transverse rf spin rotator for the n- 3 he experiment
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Transverse RF Spin Rotator for the n- 3 He experiment. Christopher Crawford University of Kentucky for the n- 3 He Collaboration n-3He Technical Review ORNL, TN 2013-01-08. Transverse RF spin rotator. Resonant RF spin rotator - PowerPoint PPT PresentationTRANSCRIPT
Transverse RF Spin Rotatorfor the n-3He experiment
Christopher CrawfordUniversity of Kentucky
for the n-3He Collaboration
n-3He Technical Review
ORNL, TN 2013-01-08
Transverse RF spin rotator
Resonant RF spin rotator• P-N Seo et al., Phys. Rev. S.T.
Accel. Beam 11, 084701 (2008)
Properties suitable for n-3He expt.• Transverse horizontal RF B-field• Longitudinal or transverse flipping• No fringe field - 100% efficiency• Real, not eddy currents along outside
minimizes RF leaked outside SR• Doesn’t affect neutron velocity• Compact geometry• Matched to the driver electronics
of the NPDGamma spin flipper
Construction• Development in parallel with similar
design for nEDM neutron guide field• Few-winding prototype built at Uky;
Real RFSF being built now
field linesend cap windings
NPDGammawindings
n-3Hewindings
Inner / outer coil design
Windings calculated using scalar potential• Uniform transverse RF field inside• Zero leakage field enforced by B.C.’s• Copper wires run along equipotentials
1. Inner region:
2. Intermediate:
3. Outer region:
4:1 inside / outside winding ratio• By choosing
appropriate radii• Perfect cos theta
windings inside & out• 48 inner loops of
18 AWG wire
Status
Waiting for winding grooves to be machined in nylon forms
Alternate winding patterns
Three possibilities all give same field in high-frequency limitINNER INNER/OUTER OUTER
easiest to wind no eddy currents no copper in beam
All three wound using same grooves
R&D: test RF fields of each winding
Holding field:
Resonant frequency:
Inductance: 4.5 mH
Capacitance: 7.5 nF
Resistance: 5.1 Ω
Maximum voltage:
Stored energy:
Dissipated power:
Quality factor: Q=151
Electrical specifications
•RF field strength depends time spent in RFSF.
•High energy neutron beams (~20 meV) will be travelling upwards of 1000 m/s
•These neutrons will spend approximately 398 microseconds inside the RFSF and need to rotate π-radians
•Flip rate:
•The maximum value of the required rotational field is then,
•The maximum value of the required RF field is exactly twice this,
•To produce this field, we calculate the maximum value of required current given the winding spacing of the inner coils.
•Proportionally Constant:
Electrical specifications