- 227 -Mazzola, Guerino / Noll, Thomas / Lluis-Puebla, Emilio: Perspectives in Mathematical and Computational Music Theory 
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Setting  t fx = IdAx , we have defined the required affine map  t 0 fx = fx + fx : Bx --> End(Ax) with
fx(/\ ox Dir)(Z) = Z -LZ/\.GDir.

This is the typical example to be memorized in the following abstract discussion of a stemma.

Let m (- V(T) be a mother. Then for each daughter x (- Dm(T ) , we define a triaffine (affine in each argument) map

 prod fx : Am × C#Dm(T )× By --> Ax, (1) y (- Dm(T)
by
 (am,(cmy,x)y (- Dm(T ),(by)y (- Dm(T)) '--> sum cm iy,x(fy(by)(rm,y(am))) = sum m y (- 0Dm(T) y,x sum m t y (- Dm(T)cy,xiy,x(fy(by)(rm,y(am))) + y (- Dm(T) cy,xiy,x(fy(rm,y(am))).
Referring to the above example, this formula describes the following: In order to determine the performance field on the frame Fx , we use the field of its mother m , we first restrict that field to any of its daughters y and get the fields rm,y(am) . These sister fields to daughter x are then deformed under the endomorphisms fy(by) = fty + f0y(by) induced by the system parameters by . These deformed fields are then transported to x and weighted by the factors cmy,x . These sister fields influence the final value of the field at daughter x . Musically, this means that the performance at x is influenced by surrounding sister fields, which are typically the fields of past and future times (past or future periods, bars, etc.).

Technically speaking, we proceed as follows: For each final vertex z (- V(T) let mz0 = r,mz1,mz2,...,mznz = z, be the ordered sequence of elements of Mz(T ) . For the root r and for each final vertex z (- V (T ) let us fix arbitrary er (- Ar , ez (- Az , respectively. The main task of inverse performance theory (Mazzola1995) is to study the set of solutions of the system of equalities

ez = mzn-1 (2) fmznz(fmznz-1(...fmz1(er,(cry1,mz1),(by1)),...),(cynzz,mznz),(bynz))
where for k = 1,...,nz the vertexes yk lie in the set Dmzk- 1(T) .

For the explicit calculation, we select a basis vx1,...,vxsx of the vector space Bx . This means that for every vertex x (- V(T) we may consider the linear operators Oxi := f0x(vxi) (- End(Ax),i = 1,...,sx as a part of our data. Whence, if we identify Bx with Csx through the basis vx1,...,vxsx , we can define the homomorphism (1) as a triaffine map

 prod fx : Am × C#Dm(T )× Csyy --> Ax y (- Dm(T )


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- 227 -Mazzola, Guerino / Noll, Thomas / Lluis-Puebla, Emilio: Perspectives in Mathematical and Computational Music Theory