H. Schmieden
University of Bonn
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Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1998
K. I. Blomqvist; Werner U. Boeglin; R. Böhm; M. O. Distler; R. Edelhoff; J. Friedrich; R. Geiges; P. Jennewein; M. Kahrau; M. Korn; H. Kramer; K.W. Krygier; V. Kunde; A. Liesenfeld; H. Merkel; K. Merle; U. Müller; R. Neuhausen; E. A. J. M. Offermann; Th. Pospischil; A.W. Richter; G. Rosner; P. Sauer; S. Schardt; H. Schmieden; A. Wagner; Th. Walcher; S. Wolf
Abstract A set-up of three high-resolution magnetic spectrometers, for simplicity named A, B and C, has been built as the central facility for the precise determination of double and triple coincidence cross sections of hadron knock-out and meson production through the scattering of electrons at the Mainz microtron MAMI. The spectrometers A and C with point-to-point optics in the dispersive plane and parallel-to-point optics in the non-dispersive plane have a solid angle of 28 msr and a momentum acceptance of 20 and 25%, respectively. They each consist of a quadrupole, a sextupole and two dipole magnets, reaching maximum momenta of 735 and 550 MeV/c, respectively. The spectrometer B has a solid angle of 5.6 msr and a somewhat reduced momentum acceptance of 15%, but it reaches a maximum momentum larger than that of the MAMI electron beam (855 MeV/c). It consists of a single-clamshell dipole magnet with point-to-point optics in both planes. Each spectrometer is equipped with a position-sensitive detector system consisting of four planes of vertical drift chambers, two planes of plastic scintillators and a threshold gas Cherenkov detector. The operational experiences demonstrate that all three spectrometers exceed the specifications. Selected results of double (e, e′ x ) and triple (e, e′ x 1 x 2 ) coincidence experiments, x 1 and x 2 standing for charged hadrons, are presented, which demonstrate the performance of the whole set-up.
Physical Review Letters | 2008
I. Jaegle; T. Mertens; A. V. Anisovich; J. C. S. Bacelar; B. Bantes; O. Bartholomy; D. Bayadilov; R. Beck; Y. A. Beloglazov; R. Castelijns; V. Crede; H. Dutz; A. Ehmanns; D. Elsner; K. Essig; R. Ewald; I. Fabry; M. Fuchs; Ch. Funke; R. W. Gothe; R. Gregor; A. Gridnev; E. Gutz; S. Hoeffgen; P. Hoffmeister; I. Horn; J. Junkersfeld; H. Kalinowsky; S. Kammer; V. Kleber
Quasifree photoproduction of eta mesons off nucleons bound in the deuteron has been measured with the CBELSA/TAPS detector for incident photon energies up to 2.5 GeV at the Bonn ELSA accelerator. The eta mesons have been detected in coincidence with recoil protons and recoil neutrons, which allows a detailed comparison of the quasifree n(gamma,eta)n and p(gamma,eta)p reactions. The excitation function for eta production off the neutron shows a pronounced bumplike structure at W=1.68 GeV (E{gamma} approximately 1 GeV), which is absent for the proton.
Physical Review Letters | 2008
I. Jaegle; T. Mertens; A. V. Anisovich; J. C. S. Bacelar; B. Bantes; O. Bartholomy; D. Bayadilov; R. Beck; Y. A. Beloglazov; R. Castelijns; V. Crede; H. Dutz; A. Ehmanns; D. Elsner; K. Essig; R. Ewald; I. Fabry; M. Fuchs; Ch. Funke; R. W. Gothe; R. Gregor; A. Gridnev; E. Gutz; S. Hoffgen; P. Hoffmeister; I. Horn; J. Junkersfeld; H. Kalinowsky; S. Kammer; V. Kleber
Quasifree photoproduction of eta mesons off nucleons bound in the deuteron has been measured with the CBELSA/TAPS detector for incident photon energies up to 2.5 GeV at the Bonn ELSA accelerator. The eta mesons have been detected in coincidence with recoil protons and recoil neutrons, which allows a detailed comparison of the quasifree n(gamma,eta)n and p(gamma,eta)p reactions. The excitation function for eta production off the neutron shows a pronounced bumplike structure at W=1.68 GeV (E{gamma} approximately 1 GeV), which is absent for the proton.
Physical Review Letters | 2008
M. Kotulla; D. Trnka; P. Muehlich; G. Anton; J. C. S. Bacelar; O. Bartholomy; D. Bayadilov; Y. A. Beloglazov; R. Bogendoerfer; R. Castelijns; V. Crede; H. Dutz; A. Ehmanns; D. Elsner; R. Ewald; I. Fabry; M. Fuchs; K. Essig; Ch. Funke; R. W. Gothe; R. Gregor; A. Gridnev; E. Gutz; S. Hoeffgen; P. Hoffmeister; I. Horn; J. Hoessl; I. Jaegle; J. Junkersfeld; H. Kalinowsky
Information on hadron properties in the nuclear medium has been derived from the photoproduction of omega mesons on the nuclei C, Ca, Nb, and Pb using the Crystal Barrel/TAPS detector at the ELSA tagged photon facility in Bonn. The dependence of the omega-meson cross section on the nuclear mass number has been compared with three different types of models: a Glauber analysis, a Boltzmann-Uehling-Uhlenbeck analysis of the Giessen theory group, and a calculation by the Valencia theory group. In all three cases, the inelastic omega width is found to be 130-150 MeV/c(2) at normal nuclear matter density for an average 3-momentum of 1.1 GeV/c. In the rest frame of the omega meson, this inelastic omega width corresponds to a reduction of the omega lifetime by a factor approximately 30. For the first time, the momentum dependent omegaN cross section has been extracted from the experiment and is in the range of 70 mb.
European Physical Journal A | 2014
E. Gutz; V. Crede; V. Sokhoyan; H. van Pee; A. V. Anisovich; J. C. S. Bacelar; B. Bantes; O. Bartholomy; D. Bayadilov; R. Beck; Y. A. Beloglazov; R. Castelijns; H. Dutz; D. Elsner; R. Ewald; F. Frommberger; M. Fuchs; Ch. Funke; R. Gregor; A. Gridnev; W. Hillert; P. Hoffmeister; I. Horn; I. Jaegle; J. Junkersfeld; H. Kalinowsky; S. Kammer; V. Kleber; Frank Klein; Friedrich Klein
Photoproduction off protons of the pπ0η three-body final state was studied with the Crystal Barrel/TAPS detector, at the electron stretcher accelerator ELSA in Bonn, for incident energies from the π0η production threshold up to 2.5 GeV. Differential cross sections and the total cross sections are presented. The use of linearly polarized photons gives access to the polarization observables Σ, Is, and Ic, the latter two characterize beam asymmetries in case of three-body final states. Δ(1232)η, N(1535)1/2−π, and pa0(980) are the dominant isobars contributing to the reaction. The partial wave analysis confirms the existence of some nucleon and Δ resonances, for which so far only fair evidence was reported. A large number of decay modes of known nucleon and Δ resonances is presented. It is shown that detailed investigations of decay branching ratios may provide a key to unravelling the structure of nucleon and Δ resonances.
Physical Review Letters | 2005
O. Bartholomy; V. Crede; H. van Pee; A. V. Anisovich; G. Anton; R. Bantes; Y. A. Beloglazov; R. Bogendörfer; R. Castelijns; A. Ehmanns; J. Ernst; I. Fabry; H. Flemming; A. Fosel; H. Freiesleben; M. Fuchs; Ch. Funke; R. W. Gothe; A. Gridnev; E. Gutz; S. Hoffgen; I. Horn; J. Hossl; R. Joosten; J. Junkersfeld; H. Kalinowsky; F. Klein; E. Klempt; H. Koch; M. Konrad
Single pi(0) photoproduction has been studied with the CB-ELSA experiment at Bonn using tagged photon energies between 0.3 and 3.0 GeV. The experimental setup covers a very large solid angle of approximately 98% of 4pi. Differential cross sections dsigma/dOmega have been measured. Complicated structures in the angular distributions indicate a variety of different resonances being produced in the s channel intermediate state gammap-->N(*)(Delta(*))-->ppi(0). A combined analysis including the data presented in this letter along with other data sets reveals contributions from known resonances and evidence for a new resonance N(2070)D15.
Physics Letters B | 2003
J. Bermuth; P. Merle; C. Carasco; D. Baumann; R. Böhm; D. Bosnar; M. Ding; M. O. Distler; J. Friedrich; J. Golak; W. Glöckle; M. Hauger; W. Heil; P. Jennewein; J. Jourdan; H. Kamada; A. Klein; M. Kohl; B. Krusche; K. W. Krygier; H. Merkel; U. Müller; R. Neuhausen; A. Nogga; Ch. Normand; E. W. Otten; Th. Pospischil; M. Potokar; D. Rohe; H. Schmieden
The charge form factor of the neutron has been determined from asymmetries measured in quasi-elastic 3 (He) over right arrow((e) over right arrow, e`n) at a momentum transfer of 0.67 (GeV/c)(2). In addition, the target analyzing power, A(y)(0), has been measured to study effects of final state interactions and meson exchange currents.
European Physical Journal A | 2005
D. I. Glazier; M. Seimetz; J. R. M. Annand; H. Arenhövel; M. Ases Antelo; C. Ayerbe; P. Bartsch; D. Baumann; J. Bermuth; R. Böhm; D. Bosnar; M. Ding; M. O. Distler; D. Elsner; J. Friedrich; S. Hedicke; P. Jennewein; G. Jover Ma nas; F. H. Klein; F. Klein; M. Kohl; K. W. Krygier; K. Livingston; I. J. D. MacGregor; M. Makek; H. Merkel; P. Merle; D. Middleton; U. Müller; R. Neuhausen
Abstract.The electric form factor of the neutron, GE,n, has been measured at the Mainz Microtron by recoil polarimetry in the quasielastic D(¯e, e’¯n)p reaction. Three data points have been extracted at squared four-momentum transfers Q2 = 0.3, 0.6 and 0.8 (GeV/c)2. Corrections for nuclear binding effects have been applied.
Physics Letters B | 2001
S. Dieterich; P. Bartsch; D. Baumann; J. Bermuth; K. Bohinc; R. Böhm; D. Bosnar; S. Derber; M. Ding; M. O. Distler; I. Ewald; J. Friedrich; R. Gilman; C. Glashausser; M. Hauger; P. Jennewein; J. Jourdan; J. J. Kelly; M. Kohl; A. Kozlov; K. W. Krygier; G. Kumbartzki; J. Lac; A. Liesenfeld; H. Merkel; U. Müller; R. Neuhausen; Th. Pospischil; R. D. Ransome; D. Rohe
We have measured the proton recoil polarization in the {sup 4}He(polarized-e, e-prime, p){sup 3}H reaction at Q{sup 2} = 0.5, 1.0, 1.6, and 2.6 (GeV/c){sup 2}. The measured ratio of polarization transfer coefficients differs from a fully relativistic calculation, favoring the inclusion of a predicted medium modification of the proton form factors based on a quark-meson coupling model. In contrast, the measured induced polarizations agree reasonably well with the fully relativistic calculation indicating that the treatment of final-state interactions is under control.
European Physical Journal A | 2007
H. van Pee; O. Bartholomy; V. Crede; A. V. Anisovich; G. Anton; R. Bantes; Yu. A. Beloglazov; R. Bogendörfer; R. Castelijns; A. Ehmanns; J. Ernst; I. Fabry; H. Flemming; A. Fosel; M. Fuchs; Ch. Funke; R. W. Gothe; A. Gridnev; E. Gutz; S. Hoffgen; I. Horn; J. Hößl; J. Junkersfeld; H. Kalinowsky; F. Klein; E. Klempt; H. Koch; M. Konrad; B. Kopf; B. Krusche
Abstract.Photoproduction of π0-mesons was studied with the Crystal-Barrel detector at ELSA for incident energies from 300MeV to 3GeV. Differential cross-sections dσ/dΩ, dσ/dt, and the total cross-section are presented. For Eγ < 3GeV, the angular distributions agree well with the SAID parametrization. At photon energies above 1.5GeV, a strong forward peaking indicates t-channel exchange to be the dominant process. The rapid variations of the cross-section with energy and angle indicate production of resonances. An interpretation of the data within the Bonn-Gatchina partial-wave analysis is briefly discussed.