R. H. Milburn
Tufts University
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Featured researches published by R. H. Milburn.
Physics Letters B | 1999
W. W. M. Allison; G. J. Alner; D. S. Ayres; G. Barr; W. L. Barrett; C. Bode; P. M. Border; C.B. Brooks; J. H. Cobb; R. Cotton; H. Courant; D. M. Demuth; T. Fields; Hugh R. Gallagher; C. Garcia-Garcia; M. C. Goodman; R. Gran; T. Joffe–Minor; T. Kafka; S. M S Kasahara; W. Leeson; P. J. Litchfield; N. P. Longley; W. A. Mann; M. L. Marshak; R. H. Milburn; W. H. Miller; L. Mualem; A. Napier; W. P. Oliver
Abstract We report a measurement of the atmospheric neutrino flavor ratio, R, using a sample of quasi-elastic neutrino interactions occurring in an iron medium. The flavor ratio (tracks/showers) of atmospheric neutrinos in a 3.9 fiducial kiloton-year exposure of Soudan 2 is 0.64±0.11(stat.)±0.06(syst.) of that expected. Important aspects of our main analysis have been checked by carrying out two independent, alternative analyses; one is based upon automated scanning, the other uses a multivariate approach for background subtraction. Similar results are found by all three approaches.
Physics Letters B | 1997
W. W. M. Allison; G. J. Alner; D. S. Ayres; W. L. Barrett; C. Bode; P. M. Border; C.B. Brooks; J. H. Cobb; D. J. A. Cockerill; R. Cotton; H. Courant; D. M. Demuth; T. Fields; Hugh R. Gallagher; C. Garcia-Garcia; M. C. Goodman; R.N. Gray; K. Johns; T. Kafka; S. M S Kasahara; W. Leeson; P. J. Litchfield; N. P. Longley; M. Lowe; W. A. Mann; M. L. Marshak; Edward May; R. H. Milburn; W. H. Miller; L. Mualem
Abstract The atmospheric neutrino flavour ratio measured using a 1.52 kton-year exposure of Soudan 2 is found to be 0.72 ± 0.19−0.07+0.05 relative to the expected value from a Monte Carlo calculation. The possible background of interactions of neutrons and photons produced in muon interactions in the rock surrounding the detector has been investigated and is shown not to produce low values of the ratio.
Physical Review Letters | 2002
E.M. Aitala; A. J. Slaughter; A.K.S. Santha; L.P. Perera; H.S. Carvalho; S. Devmal; G. Herrera; H. A. Rubin; N. W. Reay; S. MayTal-Beck; E. Wolin; A. Napier; S. Banerjee; S. Watanabe; A. Fernandez; J. Magnin; P.A. Kasper; G.F. Fox; R. H. Milburn; B. Quinn; A.M. Halling; D. A. Sanders; B. Lundberg; A. C. dos Reis; S. Takach; K. Thorne; S. Radeztsky; S. Amato; J.C. Anjos; D. Mihalcea
We study the Dalitz plot of the decay D^+ -->K^- pi^+ pi^+ with a sample of 15090 events from Fermilab experiment E791. Modeling the decay amplitude as the coherent sum of known K pi resonances and a uniform nonresonant term, we do not obtain an acceptable fit. If we allow the mass and width of the K^*_0(1430) to float, we obtain values consistent with those from PDG but the chi^2 per degree of freedom of the fit is still unsatisfactory. A good fit is found when we allow for the presence of an additional scalar resonance, with mass 797 +/- 19 +/- 43 MeV/c^2 and width 410 +/- 43 +/- 87 MeV/c^2. The mass and width of the K^*_0(1430) become 1459 +/- 7 +/- 5 MeV/c^2 and 175 +/- 12 +/- 12 MeV/c^2, respectively. Our results provide new information on the scalar sector in hadron spectroscopy.
Physical Review D | 2003
Manuel Calderon De La Barca Sanchez; W. W. M. Allison; G. J. Alner; D. S. Ayres; W. L. Barrett; P. M. Border; J. H. Cobb; D. J. A. Cockerill; H. Courant; D. M. Demuth; T. Fields; H. R. Gallagher; M. C. Goodman; T. Joffe-Minor; T. Kafka; S. M. S. Kasahara; P. J. Litchfield; W. A. Mann; M. L. Marshak; R. H. Milburn; W. H. Miller; L. Mualem; J. K. Nelson; A. Napier; W. P. Oliver; G. F. Pearce; E. A. Peterson; D. Petyt; K. Ruddick; J. Schneps
The effects of oscillations of atmospheric muon neutrinos are observed in the 5.90 fiducial kiloton-year exposure of the Soudan 2 detector. An unbinned maximum likelihood analysis of the neutrino L/E distribution has been carried out using the Feldman-Cousins prescription. The probability of the no oscillation hypothesis is 5.8x10-4. The 90% confidence allowed region in the sin**(2theta), Delta m**2 plane is presented.
Physical Review Letters | 2001
E.M. Aitala; A.K.S. Santha; L.P. Perera; H.S. Carvalho; S. Devmal; G. Herrera; H. A. Rubin; N. W. Reay; S. MayTal-Beck; E. Wolin; A. Napier; S. Banerjee; S. Watanabe; A. Fernandez; P.A. Kasper; G.F. Fox; B. Quinn; A. C. dos Reis; A.M. Halling; D. A. Sanders; B. Lundberg; S. Takach; S. Radeztsky; S. Amato; J.C. Anjos; D. Mihalcea; D. J. Summers; K. Stenson; T. Carter; S. Kwan
We have studied the diffractive dissociation into dijets of 500 GeV/c pions scattering coherently from carbon and platinum targets. Extrapolating to asymptotically high energies (where t(min)-->0), we find that when the per-nucleus cross section for this process is parametrized as sigma = sigma0Aalpha, alpha has values near 1.6, the exact result depending on jet transverse momentum. These values are in agreement with those predicted by theoretical calculations of color-transparency.
Physics Letters B | 1996
E.M. Aitala; S. Amato; J.C. Anjos; J. A. Appel; D. Ashery; Swagato Banerjee; I. Bediaga; G. Blaylock; Stephen B. Bracker; P. R. Burchat; R.A. Burnstein; T. Carter; H.S. Carvalho; N. Copty; L. Cremaldi; C. Darling; K. Denisenko; A. Fernandez; P. Gagnon; C. Gobel; K. Gounder; A.M. Halling; G. Herrera; G. Hurvits; C. James; P.A. Kasper; S. Kwan; D.C. Langs; J. Leslie; B. Lundberg
Abstract We present measurements of the production of Ds− mesons relative to Ds+ mesons as functions of xF and of pt2 for a sample of 2445 Ds decays to φπ. The Ds mesons were produced in Fermilab experiment E791 with 500 GeV/c π− mesons incident on one platinum and four carbon foil targets. The acceptance-corrected integrated asymmetry in the xF range −0.1 to 0.5 for Ds± mesons is 0.032 ± 0.022 ± 0.022, consistent with no net asymmetry. We compare the results as functions of xF and pt2 to predictions and to the large production asymmetry observed for D± mesons in the same experiment. These comparisons support the hypothesis that production asymmetries come from the fragmentation process and not from the charm quark production itself.
Physical Review Letters | 1994
G.A. Alves; D. R. Green; C. Darling; Roger L. Dixon; M.E. Streetman; M. Souza; D. Passmore; A. Napier; Z. Wu; T. Bernard; A. C. dos Reis; J. Astorga; L. Lueking; Robert Jedicke; W. J. Spalding; A. Rafatian; S. Amato; J. C. Anjos; D. J. Summers; S. Kwan; A. Wallace; Stephen B. Bracker; J. A. Appel; S. F. Takach; A. Santoro; R. H. Milburn; L. Cremaldi; D. Errede; J. M. De Miranda; P. E. Karchin
A leading charm meson is one with longitudinal momentum fraction, [ital x][sub [ital F]][gt]0, whose light quark (or antiquark) is of the same type as one of the quarks in the beam particles. We report on the production asymmetry, [ital A]=[[sigma](leading[minus][sigma](nonleading)]/[[sigma](leading)+[sigma](nonleading)] as a function of [ital x][sub [ital F]]. The data consist of 1500 fully reconstructed [ital D][sup [plus minus]] and [ital D][sup *[plus minus]] decays in Fermilab experiment E 769. We find a significant asymmetry for the production of charm quarks is not expected in perturbative quantum chromodynamics.
Physical Review Letters | 1999
S. Amato; J.C. Anjos; I. Bediaga; H.S. Carvalho; C. Gobel; J. R. T. de Mello Neto; J. M. De Miranda; A. C. dos Reis; A.F.S. Santoro; J. Solano; P. Gagnon; J. Leslie; K. O'Shaughnessy; B. T. Meadows; A.B. d'Oliveira; L.P. Perera; A.K.S. Santha; A. J. Schwartz; Sokoloff; G. Herrera; J. A. Appel; S. Banerjee; T. Carter; K. Denisenko; A.M. Halling; C. James; S. Kwan; B. Lundberg; R. Stefanski; K. Thorne
Using the large hadroproduced charm sample collected in experiment E791 at Fermilab, we report the first directly measured constraint on the decay-width difference Delta Gamma for the mass eigenstates of the D0-D0bar system. We obtain our result from lifetime measurements of the decays D0 -->K-pi+ and D0 -->K-K+, under the assumption of CP invariance, which implies that the CP eigenstates and the mass eigenstates are the same. The lifetime of D0 -->K-K+ (the CP-even final state is \tau_KK = 0.410 +/- 0.011 +/- 0.006 ps, and the lifetime of D0 -->K-pi+ (an equal mixture of CP-odd and CP-even final states is tau_Kpi = 0.413 +/- 0.003 +/- 0.004 ps. The decay-width difference is Delta Gamma = 2(Gamma_KK - Gamma_Kpi) = 0.04 +/- 0.14 +/- 0.05 ps^-1. We relate these measurements to measurements of mixing in the neutral D-meson system.
Physical Review D | 2002
J. Chung; J. L. Thron; A. Sousa; B. Speakman; W. P. Oliver; W. W. M. Allison; A. Napier; R. H. Milburn; P. M. Border; W. H. Miller; T. Joffe-Minor; G. J. Alner; H. R. Gallagher; J. Schneps; R. Gran; P. J. Litchfield; D. Petyt; M. L. Marshak; D. S. Ayres; W. L. Barrett; D. M. Demuth; N. West; W. A. Mann; M. C. Goodman; Manuel Calderon De La Barca Sanchez; L. Mualem; K. Ruddick; E. A. Peterson; S. M. S. Kasahara; J. H. Cobb
We have searched for neutron-antineutron oscillations using the 5.56 fiducial kiloton-year exposure of the Soudan 2 iron tracking calorimeter. We require candidate n-nbar occurrences to have .GE. 4 prongs (tracks and showers) and to have kinematics compatible with nbar-N annihilation within a nucleus. We observe five candidate events, with an estimated background from atmospheric neutrino and cosmic ray induced events of 4.5 \pm 1.2 events. Previous experiments with smaller exposures observed no candidates, with estimated background rates similar to this experiment. We set a lifetime lower limit for oscillation time in iron: T_A(Fe) > 7.2x10^{31} years. The corresponding lower limit for oscillation of free neutrons is \tau_{n-nbar} > 1.3x10^8 seconds.
Physical Review Letters | 1996
E.M. Aitala; A.K.S. Santha; L.P. Perera; H.S. Carvalho; G. Herrera; H. A. Rubin; N. W. Reay; S. MayTal-Beck; E. Wolin; A. Napier; S. Banerjee; S. Watanabe; A. Fernandez; P.A. Kasper; K. Stenson; B. Quinn; K. Sugano; A. C. dos Reis; A.M. Halling; B. Lundberg; S. Takach; K. Thorne; S. Radeztsky; S. Amato; J.C. Anjos; D. J. Summers; T. Carter; S. Kwan; M. V. Purohit; A.K. Tripathi
We report the result of a search for D0 - D0_bar mixing in the data from hadroproduction experiment E791 at Fermilab. We use the D* tag and semileptonic decay vertices of D0 to look for wrong-sign decays with mixing time dependence.