20 research outputs found
Polarizing a stored proton beam by spin flip?
We discuss polarizing a proton beam in a storage ring, either by selective
removal or by spin flip of the stored ions. Prompted by recent, conflicting
calculations, we have carried out a measurement of the spin flip cross section
in low-energy electron-proton scattering. The experiment uses the cooling
electron beam at COSY as an electron target. The measured cross sections are
too small for making spin flip a viable tool in polarizing a stored beam. This
invalidates a recent proposal to use co-moving polarized positrons to polarize
a stored antiproton beam.Comment: 18 pages, 6 figure
Measurement of the Spin-Dependence of the pbar-p Interaction at the AD-Ring
We propose to use an internal polarized hydrogen storage cell gas target in
the AD ring to determine for the first time the two total spin-dependent pbar-p
cross sections sigma_1 and sigma_2 at antiproton beam energies in the range
from 50 to 450 MeV. The data obtained are of interest by themselves for the
general theory of pbar-p interactions since they will provide a first
experimental constraint of the spin-spin dependence of the nucleon-antinucleon
potential in the energy range of interest. In addition, measurements of the
polarization buildup of stored antiprotons are required to define the optimum
parameters of a future, dedicated Antiproton Polarizer Ring (APR), intended to
feed a double-polarized asymmetric pbar-p collider with polarized antiprotons.
Such a machine has recently been proposed by the PAX collaboration for the new
Facility for Antiproton and Ion Research (FAIR) at GSI in Darmstadt, Germany.
The availability of an intense stored beam of polarized antiprotons will
provide access to a wealth of single- and double-spin observables, thereby
opening a new window on QCD spin physics.Comment: 51 pages, 23 figures, proposal submitted to the SPS committee of CER
Measurement of the Spin–Dependence of the Interaction at the AD–Ring
We propose to use an internal polarized hydrogen storage cell gas target in the AD ring to determine for the first time the two total spin–dependent pbar-p cross sections σ1 and σ2 at antiproton beam energies in the range from 50 to 450 MeV. The data obtained are of interest by themselves for the general theory of pbar-p interactions since they will provide a first experimental constraint of the spin–spin dependence of the nucleon–antinucleon potential in the energy range of interest. In addition, measurements of the polarization buildup of stored antiprotons are required to define the optimum parameters of a future, dedicated Antiproton Polarizer Ring (APR), intended to feed a double–polarized asymmetric pbar-p collider with polarized antiprotons. Such a machine has recently been proposed by the PAX collaboration for the new Facility for Antiproton and Ion Research (FAIR) at GSI in Darmstadt, Germany. The availability of an intense stored beam of polarized antiprotons will provide access to a wealth of single– and double–spin observables, thereby opening a new window on QCD spin physics. A recent experiment at COSY revealed that ep spin–flip cross sections are too small to cause a detectable depolarization of a stored proton beam. This measurement rules out a proposal to use polarized positrons to polarize an antiproton beam by e+pbar spin–flip interactions. Thus, our approach to provide a beam of polarized antiprotons is based on spin filtering, using an internal polarized hydrogen gas target – a method that has been tested with stored protons. We expect to produce a polarized antiproton beam with at least ten orders of magnitude higher intensity than a secondary polarized antiproton beam previously available. Provided that antiproton beams with a polarization of about 15% can be obtained with the APR, the antiproton machine at FAIR (the High Energy Storage Ring) could be converted into a double–polarized asymmetric pbar-p collider by installation of an additional COSY–like ring. In this setup, antiprotons of 3.5 GeV/c collide with protons of 15 GeV/c at c.m. energies of √s ≈ √200 GeV with a luminosity in excess of 10^31 cm−2s−1. The PAX physics program proposed for FAIR has been highly rated, and would include, most importantly, a first direct measurement of the transversity distribution of the valence quarks in the proton, and a first measurement of the moduli and the relative phase of the time–like electric and magnetic form factors G_E,M of the proton.We propose to use an internal polarized hydrogen storage cell gas target in the AD ring to determine for the first time the two total spin-dependent pbar-p cross sections sigma_1 and sigma_2 at antiproton beam energies in the range from 50 to 450 MeV. The data obtained are of interest by themselves for the general theory of pbar-p interactions since they will provide a first experimental constraint of the spin-spin dependence of the nucleon-antinucleon potential in the energy range of interest. In addition, measurements of the polarization buildup of stored antiprotons are required to define the optimum parameters of a future, dedicated Antiproton Polarizer Ring (APR), intended to feed a double-polarized asymmetric pbar-p collider with polarized antiprotons. Such a machine has recently been proposed by the PAX collaboration for the new Facility for Antiproton and Ion Research (FAIR) at GSI in Darmstadt, Germany. The availability of an intense stored beam of polarized antiprotons will provide access to a wealth of single- and double-spin observables, thereby opening a new window on QCD spin physics
Measurement of Spin Observables in the ~p ~d Breakup Reaction
We update our Letter-of-Intent 202 for Measurement of Spin Observables in the
~p ~d Breakup Reaction. An estimate of the overall beam time needed for completing
the measurements is specied and a timeline in view of the planned PAX experiments
is presented.
The proposal aims at a study of the three nucleon continuum in proton deuteron
breakup reactions, between 30 and 50 MeV proton beam energies, an energy range
where there have been few and limited measurements. The large coverage of the PAX
detection setup and the energy range chosen will provide essential new data intended
as a laboratory for chiral eective eld theory, the modern theory for nuclear forces
relevant at low and intermediate energies.
Vector and tensor analyzing powers and spin correlation coecients will be measured
and evaluated over large kinematical areas in the ve parameter phase space of
the nal state containing three nucleons. For the analysis the sampling method will
be used, a technique developed specically for the complex analysis of three particle
nal states, providing a direct comparison between experiment and theory
Spin-Filtering Studies at COSY
We propose to use an internal polarised target in the COSY ring to determine the polarisation
build–up in a proton beam. Spin–filtering experiments at COSY would provide
the necessary data to test our present understanding of spin–filtering processes in storage
rings.
Measurements of the polarisation build–up of stored protons are crucial to progress
towards the PAX goal to eventually produce stored polarised antiproton beams. The
availability of intense stored beams of polarised antiprotons will provide access to a wealth
of single– and double–spin observables, opening a new window on QCD spin physics. It
is planned to realise this experimental programme at the new Facility for Antiproton and
Ion Research (FAIR) at GSI in Darmstadt, Germany.
A recent experiment at COSY revealed that e~p spin–flip cross sections are too small to
cause a detectable depolarisation of a stored proton beam. This measurement rules out a
proposal to use polarised electrons to polarise a proton beam by ~ep spin–flip interactions.
Thus, our approach to provide a beam of polarised protons is based on spin–filtering using
an internal polarised gas target.
In total 22 weeks of beam time are needed to complete the experimental program at
COSY. We now ask for two weeks of beam time for commissioning of the low–β section
and measuring the machine acceptance