CMS-PAS-EXO-23-015 | ||
Search for vector-like leptons with long-lived particle decays in the CMS muon system | ||
CMS Collaboration | ||
20 July 2024 | ||
Abstract: This note presents a search for vector-like leptons (VLLs), which in turn decay into a long-lived pseudoscalar and a standard model tau lepton. The pseudoscalar with a mass of 2 GeV exclusively decays into a pair of photons, and is identified using the muon detector shower signature. The data analysis is carried out using a dataset of proton-proton collisions at 13 TeV collected by the CMS experiment in 2016-2018, corresponding to an integrated luminosity of 138 fb$ ^{-1} $. Selected events contain at least one reconstructed muon detector hit cluster and at least one reconstructed hadronic tau lepton. No significant excess of data events are observed with respect to the background expectation, and 95% CL limits on the vector-like lepton production cross section are derived as a function of the VLL mass and pseudoscalar lifetime. Observed (expected) exclusion of the VLL mass is up to around 690 (640) GeV, depending on the pseudoscalar lifetime. | ||
Links: CDS record (PDF) ; CADI line (restricted) ; |
Figures | |
png pdf |
Figure 1:
Feynman diagram of pair production singlet vector-like leptons ($ \tau^{\prime} $), which in turn both decay into a SM $ \tau $ lepton and a new long-lived pseudoscalar ($ a_{\tau} $). |
png pdf |
Figure 2:
Distributions of the number of hits in the cluster ($ \mathrm{N_{hits}} $) for the CSC- (left) and DT-cluster (right) categories in the in-time (IT) signal region. The black markers represent the data. The blue, green and red lines denote different signal hypotheses. The background prediction is shown in the orange histogram. The last histogram bin contains all overflow events. |
png pdf |
Figure 2-a:
Distributions of the number of hits in the cluster ($ \mathrm{N_{hits}} $) for the CSC- (left) and DT-cluster (right) categories in the in-time (IT) signal region. The black markers represent the data. The blue, green and red lines denote different signal hypotheses. The background prediction is shown in the orange histogram. The last histogram bin contains all overflow events. |
png pdf |
Figure 2-b:
Distributions of the number of hits in the cluster ($ \mathrm{N_{hits}} $) for the CSC- (left) and DT-cluster (right) categories in the in-time (IT) signal region. The black markers represent the data. The blue, green and red lines denote different signal hypotheses. The background prediction is shown in the orange histogram. The last histogram bin contains all overflow events. |
png pdf |
Figure 3:
Distributions of the number of hits in the cluster ($ \mathrm{N_{hits}} $) for the CSC- (left) and DT-cluster (right) categories in the out-of-time (OOT) control region. The black markers represent the data. The blue, green and red lines denote different signal hypotheses. The background prediction is shown in the orange histogram. The last histogram bin contains all overflow events. |
png pdf |
Figure 3-a:
Distributions of the number of hits in the cluster ($ \mathrm{N_{hits}} $) for the CSC- (left) and DT-cluster (right) categories in the out-of-time (OOT) control region. The black markers represent the data. The blue, green and red lines denote different signal hypotheses. The background prediction is shown in the orange histogram. The last histogram bin contains all overflow events. |
png pdf |
Figure 3-b:
Distributions of the number of hits in the cluster ($ \mathrm{N_{hits}} $) for the CSC- (left) and DT-cluster (right) categories in the out-of-time (OOT) control region. The black markers represent the data. The blue, green and red lines denote different signal hypotheses. The background prediction is shown in the orange histogram. The last histogram bin contains all overflow events. |
png pdf |
Figure 4:
95% CL observed and expected upper limits on the VLL production cross section as a function of the VLL mass for a pseudoscalar $ c\tau_{a}= $ 0.025 m (left), and as a function of the pseudoscalar lifetime ($ c\tau_{a} $) for VLL mass of 700 GeV (right). The pseudoscalar mass is 2 GeV. The generator LO theoretical prediction is shown (pink line). |
png pdf |
Figure 4-a:
95% CL observed and expected upper limits on the VLL production cross section as a function of the VLL mass for a pseudoscalar $ c\tau_{a}= $ 0.025 m (left), and as a function of the pseudoscalar lifetime ($ c\tau_{a} $) for VLL mass of 700 GeV (right). The pseudoscalar mass is 2 GeV. The generator LO theoretical prediction is shown (pink line). |
png pdf |
Figure 4-b:
95% CL observed and expected upper limits on the VLL production cross section as a function of the VLL mass for a pseudoscalar $ c\tau_{a}= $ 0.025 m (left), and as a function of the pseudoscalar lifetime ($ c\tau_{a} $) for VLL mass of 700 GeV (right). The pseudoscalar mass is 2 GeV. The generator LO theoretical prediction is shown (pink line). |
Summary |
A first search for singlet vector-like leptons (VLLs) that decay into a long-lived pseudoscalar and a tau lepton has been performed using the dataset of pp collisions at 13 TeV collected in 2016-2018, corresponding to an integrated luminosity of 138 fb$ ^{-1} $. This analysis targets a reconstructed signature with at least one hadronically decaying tau lepton and at least one muon detector shower resulting from the pseudoscalar decay in the CMS muon system. Selected events are categorized based on the presence of a cluster of muon detector hits in the barrel or the endcap region. No significant deviation from the background-only hypothesis is observed. The results of each category are combined to derive upper limits on the VLL production cross section as a function of the VLL mass and the proper decay length of the pseudoscalar. VLL masses are excluded up to around 690 GeV, depending on the pseudoscalar lifetime. |
References | ||||
1 | N. Kumar and S. P. Martin | Vectorlike Leptons at the Large Hadron Collider | PRD 92 (2015) 115018 | 1510.03456 |
2 | P. N. Bhattiprolu and S. P. Martin | Prospects for vectorlike leptons at future proton-proton colliders | PRD 100 (2019) 015033 | 1905.00498 |
3 | K. Kong, S. C. Park, and T. G. Rizzo | A vector-like fourth generation with a discrete symmetry from Split-UED | JHEP 07 (2010) 059 | 1004.4635 |
4 | G.-Y. Huang, K. Kong, and S. C. Park | Bounds on the Fermion-Bulk Masses in Models with Universal Extra Dimensions | JHEP 06 (2012) 099 | 1204.0522 |
5 | S. P. Martin | Extra vector-like matter and the lightest Higgs scalar boson mass in low-energy supersymmetry | PRD 81 (2010) 035004 | 0910.2732 |
6 | P. W. Graham, A. Ismail, S. Rajendran, and P. Saraswat | A Little Solution to the Little Hierarchy Problem: A Vector-like Generation | PRD 81 (2010) 055016 | 0910.3020 |
7 | M. Endo, K. Hamaguchi, S. Iwamoto, and N. Yokozaki | Higgs Mass and Muon Anomalous Magnetic Moment in Supersymmetric Models with Vector-Like Matters | PRD 84 (2011) 075017 | 1108.3071 |
8 | S. Zheng | Minimal Vectorlike Model in Supersymmetric Unification | EPJC 80 (2020) 273 | 1904.10145 |
9 | R. Nevzorov | $ E_6 $ inspired supersymmetric models with exact custodial symmetry | PRD 87 (2013) 015029 | 1205.5967 |
10 | I. Doršner, S. Fajfer, and I. Mustać | Light vector-like fermions in a minimal SU(5) setup | PRD 89 (2014) 115004 | 1401.6870 |
11 | A. Joglekar and J. L. Rosner | Searching for signatures of $ E_{\rm 6} $ | PRD 96 (2017) 015026 | 1607.06900 |
12 | ATLAS Collaboration | Combination of the searches for pair-produced vector-like partners of the third-generation quarks at $ \sqrt{s} = $ 13 TeV with the ATLAS detector | PRL 121 (2018) 211801 | 1808.02343 |
13 | CMS Collaboration | Search for pair production of vector-like quarks in leptonic final states in proton-proton collisions at $ \sqrt{s} = $ 13 TeV | JHEP 07 (2023) 020 | 2209.07327 |
14 | CMS Collaboration | Review of searches for vector-like quarks, vector-like leptons, and heavy neutral leptons in proton-proton collisions at $ \sqrt{s} = $ 13 TeV at the CMS experiment | Submitted to Phys. Rep., 2024 | CMS-EXO-23-006 2405.17605 |
15 | A. Greljo and B. A. Stefanek | Third family quark-lepton unification at the TeV scale | PLB 782 (2018) 131 | 1802.04274 |
16 | ATLAS Collaboration | Search for third-generation vector-like leptons in pp collisions at $ \sqrt{s} = $ 13 TeV with the ATLAS detector | JHEP 07 (2023) 118 | 2303.05441 |
17 | CMS Collaboration | Inclusive nonresonant multilepton probes of new phenomena at $ \sqrt s = $ 13 TeV | PRD 105 (2022) 112007 | CMS-EXO-21-002 2202.08676 |
18 | CMS Collaboration | Search for pair-produced vector-like leptons in final states with third-generation leptons and at least three b quark jets in proton-proton collisions at $ \sqrt{s} = $ 13 TeV | PLB 846 (2023) 137713 | 2208.09700 |
19 | E. Bernreuther and B. A. Dobrescu | Vectorlike leptons and long-lived bosons at the LHC | JHEP 07 (2023) 079 | 2304.08509 |
20 | CMS Collaboration | Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $ \sqrt s $ =13 TeV | PRL 127 (2021) 261804 | CMS-EXO-20-015 2107.04838 |
21 | CMS Collaboration | Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $ \sqrt{s} = $ 13 TeV | Accepted by Phys. Rev. D, 2024 | CMS-EXO-21-008 2402.01898 |
22 | CMS Collaboration | Search for long-lived heavy neutral leptons decaying in the CMS muon detectors in proton-proton collisions at $ \sqrt{s} = $ 13 TeV | PRD 110 (2024) 012004 | CMS-EXO-22-017 2402.18658 |
23 | CMS Collaboration | Performance of the CMS Level-1 trigger in proton-proton collisions at $ \sqrt{s} = $ 13 TeV | JINST 15 (2020) P10017 | CMS-TRG-17-001 2006.10165 |
24 | CMS Collaboration | The CMS trigger system | JINST 12 (2017) P01020 | CMS-TRG-12-001 1609.02366 |
25 | CMS Collaboration | The CMS experiment at the CERN LHC | JINST 3 (2008) S08004 | |
26 | CMS Collaboration | Development of the CMS detector for the CERN LHC Run 3 | JINST 19 (2024) P05064 | CMS-PRF-21-001 2309.05466 |
27 | T. Sjöstrand et al. | An introduction to PYTHIA8.2 | Comp. Phys. Comm. 191 (2015) 159 | 1410.3012 |
28 | 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 |
29 | NNPDF Collaboration | Parton distributions from high-precision collider data | EPJC 77 (2017) 663 | 1706.00428 |
30 | GEANT4 Collaboration | GEANT 4---a simulation toolkit | NIM A 506 (2003) 250 | |
31 | CMS Collaboration | Particle-flow reconstruction and global event description with the CMS detector | JINST 12 (2017) P10003 | CMS-PRF-14-001 1706.04965 |
32 | CMS Collaboration | Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid | CMS Technical Proposal CERN-LHCC-2015-010, CMS-TDR-15-02, 2015 CDS |
|
33 | CMS Collaboration | Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JINST 13 (2018) P06015 | CMS-MUO-16-001 1804.04528 |
34 | M. Cacciari, G. P. Salam, and G. Soyez | The anti-$ k_t $ jet clustering algorithm | JHEP 04 (2008) 063 | 0802.1189 |
35 | M. Cacciari, G. P. Salam, and G. Soyez | FastJet User Manual | EPJC 72 (2012) 1896 | 1111.6097 |
36 | CMS Collaboration | Pileup mitigation at CMS in 13 TeV data | JINST 15 (2020) P09018 | CMS-JME-18-001 2003.00503 |
37 | CMS Collaboration | Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV | JINST 12 (2017) P02014 | CMS-JME-13-004 1607.03663 |
38 | CMS Collaboration | Performance of missing transverse momentum reconstruction in proton-proton collisions at $ \sqrt{s} = $ 13 TeV using the CMS detector | JINST 14 (2019) P07004 | CMS-JME-17-001 1903.06078 |
39 | 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 |
40 | CMS Collaboration | Identification of hadronic tau lepton decays using a deep neural network | JINST 17 (2022) P07023 | CMS-TAU-20-001 2201.08458 |
41 | M. Ester, H.-P. Kriegel, J. Sander, and X. Xu | A density-based algorithm for discovering clusters in large spatial databases with noise | in Proceedings of the Second International Conference on Knowledge Discovery and Data Mining, 1996 | |
42 | R. A. Fisher | On the interpretation of $ \chi^{2} $ from contingency tables, and the calculation of P | J. R. Stat. Soc. 85 (1922) 87 | |
43 | S. Baker and R. D. Cousins | Clarification of the use of chi square and likelihood functions in fits to histograms | NIM 221 (1984) 437 | |
44 | J. K. Lindsey | Parametric Statistical Inference | Oxford Science Publications. Clarendon Press, ISBN 978023598, 1996 | |
45 | CMS Collaboration | Precision luminosity measurement in proton-proton collisions at $ \sqrt{s} = $ 13 TeV in 2015 and 2016 at CMS | EPJC 81 (2021) 800 | CMS-LUM-17-003 2104.01927 |
46 | CMS Collaboration | CMS luminosity measurement for the 2017 data-taking period at $ \sqrt{s} = $ 13 TeV | CMS Physics Analysis Summary, 2018 link |
CMS-PAS-LUM-17-004 |
47 | CMS Collaboration | CMS luminosity measurement for the 2018 data-taking period at $ \sqrt{s} = $ 13 TeV | CMS Physics Analysis Summary, 2019 link |
CMS-PAS-LUM-18-002 |
48 | T. Junk | Confidence level computation for combining searches with small statistics | NIM A 434 (1999) 435 | hep-ex/9902006 |
49 | A. L. Read | Presentation of search results: the CL$ _\mathrm{s} $ technique | JPG 28 (2002) 2693 | |
50 | The ATLAS Collaboration, The CMS Collaboration, The LHC Higgs Combination Group | Procedure for the LHC Higgs boson search combination in Summer 2011 | Technical Report CMS-NOTE-2011-005, ATL-PHYS-PUB-2011-11, 2011 | |
51 | G. Cowan, K. Cranmer, E. Gross, and O. Vitells | Asymptotic formulae for likelihood-based tests of new physics | EPJC 71 (2011) 1554 | 1007.1727 |
Compact Muon Solenoid LHC, CERN |