Experimental study of second sound quench detection for superconducting cavities

Superconducting rf cavities are used in particle accelerators to provide energy to the particle beam. Such cavities are mostly fabricated in niobium and often operated in superfluid helium. One of their limits of operation is the appearance of a local quench, initiated by a local field enhancement due to a defect, which leads to a normal conducting transition of the cavity. Localizing the quench area can be achieved with temperature mapping systems. Another method is the use of second sound wave propagation in superfluid helium. Measuring the time of propagation of these waves from quench location to special sensors, called oscillating superleak transducers (OSTs), and using their well-known velocity should allow trilateration. However, most of the experimental measurements on cavities show premature signals, i.e., the second sound signals arrive earlier on the OSTs than expected. This paper presents several quench experiments on cavities equipped with OSTs and temperature mapping quench detection systems. Two hypotheses can explain the observed premature signals. The first one assesses faster propagation in helium. An experimental setup has been developed for testing this hypothesis, where second sound is created by a localized heater in a controlled environment up to 4 . 3 kW = cm 2 and 2.8 J. Premature signals could not be verified in this setup. A second hypothesis based on a simple model including several processes in niobium and second sound propagation in helium is discussed. The model improves significantly the prediction of the times of arrival of the second sound waves. The overall study shows that the processes in niobium play a prominent role in the

[1]  W. Guo,et al.  Quench-Spot Detection for Superconducting Accelerator Cavities Via Flow Visualization in Superfluid Helium-4 , 2018, Physical Review Applied.

[2]  Gabriele Costanza,et al.  Vertical Test Results on ESS Medium and High Beta Elliptical Cavity Prototypes Equipped with Helium Tank , 2017 .

[3]  Y. Iwashita,et al.  Instrumentation for localized superconducting cavity diagnostics , 2017 .

[4]  J. Bremer,et al.  Study of Temperature Wave Propagation in Superfluid Helium Focusing on Radio-Frequency Cavity Cooling , 2015 .

[5]  A. Macpherson,et al.  High Flux Three Dimensional Heat Transport in Superfluid Helium and Its Application to a Trilateration Algorithm for Quench Localization With OSTs , 2015 .

[6]  R. Eichhorn,et al.  On Quench Propagation, Quench Detection and Second Sound in SRF Cavities , 2015 .

[7]  F. Éozénou,et al.  Development of vertical electropolishing process applied on 1300 and 704 MHz superconducting niobium resonators , 2014 .

[8]  B. Peters Advanced Heat Transfer Studies in Superfluid Helium for Large-scale High-yield Production of Superconducting Radio Frequency Cavities , 2014 .

[9]  A. Navitski,et al.  Progress of R&D on SRF Cavities at DESY towards the ILC Performance Goal , 2014 .

[10]  A. Nassiri,et al.  New method to improve the accuracy of quench position measurement on a superconducting cavity by a second sound method , 2012 .

[11]  F. Éozénou,et al.  Development of an advanced electropolishing setup for multicell high gradient niobium cavities , 2012 .

[12]  E. Ciapala,et al.  SECOND SOUND MEASUREMENT USING SMD RESISTORS TO SIMULATE QUENCH LOCATIONS ON THE 704 MHz SINGLE-CELL CAVITY AT CERN , 2012 .

[13]  M. Uhrmacher,et al.  Response of an oscillating superleak transducer to a pointlike heat source , 2011, 1111.5520.

[14]  Y. Maximenko QUENCH DYNAMICS IN SRF CAVITIES : CAN WE LOCATE THE QUENCH ORIGIN WITH 2ND SOUND ? , 2011 .

[15]  F. Éozénou,et al.  Aging of the HF − H 2 SO 4 electrolyte used for the electropolishing of niobium superconducting radio frequency cavities: Origins and cure , 2010 .

[16]  J. Gheller,et al.  Cryogenics Activities at the Institute of Research into the Fundamental Laws of the Universe (Irfu) , 2010 .

[17]  R. Geng,et al.  GRADIENT LIMITING DEFECTS IN 9-CELL CAVITIES EP PROCESSED AND RF TESTED AT JEFFERSON LAB* , 2009 .

[18]  R. Donnelly The two-fluid theory and second sound in liquid helium , 2009 .

[19]  R. Donnelly,et al.  The Observed Properties of Liquid Helium at the Saturated Vapor Pressure , 1998 .

[20]  I. Rudnick,et al.  The velocity of second sound near Tλ , 1969 .

[21]  A. Dessler,et al.  Amplitude Dependence of the Velocity of Second Sound , 1956 .

[22]  I. Khalatnikov DISCONTINUITIES AND HIGH-AMPLITUDE SOUND IN HELIUM II , 1952 .

[23]  H. Temperley The Theory of the Propagation in Liquid Helium II of `Temperature-Waves' of Finite Amplitude , 1951 .

[24]  E. Elsen,et al.  Diagnostics and treatment of 1.3 GHz Nb cavities , 2016 .

[25]  R. Eichhorn,et al.  On the Mystery of using Helium's second Sound for Quench Detection of a Superconducting Cavity , 2015 .

[26]  H. Hayano,et al.  COMBINED SYSTEM OF OPTICAL INSPECTION AND LOCAL GRINDER , 2014 .

[27]  C. Magne,et al.  EXPERIMENTAL INVESTIGATIONS OF THE QUENCH PHENOMENA FOR THE QUENCH LOCALIZATION BY THE SECOND SOUND WAVE METHOD , 2013 .

[28]  Z. A. Conway,et al.  DEFECT LOCATION IN SUPERCONDUCTING CAVITIES COOLED WITH HE-II USING OSCILLATING SUPERLEAK TRANSDUCERS * , 2009 .

[29]  Eric Smith,et al.  OSCILLATING SUPERLEAK TRANSDUCERS FOR QUENCH DETECTION IN SUPERCONDUCTING ILC CAVITIES COOLED WITH HE-II * , 2008 .

[30]  H. Padamsee,et al.  RF superconductivity for accelerators , 1998 .

[31]  Hasan Padamsee,et al.  FIELD EMISSION STUDIES IN SUPERCONDUCTING CAVITIES , 1987 .

[32]  A. Dessler Interactions between First and Second Sound in Liquid Helium , 1959 .