Abstract

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 ${4.3\text{ }\text{ }\mathrm{kW}/\mathrm{cm}}^{2}$ 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 second sound detection for superconducting cavities.

Highlights

  • Radio-frequency cavities are state of the art technology in high energy particle accelerators to increase the momentum of charged particles

  • The times of arrival of the second sound signal on the two nearest oscillating superleak transducers (OSTs) are represented in Fig. 5 together with the corresponding times of arrival for the following hypothesis: a pure second sound wave is emitted by a pointlike heat source situated at the quench location

  • The first approach considered for the quench localization with OSTs was based on the hypothesis of an instantaneously emitted heat wave by a pointlike source which travels from this source to the OSTs with the second sound velocity in superfluid helium

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Summary

INTRODUCTION

Radio-frequency cavities are state of the art technology in high energy particle accelerators to increase the momentum of charged particles. The mechanical systems require custom-fit frame for each cavity geometry, but for elliptical cavities they can be mounted on a rotating frame, that allows moving them around the cavity in order to locate the quench spot Another method for the detection is the utilization of the special heat transport properties in He II. We performed five tests on two single-cell superconducting cavities, with variation of the helium bath temperature for one of them, and always observed premature signals. For several single-cell cavities such tests could be realized with second sound sensors for quench localization During those tests, each cavity was equipped with a temperature mapping system, and with four OSTs facing the cavity in the equator plane, placed at around 6.5 cm from the cavity. The helium bath temperature was about 1.5 K for Cavity A and about 1.6 K for Cavity B

Quench localization with temperature mapping system
OST Measurements with varying helium temperature
Conclusions on OSTs measurement during cavity tests
PROPAGATION IN HELIUM
Heat pulse generation
Variation of the heat pulse power
Tests with a localized heater in liquid helium
Variation of the heat pulse energy
Conclusions on heater experiments
PROPAGATION IN NIOBIUM
Findings
CONCLUSION
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