Development of a prototype superconducting radio-frequency cavity for conduction-cooled accelerators
G. Ciovati, J. Anderson, S. Balachandran, G. Cheng, B. Coriton, E. Daly, P. Dhakal, A. Gurevich, F. Hannon, K. Harding, L. Holland, F. Marhauser, K. McLaughlin, D. Packard, T. Powers, U. Pudasaini, J. Rathke, R. Rimmer, T. Schultheiss, H. Vennekate, D. Vollmer
DOI 10.1103/PhysRevAccelBeams.26.044701 · Physical Review Accelerators and Beams
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
The higher efficiency of superconducting radio-frequency (SRF) cavities compared to normal-conducting ones enables the development of high-energy continuous-wave linear accelerators (linacs). Recent progress in the development of high-quality Nb3Sn film coatings along with the availability of cryocoolers with high cooling capacity at 4 K makes it feasible to operate SRF cavities cooled by thermal conduction at relevant accelerating gradients for use in accelerators. A possible use of conduction-cooled SRF linacs is for environmental applications, requiring electron beams with energy of 1–10 MeV and 1 MW of power. We have designed a 915 MHz SRF linac for such an application and developed a prototype single-cell cavity to prove the proposed design by operating it with cryocoolers at the accelerating gradient required for 1 MeV energy gain. The cavity has a ∼3 μm thick Nb3Sn film on the inner surface, deposited on a ∼4 mm thick bulk Nb substrate and a bulk ∼7 mm thick Cu outer shell with three Cu attachment tabs. The cavity was tested up to a peak surface magnetic field of 53 mT in liquid He at 4.3 K. A horizontal test cryostat was designed and built to test the cavity cooled with three Gifford-McMahon cryocoolers. The rf tests of the conduction-cooled cavity, performed at General Atomics, achieved a peak surface magnetic field of 50 mT and stable operation was possible with up to 18.5 W of rf heat load. The peak frequency shift due to microphonics was 23 Hz. These results represent the highest peak surface magnetic field achieved in a conduction-cooled SRF cavity to date and meet the requirements for a 1 MeV energy gain.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Nb3Sn Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 18 | Pressure not reported | unknown |
| Nb Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 9.2 | Pressure not reported | unknown |
Similar papers
Thermal feedback in coaxial superconducting radio frequency cavities
similarity 0.97Mattias McMullin et al.
Source status unknown — claims are unverified
Production of superconducting 1.3-GHz cavities for the European X-ray Free Electron Laser
similarity 0.97W. Singer et al.
Source status unknown — claims are unverified
Analysis of magnetic vortex dissipation in Sn-segregated boundaries in Nb3Sn superconducting RF cavities
similarity 0.96Jared Carlson et al.
Source status unknown — claims are unverified
Optimization of a traveling wave superconducting rf cavity for upgrading the International Linear Collider
similarity 0.96V. Shemelin et al.
Source status unknown — claims are unverified
Novel superconducting rf structure for ampere-class beam current for multi-GeV energy recovery linacs
similarity 0.96Z. Liu & A. Nassiri
Source status unknown — claims are unverified
Improved high-gradient performance for medium-velocity superconducting half-wave resonators: Surface preparation and trapped flux mitigation
similarity 0.96Yuting Wu et al.
Source status unknown — claims are unverified