| 1 | |
| 2 | |
| 3 | == Higgs phenomenology at hadron colliders == |
| 4 | |
| 5 | |
| 6 | ==== 1. Decays of the Higgs boson ==== |
| 7 | * A light SM Higgs boson mostly decays into %$b\bar b$%. Compute the decay rate for %$H\rightarrow b\bar b$%. |
| 8 | * For a Higgs mass of around 160 !GeV, the main decay mode is %$H\rightarrow WW$%. Compute the decay rate. |
| 9 | The Higgs branching ratios can be found [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h-br.pdf here]. |
| 10 | |
| 11 | You may also have a look at the following Mathematica [http://cp3wks05.fynu.ucl.ac.be/twiki/bin/viewfile/Physics/HiggsPheno?rev=1;filename=HDecay.nb notebook]. |
| 12 | |
| 13 | ==== 2. Gluon fusion and Higgs effective field theory ==== |
| 14 | The computation of the leading order cross-section of a Higgs boson via gluon fusion involves the computation of a top quark loop. |
| 15 | In the large top mass limit, the gluon fusion production of a Higgs boson can be described by an effective field theory where the Higgs couples directly to the gluons, |
| 16 | |
| 17 | %$\begin{cal}L\end{cal}=C_H\, H\, G_{\mu\nu}^a\, G_a^{\mu\nu}$%, |
| 18 | |
| 19 | where %$C_H$% is an effective (dimensionful) coupling constant and %$G_{\mu\nu}^a$% denotes the gluon field strength tensor. |
| 20 | |
| 21 | For details on the calculation of the top loop and the effective theory, see the notes and/or check the following Mathematica notebooks (which actually contain much more information): |
| 22 | |
| 23 | 1. pp>H at LO (1-loop): details of the calculation (Mathematica Notebook) [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/GIFSchool/HiggsGG-LO-mtfinite.nb HiggsGG-LO-mtfinite.nb] |
| 24 | 1. pp>H at NLO: details of the calculation (Mathematica Notebook) [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/GIFSchool/HiggsGG-NLO.nb higgsGG-NLO.nb] |
| 25 | 1. pp>H at NLO: cross section evaluation for the LHC (Mathematica Notebook+PDF libraries to be compiled) [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/GIFSchool/phenHiggs.tar.gz phenHiggs.tar.gz]. |
| 26 | |
| 27 | Exercise (DIFFICULT but interesting!!): Use the all the material above to derive the EFT description of a pseudo-scalar Higgs, A, |
| 28 | |
| 29 | %$\begin{cal}L\end{cal}=C_A\, A\, G_{\mu\nu}^a\, {\tilde G}_a^{\mu\nu}$%, |
| 30 | |
| 31 | where %$C_A$% is an effective (dimensionful) coupling constant and %$G_{\mu\nu}^a$% denotes the gluon field strength tensor and |
| 32 | %${\tilde G}''a^{\mu\nu}=\frac12 \epsilon^{\mu\nu\rho\sigma} G''a^{\rho\sigma}$% is its dual. Compute the loop amplitude, derive the Feynman rules |
| 33 | in the large top mass limit and calculate the LO and NLO cross sections at the LHC. |
| 34 | |
| 35 | |
| 36 | |
| 37 | ==== 3. Discover the SM Higgs at the LHC ==== |
| 38 | |
| 39 | * Find the best prediction for Higgs production at the LHC [http://maltoni.web.cern.ch/maltoni/TeV4LHC/index.html here]. |
| 40 | |
| 41 | Choose a channel and investigate signal and background: |
| 42 | |
| 43 | 1. The 4 lepton final state: %$pp \to H\to Z Z \to e^+e^- \mu^+ \mu^-$% |
| 44 | * Signal |
| 45 | * Events: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l-signal.lhe.gz Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l-signal.lhco.gz Detector Level] |
| 46 | * Plots: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l-signal-lhe.pdf Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l-signal-lhco.pdf Detector Level] |
| 47 | * Background |
| 48 | * Events: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l.lhe.gz Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l.lhco.gz Detector Level] |
| 49 | * Plots: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l-lhe.pdf Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/h4l-lhco.pdf Detector Level] |
| 50 | |
| 51 | 1. The 2 lepton + missing Et final state: %$pp \to H\to W^+ W^- \to e^- \bar \nu_e \mu^+ \nu_\mu $% |
| 52 | * Signal |
| 53 | * Events: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-signal.lhe.gz Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-signal.lhco.gz Detector Level] |
| 54 | * Plots: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-signal-lhe.pdf Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-signal-lhco.pdf Detector Level] |
| 55 | * Background |
| 56 | * Events: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-background.lhe.gz Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-background.lhco.gz Detector Level] |
| 57 | * Plots: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-background-lhe.pdf Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/hww-background-lhco.pdf Detector Level] |
| 58 | 1. Top associated production %$pp \to t\bar tH$% with %$H \to b \bar b$% |
| 59 | * Signal + Background samples: |
| 60 | * Events: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/ttbb.lhe.gz Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/ttbb.lhco.gz Detector Level] |
| 61 | * Plots: [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/ttbb-lhe.pdf Parton Level] [http://cp3wks05.fynu.ucl.ac.be/twiki/pub/Physics/DiscoverTheHiggs/ttbb-lhco.pdf Detector Level] |
| 62 | |
| 63 | |
| 64 | ==== 4. Gluon fusion vs. weak boson fusion ==== |
| 65 | * Use the web interface of !MadGraph/!MadEvent to generate the cross-sections for H+2jets at the LHC via gluon fusion and weak boson fusion. Hint: For the gluon fusion, you need to use the Higgs efective field theory (heft) in !MadGraph/!MadEvent. |
| 66 | * Plot the rapidities of the two jets for boson production channels. |
| 67 | * What do you observe? What do you conclude? |
| 68 | * What happens to this picture when a third jet is added? |
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| 70 | |
| 71 | -- Main.FabioMaltoni - 28 Aug 2008 |
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