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G. Aad, B. Abbott, D. C. Abbott,A. Abed Abud, K. Abeling, D. K. Abhayasinghe, S. H. Abidi, O. S. AbouZeid,N. L. Abraham, H. Abramowicz, H. Abreu, Y. Abulaiti,

AbstractThis article presents the results of two studies of Higgs boson properties using the $$WW^*(\rightarrow e\nu \mu \nu )jj$$ W W ∗ ( → e ν μ ν ) j j final state, based on a dataset corresponding to $${36.1}{{\mathrm{fb}}^{-1}}$$ 36.1 fb - 1 of $$\sqrt{s}=13$$ s = 13 TeV proton–proton collisions recorded by the ATLAS experiment at the Large Hadron Collider. The first study targets Higgs boson production via gluon–gluon fusion and constrains the CP properties of the effective Higgs–gluon interaction. Using angular distributions and the overall rate, a value of $$\tan (\alpha ) = 0.0 \pm 0.4 (\mathrm {stat.}) \pm 0.3 (\mathrm {syst.})$$ tan ( α ) = 0.0 ± 0.4 ( stat . ) ± 0.3 ( syst . ) is obtained for the tangent of the mixing angle for CP-even and CP-odd contributions. The second study exploits the vector-boson fusion production mechanism to probe the Higgs boson couplings to longitudinally and transversely polarised W and Z bosons in both the production and the decay of the Higgs boson; these couplings have not been directly constrained previously. The polarisation-dependent coupling-strength scale factors are defined as the ratios of the measured polarisation-dependent coupling strengths to those predicted by the Standard Model, and are determined using rate and kinematic information to be $$a_\mathrm {L}=0.91^{+0.10}_{-0.18}$$ a L = 0 . 91 - 0.18 + 0.10 (stat.)$$^{+0.09}_{-0.17}$$ - 0.17 + 0.09 (syst.) and $$a_{\mathrm {T}}=1.2 \pm 0.4 $$ a T = 1.2 ± 0.4 (stat.)$$ ^{+0.2}_{-0.3} $$ - 0.3 + 0.2 (syst.). These coupling strengths are translated into pseudo-observables, resulting in $$\kappa _{VV}= 0.91^{+0.10}_{-0.18}$$ κ VV = 0 . 91 - 0.18 + 0.10 (stat.)$$^{+0.09}_{-0.17}$$ - 0.17 + 0.09 (syst.) and $$\epsilon _{VV} =0.13^{+0.28}_{-0.20}$$ ϵ VV = 0 . 13 - 0.20 + 0.28 (stat.)$$^{+0.08}_{-0.10}$$ - 0.10 + 0.08 (syst.). All results are consistent with the Standard Model predictions.

2022The European Physical Journal C（2022）引用：10

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12Search for New Phenomena in Final States with Photons, Jets and Missing Transverse Momentum in Pp Collisions at S\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \Setlengt

G. Aad, B. Abbott, D. Abbott,A. Abed Abud,K. Abeling, D. K. Abhayasinghe, S. Abidi,A. Aboulhorma,H. Abramowicz,H. Abreu,Y. Abulaiti, A. Abusleme Hoffman,

2022Journal of High Energy Physics（2022）引用：18

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13Search for Light Long-Lived Neutral Particles That Decay to Collimated Pairs of Leptons or Light Hadrons in Pp Collisions at S\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \Usepackage{upgre

G. Aad, B. Abbott, D. Abbott,A. Abed Abud,K. Abeling,D. Abhayasinghe, S. Abidi,A. Aboulhorma,H. Abramowicz,H. Abreu,Y. Abulaiti, A. Abusleme Hoffman,

2022Journal of High Energy Physics（2022）引用：9

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14Search for Heavy, Long-Lived, Charged Particles with Large Ionisation Energy Loss in Pp Collisions at S\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \Setlength{\oddside

G. Aad, B. Abbott, D. Abbott,A. Abed Abud, K. Abeling, D. Abhayasinghe, S. Abidi, A. Aboulhorma,H. Abramowicz,H. Abreu,Y. Abulaiti, A. Abusleme Hoffman,

2022Journal of High Energy Physics（2022）

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15Measurement of the W Boson Mass

F ABE,MG ALBROW,SR AMENDOLIA,D AMIDEI,J ANTOS,C ANWAYWIESE,G APOLLINARI,H ARETI,M ATAC,P AUCHINCLOSS,F AZFAR,P AZZI,

We present a measurement of the W boson mass in W-->e(nu) decays using 1 fb-1 of data collected with the D0 detector during Run II of the Fermilab Tevatron collider. With a sample of 499830 W-->e(nu) candidate events, we measure M(W)=80.401+/-0.043 GeV. This is the most precise measurement from a single experiment.

2022Journal of High Energy Physics引用：472

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16High-precision Measurement of the W Boson Mass with the CDF II Detector

T Aaltonen,S Amerio,D Amidei,A Anastassov,A Annovi,J Antos,G Apollinari,J A Appel, T Arisawa,A Artikov,J Asaadi,W Ashmanskas,

The mass of the W boson, a mediator of the weak force between elementary particles, is tightly constrained by the symmetries of the standard model of particle physics. The Higgs boson was the last missing component of the model. After observation of the Higgs boson, a measurement of the W boson mass provides a stringent test of the model. We measure the W boson mass, M W , using data corresponding to 8.8 inverse femtobarns of integrated luminosity collected in proton-antiproton collisions at a 1.96 tera–electron volt center-of-mass energy with the CDF II detector at the Fermilab Tevatron collider. A sample of approximately 4 million W boson candidates is used to obtain M W = 80 , 433.5 ± 6.4 stat ± 6.9 syst = 80 , 433.5 ± 9.4 MeV / c 2 , the precision of which exceeds that of all previous measurements combined (stat, statistical uncertainty; syst, systematic uncertainty; MeV, mega–electron volts; c , speed of light in a vacuum). This measurement is in significant tension with the standard model expectation.

2022Science (New York, NY)

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17Erratum To: Higgs Boson Production Cross-Section Measurements and Their EFT Interpretation in the $$4\ell $$ 4 ℓ Decay Channe

G. Aad,B. Abbott, D. Abbott,A. A. Abud,K. Abeling,D. K. Abhayasinghe,S. H. Abidi,O. AbouZeid,N. Abraham,H. Abramowicz,H. Abreu,Y. Abulaiti,

In the published HTML version of this article, the affiliations of the authors of the National Research Nuclear University MEPhI, Moscow, Russia were unfortunately marked incorrectly.

2021The European Physical Journal C引用：5

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18Measurement of hadronic event shapes in high-p(T) multijet final states at root s = 13 TeV with the ATLAS detector (vol , 188, 2021)

G. Aad,B. Abbott,D. C. Abbott,A. Abed Abud,K. Abeling,D. K. Abhayasinghe,S. H. Abidi,O. S. AbouZeid,N. L. Abraham,H. Abramowicz,H. Abreu,Y. Abulaiti,

An error in the normalization of the Aplanarity and D-parameter has been found. Insufficient precision on the eigenvalue calculation can cause lambda(3) to be negative, exclusively in two-jet events, yielding an underestimation of the inclusive two-jet cross section.

2021JOURNAL OF HIGH ENERGY PHYSICS（2021）引用：5

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19Search for Supersymmetry in Events with Four or More Charged Leptons in 139 Fb−1 of S\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \Setlength{\oddsidemargin}{-69Pt} \Be

G. Aad, B. Abbott, D. Abbott,A. Abed Abud,K. Abeling,D. Abhayasinghe, S. Abidi,O. AbouZeid,N. Abraham,H. Abramowicz,H. Abreu,Y. Abulaiti,

2021Journal of High Energy Physics（2021）

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20Measurement of the Charge Asymmetry of Electrons from the Decays of $W$ Bosons Produced in $p\bar{p}$ Collisions at $\sqrt{s}=1.96$ TeV

T. Aaltonen,S. Amerio,D. Amidei,A. Anastassov,A. Annovi,J. Antos,G. Apollinari,J. A. Appel,T. Arisawa,A. Artikov,J. Asaadi,W. Ashmanskas,

At the Fermilab Tevatron proton-antiproton ($p\bar{p}$) collider, high-mass electron-neutrino ($e\nu$) pairs are produced predominantly in the process $p \bar{p} \rightarrow W(\rightarrow e\nu) + X$. The asymmetry of the electron and positron yield as a function of their pseudorapidity constrain the slope of the ratio of the $u$- to $d$-quark parton distributions versus the fraction of the proton momentum carried by the quarks. This paper reports on the measurement of the electron-charge asymmetry using the full data set recorded by the Collider Detector at Fermilab in 2001--2011 and corresponding to 9.1~fb$^{-1}$ of integrated luminosity. The measurement significantly improves the precision of the Tevatron constraints on the parton-distribution functions of the proton. Numerical tables of the measurement are provided.

2021PHYSICAL REVIEW D（2021）引用：1

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