Higgs (ATLAS/FCC)

Particles of the Standard Model of particle physics (Image: Daniel Dominguez/CERN)


The Higgs boson (H) plays a prominent role in the Standard Model (SM) of particle physics: the related Higgs field, which permeates the Universe, is responsible for the spontaneous breaking of electroweak symmetry and the origin of the masses of the elementary particles. Its role in the theory and its atypical properties (notably its spin 0) make it a fundamental subject of study, that might also have potential cosmological implications.

Since March 2021 a "Higgs'' team, working on the measurement of the properties of the Higgs boson with data from the ATLAS (A Toroidal Large ApparatuS) experiment at the Large Hadron Collider (LHC) at CERN and on the preparation of the Future Circular Collider (FCC) project has joined the Particles group. 

 

ATLAS

The ATLAS experiment (Figure 1) is a multipurpose detector, 46 m long, 25 m high, weighing 7000 tonnes, located about 100 m below ground around one of the collision points of the LHC's counter-rotating beams. It consists of six different detecting subsystems arranged concentrically, to record the momenta and directions of the particles produced in the collisions between the protons that are accelerated by the LHC. The measured quantities are used to investigate a wide range of physics processes, such as strong interactions, electroweak production of W and Z bosons, top quark and Higgs boson properties, and to search for hypothetical phenomena beyond the Standard Model such as extra dimensions or dark matter particles.

Figure 1. The ATLAS detector

After the first two data-taking phases (Run 1: 2010-2012, Run 2: 2015-2018), the LHC has entered its third data-taking period (Run 3: 2022-2025), which will be followed by a 2-year long shutdown for detector and collider upgrades  that will lead to the so-called high-luminosity phase of the LHC (HL-LHC: 2028-2040). The energy in the proton-proton center-of-mass system has gradually increased from 7-8 TeV in Run 1 to 13 TeV in Run 2 to 13.6 TeV in Run 3; it should reach its design value of 14 TeV at HL-LHC.


Scientific contributions

Since the beginning of the LHC data taking, our team has focused on the physics of the Higgs boson. It contributed to its discovery at the LHC Run 1 using its decays into two photons [1], and to the demonstration of its Yukawa couplings to the fermions of the SM through the observation of its decays into bottom quark pairs with data from Run 2 [2]. We also measured the Higgs boson mass with diphoton decays and searched for the rare Higgs boson decays to a Z boson and a photon.

Recently, our team has worked on the following analyses of the full set of proton-proton (pp) collisions collected by ATLAS during the LHC Run2:

  • The measurement of the Higgs boson production cross sections using the H→bb [3] and H→γγ [4] decays.  The H→bb decay has a large branching ratio (58%) but suffers from large background from QCD multihadron production, while the H→γγ decay has small branching ratio (0.22%) but much lower backgrounds. The cross sections are measured as a function of several kinematic quantities which can be used to probe different Higgs production mechanisms and to look for deviations from the predictions of the SM.  All the measurements are found to be in agreement with the Standard Model predictions and constraints are set on the Yukawa couplings of the Higgs boson to the bottom and charm quarks and on anomalous Higgs boson couplings to vector bosons in the Standard Model effective field theory framework.
  • The most sensitive search for the (never observed before) rare Higgs boson decay to Zγ [5]. A hint of an excess with respect to the expected background was found in the data, with a best-fit value for the signal yield normalised to the Standard Model prediction was 2.0 ± 1.0; a similar excess was found by CMS, which might hint to a possible deviation from the SM expectation that will be further investigated with more data in Run 3. The combination of our results with those by CMS [6] led fo the first evidence for this rare decay.
  • The search for the production of pairs of Higgs bosons (HH). This process is the portal to measuring the Higgs boson self-coupling parameter λ and thus the potential of the Higgs boson. We focused on the search for di-Higgs production in the final state bbγγ [7] and the final state bbττ [8], the two most sensitive final states. The analysis of the full ATLAS data collected in Run 2 of the LHC found no excess over the background. We also contributed to the combination of these results [9], which set an upper bound, with a 95% confidence level (CL), of 2.9 times the SM prediction. The result implies the following constraint on the Higgs boson self-coupling modifier κλ = λ/λSM: -1.2 < κλ < 7.2 at 95% CL, which is the tightest constraint on Higgs boson self-interactions to date. 
We also started to analyze the first LHC Run 3 data, with a first measurement of the production cross section of the Higgs boson at √s=13.6 TeV [10], and for the search for HH production in the final state bbττ.


Technical contributions 

The quality of the results of the ATLAS experiment requires proper functioning of the detector as well as a detailed understanding of the objects used in the analyses. Recently our team has been focusing on:
  • The improvement of the performance of identification of prompt photons and of rejections of candidate photons coming either from the decay of a neutral meson in a hadronic shower, or from the electromagnetic shower initiated by an electron, for the LHC Run 3 [11].
  • The characterization of the reconstruction and tagging performance of jets of particles resulting from the hadronization of a b quark, with two measurements in situ of (i) the calibration of the energy scale of the b-quark jets using ttbar events followed by a t → Wb →qqb decay and the known top quark mass [12], and (ii) the efficiency of identifying a b-quark jet, using a fit to the momentum distribution of a muon in a jet relative to the axis of the jet+muon system. [13]
  • The measurement of radiation damage to the ATLAS tracker pixel sensors [14], [15] and its implementation in the ATLAS detector simulation. With increasing luminosity radiation damage effects are not negligible, and it will be important to account for them in the simulations for the future LHC data taking phases. Methods to make simulations - that include radiation damage effects - faster are being developed by our team [16]
  • The construction and software development of the future silicon vertex detector ("ITk'') of the ATLAS experiment for the HL-LHC. We are working on the development of the digitization code of the ITk pixel sensors, and on the construction of the ITk pixel detector, having contributed to the market survey process of the various vendors of sensors and to the preparation of the next phase of pre-production and testing of modules. [17]

 

FCC

The Future Circular Collider is a proposed integrated project of next-generation collider of about 90 km in length proposed to take over from the LHC (Figure 2).
It should start during the 2040's with an initial electron-positron phase (FCC-ee) lasting around 8 years, to study in detail the properties of the electroweak bosons (W, Z), of the Higgs boson and of top quarks, running at center-of-mass energies of 91 GeV, 160 GeV, 240 GeV and 350-365 GeV, followed by a shutdown for machine and detector upgrades and then by a second data-taking phase (FCC-hh) in which proton beams would provide collisions at center of mass energies of 100 TeV or above.

Figure 2. Illustration of the potential location of the Future Circular Collider at CERN, near Geneva. Also shown are the CERN PS, SPS and LHC rings, which would be part of the FCC injection and acceleration chain.

 

Scientific contributions

Our team is contributing to the development of the physics case of the electron-positron phase of the future circular collider. The FCC-ee offers unprecedented opportunities to determine Higgs boson parameters, with over 10 million e+e- → ZH events and nearly 100 thousand WW → H events produced at center-of-mass energies around 240 and 365 GeV and with a much lower background than at the LHC, and without pileup effects. Another advantage over the LHC is related to the complete knowledge of the kinematics of the colliding e+e- particles, which makes it possible to identify the ZH events with the "recoil mass" technique, reconstructing the products of the decays of the Z boson and therefore - thanks to the conservation of energy and total momentum - the mass of the system recoiling against the Z boson. 

In spring 2021 we carried out first studies of the precision that FCC-ee could expect on the cross section of the ZH process and on the mass of the Higgs boson [18] and on its hadronic couplings (to b and c quarks and gluons), using signal and background noise events generated and interfaced to a parametric simulation of the detector response. These initial studies will be updated according to the different technologies and projects proposed for the FCC-ee detectors, optimizing the selection criteria and the fit strategies to further improve the sensitivity of the analysis [19], in view of a "Feasibility Study Report'' by 2025 for the update of the European strategy for particle physics. This will mark the completion of the FCC-ee feasibility study, and will allow the CERN Council to decide whether the project can proceed with the start of the excavation of the FCC tunnel.
Since early 2023 we are also working on the development of Geant4 simulations of a detector concept for FCC-ee (ALLEGRO [20]) centered around a high-granularity electromagnetic calorimeter. We have developed several tools for the reconstruction and identification of photons and electrons and we use them to optimize the detector design to maximize its performance.


Team members

Staff Post-docs
  • Tong LI (2023-2024)
PhD students
  • Alexis MALOIZEL (1st year, 2023-2026)
Click here for the team photo


Former post-docs

  • Giulia DI GREGORIO (2022-2023)


Former PhD students

  • Keerthi NAKKALIL (2021-2024)
  • Qiuping SHEN (2021-2024)
  • Yulei ZHANG (2021-2023)
  • Ang LI (2020-2023)
  • Romain BOUQUET (2019-2023)
  • Reem TAIBAH (2018-2021)
  • Ahmed TAREK (2016-2019) - ATLAS Thesis award 2020
  • Ilaria LUISE (2016-2019)
  • Audrey DUCOURTHIALl (2015-2018)
  • Changqiao LI (2015-2018)
  • Dilia PORTILLO (2015-2018)
  • Stefano MANZONI (2014-2017) - ATLAS Thesis award 2018
  • Kun LIU (2011-2014) - ATLAS Thesis award 2015


Useful Links

ATLAS

FCC


References

[1] ATLAS Collaboration, “Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC,” Phys. Lett. B716, 1–29 (2012), arXiv:1207.7214
[2] ATLAS Collaboration, "Observation of H->bb decays and VH production with the ATLAS detector", Phys. Lett. B 786 (2018) 59, arXiv:1808.08238
[3] ATLAS Collaboration, “Measurements of WH and ZH production in the H→bb decay channel in pp collisions at 13 TeV with the ATLAS detector,” Eur. Phys. J. C 81, 178 (2021), arXiv:2007.02873
[4] ATLAS Collaboration, "Measurements of the Higgs boson inclusive and differential fiducial cross-sections in the diphoton decay channel with pp collisions at √s=13 TeV with the ATLAS detector", arXiv:2202.00487
[5] ATLAS Collaboration, "A search for the Zγ decay mode of the Higgs boson in pp collisions at √s = 13 TeV with the ATLAS detector", Phys. Lett. B 809 (2020) 135754 arXiv:2005.05382
[6] ATLAS and CMS Collaborations, "Evidence for the Higgs boson decay to a Z boson and a photon at the LHC", ATLAS-CONF-2023-025
[7] ATLAS Collaboration, "Studies of new Higgs boson interactions through nonresonant HH production in the bbγγ final state in pp collisions at √s = 13 TeV with the ATLAS detector", JHEP 01, 066 (2024), arXiv:2310.12301 [hep-ex]
[8] ATLAS Collaboration, “Search for the non-resonant production of Higgs boson pairs via gluon fusion and vector-boson fusion in the bbττ final state in proton-proton collisions at √s = 13 TeV with the ATLAS detector,” Phys. Rev. D 110, 032012 (2024), arXiv:2404.12660 [hep-ex]
[9] ATLAS Collaboration, “Combination of searches for Higgs boson pair production in pp collisions at √s= 13 TeV with the ATLAS detector,” Phys. Rev. Lett. 133, 101801 (2024), arXiv:2406.09971 [hep-ex]
[10] ATLAS Collaboration, “Measurement of the H → γγ and H → ZZ∗ → 4l cross-sections in pp collisions at √s = 13.6 TeV with the ATLAS detector,” (2023), arXiv:2306.11379 [hep-ex]
[11] Q. Shen, "Constraints on Higgs Self-coupling via HH→bbγγ and Joint Interpretation of Single- and Double-Higgs Analyses Using Data Collected with the ATLAS Detector at √s=13 TeV", CERN-THESIS-2024-240
[12] ATLAS Collaboration, "Energy scale calibration of b-tagged jets with ATLAS Run 2 data using ttbar lepton+jets events", ATLAS-CONF-2022-004
[13] A. Li, Search for di-Higgs production and measurement of the Higgs boson self-coupling in the final state with a pair of b quarks and a pair of tau leptons with the ATLAS detector at the LHC, Perspectives on the measurement of the Higgs boson mass and the electron-positron to ZH cross-section at the Future Circular Collider, CERN-THESIS-2024-035
[14] ATLAS Collaboration, "Measurements of sensor radiation damage in the ATLAS inner detector using leakage currents", JINST 16 (2021) P0802, arXiv:2106.09287
[15] ATLAS Collaboration, Sensor Response and Radiation Damage Effects for the 3D Pixel in the ATLAS IBL Detector, JINST 19 (2024) P10008 (https://arxiv.org/abs/2407.05716)
[16] M. Bomben, K. Nakkalil, A lightweight algorithm to model radiation damage effects in Monte Carlo events for High-Luminosity LHC experiments, Sensors 2024, 24(12), 3976 (https://doi.org/10.3390/s24123976)
[17] K. Nakkalil, Amélioration du détecteur de traces (ITk) pour la phase haute luminosité d’ATLAS et mesure de la section efficace de production du boson de Higgs at 13.6 TeV, CERN-THESIS-2024-270
[18] P. Azzurri et al, "A special Higgs challenge: Measuring the mass and production cross section with ultimate precision at FCC-ee", https://arxiv.org/abs/2106.15438, EPJ+ Focus Point on A future Higgs and Electroweak factory (FCC): Challenges towards discovery
[19] B. Auchmann et al, "FCC Midterm Report", https://repository.cern/records/511pr-rd590(2024)
[20] ALLEGRO web page, https://allegro.web.cern.ch/
 


For more details

APC activity report 2017-2021: https://apc.u-paris.fr/APC_CS/en/activity-report
Publications, theses/internships/post-docs supervised: 
https://apc.u-paris.fr/APC_CS/sites/default/files/u666/apc_higgs_team_scientific_production.pdf