$\mathrm{W^+W^-}$
               production and triple gauge boson couplings at LEP energies up to 183 GeV

Abbiendi, G.; Ackerstaff, K.; Alexander, G.; Allison, J.; Altekamp, N.; Anderson, K. J.; Anderson, S.; Arcelli, S.; Asai, S.; Ashby, S. F.; Axen, D.; Azuelos, G.; Ball, A. H.; Barberio, E.; Barlow, R. J.; Bartoldus, R.; Batley, J. R.; Baumann, S.; Bechtluft, J.; Behnke, T.; Bell, K. W.; Bella, G.; Bellerive, A.; Bentvelsen, S.; Bethke, S.; Betts, S.; Biebel, O.; Biguzzi, A.; Bird, S. D.; Blobel, V.; Bloodworth, I. J.; Bock, P.; Böhme, J.; Bonacorsi, D.; Boutemeur, M.; Braibant, S.; Bright-Thomas, P.; Brigliadori, L.; Brown, R. M.; Burckhart, H.; Capiluppi, P.; Carnegie, R. K.; Carter, A. A.; Carter, J. R.; Chang, C. Y.; Charlton, D. G.; Chrisman, D.; Ciocca, C.; Clarke, P. E.L.; Clay, E.; Cohen, I.; Conboy, J. E.; Cooke, O. C.; Couyoumtzelis, C.; Coxe, R. L.; Cuffiani, M.; Dado, S.; Dallavalle, G. M.; Davis, R.; Jong, S. J. De; Roeck, A. De; Dervan, P.; Desch, K.; Dienes, B.; Dixit, M. S.; Dubbert, J.; Duchovni, E.; Duckeck, G.; Duerdoth, I. P.; Eatough, D.; Estabrooks, P. G.; Etzion, E.; Fabbri, F.; Fanti, M.; Faust, A. A.; Fiedler, F.; Fierro, M.; Fleck, I.; Folman, R.; Fürtjes, A.; Futyan, D. I.; Gagnon, P.; Gary, J. W.; Gascon, J.; Gascon-Shotkin, S. M.; Gaycken, G.; Geich-Gimbel, Ch.; Giacomelli, G.; Giacomelli, P.; Gibson, V.; Gibson, W. R.; Gingrich, D. M.; Glenzinskí, D.; Goldberg, J.; Gorn, W.; Grandi, C.; Graham, K.; Gross, E.; Grunhaus, J.; Gruwé, M.; Hanson, G.; Hansroul, M.; Hapke, M.; Harder, K.; Harel, A.; Hargrove, C. K.; Hartmann, C.; Hauschild, M.; Hawkes, C. M.; Hawkings, R. J.; Hemingway, R. J.; Herndon, M.; Herten, G.; Heuer, R. D.; Hildreth, M.; Hill, J. C.; Hobson, P. R.; Hoch, M.; Höcker, A.; Hoffman, K. D.; Homer, R. J.; Honma, A. K.; Horvath, D.; Hossain, K. R.; Howard, Robert; Hüntemeyer, P.; Igo‐Kemenes, P.; Imrie, D. C.; Ishii, K.; Jacob, F. R.; Jawahery, A.; Jérémie, H.; Jimack, M.; Jones, C. R.; Jovanović, P.; Junk, T. R.; Karlen, D.; Kartvelishvili, V.; Kawagoe, K.; Kawamoto, T.; Kayal, P. I.; Keeler, R.; Kellogg, R. G.; Kennedy, B. W.; Kim, D. H.; Klier, A.; Kluth, S.; Kobayashi, T.; Kobel, M.; Koetke, D. S.; Kokott, T. P.; Kolrep, M.; Komamiya, S.; Kowalewski, R.; Kress, T.; Krieger, P.; Krogh, J. von; Kühl, T.; Kyberd, P.; Lafferty, G. D.; Landsman, H.; Lanske, D.; Lauber, J.; Lautenschlager, S. R.; Lawson, I.; Layter, J. G.; Lazic, D.; Lee, A. M.; Lellouch, D.; Letts, J.; Levinson, L. J.; Liebisch, R.; List, B.; Littlewood, C.; Lloyd, A. W.; Lloyd, S. L.; Loebinger, F. K.; Long, G. D.; Losty, M. J.; Ludwig, J.; Liu, D.; Macchiolo, A.; Macpherson, A.; Mader, W. F.; Mannelli, M.; Marcellini, S.; Markopoulos, C.; Martin, A. J.; Martin, J. P.; Martı́nez, G.; Mäshimo, T.; Mättig, P.; McDonald, W. J.; McKenna, J. A.; Mckigney, E. A.; McMahon, Thomas J.; McPherson, R. A.; Meijers, F.; Menke, S.; Merritt, F. S.; Mes, H.; Meyer, J.; Michelini, A.; Mihara, S.; Mikenberg, G.; Miller, D. J.; Mir, R.; Mohr, W.; Montanari, A.; Mori, T.; Nagai, K.; Nakamura, I.; Neal, H.; Nellen, B.; Nisius, R.; O’Neale, S. W.; Oakham, F. G.; Odorici, F.; Ogren, H. O.; Oreglia, M. J.; Orito, S.; Pálinkás, J.; Pásżtor, G.; Pater, J. R.; Patrick, G. N.; Patt, J.; Perez-Ochoa, R.; Petzold, S.; Pfeifenschneider, P.; Pilcher, J. E.; Pinfold, J. L.; Plane, D. E.; Poffenberger, P.; Polok, J.; Przybycień, M.; Rembser, C.; Rick, H.; Robertson, S.; Robins, S. A.; Rodning, N.; Roney, J. M.; Roscoe, K.; Rossi, A. M.; Rozen, Y.; Runge, K.; Runólfsson, Ö.; Rust, D. R.; Sachs, K.; Saeki, T.; Sahr, O.; Sang, W. M.; Sarkisyan, E. K.G.; Sbarra, C.; Schaile, A. D.; Schaile, O.; Scharf, F.; Scharff-Hansen, P.; Schieck, J.; Schmitt, B.; Schmitt, S.; Schöning, A.; Schröder, M.; Schumacher, M.; Schwick, C.; Scott, W. G.; Seuster, R.; Shears, T.; Shen, B. C.; Shepherd‐Themistocleous, C. H.; Sherwood, P.; Siroli, G. P.; Sittler, A.; Skuja, A.; Smith, A. M.; Snow, G. A.; Sobie, R. J.; Söldner-Rembold, S.; Spagnolo, S.; Sproston, M.; Stahl, A.; Stephens, K.; Steuerer, J.; Stoll, K.; Strom, D.; Ströhmer, R.; Surrow, B.; Talbot, S. D.; Tanaka, Shun‐ichi; Taras, P.; Tarem, S.; Teuscher, R. J.; Thiergen, M.; Thomas, J. P.; Thomson, M. A.; Torne, Eckhard von; Torrence, E.; Towers, S.; Trigger, I. M.; Trocsanyi, Z. L.; Tsur, E.; Turcot, A. S.; Turner-Watson, M. F.; Ueda, I.; Vachon, B.; Kooten, R. Van; Vannerem, P.; Verzocchi, M.; Voss, H.; Wäckerle, F.; Wagner, A. P.; Ward, C. P.; Ward, D. R.; Watkins, P. M.; Watson, A. T.; Watson, N. K.; Wells, P. S.; Wermes, N.; White, J. S.; Wilson, G. W.; Wilson, J. A.; Wyatt, T. R.; Yamashita, Shinji; Yekutieli, G.; Zacek, V.; Zer-Zion, D.

doi:10.1007/s100529901106

Cited by 22 publications

(2 citation statements)

References 33 publications

(66 reference statements)

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“…There is a long-standing experimental interest in the polarizations of W bosons in boson-pair production. They were investigated for example in electron-positron collisions at LEP [38] with the aim of probing anomalous gauge-boson couplings.…”

Section: Introductionmentioning

confidence: 99%

Polarized electroweak bosons in W+W− production at the LHC including NLO QCD effects

Denner

Pelliccioli

2020

J. High Energ. Phys.

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The measurement of polarization fractions of massive gauge bosons at the LHC provides an important check of the Standard Model and in particular of the Electroweak Symmetry Breaking mechanism. Owing to the unstable character of W and Z bosons, devising a theoretical definition for polarized signals is not straightforward and always subject to some ambiguity. Focusing on W-boson pair production at the LHC in the fully leptonic channel, we propose to compute polarized cross-sections and distributions based on the gauge-invariant doubly-resonant part of the amplitude. We include NLO QCD corrections to the leading quark-induced partonic process and also consider the loop- induced gluon-initiated process contributing to the same final state. We present results for both an inclusive setup and a realistic fiducial region, with special focus on variables that are suited for the discrimination of polarized cross-sections and on quantities that can be measured experimentally.

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Section: Introductionmentioning

confidence: 99%

Polarized electroweak bosons in W+W− production at the LHC including NLO QCD effects

Denner

Pelliccioli

2020

J. High Energ. Phys.

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“…Measuring polarized cross sections of diboson production processes has been being performed from the LEP [1] to the LHC. Recent results include W ± Z measurements at ATLAS [2,3] and at CMS [4], same-sign W W j j at CMS [5], and Z Z at ATLAS [6].…”

Section: Introductionmentioning

confidence: 99%

NLO electroweak corrections to doubly-polarized $$W^+W^-$$ production at the LHC

Dao,

2024

Eur. Phys. J. C

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We present new results of next-to-leading order (NLO) electroweak corrections to doubly-polarized cross sections of $$W^+W^-$$ W + W - production at the LHC. The calculation is performed for the leptonic final state of $$e^{+}\mu _{e} \mu ^{-} {\bar{\nu }}_{\mu }$$ e + μ e μ - ν ¯ μ using the double-pole approximation in the diboson center-of-mass frame. NLO QCD corrections and subleading contributions from the gg, $$b{\bar{b}}$$ b b ¯ , $$\gamma \gamma $$ γ γ induced processes are taken into account in the numerical results. We found that NLO EW corrections are small for angular distributions but can reach tens of percent for transverse momentum distributions at high energies, e.g. reaching $$-40\%$$ - 40 % at $$p_{T,e}\approx 300$$ p T , e ≈ 300 GeV. In these high $$p_T$$ p T regions, EW corrections are largest for the doubly-transverse mode.

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Results From LEP 200

Fernández

2000

Particle Physics: Ideas and Recent Developments

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$\mathrm{W^+W^-}$ production and triple gauge boson couplings at LEP energies up to 183 GeV

Cited by 22 publications

References 33 publications

Polarized electroweak bosons in W+W− production at the LHC including NLO QCD effects

Polarized electroweak bosons in W+W− production at the LHC including NLO QCD effects

NLO electroweak corrections to doubly-polarized $$W^+W^-$$ production at the LHC

Results From LEP 200

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