Understanding Quality Factor Degradation in Superconducting Niobium Cavities at Low Microwave Field Amplitudes.

In niobium superconducting radio frequency (SRF) cavities for particle acceleration, a decrease of the quality factor at lower fields-a so-called low field Q slope or LFQS-has been a long-standing unexplained effect. By extending the high Q measurement techniques to ultralow fields, we discover two previously unknown features of the effect: (i) saturation at rf fields lower than E_{acc}∼0.1  MV/m; (ii) strong degradation enhancement by growing thicker niobium pentoxide. Our findings suggest that the LFQS may be caused by the two level systems in the natural niobium oxide on the inner cavity surface, thereby identifying a new source of residual resistance and providing guidance for potential nonaccelerator low-field applications of SRF cavities.

[1]  V. A. Tulin,et al.  Evidence for interacting two-level systems from the 1/f noise of a superconducting resonator , 2013, Nature Communications.

[2]  M. Siegel,et al.  Measurement of dielectric losses in amorphous thin films at gigahertz frequencies using superconducting resonators , 2010 .

[3]  W. Marsden I and J , 2012 .

[4]  Erik Lucero,et al.  Surface loss simulations of superconducting coplanar waveguide resonators , 2011, 1107.4698.

[5]  C. Antoine,et al.  Materials and surface aspects in the development of SRF Niobium cavities; EuCARD Editorial Series on , 2012 .

[6]  Luke Gordon,et al.  Hydrogen bonds in Al2O3 as dissipative two-level systems in superconducting qubits , 2014, Scientific Reports.

[7]  C. Reece,et al.  Parametric converters for detection of small harmonic displacements , 1986 .

[8]  T M Klapwijk,et al.  Evidence of a nonequilibrium distribution of quasiparticles in the microwave response of a superconducting aluminum resonator. , 2013, Physical review letters.

[9]  D. Mattis,et al.  Theory of the anomalous skin effect in normal and superconducting metals , 1958 .

[10]  C. Caves MICROWAVE CAVITY GRAVITATIONAL RADIATION DETECTORS , 1979 .

[11]  J. Cole,et al.  Observation of directly interacting coherent two-level systems in an amorphous material , 2015, Nature Communications.

[12]  Jonas Zmuidzinas,et al.  Superconducting Microresonators: Physics and Applications , 2012 .

[13]  A. Romanenko,et al.  Nitrogen and argon doping of niobium for superconducting radio frequency cavities: a pathway to highly efficient accelerating structures , 2013, 1306.0288.

[14]  S. Hunklinger,et al.  Saturation of the dielectric absorption of vitreous silica at low temperatures , 1977 .

[15]  Hasan Padamsee The science and technology of superconducting cavities for accelerators , 2001 .

[16]  S. Girvin,et al.  Observation of high coherence in Josephson junction qubits measured in a three-dimensional circuit QED architecture. , 2011, Physical review letters.

[17]  A. Grassellino,et al.  Dependence of the residual surface resistance of superconducting radio frequency cavities on the cooling dynamics around Tc , 2014, 1401.7747.

[18]  H. Neven,et al.  Observation of Classical-Quantum Crossover of 1/f Flux Noise and Its Paramagnetic Temperature Dependence. , 2016, Physical review letters.

[19]  Erik Lucero,et al.  Decoherence dynamics of complex photon states in a superconducting circuit. , 2009, Physical review letters.

[20]  A. Grassellino,et al.  Error analysis for intrinsic quality factor measurement in superconducting radio frequency resonators. , 2014, The Review of scientific instruments.

[21]  A. Grassellino,et al.  Dependence of the microwave surface resistance of superconducting niobium on the magnitude of the rf field , 2013, 1304.4516.

[22]  Clare C. Yu,et al.  Decoherence in Josephson qubits from dielectric loss. , 2005, Physical review letters.

[23]  Andrew W. Cross,et al.  Experimental Demonstration of a Resonator-Induced Phase Gate in a Multiqubit Circuit-QED System. , 2016, Physical review letters.

[24]  A. Tzalenchuk,et al.  Direct Identification of Dilute Surface Spins on Al_{2}O_{3}: Origin of Flux Noise in Quantum Circuits. , 2016, Physical review letters.

[25]  D. Tracy,et al.  A 11 a , 2016 .

[26]  F. Pegoraro,et al.  On the operation of a tunable electromagnetic detector for gravitational waves , 1978 .

[27]  A. Gurevich Theory of RF superconductivity for resonant cavities , 2017 .

[28]  Liang Jiang,et al.  Quantum memory with millisecond coherence in circuit QED , 2015, 1508.05882.

[29]  A. Romanenko,et al.  Ultra-high quality factors in superconducting niobium cavities in ambient magnetic fields up to 190 mG , 2014, 1410.7877.

[30]  H. Padamsee Superconducting Radio-Frequency Cavities , 2014 .

[31]  M. Siegel,et al.  Probing the density of states of two-level tunneling systems in silicon oxide films using superconducting lumped element resonators , 2015 .

[32]  A. Romanenko,et al.  Unprecedented quality factors at accelerating gradients up to 45 MVm−1 in niobium superconducting resonators via low temperature nitrogen infusion , 2017, 1701.06077.

[33]  A. Ringwald,et al.  A cavity experiment to search for hidden sector photons , 2007, 0707.2063.

[34]  Jonas Zmuidzinas,et al.  Experimental evidence for a surface distribution of two-level systems in superconducting lithographed microwave resonators , 2008, 0802.4457.

[35]  Jiansong Gao,et al.  The physics of superconducting microwave resonators , 2008 .

[36]  G. Ciovati,et al.  Effect of low-temperature baking on the radio-frequency properties of niobium superconducting cavities for particle accelerators , 2004 .

[37]  Andrew G. Glen,et al.  APPL , 2001 .