J. Zejma
Jagiellonian University
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Featured researches published by J. Zejma.
Physical Review D | 2015
J.M. Pendlebury; S. Afach; N. J. Ayres; C. A. Baker; G. Ban; Georg Bison; K. Bodek; Martin Burghoff; P. Geltenbort; K. Green; W. C. Griffith; M. G. D. van der Grinten; Zoran D. Grujić; P. Harris; V. Hélaine; P. Iaydjiev; S.N. Ivanov; M. Kasprzak; Y. Kermaidic; K. Kirch; H.-C. Koch; S. Komposch; A. Kozela; J. Krempel; B. Lauss; T. Lefort; Y. Lemière; D. J. R. May; M. Musgrave; O. Naviliat-Cuncic
We present for the first time a detailed and comprehensive analysis of the experimental results that set the current world sensitivity limit on the magnitude of the electric dipole moment (EDM) of the neutron. We have extended and enhanced our earlier analysis to include recent developments in the understanding of the effects of gravity in depolarizing ultracold neutrons; an improved calculation of the spectrum of the neutrons; and conservative estimates of other possible systematic errors, which are also shown to be consistent with more recent measurements undertaken with the apparatus. We obtain a net result of dn=−0.21±1.82×10−26 e cm, which may be interpreted as a slightly revised upper limit on the magnitude of the EDM of 3.0×10−26 e cm (90% C.L.) or 3.6×10−26 e cm (95% C.L.).
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 Letters | 2009
I. Altarev; C.A. Baker; G. Ban; Georg Bison; K. Bodek; M. Daum; P. Fierlinger; P. Geltenbort; K. Green; M. G. D. van der Grinten; E. Gutsmiedl; P. Harris; W. Heil; R. Henneck; M. Horras; P. Iaydjiev; S.N. Ivanov; N. V. Khomutov; K. Kirch; St. Kistryn; A. Knecht; Paul E. Knowles; A. Kozela; F. Kuchler; M. Kuźniak; T. Lauer; B. Lauss; T. Lefort; A. Mtchedlishvili; O. Naviliat-Cuncic
A clock comparison experiment, analyzing the ratio of spin precession frequencies of stored ultracold neutrons and 199Hg atoms, is reported. No daily variation of this ratio could be found, from which is set an upper limit on the Lorentz invariance violating cosmic anisotropy field b perpendicular < 2 x 10(-20) eV (95% C.L.). This is the first limit for the free neutron. This result is also interpreted as a direct limit on the gravitational dipole moment of the neutron |gn| < 0.3 eV/c2 m from a spin-dependent interaction with the Sun. Analyzing the gravitational interaction with the Earth, based on previous data, yields a more stringent limit |gn| < 3 x 10(-4) eV/c2 m.
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
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 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
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.
Physics Letters B | 2014
S. Afach; C. A. Baker; G. Ban; Georg Bison; K. Bodek; M. Burghoff; Z. Chowdhuri; M. Daum; M. Fertl; B. Franke; P. Geltenbort; K. Green; M. G. D. van der Grinten; Zoran D. Grujić; P. Harris; W. Heil; V. Hélaine; R. Henneck; M. Horras; P. Iaydjiev; S.N. Ivanov; M. Kasprzak; Y. Kermaidic; K. Kirch; A. Knecht; H.-C. Koch; J. Krempel; M. Kuźniak; B. Lauss; T. Lefort
The neutron gyromagnetic ratio has been measured relative to that of the 199Hg atom with an uncertainty of 0.8 ppm. We employed an apparatus where ultracold neutrons and mercury atoms are stored in the same volume and report the result γn/γHg=3.8424574(30).
Journal of Applied Physics | 2014
S. Afach; Georg Bison; K. Bodek; F. Burri; Z. Chowdhuri; M. Daum; M. Fertl; B. Franke; Zoran D. Grujić; V. Hélaine; R. Henneck; M. Kasprzak; K. Kirch; H.-C. Koch; A. Kozela; J. Krempel; B. Lauss; T. Lefort; Y. Lemière; M. Meier; O. Naviliat-Cuncic; F. M. Piegsa; G. Pignol; C. Plonka-Spehr; P. N. Prashanth; G. Quéméner; D. Rebreyend; S. Roccia; P. Schmidt-Wellenburg; A. Schnabel
The Surrounding Field Compensation (SFC) system described in this work is installed around the four-layer Mu-metal magnetic shield of the neutron electric dipole moment spectrometer located at the Paul Scherrer Institute. The SFC system reduces the DC component of the external magnetic field by a factor of about 20. Within a control volume of approximately 2.5m x 2.5m x 3m disturbances of the magnetic field are attenuated by factors of 5 to 50 at a bandwidth from
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
I.C. Barnett; C.P. Bee; K. Bodek; A. Budzanowski; N. Danneberg; P. Eberhardt; W. Fetscher; C. Hilbes; M. Janousch; L. Jarczyk; K. Kirch; St. Kistryn; J. Klement; K. Köhler; A. Kozela; J. Lang; G. Llosa; M. Markiewicz; X. Morelle; O. Naviliat; T. Schweizer; J. Smyrski; J. Sromicki; E. Stephan; A. Strzałkowski; K Szeker; J. Zejma
10^{-3}
Physics Letters B | 2015
S. Afach; G. Ban; Georg Bison; K. Bodek; Martin Burghoff; M. Daum; M. Fertl; B. Franke; Zoran D. Grujić; V. Hélaine; M. Kasprzak; Y. Kermaidic; K. Kirch; Paul E. Knowles; H.-C. Koch; S. Komposch; A. Kozela; J. Krempel; B. Lauss; T. Lefort; Y. Lemière; A. Mtchedlishvili; O. Naviliat-Cuncic; F. M. Piegsa; G. Pignol; P. N. Prashanth; G. Quéméner; D. Rebreyend; D. Ries; S. Roccia
Hz up to 0.5 Hz, which corresponds to integration times longer than several hundreds of seconds and represent the important timescale for the nEDM measurement. These shielding factors apply to random environmental noise from arbitrary sources. This is achieved via a proportional-integral feedback stabilization system that includes a regularized pseudoinverse matrix of proportionality factors which correlates magnetic field changes at all sensor positions to current changes in the SFC coils.