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Particle Fever 1 Introduction by Peter Skands School of Physics and Astronomy Monash University Melbourne - Aug 21 - 2015

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Page 1: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

Particle Fever

1

Introduction by Peter Skands School of Physics and Astronomy

Monash University

M e l b o u r n e - A u g 2 1 - 2 0 1 5

Page 2: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

Fundamental Particle Physics

2

The aim of particle physics is to study matter and force

at the most fundamental level

Page 3: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

P. S K A N D S

Real Da

ta

Theory vs Experiment

3

Calculat

ions

Real Un

iverse

Theory

Model

Scientific Method

Page 4: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

P. S K A N D S

๏Monash University

๏Open Day - 2015

The Large Hadron Collider

4

The Large Hadron Collider

Geneva, Switzerland

The LHC at CERN currently produces the highest energies we can create in lab conditions

“Stable beams” for run 2: June 3rd, 2015

Collision Energy now: 13 Tera-eV (~ 1 million times higher than nuclear fusion)

Page 5: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

P. S K A N D S

CERN: European Organization for Nuclear Research

5

~ 10 000 scientists work at CERN.

20 European Member S tates and around 60 other count r ies

F lags of CERN’s Member S tates

27

Yearly budget ~ 1 billion CHF ~ 1.4 billion AUD

25

7

16

13455

108

11

982

979280

45

244

Page 6: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

P. S K A N D S

๏Many from One (well … from Two, really) •Quantum processes can convert the kinetic energy of the beam particles into rest energy (mass) + momentum of outgoing particles

!!

๏What are we really colliding? •Take a look at the quantum level

Colliding Protons

6

E = mc2p

1 + p2/(m2c2)E = energy m = mass p = momentum c = speed of light

u u

d

Parton Distribution Functions

Hadrons are composite, with time-dependent structure:

udgu

p

fi(x, Q2) = number density of partons iat momentum fraction x and probing scale Q2.

Linguistics (example):F2(x, Q2) =

!

i

e2i xfi(x, Q2)

structure function parton distributions

Page 7: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

P. S K A N D S

Such Stuff as Beams are Made Of

7

๏Lifetime of typical fluctuation ~ rp/c (=time it takes light to cross a proton) •~ 10-23 s; Corresponds to a frequency of ~ 500 billion THz

๏To the LHC, that’s slow! (reaches “shutter speeds” thousands of times faster) •Planck-Einstein: E=hν ➜ νLHC = 13 TeV/h = 3.14 million billion THz

๏➜ Protons look “frozen” at moment of collision •But they have a lot more than just two “u” quarks and a “d” inside

๏Hard to calculate, so use statistics to parametrise the structure •Every so often I will pick a gluon, every so often a quark (or antiquark) •Measured at previous colliders, as function of energy fraction

๏Then compute the probability for all possible quark and gluon reactions and compare with experiments …

OK… there’s a bit more to it, but you get the idea

Page 8: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

L H C @ h o m e 2 . 0Te s t 4 T h e o r y - A V i r t u a l A t o m S m a s h e r

O v e r 2 0 0 0 b i l l i o n s i m u l a t e d c o l l i s i o n e v e n t s

p p

LHC Physics Center at CERN

������������� �����������������������*

Annex I - "Description of Work"�������������������������������������� ���������������������������� ���������!������������� ��� �� ������������"�������������������������#$%%&'(��"���� ���

Page 9: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

P. S K A N D S

Test4Theory - LHC@home

9

New Users/Day

May June July Aug Sep

July 4th 2012

The  LHC@home  2.0  project  Test4Theory  allows  users  to  par:cipate  in  running  simula:ons  of  high-­‐energy  par:cle  physics  using  their  home  computers.  

The  results  are  submiAed  to  a  database  which  is  used  as  a  common  resource  by  both  experimental  and  theore:cal  scien:sts  working  on  the  Large  Hadron  Collider  at  CERN.

http://lhcathome.web.cern.ch/projects/test4theory

Page 10: Introduction by Peter Skands School of Physics and ...skands.physics.monash.edu/slides/files/Skands-ParticleFever.pdf · Particle Fever 1 Introduction by Peter Skands School of Physics

P. S K A N D S

Higgs Discovery

1 0

HIGGS DISCOVERY!

Image credit: CERN