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Examples

As examples we will treat the tex2html_wrap_inline2257-group algebras tex2html_wrap_inline3925 of symmetric groups. Here the standard modules tex2html_wrap_inline2209 are known to be the Specht modules ([GL], 5.7, see [JK], chapter 7 for details on Specht-modules). The reader not familiar with cellular algebras may check imediately that the conditions stated in the begining of section 5 can be realised using this modules. They are labelled by the set tex2html_wrap_inline3929 of partitions of n and are defined as submodules of permutation modules tex2html_wrap_inline3933 on the cosets of parabolic subgroups corresponding to the partition tex2html_wrap_inline3045. As first example, let us look at tex2html_wrap_inline3937. Then tex2html_wrap_inline3933 is the permutation representation on the cosets of the copy of tex2html_wrap_inline3941 in tex2html_wrap_inline3943 fixing the last element n. As a tex2html_wrap_inline2257-module this is free of rank n with basis tex2html_wrap_inline3951, say. The operation of tex2html_wrap_inline3943 from the right is given by tex2html_wrap_inline3955. The Specht module tex2html_wrap_inline2209 is the free tex2html_wrap_inline2257-submodule with basis tex2html_wrap_inline3961 for tex2html_wrap_inline3963.

The symmetric bilinear form tex2html_wrap_inline3135 is given by restriction of the canonical bilinear form on tex2html_wrap_inline3933 (given by the unit matrix) to tex2html_wrap_inline2209. Thus the Gram matrix of tex2html_wrap_inline3135 is nothing but the Cartan matrix corresponding to the Dynkin diagram of type tex2html_wrap_inline3973. This in turn is just the coefficient matrix of tex2html_wrap_inline3975 with respect to the basis tex2html_wrap_inline3977 on tex2html_wrap_inline2209 and the corresponding dual basis tex2html_wrap_inline3981 on tex2html_wrap_inline2211. The image of tex2html_wrap_inline3157 is consequently the span of the columns of this matrix and is easily calculated to be the span of tex2html_wrap_inline3987 and tex2html_wrap_inline3989 for tex2html_wrap_inline3991. Therefore tex2html_wrap_inline3993 - the cokernel of tex2html_wrap_inline3157 - is generated by tex2html_wrap_inline3997 and is obviously isomorphic to tex2html_wrap_inline3999 as a tex2html_wrap_inline2257-module.

Let us show that the operation of tex2html_wrap_inline4003 on tex2html_wrap_inline3993 is trivial. We only need to check this for the long cycle tex2html_wrap_inline4007 or its inverse and tex2html_wrap_inline4009. On tex2html_wrap_inline2209 the operation is given by tex2html_wrap_inline4013 and tex2html_wrap_inline4015 for i>1 in the case of tex2html_wrap_inline3721 whereas we have tex2html_wrap_inline4021 and tex2html_wrap_inline4023 for all i>2. Transposing the corresponding coefficient matrices we get tex2html_wrap_inline4027. Since tex2html_wrap_inline4029 is congruent to tex2html_wrap_inline3997 modulo the image of tex2html_wrap_inline3157 we are done.

The Specht module of the partition tex2html_wrap_inline4035 is just the one-dimensional trivial representation with bilinear form tex2html_wrap_inline4037 being given by the trivial Gram matrix. Therefore tex2html_wrap_inline4039 holds in tex2html_wrap_inline2501. Moreover, we have shown the following equation in tex2html_wrap_inline2501:


displaymath3911

In the case of the symmetric group tex2html_wrap_inline2253 there are three partitions tex2html_wrap_inline4047 and tex2html_wrap_inline4049. The corresponding Specht modules are free tex2html_wrap_inline2257-modules of rank 1, 2 and 1, respectively. The cases tex2html_wrap_inline4059 and tex2html_wrap_inline4061 have been treated in general above. The Specht module tex2html_wrap_inline4063 is the sign representation and tex2html_wrap_inline4065. Therefore we have tex2html_wrap_inline4067. From the ordinary decomposition matrices of tex2html_wrap_inline2253 for the primes 2 and 3 we get tex2html_wrap_inline4075 and tex2html_wrap_inline4077 leading to the global decomposition matrix of tex2html_wrap_inline2253:


displaymath3912

Note that the corresponding equations according to condition (c) of Proposition 5.6 even hold in tex2html_wrap_inline2501. This will not be true in the next example tex2html_wrap_inline2255 as well as the fact that the global decomposition matrix can entirely be constructed from the knowledge of the ordinary decomposition matrices for the primes 2 and 3. On the other hand, the ordinary decomposition numbers are detected from the above by multiplying the whole table by [2] resp. [3] and then setting [2]=1 resp. [3]=1.

Before proceeding to the next example let us write down all the relations between the tex2html_wrap_inline3229 with the help of Proposition 5.8. We have to consider two pairs tex2html_wrap_inline4099 such that tex2html_wrap_inline3741. These are tex2html_wrap_inline4103 and tex2html_wrap_inline4105. We calculate tex2html_wrap_inline4107 and tex2html_wrap_inline4109. This gives tex2html_wrap_inline4111 and tex2html_wrap_inline4113 leading to the following complete set of relations for tex2html_wrap_inline4115 and tex2html_wrap_inline4117:


displaymath3913

Turning to tex2html_wrap_inline2255 we have 5 partitions tex2html_wrap_inline4123 and tex2html_wrap_inline4125. Let us first picture the global decomposition matrix and then comment it:


displaymath3914

First note that the entries [8] and [4] cannot be reconstructed from the knowledge of the ordinary decomposition matrices of tex2html_wrap_inline2255. As in the preceeding example the first row follows easily from tex2html_wrap_inline4133 and the knowledge of tex2html_wrap_inline4135 and tex2html_wrap_inline4077. Note that tex2html_wrap_inline4139 does not hold in tex2html_wrap_inline2501 but surely in tex2html_wrap_inline2941. In contrast, the equations corresponding to the rows 3,4,5 hold in tex2html_wrap_inline2501 the last two of which have been treated in the beginning of this chapter. We leave the calculation of tex2html_wrap_inline4149 as an exercise and turn to the most interesting case tex2html_wrap_inline4151.

Here the Specht module is a free tex2html_wrap_inline2257-module of rank three with basis tex2html_wrap_inline4155, say. The long cycle tex2html_wrap_inline4157 and tex2html_wrap_inline4009 operate from right by tex2html_wrap_inline4161 and tex2html_wrap_inline4163. The Gram matrix of the bilinear form is given by


displaymath3915

and therefore the image of tex2html_wrap_inline3157 is spanned by tex2html_wrap_inline4167 and tex2html_wrap_inline4169. Clearly, tex2html_wrap_inline4151 is isomorphic to [8]+[8]+[2] as a tex2html_wrap_inline2257-module. But anyway, as an A-module it is irreducible by tex2html_wrap_inline2257-sums as defined in chapter 2. Therefore it cannot be splitted in tex2html_wrap_inline2501 anymore. But we can calculate in tex2html_wrap_inline2941 as in the proof of Lemma 5.1. From the ordinary decomposition matrix for the prime 2, we get tex2html_wrap_inline4187 and by dimension arguments the 2-residual series must be


displaymath3916

which completes the verification. In order to determine the relations among the tex2html_wrap_inline3229 one calculates
eqnarray938

As in the case of tex2html_wrap_inline2253 a complete set of relations can be obtained from these formulas with help of Proposition 5.8.

Problems:


next up previous
Next: References Up: No Title Previous: Application to Cellular Algebras

Sebastian Oehms
Wed Mar 8 15:35:55 MEZ 2000