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Unification of fundamental interactions Hans Peter Nilles Physikalisches Institut Universit ¨ at Bonn Unification of fundamental interactions, Hawaii, September 2014 – p. 1/45

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Page 1: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Unification of fundamentalinteractions

Hans Peter Nilles

Physikalisches Institut

Universitat Bonn

Unification of fundamental interactions, Hawaii, September 2014 – p. 1/45

Page 2: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Standard Model

We have a standard model of elementary particle physics.It is based on

gauge symmetries SU(3)× SU(2)× U(1)

three families of quarks and leptons

a scalar Higgs boson

It is extremely successful,

but there are many free parameters

and some open questions.

Is there physics beyond the standard model?

Unification of fundamental interactions, Hawaii, September 2014 – p. 2/45

Page 3: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Outline

The Standard Model (SM)

Three basic questions

Reasons to go beyond the SM

Grand unification and supersymmetry

Extra dimensions and "Local Grand Unification"

Some group theory: The beauty of SO(10)

Strong motivation for E8

Extra dimensions from String Theory

How to test?

Unification of fundamental interactions, Hawaii, September 2014 – p. 3/45

Page 4: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

History

Gravity 1915

Quantum Electrodynamics (QED) ca. 1950

Yang-Mills theory for weak interactions 1954

"Higgs" mechanism 1964

Electroweak standard model 1967

Renormalizability of nonabelian gauge theoriesca. 1972

Quantum chromodynamics (QCD) ca. 1973

Discovery of gauge bosons W± and Z0 1983

Discovery of Higgs boson 2012

Unification of fundamental interactions, Hawaii, September 2014 – p. 4/45

Page 5: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Standard Model

Unification of fundamental interactions, Hawaii, September 2014 – p. 5/45

Page 6: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

A family of quarks and leptons

The gauge group is SU(3)× SU(2)× U(1)Y

(uα, dα)Y=1/6 (νe, e)Y=−1/2

(uα)Y=−2/3 (e)Y=1

(dα)Y=1/3

with α = 1, 2, 3 the SU(3)-index.Observe that

i

Yi = 0 and∑

i

Y 3

i = 0

Unification of fundamental interactions, Hawaii, September 2014 – p. 6/45

Page 7: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

A family of quarks and leptons

The gauge group is SU(3)× SU(2)× U(1)Y

(uα, dα)Y=1/6 (νe, e)Y=−1/2

(uα)Y=−2/3 (e)Y=1

(dα)Y=1/3 (ν)Y=0

with α = 1, 2, 3 the SU(3)-index.Observe that

i

Yi = 0 and∑

i

Y 3

i = 0

Unification of fundamental interactions, Hawaii, September 2014 – p. 7/45

Page 8: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Three basic questions

Some fundamental questions remain unanswered

The origin of the structure of a family?

Why three copies ?Question of I. Rabi: who ordered the muon?

Why gauge group SU(3)× SU(2)× U(1)?

and require physics beyond the Standard Model.

Page 9: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Three basic questions

Some fundamental questions remain unanswered

The origin of the structure of a family?

Why three copies ?Question of I. Rabi: who ordered the muon?

Why gauge group SU(3)× SU(2)× U(1)?

and require physics beyond the Standard Model.

Some other reasons to go beyond the SM

dark matter of the universe

baryon asymmetry, neutrino oscillations

“Landau Pole” of electromagnetic U(1)

Unification of fundamental interactions, Hawaii, September 2014 – p. 8/45

Page 10: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

The Quest for Unification

magnetism

electricityel.mag

weak interactions

SU(2)×U(1)

100 GeV

strong interactions (QCD)1016 GeVMGUT

celestrialmovementterrestrialmovement

GUT

Gravitation

?

1019 GeVMPlanck

Unification of fundamental interactions, Hawaii, September 2014 – p. 9/45

Page 11: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Grand Unification

Embed the SM gauge group

into a single grand unified group!

examples are SU(5) and SO(10).

Page 12: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Grand Unification

Embed the SM gauge group

into a single grand unified group!

examples are SU(5) and SO(10).

But there are a few obstacles:

“equality” of gauge coupling constants

the “doublet-triplet” splitting problem

the breakdown of the grand unified gauge group.

Unification of fundamental interactions, Hawaii, September 2014 – p. 10/45

Page 13: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Standard Model

Unification of fundamental interactions, Hawaii, September 2014 – p. 11/45

Page 14: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Supersymmetric SM

Unification of fundamental interactions, Hawaii, September 2014 – p. 12/45

Page 15: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Susy thresholds

Unification of fundamental interactions, Hawaii, September 2014 – p. 13/45

Page 16: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

New particles

Unification of fundamental interactions, Hawaii, September 2014 – p. 14/45

Page 17: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Supersymmetry

Unification of matter and radiation

consistent with grand unification

stabilizes the weak scale

provides candidates for dark matter

allows for a mechanism of baryogenesis

Page 18: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Supersymmetry

Unification of matter and radiation

consistent with grand unification

stabilizes the weak scale

provides candidates for dark matter

allows for a mechanism of baryogenesis

Preferred grand unified gauge groups

SO(10) and SU(5) include SU(3)× SU(2)× U(1)

explain the structure of families of quarks and leptons

5 + 10 representations of SU(5)

16-dimensional spinor representation of SO(10)

Unification of fundamental interactions, Hawaii, September 2014 – p. 15/45

Page 19: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Binary code for quarks and leptons

(n1, n2, n3, n4, n5) with ni = 0, 1 and∑

i

ni = even

(1, 1, 1, 1, 0) 5 combinations

(1, 1, 0; 1, 1) d

(1, 1, 1; 0, 1) (νe, e)

(1, 1, 0, 0, 0) 10 combinations

(1, 1, 0; 0, 0) u

(1, 0, 0; 1, 0) (u, d)

(0, 0, 0; 1, 1) e

(0, 0, 0, 0, 0) 1 combination νe

Unification of fundamental interactions, Hawaii, September 2014 – p. 16/45

Page 20: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Basic questions: where are we?

We have made some pogress.

The origin of the structure of a family:answer is 16-dim. spinor representation of SO(10)

Why three copies: not known yet,but group theory is proven to be unsuccessful.

Why SU(3)×SU(2)×U(1): is replaced by: why SO(10)?

Page 21: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Basic questions: where are we?

We have made some pogress.

The origin of the structure of a family:answer is 16-dim. spinor representation of SO(10)

Why three copies: not known yet,but group theory is proven to be unsuccessful.

Why SU(3)×SU(2)×U(1): is replaced by: why SO(10)?

Reminder: still some problems with grand unification:

evolution of couplings requires supersymmetry

“doublet-triplet” splitting

breakdown of grand unified group

Unification of fundamental interactions, Hawaii, September 2014 – p. 17/45

Page 22: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Why SO(10): Dynkin diagrams

Lie groups come in 4 infinite series SU(N), SP (2N),SO(2N + 1), SO(2N) and 5 exceptional groups.

Not all of them are useful for grand unification as they donot provide chiral representations to explain parity violationof weak interactions.

Unification of fundamental interactions, Hawaii, September 2014 – p. 18/45

Page 23: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Simply Laced Lie Groups

Unification of fundamental interactions, Hawaii, September 2014 – p. 19/45

Page 24: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Maximal Group E8

E8 is the maximal group.

There are, however, no chiral representations in d = 4.

Unification of fundamental interactions, Hawaii, September 2014 – p. 20/45

Page 25: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

E7

Next smaller is E7.

No chiral representations in d = 4 either.

Unification of fundamental interactions, Hawaii, September 2014 – p. 21/45

Page 26: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

E6

E6 allows for chiral representations even in d = 4.

Unification of fundamental interactions, Hawaii, September 2014 – p. 22/45

Page 27: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

E5 = D5

E5 is usually not called exceptional.

It coincides with D5 = SO(10).

Unification of fundamental interactions, Hawaii, September 2014 – p. 23/45

Page 28: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

E4 = A4

E4 coincides with A4 = SU(5).

Unification of fundamental interactions, Hawaii, September 2014 – p. 24/45

Page 29: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

E3

E3 coincides with A2 × A1 which is SU(3)× SU(2).

Unification of fundamental interactions, Hawaii, September 2014 – p. 25/45

Page 30: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Strong motivation for E8

E8 would require higher dimensions

E8 is strongly motivated from string theory(E8 × E8 heterotic string and M/F theory)

E8 has chiral representations in d = 8n+ 2

String theory requires d = 10

E8 broken in process of compactification (e.g. to E5)

Page 31: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Strong motivation for E8

E8 would require higher dimensions

E8 is strongly motivated from string theory(E8 × E8 heterotic string and M/F theory)

E8 has chiral representations in d = 8n+ 2

String theory requires d = 10

E8 broken in process of compactification (e.g. to E5)

Extra dimensions allow for the concept of“Local Grand Unification”:

this solves the doublet-triplet splitting problem

and provides the breakdown of the GUT group.

Unification of fundamental interactions, Hawaii, September 2014 – p. 26/45

Page 32: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Local Grand Unification

Unification of fundamental interactions, Hawaii, September 2014 – p. 27/45

Page 33: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

The Quest for Unification

magnetism

electricityel.mag

weak interactions

SU(2)×U(1)

100 GeV

strong interactions (QCD)1016 GeVMGUT

celestrialmovementterrestrialmovement

GUT

Gravitation

?

1019 GeVMPlanck

Unification of fundamental interactions, Hawaii, September 2014 – p. 28/45

Page 34: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Three basic questions, again

Some basic questions are answered.

The origin of the structure of a family:answer is 16-dim representation of SO(10)

Why three copies:topological properties of compactified extra dimensions

Why SO(10)?It is the grand-grand daughter E5 of E8.

Local Grand unification:allows for “incomplete multiplets”

Page 35: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Three basic questions, again

Some basic questions are answered.

The origin of the structure of a family:answer is 16-dim representation of SO(10)

Why three copies:topological properties of compactified extra dimensions

Why SO(10)?It is the grand-grand daughter E5 of E8.

Local Grand unification:allows for “incomplete multiplets”

Answers require physics beyond the SM!

We need new experimental input.

Unification of fundamental interactions, Hawaii, September 2014 – p. 29/45

Page 36: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Physics beyond the SM

Standard model is incomplete

problems with unification

dark matter

baryogenesis

inclusion of gravity

Page 37: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Physics beyond the SM

Standard model is incomplete

problems with unification

dark matter

baryogenesis

inclusion of gravity

There must be new physics somewhere.

Where is it?

Is it at the TeV scale?

Why is there no signal yet at the LHC?

Unification of fundamental interactions, Hawaii, September 2014 – p. 30/45

Page 38: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

LHC and physics beyond SM

0 2 4 6 8 10 12 140.10

0.15

0.20

0.25

0.30

Ρ

Ξf

500 1000 15002000

m 3� 2=15 TeV

Ξ3=0.33

BP2

Strong constraints on MSSM from 126 GeV Higgs mass.The coloured regions are excluded while the hatchedregion indicates the current reach of the LHC.

Unification of fundamental interactions, Hawaii, September 2014 – p. 31/45

Page 39: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Pre-LHC expectations

0 2 4 6 8 10 12 140.10

0.15

0.20

0.25

0.30

Ρ

Ξf

500 1000 15002000

m 3� 2=15 TeV

Ξ3=0.33

BP2

Constraints on MSSM from the Higgs mass.The coloured regions are excluded while the hatchedregion indicates the current reach of the LHC.

Unification of fundamental interactions, Hawaii, September 2014 – p. 32/45

Page 40: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

LHC and physics beyond SM

0 2 4 6 8 10 12 140.10

0.15

0.20

0.25

0.30

Ρ

Ξf

500 1000 15002000

m 3� 2=15 TeV

Ξ3=0.33

BP2

Strong constraints on MSSM from 126 GeV Higgs mass.The coloured regions are excluded while the hatchedregion indicates the current reach of the LHC.

Unification of fundamental interactions, Hawaii, September 2014 – p. 33/45

Page 41: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Benchmark model

Unification of fundamental interactions, Hawaii, September 2014 – p. 34/45

Page 42: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

The quest for “Precision Susy”

Two important arguments for supersymmetry

solution to the hierarchy problem

gauge coupling unification

We want to take these two arguments as serious aspossible and reanalyze the MSSM within this scheme.We make two assumptions:

demand precision gauge unification

require smallest supersymmetric masses possible

What are the consequences for the search at LHC?

Unification of fundamental interactions, Hawaii, September 2014 – p. 35/45

Page 43: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Susy thresholds

Unification of fundamental interactions, Hawaii, September 2014 – p. 36/45

Page 44: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Precision gauge unification

1

g2i (MGUT)=

1

g2i (MZ)−

bMSSMi

8π2ln

(

MGUT

MZ

)

+1

g2i,Thr

Low scale thresholds:

1

g2i,Thr

=bMSSMi − bSM

i

8π2ln

(

MSUSY

MZ

)

The measure for gauge unification:

ǫ3 =g23(MGUT)− g2

1,2(MGUT)

g21,2(MGUT)

Unification of fundamental interactions, Hawaii, September 2014 – p. 37/45

Page 45: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Unification versus MSUSY

200 500 1000 2000 5000 10 000-0.03

-0.02

-0.01

0.00

0.01

0.02

MSUSY @GeVD

Ε 3

precision unification

tan Β = 10

MSUSY should thus be in the few-TeV range.

Unification of fundamental interactions, Hawaii, September 2014 – p. 38/45

Page 46: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

The Susy-Scale

If all supersymmetric partners have the same mass M,then MSUSY = M .For non-universal masses we have an effective scale:

MSUSY ∼

m32/19

Wm

12/19

hm

3/19H

m28/19g

Xsfermion

with

Xsfermion =∏

i=1...3

m3/19

L(i)

m3/19

D(i)

m7/19

Q(i)L

m2/19

E(i)m

5/19

U (i)

Unification of fundamental interactions, Hawaii, September 2014 – p. 39/45

Page 47: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

LHC limits are weak

Unification of fundamental interactions, Hawaii, September 2014 – p. 40/45

Page 48: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Dark Matter Relic Density

-3 -2 -1 0 1 2 3

log10 WΧh 2

WD

Mh

2

Distribution of thermal neutralino relic density for thebenchmark sample with (solid) or without (dashed) theassumption of precision gauge coupling unification.

Unification of fundamental interactions, Hawaii, September 2014 – p. 41/45

Page 49: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

LHC limits are weak

Unification of fundamental interactions, Hawaii, September 2014 – p. 42/45

Page 50: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Limits from direct detection

10 20 50 100 200 500 1000 200010-48

10-47

10-46

10-45

10-44

10-43

m Χ�

1@GeVD

Σp@c

m2 D XENON 100

Direct detection experiments might check the scheme.

Unification of fundamental interactions, Hawaii, September 2014 – p. 43/45

Page 51: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

Conclusions

The quest for unification of fundamental interactions

requires new physics beyond the Standard Model:like e.g. supersymmetry and extra dimensions

Basic questions could be answered

family as a 16-dim spinor of SO(10)

SO(10) as the grand-grand daughter of E8

extra dimensions explain repetition of families

Consequences:

we need new experimental input to test the ideas!

Unification of fundamental interactions, Hawaii, September 2014 – p. 44/45

Page 52: Unification of fundamental interactionsThe Standard Model (SM) Three basic questions Reasons to go beyond the SM Grand unification and supersymmetry Extra dimensions and "Local Grand

The LHC shows us where to go

Unification of fundamental interactions, Hawaii, September 2014 – p. 45/45