Ultimate performance of a superconducting quantum detector

被引:41
作者
Semenov, A
Engel, A
Il'in, K
Gol'tsman, G
Siegel, M
Hübers, HW
机构
[1] DLR, Inst Space Sensor Technol & Planetary Explorat, D-12489 Berlin, Germany
[2] Forschungszentrum Julich, Inst Thin Films & Interfaces, D-52425 Julich, Germany
[3] Moscow State Pedag Univ, Dept Phys, Moscow 119891, Russia
关键词
D O I
10.1051/epjap:2003009
中图分类号
O59 [应用物理学];
学科分类号
摘要
We analyze the ultimate performance of a superconducting quantum detector in order to meet requirements for applications in near-infrared astronomy and X-ray spectroscopy. The detector exploits a combined detection mechanism, in which avalanche quasiparticle multiplication and the supercurrent jointly produce a voltage response to a single absorbed photon via successive formation of a photon-induced and a current-induced normal hotspot in a narrow superconducting strip. The response time of the detector should increase with the photon energy providing energy resolution. Depending on the superconducting material and operation conditions, the cut-off wavelength for the single-photon detection regime varies from infrared waves to visible light. We simulated the performance of the background-limited infrared direct detector and X-ray photon counter utilizing the above mechanism. Low dark count rate and intrinsic low-frequency cut-off allow for realizing a background limited noise equivalent power of 10(-20) WHz(-1/2) for a far-infrared direct detector exposed to 4-K background radiation. At low temperatures, the intrinsic response time of the counter is rather determined by diffusion of nonequilibrium electrons than by the rate of energy transfer to phonons. Therefore, thermal fluctuations do not hamper energy resolution of the X-ray photon counter that should be better than 10(-3) for 6-keV photons. Comparison of new data obtained with a Nb based detector and previously reported results on NbN quantum detectors support our estimates of ultimate detector performance.
引用
收藏
页码:171 / 178
页数:8
相关论文
共 24 条
[1]  
Altshuler B. A., 1985, ELECT ELECT INTERACT
[2]   Normal-metal hot-electron microbolometer with on-chip protection by tunnel junctions [J].
Chouvaev, D ;
Kuzmin, L ;
Tarasov, M .
SUPERCONDUCTOR SCIENCE & TECHNOLOGY, 1999, 12 (11) :985-988
[3]  
FRIEDRICH S, 1997, APPL PHYS LETT, V71, P39901
[4]   Picosecond superconducting single-photon optical detector [J].
Gol'tsman, GN ;
Okunev, O ;
Chulkova, G ;
Lipatov, A ;
Semenov, A ;
Smirnov, K ;
Voronov, B ;
Dzardanov, A ;
Williams, C ;
Sobolewski, R .
APPLIED PHYSICS LETTERS, 2001, 79 (06) :705-707
[5]  
GOLTSMAN G, 2001, 12 INT S SPAC TER TE
[6]  
HEIM GB, 1996, MIPS REPORT
[7]  
HETTL P, 1998, EDXRF 98 BOL IT
[8]   A Mo-Cu superconducting transition-edge microcalorimeter with 4.5 eV energy resolution at 6 keV [J].
Irwin, KD ;
Hilton, GC ;
Martinis, JM ;
Deiker, S ;
Bergren, N ;
Nam, SW ;
Rudman, DA ;
Wollman, DA .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 2000, 444 (1-2) :184-187
[9]   AN APPLICATION OF ELECTROTHERMAL FEEDBACK FOR HIGH-RESOLUTION CRYOGENIC PARTICLE-DETECTION [J].
IRWIN, KD .
APPLIED PHYSICS LETTERS, 1995, 66 (15) :1998-2000
[10]   Photon-noise-limited direct detector based on disorder-controlled electron heating [J].
Karasik, BS ;
McGrath, WR ;
Gershenson, ME ;
Sergeev, AV .
JOURNAL OF APPLIED PHYSICS, 2000, 87 (10) :7586-7588