• Non ci sono risultati.

fulltext

N/A
N/A
Protected

Academic year: 2021

Condividi "fulltext"

Copied!
2
0
0

Testo completo

(1)

DOI 10.1393/ncc/i2015-15046-9 Colloquia: IFAE 2014

IL NUOVO CIMENTO 38 C (2015) 46

Measurement of the Higgs boson properties with the ATLAS

detector

A. Gabriellion behalf of the ATLAS Collaboration

Dipartimento di Fisica, Universit`a di Roma “Sapienza”, Roma, Italy

INFN, Sezione di Roma 1, Piazzale Aldo Moro 2, 00185, Roma, Italy

received 7 January 2015

Summary. — In this paper, a brief overview of the results, based on proton-proton collision data recorded at a centre-of-mass energy of 7 TeV in 2011 and 8 TeV in 2012, for the properties of a new Higgs-like particle at 125.5 GeV are presented.

PACS 14.80.Bn – Standard Model Higgs bosons.

1. – Mass and signal strength

The mass of the newly discovered boson can be measured precisely in the high mass

resolution channels H→ γγ and H → ZZ(∗)→ 4l. Figure 1 shows the profile likelihood

ratio as a function of mHfor H→ γγ and H → ZZ(∗)→ 4l channels and their

combina-tion. The combined mass is measured to be mH= 125.5± 0.2(stat)+0.5−0.6(sys) GeV [1].

2. – Couplings

The signal strength scale factors μi,f for either the Higgs production or decay modes

were determined. However, for a consistent measurement of Higgs boson couplings, pro-duction and decay modes cannot be treated independently. The framework and bench-marks as recommended in ref. [2], measurements of coupling scale factors are implemented using a LO tree level motivated framework ref. [3]. For these measurements the following

channels are used: γγ, ZZ∗, W W∗, b¯b and τ τ .

Fermion versus vector (gauge) couplings. – This benchmark is an extension of the

single parameter fit, where different strengths for the fermion and vector couplings are

probed. It assumes that only SM particles contribute to the H→ γγ and gg → H vertex

loops, but any modification of the coupling strength factors for fermions and vector bosons are propagated through the loop calculations. In fig. 2 (left) there is a plot with

the best-fit of κV and κF with 68% CL contours.

(2)

2 A. GABRIELLI on behalf of the ATLAS COLLABORATION [GeV] H m 121 122 123 124 125 126 127 128 129 Λ -2ln 0 1 2 3 4 5 6 7 σ 1 σ 2 Preliminary ATLAS -1 Ldt = 4.6-4.8 fb ∫ = 7 TeV: s -1 Ldt = 20.7 fb ∫ = 8 TeV: s Combined (stat+sys) Combined (stat only)

γ γ → H l 4 → (*) ZZ → H

Fig. 1. – The profile likelihood ratio −2 ln Λ(mH) as a function of mH for the H → γγ and

H→ ZZ(∗)→ 4l channels and their combination, obtained by allowing the signal strengths μγγ

and μ4lto vary independently.

V κ 0.8 0.9 1 1.1 1.2 1.3 1.4 F κ -1.5 -1 -0.5 0 0.5 1 1.5 2 2.5 3 SM Best fit 68% CL 95% CL ATLASPreliminary -1 Ldt = 4.6-4.8 fb ∫ = 7 TeV, s -1 Ldt = 20.3 fb ∫ = 8 TeV, s b ,b τ τ ,ZZ*,WW*, γ γ → Combined H γ κ 0.8 0.9 1 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 g κ 0.6 0.8 1 1.2 1.4 1.6 1.8 2 2.2 2.4 SM Best fit 68% CL 95% CL ATLASPreliminary -1 Ldt = 4.6-4.8 fb ∫ = 7 TeV, s -1 Ldt = 20.3 fb ∫ = 8 TeV, s b ,b τ τ ,ZZ*,WW*, γ γ → Combined H

Fig. 2. – Correlation of the coupling scale factors κF–κV (left) and κg–κγ (right) with 68% CL

contours.

Loop structure. – Many BSM physics scenarios predict the existence of new heavy

particles, which can contribute to loop induced processes such as gg → H production

and H→ γγ decay. Effective scale factors κgand κγ are introduced to parameterise the

gg→ H and H → γγ loops to probe for contributions from non-SM particles in these

pre-cesses. In fig. 2 (right) there is a plot with the best-fit of κgand κγwith 68% CL counturs.

3. – Conclusions

Using data taken in 2011 and 2012, at centre-of-mass energies of respectively 7 TeV and 8 TeV, the ATLAS collaboration has reported the observation of a new particle with

a mass of mH = 125.5 GeV, in the search for the Standard Model Higgs boson. Within

the current statistical uncertainties and assumptions, no significant deviations from the Standard Model couplings are observed.

REFERENCES

[1] ATLAS Collaboration, “Combined measurements of the mass and signal strength of the Higgs-like boson with the ATLAS detector using up to 25 fb-1 of proton-proton collision data,” AATLAS-CONF-2013-014.

[2] LHC Higgs Cross Section Working Group,“LHC HXSWG interim recommendations to explore the coupling structure of a Higgs-like particle”, arXiv:1209.0040[hep-ph]. [3] ATLAS Collaboration, “Higgs couplings combination”. ATLAS-CONF-2014-009.

Riferimenti

Documenti correlati

This paper presents a system of propositional logic equipped with suitable modal operators to speak of rationality of players in finite games in normal form, and tries to

In this work we present a Global Emission Game with N asymmet- ric players, in which the pay-off of cooperators is affected by a Social Externalities, that we assume to be a

In the paper we have discussed how an agent based modeling techniques, combined with an evolutionary learning algorithm, resulted in a learning simulator, L-FABS, able to acquire

The fit parameters chosen for the combined STXS measurements are the cross sections for Higgs boson production in STXS region i times the branching fraction for the H → ZZ  decay, ðσ

Theoretical values for the bulk materials show, that both have a high refractive index but unfortunately the deposited amorphous layers have a higher than desirable

This paper reviews relevant programmatic and technological issues, as well as possible approaches for addressing these issues—including direct fabrication of monocrystalline

Negli ultimi anni è stato svolto un proficuo lavoro di collaborazione tra l’Agenzia per l’Italia Digitale, il Ministero della Salute, il Ministero dell’Economia e delle Finanze,