Paper | Title | Page |
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WE205 | Electro-mechanical properties of spoke-loaded superconducting cavities | 404 |
| - Z. A. Conway, J. D. Fuerst, M. P. Kelly, K. W. Shepard
ANL - G. K. Davis, J. Delayen
TJNAF
| |
| This paper presents experimental data characterizing
the electro-mechanical properties of superconducting
spoke-loaded cavities developed for high-intensity ionlinac
applications, such as the cw ANL Advanced Exotic
Beams Laboratory (AEBL) driver linac and the pulsed
FNAL High Intensity Neutrino Source (HINS, now
project X) proton driver linac. High-gradient cw
operation at 4.2 K can produce violent boiling in the
liquid helium coolant causing microphonic frequency
noise. A spoke cavity designed to minimize the effects of
helium pressure on RF eigenfrequency, the total
microphonic induced RF frequency variations, were found
to be on the level of the phase noise in the reference
oscillator. To determine the pulsed cavity RF
performance, the Lorentz transfer function was measured
and used to predict the dynamic detuning in pulsed
operation. There is good agreement between the
predicted fit and the measured data, demonstrating the
utility of the Lorentz transfer function, which can
completely characterize the dynamics of the coupling
between the mechanical cavity structure and the cavity RF
field due to the Lorentz force. | |
 | Slides(PDF) | |
WEP28 | Latest Results of ILC High-Gradient R&D 9-cell Cavities at JLAB | 525 |
| - R. L. Geng, R. Afanador, A. C. Crawford, G. K. Davis, D. Forehand, C. Dreyfus, C. Grenoble, B. Golden, R. Johnson, P. Kushnick, K. Macha, J. Mammosser, J. Saunders, A. Wu
JLab - D. Bice, D. A. Sergatskov
Fermilab
| |
| It has been over a year since JLAB started processing
and testing ILC 9-cell cavities in the frame work of
ILC high-gradient cavity R&D, aiming at the goal of a
35 MV/m gradient at a Q0 of 1E10 with a yield of 90%.
The necessary cavity processing steps include field flatness
tuning, electropolishing (EP), hydrogen out-gassing under
vacuum, high-pressure water rinsing, clean room assembly,
and low temperature bake. These are followed by RF
test at 2 Kelvin. Ultrasonic cleaning with Micro-90, an effective
post-EP rinsing recipe discovered at JLAB, is routinely
used. Seven industry manufactured 9-cell TESLAshape
cavities are processed and tested repeatedly. So far,
33 EP cycles are accumulated, corresponding to more than
65 hours of active EP time. An emphasis put on RF testing
is to discern cavity quench characteristics, including its nature
and its location. Often times, the cavity performance is
limited by thermal-magnetic quench instead of field emission.
The quench field in some cavities is lower than 20
MV/m and remains unchanged despite repeated EP, implying
material and/or fabrication defects. The quench field
in some other cavities is high but changes unpredictably
after repeated EP, suggesting processing induced defects.
Based on our experience and results, several areas are identified
where improvement is needed to improve cavity performance
as well as yield. | |
WEP32 | Performance of the CEBAF prototype cryomodule renascence | 540 |
| - C. E. Reece, E. F. Daly, G. K. Davis, M. Drury, W. R. Hicks, J. Preble, H. Wang
JLab
| |
| The prototype cryomodule Renascence was constructed as
an energy building block for securing 6 GeV operation of
CEBAF and to validate design elements for future
CEBAF upgrade modules. These elements include the
new "HG" and "LL" 7-cell cavity designs and a new tuner
design.[1,2] Issues were identified during initial testing in
2005. The module has been reworked to address the issues
with thermal stability, component breakage, and tuner
motion. In addition, opportunity was taken to employ
upgraded cleaning and assembly techniques for the cavity
string. The HOM coupler heating issue was resolved, and
seven of the eight cavities in the cryomodule have run
stably at an average of 20 MV/m CW. The cryogenic, rf,
and mechanical performance of the cryomodule are presented. Commissioning in CEBAF has just been completed in October 2007. | |
WEP62 | Diagnosis, analysis, and resolution of thermal stability issues with HOM couplers on prototype CEBAF SRF cavities | 656 |
| - C. E. Reece, E. F. Daly, G. K. Davis, W. R. Hicks, T. Rothgeb, H. L. Phillips, J. Preble, H. Wang, G. Wu
TJNAF
| |
| During initial testing of the prototype cavities
incorporated into the developmental cryomodule
Renascence severe thermal stability issues were
encountered during CW operation. Additional diagnostic
instrumentation was added. This enabled identification of
an unanticipated thermal impedance between the HOM
coupler probe feedthrough assembly and the cavity
beamtube. Subsequent detailed FE analysis successfully
modeled the situation and indicated the need for alternate
cooling path for the couplers on those cavities. HOM
damping was measured to be adequate employing only
two of the four HOM couplers. The two pickup probes on
the couplers at the input power coupler side of each cavity
were removed, the remaining HOM probe feedthroughs
were heat stationed to two-phase helium supply piping,
and a novel heat sink was added to station both the inner
and outer conductors of the remaining HOM rf cables.
The characterization measurements, analysis,
modifications, and resulting performance are presented. | |
WEP67 | Low-level RF control of microphonics in superconducting spoke-loaded cavities | 669 |
| - Z. A. Conway, M. P. Kelly, S. I. Sharamentov, K. W. Shepard
ANL - G. K. Davis, J. Delayen
TJNAF - L. R. Doolittle
LBNL
| |
| This paper presents the results of cw RF frequency
control and RF phase-stabilization experiments performed
with a piezoelectric fast tuner mechanically coupled to a
superconducting, 345 MHz, beta = 0.5 triple-spoke-loaded
cavity operating at 4.2K. The piezoelectric fast tuner
damped low-frequency microphonic-noise by an order of
magnitude. Two methods of RF phase-stabilization were
characterized: overcoupling with negative phase feedback,
and also fast mechanical tuner feedback. The beta = 0.5
triple-spoke-loaded cavity RF field amplitude and phase
errors were controlled to +(-)0.5% and +(-)30 respectively. | |