CMS-PAS-SMP-20-008 | ||
Search for the rare exclusive hadronic decay of a W boson into a pion and a photon in proton-proton collisions at 13 TeV | ||
CMS Collaboration | ||
July 2020 | ||
Abstract: A search is performed for the rare exclusive hadronic decay W→πγ in pp collisions at √s= 13 TeV. Data collected by the CMS experiment at the LHC during the 2016, 2017 and 2018 data-taking periods, which correspond to an integrated luminosity of 137 fb−1, are analyzed. The analysis exploits the W boson production from tˉt events. The leptonic decay of the W boson from one of the top quarks is used to tag the event, and the b-jets are exploited to reduce the QCD background from the hadronization of light quarks. The W boson originating from the other top quark is used to search for the W→πγ decay. The rare decay is characterized by a high-transverse momentum, isolated track and a high-energy, isolated photon. The W→πγ decay is not observed, and an upper limit is set to its branching fraction, corresponding to 1.51 × 10−5 at 95% confidence level. | ||
Links:
CDS record (PDF) ;
CADI line (restricted) ;
These preliminary results are superseded in this paper, PLB 819 (2021) 136409. The superseded preliminary plots can be found here. |
Figures | |
![]() png pdf |
Figure 1:
Distribution of the pion isolation variable. In the signal MC, represented by the dashed red line, the branching fraction for W→πγ is 10−2. |
![]() png pdf |
Figure 2:
Distributions of the BDT score for the muon (left) and electron (right) channels. |
![]() png pdf |
Figure 2-a:
Distribution of the BDT score for the muon channel. |
![]() png pdf |
Figure 2-b:
Distribution of the BDT score for the electron channel. |
![]() png pdf |
Figure 3:
Distribution of mπγ for the sum of the lepton channels. In the MC signal, represented by the dashed red line, the branching fraction for W→πγ is assumed to be 10−4. The blue line represents the best fit to the data using the model described in Eq. (2). |
Tables | |
![]() png pdf |
Table 1:
Signal efficiencies per year and per channel. |
Summary |
In summary, the first search of the rare exclusive hadronic decay W→πγ at the LHC has been presented. The search is based on the proton-proton data collected at a center-of-mass energy of 13TeV by the CMS experiment in 2016, 2017 and 2018, corresponding to an integrated luminosity of 137 fb−1. The measurement is performed on tˉt events, where one of the produced W bosons decays into leptons. The rare decay is characterized by an isolated photon and an isolated track compatible with that of a pion, for which a specific pion isolation variable is defined. The data are compatible with the background only hypothesis. The upper limit on the branching fraction of the W boson to a pion and a photon is 1.51 × 10−5 at 95% CL. This result demonstrates the possibility of performing a search for rare hadronic decays of the W bosons at the LHC, and defines a suitable search strategy. |
References | ||||
1 | Y. Grossman, M. Koenig, and M. Neubert | Exclusive radiative decays of W and Z bosons in QCD factorization | JHEP 04 (2015) 101 | 1501.06569 |
2 | T. Melia | Exclusive hadronic W decay: W→πγ and W→πππ | Nucl. Part. Phys. Proc. 273 (2016) 2012 | |
3 | G. Perez, Y. Soreq, E. Stamou, and K. Tobioka | Prospects for measuring the Higgs boson coupling to light quarks | PRD 93 (2016) 013001 | 1505.06689 |
4 | M. Mangano and T. Melia | Rare exclusive hadronic W decays in a tˉt environment | EPJC 75 (2015) 258 | 1410.7475 |
5 | CDF Collaboration | Search for the rare radiative decay: W→πγ in pˉp collisions at √s= 1.96 TeV | PRD 85 (2012) 032001 | 1104.1585 |
6 | CDF Collaboration | Search for the rare decay W±→D±sγ in pˉp collisions at √s= 1.8 TeV | PRD 122 (1998) 091101 | |
7 | CMS Collaboration | Search for W boson decays to three charged pions | PRL 122 (2019) 151802 | CMS-SMP-18-009 1901.11201 |
8 | Particle Data Group, M. Tanabashi et al. | Review of particle physics | PRD 98 (2018) 030001 | |
9 | CMS Collaboration | The CMS trigger system | JINST 12 (2017) P01020 | CMS-TRG-12-001 1609.02366 |
10 | CMS Collaboration | The CMS Experiment at the CERN LHC | JINST 3 (2008) S08004 | CMS-00-001 |
11 | T. Sjostrand et al. | An Introduction to PYTHIA 8.2 | CPC 191 (2015) 159 | 1410.3012 |
12 | P. Nason | A new method for combining NLO QCD with shower Monte Carlo algorithms | JHEP 11 (2014) 040 | hep-ph/0409146 |
13 | S. Frixione, P. Nason, and C. Oleari | Matching NLO QCD computations with parton shower simulations: the POWHEG method | JHEP 11 (2017) 070 | 0709.2092 |
14 | A. Simone, P. Nason, C. Oleari, and E. Re | A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX | JHEP 06 (2010) 043 | 1002.2581 |
15 | J. M. Campbell, R. K. Ellis, P. Nason, and E. Re | Top-pair production and decay at NLO matched with parton showers | JHEP 04 (2015) 114 | 1412.1828 |
16 | J. Alwall et al. | The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations | JHEP 07 (2014) 079 | 1405.0301 |
17 | CMS Collaboration | Event generator tunes obtained from underlying event and multiparton scattering measurements | EPJC 76 (2016) 155 | CMS-GEN-14-001 1512.00815 |
18 | CMS Collaboration | Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements | EPJC 80 (2020) 4 | CMS-GEN-17-001 1903.12179 |
19 | S. Agostinelli et al. | GEANT4 − a simulation toolkit | NIMA 506 (2003) 250 | |
20 | CMS Collaboration | Particle-flow reconstruction and global event description with the CMS detector | JINST 12 (2017) P10003 | CMS-PRF-14-001 1706.04965 |
21 | CMS Collaboration | Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at √s= 8 TeV | JINST 10 (2015) P06005 | CMS-EGM-13-001 1502.02701 |
22 | CMS Collaboration | Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s= 13 TeV | JINST 13 (2018) P06015 | CMS-MUO-16-001 1804.04528 |
23 | M. Cacciari, G. P. Salam, and G. Soyez | The anti-kT jet clustering algorithm | Journal of High Energy Physics 2008 (2008) 063 | 0802.1189 |
24 | M. Cacciari, G. P. Salam, and G. Soyez | FastJet user manual | EPJC 72 (2012) 1896 | 1111.6097 |
25 | CMS Collaboration | Heavy flavor identification at CMS with deep neural networks | CDS | |
26 | CMS Collaboration | CMS luminosity measurement for the 2016 data-taking period | CMS-PAS-LUM-15-001 | CMS-PAS-LUM-15-001 |
27 | CMS Collaboration | CMS luminosity measurement for the 2018 data-taking period at √s= 13 TeV | CMS-PAS-LUM-18-002 | CMS-PAS-LUM-18-002 |
28 | CMS Collaboration | CMS luminosity measurement for the 2017 data-taking period at √s= 13 TeV | CMS-PAS-LUM-17-004 | CMS-PAS-LUM-17-004 |
29 | CMS Collaboration | Measurement of the tˉt production cross section using events in the eμ final state in pp collisions at √s= 13 TeV | EPJC 77 (2017) 172 | CMS-TOP-16-005 1611.04040 |
30 | A. L. Read | Presentation of search results: The CL(s) technique | JPG 28 (2002) 2693 |
![]() |
Compact Muon Solenoid LHC, CERN |
![]() |
![]() |
![]() |
![]() |
![]() |
![]() |