A. R. Erwin
University of Wisconsin-Madison
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Featured researches published by A. R. Erwin.
Physics Letters B | 1988
J. Adams; A. Alavi-Harati; I. F. M. Albuquerque; T. Alexopoulos; Michael Wayne Arenton; K. Arisaka; S. Averitte; A. Barker; L. Bellantoni; A. Bellavance; J. Belz; R. Ben-David; D. R. Bergman; E. Blucher; G. J. Bock; C. Bown; S. Bright; E. Cheu; S. Childress; R. Coleman; M. Corcoran; G. Corti; B. Cox; M. Crisler; A. R. Erwin; Simon J. Field; R. Ford; G. Graham; J. Graham; K. Hagan
Abstract Data collected in Fermilab experiment E731 was used to perform the first search for the decay K L →π 0 ν ν . This decay is dominated by short distance effects and is almost entirely direct CP violating within the standard model. Cuts were developed to reject the background processes Λ→nπ0 and KL→π+e−γν. No candidate events were seen. We find BR (K L →π 0 ν ν ) −4 at the 90% confidence level.We report on a search for the rare decay K_L -> pi^0 nu nubar in the KTeV experiment at Fermilab. We searched for two-photon events whose kinematics were consistent with an isolated pi^0 coming from the decay K_L -> pi^0 nu nubar. One candidate event was observed, which was consistent with the expected level of background. An upper limit on the branching ratio was determined to be B(K_L -> pi^0 nu nubar) < 1.6E-6 at the 90% confidence level.We report on a search for the rare decay K_L -> pi^0 nu nubar in the KTeV experiment at Fermilab. We searched for two-photon events whose kinematics were consistent with an isolated pi^0 coming from the decay K_L -> pi^0 nu nubar. One candidate event was observed, which was consistent with the expected level of background. An upper limit on the branching ratio was determined to be B(K_L -> pi^0 nu nubar) < 1.6E-6 at the 90% confidence level.
Physical Review D | 2003
E. Abouzaid; Michael Wayne Arenton; A. Barker; M. Barrio; L. Bellantoni; E. Blucher; G. J. Bock; C. Bown; E. Cheu; R. Coleman; M. Corcoran; B. E. Cox; A. R. Erwin; C. O. Escobar; A. Glazov; A. Golossanov; R. A. Gomes; P. Gouffon; J. Graham; J. Hamm; Y. Hsiung; D. A. Jensen; Richard Kessler; K. Kotera; J. LaDue; A. Ledovskoy; P. McBride; E. Monnier; H. Nguyen; R. Niclasen
The authors present precision measurements of the direct CP violation parameter, Re({epsilon}{prime}/{epsilon}), the kaon parameters, {Delta}m and {tau}{sub S}, and the CPT tests, {phi}{sub {+-}} and {Delta}{phi}, in neutral kaon decays. These results are based on the full dataset collected by the KTeV experiment at Fermi National Accelerator Laboratory during 1996, 1997, and 1999. This dataset contains {approx} 15 million K {yields} {pi}{sup 0}{pi}{sup 0} decays and {approx} 69 million K {yields} {pi}{sup +}{pi}{sup -} decays. They describe significant improvements to the precision of these measurements relative to previous KTeV analyses. They find Re({epsilon}{prime}/{epsilon}) = [19.2 {+-} 1.1(stat) {+-} 1.8(syst)] x 10{sup -4}, {Delta}m = (5265 {+-} 10) x 10{sup 6} hs{sup -1}, and {tau}{sub S} = (89.62 {+-} 0.05) x 10{sup -12} s. They measure {phi}{sub {+-}} = (44.09 {+-} 1.00){sup o} and {Delta}{phi} = (0.29 {+-} 0.31){sup o}; these results are consistent with CPT symmetry.
Physics Letters B | 1998
T. Alexopoulos; E. W. Anderson; N. Biswas; A. Bujak; D.D. Carmony; A. R. Erwin; L. Gutay; A. Hirsch; C. Hojvat; V.P. Kenney; C.S. Lindsey; J. M. LoSecco; Sergei G. Matinyan; N. Morgan; S. H. Oh; N. Porile; R. P. Scharenberg; B. Stringfellow; M. Thompson; F. Turkot; W.D. Walker; C.H. Wang
Abstract We have examined charged multiplicities arising from p−p and p− p collisions over the range of center of mass energies, s , from 30 GeV to 1800 GeV. Results from Tevatron experiment E735 support the presence of double parton interactions. These processes can be seen to account for a large fraction of the increase in the non single diffraction inelastic cross section from energies of about 200 GeV to 1800 GeV.
Physical Review Letters | 2000
A. Alavi-Harati; L. Bellantoni; A. Glazov; S. A. Taegar; E. Blucher; B. Winstein; H. B. White; J. Jennings; R.A. Swanson; H. Nguyen; S. Averitte; J. Shields; D. R. Bergman; J. LaDue; G. Graham; M. Crisler; S. Hidaka; R. Tschirhart; E. C. Swallow; E. Monnier; Sunil Somalwar; V. Prasad; A. Barker; M. Pang; E. Halkiadakis; A. Golossanov; R. Ben-David; T. Nakaya; P. A. Toale; P. Shanahan
We report the first observation of a manifestly CP violating effect in the K(L)->pi+pi-e+e- decay mode. A large asymmetry was observed in the distribution of these decays in the CP-odd and T-odd angle phi between the decay planes of the e+e- and pi+pi- pairs in the K(L) center of mass system. After acceptance corrections, the overall asymmetry is found to be 13.6+-2.5 (stat) +-1.2 (syst)%. This is the largest CP-violating effect yet observed integrating over the entire phase space of a mode and the first such effect observed in an angular variable.
Physical Review Letters | 2004
T. Alexopoulos; Michael Wayne Arenton; R. F. Barbosa; A. Barker; L. Bellantoni; A. Bellavance; E. Blucher; G. J. Bock; E. Cheu; S. Childress; R. Coleman; M. Corcoran; B. E. Cox; A. R. Erwin; R. Ford; A. Glazov; A. Golossanov; J. Graham; Joachim M. Hamm; K. Hanagaki; Y. Hsiung; H. Huang; V. Jejer; D. A. Jensen; Richard Kessler; H. G. E. Kobrak; K. Kotera; J. LaDue; A. Ledovskoy; P. McBride
We present a determination of the CKM parameter |Vus| based on new measurements of the six largest KL branching fractions and semileptonic form factors by the KTeV (E832) experiment at Fermilab. We find |Vus| = 0.2252 +- 0.0008(KTeV) +- 0.0021(ext), where the errors are from KTeV measurements and from external sources. We also use the measured branching fractions to determine the CP violation parameter |eta+-| = [2.228 +- 0.005(KTeV) +- 0.009(ext)]E-3.
Physical Review D | 2004
T. Alexopoulos; Michael Wayne Arenton; R. F. Barbosa; A. Barker; L. Bellantoni; A. Bellavance; E. Blucher; G. J. Bock; E. Cheu; S. Childress; R. Coleman; M. Corcoran; B. E. Cox; A. R. Erwin; R. Ford; A. Glazov; A. Golossanov; J. Graham; Joachim M. Hamm; K. Hanagaki; Y. Hsiung; H. Huang; V. Jejer; D. A. Jensen; Richard Kessler; H. G. E. Kobrak; K. Kotera; J. LaDue; A. Ledovskoy; P. McBride
We present new measurements of the six largest branching fractions of the KL using data collected in 1997 by the KTeV experiment (E832) at Fermilab. The results are B(KL -> pi e nu) = 0.4067 +- 0.0011 B(KL -> pi mu nu) = 0.2701 +- 0.0009 B(KL -> pi+ pi- pi0) = 0.1252 +- 0.0007 B(KL -> pi0 pi0 pi0) = 0.1945 +- 0.0018 B(KL -> pi+ pi-) = (1.975 +- 0.012)E-3, and B(KL -> pi0 pi0) = (0.865 +- 0.010)E-3, where statistical and systematic errors have been summed in quadrature. We also determine the CP violation parameter |eta+-| to be (2.228 +- 0.010)E-3. Several of these results are not in good agreement with averages of previous measurements.
Physics Letters B | 1995
T. Alexopoulos; C. Allen; E. W. Anderson; V. Balamurali; S. Banerjee; P.D. Beery; P. C. Bhat; J.M. Bishop; N. Biswas; A. Bujak; D.D. Carmony; T. Carter; Y. Choi; P. L. Cole; R. DeBonte; V. DeCarlo; A. R. Erwin; C. Findeisen; A. T. Goshaw; L. Gutay; A. Hirsch; C. Hojvat; J. Jennings; V.P. Kenny; C.S. Lindsey; C. Loomis; J. M. LoSecco; T. McMahon; A.P. McManus; N. Morgan
Abstract The correlations between charged particle multiplicitie produced in forward and backward pseudorapidity regions in pp interactions have been measured with a 240 element scintillator hodoscope. The correlation coefficient and the variance of the difference of multiplicities in the two pseudorapidity regions were deterermined for s =0.3−1.8 TeV . These results have been interpreted in terms of a cluster model of particle production.
Physical Review Letters | 2008
E. Abouzaid; Michael Wayne Arenton; A. Barker; L. Bellantoni; E. Blucher; G. J. Bock; E. Cheu; R. Coleman; M. Corcoran; B. E. Cox; A. R. Erwin; C. Escobar; A. Glazov; A. Golossanov; R. A. Gomes; P. Gouffon; Y. B. Hsiung; D. A. Jensen; Richard Kessler; K. Kotera; A. Ledovskoy; P. McBride; E. Monnier; H. Nguyen; R. Niclasen; D. G. Phillips; E. Ramberg; R. E. Ray; M. Ronquest; E. Santos
We present a new determination of the parity of the neutral pion via the double Dalitz decay pi0-->e+e-e+e-. Our sample, which consists of 30,511 candidate decays, was collected from KL-->pi0pi0pi0 decays in flight at the KTeV-E799 experiment at Fermi National Accelerator Laboratory. We confirm the negative pi0 parity and place a limit on scalar contributions to the pi0-->e+e-e+e- decay amplitude of less than 3.3% assuming CPT conservation. The pi0gamma*gamma* form factor is well described by a momentum-dependent model with a slope parameter fit to the final state phase-space distribution. Additionally, we have measured the branching ratio of this mode to be B(pi0-->e+e-e+e-)=(3.26+/-0.18)x10(-5).
Physics Letters B | 2002
T. Alexopoulos; E. W. Anderson; A. Bujak; D.D. Carmony; A. R. Erwin; L. Gutay; A. Hirsch; K. Nelson; N. Porile; S. H. Oh; R. P. Scharenberg; B. Srivastava; B. Stringfellow; F. Turkot; J. Warchol; W.D. Walker
Abstract We have measured deconfined hadronic volumes, 4.4 V 3 , produced by a one-dimensional (1D) expansion. These volumes are directly proportional to the charged particle pseudorapidity densities 6.75 dN c / dη T =179.5±5(syst) MeV. Using Bjorkens 1D model, the hadronization energy density is ϵ F =1.10±0.26(stat) GeV/fm 3 corresponding to an excitation of 24.8±6.2(stat) quark–gluon degrees of freedom.
Physics Letters B | 1995
T. Alexopoulos; J. Warchol; J. Jennings; D.D. Carmony; C. Wang; Swagato Banerjee; P. C. Bhat; S. H. Oh; W.D. Walker; R. P. Scharenberg; P.D. Beery; E. W. Anderson; A. Bujak; D. Reeves; Y. Choi; B. Stringfellow; V.P. Kenney; T. Carter; N. Biswas; N. Porile; L. Gutay; D.K. Wesson; Y. Zhan; C.S. Lindsey; C. Loomis; A. Hirsch; R. DeBonte; C. Hojvat; J.M. Bishop; S.R. Stampke
Abstract The correlations between charged particle multiplicitie produced in forward and backward pseudorapidity regions in pp interactions have been measured with a 240 element scintillator hodoscope. The correlation coefficient and the variance of the difference of multiplicities in the two pseudorapidity regions were deterermined for s =0.3−1.8 TeV . These results have been interpreted in terms of a cluster model of particle production.