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Search: WFRF:(Kasper L)

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1.
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2.
  • Aaltonen, T., et al. (author)
  • Combination of Tevatron Searches for the Standard Model Higgs Boson in the W+W- Decay Mode
  • 2010
  • In: Physical Review Letters. - 0031-9007 .- 1079-7114. ; 104:6, s. 061802-
  • Journal article (peer-reviewed)abstract
    • We combine searches by the CDF and D0 Collaborations for a Higgs boson decaying to W+W-. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb(-1) of p (p) over bar collisions at root s = 1.96 TeV at the Fermilab Tevatron collider. No excess is observed above background expectation, and resulting limits on Higgs boson production exclude a standard model Higgs boson in the mass range 162-166 GeV at the 95% C.L.
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3.
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4.
  • Aaltonen, T., et al. (author)
  • Combination of CDF and D0 measurements of the W boson helicity in top quark decays
  • 2012
  • In: Physical Review D. - 1550-7998 .- 1550-2368. ; 85:7, s. 071106-
  • Journal article (peer-reviewed)abstract
    • We report the combination of recent measurements of the helicity of the W boson from top quark decay by the CDF and D0 collaborations, based on data samples corresponding to integrated luminosities of 2.7-5.4 fb(-1) of p (p) over bar collisions collected during Run II of the Fermilab Tevatron collider. Combining measurements that simultaneously determine the fractions of W bosons with longitudinal (f(0)) and right-handed (f(+)) helicities, we find f(0) = 0.722 +/- 0.081[+/- 0.062(stat) +/- 0.052(syst)] and f(+) = -0.033 +/- 0.046[+/- 0.034(stat) +/- 0.031(syst)]. Combining measurements where one of the helicity fractions is fixed to the value expected in the standard model, we find f(0) = 0.682 +/- 0.057[+/- 0.035(stat) +/- 0.046(syst)] for fixed f(+) and f(+) = -0.015 +/- 0.035[+/- 0.018(stat) +/- 0.030(syst)] for fixed f(0). The results are consistent with standard model expectations.
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5.
  • Aaltonen, T., et al. (author)
  • Evidence for a Particle Produced in Association with Weak Bosons and Decaying to a Bottom-Antibottom Quark Pair in Higgs Boson Searches at the Tevatron
  • 2012
  • In: Physical Review Letters. - 0031-9007 .- 1079-7114. ; 109:7, s. 071804-
  • Journal article (peer-reviewed)abstract
    • We combine searches by the CDF and D0 Collaborations for the associated production of a Higgs boson with a W or Z boson and subsequent decay of the Higgs boson to a bottom-antibottom quark pair. The data, originating from Fermilab Tevatron p (p) over bar collisions at root s = 1.96 TeV, correspond to integrated luminosities of up to 9.7 fb(-1). The searches are conducted for a Higgs boson with mass in the range 100-150 GeV/c(2). We observe an excess of events in the data compared with the background predictions, which is most significant in the mass range between 120 and 135 GeV/c(2). The largest local significance is 3.3 standard deviations, corresponding to a global significance of 3.1 standard deviations. We interpret this as evidence for the presence of a new particle consistent with the standard model Higgs boson, which is produced in association with a weak vector boson and decays to a bottom-antibottom quark pair.
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6.
  • Abazov, V. M., et al. (author)
  • The upgraded DO detector
  • 2006
  • In: Nuclear Instruments and Methods in Physics Research Section A. - : Elsevier BV. - 0168-9002 .- 1872-9576. ; 565:2, s. 463-537
  • Journal article (peer-reviewed)abstract
    • The DO experiment enjoyed a very successful data-collection run at the Fermilab Tevatron collider between 1992 and 1996. Since then, the detector has been upgraded to take advantage of improvements to the Tevatron and to enhance its physics capabilities. We describe the new elements of the detector, including the silicon microstrip tracker, central fiber tracker, solenoidal magnet, preshower detectors, forward muon detector, and forward proton detector. The uranium/liquid -argon calorimeters and central muon detector, remaining from Run 1, are discussed briefly. We also present the associated electronics, triggering, and data acquisition systems, along with the design and implementation of software specific to DO.
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7.
  • Abazov, V. M., et al. (author)
  • Direct observation of the strange b baryon Xi(-)(b)
  • 2007
  • In: Physical Review Letters. - 0031-9007 .- 1079-7114. ; 99:5, s. 052001-
  • Journal article (peer-reviewed)abstract
    • We report the first direct observation of the strange b baryon Xi(-)(b)(Xi) over bar (+)(b)). We reconstruct the decay Xi(-)(b)-->J/psi Xi(-), with J/psi-->mu(+)mu(-), and Xi(-)-->Lambda pi(-)-->p pi(-)pi(-) in p (p) over bar collisions at root s = 1.96 TeV. Using 1.3 fb(-1) of data collected by the D0 detector, we observe 15.2 +/- 4.4(stat)(-0.4)(+1.9)(syst) Xi(-)(b) candidates at a mass of 5.774 +/- 0.011(stat) +/- 0.015(syst) GeV. The significance of the observed signal is 5.5 sigma, equivalent to a probability of 3.3 x 10(-8) of it arising from a background fluctuation. Normalizing to the decay Lambda(b)-->J/psi Lambda, we measure the relative rate sigma(Xi(-)(b))xB(Xi(-)(b)-->J/psi Xi)/ sigma(Lambda(b))xB(Lambda(b)-->J/psi Lambda) = 0.28 +/- 0.09(stat)(-0.08)(+0.09)(syst).
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8.
  • Abazov, V. M., et al. (author)
  • Evidence for production of single top quarks and first direct measurement of vertical bar V-tb vertical bar
  • 2007
  • In: Physical Review Letters. - 0031-9007 .- 1079-7114. ; 98:18, s. 181802-
  • Journal article (peer-reviewed)abstract
    • The D0 Collaboration presents first evidence for the production of single top quarks at the Fermilab Tevatron < p(p)over bar > collider. Using a 0.9 fb(-1) dataset, we apply a multivariate analysis to separate signal from background and measure sigma(< p(p)over bar >-> tb+X,tqb+X)=4.9 +/- 1.4 pb. The probability to measure a cross section at this value or higher in the absence of a signal is 0.035%, corresponding to a 3.4 standard deviation significance. We use the cross section measurement to directly determine the Cabibbo-Kobayashi-Maskawa matrix element that describes the Wtb coupling and find 0.68 <= 1 at 95% C.L. within the standard model.
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9.
  • Abazov, V. M., et al. (author)
  • Measurement of the Lambda(0)(b) lifetime using semileptonic decays
  • 2007
  • In: Physical Review Letters. - 0031-9007 .- 1079-7114. ; 99:18, s. 182001-
  • Journal article (peer-reviewed)abstract
    • We report a measurement of the Lambda(0)(b) lifetime using a sample corresponding to 1.3 fb(-1) of data collected by the D0 experiment in 2002-2006 during run II of the Fermilab Tevatron collider. The Lambda(0)(b) baryon is reconstructed via the decay Lambda(0)(b)->mu(nu) over bar Lambda X-+(c). Using 4437 +/- 329 signal candidates, we measure the Lambda(0)(b) lifetime to be tau(Lambda(0)(b))=1.290(-0.110)(+0.119)(stat)(-0.091)(+0.087)(syst) ps, which is among the most precise measurements in semileptonic Lambda(0)(b) decays. This result is in good agreement with the world average value.
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10.
  • Abazov, V. M., et al. (author)
  • Measurement of the Lambda(b) lifetime in the exclusive decay Lambda(b)-> J/psi Lambda
  • 2007
  • In: Physical Review Letters. - 0031-9007 .- 1079-7114. ; 99:14, s. 142001-
  • Journal article (peer-reviewed)abstract
    • We have measured the Lambda(b) lifetime using the exclusive decay Lambda(b)-> J/psi Lambda, based on 1.2 fb(-1) of data collected with the D0 detector during 2002-2006. From 171 reconstructed Lambda(b) decays, where the J/psi and Lambda are identified via the decays J/psi ->mu(+)mu(-) and Lambda -> p pi, we measured the Lambda(b) lifetime to be tau(Lambda(b))=1.218(-0.115)(+0.130)(stat)+/- 0.042(syst) ps. We also measured the B-0 lifetime in the decay B-0 -> J/psi(mu(+)mu(-))K-S(0)(pi(+)pi(-)) to be tau(B-0)=1.501(-0.074)(+0.078)(stat)+/- 0.050(syst) ps, yielding a lifetime ratio of tau(Lambda(b))/tau(B-0)=0.811(-0.087)(+0.096)(stat)+/- 0.034(syst).
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  • Result 1-10 of 374
Type of publication
journal article (359)
conference paper (8)
research review (6)
other publication (1)
Type of content
peer-reviewed (364)
other academic/artistic (10)
Author/Editor
Bernardi, G. (243)
Choi, S. (243)
Abbott, B. (242)
Borissov, G. (242)
Brandt, A. (242)
Brock, R. (242)
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Burdin, S. (242)
Chakraborty, D. (242)
Cooke, M. (242)
Fox, H. (242)
Hensel, C. (242)
Kupco, A. (242)
Meyer, J. (242)
Pleier, M. -A. (242)
Sawyer, L. (242)
Schwanenberger, C. (242)
Schwienhorst, R. (242)
Severini, H. (242)
Shabalina, E. (242)
Snyder, S. (242)
Stark, J. (242)
Strauss, M. (242)
Tsybychev, D. (242)
Watts, G. (242)
White, A. (242)
Wicke, D. (242)
Zhu, J. (242)
Buescher, V. (242)
Savage, G. (242)
Bernhard, R. (242)
De La Cruz-Burelo, E ... (242)
Duperrin, A. (242)
Xie, Y. (242)
Davies, G (242)
Adams, M. (242)
Alton, A. (242)
Askew, A. (242)
Avila, C. (242)
Bagby, L. (242)
Baldin, B. (242)
Bean, A. (242)
Bertram, I. (242)
Beuselinck, R. (242)
Boehnlein, A. (242)
Bross, A. (242)
Buehler, M. (242)
Castilla-Valdez, H. (242)
Chandra, A. (242)
Choudhary, B. (242)
Claes, D. (242)
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Uppsala University (267)
Stockholm University (184)
Royal Institute of Technology (141)
Karolinska Institutet (35)
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Chalmers University of Technology (9)
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Swedish University of Agricultural Sciences (5)
Linnaeus University (4)
Malmö University (3)
Kristianstad University College (2)
The Swedish School of Sport and Health Sciences (2)
Swedish Museum of Natural History (2)
Luleå University of Technology (1)
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Stockholm School of Economics (1)
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Language
English (374)
Research subject (UKÄ/SCB)
Natural sciences (301)
Medical and Health Sciences (27)
Engineering and Technology (3)
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