An L-band superconducting cavity has been designed for acceleration of particles travelling at 81 % the speed of light (β = 0.81). Four single-cell prototypes have been being fabricated and tested. Two of these cavities were formed from standard high purity fine grain niobium sheet. The rest were fabricated from large grain niobium. The RF per-formance of the single-cell cavities indicate that the design is suitable for use in a proton linac; the highest measured accelerating gradient was about 28 MV/m. The fabrication of two 7-cell cavity prototypes is in progress
We present the first rf studies of the medium-β superconducting radio frequency (SRF) elliptical cav...
In the past two years accelerator builders have published papers describing mature designs of no few...
The LHC RF system, which must handle high intensity (0.5 A d.c.) beams, makes use of superconducting...
A 6-cell 805 MHz superconducting cavity for acceleration in the velocity range of about 0.4 to 0.53 ...
Three 6-cell 805 MHz superconducting cavity prototypes for acceleration in the velocity range of ab...
Abstract: Proton Driver needs different types of accelerating cavities to accelerate protons from 15...
Three 6-cell 805 MHz superconducting cavity prototypes for acceleration in the velocity range of abo...
This paper reports the development of 350 MHz niobium superconducting cavities for the velocity rang...
This paper reports the development of 350 MHz niobium superconducting cavities for the velocity rang...
This paper reports the development of 350 MHz niobium superconducting cavities for the velocity rang...
The authors initiated a program to develop superconducting (SC) RF for high-power proton linacs. The...
The design of an Accelerator Production of Tritium (APT) facility being investigated at Los Alamos i...
A nine-cell superconducting RF accelerating cavity is designed for the TeV electron linear accelerat...
A 972MHz, β=0.725, 9-cell niobium cavity with an optimised cell-shape was designed by using electrom...
We report on the recent progress at Jefferson Lab in developing ultra high gradient and high Q{sub 0...
We present the first rf studies of the medium-β superconducting radio frequency (SRF) elliptical cav...
In the past two years accelerator builders have published papers describing mature designs of no few...
The LHC RF system, which must handle high intensity (0.5 A d.c.) beams, makes use of superconducting...
A 6-cell 805 MHz superconducting cavity for acceleration in the velocity range of about 0.4 to 0.53 ...
Three 6-cell 805 MHz superconducting cavity prototypes for acceleration in the velocity range of ab...
Abstract: Proton Driver needs different types of accelerating cavities to accelerate protons from 15...
Three 6-cell 805 MHz superconducting cavity prototypes for acceleration in the velocity range of abo...
This paper reports the development of 350 MHz niobium superconducting cavities for the velocity rang...
This paper reports the development of 350 MHz niobium superconducting cavities for the velocity rang...
This paper reports the development of 350 MHz niobium superconducting cavities for the velocity rang...
The authors initiated a program to develop superconducting (SC) RF for high-power proton linacs. The...
The design of an Accelerator Production of Tritium (APT) facility being investigated at Los Alamos i...
A nine-cell superconducting RF accelerating cavity is designed for the TeV electron linear accelerat...
A 972MHz, β=0.725, 9-cell niobium cavity with an optimised cell-shape was designed by using electrom...
We report on the recent progress at Jefferson Lab in developing ultra high gradient and high Q{sub 0...
We present the first rf studies of the medium-β superconducting radio frequency (SRF) elliptical cav...
In the past two years accelerator builders have published papers describing mature designs of no few...
The LHC RF system, which must handle high intensity (0.5 A d.c.) beams, makes use of superconducting...