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Tail estimates: q-adic vanishing against the vacuum and finiteness of the weight strings
Statement
Let be the charge- Fock space with ground sequence and let be the opposite-channel energy. Then:
(i) Vanishing against the right tail. For a fixed type-A ground sequence, the condition means that the added integer index lies inside or below the filled right tail ; then , a sufficiently long finite prefix of this entire filled-tail wedge is already , and hence the element lies in for every .
(ii) Dual left tail. The mirrored condition with the left tail gives the same exact finite vanishing, with the roles of left and right exchanged.
(iii) Endomorphisms commuting with the loop. A nonzero-weight endomorphism of commuting with has only finitely many loop-shift/color terms on each fundamental vector; inserting deep inside a ground tail is eventually , so it converges -adically to on every vector.
(iv) The period operator. For the explicit period operator on that prepends vacuum entries and shifts every old index down by : preserves each label-weight/size component, and on the positive-size- part its -th power is as soon as . Consequently is a finite geometric sum on every nonvacuum weight, and each label weight has only finitely many partition vectors.
Facts & Assumptions
Given: The charge- Fock space, its normal partition basis, the ground sequence, and the energy with the criterion .
Finite normal words have strictly decreasing indices. Straightening preserves cardinality, total index sum and residue multiset, and keeps all indices between the input extremes. Hence an -factor word supported in an interval of fewer than integers is zero. In an interval of exactly integers there is only one possible normal -tuple, whose sum is the sum of the entire interval (Normally ordered q-wedges form a basis for every finite wedge length, The semi-infinite q-wedge Fock space and its q-adic topology).
iff . Also when ; thus shifts an index by (The level-zero vector representation, its affinization and the level-one crystal energy, The q-wedge relations coincide with the type-A energy braiding kernel).
A charge- normal word has indices . Its size is the finite excess once contains its nonvacuum part, and its label weight is . The simple roots are independent in the explicit affine datum (The semi-infinite q-wedge Fock space and its q-adic topology, The cyclic affine type A Cartan datum and its residues).
Proof
Right-tail vanishing. Put . By [F2], is equivalent to . Choose and truncate the filled tail at . The word has factors, all in the interval , which contains only integers. Every normal term of its finite straightening would have that many distinct indices inside the same interval, which is impossible by [F1]. Thus this finite word is zero, as is every longer prefix. Its semi-infinite image is zero and therefore belongs to for every at each such finite stage (and to in the Fock space). This argument concerns the whole filled tail; it does not assert that alone is zero when .
Finite shifts of . Here nonzero weight means that is homogeneous of a weight : it maps a weight space of weight into weight . Write each as a finite sum . Since and is invertible, . Thus each term replaces by , where belongs to a fixed finite set obtained from the fundamental vectors; its coefficient depends only on . A term with would be the same vector and have weight shift zero, so its coefficient is zero by homogeneity. Choose bounding the absolute values of all occurring shifts.
Definition and gradings of . On an eventually-ground word define by prepending and replacing every old index by . The simultaneous translation by preserves the finite wedge relations: all residue differences and index gaps are unchanged. The new ground tail is again the charge- tail, so this operation respects local kernels and extending a representative by ground entries, and defines a linear endomorphism of . At position , its excess above the ground index is ; the prepended entries have excess zero. The old residues are unchanged by translation by , and the new ground entries contribute zero residue-count deviation. Hence total size and label weight are preserved before and after straightening, by [F1] and [F3]. In particular preserves each label-weight/size component; this does not require a permutation of its partition labels.
Finite label weights. If has fixed label weight , then , where counts the residue- cells. Independence of the simple roots in [F3] uniquely determines all and hence . Only finitely many partitions have this size: each has at most that many positive parts, each bounded by the size. Therefore each label weight contains finitely many partition basis vectors.
Dual left-tail vanishing. The mirrored filled tail ending at is , with an extra factor on its right and the mirrored condition , equivalently . Truncate its left end at any . The resulting word has factors inside the integers of , so it is zero by the same finite normal-basis count. Extending that left end preserves zero. This is the reversed-interval version of step 1.1 and proves the dual exact finite vanishing and all its -adic estimates.
Deep replacement. Fix an eventually-ground representative of a Fock vector. At a sufficiently deep slot its index is , and the entire local block is ground. In a term of the insertion of at that slot, replace by , where . This still has exactly factors, all in . Its total index sum is the ground block's sum plus . By [F1] the only possible normal tuple of that cardinality in this interval is the complete ground tuple, whose sum is different. Every normal coefficient must therefore be zero. The block vanishes before it is wedged with the remaining factors, so the insertion is zero at every sufficiently deep slot; the cutoff is uniform for the finite shifts and, by taking a maximum, for any finite linear combination of representatives. These eventual zeros converge to zero in the separated -adic topology.
Nilpotence on positive size. On , prepends ground entries and shifts all old indices down by . The largest shifted old index is , so when all indices of the resulting word are at most . Choose a finite prefix of length whose remainder is ground and whose last ground entry is below every nonground index. Its ground sum is and its actual sum is , by step 1.3. Every normal -tuple with maximum at most satisfies , and therefore has sum at most . Straightening preserves sum and the upper bound , so no such normal term exists if . Thus the finite prefix, and hence , is zero. Equivalently the only normal charge- semi-infinite word with maximum at most is the vacuum, excluded by the preserved positive size. Since , on the size- part whenever .
Geometric inverse. On a positive-size component choose with . The finite operator sum satisfies by step 2.3. This gives the claimed finite geometric inverse on every nonvacuum label weight and the resulting isomorphism for the tail recurrence; no inverse on the vacuum component is asserted.
Conclusion. Steps 1.1 and 2.1 give the right and dual left filled-tail estimates by exact finite vanishing; step 2.2 gives eventual zero for every deep insertion of a loop-commuting homogeneous nonzero-weight endomorphism; steps 1.3, 2.3 and 3.1 give the size-preserving and label-weight-preserving period operator, its positive-size nilpotence bound and finite inverse; and step 1.4 proves finite label-weight components.
Remarks
- The estimates are proved here in the library's residue convention with the ground sequence ; none of the two-sided-unbounded evaluation statements of the earlier finite ordered tensor theory is imported.
Depends on
- The semi-infinite q-wedge Fock space and its q-adic topology
- Normally ordered q-wedges form a basis for every finite wedge length
- The vector representation has a perfect crystal of level one and a lower global basis
- The q-wedge relations coincide with the type-A energy braiding kernel
- The cyclic affine type A Cartan datum and its residues
- The level-zero vector representation, its affinization and the level-one crystal energy
Used by
Dependency tree · two levels
22 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Kashiwara-Miwa-Petersen-Yung, Perfect crystals and q-deformed Fock spaces (standard reference, not scraped)
- Masaki Kashiwara, Tetsuji Miwa and Eugene Stern, Decomposition of q-deformed Fock spaces, arXiv:q-alg/9508006 (standard reference, not scraped)