Abstract
The \(M_\mathrm {T2}\) variable, sometimes called stransverse mass, has been proven to be very sensitive to events emerging from SUSY production processes, while strongly suppressing the background due to SM processes.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
Notes
- 1.
As \(M_{\tilde{\chi }}\) is a parameter, the symbol \(M_{\tilde{\chi }}\) is chosen over \(M(\widetilde{\chi })\) in the equations of this section.
- 2.
This argument holds also for the asymmetric decay (one W boson decaying leptonically, the other one hadronically), as reasoned in [3].
- 3.
For the 7 TeV search, no CHS was applied.
- 4.
In the \(M_\mathrm {T2} b\) analysis, b jets were selected by a simple secondary vertex tagger with an efficiency of about \(40\,\%\) and a light-jet mistagging rate of \(\sim \) \(0.1\,\%\).
References
C. Lester, D. Summers, Measuring masses of semi-invisibly decaying particle pairs produced at hadron colliders. Phys. Lett. B 463, 99 (1999). doi:10.1016/S0370-2693(99)00945-4. arXiv:hep-ph/9906349
A. Barr, C. Lester, P. Stephens, A variable for measuring masses at hadron colliders when missing energy is expected; \(m_{T2}\): the truth behind the glamour. J. Phys. G 29, 2343 (2003). doi:10.1088/0954-3899/29/10/304. arXiv:hep-ph/0304226
P. Nef, Search for supersymmetry in hadronic final states using \(M_2\) in pp collisions at at \(\sqrt{s}=7\) TeV and discovery potential of top partners in composite Higgs models. Dissertation. ETH Zurich (2013). doi:10.3929/ethz-a-007635937
UA1 Collaboration, Experimental observation of isolated large transverse energy electrons with associated missing energy at \(\sqrt{s} = 540\) GeV. Phys. Lett. B 122, 103 (1983). doi:10.1016/0370-2693(83)91177-2
UA2 Collaboration, Observation of single isolated electrons of high transverse momentum in events with missing transverse energy at the CERN \(\bar{\rm p}{\rm p}\) collider. Phys. Lett. 122, 476 (1983). doi:10.1016/0370-2693(83)91605-2
W.S. Cho et al., Measuring superparticle masses at hadron collider using the transverse mass kink. JHEP 02, 035 (2008). doi:10.1088/1126-6708/2008/02/035. arXiv:0711.4526
H.-C. Cheng, Z. Han, Minimal kinematic constraints and \(m_{T2}\). JHEP 12, 063 (2008). doi:10.1088/1126-6708/2008/12/063. arXiv:0810.5178
A.J. Barr, C. Gwenlan, The race for supersymmetry: using \(m_{T2}\) for discovery. Phys. Rev. D 80, 074007 (2009). doi:10.1103/PhysRevD.80.074007. arXiv:0907.2713
CMS Collaboration, CMS physics technical design report, volume II: physics performance. J. Phys. G 34, 995 (2007). doi:10.1088/0954-3899/34/6/S01
T. Sjöstrand, S. Mrenna, P.Z. Skands, PYTHIA 6.4 physics and manual. JHEP 05, 026 (2006). doi:10.1088/1126-6708/2006/05/026. arXiv:hep-ph/0603175
M. Burns et al., Using subsystem \(M_{T2}\) for complete mass determinations in decay chains with missing energy at hadron colliders. JHEP 03, 143 (2009). doi:10.1088/1126-6708/2009/03/143. arXiv:0810.5576
M.M. Nojiri, K. Sakurai, Controlling initial state radiation in sparticle mass reconstruction. Phys. Rev. D 82, 115026 (2010). doi:10.1103/PhysRevD.82.115026. arXiv:1008.1813
CMS Collaboration, Search for supersymmetry in hadronic final states using \(M_{{\rm T}2}\) in pp collisions at \(\sqrt{s} = 7\) TeV. JHEP 10, 018 (2012). doi:10.1007/JHEP10(2012)018. arXiv:1207.1798
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
Copyright information
© 2015 Springer International Publishing Switzerland
About this chapter
Cite this chapter
Weber, H.A. (2015). Search for Supersymmetry: Using \(M_\mathrm {T2}\) as Discovery Variable. In: Search for Supersymmetry in Hadronic Final States. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-19956-6_6
Download citation
DOI: https://doi.org/10.1007/978-3-319-19956-6_6
Published:
Publisher Name: Springer, Cham
Print ISBN: 978-3-319-19955-9
Online ISBN: 978-3-319-19956-6
eBook Packages: Physics and AstronomyPhysics and Astronomy (R0)