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R. C. Webb

Bio: R. C. Webb is an academic researcher from Texas A&M University. The author has contributed to research in topics: Collider Detector at Fermilab & Neutrino. The author has an hindex of 82, co-authored 600 publications receiving 30376 citations. Previous affiliations of R. C. Webb include University of Wisconsin-Madison & Osaka City University.


Papers
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Journal ArticleDOI
D. S. Akerib1, Henrique Araujo2, X. Bai3, A. J. Bailey2, J. Balajthy4, S. Bedikian5, Ethan Bernard5, A. Bernstein6, Alexander Bolozdynya1, A. W. Bradley1, D. Byram7, Sidney Cahn5, M. C. Carmona-Benitez8, C. Chan9, J.J. Chapman9, A. A. Chiller7, C. Chiller7, K. Clark1, T. Coffey1, A. Currie2, A. Curioni5, Steven Dazeley6, L. de Viveiros10, A. Dobi4, J. E. Y. Dobson11, E. M. Dragowsky1, E. Druszkiewicz12, B. N. Edwards5, C. H. Faham13, S. Fiorucci9, C. E. Flores14, R. J. Gaitskell9, V. M. Gehman13, C. Ghag15, K.R. Gibson1, Murdock Gilchriese13, C. R. Hall4, M. Hanhardt3, S. A. Hertel5, M. Horn5, D. Q. Huang9, M. Ihm16, R. G. Jacobsen16, L. Kastens5, K. Kazkaz6, R. Knoche4, S. Kyre8, R. L. Lander14, N. A. Larsen5, C. Lee1, David Leonard4, K. T. Lesko13, A. Lindote10, M.I. Lopes10, A. Lyashenko5, D.C. Malling9, R. L. Mannino17, Daniel McKinsey5, Dongming Mei7, J. Mock14, M. Moongweluwan12, J. A. Morad14, M. Morii18, A. St. J. Murphy11, C. Nehrkorn8, H. N. Nelson8, F. Neves10, James Nikkel5, R. A. Ott14, M. Pangilinan9, P. D. Parker5, E. K. Pease5, K. Pech1, P. Phelps1, L. Reichhart15, T. A. Shutt1, C. Silva10, W. Skulski12, C. Sofka17, V. N. Solovov10, P. Sorensen6, T.M. Stiegler17, K. O'Sullivan5, T. J. Sumner2, Robert Svoboda14, M. Sweany14, Matthew Szydagis14, D. J. Taylor, B. P. Tennyson5, D. R. Tiedt3, Mani Tripathi14, S. Uvarov14, J.R. Verbus9, N. Walsh14, R. C. Webb17, J. T. White17, D. White8, M. S. Witherell8, M. Wlasenko18, F.L.H. Wolfs12, M. Woods14, Chao Zhang7 
TL;DR: The first WIMP search data set is reported, taken during the period from April to August 2013, presenting the analysis of 85.3 live days of data, finding that the LUX data are in disagreement with low-mass W IMP signal interpretations of the results from several recent direct detection experiments.
Abstract: The Large Underground Xenon (LUX) experiment is a dual-phase xenon time-projection chamber operating at the Sanford Underground Research Facility (Lead, South Dakota). The LUX cryostat was filled for the first time in the underground laboratory in February 2013. We report results of the first WIMP search data set, taken during the period from April to August 2013, presenting the analysis of 85.3 live days of data with a fiducial volume of 118 kg. A profile-likelihood analysis technique shows our data to be consistent with the background-only hypothesis, allowing 90% confidence limits to be set on spin-independent WIMP-nucleon elastic scattering with a minimum upper limit on the cross section of 7.6 × 10(-46) cm(2) at a WIMP mass of 33 GeV/c(2). We find that the LUX data are in disagreement with low-mass WIMP signal interpretations of the results from several recent direct detection experiments.

1,962 citations

Journal ArticleDOI
D. S. Akerib1, S. Alsum2, Henrique Araujo3, X. Bai4, A. J. Bailey3, J. Balajthy5, P. Beltrame, Ethan Bernard6, A. Bernstein7, T. P. Biesiadzinski1, E. M. Boulton6, R. Bramante1, P. Brás8, D. Byram9, Sidney Cahn10, M. C. Carmona-Benitez11, C. Chan12, A.A. Chiller9, C. Chiller9, A. Currie3, J. E. Cutter13, T. J. R. Davison, A. Dobi14, J. E. Y. Dobson15, E. Druszkiewicz16, B. N. Edwards10, C. H. Faham14, S. Fiorucci12, R. J. Gaitskell12, V. M. Gehman14, C. Ghag15, K.R. Gibson1, M. G. D. Gilchriese14, C. R. Hall5, M. Hanhardt4, S. J. Haselschwardt11, S. A. Hertel6, D. P. Hogan6, M. Horn6, D. Q. Huang12, C. M. Ignarra17, M. Ihm6, R.G. Jacobsen6, W. Ji1, K. Kamdin6, K. Kazkaz7, D. Khaitan16, R. Knoche5, N.A. Larsen10, C. Lee1, B. G. Lenardo7, K. T. Lesko14, A. Lindote8, M.I. Lopes8, A. Manalaysay13, R. L. Mannino18, M. F. Marzioni, Daniel McKinsey6, D. M. Mei9, J. Mock19, M. Moongweluwan16, J. A. Morad13, A. St. J. Murphy20, C. Nehrkorn11, H. N. Nelson11, F. Neves8, K. O’Sullivan6, K. C. Oliver-Mallory6, K. J. Palladino17, E. K. Pease6, P. Phelps1, L. Reichhart15, C. Rhyne12, S. Shaw15, T. A. Shutt1, C. Silva8, M. Solmaz11, V. N. Solovov8, P. Sorensen14, S. Stephenson13, T. J. Sumner3, Matthew Szydagis19, D. J. Taylor, W. C. Taylor12, B. P. Tennyson10, P. A. Terman18, D. R. Tiedt4, W. H. To1, Mani Tripathi13, L. Tvrznikova6, S. Uvarov13, J.R. Verbus12, R. C. Webb18, J. T. White18, T. J. Whitis1, M. S. Witherell14, F.L.H. Wolfs16, Jilei Xu7, K. Yazdani3, Sarah Young19, Chao Zhang9 
TL;DR: This search yields no evidence of WIMP nuclear recoils and constraints on spin-independent weakly interacting massive particle (WIMP)-nucleon scattering using a 3.35×10^{4} kg day exposure of the Large Underground Xenon experiment are reported.
Abstract: We report constraints on spin-independent weakly interacting massive particle (WIMP)-nucleon scattering using a 3.35×10^{4} kg day exposure of the Large Underground Xenon (LUX) experiment. A dual-phase xenon time projection chamber with 250 kg of active mass is operated at the Sanford Underground Research Facility under Lead, South Dakota (USA). With roughly fourfold improvement in sensitivity for high WIMP masses relative to our previous results, this search yields no evidence of WIMP nuclear recoils. At a WIMP mass of 50 GeV c^{-2}, WIMP-nucleon spin-independent cross sections above 2.2×10^{-46} cm^{2} are excluded at the 90% confidence level. When combined with the previously reported LUX exposure, this exclusion strengthens to 1.1×10^{-46} cm^{2} at 50 GeV c^{-2}.

1,844 citations

Journal ArticleDOI
Fumio Abe, H. Akimoto1, A. Akopian2, M. G. Albrow3  +443 moreInstitutions (34)
TL;DR: In this paper, the existence of the top quark was established using a data sample of collisions at the Fermilab National Ensemble (CDF) collected with the Collider Detector.
Abstract: We establish the existence of the top quark using a $67{\mathrm{pb}}^{\ensuremath{-}1}$ data sample of $\overline{p}p$ collisions at $\sqrt{s}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}1.8\mathrm{TeV}$ collected with the Collider Detector at Fermilab (CDF). Employing techniques similar to those we previously published, we observe a signal consistent with $t\overline{t}$ decay to $\mathrm{WWb}\overline{b}$, but inconsistent with the background prediction by $4.8\ensuremath{\sigma}$. Additional evidence for the top quark is provided by a peak in the reconstructed mass distribution. We measure the top quark mass to be $176\ifmmode\pm\else\textpm\fi{}8(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}10(\mathrm{syst})\mathrm{GeV}{/c}^{2}$, and the $t\overline{t}$ production cross section to be ${6.8}_{\ensuremath{-}2.4}^{+3.6}\mathrm{pb}$.

1,022 citations

Journal ArticleDOI
P. Adamson1, D. J. Auty2, D. S. Ayres3, C. Backhouse4, G.D. Barr4, M. Betancourt5, M. Bishai6, Andrew Blake7, G. J. Bock1, D. J. Boehnlein1, D. Bogert1, S. V. Cao8, S. Cavanaugh9, D. Cherdack10, S. Childress1, Joao A B Coelho11, L. Corwin12, D. Cronin-Hennessy, I. Z. Danko13, J. K. de Jong4, N. E. Devenish2, M. V. Diwan6, M. Dorman14, Carlos Escobar11, J. J. Evans, E. Falk2, G. J. Feldman9, M. V. Frohne15, H. R. Gallagher10, R. A. Gomes16, Maury Goodman3, P. Gouffon17, N. Graf18, R. Gran, K. Grzelak19, Alec Habig, J. Hartnell2, R. Hatcher1, A. Himmel20, A. Holin14, Xian-Rong Huang3, J. Hylen1, G. M. Irwin21, Z. Isvan13, D. E. Jaffe6, C. James1, D. A. Jensen1, T. Kafka10, S. M. S. Kasahara, G. Koizumi, Sacha E Kopp, M. Kordosky, A. E. Kreymer, Karol Lang, G. Lefeuvre, P. J. Litchfield, L. Loiacono, P. Lucas, W. A. Mann, Marvin L Marshak, M. Mathis, N. Mayer, A. M. McGowan, R. Mehdiyev, J. R. Meier, M. D. Messier, D. G. Michael, W. H. Miller, S. R. Mishra, John C. Mitchell, C. D. Moore, L. Mualem, S. L. Mufson, J. A. Musser, D. Naples, J. K. Nelson, Harvey B Newman, R. J. Nichol, J. A. Nowak, Juan Pedro Ochoa-Ricoux, W. P. Oliver, M. Orchanian, J. M. Paley, R. B. Patterson, Gregory J Pawloski, G. F. Pearce, S. Phan-Budd, R. K. Plunkett, X. Qiu, J. Ratchford, B. Rebel, C. Rosenfeld, H. A. Rubin, M. C. Sanchez, J. Schneps, A. Schreckenberger, P. Schreiner, P. Shanahan, Rohit Sharma, A. Sousa, N. Tagg, R. L. Talaga, J. C. Thomas, M. A. Thomson, R. Toner, D. Torretta, G. Tzanakos, J. Urheim, P. Vahle, B. Viren, J. Walding, A. C. Weber, R. C. Webb, C. White, L. H. Whitehead, Stanley G. Wojcicki, T. Yang, R. Zwaska1 
TL;DR: The results of a search for ν(e) appearance in a ν (μ) beam in the MINOS long-baseline neutrino experiment find that 2 sin(2) (θ(23))sin(2)(2θ (13))<0.12 at 90% confidence level for δ = 0 and the normal (inverted) neutrinos mass hierarchy.
Abstract: We report the results of a search for ν(e) appearance in a ν(μ) beam in the MINOS long-baseline neutrino experiment. With an improved analysis and an increased exposure of 8.2 × 10(20) protons on the NuMI target at Fermilab, we find that 2 sin(2) (θ(23))sin(2)(2θ(13))<0.12(0.20) at 90% confidence level for δ = 0 and the normal (inverted) neutrino mass hierarchy, with a best-fit of 2sin(2) (θ(23))sin(2)(2θ(13)) = 0.041(-0.031)(+0.047) (0.079(-0.053) (+0.071)). The θ(13) = 0 hypothesis is disfavored by the MINOS data at the 89% confidence level.

730 citations

Journal ArticleDOI
D. G. Michael1, P. Adamson2, P. Adamson3, P. Adamson4  +299 moreInstitutions (30)
TL;DR: In this article, the MINOS experiment reported results from its initial exposure to neutrinos from the Fermilab NuMI beam, and the rate and energy spectra of charged current muon neutrino interactions are compared in two detectors located along the beam axis at distances of 1 km and 735 km.
Abstract: This letter reports results from the MINOS experiment based on its initial exposure to neutrinos from the Fermilab NuMI beam. The rate and energy spectra of charged current muon neutrino interactions are compared in two detectors located along the beam axis at distances of 1 km and 735 km. With 1.27 x 10^{20} 120 GeV protons incident on the NuMI target, 215 events with energies below 30 GeV are observed at the Far Detector, compared to an expectation of 336 \\\\\\\\\\\\\\\\pm 14.4 events. The data are consistent with muon neutrino disappearance via oscillation with |\\\\\\\\\\\\\\\\Delta m^2_{23}| = 2.74^{+0.44}_{-0.26} x 10^{-3} eV^2/c^4 and sin^2(2\\\\\\\\\\\\\\\\theta_{23}) > 0.87 (at 60% C.L.).

517 citations


Cited by
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Journal ArticleDOI
Claude Amsler1, Michael Doser2, Mario Antonelli, D. M. Asner3  +173 moreInstitutions (86)
TL;DR: This biennial Review summarizes much of particle physics, using data from previous editions.

12,798 citations

Journal ArticleDOI
01 Apr 1988-Nature
TL;DR: In this paper, a sedimentological core and petrographic characterisation of samples from eleven boreholes from the Lower Carboniferous of Bowland Basin (Northwest England) is presented.
Abstract: Deposits of clastic carbonate-dominated (calciclastic) sedimentary slope systems in the rock record have been identified mostly as linearly-consistent carbonate apron deposits, even though most ancient clastic carbonate slope deposits fit the submarine fan systems better. Calciclastic submarine fans are consequently rarely described and are poorly understood. Subsequently, very little is known especially in mud-dominated calciclastic submarine fan systems. Presented in this study are a sedimentological core and petrographic characterisation of samples from eleven boreholes from the Lower Carboniferous of Bowland Basin (Northwest England) that reveals a >250 m thick calciturbidite complex deposited in a calciclastic submarine fan setting. Seven facies are recognised from core and thin section characterisation and are grouped into three carbonate turbidite sequences. They include: 1) Calciturbidites, comprising mostly of highto low-density, wavy-laminated bioclast-rich facies; 2) low-density densite mudstones which are characterised by planar laminated and unlaminated muddominated facies; and 3) Calcidebrites which are muddy or hyper-concentrated debrisflow deposits occurring as poorly-sorted, chaotic, mud-supported floatstones. These

9,929 citations

Journal ArticleDOI
TL;DR: The Pythia program as mentioned in this paper can be used to generate high-energy-physics ''events'' (i.e. sets of outgoing particles produced in the interactions between two incoming particles).
Abstract: The Pythia program can be used to generate high-energy-physics ''events'', i.e. sets of outgoing particles produced in the interactions between two incoming particles. The objective is to provide as accurate as possible a representation of event properties in a wide range of reactions, within and beyond the Standard Model, with emphasis on those where strong interactions play a role, directly or indirectly, and therefore multihadronic final states are produced. The physics is then not understood well enough to give an exact description; instead the program has to be based on a combination of analytical results and various QCD-based models. This physics input is summarized here, for areas such as hard subprocesses, initial- and final-state parton showers, underlying events and beam remnants, fragmentation and decays, and much more. Furthermore, extensive information is provided on all program elements: subroutines and functions, switches and parameters, and particle and process data. This should allow the user to tailor the generation task to the topics of interest.

6,300 citations

Journal ArticleDOI
TL;DR: In this article, the Wilkinson Microwave Anisotropy Probe (WMAP) 5-year data were used to constrain the physics of cosmic inflation via Gaussianity, adiabaticity, the power spectrum of primordial fluctuations, gravitational waves, and spatial curvature.
Abstract: The Wilkinson Microwave Anisotropy Probe (WMAP) 5-year data provide stringent limits on deviations from the minimal, six-parameter Λ cold dark matter model. We report these limits and use them to constrain the physics of cosmic inflation via Gaussianity, adiabaticity, the power spectrum of primordial fluctuations, gravitational waves, and spatial curvature. We also constrain models of dark energy via its equation of state, parity-violating interaction, and neutrino properties, such as mass and the number of species. We detect no convincing deviations from the minimal model. The six parameters and the corresponding 68% uncertainties, derived from the WMAP data combined with the distance measurements from the Type Ia supernovae (SN) and the Baryon Acoustic Oscillations (BAO) in the distribution of galaxies, are: Ω b h 2 = 0.02267+0.00058 –0.00059, Ω c h 2 = 0.1131 ± 0.0034, ΩΛ = 0.726 ± 0.015, ns = 0.960 ± 0.013, τ = 0.084 ± 0.016, and at k = 0.002 Mpc-1. From these, we derive σ8 = 0.812 ± 0.026, H 0 = 70.5 ± 1.3 km s-1 Mpc–1, Ω b = 0.0456 ± 0.0015, Ω c = 0.228 ± 0.013, Ω m h 2 = 0.1358+0.0037 –0.0036, z reion = 10.9 ± 1.4, and t 0 = 13.72 ± 0.12 Gyr. With the WMAP data combined with BAO and SN, we find the limit on the tensor-to-scalar ratio of r 1 is disfavored even when gravitational waves are included, which constrains the models of inflation that can produce significant gravitational waves, such as chaotic or power-law inflation models, or a blue spectrum, such as hybrid inflation models. We obtain tight, simultaneous limits on the (constant) equation of state of dark energy and the spatial curvature of the universe: –0.14 < 1 + w < 0.12(95%CL) and –0.0179 < Ω k < 0.0081(95%CL). We provide a set of WMAP distance priors, to test a variety of dark energy models with spatial curvature. We test a time-dependent w with a present value constrained as –0.33 < 1 + w 0 < 0.21 (95% CL). Temperature and dark matter fluctuations are found to obey the adiabatic relation to within 8.9% and 2.1% for the axion-type and curvaton-type dark matter, respectively. The power spectra of TB and EB correlations constrain a parity-violating interaction, which rotates the polarization angle and converts E to B. The polarization angle could not be rotated more than –59 < Δα < 24 (95% CL) between the decoupling and the present epoch. We find the limit on the total mass of massive neutrinos of ∑m ν < 0.67 eV(95%CL), which is free from the uncertainty in the normalization of the large-scale structure data. The number of relativistic degrees of freedom (dof), expressed in units of the effective number of neutrino species, is constrained as N eff = 4.4 ± 1.5 (68%), consistent with the standard value of 3.04. Finally, quantitative limits on physically-motivated primordial non-Gaussianity parameters are –9 < f local NL < 111 (95% CL) and –151 < f equil NL < 253 (95% CL) for the local and equilateral models, respectively.

5,904 citations

Journal ArticleDOI
TL;DR: The current status of particle dark matter, including experimental evidence and theoretical motivations, including direct and indirect detection techniques, is discussed in this paper. But the authors focus on neutralinos in models of supersymmetry and Kaluza-Klein dark matter in universal extra dimensions.

4,614 citations