Divided Diference Operators Omar Ortiz Department of Mathematics and Statistics University of Melbourne Parkville, VIC 3010 Australia [email protected] January 29, 2012 1 Definition Fix the following data: V a C-vector space of finite dimension n with basis v1 , . . . , vn . V ∗ the dual space of V , with basis X1 , . . . , Xn dual to v1 , . . . , vn . S = C(X1 , . . . , Xn ) the C-algebra of rational functions on V . W ⊆ GL(V ) a finite reflection group generated by the reflections s1 , . . . , sr , acting on V ∗ by contragredient: wX(v) = X(w−1 v) for w ∈ W, X ∈ V ∗ and v ∈ V ; and on S by extension: w(gh) = (wg)(wh) and w g h = wg wh for w ∈ W and g, h ∈ S. NW = hf ∈ S; tw for w ∈ W | tu tv = tuv , tw f = (wf )tw i the Nil-Hecke Algebra of W . For each reflection sα ∈ W , where α denotes the root of the reflection, the divided difference operator Tα ∈ NW is defined by 1 (1 − tsα ). α And for any w ∈ W with reduced expression w = sα1 · · · sαl we define Tw ∈ NW as Tα = Tw = Tα1 · · · Tαl . 1 2 Actions The Nil-Hecke Algebra acts naturally on the algebra of rational functions S by: f · g = f g (polynomial multiplication), for f ∈ NW and g ∈ S; tw · g = wg (contragredient action), for tw ∈ NW and g ∈ S. Therefore, the divided difference operator Tα acts on S by Tα f = f − sα f α for f ∈ S. NW also acts on the algebra ZW of global sections of the structure sheaf over the moment graph of W , ZW = {ψ : W −→ S | ψ(u) − ψ(v) ∈ αS if u = sα v}, by f · ψ(w) = (wf )ψ(w), for f ∈ NW and ψ ∈ ZW ; tu · ψ(w) = ψ(wu), for tu ∈ NW and ψ ∈ ZW . Therefore, the divided difference operator Tα acts on ZW by Tα ψ(w) = 3 ψ(w) − ψ(wsα ) wα for ψ ∈ ZW . BGG bases Recall the definition of the coinvariant algebra SW , SW = C[X1 , . . . , Xn ] , hP ∈ S W | P (0) = 0i where S W denotes the algebra of W -invariant polynomials. Q Let Q = {α | sα is a reflection} and w0 be the longest element in W (when expressed as a reduced word in the generators). Theorem 3.1 (BGG). {Pw }w∈W is a basis of SW as a C-vector space, where Pw0 = and Pw = Tw−1 w0 Pw0 . 2 1 |W | Q Theorem 3.2. {ψ w }w∈W is a basis of ZW where Q , if w = w0 ; w0 ψ (w) = 0 , if w 6= w0 . and ψ w = Tw−1 w0 ψ w0 . Theorem 3.3. The map φ : SW Pw / ZW / ψw is and algebra isomorphism. 4 Example Let V = C − span{v1 , v2 , v3 } and V ∗ = C − span{X1 , X2 , X3 }. s s s s s s 0 1 0 1 0 0 T T Let s1 = 1 0 0 = T , s2 = 0 0 1 = , T T s s s s s T s 0 0 1 0 1 0 and W = hs1 , s2 i = {c, s1 , s2 , s1 s2 , s2 s1 , s1 s2 s1 } ⊆ GL(V ). Since w0 = s1 s2 s1 is also a reflection, we will also denote it as s3 , s s s 0 0 1 l , , . s3 = s1 s2 s1 = 0 1 0 = l, l s s ls , 1 0 0 The action of W on V ∗ is given by the inverse transpose of the above matrices. But since in this case s−t i = si for i = 1, 2, 3; the action is the same as in V . Let us denote by αi the root in V ∗ corresponding to si for i = 1, 2, 3. Then α1 = X1 − X2 , α2 = X2 − X3 , α3 = X1 − X3 . The coinvariant algebra is SW = C[X1 , X2 , X3 ] . hX1 + X2 + X3 , X1 X2 + X1 X3 + X2 X3 , X1 X2 X3 i As a vector space, 3 SW 1, X1 , X2 , = C − span X 2, X X , 12 1 2 X1 X2 . The BGG basis theorem gives us Pw0 = 61 α1 α2 α3 = X12 X2 , Ps1 s2 = 31 α2 α3 = X1 X2 , Ps2 s1 = 31 α1 α3 = X12 , Ps1 = 31 (α1 + α3 ) = X1 , Ps2 = 31 (α2 + α3 ) = X1 + X2 , Pc = 1, as a basis for SW , i.e. SW 1, X1 , X1 + X2 , = C − span X 2, X X , 12 1 2 X1 X2 ; which clearly agrees with the basis above. For ZW we get the following basis elements 0 0 0 0 0 0 , ψ s1 s2 = , ψ w0 = 0 0 0 −α1 α3 −α1 α3 α1 α2 α3 0 ψ s1 0 = α3 α3 ψ s2 α = 2 α2 ψ s2 s1 = 0 −α2 α3 0 , α3 −1 ψc = −1 −1 . −1 −1 α3 4 0 , 0 −α2 α3 −1 0 α1 , α1 0
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