Hand of Anna Röntgen. From Life magazine,6 April 1896

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FROM ELECTRONS TO QUARKS The development of Particle Physics QUARKNET 2001, FSU Laura Reina

Outline ffl What is Particle Physics? ffl The origins of Particle Physics: the atom (p,e ), radioactivity, and the discovery of the neutron (n). (1895-1932) ffl Cosmic Rays: the positron (e + ), the muon (μ ± ), the pion (ß ± ;ß 0 ), and the Kaon (K ± ;K 0 ). (1932-1959) ffl Colliders: more and more particles discovered, patterns emerge (1960's and on):! leptons and hadrons! electromagnetic, weak, and strong interactions ffl the Quark Model of hadrons and QCD: strong interactions ffl The Standard Model of Electroweak interactions ffl Open Problems ffl Beyond the Standard Model

What is Particle Physics? it is explaining the physical world, from the smallest atomic scale to the astronomical scales, in terms of the same! fundamental constituents of matter ( building blocks")! fundamental forces between them ( interactions"). ffl Are there irreducible building blocks?! how many?! properties? (mass, charge, flavor,...) ffl How do they interact?! how many forces?! differences/similarities? fflwhat is mass? fflwhat is charge? +

The Origins of Particle Physics In school text books we learn that ffl All matter is composed of atoms, which themselves form aggregates called molecules. ffl An atom contains a nucleus of positive charge +Z and Z electrons. ffl If the atomic mass is A, the nucleus contains Z protons and A Z neutrons. This picture did not exist in 1895 ::: ffl atoms creation of chemists ffl electron, proton and neutron were yet to be discovered ffl atomic spectra were known but not understood ffl cathode rays" discovered: look like particles with negative charge. ::: when Röntgen discovers x-rays!

Röntgen and X-rays: Hand of Anna Röntgen From Life magazine,6 April 1896

ffl 1896-97 : cathode rays" are negatively charged particles of charge e and mass m, s.t. e=m is 2000 times larger than H + Thomson's Model of the atom ffl 1896-1900: enormous effort in study of radioactive elements (Becquerel, Curie's, Rutherford) ffl 1906-1911: Geiger, Marsden and Rutherford's scattering experiments + Rutherford's Model of the atom But:! electron orbiting around the nucleus accelerates and therefore (Maxwell) radiates! electron looses energy by radiation: orbit decays! continuum spectrum and unstable atoms. Answers: 1924-1927 Quantum Mechanics (Planck,Bohr,De Broglie,Heisenberg,Schrödinger,Dirac,...)

WHAT IS INSIDE AN ATOM? J.J. Thomson s model: Plum pudding or raisin cake model atom = sphere of positive charge (diameter 10-10 m), with electrons embedded in it, evenly distributed (like raisins in cake) i.e. electrons are part of atom, can be kicked out of it atom no more indivisible!

Geiger, Marsden, Rutherford expt.

Rutherford model RUTHERFORD MODEL OF ATOM: ( planetary model of atom ) positive charge concentrated in nucleus (<10-14 m); negative electrons in orbit around nucleus at distance 10-10 m; electrons bound to nucleus by Coulomb force.

De Broglie, Bohr model

ffl 1932 : Chadwick discovers the neutron He 4 2 + Be 9 4! C12 6 + n 1 0 + The modern atom is complete However... Most is still to come!

The Development of Particle Physics ffl Evidence of very light neutral particle in fi decay: the electron neutrino (predicted by Pauli in 1930, discovered by Cowan and Reines in 1956-58) n! p + e + μν e ffl Cosmic Rays: atmospheric nuclear collision of incoming high energy protons produce new particles! 1932: positron (e + ) (Anderson), as predicted by Dirac (1928)! 1936-1951: the muon (μ ± ) and the pion (ß ± ;ß 0 ) ß +! μ + + ν μ μ +! e + + ν e + μν μ ß 0! flfl! 1943-1959: the discovery of strange particles", the Kaon (K ± ;K 0 ; μ K 0 ) K 0! ß + + ß K +! μ + + ν μ

Beta decay β decay n p + e _ + ν e β decay changes a neutron into a proton Only observed the electron and the recoiling nucleus non-conservation of energy Pauli predicted a light, neutral, feebly interacting particle (1930) the neutrino Although accepted since it fit so well, not actually observed initiating interactions until 1956-1958 (Cowan and Reines)

Cosmic rays Discovered by Victor Hess (1912) Observations on mountains and in balloon: intensity of cosmic radiation increases with height above surface of Earth must come from outer space Much of cosmic radiation from sun (rather low energy protons) Very high energy radiation from outside solar system, but probably from within galaxy

Positron Positron (anti-electron) Predicted by Dirac (1928) -- needed for relativistic quantum mechanics existence of antiparticles doubled the number of known particles!!! Positron track going upward through lead plate Photographed by Carl Anderson (August 2, 1932), while photographing cosmic-ray tracks in a cloud chamber particle moving upward, as determined by the increase in curvature of the top half of the track after it passed through the lead plate, and curving to the left, meaning its charge is positive.

Strange particles Kaon: discovered 1947; first called V particles K 0 production and decay in a bubble chamber

1940's! 1950's A plethora of particles is discovered (mainly in cosmic rays) e, p, n, ν e, μ, (ß ± ;ß 0 ), e + plus (K ±, K 0, μ K 0 ), Λ 0, μp, (± + ; ± 0 ), Ξ,... NATURE CANNOT BE SO MESSY! + ffl Are all these particle intrinsically different? OR ffl Can we recognize patterns or symmetries in their nature (charge,mass,flavor) or the way they behave (decays)?

1950's!... A new era for particle physics We can convert energy into particles E 2 = p 2 c 2 + m 2 c 4 and reproduce the primordial stages of our universe (almost...) + Collider Physics e + e, pμp,... With High Energies we can:! make objects of large mass! resolve structure at small distances

First Great Discoveries... ffl e ± ; μ ± ; fi ± and their neutrinos (we call them Leptons) are fundamental particles and interact electromagnetically and weakly" while ffl p, n, (ß ± ;ß 0 ), (K ±, K 0, μ K 0 ), Λ 0, (± + ; ± 0 ), Ξ,... (we call them Hadrons) are not fundamental particles! + They are made of QUARKS! named up, down, and strange and they interact electromagnetically, weakly", and strongly".

Quarks carry a COLOR charge un UP quark can be 8 >< >: up up up (green) (red) (blue) and interact exchanging GLUONS, the carriers of the STRONG FORCE u gluon d u u d proton Barions (qqq) Mesons (μqq) p! uud n! ddu ß ±! uμ d(μud) ± +! uus ß 0! uμu + dμ d K ±! uμs(μus) ± 0 ; Λ 0! uds Ξ 0! uss K 0 ( K μ 0 )! μsd(sμ d) ρ! uμ d ::: :::

Both Leptons and Quarks carry a Weak Charge as well as the usual electric charge and also interact exchanging: ffl Neutral EW force carriers : fl (photon), Z 0 (M fl =0,M Z =91 GeV) ffl Charged EW force carriers : W ± (M W =80 GeV) µ + ν µ μ +! e + + μν μ + ν e W e + ν e ß +! μ + + ν μ π + u d W µ ν + µ

Strings? Extra dimensions? atoms 01 01 01 ELECTRONS nucleus protons neutrons QUARKS (up, down)

Some Milestones...! Quantum Electrodynamics (QED) (1950's), (Feynman,Schwinger,Tomonaga)! Electroweak unification: the Standard Model (1960's) (Glashow,Weinberg,Salam)! SLAC/MIT elastic/inelastic scattering from nucleons (1956-1973)! Quark Model (1964) (Gell-Mann,Zweig)! Quantum Chromodynamics (QCD) (1970's) (Gross, Wilceck, Politzer,...)

More Quarks coming along... 1974! Discovery of the charm quark (ψ = cμc, D mesons) (BNL, SLAC) 1977! Discovery of the bottom quark (Y = bμ b, B mesons) (FERMILAB, DESY) 1995! Discovery of the top quark (no bound state) (FERMILAB) And more Forces... 1983! Discovery of the W ± and Z bosons, carriers of the WEAK FORCE (CERN) + As the Standard Model predicts 1990's! Precision tests of the Standard Model (CERN,SLAC,FERMILAB)

Standard Model

Open Problems... ffl What is the origin of mass?? + the Higgs boson a very elusive particle...! no direct evidence yet! many indirect pieces of evidence ffl Do forces unify?? ffl Are there more fundamental objects than just leptons and quarks?? ffl Are there extra dimensions?? i.e. are four dimensions enough??

Direct vs Indirect Evidence ffl Either you produce a new particle: Direct Evidence or Discovery ffl Or you see it in a virtual state": Indirect Evidence Very famous example: fi decay n! p + e + μν e n u d d u d u p W e Fermi's Theory: pointlike interaction ν µ decay rate / G = g2 M 2 W d W u e _ q 2 << M W 2 d g 2 u e ν e - ν e 2 M W

Why all these particles and forces?? Who ordered it? (Rabi) ffl Most of the particle the world is made of are : electrons, protons, and neutrons (e +, u, and d quarks). ffl This is because our world lives at very low energy. ffl All other particles were created at the high energies of the very early stages of our universe and we can nowadays recreate some of them in our laboratories, even if for very short time! Tevatron (pμp), Fermilab (Chicago) (2001)! B-factories (SLAC, KEK) (e + e )(1999)! LHC (pp), CERN (Geneva, CH) (ο 2006)! NLC/Tesla (e + e ) (ο 2020?)

We may have to look back at the universe to know more and try to unify the very large with the very small!