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Featured researches published by B. Reitz.


Physics Letters B | 2002

Direct evidence for an orbital magnetic quadrupole twist mode in nuclei

B. Reitz; A. M. van den Berg; D. Frekers; F. Hofmann; M. de Huu; Y. Kalmykov; H. Lenske; P. von Neumann-Cosel; V. Yu. Ponomarev; S. Rakers; A. Richter; G. Schrieder; K. Schweda; J. Wambach; H.J. Wörtche

The reactions Ni-58(e, e) and M-58(p, p) have been studied at kinematics favorable for the excitation of J(pi) = 2(-) states by isovector spin-flip transitions with DeltaL = 1. There are states at an excitation energy E-X approximate to 10 MeV which are strongly excited in electron scattering but not in proton scattering, suggesting a predominantly orbital character. This is taken as direct evidence for the so-called twist mode in nuclei in which different layers of nuclear fluid in the upper and lower hemisphere counterrotate against each other. Microscopic quasiparticle-phonon model calculations which predict sizable orbital M2 strength at this excitation energy yield indeed a current flow pattern of the strongest transitions consistent with a twist-like motion


IEEE Transactions on Nuclear Science | 2000

Performance of an ASD-8 based wire chamber readout system

Bam Krusemann; R. Bassini; C. Bäumer; A. M. van den Berg; N. Dressnandt; D. Frekers; M. Hagemann; V. Hannen; R. Henderson; J. Heyse; E. Jacobs; M. A. de Huu; M Mielke; M. Newcomer; S. Rakers; B. Reitz; H Sohlbach; H.J. Wörtche

For the medium-energy proton polarimeter mounted at the focal-plane of the Big-Bite Spectrometer at Kernfysisch Versneller Instituut Groningen, a new wire-chamber readout has been developed. The charge-sensitive preamplifier is based on the ASD-8 B chip which has an input impedance of 115 /spl Omega/. This low impedance and the short integration time of 6 ns at a usable sensitivity of 5 fC allow high readout rates and low gas amplifications. This front-end circuit is mounted on all four multi-wire proportional chambers and on two vertical-drift chambers with 3872 wires in total. Measurements have been made using sources and intermediate energy protons. Special attention was given to determine the time-over-threshold properties of the circuit. The time-over-threshold capabilities of the readout system extend future applications to particle discrimination, or, in connection with other detector types, to energy-resolving readout. The operational performance of the readout system is presented.


Physical Review Letters | 2005

The Q{sup 2}-Dependence of the Neutron Spin Structure Function g{sub 2}{sup n} at Low Q{sup 2}

K. Kramer; D.S. Armstrong; T. Averett; W. Bertozzi; S. Binet; C. Butuceanu; A. Camsonne; Gordon D. Cates; Jian-Ping Chen; Seonho Choi; E. Chudakov; F. Cusanno; A. Deur; P. Djawotho; D. Dutta; John M. Finn; H. Gao; F. Garibaldi; O. Gayou; R. Gilman; O. Glamazdin; V. Gorbenko; K. A. Griffioen; J.-O. Hansen; D. W. Higinbotham; W. Hinton; T. Horn; Cornelis De Jager; Xiaodong Jiang; W. Korsch

We present the first measurement of the Q2 dependence of the neutron spin structure function g2(n) at five kinematic points covering 0.57 (GeV/c)2 < or = Q2 < or = 1.34 (GeV/c)2 at x approximately = 0.2. Though the naive quark-parton model predicts g2 = 0, nonzero values occur in more realistic models of the nucleon which include quark-gluon correlations, finite quark masses, or orbital angular momentum. When scattering from a noninteracting quark, g2(n) can be predicted using next-to-leading order fits to world data for g1(n). Deviations from this prediction provide an opportunity to examine QCD dynamics in nucleon structure. Our results show a positive deviation from this prediction at lower Q2, indicating that contributions such as quark-gluon interactions may be important. Precision data obtained for g1(n) are consistent with next-to-leading order fits to world data.


Nuclear Physics | 1999

Electric and magnetic giant resonances studied with electron scattering at the S-DALINAC*

P. von Neumann-Cosel; C. Bähr; F. Hofmann; F. Neumeyer; Shigeru Nishizaki; V. Yu. Ponomarev; C. Rangacharyulu; B. Reitz; A. Richter; G. Schrieder; K. Schweda; A. Stascheck; Steffen Strauch; T. Waindzoch; J. Wambach

Recent examples of giant resonance spectroscopy with electron scattering at the S-DALINAC are presented. Strength distributions and decay properties of electric resonances in 48 Ca are investigated with the (e,e′n) reaction. First results of a systematic search for spin and orbital magnetic quadrupole modes in 180° scattering are presented for 48 Ca and 90 Zr.


Physical Review Letters | 1999

Spin and orbital magnetic quadrupole resonances in 48Ca and 90Zr from 180° electron scattering

P. von Neumann-Cosel; F. Neumeyer; Shigeru Nishizaki; V. Yu. Ponomarev; C. Rangacharyulu; B. Reitz; A. Richter; G. Schrieder; D. I. Sober; T. Waindzoch; J. Wambach


Physical Review Letters | 1999

l-Forbidden M1 transition in 32S: a test of tensor corrections to the magnetic dipole operator

B. Reitz; F. Hofmann; P. von Neumann-Cosel; F. Neumeyer; C. Rangacharyulu; A. Richter; G. Schrieder; D. I. Sober; B. A. Brown


Physical Review C | 2002

Magnetic dipole transitions in 32 S from electron scattering at 180

F. Hofmann; P. von Neumann-Cosel; F. Neumeyer; C. Rangacharyulu; B. Reitz; A. Richter; G. Schrieder; D. I. Sober; L.W. Fagg; B. A. Brown


Physics Letters B | 2005

Polarized proton scattering on 58Ni at small momentum transfer: A test of the microscopic optical model and effective interactions

F. Hofmann; C. Bäumer; A. M. van den Berg; D. Frekers; V. Hannen; M.N. Harakeh; M. A. de Huu; Y. Kalmykov; P. von Neumann-Cosel; V. Yu. Ponomarev; S. Rakers; B. Reitz; A. Richter; A. Shevchenko; K. Schweda; J. Wambach; H.J. Wörtche


Physical Review C | 2000

Transverse electron scattering form factors at low momentum transfer: sensitivity to in-medium modifications of vector mesons?

P. von Neumann-Cosel; F. Neumeyer; B. Reitz; A. Richter; J. Wambach


Nuclear Physics | 2001

Decomposition of M1 transitions into isoscalar and isovector, spin and orbital contributions

Y. Fujita; T. Adachi; G.P.A. Berg; H. Ejiri; H. Fujimura; H. Fujita; M. Fujiwara; K. Hara; Mohsen Harakeh; K. Hatanaka; F. Hofmann; J. Kamiya; K. Katori; T. Kawabata; S. Mizutori; P. von Neumann-Cosel; T. Noro; B. Reitz; A. Richter; Y. Shimbara; T. Shinada; H. Ueno; M. Yoshifuku; M. Yosoi

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A. Richter

Technische Universität Darmstadt

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F. Hofmann

Technische Universität Darmstadt

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P. von Neumann-Cosel

Technische Universität Darmstadt

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J. Wambach

Technische Universität Darmstadt

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G. Schrieder

Technische Universität Darmstadt

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Y. Kalmykov

Technische Universität Darmstadt

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K. Schweda

Technische Universität Darmstadt

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F. Neumeyer

Technische Universität Darmstadt

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V. Yu. Ponomarev

Technische Universität Darmstadt

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