Upload
zahina
View
25
Download
3
Tags:
Embed Size (px)
DESCRIPTION
The Big Bang, the LHC and the Higgs Boson. Dr Cormac O’ Raifeartaigh (WIT). Overview. I. LHC What, How and Why II. Particle physics The Standard Model III. LHC Expectations T he Higgs boson and beyond Big Bang cosmology. High-energy proton beams Opposite directions - PowerPoint PPT Presentation
Citation preview
The Big Bang, the LHC and the Higgs Boson
Dr Cormac O’ Raifeartaigh (WIT)
Overview
I. LHC
What, How and Why
II. Particle physicsThe Standard Model
III. LHC Expectations
The Higgs boson and beyond
Big Bang cosmology
The Large Hadron Collider
No black holes
High-energy proton beams
Opposite directions
Huge energy of collision
Create short-lived particles
E = mc2 Detection and measurement
How
E = 14 TeV
λ =1 x 10-19 m
Ultra high vacuum
Low temp: 1.6 K
LEP tunnel: 27 km 1200 superconducting magnets
600 M collisions/sec
Why
Explore fundamental constituents of matter
Investigate inter-relation of forces that hold matter together
Glimpse of early universeHighest energy since BB
Mystery of dark matter Mystery of antimatter
T = 1019 K
t = 1x10-12 s
V = football
Cosmology
E = kT → T =
Particle cosmology
Particle detectors
4 main detectors
• CMS multi-purpose
•ATLAS multi-purpose
•ALICE quark-gluon plasma
•LHC-b antimatter decay
Particle detectors
Tracking devicemeasures momentum of charged particle
Calorimeter measures energy of particle by
absorption
Identification detector measures velocity of particle by Cherenkov radiation
II Particle physics (1930s)
• electron (1895)
• proton (1909)
• nuclear atom (1911)RBS
• what holds nucleus together?• what holds electrons in place?• what causes radioactivity?
Periodic Table: protons (1918)
• neutron (1932)
Four forces of nature Force of gravityHolds cosmos togetherLong range
Electromagnetic force Holds atoms together
Strong nuclear force: holds nucleus together
Weak nuclear force: Beta decay
The atom
Strong force
SF >> em
charge indep
protons, neutrons
short range
HUP
massive particle
Yukawa pion
3 charge states
New particles (1950s)
Cosmic rays Particle accelerators
cyclotronπ + → μ + + ν
Particle Zoo (1960s)
Over 100 particles
Quarks (1960s)
new periodic tablep+,n not fundamental symmetry arguments
(SU3 gauge symmetry)
SU3 → quarksnew fundamental particlesUP and DOWNprediction of -
Stanford experiments 1969
Gell-Mann, Zweig
Quantum chromodynamics
scattering experiments
colour
SF = chromodynamics
asymptotic freedom
confinement
infra-red slavery
The energy required to produce a separation far exceeds the pair production energy of a quark-antiquark pair,
Quark generations
Six different quarks(u,d,s,c,t,b)
Six leptons
(e, μ, τ, υe, υμ, υτ)
Gen I: all of matter
Gen II, III redundant
Electro-weak interaction
Gauge theory of em and w interaction
Salaam, Weinberg, Glashow
Above 100 GeV
Interactions of leptons by exchange of W,Z bosons
Higgs mechanism to generate mass
Predictions• Weak neutral currents (1973)• W and Z gauge bosons (CERN, 1983)• Higgs boson
The Origin of MassThe strong nuclear force cannot explain the mass of the electron though…
The Higgs BosonWe suspect the vacuum is full of another sort of matter that is responsible – the higgs…. a new sort of matter – a scalar?
Or very heavy quarks top mass = 175 proton mass
To explain the W mass the higgs vacuum must be 100 times denser than nuclear matter!!
It must be weak charged but not electrically charged
The Standard Model (1970s)
Strong force = quark force (QCD)
EM + weak force = electroweak
Matter particles: fermions
(quarks and leptons)
Force particles: bosons
Prediction: W+-,Z0 boson
Detected: CERN, 1983
Standard Model : 1980s
• Experimental success but Higgs boson outstanding
Key particle: too heavy?
III LHC expectations (SM)
Higgs boson
Determines mass of other particles
120-180 GeV
Set by mass of top quark, Z boson
Search…surprise?
Main production mechanisms of the Higgs at the LHC
Ref: A. Djouadi,hep-ph/0503172
For low Higgs mass mh 150 GeV, the Higgs mostly decays to two b-quarks, two tau leptons, two gluons and etc.
In hadron colliders these modes are difficult to extract because of the large QCD jet background.
The silver detection mode in this mass range is the two photons mode: h , which like the gluon fusion is a loop-induced process.
Higgs decay channels
Decay channels depend on the Higgs mass:
Ref: A. Djouadi, hep-ph/0503172
Ref: hep-ph/0208209
A summary plot:
Expectations: Beyond the SM
Unified field theory
Grand unified theory (GUT): 3 forces
Theory of everything (TOE): 4 forces
Supersymmetry
symmetry of fermions and bosons
improves GUT
makes TOE possible
Phenomenology
Supersymmetric particles?
Not observed: broken symmetry
IV Expectations: cosmology
√ 1. Exotic particles:S
√ 2. Unification of forces
3. Nature of dark matter?neutralinos?
4. Missing antimatter? LHCb
High E = photo of early U
1. Unification of forces: SUSY
2. SUSY = dark matter? double whammy
3. Matter/antimatter asymmetry?
LHCb
Particle cosmology
LHCb
Tangential to ringB-meson collectionDecay of b quark, antiquarkCP violation (UCD group)
• Where is antimatter?• Asymmetry in M/AM decay• CP violation
Quantum loops
SummaryHiggs bosonClose chapter on SM
Supersymmetric particlesOpen new chapter: TOE
CosmologyNature of Dark MatterMissing antimatter
Unexpected particles?New avenues
http://coraifeartaigh.wordpress.com
Epilogue: CERN and Ireland
World leader
20 member states
10 associate states
80 nations, 500 univ.
Ireland not a member
No particle physics in Ireland
European Organization for Nuclear Research