HAL Id: hal-00000907
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Preprint submitted on 1 Dec 2003
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Spin-preserving Knuth correspondences for ribbon tableaux
Marc van Leeuwen
To cite this version:
Marc van Leeuwen. Spin-preserving Knuth correspondences for ribbon tableaux. 2003. �hal-00000907�
ccsd-00000907 (version 1) : 1 Dec 2003
Spin-preserving Knuth correspondences for ribbon tableaux
Marc A. A. van Leeuwen
Universit´ e de Poitiers, D´ epartement de Math´ ematiques,
UFR Sciences SP2MI, T´ el´ eport 2, BP 30179, 86962 Futuroscope Chasseneuil Cedex, France [email protected]
URL: http://www-math.univ-poitiers.fr/~maavl/
ABSTRACT
The RSK correspondence generalises the Robinson-Schensted correspondence by replacing permutation ma- trices by matrices with entries in N, and standard Young tableaux by semistandard ones. For r ∈ N >0 , the Robinson-Schensted correspondence can be trivially extended, using the r-quotient map, to one between coloured permutations and pairs of standard r-ribbon tableaux built on a fixed r-core (the Stanton-White correspondence). Viewing coloured permutations as matrices with entries in N r and total sum of coefficients in each row or column equal to 1 (so the unique non-zero entry is one of the r a generators of N r ), this corre- spondence can also be generalised to arbitrary matrices with entries in N r and pairs of semistandard r-ribbon tableaux built on a fixed r-core; the generalisation is derived from the RSK correspondence, again using the r-quotient map. Shimozono and White recently defined a more interesting generalisation of the Robinson- Schensted correspondence to coloured permutations and standard r-ribbon tableaux, one that (unlike the Stanton-White correspondence) respects the spin statistic (total height of ribbons) on standard r-ribbon tableaux, relating it directly to the colours of the coloured permutation. We define a construction estab- lishing a bijective correspondence between general matrices with entries in N r and pairs of semistandard r-ribbon tableaux built on a fixed r-core, which respects the spin statistic on those tableaux in a similar manner, relating it directly to the matrix entries. We also define a similar generalisation of the asymmetric RSK correspondence, in which case the matrix entries are taken from {0, 1} r .
More surprising than the existence of such a correspondence is the fact that its construction falsifies the conventional wisdom that Knuth correspondences should be derived from Schensted correspondences via the method of standardisation. Such a method does not work for general r-ribbon tableaux, since no ribbon Schensted insertion can preserve standardisations of horizontal strips (with one notable exception in the case r = 2 of domino tableaux). Instead, we use the analysis of Knuth correspondences by Fomin to focus on the correspondence at the level of a single matrix entry and one pair of ribbon strips. We define such a correspondence by a non-trivial generalisation of the idea underlying the Shimozono-White correspondence, which takes the form of an algorithm traversing the edge sequences of the shapes involved. As a result of the particular way in which this traversal has to be set up, our construction directly generalises neither the Shimozono-White correspondence nor the RSK correspondence: it specialises to the transpose of the former, and to the variation of the latter called the Burge correspondence.
Our constructions can be interpreted as bijective proofs of certain generating series identities. With G (r) λ (q, X) = P
P q 2 spin(P) X wt(P) ∈ Z[q][[X]], summed over semistandard r-ribbon tableaux P of shape λ, the first such identity is
X
λ≥
r(0)
G (r) λ (q
12, X)G (r) λ (q
12, Y ) = Y
i,j∈ N r−1 Y
k=0
1 1 − q k X i Y j ;
this can be considered the q-analogue of an r-fold Cauchy identity, since for q = 1 each G (r) λ (q
12, X) factors into a product of r Schur functions. It is equivalent to a commutation relation for certain operators acting on a q-deformed Fock space, obtained by Kashiwara, Miwa and Stern. Our asymmetric correspondence bijectively proves
X
λ≥
r(0)
G (r) λ (q
1
2
, X) G e (r) λ (q
1
2
, Y ) = Y
i,j∈ N r−1 Y
k=0
(1 + q k X i Y j ).
where G e (r) λ (q, X) = P
P q 2 spin
t