B. Lundberg
Fermilab
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Featured researches published by B. Lundberg.
Physics Letters B | 2001
K. Kodama; N. Ushida; C. Andreopoulos; N. Saoulidou; G. Tzanakos; P. M. Yager; B. Baller; D. J. Boehnlein; Walter Freeman; B. Lundberg; J. Morfin; R. Rameika; J. C. Yun; J.S. Song; C.S. Yoon; S.H. Chung; P. Berghaus; M. Kubantsev; Neville W. Reay; R. A. Sidwell; N.R. Stanton; S. Yoshida; S. Aoki; T. Hara; J. T. Rhee; D. P. Ciampa; C. Erickson; M. Graham; K. Heller; R. Rusack
Abstract The DONUT experiment has analyzed 203 neutrino interactions recorded in nuclear emulsion targets. A decay search has found evidence of four tau neutrino interactions with an estimated background of 0.34 events. This number is consistent with the Standard Model expectation.The DONUT experiment has analyzed 203 neutrino interactions recorded in nuclear emulsion targets. A decay search has found evidence of four tau neutrino interactions with an estimated background of 0.34 events. This number is consistent with the Standard Model expectation.
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.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
K. Kodama; N. Saoulidou; G. Tzanakos; B. Baller; B. Lundberg; R. Rameika; J.S. Song; C.S. Yoon; S.H. Chung; S. Aoki; T. Hara; C. Erickson; K. Heller; R. Schwienhorst; J. Sielaff; J. Trammell; K. Hoshino; H. Jiko; J. Kawada; T Kawai; M. Komatsu; H Matsuoka; M. Miyanishi; M Nakamura; T. Nakano; K. Narita; K. Niwa; N. Nonaka; K. Okada; O. Sato
Abstract The DONUT experiment used an emulsion/counter-hybrid-detector, which succeeded in detecting tau–neutrino charged-current interactions. A new method of emulsion analysis, NETSCAN, was used to locate neutrino events and detect tau decays. It is based on a fully automated emulsion readout system (Ultra Track Selector) developed at Nagoya University. The achieved plate-to-plate alignment accuracy of ∼0.2 μm over an area of 2.6 mm ×2.6 mm permitted an efficient and systematic tau decay search using emulsion data. Moreover, this accuracy allowed measurement of particle momenta by multiple Coulomb scattering, and contributed to the efficient background rejection for the ν τ candidates. This paper describes details of our emulsion analysis methods.
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 | 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.
Physics Letters B | 2001
R. Schwienhorst; D. P. Ciampa; C. Erickson; M. Graham; K. Heller; R. Rusack; J. Sielaff; J. Trammell; J. Wilcox; K. Kodama; N. Ushida; C. Andreopoulos; N. Saoulidou; G. Tzanakos; P. M. Yager; B. Baller; D. J. Boehnlein; Walter Freeman; B. Lundberg; J. Morfin; R. Rameika; J. C. Yun; J.S. Song; C.S. Yoon; S.H. Chung; P. Berghaus; M. Kubantsev; Neville W. Reay; R. A. Sidwell; N.R. Stanton
Abstract Using a neutrino beam in which a ντ component was identified for the first time, the ντ magnetic moment was measured based on a search for an anomalous increase in the number of neutrino–electron interactions. One such event was observed when 2.3 were expected from background processes, giving an upper 90% confidence limit on μντ of 3.9×10−7μB.Using a prompt neutrino beam in which a nu_tau component was identified for the first time, the nu_tau magnetic moment was measured based on a search for an anomalous increase in the number of neutrino-electron interactions. One such event was observed when 2.3 were expected from background processes, giving an upper 90% confidence limit of 3.9x10^-7 Bohr magnetons.
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.
Physics Letters B | 1999
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; S. Devmal; A. Fernandez; G.F. Fox; P. Gagnon; C. Gobel; K. Gounder; A.M. Halling; G. Herrera; G. Hurvits; C. James; P.A. Kasper; S. Kwan; D.C. Langs
Abstract We report the results of a search for flavor-changing neutral current, lepton-flavor violating, and lepton-number violating decays of D + , D s + , and D 0 mesons (and their antiparticles) into modes containing muons and electrons. Using data from Fermilab charm hadroproduction experiment E791, we examine the π ll and K ll decay modes of D + and D s + and the l + l − decay modes of D 0 . No evidence for any of these decays is found. Therefore, we present branching-fraction upper limits at 90% confidence level for the 24 decay modes examined. Eight of these modes have no previously reported limits, and fourteen are reported with significant improvements over previously published results.
Physics Letters B | 1997
E.M. Aitala; S. Amato; J.C. Anjos; J. A. Appel; Daniel 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 report results of a search for CP violation in the singly Cabibbo-suppressed decays D + → K − K + π + , φπ + , K ∗ (892) 0 K + , and π − π + π + based on data from the charm hadroproduction experiment E791 at Fermilab. We search for a difference in the D + and D − decay rates for each of the final states. No evidence for a difference is seen. The decay rate asymmetry parameters ( A CP ), defined as the difference in the D + and D − decay rates divided by the sum of the decay rates, are measured to be: A CP ( KKπ ) = −0.014±0.029, A CP ( φπ ) = −0.028±0.036, A CP (K ∗ (892)K) = −0.010±0.050 and A CP ( πππ ) = −0.017±0.042.We report results of a search for CP violation in the singly Cabibbosuppressed decays D → KKπ, φπ, K(892)0K+, and πππ based on data from the charm hadroproduction experiment E791 at Fermilab. We search for a difference in the D and D decay rates for each of the final states. No evidence for a difference is seen. The decay rate asymmetry parameters (ACP ), defined as the difference in the D + and D decay rates divided by the sum of the decay rates, are measured to be: ACP (KKπ) = −0.014 ± 0.029, ACP (φπ) = −0.028 ± 0.036, ACP (K(892)K) = −0.010 ± 0.050, and ACP (πππ) = −0.017 ± 0.042. PACS numbers: 11.30.Er, 12.15.Ji, 13.25.Ft, 14.40.Lb Typeset using REVTEX