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Particle Physics and LHC Physics David Krofcheck Canterbury Teachers Workshop July 18 th D. Krofcheck Canterbury Teachers Workshop 1

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Particle Physics and LHC Physics. David Krofcheck Canterbury Teachers Workshop July 18 th. The place to be for high energy physicists. Lac Léman. Jura. CERN (FR). Geneva airport. CERN (CH). Large Hadron Collider. 27 km (17 miles) circumference - PowerPoint PPT Presentation

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Page 1: Particle Physics and LHC Physics

Particle Physics and LHC Physics

David Krofcheck

Canterbury Teachers Workshop July 18th

D. Krofcheck Canterbury Teachers Workshop 1

Page 2: Particle Physics and LHC Physics

Large Hadron Collider

CMSexperiment

Thanks to Lucas Taylor, 2012

The place to be for high energy physicists

CERN (CH)

CERN (FR)

Genevaairport

Lac LémanJura

Page 3: Particle Physics and LHC Physics

Large Hadron Collider

CMSexperiment

Thanks to Lucas Taylor, 2012

Large Hadron Collider

3

• 27 km (17 miles) circumference

• 1600 superconducting magnets at 1.9° K (-271.3° C or – 459.7° F)

• 120 tonnes of liquid helium

• Accelerates beams of protons to 99.9999991% the speed of light

Large Hadron Collider

Page 4: Particle Physics and LHC Physics

The CMS detector at the Large Hadron Collider

Muon Barrel

Tracker (Pixels and Strips)

EM Calorimeter Hadron Calorimeter

Muon Endcaps

Forward Calorimeter

Beam Scintillator Counters

CASTOR

ZDC

D. Krofcheck Pitt/CMU July 2011 4

New Zealand

Page 5: Particle Physics and LHC Physics

D. Krofcheck Pitt/CMU July 2011 5

The really important CMS detectors

Page 6: Particle Physics and LHC Physics

Aristotle : all matter is made up of various combinations of Earth, air, fire and water

What is matter?

This belief about the nature of matter lasted for 2000 years

solids

liquids

gases

change

D. Krofcheck Canterbury Teachers Workshop 6

Page 7: Particle Physics and LHC Physics

Democritus

Lucretius

John Dalton

Development of the Atomic Theory

Aristotle

D. Krofcheck Canterbury Teachers Workshop 7

Page 8: Particle Physics and LHC Physics

Ideas about Atoms

1800’s

John Dalton – meteorologist and teacher

- successfully explained chemical reactions by proposing all matter is made up of atoms.

- BUT they had no direct evidence!D. Krofcheck Canterbury Teachers Workshop 8

Page 9: Particle Physics and LHC Physics

DmitriMendeleev

Russian

1834-1907

Periodic TableSimilar chemical properties

D. Krofcheck Canterbury Teachers Workshop 9

Page 10: Particle Physics and LHC Physics

Periodic Table

?

Atoms

Rutherford (1909)

Bohr (1913)D. Krofcheck Canterbury Teachers Workshop 10

Page 11: Particle Physics and LHC Physics

...

proton neutron electron

• Are these the elementary particles, ?

• Are they composed of even more elementary particles??

• Particle and Nuclear Physics are the studies to answer this questionD. Krofcheck Canterbury Teachers Workshop 11

Page 12: Particle Physics and LHC Physics

Matter Particles

1932 p, n, e ν

1937 μ

1940s mesons π, K

1950s particles Λ, Δ, Σ, ...

…hundreds of new particles were discovered!

D. Krofcheck Canterbury Teachers Workshop 12

Page 13: Particle Physics and LHC Physics

In 1964 the idea of quarks was proposed… quark

s

u

d

u

proton

d

u

d

neutron

Gell-Mann

Zweig

These were elementary particle of, fractional electric charge, different flavours

D. Krofcheck Canterbury Teachers Workshop 13

Page 14: Particle Physics and LHC Physics

What is the composition of the proton

d u

uq(u) = +2/3q(d) = -1/3

q(p) = +1

...and of the neutrond u

d q(n) = -1/3 - 1/3 + 2/3= 0

D. Krofcheck Canterbury Teachers Workshop 14

Page 15: Particle Physics and LHC Physics

What glues the quarks together?

u u

d protonGluons, of course

D. Krofcheck Canterbury Teachers Workshop 15

Page 16: Particle Physics and LHC Physics

Elementary particles of matter

1st family: u, d, e- , e

2nd family: c, s, - ,

3rd family: t, b, - ,

lept

ons

1897

1995

Higgs4 July, 2012D. Krofcheck Canterbury Teachers Workshop 16

Page 17: Particle Physics and LHC Physics

Antimatter

Every particle has its antiparticle, of the same mass but opposite quantum numbers

eg. electron, e- : q(e-) =-1 , spin = -1/2 , m(e-) = 9.110-28 gr. positron, e+ : q(e+) =+1 , spin = +1/2 , m(e+) = 9.110-28 gr.

D. Krofcheck Canterbury Teachers Workshop 17

Page 18: Particle Physics and LHC Physics

Electromagnetic ForceGravitational Force

Strong Colour Force Weak Force

.... .

.átomo

nuclei n p + e- + e

d u + e- + e

1

10-2

10-5

10-40

All these interactions are manifestations of only

4 basic interactions

Page 19: Particle Physics and LHC Physics

Interaction Type

Electromagnetic γ (photon)

Strong g (gluon)

Weak bosons W, Z

Gravitational G (graviton)

Still not detected experimentally

Mediating Particle

Page 20: Particle Physics and LHC Physics

Example: Electromagnetic interaction

+ -+-p pe + e+

http://www.cerimes.education.fr/

Page 21: Particle Physics and LHC Physics

The Fundamental Interactionsare produced by the exchange of a particle mediator

The particles of matter interact across a distance by exchanging a “messenger” particle

http://www.cerimes.education.fr/

The interaction range decreases as the mass of the messenger particle increases.

Page 22: Particle Physics and LHC Physics

Standard Model of Particle Physics In a quantum description of matter and the laws of interaction

between them still do not know how to incorporate gravitation, but the rest of interactions are well described by a mathematical theory, the

Standard Model, able to make predictions that have been confirmed in experiments.

lept

ons

•M

esse

nger

s •

inte

ract

ions

Page 23: Particle Physics and LHC Physics

Standard Model

(~1980)

Components of matter Interactions

Symmetry

This model requires that the particle messengers are massless,But the W and Z are very heavy!! problem of the origin of mass

Page 24: Particle Physics and LHC Physics

Higgs Boson The British physicist Dr. Peter Higgs proposed (1964) the so-called Higgs mechanism:All the particles would be generated in the Big Bang without mass, but by interacting with the field created by the Higgs particle, the particles would acquire mass, the greater, the greater the interaction. This field would fill the whole universe.

Interaction with the Higgs field

Friction with a viscous liquid≡

Page 25: Particle Physics and LHC Physics

Higgs BosonThe British physicist Dr. Peter Higgs proposed (1964) the so-called Higgs mechanism:All the particles would be generated in the Big Bang without mass, but by interacting with the field created by the Higgs particle, the particles would acquire mass, the greater, the greater the interaction. This field would fill the whole universe.

Unico “Higgs” observado hasta ahora en un experimento…el propio Dr. Higgs!!

Friction with a viscous liquid≡Interaction with the

Higgs field

Page 26: Particle Physics and LHC Physics

Higgs Boson

.

A recent view of a Higgs at the CMS experiment

This particle predicted has not yet been unambiguously detected in experiments, hopefully we are hot on the trail!

Page 27: Particle Physics and LHC Physics

!!?? H Z0 Z0 μ+ μ- μ+ μ-

Page 28: Particle Physics and LHC Physics

Gauge Bosons – Z0 First detection in HI collisions!

First step is to find Z0 bosons in PbPb collisions

Z0 → μ+μ - observed for the first time in HI collisions!

Page 29: Particle Physics and LHC Physics

29

Z0 → e+e- observed for the first time in HI collisions!

Z0 → e+e- event candidate

Page 30: Particle Physics and LHC Physics

lead + lead collisions may liberate quarks

Page 31: Particle Physics and LHC Physics

Jet production in pp collisions

jet-jet correlation in QCD “vacuum”

D. Krofcheck Dijet Probes of Hot Nuclear Matter at the LHC 31

Jet

Jet

Page 32: Particle Physics and LHC Physics

Jet production in PbPb collisionsjet-jet correlation in QCD “medium”

γ – jet correlation to probe the medium?

D. Krofcheck Dijet Probes of Hot Nuclear Matter at the LHC 32

Page 33: Particle Physics and LHC Physics

E-ΔΕ1

E-ΔΕ2

Dijet imbalance in PbPb collisionsΔφ

Phys. Rev. C 84, 024906 (2011)

D. Krofcheck Dijet Probes of Hot Nuclear Matter at the LHC 33

Page 34: Particle Physics and LHC Physics

Jet production in PbPb collisions

D. Krofcheck Dijet Probes of Hot Nuclear Matter at the LHC 34

gamma-jet correlation in QCD “medium”

Gamma

Nuclear remnant Nuclear remnant

Page 35: Particle Physics and LHC Physics

• Momentum ratio shifts/decreases with centrality– jets shifting below the 30 GeV pT threshold not included

Submitted to PLB, arXiv:1205.0206

Observed momentum imbalance in γ – jet correlation

D. Krofcheck Dijet Probes of Hot Nuclear Matter at the LHC 35

Page 36: Particle Physics and LHC Physics
Page 37: Particle Physics and LHC Physics
Page 38: Particle Physics and LHC Physics

Energy Units!

1 eV = 1 electron VoltEnergy to ionise hydrogen = 13.6 eV

1 keV(kilo) = 1,000 eV = 103 eVMedical X-ray ~ 200 keV

1 MeV(Mega) = 1,000,000 eV = 106 eVAlpha particle decay of uranium 4.2 MeV

1 GeV(Giga) = 1,000,000,000 eV = 109 eVLEP collider beam (1989-2000) = 45 GeV

1 TeV(Tera) = 1,000,000,000,000 eV = 1012 eVHighest energy accelerator in world = 1 TeV (Tevatron)

Electron Volt – Energy gained by an electron when accelerated in an electric field through a potential difference of 1 volt.

Highest energiesfound in cosmic rays (>1020 eV)

Page 39: Particle Physics and LHC Physics

Interactions between matter particles

Page 40: Particle Physics and LHC Physics

Why are there so many different substances in the world?

D. Krofcheck Canterbury Teachers Workshop 40