Emission of polarized photons from unpolarized electrons moving in crystals

Radiation emitted by unpolarized high-energy electrons penetrating crystals may be linearly polarized. This occurs when the particle velocity makes an angle, with respect to some major crystal axis, being sufficiently larger than the axial-channelling angle. For such orientation, a complete description of spectral and polarization characteristics of the radiation is derived. At planar channelling, a non-perturbative contribution to the probability of the process appears caused by the plane field, and we must solve exactly a one~-~dimensional mechanical problem. For that, the approximate form of the actual plane potential is suggested which provides a precise fit for any crystal plane and an analytical solution to the motion problem. In a practical case, we must consider electron-photon showers developing in sufficiently thick crystals. For the first time, this development is described taking into account the polarization of photons. We discuss qualitative features of the phenomenon, present results of numerical calculations for thin and thick crystals, and evaluate the possibility of the use of differently oriented crystals in a polarized hard photon source.Comment: 16 pages, 7 PostScript figure

Polarization effects in non-relativistic epep scattering

The cross section which addresses the spin-flip transitions of a proton (antiproton) interacting with a polarized non-relativistic electron or positron is calculated analytically. In the case of attraction, this cross section is greatly enhanced for sufficiently small relative velocities as compared to the result obtained in the Born approximation. However, it is still very small, so that the beam polarization time turns out to be enormously large for the parameters of $e^{\pm}$ beams available now. This practically rules out a use of such beams to polarize stored antiprotons or protons.Comment: 9 pages; version accepted for publication in Nucl.Instr.Methods B where cross sections without averaging over directions of relative velocities are adde

Spin effects in ppˉp\bar p interaction and their possible use to polarize antiproton beams

Low energy $p\bar p$ interaction is considered taking into account the polarization of both particles. The corresponding cross sections are calculated using the Paris nucleon-antinucleon optical potential. Then they are applied to the analysis of the polarization buildup which is due to the interaction of stored antiprotons with polarized protons of a hydrogen target. It is shown that, at realistic parameters of a storage ring and a target, the filtering mechanism provides a noticeable polarization in a time comparable with the beam lifetime.Comment: 10 pages, 4 figure

On measurement of beam size in linear colliders using beamstrahlung and pair creation

SIGLEAvailable at INIST (FR), Document Supply Service, under shelf-number : RP 10290 / INIST-CNRS - Institut de l'Information Scientifique et TechniqueFRFranc

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