CMS-SMP-18-009 ; CERN-EP-2019-001 | ||
Search for W boson decays to three charged pions | ||
CMS Collaboration | ||
30 January 2019 | ||
Phys. Rev. Lett. 122 (2019) 151802 | ||
Abstract: For the first time, a search for the rare decay of the W boson to three charged pions has been performed. Proton-proton collision data recorded by the CMS experiment at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 77.3 fb$^{-1}$, have been analyzed. No significant excess is observed above the background expectation. An upper limit of 1.01$\times10^{-6}$ is set at 95% confidence level on the branching fraction of the W boson to three charged pions. This provides a strong motivation for theoretical calculations of this branching fraction. | ||
Links: e-print arXiv:1901.11201 [hep-ex] (PDF) ; CDS record ; inSPIRE record ; HepData record ; CADI line (restricted) ; |
Figures | |
png pdf |
Figure 1:
Observed and expected distributions of $ {m_{3 {\pi}}} $, using 77.3 fb$^{-1}$ of data collected in 2016 and 2017. The normalization of the expected backgrounds results from the maximum likelihood fit to the data, which includes all systematic uncertainties. The background contributions are stacked upon each other, and the "Others" background contribution includes events from diboson, triboson, $ {{\mathrm {t}\overline {\mathrm {t}}}} $, single top quark, $ {{\mathrm {t}\overline {\mathrm {t}}}} {\mathrm {Z}} $, and $ {{\mathrm {t}\overline {\mathrm {t}}}} {\mathrm {W}}$ production. The uncertainty band includes both statistical and systematic sources of uncertainty. The signal is normalized to $\mathcal {B}({\mathrm {W}}\to 3 {\pi})=10^{-6}$, and is shown as an open stacked histogram. |
png pdf |
Figure 2:
Observed and expected upper limits on $\mathcal {B}({\mathrm {W}}\to 3 {\pi})$ at 95%CL. The expected limit corresponds to the assumption $\mathcal {B}({\mathrm {W}}\to 3 {\pi})=$ 0. |
Summary |
In summary, the first search for the rare decay of the W boson to three charged pions has been performed. The data correspond to an integrated luminosity of 77.3 fb$^{-1}$ of proton-proton collisions collected in the CMS detector at a center-of-mass energy of 13 TeV. Events with W bosons are selected with a trigger that requires two $\tau$ leptons decaying to hadrons and a neutrino. The data are compatible with the background hypothesis. The upper limit on the branching fraction of the W boson to three charged pions is 1.01$\times10^{-6}$ at 95%CL, which reduces the previous range of values and motivates theoretical calculations of this branching fraction. |
References | ||||
1 | Y. Grossman, K. Matthias, 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 $ \to \pi \gamma $ and W $ \to \pi^+ \pi^+ \pi^- $ | in 37th International Conference on High Energy Physics, p. 2102 Valencia, Spain, 2014 [Nucl. Part. Phys. Proc. 273 (2016) 2102] | |
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 | CDF Collaboration | Search for the rare decay $ W^\pm \to D_s^{+-} \gamma $ in $ \textrm{p}\bar{\textrm{p}} $ collisions at $ \sqrt{s} = $ 1.8 TeV | PRD 58 (1998) 091101 | |
5 | CDF Collaboration | Search for the rare radiative decay: $ W\rightarrow\pi\gamma $ in $ \textrm{p}\bar{\textrm{p}} $ collisions at $ \sqrt{s} = $ 1.96 TeV | PRD 85 (2012) 032001 | 1104.1585 |
6 | Particle Data Group, M. Tanabashi et al. | Review of particle physics | PRD 98 (2018) 030001 | |
7 | M. Mangano and T. Melia | Rare exclusive hadronic W decays in a $ \mathrm{t\bar{t}} $ environment | EPJC 75 (2015) 258 | 1410.7475 |
8 | CMS Collaboration | Reconstruction and identification of $ \tau $ lepton decays to hadrons and $ \nu_\tau $ at CMS | JINST 11 (2016) P01019 | CMS-TAU-14-001 1510.07488 |
9 | CMS Collaboration | Performance of reconstruction and identification of $ \tau $ leptons decaying to hadrons and $ \nu_\tau $ in pp collisions at $ \sqrt{s}= $ 13 TeV | JINST 13 (2018) P10005 | CMS-TAU-16-003 1809.02816 |
10 | CMS Collaboration | The CMS trigger system | JINST 12 (2017) P01020 | CMS-TRG-12-001 1609.02366 |
11 | CMS Collaboration | The CMS experiment at the CERN LHC | JINST 3 (2008) S08004 | CMS-00-001 |
12 | T. Sjostrand et al. | An introduction to PYTHIA 8.2 | CPC 191 (2015) 159 | 1410.3012 |
13 | 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 |
14 | R. Frederix and S. Frixione | Merging meets matching in MC@NLO | JHEP 12 (2012) 061 | 1209.6215 |
15 | J. Alwall et al. | Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions | EPJC 53 (2008) 473 | 0706.2569 |
16 | P. Nason | A new method for combining NLO QCD with shower Monte Carlo algorithms | JHEP 11 (2004) 040 | hep-ph/0409146 |
17 | S. Frixione, P. Nason, and C. Oleari | Matching NLO QCD computations with parton shower simulations: the POWHEG method | JHEP 11 (2007) 070 | 0709.2092 |
18 | S. Alioli, P. Nason, C. Oleari, and E. Re | NLO Higgs boson production via gluon fusion matched with shower in POWHEG | JHEP 04 (2009) 002 | 0812.0578 |
19 | S. Alioli, 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 |
20 | S. Alioli et al. | Jet pair production in POWHEG | JHEP 04 (2011) 081 | 1012.3380 |
21 | CMS Collaboration | Event generator tunes obtained from underlying event and multiparton scattering measurements | EPJC 76 (2016) 155 | CMS-GEN-14-001 1512.00815 |
22 | NNPDF Collaboration | Parton distributions for the LHC Run II | JHEP 04 (2015) 040 | 1410.8849 |
23 | GEANT4 Collaboration | GEANT4--a simulation toolkit | NIMA 506 (2003) 250 | |
24 | CMS Collaboration | Particle-flow reconstruction and global event description with the CMS detector | JINST 12 (2017) P10003 | CMS-PRF-14-001 1706.04965 |
25 | M. Cacciari, G. P. Salam, and G. Soyez | The anti-$ {k_{\mathrm{T}}} $ jet clustering algorithm | JHEP 04 (2008) 063 | 0802.1189 |
26 | M. Cacciari, G. P. Salam, and G. Soyez | FastJet user manual | EPJC 72 (2012) 1896 | 1111.6097 |
27 | M. Cacciari and G. P. Salam | Dispelling the $ N^{3} $ myth for the $ {k_{\mathrm{T}}} $ jet-finder | PLB 641 (2006) 57 | hep-ph/0512210 |
28 | Y. Li and F. Petriello | Combining QCD and electroweak corrections to dilepton production in FEWZ | PRD 86 (2012) 094034 | 1208.5967 |
29 | CMS Collaboration | Observation of the Higgs boson decay to a pair of $ \tau $ leptons with the CMS detector | PLB 779 (2018) 283 | CMS-HIG-16-043 1708.00373 |
30 | CMS Collaboration | Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV | JINST 13 (2018) P05011 | CMS-BTV-16-002 1712.07158 |
31 | CMS Collaboration | CMS luminosity measurements for the 2016 data taking period | CMS-PAS-LUM-17-001 | CMS-PAS-LUM-17-001 |
32 | CMS Collaboration | CMS luminosity measurement for the 2017 data-taking period at $ \sqrt{s} = $ 13 TeV | CMS-PAS-LUM-17-004 | CMS-PAS-LUM-17-004 |
33 | J. M. Campbell and R. K. Ellis | MCFM for the Tevatron and the LHC | NPPS 205-206 (2010) 10 | 1007.3492 |
34 | M. Beneke, P. Falgari, S. Klein, and C. Schwinn | Hadronic top quark pair production with NNLL threshold resummation | NPB 855 (2012) 695 | 1109.1536 |
35 | M. Cacciari et al. | Top pair production at hadron colliders with next-to-next-to-leading logarithmic soft-gluon resummation | PLB 710 (2012) 612 | 1111.5869 |
36 | P. Barnreuther, M. Czakon, and A. Mitov | Percent level precision physics at the Tevatron: First genuine NNLO QCD corrections to $ \mathrm{q\bar{q}}\to \mathrm{t\bar{t}} + X $ | PRL 109 (2012) 132001 | 1204.5201 |
37 | M. Czakon and A. Mitov | NNLO corrections to top pair production at hadron colliders: the quark-gluon reaction | JHEP 01 (2013) 080 | 1210.6832 |
38 | M. Czakon and A. Mitov | NNLO corrections to top pair production at hadron colliders: the all-fermionic scattering channels | JHEP 12 (2012) 054 | 1207.0236 |
39 | M. Czakon, P. Fiedler, and A. Mitov | Total top quark pair production cross section at hadron colliders through O($ \alpha_s^4 $) | PRL 110 (2013) 252004 | 1303.6254 |
40 | M. Czakon and A. Mitov | Top++: A program for the calculation of the top pair cross section at hadron colliders | CPC 185 (2014) 2930 | 1112.5675 |
41 | R. Gavin, Y. Li, F. Petriello, and S. Quackenbush | W physics at the LHC with FEWZ 2.1 | CPC 184 (2013) 208 | 1201.5896 |
42 | K. Melnikov and F. Petriello | Electroweak gauge boson production at hadron colliders through $ O(\alpha_S^2) $ | PRD 74 (2006) 114017 | hep-ph/0609070 |
43 | ATLAS and CMS Collaborations, LHC Higgs Combination Group | Procedure for the LHC Higgs boson search combination in Summer 2011 | ATL-PHYS-PUB 2011-11, CMS NOTE 2011/005 | |
44 | T. Junk | Confidence level computation for combining searches with small statistics | NIMA 434 (1999) 435 | hep-ex/9902006 |
45 | A. L. Read | Presentation of search results: the CL$ _s $ technique | JPG 28 (2002) 2693 |
Compact Muon Solenoid LHC, CERN |