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Contributions à l'Etude du Vertex Topologique en Théorie ... - Toubkal

Contributions à l'Etude du Vertex Topologique en Théorie ... - Toubkal

Contributions à l'Etude du Vertex Topologique en Théorie ... - Toubkal

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013509-4 Drissi, Jehjouh, and Saidi J. Math. Phys. 50, 013509 2009R 3 q,t = 1−q k−1 t l .k,l=12.8By setting t=q back in 2.8, we get the standard C 3 q relation. The explicit expression of therefined R q,t in terms of Schur functions can be found in Ref. 8.C. Shifted S 3 „q…The shifted 3d MacMahon S 3 q is the g<strong>en</strong>erating functional of strict plane partitions. Theexplicit expression of S 3 q has be<strong>en</strong> derived by Foda and Wheeler by using transfer matrixmethod. It reads asS 3 q = n=1 n1+qn n, 2.91−qand has an interpretation in the BKP hierarchy of the so-called neutral free fermions. It wasclaimed in Ref. 15 that S 3 q could be relevant to the topological string <strong>du</strong>al to ON Chern–Simon theory in the limit N→.III. SHIFTED TOPOLOGICAL VERTEXThe expression Eq. 2.9 of the shifted topological vertex has be<strong>en</strong> derived in the abs<strong>en</strong>ce ofany kind of boundary conditions. Here, we want to complete this result by considering the derivationof the shifted topological vertex S with g<strong>en</strong>eric boundary conditions with the property,S = S q, S = S 3 q. 3.1Notice that S q g<strong>en</strong>erates the shifted 3d partitions with boundary conditions giv<strong>en</strong> by the strict2d partitions ,, along the axis x 1 ,x 2 ,x 3 . For the definitions of the shifted 3d and strict 2dpartitions, see the App<strong>en</strong>dix.The main result of this section is collected in the following proposition where some terminologyhas be<strong>en</strong> borrowed from: 8Proposition 1: The perp<strong>en</strong>dicular shifted topological vertex S q with g<strong>en</strong>eric boundaryconditions, giv<strong>en</strong> by three strict 2d-partitions ,,, reads as follows:L q = f S 1−qn1+q nn, 3.2which can be also put in the normalized formn=1In relation 3.2, the numerical factor f isS = S L ,L q =1.3.3f =2 l+l+l q 1/22 + 2 + 2 ,f q =1,where 2 = i i 2 and l is the l<strong>en</strong>gth of the strict partition that is the number parts of the strict2d partition = 1 ,..., l ,0,....The function S q is the perp<strong>en</strong>dicular partition function of shifted 3d-partitions. It reads interms of Schur functions P t / and Q / as follows:3.4Downloaded 24 Mar 2009 to 140.105.16.64. Redistribution subject to AIP lic<strong>en</strong>se or copyright; see http://jmp.aip.org/jmp/copyright.jsp

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