This title appears in the Scientific Report :
2016
Please use the identifier:
http://dx.doi.org/10.1103/PhysRevC.94.035501 in citations.
Please use the identifier: http://hdl.handle.net/2128/12872 in citations.
Polarized proton-deuteron scattering as a test of time-reversal invariance
Polarized proton-deuteron scattering as a test of time-reversal invariance
Scattering of protons with transversal polarization ppy on deuterons with tensor polarization Pxz provides a null-test signal for time-reversal (T) invariance violating but parity (P) conserving effects. We calculate the corresponding null-test observable at beam energies 100–1000MeV within the spin...
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Personal Name(s): | Uzikov, Yu. N. |
---|---|
Haidenbauer, J. (Corresponding author) | |
Contributing Institute: |
Theorie der Starken Wechselwirkung; IAS-4 Theorie der starken Wechselwirkung; IKP-3 |
Published in: | Physical Review C Physical review / C, 94 94 (2016 2016) 3 3, S. 035501 035501 |
Imprint: |
Woodbury, NY
Inst.
2016
2016-09-20 2016-09-01 |
DOI: |
10.1103/PhysRevC.94.035501 |
Document Type: |
Journal Article |
Research Program: |
Condensed Matter and Molecular Building Blocks Computational Science and Mathematical Methods |
Link: |
OpenAccess OpenAccess |
Publikationsportal JuSER |
Please use the identifier: http://hdl.handle.net/2128/12872 in citations.
Scattering of protons with transversal polarization ppy on deuterons with tensor polarization Pxz provides a null-test signal for time-reversal (T) invariance violating but parity (P) conserving effects. We calculate the corresponding null-test observable at beam energies 100–1000MeV within the spin-dependent Glauber theory considering T-violating P-conserving nucleon-nucleon interactions. The S-wave component of the deuteron wave function as well as the D wave are taken into account and the latter is found to play an important role for the magnitude and the energy dependence of the observable in question. Specifically, with inclusion of the D wave the maximum of the obtained signal is shifted to higher beam energies, i.e., to 700–800 MeV. |