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Transcript of Why Supersymmetry is Super · PDF file4/15/09 Andrew Larkoski SASS 2 Outline • Introduce...
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4/15/09 Andrew Larkoski SASS 1
Why Supersymmetry is SuperAndrew Larkoski
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4/15/09 Andrew Larkoski SASS 2
Outline
• Introduce Quantum Field Theory
• Incorporating Supersymmetry in a Quantum Field Theory
• The MSSM
• Motivations for Supersymmetry in the “Real World”
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4/15/09 Andrew Larkoski SASS 3
Definition of a Quantum Field Theory
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4/15/09 Andrew Larkoski SASS 4
• Not Lorentz invariant• Unequal number of time and space derivatives• Explicit mass in denominator• Potential usually depends explicitly on position
Quantum Mechanics and Relativity
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4/15/09 Andrew Larkoski SASS 5
Quantum Mechanics and Relativity
• Different approach: Make a relativistic theory quantum mechanical!
• A Classical Field Theory is Lorentz invariant• How to make it quantum mechanical:
• Promote classical fields to operators!
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4/15/09 Andrew Larkoski SASS 6
Quantum Mechanics and Relativity
• Moral:
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4/15/09 Andrew Larkoski SASS 7
Quantum Field Theory
• Spin defines transformations under rotations and boosts• Quantum Field Theory naturally explains spin
• Not added ad hoc as in non-relativistic qm
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4/15/09 Andrew Larkoski SASS 8
Kinetic energy Shear energy Mass energy
Potential Energy
Example: Scalar (spin 0) theory
Euler-Lagrange Equation:
Quantum Mechanical identification:
Einstein’s relation:
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4/15/09 Andrew Larkoski SASS 9
Example: Fermion (spin 1/2) theory
Aligns spins MassDisplaces fermionsSpins anti-aligned
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4/15/09 Andrew Larkoski SASS 10
Supersymmetry
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4/15/09 Andrew Larkoski SASS 11
Familiar Quantum Operators
• Example: Momentum
• Momentum is a vector (a boson)• Momentum is Hermitian• Momentum satisfies commutation relations
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4/15/09 Andrew Larkoski SASS 12
Unfamiliar Quantum Operators
• Q is a fermion! (spin 1/2)• Q is not Hermitian!
• Eigenstates of Q do not have well-defined spin
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4/15/09 Andrew Larkoski SASS 13
Unfamiliar Quantum Operators
• Q satisfies anti-commutation relations:
• Look familiar?
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4/15/09 Andrew Larkoski SASS 14
Unfamiliar Quantum Operators
• Spin 1/2 or two-state raising and lowering operators!
• Rescale Q:
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4/15/09 Andrew Larkoski SASS 15
Summary
• Q satisfies the algebra:
• Q interpolates between two states:
• Q called the supercharge• f and b are superpartners and form a supermultiplet
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4/15/09 Andrew Larkoski SASS 16
Simplest Supersymmetric Model
• Massless, noninteracting Wess-Zumino model:
• is a complex scalar field:
• is a spin 1/2 fermion field:
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4/15/09 Andrew Larkoski SASS 17
Wess-Zumino Model
• Transformations of fields under supersymmetry:
• Leave the Wess-Zumino Lagrangian invariant:
• Wess-Zumino Lagrangian is supersymmetric!
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4/15/09 Andrew Larkoski SASS 18
What does Supersymmetry mean?
• Consider two electrons; one at rest, one with velocity v:
vee
• Lorentz transformations can change velocities• Doesn’t change laws of physics• Consequence: velocity is not a quantum number
• Consider a fermion and boson:
f b
• Supersymmetry doesn’t change laws of physics• Does change spin!• Consequence: spin is not a quantum number!
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4/15/09 Andrew Larkoski SASS 19
What does Supersymmetry mean? Summary
• Maps boson degrees of freedom to fermion degrees of freedom:
• Theory must have equal numbers of fermion and boson d.o.f.s• Boson and fermion superpartners must have same interactions
• Same mass, same charges• Moral:
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4/15/09 Andrew Larkoski SASS 20
The Minimal Supersymmetric Standard Model
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4/15/09 Andrew Larkoski SASS 21
• “Minimal Supersymmetric”: The absolute minimumnumber of additional particles to make the Standard Modelsupersymmetric
• Can particles in the Standard Model be superpartners?
Minimal Supersymmetric Standard Model
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4/15/09 Andrew Larkoski SASS 22
• “Minimal Supersymmetric”: The absolute minimumnumber of additional particles to make the Standard Modelsupersymmetric
• Can particles in the Standard Model be superpartners?
• No! No particles have same charges or mass andspin differing by 1/2
• Need to double particle content!
Minimal Supersymmetric Standard Model
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4/15/09 Andrew Larkoski SASS 23
• Superpartners in the MSSM:
• Scalar partner to a fermion = sfermion
• Partner to electron = selectron
• Partner to top quark = stop
• Fermion partner to a boson = bosino
• Partner to photon = photino
• Partner to gluon = gluino
• I make no apology for the nomenclature; it is terribly silly
Minimal Supersymmetric Standard Model
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4/15/09 Andrew Larkoski SASS 24
• A (major) problem
• Supersymmetry demands superpartners have same mass
• We don’t observe a negatively charged, scalar withmass of 511 keV (the selectron)
• Supersymmetry cannot be an exact symmetry of ourworld!
• Sparticle masses must be > 100 GeV to escape detection
• Many models predict masses in LHC range
• Very exciting! (pending LHC problems)
Minimal Supersymmetric Standard Model
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4/15/09 Andrew Larkoski SASS 25
Motivations for Supersymmetry in the Real World
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4/15/09 Andrew Larkoski SASS 26
Unification of Coupling Constants
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4/15/09 Andrew Larkoski SASS 27
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4/15/09 Andrew Larkoski SASS 28
Unification of Electricity and Magnetism
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4/15/09 Andrew Larkoski SASS 29
Unification of Electricity and Magnetism
• Maxwell’s equations unify E and B fields• Relates electric and magnetic couplings:
• Conversely, if couplings can be related, fields can be unified!• (At least a very strong indication of unification)
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4/15/09 Andrew Larkoski SASS 30
Unification in the Standard Model
• Three forces in Standard Model• Electromagnetism• Weak• Strong
• Three couplings in Standard Model relating strengths of forces• If these couplings can be related, forces could be unified!
• Could “explain” forces and their strengths
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4/15/09 Andrew Larkoski SASS 31
Unification in the Standard Model
• How to relate them?• Couplings depend on distance (energy)!• An electron polarizes the region of space around it• Dipoles screen bare electron charge• Closer to electron, charge looks larger!
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4/15/09 Andrew Larkoski SASS 32
Unification in the Standard Model
• Standard Model: dashed• No unification
• Standard Model + Supersymmetry: solid• Unification!
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4/15/09 Andrew Larkoski SASS 33
Hierarchy Problem
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4/15/09 Andrew Larkoski SASS 34
A Problem with Fundamental Scalars
• Or, why a massless fermion stays massless
• Recall massless fermion Lagrangian:
fv = c
spinf
v = c
spin
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4/15/09 Andrew Larkoski SASS 35
A Problem with Fundamental Scalars
• Mass term requires anti-aligned spins:
• Quantum Mechanics respects Lorentz invariance• Velocity and spin are locked in place• Such a term can never be generated!• Massless fermion stays massless!
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4/15/09 Andrew Larkoski SASS 36
A Problem with Fundamental Scalars
• Consider a massless, fundamental scalar:
• Scalar has no intrinsic direction or vector• Mass term of Lagrangian is not disallowed by any symmetries:
• Anything that is not forbidden will happen in QM• Mass term is generated quantum mechanically!
s v = c s v = c
• (Composite scalars do not suffer this problem as they aremade of fermions and inherit chiral symmetry)
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4/15/09 Andrew Larkoski SASS 37
Standard Model Higgs Scalar Boson
• In the Standard Model, Higgs boson is responsible for mass• All particles have mass proportional to Higgs mass
• How does quantum mechanics affect Higgs mass?• Interactions with bosons: increases mass• Interactions with fermions: decreases mass
• In Standard Model, these contributions are unrelated• Quantum mechanic shifts can be (essentially) unbounded!• Obviously a bad thing
• Requiring supersymmetry:• Fermions and bosons have same interactions with Higgs• Contributions to Higgs mass exactly cancel!• A good thing
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4/15/09 Andrew Larkoski SASS 38
Standard Model Higgs mass
• Resolves the hierarchy problem:Supersymmetry resolves the hierarchy problem by demanding that fermion and boson contributions tothe higgs mass exactly cancel.
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4/15/09 Andrew Larkoski SASS 39
Things I Didn’t Discuss
• Other solutions to the Hierarchy problem:
• Extra Dimensions
• Randall-Sundrum Models, etc.
• Composite Higgs models
• Technicolor, etc.
• None, there is no Hierarchy problem
• Split Supersymmetry, etc.
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4/15/09 Andrew Larkoski SASS 40
• Other connections of Supersymmetry• Adding more supersymmetries
• Have only considered N = 1• Can add more supercharges to consider largersupermultiplets• Conformal theories; AdS/CFT
• Gravity + Supersymmetry = Supergravity• Could be a way to control the divergences thattrouble a quantum theory of gravity
• String Theory• Requires supersymmetry• Currently the best quantum theory of gravity
Things I Didn’t Discuss
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4/15/09 Andrew Larkoski SASS 41
An Explanation of Dark Matter
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4/15/09 Andrew Larkoski SASS 42
An Explanation of Dark Matter
• I won’t motivate the existence of dark matter here
• Necessary to explain the rotation curves of galaxies
• Necessary to explain the distribution of mass and thegravitational potential well in the Bullet Cluster
• There are many reasons that Standard Model particlescould not be dark matter
• Dark matter is dark, must be neutral and stable
• Could possibly be neutrinos but are much to light toremain contained in galaxies
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4/15/09 Andrew Larkoski SASS 43
An Explanation of Dark Matter
• Supersymmetry “naturally” includes heavy, neutralWeakly interacting particles!
• Called WIMPs
• Constraints on cosmological parameters demand itsmass be in the 100 GeV-1 TeV range