セミナー@富山大学 2012.04.17

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Generating multi-jet events with MadGraph

Yoshitaro Takaesu (KEK)

October 27, 2016 1

Overview: Simulation for LHC

October 27, 2016 2

Parton Shower Generator

Matrix Element Generator

Event Generator

Detector Simulator

Importance of multi-jet at the LHC

Multi-jet signature appears in many New Physics models.

Event Generator should be able to generate > 4 jets.

October 27, 2016 3

Status of ME Generators

Model Alpgen HELAC Sherpa MadGraph

SM 6 jets 10 jets ? 6,7 jets 4,5 jets

MSSM ✕ ? 5 jets 4,5 jets

Others ✕ ✕ 5 jets 4,5 jets

There is no ME generator which can simulate New Physics with > 5 jets.

October 27, 2016 4

What is MadGraph?

5

Matrix-Element & Event Generator

October 27, 2016 5

Input

Event generator (MadEvent)

Output

Matrix-Element Generator (“MadGraph”)

+ Fortran Code

Model + process

Events

October 27, 2016 6

MG

MSSM, ADD,

2HDM,etc

Feyn-Rules

Higher Dim. Op.

Spin-3/2

Spin-2

NLO

Interface

PYTHIA

Detector Simulator

ROOTLagrangian

Limitation of MGGenerated Codes (> 8MB) cannot be compiled in usual PC.

October 27, 2016 7

8 MB

The file size of codes for QCD processes

Structure of QCD Amp

October 27, 2016 8Color flow

Color Factorcolor-ordered amp.

i: Color flow

October 27, 2016 9

Color Flow

Structure of QCD Amp

October 27, 2016 10Color flow

Color Factorcolor-ordered amp.

i: Color flow

How to overcomethe Limitation

October 27, 2016 11

October 27, 2016 12

STRATEGY

Divide

Speed up • Amp EvaluationOff• -shell Recursive Relations

• Re-organize Color Summation1/Nc expansion

Speed up Amp Evaluation

October 27, 2016 13

October 27, 2016 14

Off-shell Recursive Relations

Step #

# of vertex evaluations

October 27, 2016 15

Time performance

October 27, 2016 16

October 27, 2016 17

Recursive Relations for gluonic sub-amplitude

Re-organize Color Sum

October 27, 2016 18

October 27, 2016 19

1/Nc expansion

Polynomial of Nc:

Multi-jet event generation

Generate events with • Leading Color Approximation

For each event, include • higher order corrections into its weight.

October 27, 2016 20

Leading color summation

Color-flow sampling

( ~ 40,000 for gg -> 7g )

October 27, 2016 21

Too LARGE

Event is a set of momenta, helicities and a color flow

Higher order corrections

• For each event with a color flow

– Specify needed color flows for the higher order corrections

– Evaluate higher order corrections for the phase space point and reweight

– Re-unweight

October 27, 2016 22

Sample Results

October 27, 2016 23

October 27, 2016 24

October 27, 2016 25

Total cross sections

October 27, 2016 26

October 27, 2016 27

Distributions

ConclusionWe proposed a method to generate multi• -jet events with MadGraph.

Implemented gluonic off– -shell recursive relations and generate color-ordered amps.

Generated LO events by sampling color flows–

Shown results for gluonic processes for LO event –

generation.

October 27, 2016 28

OutLook

Include higher order corrections in • 1/Nc exp.

Generate events with quarks•

Detailed study for many distributions of Multi• -jet events

Apply the framework to New Physics • Pheno.

October 27, 2016 29

October 27, 2016 30

In color decomposition, we usually use Gell-Man matrices or modified matrices for .

Gell-Man:

Modified:

Color-Flow decomposition uses another set of matrices for .

Here are the generators of .

By using this basis, we can simplify the color factors as much as we can: 0 or 1.

Color-Flow basis

33

QCD Lagrangian can be written as

34

We rewrite this by introducing a U(1) gauge boson

35

9 U(3) gluons are independent and their generator matrices are

The color of a gluon can be expressed by a set of color indeces: (i, j).

There is also the abelian gluon in this theory.

Feynman Rules 1

36

Color Flow diagrams

Color Flow

Feynman Rules 2

37

The abelian gluon is decoupled from U(3) gluons.

This is the color-flow decomposition of a n-gluon amplitude.

From these rules, we evaluate a color-fixed scattering amplitude.

n-gluon amplitude

: (n-1)! non-cyclic permutaions

For n-gluon case, are the same asthe Color-Ordered ones.

color factor: 0 or1 partial amplitude

We add abelian gluon amplitudes to the U(3) gluon ones.

e.g.)

1 quark line and amplitude

There are other contributions from propagating abelian gluons

e.g.)

2 quark lines and amplitude

October 27, 2016 41

Amplitude

Color Basis

Helicity &Color

Sum

Recursive Relations

Color-Flow Basis

– Compilable

– Symmetric

– Gauge invariant

October 27, 2016 42

Off-shell Recursive Relations

Divide MG code by C.O. Amp

are

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