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Toward THz Single Photon Detection with a Superconducting Nanobolometer

Daniel F. Santavicca, Bertrand Reulet, Boris S. Karasik, Sergei V. Pereverzev, David I. Olaya, M. E. Gershenson, Luigi Frunzio, D. E. Prober

Published Apr 1, 2009• 0 citations
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We propose a new detection technique based on radio-frequency (RF) bias and readout of an antenna-coupled superconducting nanobolometer. This approach is suitable for Frequency-Division-Multiplexing (FDM) readout of large arrays using broadband low-noise RF amplifier. We call this new detector RFTES. This feasibility study was made on demonstrator devices which are made in all-Nb technology and operate at 4.2 K. The studied RFTES devices consist of an antenna-coupled superconducting nanobolometer made of ultrathin niobium films with transition temperature Tc = 5.2 K. The 0.65-THz antenna and nanobolometer are embedded as a load into a GHz-range coplanar niobium resonator (Tc = 8.9 K, Q = 4000). To heat the superconducting Nb nanobolometer close to the Tc, the RF power at resonator frequency f = 5.8 GHz is applied via a transmission line which is weakly coupled (-11 dB) to the loaded resonator. The THz-antenna of RFTES was placed in the focus of a sapphire immersion lens inside a He4-cryostat equipped with an optical window and a semiconductor RF amplifier. We have demonstrated optical response of the RFTES to THz radiation. The demonstrator receiver system employing the RFTES device showed an optical Noise-Equivalent Power (NEP) 1e-14 W/sqrt(Hz) at 4.2 K.
We are developing hot-electron superconducting transition-edge sensors (TES) capable of counting THz photons and operating at . We fabricated superconducting Ti nanosensors with Nb contacts with a volume of on planar Si substrates and have measured the thermal conductance in the material, G=4times10-3W/K at 0.3 K, caused predominantly by the weak electron-phonon coupling. The corresponding phonon-noise NEP=3times10-19W/Hz1/2. Detection of single optical photons (1550 nm and 670 nm wavelength) has been demonstrated for larger devices and yielded the thermal time constants of 30 mus at 145 mK and of 25 mus at 190 mK. This hot-electron direct detector (HEDD) is expected to have a small enough energy fluctuation noise for detecting individual photons with v>THz where NEP~3times10-20W/Hz1/2is needed for spectroscopy in space.
Ultralight bosonic dark matter with masses in the meV range, corresponding to terahertz (THz) Compton frequencies, remains largely unexplored due to the difficulty of achieving both efficient signal conversion and single-photon-sensitive detection at THz frequencies. We propose a hybrid detection architecture that integrates a dielectric haloscope, Rydberg-atom transducer, and superconducting nanowire single-photon detection within a unified cryogenic platform operating at ≲1 K\lesssim 1\,\text{K}≲1K. The dielectric haloscope converts dark matter into THz photons via phase-matched resonant enhancement, achieving form factors C∼0.4C \sim 0.4C∼0.4 and loaded quality factors QL∼104Q_L \sim 10^4QL​∼104. A cold 87^{87}87Rb ensemble then coherently up-converts the THz signal to the optical domain through six-wave mixing among Rydberg states. The intrinsic directionality and narrow bandwidth (Δνatomic∼1 MHzΔν_{\mathrm{atomic}} \sim 1\,\text{MHz}Δνatomic​∼1MHz) of this process provide extra suppression of isotropic thermal backgrounds. With 10 days of integration at 0.3 K0.3\,\text{K}0.3K, we project sensitivity to the axion-photon coupling gaγγ∼10−13 GeV−1g_{aγγ} \sim 10^{-13}\,\mathrm{GeV}^{-1}gaγγ​∼10−13GeV−1 at ma∼0.4 meVm_a \sim 0.4\,\text{meV}ma​∼0.4meV, reaching the QCD axion band and opening the THz window for searches of both axion and dark photon dark matter.