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Featured researches published by H. O. Meyer.


Nuclear Physics | 1992

Total cross section for p+p→p+p+π0 close to threshold

H. O. Meyer; C. J. Horowitz; H. Nann; P. V. Pancella; S. F. Pate; R.E. Pollock; B. von Przewoski; T. Rinckel; M. A. Ross; F. Sperisen

Abstract Making use of an electron-cooled beam in the IUCF storage ring, we have measured the total cross section σ tot for pp→pp π 0 at 31 bombarding energies between 285 and 325 MeV. At a level of about 5%, the data show no fluctuations that could be associated with the onset of other pion production channels. A calculation of the single-partial-wave cross section σ ss , including direct production only (no rescattering), falls short of the experiment by a factor of 5.2±0.3, but reproduces the observed energy dependence when scaled. This energy dependence is explained by contributions from the phase-space factor and the final-state interaction between the outgoing nucleons. The relative importance of higher partial waves is deduced from the energy dependence of σ tot as well as from the angular distributions of reaction protons.


Physical Review C | 2006

Analyzing powers and spin correlation coefficients for p+d elastic scattering at 135 and 200 MeV

B. v. Przewoski; H. O. Meyer; J.T. Balewski; W. W. Daehnick; J. Doskow; W. Haeberli; R. Ibald; B. Lorentz; R.E. Pollock; P. V. Pancella; F. Rathmann; T. Rinckel; Swapan K. Saha; B. Schwartz; Pia Thörngren-Engblom; A. Wellinghausen; Tom Jack Whitaker; T. Wise

The proton and deuteron analyzing powers and ten of the possible 12 spin correlation coefficients have been measured for p+d elastic scattering at proton bombarding energies of 135 and 200 MeV. The results are compared with Faddeev calculations using two different NN potentials. The qualitative features of the extensive data set on the spin dependence in p+d elastic scattering over a wide range of angles presented here are remarkably well explained by two-nucleon force predictions without inclusion of a three-nucleon force. The remaining discrepancies are, in general, not alleviated when theoretical three-nucleon forces are included in the calculations.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993

Test of a windowless storage cell target in a proton storage ring

M.A. Ross; W.K. Pitts; W. Haeberli; H. O. Meyer; S. F. Pate; R.E. Pollock; B. von Przewoski; T. Rinckel; J. Sowinski; F. Sperisen; P. V. Pancella

Abstract Stored ion beams offer the possibility to use polarized internal targets that consist of a source of polarized atoms in conjunction with a long, narrow, windowless target cell to enhance the target thickness. In this paper, we discuss the effect of such a cell on the performance of the storage ring, based on measurements carried out with the Indiana Cooler. A prototype target cell was constructed and was operated with a controlled flow of H 2 target gas in a beam of stored protons. Detection of protons scattered at angles from 4° to 15° in coincidence with the associated recoil particles was used to identify elastic scattering. The results show that the presence of a 25 cm long target cell with a rectangular opening of 6.4 mm by 7.9 mm is compatible with operation of the Cooler ring. This demonstrates the feasibility of an important component of experiments with stored, polarized beams and carrier-free polarized, internal targets.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994

Performance of a polarized-hydrogen storage cell target

M.A. Ross; A.D. Roberts; T. Wise; W. Haeberli; W.A. Dezarn; J. Doskow; H. O. Meyer; R.E. Pollock; B. v. Przewoski; T. Rinckel; F. Sperisen; P. V. Pancella

Abstract A storage cell has been constructed for use as an internal polarized gas target in the storage ring at the Indiana University Cyclotron Facility. The storage cell has thin teflon walls which allow for detection of low energy recoil particles. We report on nuclear polarization measurements of hydrogen atoms, produced by an atomic beam source, in this storage cell. The results indicate that a target polarization in excess of 0.70 is achieved. We discuss the design and construction details of a storage cell target and the polarization results which are based on low-energy pp spin correlation measurements using the University of Wisconsin tandem accelerator.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995

Polarized internal gas target for hydrogen and deuterium at the IUCF Cooler Ring

W.A. Dezarn; J. Doskow; J.G. Hardie; H. O. Meyer; R.E. Pollock; B. von Przewoski; T. Rinckel; F. Sperisen; W. Haeberli; B. Lorentz; F. Rathmann; M.A. Ross; T. Wise; P. V. Pancella

Abstract A polarized internal gas target has been constructed and used at the IUCF Cooler Ring. Polarized hydrogen atoms produced by a high-intensity atomic beam source are injected into a target cell whose Teflon walls are thin enough to allow low-energy recoil particles to be detected in coincidence with forward scattered particles. An average proton target polarization of 0.740±0.013 has been measured.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993

Interaction of stored, cooled proton beams with fiber targets

B. v. Przewoski; H. O. Meyer; W.R. Lozowski; S. F. Pate; R.E. Pollock; T. Rinckel; P. Schwandt; F. Sperisen; W.A. Dezarn; P. Heimberg; P. V. Pancella

Abstract The use of thin fibers as internal targets for nuclear physics experiments in storage rings is discussed. We have measured the lifetime and the energy spread of stored, electron-cooled beams in the presence of an internal carbon fiber target. Measurements have been carried out in the Indiana Cooler with proton beams between 100 MeV and 300 MeV. The effect of the inhomogeneous fiber target on the beam is the same as that of a homogeneous gas target of equivalent thickness within the accuracy of the measurement. The measurements are compared with a Monte Carlo simulation of the stored beam. It is demonstrated that charging of the fiber target can significantly affect the lifetime and energy spread of the stored beam.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993

Beam loss rates with an internal gas target in an electron-cooled storage ring Implications for luminosity optimization

R.E. Pollock; Vladimir P. Derenchuk; X. Pei; T. Sloan; F. Sperisen; H. O. Meyer; B. v. Przewoski; T. Rinckel; P. V. Pancella; M.A. Ross; W. K. Pitts

Measurements have been made in the Cooler ring at the Indiana University Cyclotron Facility (IUCF) of the mean lifetime of stored and electron-cooled proton beams in the presence of various target gas species at two ring locations differing in dispersion. A broad range of beam energy Tb, target atomic number Zt and thickness xt was employed. The loss (removal) cross sectionσL per target atom, extracted from the lifetime measurement, exhibits a minimum for small xt which is found to scale with (ZtTb)2. This behavior is expected because forward Coulomb scattering from target nuclei should be the dominant loss mechanism under the conditions of measurement. A marked increase in σL for larger xt is attributed to emittance growth arising from multiple scattering in competition with the transverse cooling rate. Lattice dispersion at the target increases the contribution to beam heating by electrons in the target atoms and introduces an additional loss mechanism. From the measured σL and beam lifetime, a time cycle may be selected which gives the optimum time-averaged luminosity for a given experiment. Scaling of σL allows prediction of the optimum luminosity over the full operating regime of the cooling ring.


Physical Review C | 2001

Spin correlations in

W. W. Daehnick; Swapan K. Saha; R. W. Flammang; H. O. Meyer; J.T. Balewski; R.E. Pollock; B. von Przewoski; T. Rinckel; P. Thörngren-Engblom; A. Wellinghausen; B. Lorentz; F. Rathmann; B. Schwartz; T. Wise; P. V. Pancella

A first measurement of longitudinal as well as transverse spin correlation coefficients for the reaction


Physica Scripta | 1993

\vec{p}\vec{p}\to pn\pi^{+}

H. Rohdjeß; H. O. Meyer; P. V. Pancella; S. F. Pate; M A Pickar; R.E. Pollock; B. v. Przewoski; T. Rinckel; W. Scobel; P P Singh; F. Sperisen; L Sprute

vec{p}vec{p}to pnpi^+


SPIN 2002: 15th International Spin Physics Symposium and Workshop on Polarized Electron Sources and Polarimeters | 2003

pion production near threshold

V. S. Morozov; M. Q. Crawford; Z. B. Etienne; M. C. Kandes; A. D. Krisch; M. A. Leonova; D. W. Sivers; V. K. Wong; K. Yonehara; V. A. Anferov; H. O. Meyer; P. Schwandt; Edward J. Stephenson; B. von Przewoski

was made using a polarized proton target and a polarized proton beam. We report kinematically complete measurements for this reaction at 325, 350, 375 and 400 MeV beam energy. The spin correlation coefficients

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S. F. Pate

New Mexico State University

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W. Haeberli

University of Wisconsin-Madison

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T. Wise

University of Wisconsin-Madison

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