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- Indico Weeks View
After about one year from the release of the new
The workshop will be held in person (if you are interested in registering for remote attendance, please contact Emanuele Bagnaschi -- emanuele.bagnaschi@cern.ch).
Confirmed speakers:
Organizing committee
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, MW, using data corresponding to 8.8 inverse femtobarns of integrated luminosity collected in proton-antiproton collisions at a 1.96 TeV 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 MW=80,433.5±6.4stat±6.9syst=80,433.5±9.4 MeV/c2, the precision of which exceeds that of all previous measurements combined. This measurement is in significant tension with the standard model expectation.
This talk will review the ATLAS measurement of the W-boson mass, with an emphasis on the recent reanalysis of 7 TeV data, and on the uncertainties due to the modelling of the vector boson production and decay.
Precision measurements of W Boson production are of great interest in improving understanding of the proton structure, and as a precursor to measurements of the W mass. Measurements of differential and polarized W production cross sections will be discussed, including implications for improving knowledge of the proton PDF. Preliminary studies of experimental aspects of W mass measurements using Z events as a proxy
will also be discussed.
With the analysis of 2016 data provided by the LHC, the LHCb Collaboration demonstrated its capability in a measurement of the W boson mass. By including data collected in 2017 and 2018, the statistical precision will be improved by roughly a factor of two. Many efforts are being put in-place in order to reduce both the experimental and theoretical systematic uncertainties via a more detailed study of the detector effects and the modelling of the W boson production at the LHC.
The LHCb Collaboration is currently analyzing all the data collected in the Run 2 (2016-2018) of the LHC following a more careful treatment of the curvature biases and detector efficiencies, as well as exploring the most recent developments in the event generators and parton distribution functions (PDFs). The measurement of the W mass at LHCb is particularly interesting due to the anti-correlation of the PDF uncertainties with respect to ATLAS and CMS, since it provides a complementary coverage in pseudorapidity.
A combination of all the measurements at the LHC will allow to achieve a sensitivity closer to the global EW fit, and help to clarify the picture around the W boson mass after the most recent results.
This talk will attempt to summarise the main issues related to achieving a 10-15 MeV precision on a W mass measurement at hadron colliders today. These cover crucial experimental aspects (muon momentum scale, hadronic recoil, pile-up) and also physics modelling issues, mostly related to the theoretical knowledge of pTW/pTZ in a region where resummation, heavy flavour, and non-perturbative contributions matter more than fixed-order perturbative calculations.
The calculation of fixed-order predictions at the third perturbative order (N3LO) in the NNLOJET framework is presented, as well predictions further matched to transverse momentum resummation at N3LL with the RadISH framework. A focus will be paced on the phenomenological impact of these corrections, the associated theory uncertainties, and the computational challenges.
In this talk we will present selected QCD resummed predictions for the Drell-Yan process. In particular, the recent N4LL QCD calculation will be discussed and also the QCD+QED NLL results will be presented.
This seminar presents a precise measurement of the production properties of the Z-boson in the full phase space of the decay leptons, based on 8 TeV pp collision data collected by the ATLAS experiment in 2012. The double-differential cross-section distributions in Z-boson transverse momentum and rapidity are measured in the pole region. In a novel approach, the measured Z transverse momentum is used to determine the strong coupling constant. The analysis uses state-of-the-art predictions at third order accuracy in perturbative QCD, supplemented by resummation of logarithmically-enhanced contributions in the small transverse-momentum region of the lepton pairs. The extracted
See also https://indico.cern.ch/event/1231802/ .
High-precision DY predictions are a crucial ingredient in current W-boson mass analyses. I present predictions at the level of
In a second part I give a brief overview of the activities of the LHC EWWG, where various groups benchmark DY transverse-momentum resummation and push developments towards more precise DY modeling.
I will review the traditional approach for the determination of the W boson mass at hadron colliders from the kinematical distributions of the charged-current Drell-Yan process. I will then present a new observable which allows this determination, with the possibility of a simple discussion and estimate of the associated QCD uncertainties.
The calculation of radiative corrections to resonance processes poses issues with gauge invariance owing to the necessary mix of perturbative orders after some Dyson summation of the potentially resonant propagator corrections. The talk reviews various schemes proposed to cure this problem and quantifies the corresponding theory uncertainties in the evaluation of electroweak corrections to Drell-Yan-like W/Z production. NLO electroweak corrections to W/Z production are also discussed for some scenarios of physics beyond the Standard Model such as a singlet Higgs extension, the Two-Higgs-Doublet Model, and the Minimal Supersymmetric Standard Model.
The determination of Parton Distribution Functions (PDFs) is a crucial theoretical input for precise electroweak measurements at hadron colliders, in particular for the W mass measurements at the LHC. In this talk, I will describe the methodological advances in modern PDF determinations, with a particular focus on NNPDF. I will then mention new interesting challenges that modern fits of PDFs face at the precision frontier, in which it is crucial to assess the robustness of the uncertainties associated with the theory predictions.
How well do we know the inner structure of protons? The answer depends not only on the precision of experimental measurements and theoretical predictions but, as was pointed out recently, on the procedure of sampling of the allowed PDF solutions over the multidimensional parameter space. With large data samples, phenomenological PDF fits are at a risk of the big-data paradox, which takes over the law of large numbers and implies that more experimental data do not automatically raise the accuracy of PDFs. Close attention to the data quality and sampling of possible PDF solutions is as essential, as well as the distinction between aleatory and epistemic uncertainties. I will summarize efforts in the CTEQ-TEA group to understand and reduce all such PDF uncertainties and provide independent methods to validate PDF uncertainty estimates in precision EW measurements.
For those who have expressed interest, we have reserved a place for us at the "Le Gruyérien - Plainpalais" at 20.30.
Restaurant Le Gruyérien
Boulevard de Saint-Georges 65
1205 Genève
Tél. +41 22 320 81 84
https://www.le-gruyerien.ch/gruyerien/plainpalais/
https://goo.gl/maps/HJizqEXBDF9nQd9w6
This talk will give an overview of the prospects for future e+e- colliders to make incisive measurements of the W mass with techniques that are highly complementary to the hadron collider approach. Examples will be drawn from ILC and other accelerator designs such as FCC-ee and ReLiC and will cover threshold lineshape based measurements and continuum reconstruction of the W mass as was already established at LEP2.
The bottom line is that the next generation of colliders designed for exploring the Higgs will also be very well equipped for advancing our knowledge of the W mass to MeV level precision either concurrently with ZH production operation or with operation near WW threshold.
An overview is given on the the various steps to get precise SM predictions of the W-boson mass from a given set of input parameters (Fermi constant, electromagnetic fine structure constant, Z-boson mass, top-quark and Higgs-boson masses, strong coupling constant), in the on-shell scheme and the MS-bar scheme. The current status is reviewed, topical predictions and their uncertainties are presented and discussed.
We discuss the role of MW in the context of global fits of electroweak precision observables, and the compatibility of the current experimental value with the SM. We then generalize the analysis to physics beyond the SM, considering oblique NP and the SMEFT.
I will discuss the interpretation of the recent CDF W mass measurement as part of a global analysis in the SMEFT framework at linear, dimension-6 level. Combining data from EW precision observables, Higgs signal strengths and diboson production allows for the identification of the preferred regions of parameter space in light of this measurement. I will also discuss how one can use the SMEFT results to determine which single-field extensions of the SM are able to account for the deviation. Finally I will comment on the impact of dimension-8 effects in a model with a hyper charge-zero electroweak triplet scalar in relation to the W-mass anomaly.
I will discuss the combination procedure of measurements with correlated uncertainties, including a brief description of the general formalism assuming multivariate Gaussian distributions,as well as concrete examples of a simplified approach. I will also comment on PDG scale factors and an alternative.
I will investigate the capability of the 2HDM+a of accommodating the recently reported anomalies in the measurements of the mass of the W and g-2. Potential connections with the DM puzzle will be also investigated.
One year ago, the CDF collaboration reported a new precision measurement of the
In this talk, I will investigate possible new physics contributions to
We critically analyse the future of composite dynamics via the impact of non standard model Higgs on the (non) observed g-2 and W-mass anomalies.
We show that a larger W boson mass can be explained by nonaligned vacuum expectation values of isospin triplet scalar fields in the Georgi-Machacek model extended with custodial symmetry-breaking terms in the potential. The latter is required to avoid an undesirable Nambu-Goldstone boson as well as to be the consistent treatment of radiative corrections. With the W mass as one of the renormalization inputs at the one-loop level, we derive the required difference in the triplet vacuum expectation values, followed by a discussion of phenomenological consequences in the scenario.
It is known that the recently reported shift of the W boson mass can be easily explained by an
Surprisingly, the addition of a TeV scale complex triplet Higgs boson to the standard model leads to a precise unification of the gauge couplings at around
Although it seems the proton decay constraints would doom such a low uni cation scale, I will show that the constraints can be avoided by introducing vector-like fermions which mix with the SM fermions through mass terms involving the GUT breaking Higgs field.
As I will discuss, this will lead to a scenario which is not ruled out but could be tested in near future proton decay experiments. Importantly, the simplest viable model only requires the addition of one pair of vector-like fermions transforming 10 and 10.
I will also discuss a minor tweak to this model which will allow us to identify the other triplet as dark matter. Lastly, I will discuss the more general ramifications of the W boson mass for grand unification .
In this talk I consider the W mass, assuming that a measured value different from the SM prediction is due to BSM physics, within the bigger picture of signs for new physics (anomalies). In particular, a positive shift in the W mass can be obtained with leptoquarks, vector-like quarks, Z' bosons and a scalar triplet (Y=0). I discuss which anomalies can be explained by these particles as well and to which interesting experimental signals these SM extensions lead.
We discuss a possibility to probe a large class of scenarios beyond the Standard Model simultaneously explaining the recent CDF II measurement of the W boson mass and predicting first-order phase transitions testable in future gravitational-wave experiments. We discuss this methodology focusing on a specific example of the Standard Model extension with an additional scalar