Готові списки джерел за темами / Standard Electroweak Model

Добірка наукової літератури з теми "Standard Electroweak Model"

Автор: Grafiati
Опубліковано: 7 вересня 2023

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Статті в журналах з теми "Standard Electroweak Model"

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BARKER, ANTHONY R. "STATUS OF STANDARD MODEL PARAMETERS." International Journal of Modern Physics A 16, supp01a (October 2001): 25–40. http://dx.doi.org/10.1142/s0217751x01006280.

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Анотація:
Recent experimental progress in determining the parameters of the electroweak sector of the Standard Model is summarized. The principal topics addressed include the precision determination of electroweak parameters using LEP and SLD data at the Z0 pole, measurements of the W mass by LEP-II, CDF, and D0, and determination of the elements of the CKM matrix using a variety of experimental methods.
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2

TANG, YONG. "VACUUM STABILITY IN THE STANDARD MODEL." Modern Physics Letters A 28, no. 04 (January 29, 2013): 1330002. http://dx.doi.org/10.1142/s0217732313300024.

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The long-awaited Higgs particle H around 125 GeV has been observed at the LHC. Interpreting it as the Standard Model Higgs boson and if there is no new physics between electroweak and Planck scale, we then do not have a stable vacuum. Here, we give a brief review of the electroweak vacuum stability and some related theoretical issues in the Standard Model. Possible ways to save the stability are also discussed.
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3

Marciano, W. J., and Z. Parsa. "Electroweak Tests of the Standard Model." Annual Review of Nuclear and Particle Science 36, no. 1 (December 1986): 171–205. http://dx.doi.org/10.1146/annurev.ns.36.120186.001131.

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4

Erler, Jens. "Tests of the Electroweak Standard Model." Journal of Physics: Conference Series 485 (March 24, 2014): 012010. http://dx.doi.org/10.1088/1742-6596/485/1/012010.

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5

Haidt, D. "Status of the electroweak standard model." Nuclear Physics B - Proceedings Supplements 13 (February 1990): 3–14. http://dx.doi.org/10.1016/0920-5632(90)90032-p.

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6

Dydak, F. "Electroweak standard model: Tests at LEP." Nuclear Physics A 546, no. 1-2 (August 1992): 85–105. http://dx.doi.org/10.1016/0375-9474(92)90503-c.

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7

KAZAKOV, D. I. "BEYOND THE STANDARD MODEL." International Journal of Modern Physics A 22, no. 30 (December 10, 2007): 5502–12. http://dx.doi.org/10.1142/s0217751x07038761.

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Анотація:
Review of recent developments in attempts to go beyond the Standard Model is given. We concentrate on three main unresolved problems: mechanism of electroweak symmetry breaking, expected new physics at the TeV scale (mainly SUSY) and the origin of the Dark matter.
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8

KITAZAWA, NORIAKI. "VACUUM ALIGNMENT IN THE TOP MODE STANDARD MODEL." Modern Physics Letters A 06, no. 40 (December 28, 1991): 3691–96. http://dx.doi.org/10.1142/s0217732391004279.

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Анотація:
We study the vacuum alignment in the top mode Standard Model in which the electroweak symmetry breaking is triggered by the top quark condensation. Including the QCD effects through the Cornwall-Jackiw-Tomboulis effective potential, we establish that the correct electroweak symmetry breaking SU (2)L × U (1)Y → U (1) em occurs in this model in 1/N leading and improved ladder approximation.
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9

Li, Shu. "Standard model measurements with ATLAS (+CMS) detector(s)." International Journal of Modern Physics: Conference Series 39 (January 2015): 1560102. http://dx.doi.org/10.1142/s2010194515601027.

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Анотація:
We present a broad range of Standard Model measurements performed in proton-proton collisions at the LHC on a variety of topics [Formula: see text]jets production and ratios, the electroweak multi-boson production, [Formula: see text] heavy flavor decay production, jet production, photon physics, the Standard Model soft QCD and diffractive physics. The latest public results from ATLAS experiment are obtained at the center-of-mass energy of both 7 TeV and 8 TeV, which covers total cross sections, fiducial cross sections, differential cross sections wherever available and comparison with Leading-Order/Next-to-Leading-Order/Next-to-Next-to-Leading-Order theory predictions. These measurements provide important tests for perturbative QCD, electroweak multi-boson interactions, Electroweak Symmetry Breaking over a broad kinematic range and constraints for PDFs. Model-independent new physics searches are also performed by probing anomalous gauge bosons couplings using effective Lagrangian or effective field theory formalism.
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10

Batebi, S., M. Haghighat, S. Tizchang, and H. Akafzade. "Higgs couplings in noncommutative Standard Model." International Journal of Modern Physics A 30, no. 20 (July 19, 2015): 1550108. http://dx.doi.org/10.1142/s0217751x15501080.

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We consider the Higgs and Yukawa parts of the Noncommutative Standard Model (NCSM). We explore the NC-action to give all Feynman rules for couplings of the Higgs boson to electroweak gauge fields and fermions.
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Дисертації з теми "Standard Electroweak Model"

1

Fromme, Lars. "Electroweak baryogenesis in extensions of the standard model." [S.l.] : [s.n.], 2006. http://deposit.ddb.de/cgi-bin/dokserv?idn=980804515.

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2

Díaz, Méndez Enrique. "Electroweak scale neutrinos." To access this resource online via ProQuest Dissertations and Theses @ UTEP, 2009. http://0-proquest.umi.com.lib.utep.edu/login?COPT=REJTPTU0YmImSU5UPTAmVkVSPTI=&clientId=2515.

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3

Yamashita, Hiroki 1981. "Electroweak phase transition and singlet Majoron model." Thesis, McGill University, 2007. http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=101691.

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Анотація:
First, we review the basics of baryogenesis and models for baryogenesis in the early literature. Then, we discuss the main theme in this thesis, electroweak baryogenesis, which utilizes the electroweak phase transition. We present how the phase transition can be used to achieve baryogenesis. Next, we develop our model, which is the Standard Model with a singlet field coupled to the Higgs doublet negatively and to the right-handed neutrinos. It is a simple extension of the singlet Majoron model. We focus on numerical analysis of the model. Parameter space satisfying all the conditions are found and relevant quantities, such as the critical temperature, the Higgs mass, and the mixing angle are found as well. It turns out that LEP bound on the Higgs mass and the mixing angle is a strong constraint, and only a small fraction of parameter space is acceptable for attaining a strong enough phase transition for baryogenesis.
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4

Athron, Peter. "Aspects of electroweak symmetry breaking in physics beyond the standard model." Thesis, University of Glasgow, 2008. http://theses.gla.ac.uk/513/.

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Анотація:
Fine tuning in the Standard Model (SM) is the basis for a widespread expectation that the minimal model for electroweak symmetry breaking, with a single Higgs boson, is not realised in nature and that new physics, in addition to (or instead of) the Higgs, will be discovered at the Large Hadron Collider (LHC). However constraints on new physics indicate that many models which go beyond the SM (BSM) may also be fine tuned (although to a much lesser extent). To test this a reliable, quantitative measure of tuning is required. We review the measures of tuning used in the literature and propose an alternative measure. We apply this measure to several toy models and a constrained version of the Minimal Supersymmetric Standard Model. The Exceptional Supersymmetric Standard Model (E6SSM) is another BSM motivated by naturalness. As a supersymmetric theory it solves the SM hierarchy problem and by breaking a new gauged U(1) symmetry it also solves the μ-problem of the MSSM. We investigate the Renormalisation Group Evolution of the model and test for radiative electroweak symmetry breaking in two versions of the model with different high scale constraints. First we briefly look at scenarios with non-universal Higgs masses at the GUT scale and present a particle spectrum that could be observed at the LHC. Secondly we study the constrained E6SSM (CE6SSM), with universal scalar (m0), trilinear (A0) and gaugino (M) masses. We reveal a large volume of CE6SSM parameter space where the correct breakdown of the gauge symmetry can be achieved and all experimental constraints can be satisfied. We present benchmark points corresponding to different patterns of the particle spectrum. A general feature of the benchmark spectra is a light sector of SUSY particles consisting of a light gluino, two light neutralinos and a light chargino. Although the squarks, sleptons and Z′ boson are typically much heavier, the exotic color triplet charge 1/3 fermions as well as the lightest stop can be also relatively light leading to spectacular new physics signals at the LHC.
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5

Marx, Marilyn. "Standard model and exotic diboson production with the ATLAS detector." Thesis, University of Manchester, 2013. https://www.research.manchester.ac.uk/portal/en/theses/standard-model-and-exotic-diboson-production-with-the-atlas-detector(7a674cb6-dd88-46d3-9506-6b9f1074eac7).html.

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6

Fok, Ricky. "Scenarios of Physics Beyond the Standard Model." Thesis, University of Oregon, 2011. http://hdl.handle.net/1794/11940.

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Анотація:
xviii, 124 p. : ill. (some col.)
This dissertation discusses three topics on scenarios beyond the Standard Model. Topic one is the effects from a fourth generation of quarks and leptons on electroweak baryogenesis in the early universe. The Standard Model is incapable of electroweak baryogenesis due to an insufficiently strong enough electroweak phase transition (EWPT) as well as insufficient CP violation. We show that the presence of heavy fourth generation fermions solves the first problem but requires additional bosons to be included to stabilize the electroweak vacuum. Introducing supersymmetric partners of the heavy fermions, we find that the EWPT can be made strong enough and new sources of CP violation are present. Topic two relates to the lepton avor problem in supersymmetry. In the Minimal Supersymmetric Standard Model (MSSM), the off-diagonal elements in the slepton mass matrix must be suppressed at the 10-3 level to avoid experimental bounds from lepton avor changing processes. This dissertation shows that an enlarged R-parity can alleviate the lepton avor problem. An analysis of all sensitive parameters was performed in the mass range below 1 TeV, and we find that slepton maximal mixing is possible without violating bounds from the lepton avor changing processes: μ [arrow right] eγ; μ [arrow right] e conversion, and μ [arrow right] 3e. Topic three is the collider phenomenology of quirky dark matter. In this model, quirks are particles that are gauged under the electroweak group, as well as a \dark" color SU (2) group. The hadronization scale of this color group is well below the quirk masses. As a result, the dark color strings never break. Quirk and anti-quirk pairs can be produced at the LHC. Once produced, they immediately form a bound state of high angular momentum. The quirk pair rapidly shed angular momentum by emitting soft radiation before they annihilate into observable signals. This dissertation presents the decay branching ratios of quirkonia where quirks obtain their masses through electroweak symmetry breaking. This dissertation includes previously published and unpublished co-authored material.
Committee in charge: Dr. Davison Soper: Chair; Dr. Graham Kribs: Advisor; Dr. Ray Frey: Member; Dr. Michael Kellman: Outside Member
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7

Del, Donno Antonio. "Testing electroweak baryogenesis at LHC in a minimal extension of the Standard Model." Master's thesis, Alma Mater Studiorum - Università di Bologna, 2018. http://amslaurea.unibo.it/17052/.

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Анотація:
Il modello standard è la teoria che descrive con spettacolare accuratezza le interazioni fra i costituenti fondamentali della materia come oggi ci sono noti. Nonostante il successo nel confronto fra teoria ed esperimenti, diverse questioni rimangono insolute. Indicazioni esistono riguardo l'esistenza di fisica oltre il modello standard, anche se ancora ignoriamo la sua natura. L'obiettivo principale di questo lavoro è di caratterizzare una delle più semplici estensioni del modello standard che prevede un singoletto scalare interagente con il solo bosone di Higgs. Questo nuovo stato potrebbe avere un'influenza sulla fenomenologia del bosone di Higgs ai collider e dare luogo al meccanismo della bariogenesi elettrodebole. Una volta classificate le differenti possibilità, concentriamo la nostra attenzione su un modello semplificato caratterizzato da una simmetria $\mathbb{Z}_{2}$, nel quale le modifiche al self-coupling del bosone di Higgs possono apparire solo ad un loop. Il calcolo dei contributi corrispondenti permette di identificare la regione dello spazio dei parametri dove è possibile ottenere una transizione di fase elettrodebole del primo ordine, e di verificare se le deviazioni dalle previsioni del modello standard possano essere rilevabili ad LHC. Consideriamo sia il modello completo che la corrispondente approssimazione effettiva, studiandone il regime di applicabilità. Infine, otteniamo le previsioni per la produzione di una coppia di bosoni di Higgs. I nostri risultati preliminari mostrano come nelle regioni dello spazio dei parametri nelle quali è possibile avere la transizione del primo ordine un approccio effettivo sia sufficiente a riprodurre il modello completo. Inoltre, le differenze di shape e sezione d'urto fra la estensione con un singoletto ed il modello standard sono visibili per valori della massa del singoletto potenzialmente rilevabili a LHC.
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8

Tayduganov, Andrey. "Electroweak radiative B-decays as a test of the Standard Model and beyond." Phd thesis, Université Paris Sud - Paris XI, 2011. http://tel.archives-ouvertes.fr/tel-00648217.

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Recently the radiative B-decay to strange axial-vector mesons, B--> K1(1270) gamma, was observed with a rather large branching ratio. This process is particularly interesting as the subsequent K1-decay into its three-body final state allows us to determine the polarization of the photon, which is mostly left(right)-handed for Bbar(B) in the Standard Model while various new physics models predict additional right(left)-handed components. In this thesis, a new method is proposed to determine the polarization, exploiting the full Dalitz plot distribution, which seems to reduce significantly the statistical errors on the polarization parameter lambda_gamma measurement.This polarization measurement requires, however a detailed knowledge of the K1--> K pi pi strong interaction decays, namely, the complex pattern of the various partial wave amplitudes into several possible quasi-two-body channels as well as their relative phases. A number of experiments have been done to extract all these information while there remain various problems in the previous studies. In this thesis, we investigate the details of these problems. As a theoretical tool, we use the 3P0 quark-pair-creation model in order to improve our understanding of strong K1 decays.Finally we try to estimate some theoretical uncertainties: in particular, the one coming from the uncertainty on the K1 mixing angle, and the effect of a possible ''off-set'' phase in strong decay S-waves. According to our estimations, the systematic errors are found to be of the order of sigma(lambda_gamma)^th<20%. On the other hand, we discuss the sensitivity of the future experiments, namely the SuperB factories and LHCb, to lambda_gamma. Naively estimating the annual signal yields, we found the statistical error of the new method to be sigma(lambda_gamma)^stat<10% which turns out to be reduced by a factor 2 with respect to using the simple angular distribution.We also discuss a comparison to the other methods of the polarization measurement using processes, such as B--> K* e^+ e^-, Bd--> K* gamma and Bs--> phi gamma, for the determination of the ratio of the Wilson coefficients C7gamma^'eff/C7gamma^eff. We show an example of the potential constraints on C7gamma^'eff/C7gamma^eff. in several scenarios of supersymmetric models.
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9

Lyonnet, Florian. "New heavy resonances : from the electroweak to the planck scale." Thesis, Grenoble, 2014. http://www.theses.fr/2014GRENY035/document.

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Le principe d'invariance de jauge local est au centre de la physique des particules moderne. Dans le modèle standard (MS), il repose sur le groupe de jauge ad hoc SU(3)_c x SU(2)_L x U(1)_Y. L'idée d'étendre ce groupe de jauge est particulièrement attrayante dans une perspective de ``Grand Unified Theory'' (GUT) où le MS est la limite basse énergie d'une théorie plus fondamentale basée sur un groupe de jauge beaucoup plus large tel que SO(10) ou E(6). En effet, lors de la brisure de symétrie du groupe de GUT au MS, des facteurs de groupe non-brisés supplémentaires, tels que U(1) ou SU(2), peuvent apparaitre. Ce manuscrit est consacré à la phénoménologie de modèles avec un groupe de jauge étendu. En particulier, les études présentées sont centrées sur les modèles basés sur le groupe de jauge SU(2) x SU(2) x U(1) dénotés G(221). De manière générique, ces modèles prédisent de nouveaux bosons de jauges, Z' et W'.Après une brève présentation des modèles G(221), un nouveau code publique, PyR@TE, qui permet de déterminer les équations du groupe de renormalisation à deux boucles pour une théorie de jauge arbitraire est introduit. Ce code est ensuite utilisé pour déterminer les RGEs des modèles de la classe G(221). La suite du manuscrit est dédiée à la présentation des résultats obtenus sur le calcul des corrections radiatives QCD de la production électrofaible d'une paire de quarks top dans le cadre des modèles G(221), i.e. en présence d'un nouveau boson de jauge Z'. Ces résultats font l'objet d'une implémentation dans le générateur d'événements Monte Carlo POWHEG BOX et les premiers résultats numériques obtenus sont présentés. Les derniers développements concernant le calcul des corrections QCD à la production électrofaible de single-top sont également revus. Enfin, la dernière partie de ce manuscrit est consacrée à l'étude de l'impact de nouvelles résonances W', Z', telles que celles présentes dans les modèles G(221), sur l'interaction des neutrinos d'ultra-haute énergie dans l'atmosphère. Ces interactions sont recherchées par l'observatoire Pierre Auger dans les douches de particules produites par l'interaction des rayons cosmiques avec les particules de l'atmosphère
The principle of local gauge invariance is a pillar of modern particle physics theories and in the SM relies on the ad-hoc gauge group structure SU(3)_c x SU(2)_L x U(1)_Y. Extending this gauge group is very well motivated in a Grand Unified Theory (GUT) perspective in which the SM is the low-energy limit of a more fundamental theory based on a larger gauge group like SO(10) or E(6). Indeed, the symmetry breaking (SB) of the underlying GUT gauge group, down to the SM one, leaves some additional group factors unbroken, such as U(1) or SU(2). In this spirit, we focus in this manuscript on the phenomenology of extended gauge group models and on the new heavy neutral and charged resonances, generically called Z' and W' predicted by these.In this manuscript we present different aspects of the phenomenology of the G(221) models. After reviewing these extensions, we present a public tool, PyR@TE, that aims at automating the calculation of RGEs at two-loop for arbitrary gauge theories and exemplify its use with the G(221) models. In a second part, we present our results for the calculation of the QCD corrections to the electroweak top-pair production as well as their implementation in a general purpose Monte Carlo generator allowing for a consistent matching of next-to-leading order (NLO) matrix elements with parton shower algorithms, the POWHEG BOX. We then review the status of our calculation of the QCD corrections to the electroweak single-top production. Finally, we present a different aspect of the phenomenology of new heavy resonances, Z', W' by studying their impact on the interaction of ultra-high energy neutrinos in the atmosphere. For definiteness we consider the Pierre Auger Observatory, which is sensible to showers initiated by neutrinos of extreme energies up to 10E12 GeV
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10

Xue, Ying. "Quantum field-theoretical investigations in nonperturbative QCD and beyond-the-standard-model electroweak physics." Thesis, National Library of Canada = Bibliothèque nationale du Canada, 1998. http://www.collectionscanada.ca/obj/s4/f2/dsk2/tape15/PQDD_0012/NQ31168.pdf.

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Книги з теми "Standard Electroweak Model"

1

P, Langacker, ed. Precision tests of the standard electroweak model. Singapore: World Scientific, 1995.

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2

Introduction to electroweak unification: Standard model from tree unitarity. Singapore: World Scientific, 1994.

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3

Donoghue, John F. Dynamics of the standard model. Cambridge: Cambridge University Press, 1992.

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4

Donoghue, John F. Dynamics ofthe standard model. Cambridge: Cambridge University Press, 1992.

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5

Derdziński, Andrzej. Geometry of the standard model of elementary particles. Berlin: Springer-Verlag, 1992.

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6

Furtado, Valle José Wagner, Velasco J, and International Workshop on Electroweak Physics Beyond the Standard Model (1991 : Valencia, Spain), eds. Electroweak physics beyond the standard model: Valéncia, Spain : 2-5 October 1991. Singapore: World Scientific, 1992.

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7

Electroweak physics at LEP and LHC. Heidelberg [Germany]: Springer, 2010.

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8

An introduction to relativistic processes and the standard model of electroweak interactions. Milan, IT: Springer, 2006.

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9

Bardin, D. The standard model in the making: Precision study of the electroweak interactions. Oxford: Clarendon Press, 1999.

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10

Becchi, Carlo M., and Giovanni Ridolfi. An introduction to relativistic processes and the standard model of electroweak interactions. Milano: Springer Milan, 2006. http://dx.doi.org/10.1007/88-470-0421-7.

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Частини книг з теми "Standard Electroweak Model"

1

Boonekamp, Maarten, Stefan Dittmaier, and Matthias Mozer. "Electroweak Standard Model Physics." In The Large Hadron Collider, 95–138. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-15001-7_4.

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2

Martin, Stephen P., and James D. Wells. "The Standard Electroweak Model." In Graduate Texts in Physics, 269–305. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-031-14368-7_10.

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3

Scheck, F. "Beyond the Minimal Standard Model." In Electroweak and Strong Interactions, 277–355. Berlin, Heidelberg: Springer Berlin Heidelberg, 1996. http://dx.doi.org/10.1007/978-3-662-03245-9_4.

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4

Langacker, P. "Status of the Standard Electroweak Model." In XXIV International Conference on High Energy Physics, 190–218. Berlin, Heidelberg: Springer Berlin Heidelberg, 1989. http://dx.doi.org/10.1007/978-3-642-74136-4_11.

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5

Altarelli, Guido, and Stefano Forte. "The Standard Model of Electroweak Interactions." In Particle Physics Reference Library, 35–81. Cham: Springer International Publishing, 2020. http://dx.doi.org/10.1007/978-3-030-38207-0_3.

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AbstractIn this chapter, we summarize the structure of the standard EW theory and specify the couplings of the intermediate vector bosons W±, Z and of the Higgs particle with the fermions and among themselves, as dictated by the gauge symmetry plus the observed matter content and the requirement of renormalizability
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6

Böhm, Manfred, Ansgar Denner, and Hans Joos. "Extensions of the Standard Model." In Gauge Theories of the Strong and Electroweak Interaction, 716–41. Wiesbaden: Vieweg+Teubner Verlag, 2001. http://dx.doi.org/10.1007/978-3-322-80160-9_5.

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7

Baur, U. "Electroweak Vector Bosons: Standard Model and Beyond." In XXIV International Conference on High Energy Physics, 1256–64. Berlin, Heidelberg: Springer Berlin Heidelberg, 1989. http://dx.doi.org/10.1007/978-3-642-74136-4_148.

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8

Bilenky, Samoil. "The Standard Model of the Electroweak Interaction." In Introduction to the Physics of Massive and Mixed Neutrinos, 35–65. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-74802-3_3.

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9

Bilenky, Samoil. "The Standard Model of the Electroweak Interaction." In Introduction to the Physics of Massive and Mixed Neutrinos, 29–60. Berlin, Heidelberg: Springer Berlin Heidelberg, 2010. http://dx.doi.org/10.1007/978-3-642-14043-3_3.

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Ho-Kim, Quang, and Xuan-Yem Pham. "The Standard Model of the Electroweak Interaction." In Elementary Particles and Their Interactions, 305–42. Berlin, Heidelberg: Springer Berlin Heidelberg, 1998. http://dx.doi.org/10.1007/978-3-662-03712-6_9.

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Тези доповідей конференцій з теми "Standard Electroweak Model"

1

Frey, Raymond E. "Recent electroweak results from SLC/SLD." In Beyond the standard model. American Institute of Physics, 1997. http://dx.doi.org/10.1063/1.54489.

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2

Wagner, Robert G. "Recent electroweak measurements from the Tevatron." In Beyond the standard model. American Institute of Physics, 1997. http://dx.doi.org/10.1063/1.54494.

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3

Altarelli, Guido. "Electroweak Standard Model." In Corfu Summer Institute on Elementary Particle Physics. Trieste, Italy: Sissa Medialab, 1999. http://dx.doi.org/10.22323/1.001.0001.

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4

Dominici, D. "A strong electroweak sector with decoupling at low energy." In Beyond the standard model. American Institute of Physics, 1997. http://dx.doi.org/10.1063/1.54461.

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5

He, Hong-Jian, Yu-Ping Kuang, and C. P. Yuan. "Probing electroweak symmetry breaking via WW interactions at High Energy Colliders." In Beyond the standard model. American Institute of Physics, 1997. http://dx.doi.org/10.1063/1.54448.

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6

Jikia, Georgy. "Pair production of W bosons at the photon linear collider: a window to the electroweak symmetry breaking?" In Beyond the standard model. American Institute of Physics, 1997. http://dx.doi.org/10.1063/1.54504.

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7

Hollik, Wolfgang. "Status of the electroweak standard model." In The XVI international sympsosium on lepton and photon interactions. AIP, 1994. http://dx.doi.org/10.1063/1.45459.

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8

Erler, Jens. "Electroweak tests of the standard model." In 11TH CONFERENCE ON THE INTERSECTIONS OF PARTICLE AND NUCLEAR PHYSICS: (CIPANP 2012). AIP, 2013. http://dx.doi.org/10.1063/1.4826727.

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9

Valle, J. W. F., and J. Velasco. "Electroweak Physics Beyond the Standard Model." In International Workshop. WORLD SCIENTIFIC, 1992. http://dx.doi.org/10.1142/9789814538091.

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10

Erler, Jens. "Electroweak Standard Model and Precision Tests." In PARTICLES AND FIELDS: Tenth Mexican School on Particles and Fields. AIP, 2003. http://dx.doi.org/10.1063/1.1594339.

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Звіти організацій з теми "Standard Electroweak Model"

1

Koetke, D. D. High sensitivity tests of the standard model for electroweak interactions. Office of Scientific and Technical Information (OSTI), January 1992. http://dx.doi.org/10.2172/5859913.

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2

Rowson, Peter C. A COMBINATION OF PRELIMINARY ELECTROWEAK MEASUREMENTS AND CONSTRAINTS ONTHE STANDARD MODEL. Office of Scientific and Technical Information (OSTI), September 2002. http://dx.doi.org/10.2172/801809.

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3

Abbaneo, J. A Combination of Preliminary Electroweak Measurements and Constraints on the Standard Model. Office of Scientific and Technical Information (OSTI), January 2004. http://dx.doi.org/10.2172/826675.

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4

Su, Dong. A Combination of Preliminary Electroweak Measurements and Constraints on the Standard Model. Office of Scientific and Technical Information (OSTI), May 2003. http://dx.doi.org/10.2172/813338.

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5

De Groot, Nicolo. A Combination of Preliminary Electroweak Measurements and Constraints on the Standard Model. Office of Scientific and Technical Information (OSTI), August 2003. http://dx.doi.org/10.2172/815298.

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Abbaneo, D. A Combination of Preliminary Electroweak Measurements And Constraints on the Standard Model (2004). Office of Scientific and Technical Information (OSTI), March 2005. http://dx.doi.org/10.2172/839900.

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7

Rizzo, Thomas G. Electroweak Precision Measurements and Collider Probes of the Standard Model with Large Extra Dimensions. Office of Scientific and Technical Information (OSTI), June 1999. http://dx.doi.org/10.2172/10055.

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8

Fahland, Tom R. Test of the Electroweak Sector of the Standard Model by Measuring the Anomalous $WW(\gamma)$ Couplings. Office of Scientific and Technical Information (OSTI), January 1997. http://dx.doi.org/10.2172/1421723.

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Koetke, D. D., R. W. Manweiler, and T. D. Shirvel Stanislaus. High sensitivity tests of the standard model for electroweak interactions. [Lepton-family-number-violating decay; Michel [rho] parameter]. Office of Scientific and Technical Information (OSTI), January 1993. http://dx.doi.org/10.2172/6832260.

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10

Kelly, Michael Lawrence. Test of the Standard Model of electroweak interactions by measuring the anomalous $WW\gamma$ couplings at √s = 1.8-TeV. Office of Scientific and Technical Information (OSTI), April 1996. http://dx.doi.org/10.2172/878993.

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