Utrecht University The Nature of and Gerard t

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Utrecht University The Nature of and Gerard ’t Hooft Stockholm, August 27, 2004

Utrecht University The Nature of and Gerard ’t Hooft Stockholm, August 27, 2004

Sir James Clark Maxwell 1831 -1879 - Statistical Mechanics - Thermodynamics - Improved the

Sir James Clark Maxwell 1831 -1879 - Statistical Mechanics - Thermodynamics - Improved the mathematical formulation of Michael Faraday’s theories of electricity and magnetic lines of force. . .

The electro-magnetic force

The electro-magnetic force

Albert Einstein 1879 – 1955 1905: - Photo-electric effect - Special Relativity - Brownian

Albert Einstein 1879 – 1955 1905: - Photo-electric effect - Special Relativity - Brownian motion; statistical mechanics 1915: General relativity (gravitation)

Special Relativity

Special Relativity

Quantum Mechanics

Quantum Mechanics

Special Relativity + Quantum Mechanics = Elementary Particle Physics ( = High Energy Physics

Special Relativity + Quantum Mechanics = Elementary Particle Physics ( = High Energy Physics = Quantum Field Theory )

photon 1969 Leptons antileptons mesons Hadrons This is only 4 % of the matter

photon 1969 Leptons antileptons mesons Hadrons This is only 4 % of the matter in the Universe ! (See Licia Verde’s talk) baryons anti

Known from experiment Forces: the ELECTRO MAGNETIC force the forces the STRONG force the

Known from experiment Forces: the ELECTRO MAGNETIC force the forces the STRONG force the WEAK force

The Yang-Mills Field C. N. Yang and R. L. Mills, 1954

The Yang-Mills Field C. N. Yang and R. L. Mills, 1954

Yang - Mills quanta - o + proton - + o neutron

Yang - Mills quanta - o + proton - + o neutron

Multiplets According to the Yang-Mills-theory P N Nucleons pions Yang-Mills bosons

Multiplets According to the Yang-Mills-theory P N Nucleons pions Yang-Mills bosons

Peter Higgs

Peter Higgs

Breaking Rotational Symmetry THIS becomes an essential degree of freedom. . . … turning

Breaking Rotational Symmetry THIS becomes an essential degree of freedom. . . … turning the gauge force carriers massive ! And THIS is the Higgs degree of Freedom

S. L. Glashow St. Weinberg A. Salam

S. L. Glashow St. Weinberg A. Salam

Weinberg’s lepton model Leptons Gauge bosons Weinberg Model Higgs Anti – Leptons

Weinberg’s lepton model Leptons Gauge bosons Weinberg Model Higgs Anti – Leptons

The hadronic particles … Proton Antiproton Lambda Pi-plus Pi-zero

The hadronic particles … Proton Antiproton Lambda Pi-plus Pi-zero

The Yang-Mills Color Field Quantum Chromo Dynamics

The Yang-Mills Color Field Quantum Chromo Dynamics

Quark species weak quarks Antiquarks u u u d d d c strong c

Quark species weak quarks Antiquarks u u u d d d c strong c c s s t t b b s t b up down charm strange top bottom

The Standard Model Generation III Leptons Quarks Gauge Bosons g Higgs Graviton

The Standard Model Generation III Leptons Quarks Gauge Bosons g Higgs Graviton

Total cross sections CESR DORIS PEP PETRA TRISTAN

Total cross sections CESR DORIS PEP PETRA TRISTAN

The fourth force: Gravitation

The fourth force: Gravitation

The highway across the desert Today’s Limit … Planck length : GUTs

The highway across the desert Today’s Limit … Planck length : GUTs

SU(4) x SU(2) Further unification SO(10) 3 generations

SU(4) x SU(2) Further unification SO(10) 3 generations

The Super. String Theory

The Super. String Theory

A Black Hole

A Black Hole