peter athron david miller in collaboration with fine tuning in supersymmetric models

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Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

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Page 1: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Peter Athron

David Miller

In collaboration with

Fine Tuning In Supersymmetric Models

Page 2: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Overview

Little Hierarchy Problem

Traditional Measure

Define New Measure

Illustrate with SM Hierarchy Problem

Application to MSSM

Page 3: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

MSSM EWSB constraint (Tree Level) :

Sparticle mass limits ) Parameters

But

Little Hierarchy Problem

Peter Athron
Phrase better!!Maybe too long for slide?Just say some of this and display Key Words??
Page 4: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

R. Barbieri & G.F. Giudice, (1988)

Define Tuning

is fine tuned

% change in from 1% change in

Observable

Parameter

Traditional Measure

Peter Athron
Actually I've completely forgotten what this means!I should find out and then explain!!
Page 5: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Limitations of the Traditional Measure

Considers each parameter separately

The fine tuning is about cancellations between parameters . A good fine tuning measure considers all parameters together.

Implicitly assumes a uniform distribution of parameters

Parameters in LGUT may be different to those in LSUSY Corresponds to choosing parameters from a different probability distribution

Takes infinitesimal perturbations about the point

MSSM observables are complicated functions of many parameters. Many small isolated regions of parameter space may give the same value of the observable.

Considers only one observable

Theories may contain tunings in more than one observable

Peter Athron
Shouldn't I be calling them definitions?
Page 6: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

the volume of parameter space,

the subspace of s.t. the observables

Tuning occurs when variations in dimensionless parameters ) larger variations in dimensionless observables.

Parameter space point,

Tuning is defined as:

New Measure

Peter Athron
I think another key difference between our measure and Barbieri and Giudice's is that they take the limit where the variations go to zero. We don't want to do that!. We want the variations to be large so that cancellations are included! If our variations were too large in extent then we might not pick up finetuning as the Observable would move out of the region where experimental cuts in the space lead to the requirement of fine tuning. I.e m_h = 10TeV will be naturally produced by p_i of that scale which are not ruled out!
Peter Athron
Should I keep 'natural' in there
Peter Athron
B&G defined tuning as a function of the observable and a parameter. It was the level of tuning needed for in that parameter, with all others fixed, in order to get the observered value. we define tuning only as a function of the observable and consider how it responds to (uncorrelated) fluctuation in all the parameters
Page 7: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models
Page 8: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

SM Revisited

Page 9: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models
Page 10: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Choose a point P in the parameter space at GUT scale Take random fluctuations about this point. Using a modified version of Softsusy (B.C. Allanach)

Run to Electro-Weak Symmetry Breaking scale. Predict Mz and sparticle masses

Count how often Mz (and sparticle masses) is ok Apply fine tuning measure

Fine Tuning in the MSSM

Page 11: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

For example . . .

MSUGRA benchmark point SPS1a:

ALL

Page 12: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models
Page 13: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

If the tuning in the MSSM is fine for flat probability distributions:

Nature is fine tuned.

EWSB by some other mechanism than the Higgs

e.g. Technicolor

The Hierarchy problem is solved other new physics

e.g. Little Higgs, Large Extra Dimensions

Extended Higgs sector SSM’s are favoured e.g. NMSSM, nMSSM, ESSM

The MSSM parameters are not all equally likely.

What probability distribution ameliorates this tuning?

Is there a GUT with this distribution?

Page 14: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Fine Tuning in the SM SUSY

Broken SUSY appears fine tuned Little Hierarchy Problem Hint for a GUT theory?

Current measures of tuning neglect: Probability distribution of parameters. Many parameter nature of fine tuning Additional tunings in other observables Cancellations a finite distance from point

New measure addresses these issues Demonstrates an increase in tuning with the susy

scale.

Conclusions

Page 15: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Numerical Approximation

Where is the number of points in space

Page 16: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

+

physical mass = “bare mass” + “loops”

= +

divergent Cut off integral at Planck Scale

Fine tuning

Hierarchy Problem

Page 17: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Supersymmetry The only possible extension to space-time

Unifies gauge couplings

Provides Dark Matter candidates

Baryogenesis in the early universe

Elegant solution to the Hierarchy Problem!

Essential ingredient for M-Theory

Peter Athron
Do i mention Coleman-Mandula theorem on slide?Think carefully about phrasing.
Peter Athron
Do i really mean this. Might sound like I'm claiming susy is a gut. Susy allows running gauge couplings to intersect at at a single point. Could add graph showing couplings unifying
Page 18: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

Bosonic degrees of freedom = Fermionic degrees of freedom.

) Two scalar superpartners for each fermion

In Susy

No Fine Tuning?

Quadratic divergences cancelled!

Page 19: Peter Athron David Miller In collaboration with Fine Tuning In Supersymmetric Models

MSSM At Tree Level:

Sparticle mass limits ) Parameters

But

Exact Susy Softly Broken Susy

LEP search fruitless!! Lower bounds on sparticles

Fine Tuning reintroduced?

Little Hierarchy Problem

Peter Athron
Phrase better!!Maybe too long for slide?Just say some of this and display Key Words??