-
Constraints on Photon Beam Line
-
Energy resolution of photons on target:
E < 0.5%
-
Photon flux capability up to 108 /s
within the interval 75-95% E0.
-
Linear polarization as large as possible, requires coherent bremsstrahlung from a
crystal radiator and collimation of photon beam to 100µr or better.
-
Long collimation space between radiator and experimental target to allow angle-displacement
dispersion to develop: 60-100m from radiator to defining collimator.
-
Virtual focus of electron beam at the entrance to defining collimator, r.m.s. of virtual
beam spot 100µm.
-
Fine steering of electron beam just before bremsstrahlung target, stabilized by feedback
from sensors built into the collimator, to an accuracy of 2µr.
-
Beam spot size at radiator as large as possible to extend crystal lifetime, alternative
is to scan the crystal across the beam spot during running.
-
Sufficient beam current, dump capability to give necessary flux with collimation,
10µA is desirable.
-
Tagger magnet capable of bending 50% E0 electrons into instrumented focal
plane and bend beam part way into beam dump.
-
Special focal plane segment with high segmentation over a small bite for use with
collimated beam.
-
Tagger magnet designed to be usable at 24GeV, in case of future upgrade.
-
Design Choices
-
Beam dumped in horizontal plane.
-
Beam transport, shielding, dump designed for a maximum of 10µA at 24GeV.
-
Two extra dipoles after tagger magnet bend the beam to 15o into the
beam dump.
-
Spearate buildings for tagger, experimental hall.
-
Facility housed in two buildings (tagger + experimental hall) above ground,
connected by concrete tunnel into which one could mount a beam pipe or helium
bag to transport the photon beam, signal cables, etc., dry but not air-tight.
-
Last 20' of tunnel before experimental hall is a rectangular cavity with concrete
walls thick enough to shield the experiment from collimation debris. This is
space for the collimation and sweeping magnet systems
-
Tagging counters can be small (1" high) with sigle phototubes on each counter.
Instrumenting the full tagger focal plane 50-95% E0 with
E=0.5% counters = 90 channels. This
segmentation is sufficient to handle the rates up to 108/s within
25% of E0 when running without collimation.
-
Focal plane must be reconfigurable to a more compact configuration for running
with collimation and coherent bremsstrahlung..
-
Tagger magnet runs initially at 1T field so that at 24GeV it can still bend the beam
into the same path and tag the same bite running at 2T.
Drawings and Specifications
Notes on Coherent Bremsstrahlung
|
Intense Beams of Polarized and Nearly Monochromatic Photons
from Coherent Bremsstrahlung
presented at the
Workshop on Physics with 8+GeV Photons Beams
(Indiana Univ., Bloomington, July 14-16, 1997)
by R.T. Jones
|
(postscript, 1.1Mb)
|
|
A Photon Beam for a Vector Meson Spectroscopy Facility at CEBAF
presented at the
Workshop on Hybrids and Photoproduction Physics
(N.C. State Univ., Raleigh, NC, Nov. 13-15, 1997)
by R.T. Jones
|
(transparencies)
|
|
The Beamline for a new Meson Photoporoduction Facility for
CEBAF at 12GeV
presented at the
Physics with 8+GeV Photons Workshop
(CMU, Pittsburgh, March 13-14, 1998)
by R.T. Jones
|
(transparencies)
|
|
Optimal Photon Sources for CEBAF at Higher Energies
presented at the
Physics and Instrumentation with 6-12 GeV Electrons
(Jefferson Lab, Newport News, June 13-15, 1998)
by R.T. Jones
|
(proceedings)
|
Richard Jones
University of Connecticut / Jefferson Lab
``Inclusive cross sections for pion and proton production by photons
using collimated coherent bremsstrahlung''
by W. Kaune, G. Miller, W. Oliver, R.W. Williams, and K.K. Young
(University of Washington) Phys. Rev. D11 no.3 pp.478-494,1975
``Coherent bremsstrahlung in crystals as a tool for producing high
energy photon beams to be used in photoproducion experiments at CERN
SPS'' by H. Bilokon, G. Bologna, F. Celani, B. D'Ettorre Piazzoli,
R. Falcioni, G. Mannocchi, and P. Picchi Nucl. Instr. Meth. 204
pp.299-310,1983