temporary spectrometer for RUBICON experiment ATF beamline 2 K Kusche M Fedurin RSC meeting Jan 20 2015 Description Temporary spectrometer required for RUBICON experiment at ATF Primary goals are electron beam modulation and xray detection ID: 393069
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Slide1
Shielding review for temporary spectrometer for RUBICON experiment, ATF beamline #2
K. Kusche, M. Fedurin
RSC meeting, Jan 20, 2015Slide2
DescriptionTemporary spectrometer required for RUBICON experiment at ATF. Primary goals are electron beam modulation and x-ray detection.
Spectrometer consists of dipole,
imaging system (within vacuum
cross), Be window.Position on beamline #2 constrained by electron and laser beam optics. Too far upstream to utilize existing spectrometer.Slide3
ATF Experimental HallSlide4
Configuration detailsThe dipole center is 115” inches downstream from the
existing
dipole at the head of beamline #2, aligned along
electron beam axis.The dipole can bend the beam in the horizontal plane only (±30 degrees @40 MeV).
1” Beryllium
window on the end of the
spectrometer’s vacuum cross allows
for on-axis x-ray detection. The upstream Be window surface will be under vacuum, the downstream side at atmospheric pressure.Slide5
Beam parametersRoutine
operation for this experiment is 50 MeV, 200 pC, 1.5 Hz with no experiment-induced beam modulation.
With
modulation, the 200 pC will be spread horizontally over 40-110 MeV range on the spectrometer. Modulation only occurs during CO2 laser pulse (limited to 0.05 Hz, which is once per 30 unmodulated bunches).The routine condition is
with the dipole powered
and electron beam imaged
in the spectrometer. Slide6
Dipole parametersPower supply for the temporary dipole is bipolar and limited to ±10 A. (±30 degrees @40 MeV)
Magnet pole gap: vertical =1.25” , horizontal= 8” diameter (limited by vacuum chamber to 30 degree slice
)
If the dipole were turned off or failed, the electron beam would proceed straight at the Be window.