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Irreducible extremal cyclic Virasoro modules in boundary Fock spaces
Statement
Use the oscillator spaces, modes and screening coefficients of the rank-one oscillator data. Fix integers and , and set Then the actual cyclic Virasoro modules generated by the indicated Fock vacua satisfy Their -characters are respectively Here is the unique simple highest-weight quotient of the ordinary Verma module. These are full algebraic modules at all grades; no truncation is asserted.
Statement references
Rank-one Feigin–Fuchs oscillator spaces and long-screening coefficients
Background-charge oscillator modes and integral long screenings
Reflected oscillator pairing and transpose of the long screening
Exact lengths of boundary long-screening strings
Single-chain maximal submodules at boundary Virasoro central charges
Facts & Assumptions
Given: The parameters, oscillator spaces, modes and actual cyclic modules in the Statement.
Rank-one Feigin–Fuchs oscillator spaces and long-screening coefficients gives the polynomial charge spaces. Their degree- monomial basis has the partition dimension .
Background-charge oscillator modes and integral long screenings proves the actual Virasoro action, vacuum highest weights and integral-charge screening commutation for every integer used here.
Reflected oscillator pairing and transpose of the long screening proves the degreewise nondegenerate pairing at reflected charge , with and the exact screening transpose.
Exact lengths of boundary long-screening strings proves the exact nonzero maximal powers and and their next-power vanishing.
Single-chain maximal submodules at boundary Virasoro central charges identifies the first embedded Verma as the maximal proper submodule. For its first grade is and highest weight ; for they are and .
PBW basis and grades of Virasoro Verma modules gives the partition dimension and negative PBW word basis at every Verma grade.
Proof
Here a singular vector means a nonzero -eigenvector annihilated by every with . This is exactly the highest-weight-vector condition stated in [F2].
The oscillator monomials , where is finitely supported, have degree and are indexed by partitions of , so . Substitution in the current vacuum-weight formula [F2] gives and . The charges are integral for the screening hypotheses: and are integers. Thus each composition used in [F4] is defined under [F2].
Fix , let , so , and set . By [F4] this vector is nonzero in ; by [F2] it is singular. Screening commutation preserves its weight, which is , while the target vacuum in has weight . Its relative oscillator level is
The highest-vector property defines a Verma map sending its top to ; its image is the stated cyclic module. For a level- PBW word , the adjoint identity in [F3] gives , because is a nonempty product of positive modes and each positive mode kills the singular vector . Nondegeneracy of the pairing makes a nonzero functional on , so the level- image is proper. Its domain and target both have dimension by [F1] and [F6]; hence has a nonzero vector at level .
The kernel of is a proper graded submodule because its highest vector maps to a nonzero vacuum. By [F5], it lies in the maximal proper submodule of , whose first nonzero level is and whose grade- space is one-dimensional. Step 3.1 then implies contains that first singular vector; since this vector generates , while , equality follows. Thus the actual cyclic image is , with the first character in the Statement by [F5].
For , put , so . The vector is nonzero by [F4], singular by [F2], and has weight ; the target vacuum weight is , so its positive relative level is . The same adjoint calculation as in step 3.1 makes the level- Verma-map image proper. Equal level dimensions [F1, F6] give a nonzero kernel vector there. By [F5], the kernel is contained in the first maximal submodule, meets its one-dimensional first grade, and therefore equals it. This proves the second cyclic irreducibility and character formula.
Depends on
Rank-one Feigin–Fuchs oscillator spaces and long-screening coefficients
Background-charge oscillator modes and integral long screenings
Reflected oscillator pairing and transpose of the long screening
Exact lengths of boundary long-screening strings
Single-chain maximal submodules at boundary Virasoro central charges
PBW basis and grades of Virasoro Verma modules