/
A Realization of Effective SUSY A Realization of Effective SUSY

A Realization of Effective SUSY - PowerPoint Presentation

yoshiko-marsland
yoshiko-marsland . @yoshiko-marsland
Follow
390 views
Uploaded On 2016-11-23

A Realization of Effective SUSY - PPT Presentation

Zhen hua Zhao ITPCAS Liu amp Zhao   arXiv13127389 1 Contents Motivation The Model Phenomenological Consequence Summary 2 Higgs with 125 GeV mass 3 SM is completed and selfconsistent ID: 492481

susy gauge generation coupling gauge susy coupling generation scale arxiv higgs tev mass sector amp problem symmetry squarks hep

Share:

Link:

Embed:

Download Presentation from below link

Download Presentation The PPT/PDF document "A Realization of Effective SUSY" is the property of its rightful owner. Permission is granted to download and print the materials on this web site for personal, non-commercial use only, and to display it on your personal computer provided you do not modify the materials and that you retain all copyright notices contained in the materials. By downloading content from our website, you accept the terms of this agreement.


Presentation Transcript

Slide1

A Realization of Effective SUSY

Zhen-hua ZhaoITP,CAS Liu & Zhao   arXiv:1312.7389

1Slide2

Contents

MotivationThe ModelPhenomenological ConsequenceSummary2Slide3

Higgs with 125

GeV mass3

SM is completed and self-consistentSlide4

Gauge Hierarchy Problem

When extrapolated to higher scale Λ, Higgs mass suffers quadratic divergence problem

TeV

SUSY is good candidate for solving this problem

4Slide5

Search for SUSY

Nothing found5Slide6

Motivation

LHC constraints on SUSY particles 1st & 2nd generation squarks heavy as 10 TeVOriginal motivation for SUSY: Naturalness 3

rd

generation &

Higgsino

,

gaugino

light as 1

TeV

A model realizing this mass spectrum needed

6Slide7

Effective SUSY

For solving FCNC problem induced by soft terms“irrelevancy” hypothesis: 1st&2nd

generation

squarks

very heavy e.g. 10

TeV

“Naturalness” criterion:

3

rd

generation

squarks

should stay at 1

TeV

7

A. G. Cohen et al

hep

-ph/9607394Slide8

Framework

8

Liu

hep

-ph/0408234

N. Craig et al

arXiv:1103.3708Slide9

Gauge-Mediated-SUSY-Breaking

Hidden SectorG1 Sector

G2 Sector

9Slide10

Gauge Symmetry Breaking

G1G2

SM Gauge Symmetry

10Slide11

Gauge Coupling Constants

11

orSlide12

Yukawa Coupling

Only Yukawa coupling for 3rd generation allowed Irrelevant operators allowed by G1 G2 exist

After Gauge Symmetry Breaking

12Slide13

Produce Yukawa Coupling

An extra vector-like generation under G2

13

N. Craig et al

arXiv:1103.3708Slide14

Higgs mass and A-term

A. Arbey et al arXiv:1112.3028

14Slide15

Higgs-Messenger coupling

Z. F. Kang et al arXiv:1203.2336

15Slide16

Fields in G2 sector

16Slide17

Strong Unification

The ratio of gauge couplings flow to an infrared fixed point

D.

Ghilencea

et al

hep

-ph/9707462

17

Landau Pole

EW scale

Intermediate scale M

Slide18

Gauge coupling running

Landau Pole

EW scale

Intermediate scale M

18

Slide19

Summary

Effective SUSY can reconcile naturalness requirement with experimental results A realistic model is introduced and its phenomenological consequence discussedNot only hierarchy among sparticles but also fermions among three generations can be producedStrong coupling can be predicted without Grand Unification

19