Georg Bison
Paul Scherrer Institute
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Featured researches published by Georg Bison.
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.).
Journal of The Optical Society of America B-optical Physics | 2005
Georg Bison; Robert Wynands; Antoine Weis
Cardiomagnetometry is a growing field of noninvasive medical diagnostics that has triggered a need for affordable high-sensitivity magnetometers. Optical pumping magnetometers (OPMs) are promising candidates for satisfying that need since it has been demonstrated that they can be used to map the magnetic field of the beating human heart. We discuss the principle of a phase-detecting OPM and describe the procedures used to optimize its performance. The optimized OPM has an intrinsic magnetometric sensitivity of 63 fT/Hz^1/2 and a measurement bandwidth of 140 Hz with a spatial resolution of 28 mm, measured in a weakly shielded environment. We further discuss the fundamental limitations of frequency- and phase-detecting magnetometers on the basis of information theory.
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.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009
I. Altarev; G. Ban; Georg Bison; K. Bodek; Martin Burghoff; Milan Cvijovic; M. Daum; P. Fierlinger; E. Gutsmiedl; Gabriele Hampel; W. Heil; R. Henneck; M. Horras; N. V. Khomutov; K. Kirch; St. Kistryn; S. Knappe-Grüneberg; A. Knecht; Paul E. Knowles; A. Kozela; J. V. Kratz; F. Kuchler; M. Kuźniak; T. Lauer; B. Lauss; T. Lefort; A. Mtchedlishvili; O. Naviliat-Cuncic; S. Paul; A. S. Pazgalev
The effort towards a new measurement of the neutron electric dipole moment (nEDM) at the Paul Scherrer Instituts (PSI) new high intensity source of ultracold neutrons (UCN) is described. The experimental technique relies on Ramseys method of separated oscillatory fields, using UCN in vacuum with the apparatus at ambient temperature. In the first phase, R&D towards the upgrade of the RAL/Sussex/ILL apparatus is being performed at the Institut Laue-Langevin (ILL). In the second phase the apparatus, moved from ILL to PSI, will allow an improvement in experimental sensitivity by a factor of 5. In the third phase, a new spectrometer should gain another order of magnitude in sensitivity. The improvements will be mainly due to (1) much higher UCN intensity, (2) improved magnetometry and magnetic field control, and (3) a double chamber configuration with opposite electric field directions.
Physical Review A | 2006
Antoine Weis; Georg Bison; A. S. Pazgalev
We present a theoretical study of the spectra produced by optical\char21{}radio-frequency double resonance devices, in which resonant linearly polarized light is used in the optical pumping and detection processes. We extend previous work by presenting algebraic results which are valid for atomic states with arbitrary angular momenta, arbitrary rf intensities, and arbitrary geometries. The only restriction made is the assumption of low light intensity. The results are discussed in view of their use in optical magnetometers.
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).
Physical Review A | 2006
Gianni Di Domenico; Georg Bison; Stephan Groeger; Paul E. Knowles; A. S. Pazgalev; Martin Rebetez; H. Saudan; Antoine Weis
We present an experimental study of the spectra produced by optical-radio-frequency double resonance in which resonant linearly polarized laser light is used in the optical pumping and detection processes. We show that the experimental spectra obtained for cesium are in excellent agreement with a very general theoretical model developed in our group [Weis, Bison, and Pazgalev, Phys. Rev. A 74, 033401 (2006)] and we investigate the limitations of this model. Finally, the results are discussed in view of their use in the study of relaxation processes in aligned alkali-metal vapors.
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
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
10^{-3}
European Physical Journal D | 2015
H.-C. Koch; Georg Bison; Zoran D. Grujić; W. Heil; M. Kasprzak; Paul E. Knowles; A. Kraft; A. S. Pazgalev; A. Schnabel; Jens Voigt; Antoine Weis
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.