G. E. Hogan
United States Department of Energy
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Physical Review Letters | 1999
M.L. Brooks; A. Empl; W. von Witsch; X.L. Tu; S.C. Wright; L. A. Van Ausdeln; K. Lan; R. Manweiler; Y. Chen; Kroupa; Cooper; J. J. Szymanski; L. E. Piilonen; C. A. Gagliardi; B. Mayes; K. O. H. Ziock; D. D. Koetke; E.B. Hughes; T. D. S. Stanislaus; G. E. Hogan; R. E. Mischke; J. E. Knott; E. Hungerford; K. M. Stantz; Peter S. Cooper; M. Dzemidzic; C. C. H. Jui; R. E. Tribble
The transport properties of a quasi-three-dimensional, 200 layer quantum well structure are investigated at integer filling in the quantum Hall state. We find that the transverse magnetoresistance R xx , the Hall resistance R xy , and the vertical resistance R zz all follow a similar behavior with both temperature and in-plane magnetic field. A general feature of the influence of increasing in-plane field B in is that the Hall conductance quantization first improves, but above a characteristic value B C in , the quantization is systematically removed. We consider the interplay of the chid edge state transport and the bulk (quantum Hall) transport properties. This mechanism may arise from the competition of the cyclotron energy with the superlattice band structure energies. A comparison of the resuIts with existing theories of the chiral edge state transport with in-plane field is also discussed.An experiment has been performed to search for the muon- and electron-number non-conserving decay mu+ to e+_gamma. The upper limit for the branching ratio to be GAMMA(mu+ to e+_gamma)/GAMMA(mu+ to e+_nu_nubar) < 1.2e-11 with 90% confidence.
Physical Review Letters | 1986
Richard D. Bolton; J. D. Bowman; Cooper; J. S. Frank; A.L. Hallin; P.A. Heusi; C. M. Hoffman; G. E. Hogan; F. G. Mariam; Howard S. Matis; R. E. Mischke; D. E. Nagle; Leo Piilonen; V. Sandberg; Gary H. Sanders; U. Sennhauser; R. Werbeck; Russell A. Williams; S.L. Wilson; R. Hofstadter; E. B. Hughes; M.W. Ritter; D. Grosnick; S.C. Wright; V.L. Highland; J. McDonough
This Letter reports a new experimental search for the family-number-nonconserving decay ..mu../sup +/ ..-->.. e/sup +/..gamma... There is no evidence for the presence of this decay mode. The upper limit for the branching ratio is GAMMA(..mu.. ..-->.. e..gamma..)/GAMMA(..mu.. ..-->.. enu anti nu) < 4.9 x 10/sup -11/ (90% C.L.). 13 refs., 3 figs.
Nuclear Instruments and Methods | 1981
Gary H. Sanders; Gregory W. Hart; G. E. Hogan; J. S. Frank; C. M. Hoffman; Howard S. Matis; V. D. Sandberg
Abstract A high performance, low cost discriminator employing both the leading edge and constant fraction trigger techniques has been developed. This hybrid design provides an experiment with the ultimate in on-line and off-line time resolution. The discriminator has been developed for use with a large modular detector using both NaI(Tl) and plastic scintillators.
Physical Review Letters | 1999
M.L. Brooks; Y. Chen; M. D. Cooper; Peter S. Cooper; M. Dzemidzic; A. Empl; C. A. Gagliardi; G. E. Hogan; E.B. Hughes; E. Hungerford; C. C. H. Jui; J. E. Knott; D. D. Koetke; M. A. Kroupa; K. Lan; R. Manweiler; B. Mayes; R. E. Mischke; L. E. Piilonen; T. D. S. Stanislaus; K. M. Stantz; J. J. Szymanski; R. E. Tribble; X.L. Tu; L. A. Van Ausdeln; W. von Witsch; S.C. Wright; K. O. H. Ziock
The transport properties of a quasi-three-dimensional, 200 layer quantum well structure are investigated at integer filling in the quantum Hall state. We find that the transverse magnetoresistance R xx , the Hall resistance R xy , and the vertical resistance R zz all follow a similar behavior with both temperature and in-plane magnetic field. A general feature of the influence of increasing in-plane field B in is that the Hall conductance quantization first improves, but above a characteristic value B C in , the quantization is systematically removed. We consider the interplay of the chid edge state transport and the bulk (quantum Hall) transport properties. This mechanism may arise from the competition of the cyclotron energy with the superlattice band structure energies. A comparison of the resuIts with existing theories of the chiral edge state transport with in-plane field is also discussed.An experiment has been performed to search for the muon- and electron-number non-conserving decay mu+ to e+_gamma. The upper limit for the branching ratio to be GAMMA(mu+ to e+_gamma)/GAMMA(mu+ to e+_nu_nubar) < 1.2e-11 with 90% confidence.
Intersections between particle and nuclear physics | 1997
Leo Piilonen; J. F. Amann; Richard D. Bolton; Y. Chen; M. D. Cooper; Peter S. Cooper; M. Dzemidzic; W. Foreman; C. A. Gagliardi; D. Haim; R. Harrison; G. Hart; G. E. Hogan; E. Hungerford; C. C. H. Jui; J. E. Knott; D. D. Koetke; T. Kozlowski; M. A. Kroupa; K. Lan; F. S. Lee; F. Liu; R. Manweiler; B. Mayes; R. E. Mischke; C. Pillai; L. Pinsky; S. Schilling; T. D. S. Stanislaus; K. M. Stantz
We report on the status of LAMPF experiment E-1240 to measure the Michel ρ parameter in direct muon decay. This experiment ran in 1993, and the data are currently being analyzed. The expected precision on the ρ parameter is ±0.0008. This result will provide better constraints on new physics, particularly on the charged vector bosons’ mixing angle ζ in the manifestly left-right symmetric extension of the Standard Model.
The 5th conference on the intersections of particle and nuclear physics | 1995
X.L. Tu; J. F. Amann; Richard D. Bolton; Y. Chen; M. D. Cooper; Peter S. Cooper; M. Dzemidzic; W. Foreman; C. A. Gagliardi; D. Haim; R. Harrison; G. Hart; G. E. Hogan; E. Hungerford; C. C. H. Jui; J. E. Knott; D. D. Koetke; T. Kozlowski; M. A. Kroupa; K. Lan; F. Liu; R. Manweiler; B. Mayes; R. E. Mischke; J. N. Otis; L. E. Piilonen; C. Pillai; L. Pinsky; S. Schilling; T. D. S. Stanislaus
A new measurement of the Michel parameter ρ in normal muon decay has been performed using the MEGA positron spectrometer. Over 500 million triggers were recorded and the data are currently being analyzed. The previous result has a precision on the value of ρ±0.0026. The present experiment expects to improve the precision to ±0.0008 or better. The improved result will be a precise test of the standard model of electroweak interactions for a purely leptonic process. It also will provide a better constraint on the WR−WL mixing angle in the left‐right symmetric models.
Physical Review Letters | 1986
C. M. Hoffman; Richard D. Bolton; J. D. Bowman; Cooper; J. S. Frank; P.A. Heusi; A.L. Hallin; G. E. Hogan; F. G. Mariam; Howard S. Matis
This Letter reports a new experimental search for the family-number-nonconserving decay ..mu../sup +/ ..-->.. e/sup +/..gamma... There is no evidence for the presence of this decay mode. The upper limit for the branching ratio is GAMMA(..mu.. ..-->.. e..gamma..)/GAMMA(..mu.. ..-->.. enu anti nu) < 4.9 x 10/sup -11/ (90% C.L.). 13 refs., 3 figs.
Physical Review Letters | 1986
Richard D. Bolton; J. D. Bowman; M. D. Cooper; J. S. Frank; A.L. Hallin; P.A. Heusi; C. M. Hoffman; G. E. Hogan; F. G. Mariam; Howard S. Matis; R. E. Mischke; D. E. Nagle; Leo Piilonen; V. Sandberg; Gary H. Sanders; U. Sennhauser; R. Werbeck; Russell A. Williams; S.L. Wilson; R. Hofstadter; E. B. Hughes; M.W. Ritter; D. Grosnick; S.C. Wright; V.L. Highland; J. McDonough
This Letter reports a new experimental search for the family-number-nonconserving decay ..mu../sup +/ ..-->.. e/sup +/..gamma... There is no evidence for the presence of this decay mode. The upper limit for the branching ratio is GAMMA(..mu.. ..-->.. e..gamma..)/GAMMA(..mu.. ..-->.. enu anti nu) < 4.9 x 10/sup -11/ (90% C.L.). 13 refs., 3 figs.
Physical Review Letters | 1986
Richard D. Bolton; P.A. Heusi; Gary H. Sanders; R. Hofstadter; J. D. Bowman; S.C. Wright; V. Sandberg; Russell A. Williams; A.L. Hallin; R. E. Mischke; J. S. Frank; Cooper; J. McDonough; Leo Piilonen; M.W. Ritter; E. B. Hughes; U. Sennhauser; R. Werbeck; D. Grosnick; G. E. Hogan; Howard S. Matis; C. M. Hoffman; V.L. Highland; D. E. Nagle; S.L. Wilson; F. G. Mariam
This Letter reports a new experimental search for the family-number-nonconserving decay ..mu../sup +/ ..-->.. e/sup +/..gamma... There is no evidence for the presence of this decay mode. The upper limit for the branching ratio is GAMMA(..mu.. ..-->.. e..gamma..)/GAMMA(..mu.. ..-->.. enu anti nu) < 4.9 x 10/sup -11/ (90% C.L.). 13 refs., 3 figs.
Physical Review D | 1988
Richard D. Bolton; P. A. Heusi; Gary H. Sanders; R. Hofstadter; S.C. Wright; V. Sandberg; Russell A. Williams; A. L. Hallin; R. E. Mischke; J. S. Frank; Cooper; J. McDonough; Leo Piilonen; Ritter Mw; E. B. Hughes; U. Sennhauser; R. Werbeck; D. P. Grosnick; G. E. Hogan; Howard S. Matis; C. M. Hoffman; V.L. Highland; Wilson Sl; F. G. Mariam