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Featured researches published by R. Poutissou.


Physical Review D | 2009

Study of the decay K+→π+νν̄ in the momentum region 140<Pπ<199MeV/c

A. V. Artamonov; B. Bassalleck; B. Bhuyan; E. W. Blackmore; D. A. Bryman; S. Chen; I-H. Chiang; I.-A. Christidi; P. S. Cooper; M. V. Diwan; J. S. Frank; T. Fujiwara; J. Hu; J. Ives; D. E. Jaffe; S. Kabe; S. H. Kettell; M. Khabibullin; A. Khotjantsev; P. Kitching; M. Kobayashi; T. K. Komatsubara; A. Konaka; A. P. Kozhevnikov; Y. Kudenko; A. Kushnirenko; Leonid G. Landsberg; B. Lewis; K. K. Li; L. S. Littenberg

Experiment E949 at Brookhaven National Laboratory has observed three new events consistent with the decay K+ => pi+,nu,nubar in the pion momentum region 140 pi+,nu,nubar events to seven. Combining this observation with previous results, assuming the pion spectrum predicted by the standard model, results in a branching ratio of (1.73+1.15-1.05)e-10. An interpretation of the results for alternative models of the decay K^ => pi+,nothing is also presented.


Physical Review Letters | 1996

Radiative Muon Capture on Hydrogen and the Induced Pseudoscalar Coupling

G. Jonkmans; S. Ahmad; D.S. Armstrong; G. Azuelos; W. Bertl; M. Blecher; C. Q. Chen; P. Depommier; B. Doyle; T. von Egidy; T. P. Gorringe; P. Gumplinger; M. Hasinoff; D. Healey; A. J. Larabee; J. A. Macdonald; S.C. McDonald; M. Munro; J.-M. Poutissou; R. Poutissou; B. C. Robertson; D. G. Sample; E. Saettler; C. Sigler; Geoffrey Taylor; D. H. Wright; N. S. Zhang

Next to the hydrogen atom, the µ − p system is the most fundamental lepton-hadron system; therefore it can be used to test and extend our basic knowledge of the weak semi-leptonic interaction between leptons and quarks. Radiative muon capture (RMC) is much more sensitive than ordinary muon capture (OMC) to the induced pseudoscalar coupling constant of the weak semi-leptonic current because of the much larger range of momentum transfers which can occur in RMC. A status report on TRIUMF E452, Radiative Muon Capture on Hydrogen, which is anticipating a 10% measurement of this coupling constant, is presented.


Physical Review D | 2015

Search for heavy neutrinos in K+→μ+νH decays

A. V. Artamonov; B. Bassalleck; B. Bhuyan; E. W. Blackmore; D. A. Bryman; S. Chen; I-H. Chiang; I.-A. Christidi; P. S. Cooper; M. V. Diwan; J. S. Frank; T. Fujiwara; J. Hu; J. Ives; A. Izmaylov; D. E. Jaffe; S. Kabe; Steven H. Kettell; M. Khabibullin; A. Khotjantsev; P. Kitching; M. Kobayashi; T. K. Komatsubara; A. Konaka; Y. Kudenko; Leonid G. Landsberg; B. Lewis; K. K. Li; Laurence S. Littenberg; J. A. Macdonald

Evidence of a heavy neutrino, ν H , in the K + → μ + ν H decays was sought using the E949 experimental data with an exposure of 1.70 × 1 0 12 stopped kaons. With the major background from the radiative K + → μ + ν μ γ decay understood and suppressed, upper limits (90%xa0C.L.) on the neutrino mixing matrix element between the muon and heavy neutrinos, | U μ H | 2 , were set at the level of 1 0 - 7 to 1 0 - 9 for the heavy neutrino mass region 175 to 300 MeV / c 2 .


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992

A detector to search for K+ → π+ νν

M. S. Atiya; I-H. Chiang; J.S. Frank; E. Garber; J. S. Haggerty; M. M. Ito; T.F. Kycia; K.K. Li; L. S. Littenberg; C. Ng; I. Polk; R. Rosenka; A.K. Sambamurti; A. Stevens; R.C. Strand; C. Zein; D. S. Akerib; H. Edwards; W.C. Louis; Daniel Marlow; P. D. Meyers; M.A. Selen; F. C. Shoemaker; A. J. S. Smith; S. Ahmad; Ewart W. Blackmore; D. A. Bryman; J.V. Cresswell; L. Felawka; N. Khan

Abstract The detector built for experiment 787 to measure the decay K + → π + ν ν at Brookhaven National Laboratory is describe


Physics Letters B | 2002

Search for the decay in the momentum region Pπ<195 MeV/c

S. S. Adler; Masakazu Aoki; M Ardebili; M. Atiya; A. O. Bazarko; P. C. Bergbusch; B Bhuyan; E. W. Blackmore; D. A. Bryman; I-H. Chiang; M.R. Convery; M. V. Diwan; J. S. Frank; J. S. Haggerty; T. Inagaki; Masaharu Ito; V. Jain; D. E. Jaffe; S. Kabe; M. Kazumori; Steven H. Kettell; P. Kitching; M. Kobayashi; T. K. Komatsubara; A. Konaka; Y. Kuno; M. Kuriki; T. F. Kycia; K. K. Li; Laurence S. Littenberg

Abstract We have searched for the decay K + →π + ν ν in the kinematic region with pion momentum below the K + → π + π 0 peak. One event was observed, consistent with the background estimate of 0.73±0.18. This implies an upper limit on B(K + →π + ν ν ) −9 (90% C.L.), consistent with the recently measured branching ratio of 1.57 +1.75 −0.82 ×10 −10 , obtained using the standard model spectrum and the kinematic region above the K + → π + π 0 peak. The same data were used to search for K + → π + X 0 , where X 0 is a weakly interacting neutral particle or system of particles with 150 M X 0 c 2 .We have searched for the decay


Physical Review Letters | 2008

New measurement of the K+→π+νν̄ branching ratio

A. V. Artamonov; B. Bassalleck; B. Bhuyan; E. W. Blackmore; D. A. Bryman; S. Chen; I-H. Chiang; I.-A. Christidi; P. S. Cooper; M. V. Diwan; J. S. Frank; T. Fujiwara; J. Hu; J. Ives; D. E. Jaffe; S. Kabe; S. H. Kettell; M. Khabibullin; A. Khotjantsev; P. Kitching; M. Kobayashi; T. K. Komatsubara; A. Konaka; A. P. Kozhevnikov; Y. Kudenko; A. Kushnirenko; Leonid G. Landsberg; B. Lewis; K. K. Li; L. S. Littenberg

K^+ to pi^+ nu barnu


Physical Review Letters | 1993

Search for the decay [ital K][sup +][r arrow][pi][sup +][nu][bar [nu]]

Atiya; I-H. Chiang; J. S. Frank; J. S. Haggerty; Masaharu Ito; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Sambamurti; A. Stevens; R. C. Strand; W. C. Louis; D. S. Akerib; D. Marlow; P. D. Meyers; Selen; F. C. Shoemaker; A. J. S. Smith; E. W. Blackmore; D. A. Bryman; L. Felawka; P. Kitching; A. Konaka; Y. Kuno; J. A. Macdonald; Toshio Numao; P. Padley; J.-M. Poutissou; R. Poutissou; J. Roy

in the kinematic region with pion momentum below the


Physical Review Letters | 1997

Observation of the decay K+ → π+ μ+ μ−

P. Kitching; T. Nakano; M. Rozon; R. Soluk; S. S. Adler; M. S. Atiya; I-H. Chiang; J. S. Frank; J. S. Haggerty; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Sambamurti; A. Stevens; R. C. Strand; C. Witzig; W. C. Louis; D. S. Akerib; M. Ardebili; M. R. Convery; Masaharu Ito; D. Marlow; R. A. McPherson; P. D. Meyers; M. A. Selen; F. C. Shoemaker; A. J. S. Smith; E. W. Blackmore; D. A. Bryman; L. Felawka

K^+ to pi^+ pi^0


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997

500-MHz transient digitizers based on GaAs CCDs

D. A. Bryman; M. Constable; J.V. Cresswell; Andrew Daviel; M. LeNoble; J Mildenberger; R. Poutissou

peak. One event was observed, consistent with the background estimate of


Nuclear Physics B - Proceedings Supplements | 2001

TWIST- The TRIUMF weak interaction symmetry test the Michel parameters from μ+ decay

N.L. Rodning; W. Andersson; Y. Davydov; P. Depommier; J. Doornbos; W. Faszer; Carl A. Gagliardi; A. Gaponenko; D.R. Gill; P.W. Green; P. Gumplinger; J.C. Hardy; M. D. Hasinoff; R. Helmer; R. Henderson; P. Kitching; D. D. Koetke; E. Korkmaz; A. Khruchinsky; D. Maas; J. A. Macdonald; R. P. MacDonald; R. Manweiler; G. Marshall; T. Mathie; J. R. Musser; P. Nord; A. Olin; R. Openshaw; D. Ottewell

0.73pm 0.18

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D. A. Bryman

University of British Columbia

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I-H. Chiang

Brookhaven National Laboratory

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J. S. Frank

Brookhaven National Laboratory

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K. K. Li

Brookhaven National Laboratory

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L. S. Littenberg

Brookhaven National Laboratory

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