Title :
Superconducting nanostructures for counting of single photons in the infrared range
Author :
Chulkova, G. ; Milostnaya, I. ; Korneev, A. ; Minaeva, O. ; Rubtsova, I. ; Voronov, B. ; Okunev, O. ; Smirnov, K. ; Gol´tsman, G. ; Kitaygorsky, J. ; Cross, A. ; Pearlman, A. ; Sobolewski, R. ; Slysz, W.
Author_Institution :
Moscow State Pedagogical Univ., Russia
Abstract :
We present our studies on ultrafast superconducting single-photon detectors (SSPDs) based on ultrathin NbN nanostructures. Our SSPDs are patterned by electron beam lithography from 4-nm thick NbN film into meander-shaped strips covering square area of 10×10 μm2. The advances in the fabrication technology allowed us to produce highly uniform 100-120-nm-wide strips with meander filling factor close to 0.6. The detectors exploit a combined detection mechanism, where upon a single-photon absorption, an avalanche of excited hot electrons and the biasing supercurrent, jointly produce a picosecond voltage transient response across the superconducting nanostrip. The SSPDs are typically operated at 4.2 K, but they have shown that their sensitivity in the infrared radiation range can be significantly improved by lowering the operating temperature from 4.2 K to 2 K. When operated at 2 K, the SSPD quantum efficiency (QE) for visible light photons reaches 30-40%, which is the saturation value limited by optical absorption of our 4-nm-thick NbN film. For 1.55 μm photons, QE was ∼20% and decreases exponentially with the increase of the optical wavelength, but even at the wavelength of 6 μm the detector remains sensitive to single photons and exhibits QE of about 10-2%. The dark (false) count rate at 2 K is as low as 2 × 10-4 s-1, what makes our detector essentially a background-limited sensor. The very low dark-count rate results in the noise equivalent power (NEP) as low as 10-18 WHz-12/ for the mid-infrared range (6 μm). Further improvement of the SSPD performance in the mid-infrared range can be obtained by substituting NbN for the other, lower-Tc superconductors with the narrow superconducting gap and low quasiparticle diffusivity. The use of such materials will shift the cutoff wavelength towards the values even longer than 6 μm.
Keywords :
diffusion; electron beam lithography; hot carriers; infrared detectors; nanostructured materials; niobium compounds; photon counting; quasiparticles; superconducting photodetectors; superconducting thin films; 1.55 mum; 100 to 120 nm; 2 to 4.2 K; 4 nm; 6 mum; NbN; NbN film; SSPD quantum efficiency; background-limited sensor; biasing supercurrent; cutoff wavelength shift; dark count rate; electron beam lithography; excited hot electrons; fabrication technology; infrared radiation sensitivity; lower-Tc superconductors; meander filling factor; meander-shaped strips; narrow superconducting gap; noise equivalent power; optical absorption; picosecond voltage transient response; quasiparticle diffusivity; single photon counting; single-photon absorption; superconducting nanostrip; superconducting nanostructures; superconducting single-photon detectors; ultrafast single-photon detectors; ultrathin NbN nanostructures; visible light photons; Detectors; Electromagnetic wave absorption; Nanostructures; Optical films; Optical saturation; Optical sensors; Strips; Superconducting films; Superconducting photodetectors; Ultrafast optics;
Conference_Titel :
Advanced Optoelectronics and Lasers, 2005. Proceedings of CAOL 2005. Second International Conference on
Print_ISBN :
0-7803-9130-6
DOI :
10.1109/CAOL.2005.1553930