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Kontsevich quantization formula

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In mathematics, the Kontsevich quantization formula describes how to construct a generalized ★-product operator algebra from a given arbitrary Poisson manifold. This operator algebra amounts to the deformation quantization of the corresponding Poisson algebra. It is due to Maxim Kontsevich.

Contents

Deformation quantization of a Poisson algebra

Given a Poisson algebra (A, {⋅, ⋅}), a deformation quantization is an associative unital product ★ on the algebra of formal power series in ħ, A[[ħ]], subject to the following two axioms,

f g = f g + O ( ) [ f , g ] = f g g f = i { f , g } + O ( 2 )

If one were given a Poisson manifold (M, {⋅, ⋅}), one could ask, in addition, that

f g = f g + k = 1 k B k ( f g ) ,

where the Bk are linear bidifferential operators of degree at most k.

Two deformations are said to be equivalent iff they are related by a gauge transformation of the type,

{ D : A [ [ ] ] A [ [ ] ] k = 0 k f k k = 0 k f k + n 1 , k 0 D n ( f k ) n + k

where Dn are differential operators of order at most n. The corresponding induced ★-product, ★′, is then

f g = D ( ( D 1 f ) ( D 1 g ) ) .

For the archetypal example, one may well consider Groenewold's original "Moyal–Weyl" ★-product.

Kontsevich graphs

A Kontsevich graph is a simple directed graph without loops on 2 external vertices, labeled f and g; and n internal vertices, labeled Π. From each internal vertex originate two edges. All (equivalence classes of) graphs with n internal vertices are accumulated in the set Gn(2).

An example on two internal vertices is the following graph,

Associated bidifferential operator

Associated to each graph Γ, there is a bidifferential operator BΓ( f, g) defined as follows. For each edge there is a partial derivative on the symbol of the target vertex. It is contracted with the corresponding index from the source symbol. The term for the graph Γ is the product of all its symbols together with their partial derivatives. Here f and g stand for smooth functions on the manifold, and Π is the Poisson bivector of the Poisson manifold.

The term for the example graph is

Π i 2 j 2 i 2 Π i 1 j 1 i 1 f j 1 j 2 g .

Associated weight

For adding up these bidifferential operators there are the weights wΓ of the graph Γ. First of all, to each graph there is a multiplicity m(Γ) which counts how many equivalent configurations there are for one graph. The rule is that the sum of the multiplicities for all graphs with n internal vertices is (n(n + 1))n. The sample graph above has the multiplicity m(Γ) = 8. For this, it is helpful to enumerate the internal vertices from 1 to n.

In order to compute the weight we have to integrate products of the angle in the upper half-plane, H, as follows. The upper half-plane is H ⊂ ℂ, endowed with a metric

d s 2 = d x 2 + d y 2 y 2 ;

and, for two points z, wH with zw, we measure the angle φ between the geodesic from z to i and from z to w counterclockwise. This is

ϕ ( z , w ) = 1 2 i log ( z w ) ( z w ¯ ) ( z ¯ w ) ( z ¯ w ¯ ) .

The integration domain is Cn(H) the space

C n ( H ) := { ( u 1 , , u n ) H n : u i u j i j } .

The formula amounts

w Γ := m ( Γ ) ( 2 π ) 2 n n ! C n ( H ) j = 1 n d ϕ ( u j , u t 1 ( j ) ) d ϕ ( u j , u t 2 ( j ) ) ,

where t1(j) and t2(j) are the first and second target vertex of the internal vertex j. The vertices f and g are at the fixed positions 0 and 1 in H.

The formula

Given the above three definitions, the Kontsevich formula for a star product is now

f g = f g + n = 1 ( i 2 ) n Γ G n ( 2 ) w Γ B Γ ( f g ) .

Explicit formula up to second order

Enforcing associativity of the ★-product, it is straightforward to check directly that the Kontsevich formula must reduce, to second order in ħ, to just

f g = f g + i 2 Π i j i f j g 2 8 Π i 1 j 1 Π i 2 j 2 i 1 i 2 f j 1 j 2 g 2 12 Π i 1 j 1 j 1 Π i 2 j 2 ( i 1 i 2 f j 2 g i 2 f i 1 j 2 g ) + O ( 3 )

References

Kontsevich quantization formula Wikipedia