Upload
alvin-herron
View
212
Download
0
Tags:
Embed Size (px)
Citation preview
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Abigail Bickley, Dept of Chemistry, July 25, 2008
Large Hadron Collider
July 25, 2008 Abigail Bickley, PAN 2008 2
Where is the LHC?
July 25, 2008 Abigail Bickley, PAN 2008 3
Where is the LHC?Switzerland
France
Circumference: 27km = 16.8miles
July 25, 2008 Abigail Bickley, PAN 2008 4
Where is the LHC?
July 25, 2008 Abigail Bickley, PAN 2008 5
Deconstructing a Name• Collider:
– Two beams of particles circulate in opposite directions around the ring
– Beams intersect at 4 locations
– These locations are where the collisions occur and are observed by warehouse sized detectors
• Hadron• Large
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
July 25, 2008 Abigail Bickley, PAN 2008 6
Deconstructing a Name• Collider • Hadron:
– General category for the type of particles accelerated (protons and heavy nuclei)– Hadrons (from the Greek ‘adros’ meaning ‘bulky’) are particles composed of quarks.
The protons and neutrons that atomic nuclei are made of belong to this family. On the other hand, leptons are particles that are not made of quarks. Electrons and muons are examples of leptons (from the Greek ‘leptos’ meaning ‘thin’).
• Large
10-10 m
u u
d
10-15 m10-9 m
July 25, 2008 Abigail Bickley, PAN 2008 7
Deconstructing a Name• Large:
– The size of an accelerator is related to the maximum beam energy obtainable.– This is a function of the radius of the machine and the strength of the dipole
magnetic field that keeps particles in their orbits. – The LHC re-uses the 27‑km circumference tunnel that was built for the previous
big accelerator, LEP. – The size of the tunnel, magnets, cavities and other essential elements of the
machine, represent themain constraints that determine the design energy of 7 TeV per proton beam.
July 25, 2008 Abigail Bickley, PAN 2008 8
Colliders vs Cyclotrons• Cyclotrons:
– Produces a single beam of ions that are directed towards a stationary target
– Maximum beam energy is dependent upon the radius of the cyclotron
• Colliders:– When two beams collide, the energy of
the collision is the sum of the energies of the two beams.
– A beam of the same energy that hits a fixed target would produce a collision of much less energy.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
€
ECollision ∝ Ebeam
€
ECollision = Ebeam1 + Ebeam2
July 25, 2008 Abigail Bickley, PAN 2008 9
Recipe for Creating an Ion Beam
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
1 Ion Source:– All protons accelerated at CERN are obtained from standard hydrogen.– Protons are isolated by stripping orbiting electrons off of hydrogen atoms.– Although proton beams at the LHC are very intense, only 2 nanograms of
hydrogen are accelerated each day. – It would take the LHC about 1 million years to accelerate 1 gram of
hydrogen.
July 25, 2008 Abigail Bickley, PAN 2008 10
Recipe for Creating an Ion Beam
2 Multi-Stage Acceleration:– The accelerator complex is a succession of machines with
increasingly higher energies. – Each machine injects the beam into the next one, which brings the
beam to an even higher energy.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
0.050 GeV
1.4 GeV
25 GeV
450 GeV
7000 GeV
July 25, 2008 Abigail Bickley, PAN 2008 11
Recipe for Creating an Ion Beam
3 LHC = Final Acceleration– Protons at full energy in the LHC will be traveling at
0.999999991 times the speed of light. – Each proton will go round the 27 km ring more than 11,000 times
a second.– Entire acceleration process takes ~30min
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
July 25, 2008 Abigail Bickley, PAN 2008 12
Recipe for Creating an Ion Beam
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
4 Collision Tuning:– Beam is produced in “bunches” not a continuous stream of particles.– A filled ring contains 2808 bunches.– Each bunch contains 1.1x1011 protons– Arrival of bunches from both beams at the interaction region must be
timed perfectly to create collisions– 600M collisions per second
July 25, 2008 Abigail Bickley, PAN 2008 13
Power Consumption
• Annual operation requires 800,000 MWh• Equivalent to the entire state of Geneva• Machine only operates 270 days/year• Cooling of the superconducting magnets consumes the
majority of the power (9593 total magnets)• Electricity is provided by France
– 20% of French electricity is generated in nuclear power plants
July 25, 2008 Abigail Bickley, PAN 2008 14
CERN Price Tag
Annual energy cost: $30M
Construction Costs
Personnel Materials Total
Facility $890M $3550M $4,440M
Injector $87M $67M $154M
Computing $87M $87M $174M
Total $1,064M $3,704M $4,768M
July 25, 2008 Abigail Bickley, PAN 2008 15
Existing Colliders/AcceleratorsFacility Location Max
EnergySpecies Science
LHC France & Switzerland
7 TeV
2.76 TeV/u
Proton
Lead
Higgs, Super Symmetry, etc
RHIC Brookhaven, NY 200 GeV Proton, Gold Quark Gluon Plasma
Tevatron Batavia, Il 1 TeV (Anti)-Proton Top quark
CEBAF Newport News, VA 4 GeV
(12 GeV)
Electrons Nucleon sub-structure
RHIC from space
July 25, 2008 Abigail Bickley, PAN 2008 16
Why Collide Nuclei?
July 25, 2008 Abigail Bickley, PAN 2008 17
Evolution of the Universe
LHC equivalent to t = 10-25seconds.As time progressed the universe expanded and cooled.
Free quarks and gluons became confined.
July 25, 2008 Abigail Bickley, PAN 2008 18
The Particle Zoo• The nucleus of an atom is
composed of protons & neutrons
• But these particles also have a quark substructure– Proton = uud– Neutron = udd
• The antimatter equivalent to the proton is the antiproton (uud)
Proton
July 25, 2008 Abigail Bickley, PAN 2008 19
The Particle ZooQuark Charge Mass
Up +2/3 1.9 MeV
Down -1/3 4.4 MeV
Strange -1/3 87 MeV
Charm +2/3 1.32 GeV
Bottom (Beauty)
-1/3 4.24 GeV
Top
(Truth)
+2/3 172.7 GeV
July 25, 2008 Abigail Bickley, PAN 2008 20
Scientific Goals of LHC: Higgs Boson
• The Higgs boson is a hypothesised particle which, if it exists, would give the mechanism by which particles acquire mass.
• Referred to in the lay press as the “God particle”• Higgs proposed that the whole of space is permeated by a field, similar
in some ways to the electromagnetic field. • As particles move through space they travel through this field, and if
they interact with it they acquire what appears to be mass. • This is similar to the action of viscous forces felt by particles moving
through any thick liquid. the larger the interaction of the particles with the field, the more mass they appear to have.
• Force carrier of the Higgs field is the Higgs boson.
‘Well, either we've found the Higgs boson, or Fred's just put the kettle on’
http://www.oufusion.org.uk/newssummer01/fusionnewssummer01.htm
July 25, 2008 Abigail Bickley, PAN 2008 21
Scientific Goals of LHC• What is dark matter?
– Observations of visible matter accounts for only 4% of the Universe.
– The search is open for particles or phenomena responsible for dark matter (23%) and dark energy (73%).
– A very popular idea is that dark matter is made of neutral but still undiscovered supersymmetric particles.– The gravitational effect of dark matter may make galaxies spin faster than expected– The gravitational field of dark matter deviates the light of objects behind it.
July 25, 2008 Abigail Bickley, PAN 2008 22
Common Misconceptions
– Theoretical existence– Created in high energy collisions of particles such as the protons– Public concern is that the energy of the collisions at the LHC will be sufficient
to create microscopic black holes
• Scientific Rebuttal:– Cosmic rays are particles produced in outer space that are accelerated to
energies far exceeding those of the LHC. – Cosmic rays travel throughout the Universe, and have been bombarding the
Earth’s atmosphere continually since its formation 4.5 billion years ago. – Since the much higher-energy collisions provided by nature for billions of years
have not harmed the Earth, there is no reason to think that any phenomenon produced by the LHC will do so.
Massive Black Hole
• Public concern exists about the possibility of black hole creation at LHC
• Macroscopic Black Holes:– Massive black holes are formed in nature as a
result of star collapse– Results in a very large amount of matter being
confined to a very small volume
• Microscopic Black Holes:
July 25, 2008 Abigail Bickley, PAN 2008 23
Watching a Collision• Microscopic view
0 fm/c ~2 fm/c ~7 fm/c >7fm/c
Time ~6x10-24s ~21x10-24s >21x10-24s
Remember: E=mc2 so lots of energy means lots of mass!!!
July 25, 2008 Abigail Bickley, PAN 2008 24
Watching a Collision
July 25, 2008 Abigail Bickley, PAN 2008 25
The Detectors: CMS• Compact Muon
Solenoid
• Cylindrical detector– 69ft long– 52ft diameter– 25,000,000lbs
• Cost:– $480M
• Collaboration:– ~2600 people– 180 institutions– 38 countries
Scientific Goal:general‑purpose detector designed to cover the widestpossible range of physics, from the search for the Higgsboson to supersymmetry (SUSY) and extra dimensions
July 25, 2008 Abigail Bickley, PAN 2008 26
The Detectors: CMS• Compact Muon
Solenoid
• Cylindrical detector– 69ft long– 52ft diameter– 25,000,000lbs
• Cost:– $480M
• Collaboration:– ~2600 people– 180 institutions– 38 countries
Scientific Goal:general‑purpose detector designed to cover the widestpossible range of physics, from the search for the Higgsboson to supersymmetry (SUSY) and extra dimensions
July 25, 2008 Abigail Bickley, PAN 2008 27
The Detectors: ATLAS • No acronym
• Dimensions– 151ft long– 82ft diameter– 7,000,000lbs
• Cost:– $520M
• Collaboration:– 1900 people
– 164 institutions
– 35 countriesScientific Goal:general‑purpose detector designed to cover the widestpossible range of physics, from the search for the Higgsboson to supersymmetry (SUSY) and extra dimensions
July 25, 2008 Abigail Bickley, PAN 2008 28
The Detectors: ATLAS • No acronym
• Dimensions– 151ft long– 82ft diameter– 7,000,000lbs
• Cost:– $520M
• Collaboration:– 1900 people
– 164 institutions
– 35 countriesScientific Goal:general‑purpose detector designed to cover the widestpossible range of physics, from the search for the Higgsboson to supersymmetry (SUSY) and extra dimensions
July 25, 2008 Abigail Bickley, PAN 2008 29
The Detectors: ALICE• A Large Ion Collider
Experiment
• Cylindrical detector– 85ft long– 52ft diameter– 10,000,000lbs
• Cost:– $110M
• Collaboration:– 1500 people – 104 institutions– 31 countries
Scientific Goal:specialized in analysing lead-ion collisions. It will study the properties of quark-gluon plasma, a state of matter where quarks and gluons, under conditions of very high temperaturesand densities, are no longer confined inside hadrons. Such astate of matter probably existed just after the Big Bang, before Particles such as protons and neutrons were formed.
July 25, 2008 Abigail Bickley, PAN 2008 30
The Detectors: ALICE• A Large Ion Collider
Experiment
• Cylindrical detector– 85ft long– 52ft diameter– 10,000,000lbs
• Cost:– $110M
• Collaboration:– 1500 people – 104 institutions– 31 countries
Scientific Goal:specialized in analysing lead-ion collisions. It will study the properties of quark-gluon plasma, a state of matter where quarks and gluons, under conditions of very high temperaturesand densities, are no longer confined inside hadrons. Such astate of matter probably existed just after the Big Bang, before Particles such as protons and neutrons were formed.
July 25, 2008 Abigail Bickley, PAN 2008 31
The Detectors: ALICE• A Large Ion Collider
Experiment
• Cylindrical detector– 85ft long– 52ft diameter– 10,000,000lbs
• Cost:– $110M
• Collaboration:– 1500 people – 104 institutions– 31 countries
Scientific Goal:specialized in analysing lead-ion collisions. It will study the properties of quark-gluon plasma, a state of matter where quarks and gluons, under conditions of very high temperaturesand densities, are no longer confined inside hadrons. Such astate of matter probably existed just after the Big Bang, before Particles such as protons and neutrons were formed.
ALICE Virtual Tour
July 25, 2008 Abigail Bickley, PAN 2008 32
The Detectors: LHCb
Scientific Goal:specializes in the study of the slight asymmetry between matterand antimatter present in interactions of B-particles (particlescontaining the b quark). Understanding it should prove invaluablein answering the question: “Why is our Universe made of the matterwe observe?”
• Large Hadron Collider beauty
• Dimensions
– 69ft long
– 33ft high
– 43ft wide
– 5,600,000lbs
• Cost:
– $520M
• Collaboration:– 650 people – 47 institutions– 14 countries
July 25, 2008 Abigail Bickley, PAN 2008 33
The Detectors: LHCb
Scientific Goal:specializes in the study of the slight asymmetry between matterand antimatter present in interactions of B-particles (particlescontaining the b quark). Understanding it should prove invaluablein answering the question: “Why is our Universe made of the matterwe observe?”
• Large Hadron Collider beauty
• Dimensions
– 69ft long
– 33ft high
– 43ft wide
– 5,600,000lbs
• Cost:
– $520M
• Collaboration:– 650 people – 47 institutions– 14 countries
July 25, 2008 Abigail Bickley, PAN 2008 34
Data Rates and Volume• Raw Rate:
– 150M sensors record data at 40M/s
• Filtered Rate:– 100 collisions per sec
• Annual Data:– 15PB = 15,000,000GB– 100,000 DVDs per year
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
3miles
9.3miles
18.6miles12.4miles
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
July 25, 2008 Abigail Bickley, PAN 2008 35
The Grid
• Data access required for all collaborators• Geographically dispersed globally• The creation of a "virtual supercomputer" composed of a network of
loosely-coupled computers, acting in concert to perform very large tasks.
July 25, 2008 Abigail Bickley, PAN 2008 36http://www.symmetrymagazine.org/breaking/2008/04/14/what-can-we-expect-from-the-lhc/
Countdown….• June 16th, 2008: beam pipe completed• August 2008: beam injection into LHC• October 2008: beam circulation• December: first collisions???!!!
July 25, 2008 Abigail Bickley, PAN 2008 37
Stay Tuned….
July 25, 2008 Abigail Bickley, PAN 2008 38
Resources• LHC Homepage
– http://lhc.web.cern.ch/lhc/
• LHC Status & Schedule– http://www.lhcountdown.com/
• US LHC– http://www.uslhc.us/LHC_Science
• LHC Safety– http://public.web.cern.ch/Public/en/LHC/Safety-en.html
• CERN Web– http://public.web.cern.ch/Public/en/LHC/WhyLHC-en.html