. Kooi, Jérôme Pety, B. Bumble +4 more

We report on a 850-GHz superconducting-insulator-superconducting (SIS) heterodyne receiver employing an RF-tuned niobium tunnel junction with a current density of 14 kA/cm^2, fabricated on a 1-µm Si_3N_4 supporting membrane. Since the mixer is designed to be operated well above the superconducting gap frequency of niobium (2Δ/h ≈ 690 GHz), special care has been taken to minimize niobium transmission-line losses. Both Fourier transform spectrometer (FTS) measurements of the direct detection performance and calculations of the IF output noise with the mixer operating in heterodyne mode, indicate an absorption loss in the niobium film of about 6.8 dB at 822 GHz. These results are in reasonably good agreement with the loss predicted by the Mattis-Bardeen theory in the extreme anomalous limit. From 800 to 830 GHz, we report uncorrected receiver noise temperatures of 518 or 514 K when we use Callen and Welton's law to calculate the input load temperatures. Over the same frequency range, the mixer has a 4-dB conversion loss and 265 K ± 10 K noise temperature. At 890 GHz, the sensitivity of the receiver has degraded to 900 K, which is primarily the result of increased niobium film loss in the RF matching network. When the mixer was cooled from 4.2 to 1.9 K, the receiver noise temperature improved about 20% 409-K double sideband (DSB). Approximately half of the receiver noise temperature improvement can be attributed to a lower mixer conversion loss, while the remainder is due to a reduction in the niobium film absorption loss. At 982 GHz, we measured a receiver noise temperature of 1916 K.

IEEE Transactions on Microwave Theory and Techniques•Jan 1, 1998•21 citations
We report on a 850-GHz superconducting-insulator-superconducting (SIS) heterodyne receiver employing an RF-tuned niobium tunnel junction with a current density of 14 kA/cm^2, fabricated on a 1-µm Si_3N_4 supporting membrane. Since the mixer is designed to be operated well above the superconducting gap frequency of niobium (2Δ/h ≈ 690 GHz), special care has been taken to minimize niobium transmission-line losses. Both Fourier transform spectrometer (FTS) measurements of the direct detection performance and calculations of the IF output noise with the mixer operating in heterodyne mode, indicate an absorption loss in the niobium film of about 6.8 dB at 822 GHz. These results are in reasonably good agreement with the loss predicted by the Mattis-Bardeen theory in the extreme anomalous limit. From 800 to 830 GHz, we report uncorrected receiver noise temperatures of 518 or 514 K when we use Callen and Welton's law to calculate the input load temperatures. Over the same frequency range, the mixer has a 4-dB conversion loss and 265 K ± 10 K noise temperature. At 890 GHz, the sensitivity of the receiver has degraded to 900 K, which is primarily the result of increased niobium film loss in the RF matching network. When the mixer was cooled from 4.2 to 1.9 K, the receiver noise temperature improved about 20% 409-K double sideband (DSB). Approximately half of the receiver noise temperature improvement can be attributed to a lower mixer conversion loss, while the remainder is due to a reduction in the niobium film absorption loss. At 982 GHz, we measured a receiver noise temperature of 1916 K.