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Big Bang Experiment
Theories of the Origin of the
               Universe
   Theological “Theories”:
       Greek Mythology (Chaos)
       Hindu Mythology(Cosmic sleep of gods)
       Chinese creation myth (Pangu)
       Biblical account of the creation (God)


   Scientific Theories:
   Steady State
   Plasma theory
   Inflation Universe
   Big Bounce
   Cyclic Universe
   Big Bang
Evidence for the Big Bang
   Theory predicts an expanding universe
       Confirm by Red Shift (Doppler effect) in spectrum


   Theory predicts cosmic background radiation
       Background radiation was discovered in 1964 by
        Arno Penzias and Robert Wilson, who later won the
        Nobel Prize for this discovery
The Big Bang
• The universe does not
  expand into space – space
  itself expands

• Extrapolating back, space
  was small – the Big Bang


• Other dimensions could exist but still be small. String theory
  requires 6 extra dimensions.

• How can we test this possibility?
The Large Hadron Collider
LHC is located at CERN        The LHC collides protons
CERN is located near Geneva   Center of Mass E=14 TeV ~7X Fermilab
Part of CERN is in France     Very high luminosity ~100X Fermilab
The Large Hadrons Collider
Magnetic field at 7 TeV: 8.33 Tesla
Operating temperature: 1.9 K
Number of magnets: ~9300
Number of main dipoles: 1232
Number of quadrupoles: ~858
Number of correcting magnets: ~6208
Number of RF cavities: 8 per beam;
 Field strength at top energy ≈ 5.5 MV/m
 Power consumption: ~120 MW
The LHC what for ?
   Particle physics needs proton-proton centre of
    mass energy in the 1 TeV region where the
    Standard Model without Higgs Sector is
    expected to fail.
   Need for a exploratory machine (= high
    discovery potential) to search for Higgs and the
    spectrum of SUSY particles.
Why large ?
   Colliders use magnetic fields in order to keep
    particles on a circular orbit with radius R
       R [m] = 3.33 p [GeV] / B [T]
   B limited by technology, cost, power
    consumption to < 10 T
       For p = 10000 GeV, R > 3 km (circumference C > 20
        km)
       Not all the circumference can be covered by dipoles
Why a hadron (pp) collider ?

   Hadron colliders are exploratory machines giving access to a diversity of
    physics processes
       Hadronic
       Protonic (gg, qg, qq)
   proton-proton centre of mass energy
       Not fixed = covers wide energy range (“broad band”)
       Lower than the pp center of mass energy (~1/6)
       Need pp center of mass energy of O(10 TeV) to reach 1 TeV proton-proton centre of
        mass energy.
   Proton luminosity
       Depending on the proton luminosity and the proton distribution function (pdf) of the
        proton.
Why collider ?
   Proton beam on fixed target
       √s = √(2pmp) ~ √p
                 p




   Two protons of equal energy colliding
       √s = 2p ~ p

                       p    p
Already today, beams are available
close to the nominal beam parameters
required for the LHC !




                                                450 GeV

                                       26 GeV




                                                          LEAR => LEIR
Superconducting Cables


                                                       ∅1 mm

    ∅6 µm

 Typical value for operation at 8 T and 1.9 K: 800 A




            Rutherford cable

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KANAHIYA

  • 2. Theories of the Origin of the Universe  Theological “Theories”:  Greek Mythology (Chaos)  Hindu Mythology(Cosmic sleep of gods)  Chinese creation myth (Pangu)  Biblical account of the creation (God)  Scientific Theories:  Steady State  Plasma theory  Inflation Universe  Big Bounce  Cyclic Universe  Big Bang
  • 3. Evidence for the Big Bang  Theory predicts an expanding universe  Confirm by Red Shift (Doppler effect) in spectrum  Theory predicts cosmic background radiation  Background radiation was discovered in 1964 by Arno Penzias and Robert Wilson, who later won the Nobel Prize for this discovery
  • 4. The Big Bang • The universe does not expand into space – space itself expands • Extrapolating back, space was small – the Big Bang • Other dimensions could exist but still be small. String theory requires 6 extra dimensions. • How can we test this possibility?
  • 5. The Large Hadron Collider LHC is located at CERN The LHC collides protons CERN is located near Geneva Center of Mass E=14 TeV ~7X Fermilab Part of CERN is in France Very high luminosity ~100X Fermilab
  • 6. The Large Hadrons Collider Magnetic field at 7 TeV: 8.33 Tesla Operating temperature: 1.9 K Number of magnets: ~9300 Number of main dipoles: 1232 Number of quadrupoles: ~858 Number of correcting magnets: ~6208 Number of RF cavities: 8 per beam; Field strength at top energy ≈ 5.5 MV/m Power consumption: ~120 MW
  • 7. The LHC what for ?  Particle physics needs proton-proton centre of mass energy in the 1 TeV region where the Standard Model without Higgs Sector is expected to fail.  Need for a exploratory machine (= high discovery potential) to search for Higgs and the spectrum of SUSY particles.
  • 8. Why large ?  Colliders use magnetic fields in order to keep particles on a circular orbit with radius R  R [m] = 3.33 p [GeV] / B [T]  B limited by technology, cost, power consumption to < 10 T  For p = 10000 GeV, R > 3 km (circumference C > 20 km)  Not all the circumference can be covered by dipoles
  • 9. Why a hadron (pp) collider ?  Hadron colliders are exploratory machines giving access to a diversity of physics processes  Hadronic  Protonic (gg, qg, qq)  proton-proton centre of mass energy  Not fixed = covers wide energy range (“broad band”)  Lower than the pp center of mass energy (~1/6)  Need pp center of mass energy of O(10 TeV) to reach 1 TeV proton-proton centre of mass energy.  Proton luminosity  Depending on the proton luminosity and the proton distribution function (pdf) of the proton.
  • 10. Why collider ?  Proton beam on fixed target  √s = √(2pmp) ~ √p p  Two protons of equal energy colliding  √s = 2p ~ p p p
  • 11.
  • 12. Already today, beams are available close to the nominal beam parameters required for the LHC ! 450 GeV 26 GeV LEAR => LEIR
  • 13. Superconducting Cables ∅1 mm ∅6 µm Typical value for operation at 8 T and 1.9 K: 800 A Rutherford cable