Upload
kellie-hampton
View
224
Download
0
Embed Size (px)
DESCRIPTION
CERN, 8 February, 2001 Egil Lillestøl, CERN & Univ. of Bergen Can not use light microscopes to study atoms !!! Quantum mechanics tells us that particles behave like waves and visa versa: h/p Use electron microscopes LEP the world’s biggest electron microscope electron
Citation preview
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Lectures recorded at :
http://www.cern.ch/wlap
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Can not use light microscopes to study atoms !!!
Quantum mechanics tells us thatparticles behave like waves and visa versa:
h/p
Use electron microscopes
LEP the world’s biggestelectron microscope
electron
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
electron
quark
New Stuff from E = Mc2
New, unstable particles, can NOT be explainedas made of up and down quarks only.
High Energy electron-proton scattering
Jet ofParticles
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
electron(energy U)
U= 1 eV= 1.6x10-19J(speed at positive plate18 000 km/s)
1 keV = 103 eV1 MeV = 106 eV1 GeV = 109 eV1 TeV = 1012 eV
LEP = 209 GeVLHC = 14 TeV
Practical Units
- +
1 Volt
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Einstein: E = Mc2
pc
use units such that c =1 E (GeV or MeV)p (GeV/c or MeV/c)M (GeV/c2 or MeV/c2)
M0c2Mproton = 0.931 GeV/c2 ≈ 1 GeV/c2 Melectron = 0.5 MeV/c2
( Mtop = 170 GeV/c2 )proton diameter = length scale:10-15 m = 1 fermi (femtometer)
E
Special Relativity:( E2= (pc)2 + (M0c2)2 )
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Creating New Matter with LEP
fully described by the Standard Model :
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Ingredients of the Standard Model
To explain all matter we need three generations of quarks We also have three generations of leptons.
THE COMPLETE PICTURE:
Quarks Leptons
charges: 2/3 -1/3 0 -1 up down e electron (e) charm strange muon ()
top bottom tau
Two different sorts of Matter particles:-composite particles made up of quarks (called HADRONS)-non composite particles like electrons and neutrinos (LEPTONS)
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
u
d
c
s
t
b
e
e
Charge
+2/3
-1/3
0
-1
quarks (q)
leptons
“Fundamental” Matter Particles
heavier
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
q q q
Composite Matter Particles (hadrons)made out of quarks ( q ) and anti quarks ( q )
Baryons Mesons
q q q q q
Anti BaryonsHundreds of possible
combinations or particles
hadrons
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Forces of Nature
name of field (wave) force carrier (particle)
gravitational field graviton (?) electromagnetic field (a) (photon) weak field Z0, W+, W-
strong (color) field 8 gluons, g
higgs field (*) h0, H0, H+, H-..
(*)Unifying the weak and the electromagnetic fieldsgiving mass to the Z and the W’s - all other particles !!!
(a) Electric and Magnetic Fields Unified by Maxwell (1864)
Big Question: Can all Force Fields be unified ?
(*)
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
the Strong Field (gluons) couple to Quarksthe Weak field (W’s and Z) couple to Leptonsthe Electromagnetic field couple to Charge
(classical: F = qE)the Gravitational field couple to Mass
(Newton: F = mg)
the Higgs field couple to Mass ! ! !In fact the Higgs field is responsible for the mass !
Can detailed studies of large number of Higgs Particlesgive us the explanation why we have three families ofquarks and leptons, and why they have such enormousmass differences ??
How the forces work
LHC will tell us !
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
The Forces and Particles as Fields
Newton and Gravity
Faraday and Fields
Forces as “Exchange” Particles
Particles as Fields
Forces and Particles as Quantum Fields
Quantum Fields are part of Space itself !
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
How does a point in empty space know exactlythe variety of particles it can produceand all their properties and their forces .... ???
Back to Heisenberg and Faraday:Particles and Forces are Quantum Fields fillingevery point of “Empty” Space (or the “Vacuum”).
The Fields materialize as Particles whenEnergy is fed into this Vacuum.
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Heisenberg’s Uncertainty Relation:
(x)(p) ≈ h/(2) or (t)(E) ≈ h/(2)
(valid for the Fields as well as the Vacuum)
h is Planck’s constant - a very small number, (6.6x10-34Js)x is position, p is momentum,t is time, and E is energy.(x) means uncertainty in position, etc
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Structures are temporary, the Pattern lasts for ever !
In every Point of “Empty” Space there is full Information on all possible particles andall the fundamental forces !
Particles are produced when energy is fed into the Vacuum.Particles appear and disappear, but the “memory” remains
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
With LEP Blowing into the Vacuum producing the Z0 particle
Energy (e+ + e-)
Collision Probability
Z0-mass
resonance curve
resonance width (E)
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
e- e+
e- e+
lepton
anti lepton
3 jetsZ0 Decays :
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
1989-1995: The 4 LEP experimentscollected and studied 17 million Z particles
Z particles decays “democratically” into all possible quark-anti quark pairs (sometimes accompanied by one or more gluons)and all possible lepton-anti lepton pairs.
Quarks and gluons seen as jets, and charged leptons as single tracksneutrino-anti neutrino pairs are NOT observed
However, the number of different neutrino species can be found from the resonance width (or lifetime) of the
Z particle
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Z0 resonance (line shape):
E (or M) = 91.2 GeV
E (or M) = 2.5 GeV
Heisenberg: (E) (t) = h/2 (h = 4x10-24 GeVs)
(t) is the lifetime and (E) the resonance widthgiving = 10-25 s corresponding to
Only three light neutrino species, i.e.only three lepton generations,and three quark generations.
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Z0
Lifetime of Z0 like water in a leaking bucket:
the more and bigger the holes - the shorter the lifetime
a hole = a decay channel; Sizes of the holes can be calculated using the Standard Model
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
How many “Holes” ?
Quark pairs: charge numberd-d, s-s, b-b 1/3 3 (x3)u-u, c-c 2/3 2 (x3)
Lepton pairs: charge numbere--e+, -- +, -- +, 1 3e- e, - , ? 0 2+?
Autumn 1989:Perfect match with 3 different neutrino species.
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
LEP, the Top and the Higgs
H
t tg
b b
jets
The “tune” of the bb-note has anearly imperceptible “overtone” due to the presence of thehiggs and the top quarks
This overtone can be measured and calculatedfrom the Standard Model with the higgs massand the top mass as free parameters
Predictions: top mass ≈ 175 GeV and higgs mass < 1000 GeV
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
LEP and the Higgs
Fermilab found the top with mass as predicted from LEP:
Standard Model Higgs: MH < 1000 GeV
Lightest Super Symmetric Higgs Mh < 200 GeV
Best fit : Mh ≈ 100 GeV
Within reach of LEP200 !
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Is the Higgs Idea falsified ?
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Higgs Hunting with LEP (Total energy 206.6 GeV)
e- e+H (115 GeV)
Z (91 GeV)
two Higgs jetscontainingB-particles
two Z jets
2.5 effect for a Higgs Particle at 115 GeV
(e- + e+) -----> (Z0 + H) -----> 4 jets
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
ALEPH DELPHI
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
B - Particles in DELPHI
CERN, 8 CERN, 8 February, 2001February, 2001Egil Lillestøl, CERN & Univ. of BergenEgil Lillestøl, CERN & Univ. of Bergen
Questions for the LHC
- Does Higgs Particles exist ?- Can all the Forces and Particles be unified ? (Super Symmetry)- Is Dark Matter made of Super Symmetric Particles ?- What happened to the Antimatter in the Universe ?- Did the Universe go through a Phase of Quark-Gluon Plasma ?- Are the Fundamental Particles two-dimensional Strings ?- Does the Universe have more than three Spatial Dimensions ?- Are there more Forces and Particles to be discovered ?- Accelerating Expansion of the Universe and Dark Matter- Could everything be just wrong ?
The LHC Experiments will be very Exciting !