M. Bychkov
University of Virginia
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Featured researches published by M. Bychkov.
Physical Review Letters | 2004
D. Pocanic; S. M. Korenchenko; A. S. Korenchenko; L. C. Smith; V. V. Sidorkin; H.P. Wirtz; W. Li; Y. Wang; B. G. Ritchie; V. Baranov; E. Frlez; T. Kozlowski; J.F. Crawford; N. P. Kravchuk; R. Minehart; Wilhelm Bertl; S. Ritt; B.A. VanDevender; N. A. Kuchinsky; A.M. Rozhdestvensky; M. Daum; D. Mzhavia; K. O. H. Ziock; M. Bychkov; I. Supek; Ch. Brönnimann; N. V. Khomutov; Z. Tsamalaidze
Using a large acceptance calorimeter and a stopped pion beam we have made a precise measurement of the rare pi(+)-->pi(0)e(+)nu (pi(beta)) decay branching ratio. We have evaluated the branching ratio by normalizing the number of observed pi(beta) decays to the number of observed pi(+)-->e(+)nu (pi(e2)) decays. We find the value of Gamma(pi(+)-->pi(0)e(+)nu)/Gamma(total)=[1.036+/-0.004(stat)+/-0.004(syst)+/-0.003(pi(e2))]x10(-8), where the first uncertainty is statistical, the second systematic, and the third is the pi(e2) branching ratio uncertainty. Our result agrees well with the standard model prediction.
Physical Review Letters | 2004
E. Frlež; D. Pocanic; V. Baranov; W. Bertl; M. Bychkov; N. V. Khomutov; A. S. Korenchenko; S. M. Korenchenko; T. Kozlowski; N. P. Kravchuk; N. A. Kuchinsky; Wenhui Li; R. Minehart; D. Mzhavia; B. G. Ritchie; S. Ritt; A. M. Rozhdestvensky; V. V. Sidorkin; L. C. Smith; I. Supek; Zviad Tsamalaidze; B.A. VanDevender; E. P. Velicheva; Yanchu Wang; H.-P. Wirtz; K. O. H. Ziock
We have studied radiative pion decays pi(+)-->e(+)nugamma in three broad kinematic regions using the PIBETA detector and a stopped pion beam. Based on Dalitz distributions of 41 601 events we have evaluated absolute pi-->enugamma branching ratios in the three regions. Minimum chi(2) fits to the integral and differential (E(e(+)),E(gamma)) distributions result in the axial-to-vector weak form factor ratio of gamma identical with F(A)/F(V)=0.443(15), or F(A)=0.0115(4) with F(V)=0.0259. However, deviations from standard model predictions in the high-E(gamma)-low-E(e(+)) kinematic region indicate the need for further theoretical and experimental work.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009
D. Pocanic; R. Alarcon; L.P. Alonzi; S. Baeßler; S. Balascuta; J. D. Bowman; M. Bychkov; J. Byrne; J. R. Calarco; V. Cianciolo; C. Crawford; E. Frlež; M. T. Gericke; G. L. Greene; R. Grzywacz; Vladimir Gudkov; F. W. Hersman; Andreas Klein; J. Martin; S. A. Page; A. Palladino; S. I. Penttilä; K. Rykaczewski; W. S. Wilburn; A. R. Young; G. R. Young
The Nab collaboration will perform a precise measurement of a, the electron-neutrino correlation parameter, and b, the Fierz interference term in neutron beta decay, in the Fundamental Neutron Physics Beamline at the SNS, using a novel electric/magnetic field spectrometer and detector design. The experiment is aiming at the 10{sup -3} accuracy level in {Delta}a/a, and will provide an independent measurement of {lambda} = G{sub A}/G{sub V}, the ratio of axial-vector to vector coupling constants of the nucleon. Nab also plans to perform the first ever measurement of b in neutron decay, which will provide an independent limit on the tensor weak coupling.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2004
E. Frlež; D. Pocanic; K. Assamagan; Yu. Sh. Bagaturia; V. Baranov; W. Bertl; Ch. Brönnimann; M. Bychkov; J.F. Crawford; M. Daum; Th. Flügel; R. Frosch; Roland Horisberger; V. Kalinnikov; V. Karpukhin; N. V. Khomutov; Jason Edwin Koglin; A. S. Korenchenko; S. M. Korenchenko; T. Kozlowski; B. Krause; N. P. Kravchuk; N. A. Kuchinsky; W. Li; David Wayne Lawrence; R. Minehart; D. Mzhavia; H. Obermeier; D. Renker; B. G. Ritchie
Abstract We describe the design, construction and performance of the PIBETA detector built for the precise measurement of the branching ratio of pion beta decay, π + →π 0 e + ν e , at the Paul Scherrer Institute. The central part of the detector is a 240-module spherical pure CsI calorimeter covering ∼3 π sr solid angle. The calorimeter is supplemented with an active collimator/beam degrader system, an active segmented plastic target, a pair of low-mass cylindrical wire chambers and a 20-element cylindrical plastic scintillator hodoscope. The whole detector system is housed inside a temperature-controlled lead brick enclosure, which in turn is lined with cosmic muon plastic veto counters. Commissioning and calibration data were taken during two 3-month beam periods in 1999/2000 with π + stopping rates between 1.3·10 3 π + / s and 1.3·10 6 π + / s . We examine the timing, energy and angular detector resolution for photons, positrons and protons in the energy range of 5– 150 MeV , as well as the response of the detector to cosmic muons. We illustrate the detector signatures for the assorted rare pion and muon decays and their associated backgrounds.
Physical Review Letters | 2008
M. Bychkov; D. Počanić; B. Vandevender; V. Baranov; W. Bertl; Yu. M. Bystritsky; E. Frlež; V. A. Kalinnikov; N. V. Khomutov; A. S. Korenchenko; S. M. Korenchenko; M. Korolija; T. Kozlowski; N. P. Kravchuk; N. A. Kuchinsky; W. Li; D. Mekterovic; D. Mzhavia; S. Ritt; P. Robmann; O. A. Rondon-Aramayo; A. M. Rozhdestvensky; T. Sakhelashvili; S. Scheu; U. Straumann; I. Supek; Z. Tsamalaidze; A. van der Schaaf; E. P. Velicheva; V. P. Volnykh
We have measured the pi+-->e+ nugamma branching ratio over a wide region of phase space, based on a total of 65 460 events acquired using the PIBETA detector. Minimum-chi2 fits to the measured (E(e+), E(gamma) energy distributions result in the weak form factor value of F(A)=0.0119(1) with a fixed value of F(V)=0.0259. An unconstrained fit yields F(V)=0.0258(17) and F(A)=0.0117(17). In addition, we have measured a=0.10(6) for the dependence of F(V) on q2, the e+ nu pair invariant mass squared, parametrized as F(V)(q2)=F(V)(0)(1+aq(2)). The branching ratio for the kinematic region E(gamma)>10 MeV and theta(e(+)gamma)>40 degrees is measured to be B(expt)=73.86(54)x10(-8). Earlier deviations we reported in the high-E(gamma)-low-E(e+) kinematic region are resolved without a tensor term. We also derive new values for the pion polarizability alpha(E)=2.78(10)x10(-4) fm3 and neutral pion lifetime tau(pi0)=(8.5+/-1.1)x10(-17) s.
Physical Review Letters | 2009
E. Frlež; L. P. Alonzi; V. Baranov; W. Bertl; M. Bychkov; Yu. M. Bystritsky; N. V. Khomutov; A. S. Korenchenko; S. M. Korenchenko; M. Korolija; T. Kozlowski; N. P. Kravchuk; N. A. Kuchinsky; D. Mekterovic; D. Mzhavia; A. Palladino; D. Pocanic; P. Robmann; A. M. Rozhdestvensky; V. V. Sidorkin; U. Straumann; I. Supek; P. Truöl; A. van der Schaaf; E. P. Velicheva; V. V. Volnykh
The PEN Collaboration is conducting a new measurement of the π+ → e + vL branching ratio at the Paul Scherrer Institute, with the goal uncertainty of δB/B πe2 = 5 × 10−4 or lower. At present, the combined accuracy of all published πe2 decay measurements lags behind the theoretical calculation by a factor of 40. In this contribution we report on the PEN detector configuration and its performance during two development runs done in 2007 and 2008.
Physical Review Letters | 2009
M. Bychkov; D. Počanić; B. Vandevender; V. Baranov; W. Bertl; Yu. M. Bystritsky; E. Frlez; V. A. Kalinnikov; N. V. Khomutov; A. S. Korenchenko; S. M. Korenchenko; M. Korolija; T. Kozlowski; N. P. Kravchuk; N. A. Kuchinsky; W. Li; D. Mekterovic; D. Mzhavia; S. Ritt; P. Robmann; O. A. Rondon-Aramayo; A. M. Rozhdestvensky; T. Sakhelashvili; S. Scheu; U. Straumann; I. Supek; Z. Tsamalaidze; A. van der Schaaf; E. P. Velicheva; V. P. Volnykh
We have measured the pi+-->e+ nugamma branching ratio over a wide region of phase space, based on a total of 65 460 events acquired using the PIBETA detector. Minimum-chi2 fits to the measured (E(e+), E(gamma) energy distributions result in the weak form factor value of F(A)=0.0119(1) with a fixed value of F(V)=0.0259. An unconstrained fit yields F(V)=0.0258(17) and F(A)=0.0117(17). In addition, we have measured a=0.10(6) for the dependence of F(V) on q2, the e+ nu pair invariant mass squared, parametrized as F(V)(q2)=F(V)(0)(1+aq(2)). The branching ratio for the kinematic region E(gamma)>10 MeV and theta(e(+)gamma)>40 degrees is measured to be B(expt)=73.86(54)x10(-8). Earlier deviations we reported in the high-E(gamma)-low-E(e+) kinematic region are resolved without a tensor term. We also derive new values for the pion polarizability alpha(E)=2.78(10)x10(-4) fm3 and neutral pion lifetime tau(pi0)=(8.5+/-1.1)x10(-17) s.
arXiv: Nuclear Experiment | 2014
D. Počanić; E. Munyangabe; M. Bychkov; L. P. Alonzi; V. Baranov; W. Bertl; Yu. M. Bystritsky; E. Frlež; V. A. Kalinnikov; N. V. Khomutov; A. S. Korenchenko; S. M. Korenchenko; M. Korolija; T. Kozlowski; N. P. Kravchuk; N. A. Kuchinsky; M. C. Lehman; D. Mekterovic; D. Mzhavia; A. Palladino; P. Robmann; A. M. Rozhdestvensky; I. Supek; P. Truöl; Z. Tsamalaidze; A. van der Schaaf; B. Vandevender; E. P. Velicheva; V. P. Volnykh
Simple dynamics, few available decay channels, and highly controlled radiative and loop corrections, make pion and muon decays a sensitive means of exploring details of the underlying symmetries. We review the current status of the rare decays: π+ → e+ν (πe2), π+ → e+νγ (πe2γ), π+ → π0e+ν (πe3), and
arXiv: High Energy Physics - Experiment | 2013
D. Počanić; A. Palladino; L. P. Alonzi; V. Baranov; W. Bertl; M. Bychkov; Yu. M. Bystritsky; E. Frlež; V. A. Kalinnikov; N. V. Khomutov; A. S. Korenchenko; S. M. Korenchenko; M. Korolija; T. Kozlowski; N. P. Kravchuk; N. A. Kuchinsky; M. C. Lehman; D. Mekterovic; E. Munyangabe; D. Mzhavia; P. Robmann; A. M. Rozhdestvensky; S. N. Shkarovskiy; U. Straumann; I. Supek; P. Truöl; Z. Tsamalaidze; A. van der Schaaf; E. P. Velicheva; V. P. Volnykh
\mu^+ \to e^+\nu \bar{\nu}\gamma
11TH CONFERENCE ON THE INTERSECTIONS OF PARTICLE AND NUCLEAR PHYSICS: (CIPANP 2012) | 2013
S. Baeßler; R. Alarcon; L.P. Alonzi; S. Balascuta; L. Barrón-Palos; J. D. Bowman; M. Bychkov; J. Byrne; J. R. Calarco; T. Chupp; T. V. Cianciolo; C. Crawford; E. Frlež; M. T. Gericke; F. Glück; G. L. Greene; R. Grzywacz; Vladimir Gudkov; D. Harrison; F. W. Hersman; T. Ito; M. Makela; J. Martin; P. L. McGaughey; S. McGovern; S. A. Page; S. I. Penttilä; D. Pocanic; K. Rykaczewski; A. Salas-Bacci
. For the latter we report new preliminary values for the branching ratio B(Eγ > 10 MeV, θeγ > 30°) = 4.365 (9)stat (42)syst × 10-3, and the decay parameter