E. Stephan
University of Silesia in Katowice
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Featured researches published by E. Stephan.
Physical Review C | 2005
S. Kistryn; E. Stephan; A. Biegun; K. Bodek; A. Deltuva; E. Epelbaum; K. Ermisch; W. Glöckle; J. Golak; N. Kalantar-Nayestanaki; H. Kamada; M. Kis; B. Klos; A Kozela; J Kuros-Zolnierczuk; M. Mahjour-Shafiei; Ulf G. Meissner; A. Micherdzińska; A. Nogga; Pieter Sauer; R. Skibiński; R. Sworst; H. Witała; J. Zejma; W. Zipper; J. Kurol-Zolnierczuk; A. Micherdzilska; R. Skibilski; B. Kos
High-precision cross-section data of the deuteron-proton breakup reaction at 130 MeV are presented for 72 kinematically complete configurations. The data cover a large region of the available phase space, divided into a systematic grid of kinematical variables. They are compared with theoretical predictions, in which the full dynamics of the three-nucleon (3N) system is obtained in three different ways: realistic nucleon-nucleon (NN) potentials are combined with model 3N forces (3NFs) or with an effective 3NF resulting from explicit treatment of the Delta-isobar excitation. Alternatively, the chiral perturbation theory approach is used at the next-to-next-to-leading order with all relevant NN and 3N contributions taken into account. The generated dynamics is then applied to calculate cross-section values by rigorous solution of the 3N Faddeev equations. The comparison of the calculated cross sections with the experimental data shows a clear preference for the predictions in which the 3NFs are included. The majority of the experimental data points are well reproduced by the theoretical predictions. The remaining discrepancies are investigated by inspecting cross sections integrated over certain kinematical variables. The procedure of global comparisons leads to establishing regularities in disagreements between the experimental data and the theoretically predicted values of the cross sections. They indicate deficiencies still present in the assumed models of the 3N system dynamics.
Physics Letters B | 2006
St. Kistryn; E. Stephan; B. Kłos; A. Biegun; K. Bodek; I. Ciepał; A. Deltuva; A. C. Fonseca; N. Kalantar-Nayestanaki; M. Kis; A. Kozela; M. Mahjour-Shafiei; A. Micherdzinska; P. U. Sauer; R. Sworst; J. Zejma; W. Zipper
High precision cross-section data of the deuteron–proton breakup reaction at 130 MeV deuteron energy are compared with the theoretical predictions obtained with a coupled-channel extension of the CD Bonn potential with virtual Δ-isobar excitation, without and with inclusion of the long-range Coulomb force. The Coulomb effect is studied on the basis of the cross-section data set, extended in this work to about 1500 data points by including breakup geometries characterized by small polar angles of the two protons. The experimental data clearly prefer predictions obtained with the Coulomb interaction included. The strongest effects are observed in regions in which the relative energy of the two protons is the smallest.
Physical Review C | 2008
A. Ramazani-Moghaddam-Arani; H. R. Amir-Ahmadi; A. D. Bacher; C. D. Bailey; A. Biegun; M. Eslami-Kalantari; I. Gasparic; L. Joulaeizadeh; N. Kalantar-Nayestanaki; St. Kistryn; A. Kozela; H. Mardanpour; Johannes Messchendorp; A. M. Micherdzinska; H. Moeini; S. Shende; E. Stephan; E.J. Stephenson; R. Sworst
Observables in elastic proton-deuteron scattering are sensitive probes of the nucleon-nucleon interaction and three-nucleon force effects. The present experimental database for this reaction is large, but contains a large discrepancy between data sets for the differential cross section taken at 135 MeV/nucleon by two experimental research groups. This article reviews the background of this problem and presents new data taken at Kernfysisch Versneller Instituute (KVI). Differential cross sections and analyzing powers for the
Physical Review Letters | 2003
R. Huber; J. Lang; S. Navert; J. Sromicki; K. Bodek; St. Kistryn; J. Zejma; O. Naviliat-Cuncic; E. Stephan; W. Haeberli
{}^{2}\mathrm{H}(\stackrel{\ensuremath{\rightarrow}}{p},d)p
Physical Review Letters | 2009
A. Kozela; G. Ban; A Bialek; K. Bodek; P Gorel; K. Kirch; St. Kistryn; O. Naviliat-Cuncic; N. Severijns; E. Stephan; J. Zejma
and
Physics Letters B | 2010
H. Mardanpour; H. R. Amir-Ahmadi; R. Benard; A. Biegun; M. Eslami-Kalantari; L. Joulaeizadeh; N. Kalantar-Nayestanaki; M. Kis; St. Kistryn; A. Kozela; H. Kuboki; Y. Maeda; M. Mahjour-Shafiei; J. G. Messchendorp; K. Miki; S. Noji; A. Ramazani-Moghaddam-Arani; Hideyuki Sakai; M. Sasano; K. Sekiguchi; E. Stephan; R. Sworst; Y. Takahashi; K. Yako
{}^{1}\mathrm{H}(\stackrel{\ensuremath{\rightarrow}}{d},d)p
Modern Physics Letters A | 2009
M. Eslami-Kalantari; H. R. Amir-Ahmadi; A. Biegun; I. Gasparic; L. Joulaeizadeh; N. Kalantar-Nayestanaki; St. Kistryn; A. Kozela; H. Mardanpour; J. G. Messchendorp; H. Moeini; A. Ramazani-Moghaddam-Arani; S. Shende; E. Stephan; R. Sworst
reactions at 135 MeV/nucleon and 65 MeV/nucleon, respectively, have been measured. The differential cross-section data differ significantly from previous measurements and consistently follow the energy dependence as expected from an interpolation of published data taken over a large range at intermediate energies.
Nuclear Physics | 2017
P. Adlarson; W. Augustyniak; W. Bardan; M. Bashkanov; F. S. Bergmann; M. Berłowski; H. Bhatt; A. Bondar; M. Büscher; H. Calen; I. Ciepał; H. Clement; E. Czerwiński; K. Demmich; R. Engels; A. Erven; W. Erven; W. Eyrich; P. Fedorets; K. Föhl; K. Fransson; F. Goldenbaum; A. Goswami; K. Grigoryev; C.-O. Gullström; L. Heijkenskjöld; V. Hejny; N. Hüsken; L. Jarczyk; T. Johansson
The transverse polarization of electrons emitted in the beta decay of polarized 8Li nuclei has been measured. For the time-reversal violating triple correlation parameter we find R=(0.9+/-2.2)x10(-3). This result is in agreement with the standard model and yields improved constraints on exotic tensor contributions to the weak interaction. Combined with other experimental results and using a model for the coupling constants, a new limit for the mass of a possible scalar leptoquark, m(LQ)>560 GeV/c(2) (90% C.L.), is obtained.
Physical Review C | 2016
P. Adlarson; B. Kamys; K. Grigoryev; H. Clement; S. Kistryn; N. Hüsken; W. Augustyniak; J. Zlomanczuk; F. S. Bergmann; T. Skorodko; V. Serdyuk; H. Calen; P. Wurm; V. Hejny; M. Berłowski; G. Khatri; A. Zink; R. Stassen; B. Shwartz; B. Mariański; O. Rundel; B. Kłos; R. Varma; R. Siudak; G. Kemmerling; K. Pysz; U. Wiedner; W. Erven; M. Mikirtychiants; B. Lorentz
Both components of the transverse polarization of electrons (sigmaT1, sigmaT2) emitted in the beta-decay of polarized, free neutrons have been measured. The T-odd, P-odd correlation coefficient quantifying sigmaT2, perpendicular to the neutron polarization and electron momentum, was found to be R=0.008+/-0.015+/-0.005. This value is consistent with time reversal invariance and significantly improves limits on the relative strength of imaginary scalar couplings in the weak interaction. The value obtained for the correlation coefficient associated with sigmaT1, N=0.056+/-0.011+/-0.005, agrees with the Standard Model expectation, providing an important sensitivity test of the experimental setup.
European Physical Journal A | 2016
P. Adlarson; W. Augustyniak; W. Bardan; M. Bashkanov; F. S. Bergmann; M. Berłowski; H. Bhatt; A. Bondar; M. Büscher; H. Calen; I. Ciepa; H. Clement; E. Czerwiński; K. Demmich; R. Engels; A. Erven; W. Erven; W. Eyrich; P. Fedorets; K. Foehl; K. Fransson; F. Goldenbaum; A. Goswami; K. Grigoryev; C.-O. Gullström; L. Heijkenskjöld; V. Hejny; N. Huesken; L. Jarczyk; Tord Johansson
Abstract Precision data are presented for the break-up reaction, H 2 ( p → , p p ) n , within the framework of nuclear-force studies. The experiment was carried out at KVI using a polarized-proton beam of 190 MeV impinging on a liquid-deuterium target and by exploiting the detector, BINA. Some of the vector-analyzing powers are presented and compared with state-of-the-art Faddeev calculations including three-nucleon forces effect. Significant discrepancies between the data and theoretical predictions were observed for kinematical configurations which correspond to the H 2 ( p → , He 2 ) n channel. These results are compared to the H 2 ( p → , d ) p reaction to test the isospin sensitivity of the present three-nucleon force models. The current modeling of two and three-nucleon forces is not sufficient to describe consistently polarization data for both isospin states.