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Theoretische Physik – Fundamentale Wechselwirkungen

Daniel Grumiller

Institute for Theoretical Physics Vienna University of Technology

Proseminar LV 138.039, 27. Mai 2011

(2)

Outline

Fundamentale Wechselwirkungen Particle Physics

Cosmology

Energy budget of the Universe

Personen am Institut

(3)

Outline

Fundamentale Wechselwirkungen Particle Physics

Cosmology

Energy budget of the Universe

Personen am Institut

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 3/18

(4)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

(5)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 4/18

(6)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

(7)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 4/18

(8)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

(9)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 4/18

(10)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

(11)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 4/18

(12)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

(13)

Periodic Table of Elementary Particles

Particles we know and have observed: I Three light generations

I Two leptons and quarks in each

I All matter particles are fermions (spin 1/2)

I Characterized by charges and masses

I Only difference between generations: masses!

I Forces mediated by particles (spin 1)

I Electromagnetic force: photonγ

I Weak force: vector bosons W±, Z

I Strong force: gluons g

I That’s it! (well, almost...)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 4/18

(14)

Standard Model of Particle Physics A theory of (almost) everything:

Standard Model (SM) Lagrange density Fµν: bosons,Ψ: fermions,Φ: Higgs

I All experiments so far in accordance with SM!

I Amazingly accurate!

e.g. gyromagnetic ratio of µ Experiment (2002):

gexpµ

2 = 1.0011659209±0.0000000005

Theory (2009):

gµthe

2 = 1.0011659183±0.0000000004 I Currently SM improved at LHC

(15)

Standard Model of Particle Physics A theory of (almost) everything:

Standard Model (SM) Lagrange density Fµν: bosons,Ψ: fermions,Φ: Higgs

I All experiments so far in accordance with SM!

I Amazingly accurate!

e.g. gyromagnetic ratio of µ Experiment (2002):

gexpµ

2 = 1.0011659209±0.0000000005

Theory (2009):

gµthe

2 = 1.0011659183±0.0000000004

I Currently SM improved at LHC

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 5/18

(16)

Standard Model of Particle Physics A theory of (almost) everything:

Standard Model (SM) Lagrange density Fµν: bosons,Ψ: fermions,Φ: Higgs

I All experiments so far in accordance with SM!

I Amazingly accurate!

e.g. gyromagnetic ratio of µ Experiment (2002):

gexpµ

2 = 1.0011659209±0.0000000005

Theory (2009):

gµthe

2 = 1.0011659183±0.0000000004 I Currently SM improved at LHC

(17)

Gravity

Gravity = Geometry

I SM describes three of four forces as Quantum Field Theories

I Gravity so far is described mostly as classical theory, General Relativity

I General Relativity = geometry = theory of metricgµν

I Einstein eqs. deceptively simple

Rµν−1

2gµνR= 8πG Tµν

left: geometry, right: matter

I Tested to high accuracy:

Perihelion shifts (β−1<2·10−4) Radar echo delay (γ−1<2·10−5) Binary pulsars (α3<4·10−20)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 6/18

(18)

Gravity

Gravity = Geometry

I SM describes three of four forces as Quantum Field Theories

I Gravity so far is described mostly as classical theory, General Relativity

I General Relativity = geometry = theory of metricgµν

I Einstein eqs. deceptively simple

Rµν−1

2gµνR= 8πG Tµν

left: geometry, right: matter

I Tested to high accuracy:

Perihelion shifts (β−1<2·10−4) Radar echo delay (γ−1<2·10−5) Binary pulsars (α3<4·10−20)

(19)

Gravity

Gravity = Geometry

I SM describes three of four forces as Quantum Field Theories

I Gravity so far is described mostly as classical theory, General Relativity

I General Relativity = geometry = theory of metricgµν

I Einstein eqs. deceptively simple

Rµν−1

2gµνR= 8πG Tµν

left: geometry, right: matter

I Tested to high accuracy:

Perihelion shifts (β−1<2·10−4) Radar echo delay (γ−1<2·10−5) Binary pulsars (α3<4·10−20)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 6/18

(20)

Gravity

Gravity = Geometry

I SM describes three of four forces as Quantum Field Theories

I Gravity so far is described mostly as classical theory, General Relativity

I General Relativity = geometry = theory of metricgµν

I Einstein eqs. deceptively simple

Rµν−1

2gµνR= 8πG Tµν

left: geometry, right: matter

I Tested to high accuracy:

Perihelion shifts (β−1<2·10−4) Radar echo delay (γ−1<2·10−5) Binary pulsars (α3<4·10−20)

(21)

Gravity

Gravity = Geometry

I SM describes three of four forces as Quantum Field Theories

I Gravity so far is described mostly as classical theory, General Relativity

I General Relativity = geometry = theory of metricgµν

I Einstein eqs. deceptively simple

Rµν−1

2gµνR= 8πG Tµν

left: geometry, right: matter

I Tested to high accuracy:

Perihelion shifts (β−1<2·10−4) Radar echo delay (γ−1<2·10−5) Binary pulsars (α3<4·10−20)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 6/18

(22)

Missing Entries in the Periodic Table Particle in the SM not found yet:

Higgs particle! (or whatever causes electro-weak symmetry breaking...) LHC will find it this decade!

Particles beyond SM not found yet:

Graviton (gravitational wave) LIGO will find it this decade! Further particles beyond SM? Inflaton?, SUSY?, Axions?, Dark Spinors?, Kaluza–Kleins?, ... LHC and Astro/Astroparticle- -physics may find clues!

(23)

Missing Entries in the Periodic Table Particle in the SM not found yet:

Higgs particle! (or whatever causes electro-weak symmetry breaking...) LHC will find it this decade!

Particles beyond SM not found yet:

Graviton (gravitational wave) LIGO will find it this decade!

Further particles beyond SM? Inflaton?, SUSY?, Axions?, Dark Spinors?, Kaluza–Kleins?, ... LHC and Astro/Astroparticle- -physics may find clues!

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 7/18

(24)

Missing Entries in the Periodic Table Particle in the SM not found yet:

Higgs particle! (or whatever causes electro-weak symmetry breaking...) LHC will find it this decade!

Particles beyond SM not found yet:

Graviton (gravitational wave) LIGO will find it this decade!

Further particles beyond SM?

Inflaton?, SUSY?, Axions?, Dark Spinors?, Kaluza–Kleins?, ...

LHC and Astro/Astroparticle- -physics may find clues!

(25)

Brief History of the Universe

CMB:

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 8/18

(26)

Brief History of the Universe

CMB:

I 370000 years: 3000K≈0.3eV

I Universe became transparent

I Fluctuations: “echo” of Big Bang

I COBE (1989-1993), WMAP (since 2001), Planck (since 2009)

(27)

Brief History of the Universe

CMB:

I 370000 years: 3000K≈0.3eV

I Universe became transparent

I Fluctuations: “echo” of Big Bang

I COBE (1989-1993), WMAP (since 2001), Planck (since 2009)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 8/18

(28)

Brief History of the Universe

CMB:

I 370000 years: 3000K≈0.3eV

I Universe became transparent

I Fluctuations: “echo” of Big Bang

I COBE (1989-1993), WMAP (since 2001), Planck (since 2009)

(29)

Brief History of the Universe

CMB:

I 370000 years: 3000K≈0.3eV

I Universe became transparent

I Fluctuations: “echo” of Big Bang

I COBE (1989-1993), WMAP (since 2001), Planck (since 2009)

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 8/18

(30)

Brief History of the Universe

CMB:

Above: COBE satellite (900km) Below: WMAP satellite at Lagrange point L2 (1.5∗106km)

(31)

Standard Model of Cosmology A theory of (almost) everything:

I Cosmology is now a precision science!

I E.g. energy densities know within %-range:

b,Ων,Ωγ,Ωm,ΩΛ, ... (baryons, neutrinos, radiation, matter, cosmological constant, ...)

I Currently many experiments!

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 9/18

(32)

Standard Model of Cosmology A theory of (almost) everything:

I Cosmology is now a precision science!

I E.g. energy densities know within %-range:

b,Ων,Ωγ,Ωm,ΩΛ, ...

(baryons, neutrinos, radiation, matter, cosmological constant, ...)

I Currently many experiments!

(33)

Standard Model of Cosmology A theory of (almost) everything:

I Cosmology is now a precision science!

I E.g. energy densities know within %-range:

b,Ων,Ωγ,Ωm,ΩΛ, ...

(baryons, neutrinos, radiation, matter, cosmological constant, ...)

I Currently many experiments!

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 9/18

(34)

Summary of What We Know

I Standard Models of Particle Physics and Cosmology (including General Relativity) consistent with nearly everything that we observe in Nature, with amazing accuracy

I Missing pieces that we know indirectly to exist are Higgs and graviton

I If they exist both will be found in this decade

Is anything else missing?

(35)

Summary of What We Know

I Standard Models of Particle Physics and Cosmology (including General Relativity) consistent with nearly everything that we observe in Nature, with amazing accuracy

I Missing pieces that we know indirectly to exist are Higgs and graviton

I If they exist both will be found in this decade

Is anything else missing?

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 10/18

(36)

Summary of What We Know

I Standard Models of Particle Physics and Cosmology (including General Relativity) consistent with nearly everything that we observe in Nature, with amazing accuracy

I Missing pieces that we know indirectly to exist are Higgs and graviton

I If they exist both will be found in this decade

Is anything else missing?

(37)

Summary of What We Know

I Standard Models of Particle Physics and Cosmology (including General Relativity) consistent with nearly everything that we observe in Nature, with amazing accuracy

I Missing pieces that we know indirectly to exist are Higgs and graviton

I If they exist both will be found in this decade

Is anything else missing?

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 10/18

(38)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation: cosmological constant

I BUT: why so small??? 10−123

(39)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation: cosmological constant

I BUT: why so small??? 10−123

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 11/18

(40)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation: cosmological constant

I BUT: why so small??? 10−123

(41)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation: cosmological constant

I BUT: why so small??? 10−123

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 11/18

(42)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation: cosmological constant

I BUT: why so small??? 10−123

(43)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation:

cosmological constant

I BUT: why so small??? 10−123

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 11/18

(44)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation:

cosmological constant

I BUT: why so small??? 10−123

(45)

What is the Universe made of?

Collect all the available data:

I Progress of last two decades: we understand less than 5% of the Universe, and we know it!

I Dark Matter: many indications, many candidates

I Plausible candidate: SUSY

I Might be discovered at LHC

I More than 70% “Dark Energy”

I Simplest correct explanation:

cosmological constant

I BUT: why so small??? 10−123

Unresolved fundamental issues!

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Fundamentale Wechselwirkungen 11/18

(46)

Outline

Fundamentale Wechselwirkungen Particle Physics

Cosmology

Energy budget of the Universe

Personen am Institut

(47)

Herbert Balasin — Allgemeine Relativit¨atstheorie

Klassische und Quantenaspekte

Steckbrief:

Herbert Balasin 27 publications Recent collaborations:

U. Br¨unn U. Tours Vienna U.

Distributionelle Relativit¨atstheorie und Schleifen-Quantengravitation

Ultrarelativistische Schwarze L¨ocher Quantisierung von pp-Gravitationswellen

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Personen am Institut 13/18

(48)

Daniel Grumiller — Schwarze L¨ocher

Quantengravitation, das holographische Prinzip und Anwendungen

Steckbrief:

Daniel Grumiller 67 publications Recent collaborations:

ASC and LMU Munich Brown U.

Charles U.

ESA ETH Zurich Leipzig U.

Michigan U.

MIT Pamukkale U.

Penn State U.

Perimeter Institute Sao Paulo ABC Federal St. Petersburg State U.

Uppsala U.

Waterloo U.

Washington U. (Seattle) Waterloo U.

YITP Stony Brook

Schwarze L¨ocher in Astrophysik und Kosmologie...

... und neuerdings auch in Elementarteilchenphysik und kondensierter Materie mittels der AdS/CFT Korrespondenz

(49)

Anton Rebhan — Quark-Gluon-Plasmaphysik

Schwerionenst¨osse am RHIC und am LHC

Steckbrief:

Anton Rebhan 135 publications Recent Collaborations:

Bielefeld U.

Brandon U.

Cambridge U. DAMTP Chicago U.

Dubna JINR

Ecole Normale Superieure ECT Trento

Frankfurt U. FIAS Gettysburg Coll.

Hannover U.

Helsinki U.

Leipzig U.

Madrid IFT and AU Saclay SPhT Santa Barbara KITP Washington U. (Seattle) Winnipeg U.

YITP Stony Brook

Schwerionenkollisions-Event im STAR Detektor am RHIC:

Theoretische Beschreibung mit thermischer Quantenfeldtheorie und AdS/CFT Korrespondenz

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Personen am Institut 15/18

(50)

Andreas Schmitt — Dense quark matter

Color superconductivity and compact stars

Steckbrief:

Andreas Schmitt 30 publications Recent collaborations:

Frankfurt U.

Hefei CUST MIT

North Carolina State U.

Saga U.

Washington U. (St. Louis) YITP Stony Brook

Das Phasendiagramm der QCD — ein ungel¨ostes Problem!

liq

T

µ

gas

QGP

CFL

nuclear superfluid

heavy ion collider

neutron star

non−CFL hadronic

(51)

Manfred Schweda — Nicht-kommutative Quantenfeldtheorie

Physikalische Gesetze in nicht-kommutativer Raumzeit

Steckbrief:

Manfred Schweda 112 publications Recent collaborations:

Espirito Santo U.

Fed. Fluminense U.

Lyon IPN Leipzig MPI U. Vienna Vicosa federal U.

Kurze Distanzen: Unsch¨arfe in Raumzeit!

QFT = Quantenfeldtheorie

D. Grumiller — Theoretische Physik – Fundamentale Wechselwirkungen Personen am Institut 17/18

(52)

Harald Skarke — Stringtheorie

Die Geometrie der verborgenen Dimensionen

Steckbrief:

Harald Skarke 33 publications

Eine Calabi-Yau Mannigfaltigkeit:

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