Abstract

The most challenging issue for understanding the performance of superconducting radio-frequency (rf) cavities made of high-purity (residual resistivity ratio $>200$) niobium is due to a sharp degradation (``$Q$-drop'') of the cavity quality factor ${Q}_{0}({B}_{p})$ as the peak surface magnetic field (${B}_{p}$) exceeds about 90 mT, in the absence of field emission. In addition, a low-temperature ($100--140\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$) in situ baking of the cavity was found to be beneficial in reducing the $Q$-drop. In this contribution, we present the results from a series of rf tests at 1.7 and 2.0 K on a single-cell cavity made of high-purity large (with area of the order of few ${\mathrm{cm}}^{2}$) grain niobium which underwent various oxidation processes, after initial buffered chemical polishing, such as anodization, baking in pure oxygen atmosphere, and baking in air up to $180\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$, with the objective of clearly identifying the role of oxygen and the oxide layer on the $Q$-drop. During each rf test a temperature mapping system allows measuring the local temperature rise of the cavity outer surface due to rf losses, which gives information about the losses location, their field dependence, and space distribution. The results confirmed that the depth affected by baking is about 20--30 nm from the surface and showed that the $Q$-drop did not reappear in a previously baked cavity by further baking at $120\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$ in pure oxygen atmosphere or in air up to $180\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$. These treatments increased the oxide thickness and oxygen concentration, measured on niobium samples which were processed with the cavity and were analyzed with transmission electron microscope and secondary ion mass spectroscopy. Nevertheless, the performance of the cavity after air baking at $180\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$ degraded significantly and the temperature maps showed high losses, uniformly distributed on the surface, which could be completely recovered only by a postpurification treatment at $1250\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$. A statistic of the position of the ``hot spots'' on the cavity surface showed that grain boundaries are not the preferred location. An interesting correlation was found between the $Q$-drop onset, the quench field, and the low-field energy gap, which supports the hypothesis of thermomagnetic instability governing the $Q$-drop and the baking effect.

Highlights

  • Superconducting elliptical rf cavities operating in the TM010 mode are commonly used to accelerate particle beams in a variety of accelerator facilities throughout the world

  • The results from the anodization experiments confirm that the changes produced by the low-temperature in situ baking occur within about 30 nm deep into the niobium

  • These results, combined with the fact that the baking effect is stable after exposure of the cavity to air for many months and to successive high-pressure water rinsing, exclude the possibility of the Q-drop being caused by adsorbates on the surface

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Summary

Introduction

Superconducting elliptical rf cavities operating in the TM010 mode are commonly used to accelerate particle beams in a variety of accelerator facilities throughout the world. Niobium has been the material of choice for this application mainly due to its formability, relatively high critical temperature, and the highest lower critical magnetic fields among all superconductors. The significant improvements of surface cleaning techniques and control of contamination in recent years allowed one to reduce or eliminate field emission and to consistently improve the peak electric and magnetic fields on the cavity surface and the operational accelerating gradient. A few single-cell cavities have achieved Bp-values close to the thermodynamic critical field of niobium [1]. Even field emission free superconducting cavities made of bulk niobium often show a severe degradation of the quality factor Q0 as Bp exceeds 90 mT.

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