Fundamental structures of 2d CFT
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The Virasoro algebra and its representations
See Sections 1.1.1 to 1.1.4 of Ref.[1]
Course questions
- Does the Virasoro algebra's central term affect global conformal transformations?
- Given two CFTs, each one with its own Virasoro algebra, what is the Virasoro algebra for the product CFT? What is its central charge?
- Write a basis of a Verma module's level 5.
- From its explicit expression, check that a level-3 null vector is annihilated by and . Is it necessary to check it for as well?
- In the case find the levels of all the null vectors in the Verma module with dimension . How many degenerate quotients does this Verma module have?
Exercises
- Eigenvalues of differ by integers in indecomposable representations of the Virasoro algebra: see Exercise 1.7 of Ref.[2]
- Decomposing Virasoro representations into representations: see Exercise 1.8 of Ref.[2]
- The existence of a Hermitian form on the space of states is a necessary condition for unitarity, and occurs also in many non-unitary CFTs. Show that if there is a Hermitian form that is compatible with the Virasoro algebra and is such that is self-conjugate, then the central charge is real. For a more precise statement of the problem and a few hints, see Exercise 1.9 of Ref.[2]
- Alternative spanning set of a Verma module: see Exercise 2.2 of Ref.[2]
Fields and operator product expansions
See Sections 1.2.1 to 1.2.3 of Ref.[1]
Course questions
- For a primary field, write the OPE of the energy-momentum tensor with , and compare with the OPE of with itself.
- Is related to ? To ?
- Assuming the coefficients are known, compute the first few orders of the OPEs and .
FOGO: Global vs local conformal symmetry in OPEs
In a CFT with local conformal symmetry, we recall that the contribution of and its descendants in an OPE of 2 primary fields reads
where is a basis of Virasoro creation operators.
- What would be the analogous formula in a CFT with only global conformal symmetry? Show that its universal coefficients are parametrized by integers , and write these coefficients as .
- Compute the coefficients and , and compare them with .
- In order to explain why , find how the coefficients behave under a change of basis . Which value leads to ?
- Show that is a global primary field.
Other exercises
- Virasoro algebra and OPE: see Exercise 2.11 of Ref.[2]
Fusion rules and minimal models
See Sections 1.2.4, 1.2.5, 2.2.1 and 2.2.3 of Ref.[1]
Course questions
- Write the fusion products of the degenerate representation with a Verma module or with another degenerate representation. In which cases are there fewer than 6 terms?
- At generic central charge, find all subrings of the fusion ring of degenerate representations. Are there any finite-dimensional subrings?
- What is the smallest Kac table that is not displayed in the article w:minimal model (physics)?
Exercises
- Structure of fully degenerate representations: see Exercise 2.5 of Ref.[2]
- Characters of Virasoro representations: see Exercise 2.6 of Ref.[2]
- Unitarity and negative conformal dimensions in minimal models: see Exercise 3.11 of Ref.[2]
- In which minimal models do fusion rules have a symmetry like in the Ising case?
- Write the fusion rules of the minimal model AMM.
Correlation functions and conformal blocks
See Section 1.3 of Ref.[1]
Course questions
- Assuming we know , compute .
- Write the generators of the conformal algebra , in terms of Virasoro generators .
- Assuming for some primary fields , what can we say on the conformal spin of ?
Exercises
- Behaviour of the energy-momentum tensor at infinity: see Exercise 2.10 of Ref.[2]
- Creation operators as differential operators: see Exercise 2.13 of Ref.[2]
- Logarithmic correlation functions: see Exercise 2.15 of Ref.[2]
- Permutations and 4-point functions: see Exercise 2.16 of Ref.[2]