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Heavy Search at LHC Yuhan Guo Vanderbilt University

Standard Model (mediators) Electromagnetic interaction Acts on Mediator Acts on Mediator Acts on Mediator Gravitation Acts on Mediator??? • Laser Interferometer Gravitational-Wave Observatory (LIGO) • September 14, 2015 – GW from Colliding Black Holes • August 8, 2017 – GW from Colliding Stars Large

The Large (LHC)

Model & Parameters

Can we produce enough graviton events at LHC? Production Mechanism & Decay Channel

Kinematics Phenomenology

Study Optimization Study

What’s our optimal strategy Selection Criteria of detecting graviton?

(maximize significance) Predictions page 1/5

3 2 2 4 a a g g 3 u u u u 5 a g g u u~ u~ 4 a g 6 5 g

u~

1 1 6 Production Mechanism & diagram 1 QCD=2, QED=2 diagram 2 QCD=2, QED=2 4 2 page 2/42 4 a Decay Channel a g g 3 u u~ u~ u 5 a 2 2 g g 6 6 d d u~ d u d u~ 3 page 5/8 a g 5 6 g 4 4 z a u~ a a 1 1 y2 y2 6 2 3 2 3 d a a d diagram 3 QCD=2, QED=2a a diagram 4 QCD=2, QED=2 d d a 3 z 3 d d

a 6 2 z 6 2 u u u u3 3 u 5 u a 5 a 1 g 1 g 5 5 u u 4 4 u u u~ u~ diagram 7 DMT=2, QCD=0, QED=2 diagram 8 a DMT=2, QCD=0, QED=2 a g g u a u a u~ u u u~ 4 4 1 Vector Fusion 1 5 6 2 g 2 6 4 g 5 diagramd 25 QCD=0, QED=4 6 diagram 26 QCD=0, QED=4 a Diphoton channel d d y2 1 Background d a 1 2 3 4 2 3 d z a diagramd 5 QCD=2,a QED=2 d 3 diagram 6 QCD=2, QED=2 a y2 a 6 d~ a d~ a 4 a Diagrams4 made by MadGraph5_aMC@NLO z 3 d~ d~ u d u d u u 6 5 6 5 1 a 1 z u u u u 1 diagram 9 DMT=2, QCD=0,5 QED=2 1 diagram 10 DMT=2,5 QCD=0, QED=2

diagram 27 QCD=0, QED=4 diagram 28 QCD=0, QED=4

2 4 2 4 a a 2 d 2 d 3 3 d a y2 d a y2 d a a

d 4 3 d 4 3 d~ d~ a a z d 6 d a 6 d d

a 6 z 6 u u u u u u 5 u u 5 5 5 1 1 1 1

diagram 29 QCD=0, QED=4 diagram 30 QCD=0, QED=4 diagram 11 DMT=2, QCD=0, QED=2 diagram 12 DMT=2, QCD=0, QED=2

Diagrams made by MadGraph5_aMC@NLO Diagrams made by MadGraph5_aMC@NLO Vector Boson Fusion

• Why VBF? • Significant reduction of the QCD background • Enhanced cross section at large scales

• Features • Large dijet mass, energetic jets

• Jets are forward & in opposite atmosphere (large ) | Δη jj |

à Use the unique features of VBF to design the searching strategy! Cross Section – Graviton Mass 106 pp → G + 0j, κ = 1 g,q [pb] 5 σ 10 0 pp → G + jj, α , κ = 1 QCD B,W,H 4 10 0 pp → G + jj, α , κ = 1, |Δη | > 4.0 QCD B,W,H jj 103

102

10

1

10−1

10−2

10−3

10−4 0 500 1000 1500 2000 2500 3000 MG [GeV] N = σ ⋅ L (Event rate = cross section * luminosity) −1 Assuming : Lint =1000 fb 5 If , we have events mG = 500GeV 10 3 If , we have events mG = 3000GeV 10 page 1/1

2

u~

y2 3

u Compare: DY with varying 1 strong coupling constants

diagram 1 DMT=1, QCD=0, QED=0

Diagrams made by MadGraph5_aMC@NLO Kinematics

• Decay channel à Key variable: diphoton mass

γ1 γ2 mγγ = 2 | pT || pT | cosh Δηγγ

• VBF features: • Large dijet mass • Energetic & forward jets 1 -1 LHC s=13TeV Lint=100.0 fb 1 pp → j j G (→ γ γ), m = 100 GeV 10− G Events pp → j j G (→ γ γ), m = 500 GeV G pp → j j G (→ γ γ), m = 1000 GeV 10−2 G pp → j j γ γ pp → j j γ γ QCD = 0 10−3

10−4

10−5

10−6

0 500 1000 1500 2000 2500 M ( γ γ ) [ GeV/c2 ] 1 2

Diphoton Mass Dijet Mass Decay width scenarios WG =10GeV

Decay width scenarios

WG =10%M G WG =10GeV

WG =10%M G Optimization study

• Fix diphoton mass window at 2σ • Optimize the selection cuts for the kinematics to maximize S significance = S + B + (0.25B)2 • 3 mass points: 150 GeV, 250 GeV, 500 GeV • 2 decay width scenarios

WG =10GeV WG =10%M G

• Increase background statistics to optimize cuts for higher mass (1000 GeV) Selection criteria (not final)

Delta eta (j1 j2) > 4.0 WG =10GeV

WG =10%M G > 6.0 P_T (gamma2) > 30 GeV/c M (j1 j2) > 1000 GeV/c^2 P_T (j1) > 30 GeV/c P_T (j2) > 30 GeV/c P_T (gamma1) > 60 GeV/c

Reference

• http://www.physik.uzh.ch/en/researcharea/lhcb/outreach/ StandardModel.html • Alvarez-Gaume L., Ellis J., 2008, APJ, 672, 834 • http://cms.web.cern.ch/news/observation-new-- mass-125-gev • CMS Collaboration. Letters B 716 (2012) 30–61. • A. Flórezb, A. Gurrola, W, Johns, Y.D. Oh, P. Sheldon, D. Teague, T. Weiler. Physics Letter B, Volume 767, 10 April 2017, Pages 126-132.