Overview of Particle Physics -- the path to the Standard Model 1 Topics historical flashback over development of the field o o o o o “prehistory” 19th century electron, radioactivity, nucleus cosmic rays spectroscopy era collider era standard model of particle physics 2 A Century of Particle Physics J.J Thomson Top quark 1995 Electron – 1897 3 Sizes and distance scales visible light: wavelength ≈5∙10-7m virus 10-7m molecule 10-9m atom 10-10m nucleus 10-14m nucleon 10-15m quark <10-18m 4 The Building Blocks of a Dew Drop dew drop: 1021 molecules of water. Each molecule = one oxygen atom and two hydrogen atoms (H2O). Atom: nucleus surrounded by electrons. Electrons bound to the nucleus by photons nucleus of a hydrogen atom = single proton. Proton: three quarks, held together by gluons just as photons hold the electron to the nucleus in the atom 5 Very early era (19th century) chemistry, electromagnetism discharge tubes, “canal rays”, “cathode rays” photoelectric effect (Hertz, 1887) radioactivity (Becquerel, 1895) X-rays (Röntgen, 1895) 6 Atoms, Nucleus electron: first hint that atom not indivisible natural radioactivity understanding of composition of atom, nucleus atom = nucleus surrounded by electrons (Geiger, Marsden, Rutherford, 1906 -1911) hydrogen nucleus = proton, is component of all nuclei (1920) neutron (Bothe, Becker, Joliot-Curie, Chadwick, 1930 – 1932) 7 8 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 9 10 Cosmic rays -- “elementary” particles new detectors (cloud chambers, emulsions) exposed to cosmic rays discovery of many new particles positron (anti-electron) : predicted by Dirac (1928), discovered by Anderson 1932 muon (μ): 1937 Nedermeyer pion (π) predicted by Yukawa (1935), observed 1947 (Lattes, Occhialini, Powell) strange particles (K, Λ, Σ,….. 11 Particle Zoo 1940’s to 1960’s : Plethora of new particles discovered (mainly in cosmic rays): e-, p, n, ν, μ-, π±, π0, Λ0, Σ+ , Σ0 , Ξ,…. question: Can nature be so messy? are all these particles really intrinsically different? or can we recognize patterns or symmetries in their nature (charge, mass, flavor) or the way they behave (decays)? 12 The Particle Zoo! ± , 0 , ± , e, ± 0 0 K , K S, K L, 0 + , p, n, , 0 , , , … 13 Particle spectroscopy era 1950’s – 1960’s: accelerators, better detectors even more new particles are found, many of them extremely short-lived (decay after 10-21 sec) 1962: “eightfold way”, “flavor SU(3)” symmetry (Gell-Mann, Ne’eman) allows classification of particles into “multiplets” Mass formula relating masses of particles in same multiplet quark model – three different kinds of quarks (u, d, s) Allows prediction of new particle Ω- , with all of its properties (mass, spin, expected decay modes,..) subsequent observation of Ω- with expected 14 properties at BNL (1964) ΩBNL 1964 http://www.bnl.gov/bnlweb/history/Omega-minus.asp eight-fold way quark model – particles made up of three different “quarks” – u, d, s p = uud, n = udd,… Ω- = sss refinement of these ideas, more quarks, “color”, gauge field theory Standard Model 15 Standard Model A theoretical model of interactions of elementary particles, based on quantum field theory Symmetry: SU(3) x SU(2) x U(1) “Matter particles” Quarks: up, down, charm,strange, top, bottom Leptons: electron, muon, tau, neutrinos “Force particles” Gauge Bosons o (electromagnetic force) o W, Z (weak, electromagnetic) o g gluons (strong force) Higgs boson spontaneous symmetry breaking of SU(2) mass 16 Contemporary Physics Education Project17 Particles of Standard Model Leptons -1/3 -1 0 u u u d d d e e c c c s s s t t t b b b t t g g g g g g g g I II III Z W± Bosons Fermions +2/3 Quarks 18 “every-day” matter Proton Neutron d u u u d Photon d Electron e Electron Neutrino e 19 Electromagnetic interaction Proton q1 Photon q1q2 F k 2 r Electron q2 20 Weak interaction Beta decay Neutron u d Mean lifetime of a free neutron ~ 10.3 minutes Proton d u d Mean lifetime of a free proton > 1031 years! u W- Anti-electron Neutrino Electron e e 21 The Strong Force d u g u Strong force caused by the exchange of gluons d 22 Forces (interactions) Strong interaction 1 Binds protons and neutrons to form nuclei Electromagnetic interaction 10-2 Binds electrons and nuclei to form atoms Binds atoms to form molecules etc. Weak interaction 10-10 Causes radioactivity Gravitational interaction 10-39 Binds matter on large scales 23 What holds the world together? interaction strong electromagnetic weak gravity participants quarks charged particles all particles all particles 1 10-2 10-10 10-39 g gluon relative strength field quantum (boson) photon W± Z0 G graviton 24 The Discovery of Top Quark 1977 – 1992 Many null results 1992 – 1993 A few interesting events show up 1994, CDF First evidence mt ~ 170 GeV/c2 1995 – CDF, DØ Discovery! 1994, DØ mt > 131 GeV/c2 25 Creating Top Anti-Top Quark pairs b P t t b e t uc -1/ 3 2 / 3 W e t d s P -2 / 3 1/ 3 e t uc - W - - - e t d s 26 - Artist’s impression of a top event 27 What do we actually “see” _ t t e jets Muon Jet-1 Jet-2 Missing energy Electron 28 “event display” of a DØ top event t t e jets 29 Ωb (http://www.fnal.gov/pub/presspass/images/DZero-Omega-discovery.html 2008 DØ experiment at Fermilab: discover brother of Ω- , the Ωb Ω- = sss, Ωb = ssb, theory predicts properties, decay modes, .. confirmed by experiment 30 Summary we’ve come a long way …… Standard Model (theory of particle interactions) works embarrassingly well! Has been tested by many hundreds of precision measurements over last three decades – very few measurements differ by more than 1 or 2 standard deviations Even some amount of frustration – always hope to see experimental result in disagreement with theory But there are some open questions ………………… 31