The first Multi Purpose Spectrometer meeting has been organized by the MPS collaboration [Perdrisat, Garibaldi] with the goals of:
The Multi Purpose Spectrometer [Bogdan], under design and
development for the GEP5 experiment,
will provide 70 msr solid angle at 15 degree and 2-10 GeV/c momentum acceptance.
It will consist of a 46 cm gap, 2-3 Tesla meter dipole magnet (from BNL), and will be
equipped by a combination of the following detectors:
In the original, prelimimary definition, the tracking system is
based on a Micro-Pattern Gas Detector technology
(likely GEM, [Cisbani])
which supports high rate and provides high resolution (70 um)
correspondig to a momentum
resolution of 0.5% at 5 GeV/c and an angular resolution of 0.3 mr.
The same MPGD technology will be used for the large trackers in the polarimeters,
which can be designed to be also used in the BigBite spectrometer to improve
its momentum resolution and consequently to extend the maximum
particle momentum.
Several hot physics cases can beneficiate from the use of the MPS equipments, combined to the 11 GeV which will be available at JLab and the high luminosity expected for the Hall A,
First of all, the nucleon form factors measurements can be extended at high Q2 (GMP, GMN and GEN, in addition to GEP) thanks to the much higher rate supported by MPS, the large momentum acceptance and the availability in Hall A of polarized neutron target that can support high currents (up to 100 uA); work on the upgrade the Hall A 3He polarized target is moving in two directions: new metal (gold coated aluminium) cell and better gas mixing via convective circulation [Cates].
The improvement on the 3He target and the availability of MPS configured with the
hadron PID RICH detector and BigBite
with part of the GEM trackers used in GEP5, can be successfully exploited for new measurements of
pion and kaon single spin asymmetry on transversely polarized neutron in the DIS region,
at high Q2 and in partially unexplored x (Bjorken)
valence region (0.2-0.7) [Cisbani], with superior statistics.
These measurements would contribute additional data for the extraction of the Collins and Sievers asymmetries and their associated Transversity and Sivers transverse momentum distribution functions, related to the spin structure of the nucleon and the orbital angular momentum of the quark in the nucleon.
Meson Photoproduction and high Mass Resonance [Annand, Gilman]
Remarkable advantage will be offered by the MPS equipment in the extension to higher x (and one more energy scan at 11 GeV) of the already approved measurement of the A1N asymmetry, a crucial step in understanding valence nucleon structure [Nilanga].
Use of MPS in place of BigbBite (or BigBite equipped with the MPS GEM tracters), will improve and extend Q2 to 10 GeV2 the measurements of threshold pion production at high Q2, complementary to the low Q2 measurements recently taken in Hall A. A discussion on this direction is going on, within the threshold pion experiments promoters [Lindgren].
The measure of the charge pion form factor at high Q2 [Bogdan], a proposal presented in Hall C for the 12 GeV era+, can also benefit of the larger solid angle of MPS (respect to SHMS), even at low scattering angle.
The low cross section of J/Psi (photo)production may be investigated at JLab12 (proposal submitted in HallC and LOI in HallB) thanks to the high luminosity, using the e+e- (and mu+ mu-) decay [Chudakov]. Two MPS magnets equipped for electron/positron detection at very forward angles (GEM tracking availables from GEP5) would improve significantly the statistics (or reduce the requested data taking time), however a detailed analysis should be carried on.
A coherent program of Parity Violation DIS precision measurements, with well defined kinematics over a broad Q2 and x range would provide access to search charge asymmetry violation at partonic level, to measure d(x)/u(x) at x close to 1, to study higher twist effects and to probe LHC scale via weak neutral current axial-bector quark coupling [Paschke]. A solenoid spectrometer is expected to be the optimal solution, however, the relatively large MPS and Hall A high luminosity may play an interesting role.
From the different physics talks has clearly emerged the strong impact on JLab physics progam of the MPS equipments and the high luminosity expected for Hall A. Taking this into account and the achievement of the GEP5 experiment, at least three initiatives are in progress: