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 finite-dimensional
Poisson manifold In differential geometry, a field in mathematics, a Poisson manifold is a smooth manifold endowed with a Poisson structure. The notion of Poisson manifold generalises that of symplectic manifold, which in turn generalises the phase space from Hami ...
. This operator algebra amounts to the
deformation quantization In mathematics and physics, deformation quantization roughly amounts to finding a (quantum) algebra whose classical limit is a given (classical) algebra such as a Lie algebra or a Poisson algebra. In physics Intuitively, a deformation of a math ...
of the corresponding Poisson algebra. It is due to
Maxim Kontsevich Maxim Lvovich Kontsevich (, ; born 25 August 1964) is a Russian and French mathematician and mathematical physicist. He is a professor at the Institut des Hautes Études Scientifiques and a distinguished professor at the University of Miami. He ...
.


Deformation quantization of a Poisson algebra

Given a
Poisson algebra In mathematics, a Poisson algebra is an associative algebra together with a Lie bracket that also satisfies Leibniz's law; that is, the bracket is also a derivation. Poisson algebras appear naturally in Hamiltonian mechanics, and are also central ...
, a deformation quantization is an associative unital product \star on the algebra of formal
power series In mathematics, a power series (in one variable) is an infinite series of the form \sum_^\infty a_n \left(x - c\right)^n = a_0 + a_1 (x - c) + a_2 (x - c)^2 + \dots where ''a_n'' represents the coefficient of the ''n''th term and ''c'' is a co ...
in , subject to the following two axioms, :\begin f\star g &=fg+\mathcal(\hbar)\\ ,g&=f\star g-g\star f=i\hbar\+\mathcal(\hbar^2) \end If one were given a Poisson manifold , one could ask, in addition, that :f\star g=fg+\sum_^\infty \hbar^kB_k(f\otimes g), where the are linear bi
differential operator In mathematics, a differential operator is an operator defined as a function of the differentiation operator. It is helpful, as a matter of notation first, to consider differentiation as an abstract operation that accepts a function and retur ...
s of degree at most . Two deformations are said to be equivalent iff they are related by a gauge transformation of the type, :\begin D: A \hbar\to A \hbar \\ \sum_^\infty \hbar^k f_k \mapsto \sum_^\infty \hbar^k f_k +\sum_ D_n(f_k)\hbar^ \end where are differential operators of order at most . The corresponding induced \star-product, \star', is then :f\,'\,g = D \left ( \left (D^f \right )\star \left (D^g \right ) \right ). For the archetypal example, one may well consider Groenewold's original "Moyal–Weyl" \star-product.


Kontsevich graphs

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


Associated bidifferential operator

Associated to each graph , there is a bidifferential operator 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 is the product of all its symbols together with their partial derivatives. Here ''f'' and ''g'' stand for smooth functions on the manifold, and is the
Poisson bivector In differential geometry, a field in mathematics, a Poisson manifold is a smooth manifold endowed with a Poisson structure. The notion of Poisson manifold generalises that of symplectic manifold, which in turn generalises the phase space from Hami ...
of the Poisson manifold. The term for the example graph is :\Pi^\partial_\Pi^\partial_f\,\partial_\partial_g.


Associated weight

For adding up these bidifferential operators there are the weights of the graph . First of all, to each graph there is a multiplicity which counts how many equivalent configurations there are for one graph. The rule is that the sum of the multiplicities for all graphs with internal vertices is . The sample graph above has the multiplicity . For this, it is helpful to enumerate the internal vertices from 1 to . In order to compute the weight we have to integrate products of the angle in the
upper half-plane In mathematics, the upper half-plane, is the set of points in the Cartesian plane with The lower half-plane is the set of points with instead. Arbitrary oriented half-planes can be obtained via a planar rotation. Half-planes are an example ...
, ''H'', as follows. The upper half-plane is , endowed with the
Poincaré metric In mathematics, the Poincaré metric, named after Henri Poincaré, is the metric tensor describing a two-dimensional surface of constant negative curvature. It is the natural metric commonly used in a variety of calculations in hyperbolic geometry ...
:ds^2=\frac; and, for two points with , we measure the angle between the geodesic from to and from to counterclockwise. This is :\phi(z,w)=\frac\log\frac. The integration domain is ''C''''n''(''H'') the space :C_n(H):=\. The formula amounts :w_\Gamma:= \frac\int_ \bigwedge_^n\mathrm\phi(u_j,u_)\wedge\mathrm\phi(u_j,u_), where ''t''1(''j'') and ''t''2(''j'') are the first and second target vertex of the internal vertex . The vertices ''f'' and ''g'' are at the fixed positions 0 and 1 in .


The formula

Given the above three definitions, the Kontsevich formula for a star product is now :f\star g = fg+\sum_^\infty\left(\frac\right)^n \sum_ w_\Gamma B_\Gamma(f\otimes g).


Explicit formula up to second order

Enforcing associativity of the \star-product, it is straightforward to check directly that the Kontsevich formula must reduce, to second order in , to just :\begin f\star g &= fg +\tfrac\Pi^\partial_i f\,\partial_j g -\tfrac\Pi^\Pi^\partial_\,\partial_f \partial_\,\partial_g\\ & - \tfrac\Pi^\partial_\Pi^(\partial_\partial_f \,\partial_g -\partial_f\,\partial_\partial_g) +\mathcal(\hbar^3) \end


References

{{DEFAULTSORT:Kontsevich Quantization Formula Mathematical quantization