S.J. Barish
Carnegie Mellon University
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by S.J. Barish.
Physics Letters B | 1979
M. Derrick; A. Fridman; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel; A. T. Laasanen
Abstract Using new ν p charged-current data from the Fermilab 15 foot hydrogen bubble chamber, some properties of the ν -induced hadronic jets are studied. The angular size of the jets is measured and compared with results from e + e − annihilation. The jets in the two processes are found to be quite similar in terms of the variables sphericity, thrust, and energy flow.
Physics Letters B | 1980
M. Derrick; E. Fernandez; L. Hyman; G. Levman; D. Koetke; B. Musgrave; P. Schreiner; R. Singer; S. Toaff; S.J. Barish; A. Engler; R.W. Kraemer; B.J. Stacey; M. Tabak; R. Ammar; D. Coppage; D. Day; R. Davis; N. Kwak; R. Stump; V. E. Barnes; D.D. Carmony; A. F. Garfinkel; C. Kennedy; G.M. Radecky
Abstract We have measured the excitation function for the neutral current process νn→νpπ− as a function of neutrino energy. Our data give a cross section ratio R=σ(νpπ−)/σ(μ−pπ+)=0.11±0.022 over the energy interval (0.3⩽E ν⩽1.5)GeV. This measurement of single-pion production in a kinematically defined reaction is the first to use a deuterium target. The R value, as well as other characteristics of the data, agrees with the Adler model for single-pion production via the neutral current and gives a value of sin2θw=0.26±0.09.
Physics Letters B | 1980
M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel; A. T. Laasanen
Abstract Using data from the Fermilab 15 ft hydrogen bubble chamber, we have studied inclusive ϱ0 production in antineutrino-proton charged-current interactions. We measure (0.21 ± 0.03) ϱ0/event, corresponding to ϱ0/π−=0.12 ± 0.02. As a function of Q2 and for hadronic masses above a threshold region, the ϱ0/π− ratio shows little variation. At least 50% of the ϱ0s are consistent with coming from the current fragmentation region. The results agree reasonably well with the predictions of the quark fragmentation model of Feynman and field.
Physics Letters B | 1980
M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel; A. T. Laasanen
Abstract The hadronic system produced in charged-current antineutrino interactions is used to study fragmentation of the d-quark. Some problems encountered in defining the current quark fragments are discussed. The properties of the fragmentation function are in good agreement with the expectations of the naive quark-parton model and, in particular, at the present level of statistics we find no need for either a Q 2 -or an x BJ -dependence.
Physics Letters B | 1980
S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel; A. T. Laasanen
Abstract We present data on the reaction ν p → μ + pπ − from an exposure of the Fermilab 15 ft hydrogen bubble chamber. The channel cross section for 5 GeV ν GeV and M( p π − ) GeV is σ = (27 ± 5) × 10 −40 cm 2 . This cross section is dominated by the I = 1 2 production amplitude.
Physical Review D | 1981
G.M. Radecky; V. E. Barnes; D.D. Carmony; A. F. Garfinkel; M. Derrick; E. Fernandez; L. Hyman; G. Levman; D. Koetke; B. Musgrave; P. Schreiner; R. Singer; A. Snyder; S. Toaff; S.J. Barish; A. Engler; R.W. Kraemer; K. Miller; B.J. Stacey; R. Ammar; D. Coppage; D. Day; Robert F. Davis; N. Kwak; R. Stump
Physical Review D | 1982
M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; V. E. Barnes; T.S. Carman; D.D. Carmony; C. Davis; E. Fernandez; A. F. Garfinkel; A. T. Laasanen
Physical Review D | 1982
R. Brock; S.J. Barish; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; V. E. Barnes; T.S. Carman; D.D. Carmony; C. Davis; E. Fernandez; A. F. Garfinkel; A. T. Laasanen
Physical Review Letters | 1979
E. Fernandez; V. E. Barnes; T.S. Carman; D.D. Carmony; C. Davis; A. F. Garfinkel; A. T. Laasanen; M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak
Physical Review D | 1978
M. Derrick; P. Gregory; L. Hyman; K. Jaeger; D. Lissauer; R.J. Miller; B. Musgrave; J. J. Phelan; P. Schreiner; R. Singer; S.J. Barish; A. Engler; G. Keyes; R.W. Kraemer; T. Kikuchi; V. E. Barnes; D.D. Carmony; A. F. Garfinkel; A. T. Laasanen