Introduction to Supersymmetry and Supergravity
Simon Albino II. Institute for Theoretical Physics at DESY, University of Hamburg [email protected]
Every Wednesday and Thursday 8:30-10:00am, starting 3rd November, in room 2, building 2a, DESY
Lecture notes at www.desy.de/~simon/teaching/susy.html
Abstract
These lectures give a fairly formal developement of supersymmetry, beginning with some technical footing in symmetries (internal and external) in general in relativistic quantum mechanics, and a brief outline of the standard model and its GUT extensions. Following the Haag-Lopuszanski-Sohnius theorem, we allow for fermionic symmetry generators, and determine their properties and algebra using the restrictions of the Coleman-Mandula theorem. As an illustration we construct the supersymmetric field theory Lagrangian for the chiral supermultiplet, then discuss the more formal approach to constructing general supersymmetric field theories using superfields in superspace, including the development of supersymmetric gauge theories. Spontaneous supersymmetry breaking is discussed in some detail. Using the superfield formalism, the minimally supersymmetric standard model is developed. Next we develop supergravity, firstly in the weak field case and then to all orders. Finally, the more advanced topics of higher dimensions, extended supersymmetry and duality are discussed. The lectures will mostly follow Volume III of S. Weinberg’s “The Quantum Theory of Fields”. IMPORTANT
Lecture notes are at www.desy.de/~simon/teaching/susy.html. They will change! • If you get stuck, please email me at [email protected] • If you find a mistake, please email me at [email protected] • Please let me know by email that you will attend this course so I can put you on the mailing list • (and thus notify you at the last minute of room changes, cancellations, help with problems etc.). Every second Thursday I will try to allocate time for you to ask more detailed questions, • for you to work through and present derivations outlined in the lectures, and (if time) for you to present solutions to interesting problems. There is alot of algebra to deal with in SUSY... • so please think about the ratio of algebraic explanations to material that you would like! My suggestion: Try to derive some results in detail at home, and present your derivations every second Thursday. • I am setting up an online forum where you can ask / answer SUSY questions. • Usually in the lecture notes, I give the result first and then outline the derivation in smaller font below. • I use the Einstein summation convention, i.e. and e.g. 3 X Xµ X Xµ (and not just for spacetime indices). • i=0 µ → µ Any questions? P • Contents
1 Quantum mechanics of particles 2
1.1 Basic principles ...... 2
1.2 Fermionic and bosonic particles ...... 4
2 Symmetries in QM 6
2.1 Unitary operators ...... 6
2.2 (Matrix) Representations ...... 10
2.3 External symmetries ...... 16
2.3.1 Rotation group representations ...... 16
2.3.2 Poincar´eand Lorentz groups ...... 20
2.3.3 Relativistic quantum mechanical particles ...... 22
2.3.4 Quantum field theory ...... 25
2.3.5 Causal field theory ...... 27
2.3.6 Antiparticles ...... 28 2.3.7 Spin in relativistic quantum mechanics ...... 29
2.3.8 Irreducible representation for fields ...... 31
2.3.9 Massive particles ...... 32
2.3.10 Massless particles ...... 33
2.3.11 Spin-statistics connection ...... 35
2.4 External symmetries: fermions ...... 37
1 2.4.1 Spin 2 fields ...... 37
1 2.4.2 Spin 2 in general representations ...... 44
2.4.3 The Dirac field ...... 49
2.4.4 The Dirac equation ...... 51
2.4.5 Dirac field equal time anticommutation relations ...... 52
2.5 External symmetries: bosons ...... 53
2.6 The Lagrangian Formalism ...... 57
2.6.1 Generic quantum mechanics ...... 57
2.6.2 Relativistic quantum mechanics ...... 58 2.7 Path-Integral Methods ...... 61
2.8 Internal symmetries ...... 62
2.8.1 Abelian gauge invariance ...... 64
2.8.2 Non-Abelian gauge invariance ...... 66
2.9 The Standard Model ...... 68
2.9.1 Higgs mechanism ...... 70
2.9.2 Some remaining features ...... 74
2.9.3 Grand unification ...... 76
2.9.4 Anomalies ...... 78
3 Supersymmetry: development 79
3.1 Why SUSY? ...... 79
3.2 Haag-Lopuszanski-Sohnius theorem and SUSY algebra ...... 83
3.3 Supermultiplets ...... 90
3.3.1 Field supermultiplets (the left-chiral supermultiplet) ...... 95
3.4 Grassman variables ...... 100 3.5 Superfields and Superspace ...... 101
3.5.1 Chiral superfield ...... 106
3.5.2 Supersymmetric Actions ...... 111
3.6 Superspace integration ...... 116
3.7 Supergraphs ...... 117
3.8 SUSY current ...... 124
3.9 Spontaneous supersymmetry breaking ...... 128
3.9.1 O’Raifeartaigh Models ...... 129
3.10 Supersymmetric gauge theories ...... 130
3.10.1 Gauge-invariant Lagrangians ...... 135
3.10.2 Spontaneous supersymmetry breaking in gauge theories ...... 139
4 The Minimally Supersymmetric Standard Model 143
4.1 Left-chiral superfields ...... 143
4.2 Supersymmetry and strong-electroweak unification ...... 147
4.3 Supersymmetry breaking in the MSSM ...... 149 4.4 Electroweak symmetry breaking in the MSSM ...... 157
4.5 Sparticle mass eigenstates ...... 162
5 Supergravity 164
5.1 Spinors in curved spacetime ...... 164
5.2 Weak field supergravity ...... 168
5.3 Supergravity to all orders ...... 176
5.4 Anomaly-mediated SUSY breaking ...... 183
5.5 Gravity-mediated SUSY breaking ...... 184
6 Higher dimensions 187
6.1 Spinors in higher dimensions ...... 187
6.2 Algebra ...... 190
6.3 Massless multiplets ...... 194
6.4 p-branes ...... 197 7 Extended SUSY 198 [email protected] 2 1 Quantum mechanics of particles
1.1 Basic principles
Physical states represented by directions of vectors (rays) i in Hilbert space of universe. | i
Write conjugate transpose i † as i , scalar product j † i as j i . | i h | | i · | i h | i
Physical observable represented by Hermitian operator A = A† such that A = i A i . h ii h | | i Functions of observables represented by same functions of their operators, f(A).
Errors i A2 i A 2 etc. vanish when i = a , h | | i−h ii | i | i where A a = a a , i.e. a is A eigenstate, real eigenvalue a. a form complete basis. | i | i | i | i If 2 observables A, B do not commute, [A, B] = 0, eigenstates of A do not coincide with those of B. 6 If basis X(a, b) are A, B eigenstates, any i = C X obeys [A, B] i = 0 = [A, B]=0. | i | i X iX| i | i ⇒ P If A, B commute, their eigenstates coincide.
AB a = BA a = aB a , so B a a . | i | i | i | i∝| i [email protected] 3 Completeness relation: a a = 1 . a | ih | P Expand i = W a then act from left with a′ W ′ = a′ i , so i = a a i | i a ia| i h | −→ ia h | i | i a | ih | i P P 2 Probability to observe system in eigenstate a of A to be in eigenstate b of B: Pa b = b a . | i | i → |h | i| Iα Pa b are the only physically meaningful quantities, thus i and e i for any α represent same state. → | i | i
a Pb a = 1 for some state b as expected. b = a a b a . Act from left with b gives 1 = a a b b a . → | i | i h | i| i h | h | ih | i P P P Principle of reversibility: Pa b = Pb a. b a = a b ∗ → → h | i h | i
IHt Time dependence: Time evolution of states: i, t = e− i , H is Hamiltonian with energy eigenstates. | i | i 2 IHt Probability system in state i observed in state j time t later = Mi j , transition amplitude Mi j = j e− i . | i | i | → | → h | | i IHt IHt Average value of observable Q evolves in time as Q (t)= i e Qe− i . h ii h | | i Q is conserved [Q, H]=0 ( Q (t) independent of t). ⇐⇒ h i [email protected] 4 1.2 Fermionic and bosonic particles
Particle’s eigenvalues = σ. Particle states σ, σ′, ... completely span Hilbert space. Vacuum is 0 = . | i | i |i
σ, σ′, ... = σ′, σ, ... for bosons/fermions. Pauli exclusion principle: σ, σ, σ′... =0 if σ fermionic. | i ±| i | i
Iα 2Iα Iα σ, σ′,... and σ′,σ,... are same state, σ, σ′,... = e σ′,σ,... = e σ, σ′,... = e = 1. | i | i | i | i | i ⇒ ±
Creation/annihilation operators: aσ† σ′,σ′′, ... = σ, σ′,σ′′, ... , so σ, σ′, ... = aσ† a† . . . 0 . | i | i | i σ′ | i
[aσ† , a† ] =[aσ, aσ ] = 0 (bosons/fermions). σ′ ∓ ′ ∓
σ, σ′,... = a† a† ′ ... = σ′,σ,... = a† ′ a† ... | i σ σ | i ±| i ± σ σ| i a removes σ particle = a 0 =0. σ ⇒ σ| i
E.g. (a σ′, σ′′ )† σ′′′ = σ′, σ′′ (a† σ′′′ ) = 0 unless σ = σ′, σ′′′ = σ′′ or σ = σ′′, σ′′′ = σ′. i.e. a σ′, σ′′ = δ ′′ σ′ δ ′ σ′′ . σ| i ·| i h | σ| i σ| i σσ | i± σσ | i
[aσ, a† ] = δσσ . σ′ ∓ ′
e.g. 2 fermions a† ′′ a† ′′′ 0 : Operator a† a ′ replaces any σ′ with σ, must still vanish when σ′′ = σ′′′. σ σ | i σ σ
Check: (a† a ′ )a† ′′ a† ′′′ 0 = a† a† ′′ a ′ a† ′′′ 0 + δ ′ ′′ a† a† ′′′ 0 = δ ′ ′′′ a† a† ′′ 0 + δ ′ ′′ a† a† ′′′ 0 . σ σ σ σ | i − σ σ σ σ | i σ σ σ σ | i − σ σ σ σ | i σ σ σ σ | i [email protected] 5 ∞ ∞ † † Expansion of observables: Q = N=0 M=0 CNM;σ ...σ ;σ ...σ1 a ...a aσM ...aσ1. 1′ N′ M σ1′ σN′ P P Can always tune the CNM to give any values for 0 aσ′ ...aσ′ Qa† ...a† 0 . h | 1 L σ1 σK | i
Commutations with additive observables: [Q, aσ† ]= q(σ)aσ† (no sum) , where Q is an observable such that for σ, σ′,... , total Q = q(σ)+ q(σ′)+ . . . and Q 0 = 0 (e.g. energy). | i | i
Check for each particle state: Qa† 0 = q(σ)a† 0 + a† Q 0 = q(σ)a† 0 , σ| i σ| i σ | i σ| i
Qa† a† ′ 0 = a† Qa† ′ 0 + q(σ)a† a† ′ 0 = a† a† ′ Q 0 + q(σ′)a† a† ′ 0 + q(σ)a† a† ′ 0 = (q(σ) + q(σ′))a† a† ′ 0 etc. σ σ | i σ σ | i σ σ | i σ σ | i σ σ | i σ σ | i σ σ | i Note: Conjugate transpose is [Q, a ]= q(σ)a . σ − σ
Number operator for particles with eigenvalues σ is a† aσ (no sum). E.g. (a† aσ)a† a† a† ′ 0 = 2a† a† a† ′ 0 . σ σ σ σ σ | i σ σ σ | i
Additive observable: Q = σ q(σ)aσ† aσ . E.g. Q = H, (free) Hamiltonian, q(σ) = Eσ, energy eigenvalues. P [email protected] 6 2 Symmetries in QM
2.1 Unitary operators
Symmetry is powerful tool: e.g. relates different processes.
Symmetry transformation is change in our point of view (e.g. spatial rotation / translation), does not change experimental results. i.e. all i U i does not change any j i 2. | i −→ | i |h | i| Continuous symmetry groups G require U unitary:
j i j U †U i = j i , so U †U = UU † = 1 , includes U = 1. h | i→h | | i h | i Wigner + Weinberg: General physical symmetry groups require U unitary,
or antiunitary: j i j U †U i = j i ∗ = i j , e.g. (discrete) time reversal. h | i→h | | i h | i h | i
A unaffected (and f(A) in general), so must have A UAU † . h i h i →
IHt IHt Transition amplitude Mi j unaffected by symmetry transformation, i.e. j U †e− U i = j e− i , → h | | i h | | i which requires [U, H] = 0 if time translation and symmetry transformation commute. [email protected] 7 Parameterize unitary operators as U = U(α), αi real, i = 1, ..., d(G). d(G) is dimension of G, minimum no. of paramenters required to distinguish elements.
Choose group identity at α = 0, i.e. U(0) = 1.
So for small α , can write U(α) 1 + It α . i ≈ i i ti are the linearly independent generators of G. Since U †U = 1, ti = ti†, i.e. ti are Hermitian .
[U, H]=0 = [t ,H] = 0, so conserved observables are generators. ⇒ i 1 Can replace all t t′ = M t if M invertible and real, because then α′ = α M − real. i → i ij j i j ji
In general, U(α)U(β)= U(γ(α, β)) (up to possible phase eIρ, removable by enlarging group). [email protected] 8 U(α) = exp [It α ] if Abelian limit is obeyed: whenever β α , U(α)U(β)= U(α + β) i i i ∝ i (usually true for physical symmetries, e.g. rotation about same line / translation in same direction).
Can write U(α)=[U(α/N)]N , then for N is [1 + It α /N + O(1/N 2)]N = exp[It α ] + O 1 . → ∞ i i i i N
Lie algebra: [ti, tj]= ICijktk , where Cijk are the structure constants
1 appearing in U(α)U(β)= U(α + β + 2ICαβ + cubic and higher)
2 2 (where (Cαβ)k = Cijkαiβj, and no O(α ) ensures U(α)U(0) = U(α), likewise no O(β )).
LHS: eIαteIβt 1 + Iαt 1(αt)2 1 + Iβt 1(βt)2 ≈ − 2 × − 2 1 + I(αt + βt) 1 (αt)2 + (βt)2 + 2(αt)(βt) ≈ − 2 h i I(α+β+ 1 ICαβ)t 1 1 1 2 RHS: e 2 1 + I(α + β + ICαβ)t (α + β + ICαβ)t ≈ 2 − 2 2 1 + I(αt + βt + 1ICαβt) 1 (αt)2 + (βt)2 + (αt)(βt) + (βt)(αt) , ≈ 2 − 2 h i 1 1 i.e. 2ICijkαiβjtk = 2 [αiti, βjtj].
Now take all α , β zero except e.g. α = β = ǫ IC t =[t ,t ] etc., gives Lie algebra. i j 1 2 → 12k k 1 2 [email protected] 9 In fact, Lie algebra completely specifies group in non-small neighbourhood of identity.
This means that for U(α)U(β)= U(γ), γ = γ(α, β) can be found from Lie algebra.
We have shown this above in small neighbourhood of identity, i.e. to 2nd order in α, β, only.
Check to 3rd order: Write X = αiti, Y = βiti, can verify Baker-Hausdorff formula 1 I exp[IX] exp[IY ] = exp[I(X + Y ) [X,Y ]+ ([X, [Y, X]]+[Y, [X,Y ]]) + quadratic and higher]. − 2 12 has the form Iγiti, γi real | {z }
Lie algebra implies: 1. C = C (antisymmetric in i, j). Cijk can be chosen antisymmetric in i,j,k (see later). ijk − jik
2. Cijk real.
Conjugate of Lie Algebra is t†,t† = IC∗ t† , which is negative of Lie Algebra because t† = t . j i − ijk k i i h i
Thus Cijk∗ tk = Cijktk, but tk linearly independent so Cijk∗ = Cijk.
2 Iα t 2 Iα t 2 3. t = tjtj is invariant (commutes with all ti, so transforming gives e i it e− k k = t ).
[t2,t ] = t [t ,t ]+[t ,t ]t = IC t ,t = 0 by (anti)symmetry in (j, i) j,k. i j j i j i j jik{ j k}
Examples: Rest mass, total angular momentum. tjtj doesn’t have to include all j, only subgroup. [email protected] 10 2.2 (Matrix) Representations
Physically, matrix representation of any symmetry group G of nature formed by particles:
( ) General transformation of aσ† : U(α)aσ† U †(α)= Dσσ (α)a† , with invariant vacuum: U(α) 0 = 0 . ′ σ′ | i | i
U(α)a† 0 is 1 particle state, so must be linear combination of a† ′ 0 , i.e. U(α)a† 0 = D ′ (α)a† ′ 0 . σ| i σ | i σ| i σσ σ | i
Thus U(α)a† a† ′ 0 = D ′′ (α)D ′ ′′′ (α)a† ′′ a† ′′′ 0 etc. σ σ | i σσ σ σ σ σ | i i D(α) matrices furnish a representation of G , matrix generators (t )σ′σ with same Lie algebra [ti, tj]σσ′ = ICijk(tk)σσ′.
Since U(α)U(β) = U(γ), must have Dσ′′σ′ (α)Dσ′σ(β) = Dσ′′σ(γ).
Iαiti If Abelian limit of page 8 is obeyed, Dσ σ(α)= e . ′ σ′σ