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Modules and fusion for the one-dimensional vertex algebra
Example
Take , , , and conformal vector , with central charge zero. Its grading-restricted generalized modules are exactly finite-dimensional complex vector spaces with and weight zero. Use the trivial auxiliary groups throughout: , for every module , and all other components vanish. The category has all finite-dimensional complex vector spaces and all linear maps. For finite-dimensional , every logarithmic intertwining operator is constant in the variable and has the form for a unique bilinear map . Thus For every , the P(z)-tensor product is , with universal map ; the completion equals the module. Contragredients are the usual finite-dimensional duals, and all multipoint matrix coefficients are constant, so their convergence and continuation hold directly. This example uses no generic HLZ existence or convergence theorem.
Example references
Vertex algebra in the state–field convention
Module for an ordinary vertex algebra
Conformal vertex algebra of CFT type
Grading-restricted generalized module
Logarithmic intertwining operator
P(z)-tensor product in a module category
Contragredient module of a generalized module
C1-cofinite generalized module in the ungraded HLZ convention
Facts & Assumptions
Given: Finite-dimensional complex vector spaces, including the zero space, and the displayed scalar state-field map.
The vertex-algebra and module axioms are those of Vertex algebra in the state–field convention and Module for an ordinary vertex algebra. For the conformal grading and finite-dimensional generalized weight spaces use Conformal vertex algebra of CFT type and Grading-restricted generalized module.
The formal logarithmic series, Jacobi, derivative and Möbius-bracket conditions are those of Logarithmic intertwining operator.
The P(z)-map and representing property are those of P(z)-intertwining map and P(z)-tensor product in a module category.
Contragredient module of a generalized module, C1-cofinite generalized module in the ungraded HLZ convention and Quasi-finite-dimensional generalized module specify respectively the opposite-field restricted dual, the positive-weight (-1)-mode quotient and the finite weight-cutoff condition.
Verification
Only the st mode is nonzero. Truncation, creation and vacuum hold immediately, translation has both sides zero, and scalar fields commute, so locality holds with exponent zero. The zero conformal field has for every and satisfies Virasoro with ; , and all other graded pieces vanish. Thus has exactly the stipulated conformal structure.
On any module, linearity and vacuum force , hence and . Conversely this action satisfies Jacobi because each term is a scalar multiple of the basic formal identity This identity follows coefficientwise by expanding each integer power with the binomial convention. The only possible generalized eigenvalue of the zero is zero. Thus grading restriction is exactly finite-dimensionality of ; its real lower weight bound is zero. Every linear map between these spaces commutes with all fields.
Since , the derivative identity forces . Write each coefficient as with a finite polynomial. Its derivative is . For , its top coefficient forces ; for one has . Distinct exponents remain distinct after differentiation. The only remaining term is therefore a constant , bilinear in . Conversely any such has the required truncation, zero derivative and zero Möbius brackets. Its Jacobi identity is the scalar delta identity in step 2.1 multiplied by for the state . Thus the assignment is a linear bijection, and bases of show its dimension is the displayed product.
The completion of is , since it has only weight zero. With the specified trivial auxiliary grading, every linear map preserves auxiliary degree and its two input degrees add to zero. A P(z)-map is consequently just a linear map : weight compatibility is automatic and lower truncation is automatic outside that single weight. Its Jacobi identity reduces to multiplied by its value and the scalar state; this is the identity in step 2.1 with , with the prescribed formal expansions. All three brackets vanish. Every linear map is therefore admitted. Composition with the identity of gives precisely the required natural bijection of Hom spaces. This proves the P(z)-universal property directly for every .
Because , and its quotient has dimension . Each strict weight cutoff is either zero or , hence finite dimensional. The opposite transform fixes , so its transposed scalar field on is again scalar multiplication, and evaluation is a module isomorphism by finite-dimensional linear algebra. Every finite product or iterate of the operators from step 3.1 is an actual finite composition of bilinear maps, independent of all insertion variables. There is a single nonzero weight projection, so the projected series are finite. Matrix coefficients converge absolutely, extend as single-valued constant functions, and have a regular expansion with exponent zero and logarithmic degree zero at every boundary divisor.
The associator sends to , unit maps are scalar multiplication, and the braiding sends to . Their inverses are the reverse rebracketing, insertion of , and the reverse flip. They are linear module maps and natural because their formulas commute with arbitrary linear maps on the factors. Both routes through the associativity pentagon send to ; both triangle routes send to . In the first hexagon both routes send to , and in the second both send to . Pure tensors span, so these verify all coherence equations. Choosing a basis of with dual , evaluation and coevaluation have triangle composites and . These formulas also cover dimension zero by the empty sum. Hence this particular example has duality by direct verification.
Depends on
Vertex algebra in the state–field convention
Module for an ordinary vertex algebra
Conformal vertex algebra of CFT type
Grading-restricted generalized module
Logarithmic intertwining operator
P(z)-intertwining map
P(z)-tensor product in a module category
Contragredient module of a generalized module
C1-cofinite generalized module in the ungraded HLZ convention
Quasi-finite-dimensional generalized module