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2017:groups:higgs:lsp [2017/06/20 15:43]
haiying.cai
2017:groups:higgs:lsp [2017/10/01 11:20] (current)
jonathan.butterworth
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-__Interested people:__ //Jose Miguel No, Jose Zurita, Stefania Gori, Ken Mimasu, Linda Finco, Sijing Zhang, Susan Gascon-Shotkin,​ Grégory Moreau, Haiying Cai, Sylvain Fichet, Thomas Flacke, Stefan Liebler, //+__Interested people:__ //Jose Miguel No, Jose Zurita, Stefania Gori, Ken Mimasu, Linda Finco, Sijing Zhang, Susan Gascon-Shotkin,​ Grégory Moreau, Haiying Cai, Sylvain Fichet, Thomas Flacke, Stefan Liebler, ​Daniele Barducci, Andrei Angelescu, Jon Butterworth//
  
  
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 Looking at scalar couplings to fermions, other production and decay modes ($\phi \to \tau \tau$ or $\phi \to b \bar b$ [reconstructing the invariant scalar mass]) could be studied as well. Looking at scalar couplings to fermions, other production and decay modes ($\phi \to \tau \tau$ or $\phi \to b \bar b$ [reconstructing the invariant scalar mass]) could be studied as well.
  
-Gauge invariant (pseudo-)scalar couplings to ZZ, WW, $\gamma\gamma$,​ $\gamma$Z, gluon-gluon:​ $$\frac{\phi}{\Lambda_1}\vert D_\mu H\vert^2 \ \ (for scalars ​only) \ \ and \ \ \frac{\phi}{\Lambda_2} Tr[V_{\mu\nu} \tilde V^{\mu\nu}] \ .$$ +Gauge invariant (pseudo-)scalar couplings to ZZ, WW, $\gamma\gamma$,​ $\gamma$Z, gluon-gluon:​ $$\frac{\phi}{f_H}\vert D_\mu H\vert^2 ​   
 +\ \ \frac{\phi}{f_Z} Tr[V_{\mu\nu} V^{\mu\nu}]  
 +\ \ and \ \ \frac{\phi}{\tilde f_Z} Tr[V_{\mu\nu} \tilde V^{\mu\nu}] \ .$$ 
  
 Two other effective parameters: $\phi$ mass ($m_\phi$) and Branching for $\phi \to \gamma \gamma$ ($B_\gamma$). Two other effective parameters: $\phi$ mass ($m_\phi$) and Branching for $\phi \to \gamma \gamma$ ($B_\gamma$).
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 (2) produce kinematical distributions for the signal with MadGRAPH (directly from the LHE files with madAnalysis for example) (2) produce kinematical distributions for the signal with MadGRAPH (directly from the LHE files with madAnalysis for example)
 (3) interface the DELPHES detector response simulator (at the MadGRAPH level) (3) interface the DELPHES detector response simulator (at the MadGRAPH level)
-(4) compare distributions for SM-like couplings ($1/\Lambda_1$) and kinetic-like couplings ($1/\Lambda_2$) [also to develop a discrimination test between e.g. a light Higgs and a radion] ​+(4) compare distributions for SM-like couplings ($1/f_H$) and kinetic-like couplings ($1/​f_Z$, ​$1/\tilde f_Z$) [also to develop a discrimination test between e.g. a light Higgs and a radion] ​
 (5) simulate SM background events as well (main physical one: Drell-Yan + double ISR/FSR ?)  (5) simulate SM background events as well (main physical one: Drell-Yan + double ISR/FSR ?) 
 (6) optimise a set of selection cuts (6) optimise a set of selection cuts
-(7) obtain a sensitivity plot (prospective for Run 2) in the 3-dimension ​parameter space: $m_\phi$, $1/\Lambda_1$, $1/\Lambda_2$ [=couplings for the considered gauge bosons] for $B_\gamma$=100% (plot to be simply rescaled accordingly to the wanted $B_\gamma$ value then). (+motivate EXP analysis of exclusion limits from Run 1 data?).+(7) obtain a sensitivity plot (prospective for Run 2) in the parameter space: $m_\phi$, $1/f_H$, $1/f_Z$, $1/\tilde f_Z$ [=couplings for the considered gauge bosons] for $B_\gamma$=100% (plot to be simply rescaled accordingly to the wanted $B_\gamma$ value then). (+motivate EXP analysis of exclusion limits from Run 1 data?).
  
 Goal: derive a generic plot that can be recast to any specific theoretical scenario with a light (pseudo-)scalar,​ and, determine its complementarity with LEP(,EWPT) bounds. Goal: derive a generic plot that can be recast to any specific theoretical scenario with a light (pseudo-)scalar,​ and, determine its complementarity with LEP(,EWPT) bounds.
  
 +Tools: Some of us are looking at this using [[2017:​groups:​tools:​contur_for_light_scalar_particles|Contur]].
  
    
2017/groups/higgs/lsp.1497966217.txt.gz · Last modified: 2017/06/20 15:43 by haiying.cai