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Partition theorem, cluster theorems

The fundamental idea behind the cumulant expansion, the Ursell development, Mayer's cluster theorem, and the linked cluster theorem from quantum field theory can be represented most succinctly by considering the idea of structuring a set of objects. To define, each structuring of an n-set of objects is a way that a set of objects may be named or organized. For instance, we have the uniform structure, which is the set itself. We may also have a structure like permutation, which is any ordering of the objects. There is also the structure of partitioning a set of objects. Consider the operation of partitioning the n-set into subsets. For example, tex2html_wrap_inline13337 is one partition of tex2html_wrap_inline13339. How many ways can a structure of a certain type be imposed? Let tex2html_wrap_inline13341 be the exponential generating function for a structure of type M. Then there are tex2html_wrap_inline13345 ways that an n-set can be structured according to M. For example, there is one way that the uniform structure can be imposed on any non-empty n-set. Therefore, the generating function for the uniform structure is tex2html_wrap_inline13353. Now consider the notion of structuring a set of structures. In how many ways can this be done? In general, if there are several structures of type tex2html_wrap_inline13355, and the structures are themselves organized into a structure of type tex2html_wrap_inline13357 then the generating function for tex2html_wrap_inline13357 structured tex2html_wrap_inline13355 structures is tex2html_wrap_inline13363.

: Structure Composition or Structure Substitution. Let tex2html_wrap_inline13365 be the generating function for a structure of type tex2html_wrap_inline13357, and similarly for tex2html_wrap_inline13369. The number of ways that an n-set can be first partitioned into subsets, then each subset structured by tex2html_wrap_inline13355, and then these structured subsets taken as objects and structured by tex2html_wrap_inline13357 is given by the coefficient of tex2html_wrap_inline13377 in tex2html_wrap_inline13363.

Proof: Take any partition of the n set. There are tex2html_wrap_inline13383 subsets of size 1, tex2html_wrap_inline13387 subsets of size 2, tex2html_wrap_inline13391tex2html_wrap_inline13393 subsets of size k. Thus tex2html_wrap_inline13397. We may permute subsets of the same cardinality, and within any subset we may permute the objects. Thus there are
equation953
such partitions. For each of these partitions, each subset of the partition is structured by tex2html_wrap_inline13355, and the number of ways that the partitioning and tex2html_wrap_inline13355 structuring may be done is then
equation958
Now, the number of ways these structured subsets may be structured by tex2html_wrap_inline13357 is given by tex2html_wrap_inline13405 times this, where tex2html_wrap_inline13407, and the contribution to the coefficient of tex2html_wrap_inline13409 in the generating function for the compound structure is found by multiplying by tex2html_wrap_inline13411. This contribution is found in tex2html_wrap_inline13363 from the term tex2html_wrap_inline13415 as
equation973
Conversely, every such term represents some partition of the n-set into q subsets with structuring of the set of subset objects according to tex2html_wrap_inline13357 (the factor tex2html_wrap_inline13405) and with structuring of each subset according to tex2html_wrap_inline13355. QED.

Now we are ready to prove the various forms of the partition theorem which have been found useful in many-body physics.

First, there are two observations that need to be made that make the preceding theorem more general: 1. It is possible to generalize the theorem above to the notion of weighted objects. The weight of a single object is assigned then by some function (tex2html_wrap_inline13355 above) of the single object, and need not be an integer as might have been assumed in the proof of the structure composition theorem. As before let the weight of a compound object be the product of the weights of the objects making up the compound object. 2. It is possible to label any set in any manner desired, and to each labeled set associate a distinct cluster (some abstract mapping for now, later a cluster is defined as a connected graph) dependent only upon the labels that the set has associated with it (independent of any ordering that might have been utilized). The labeling set may be of any nonempty size, even though only as many labels appear (perhaps not distinct) as there are elements in the set. The object that the set of a given size then represents is then the set of all clusters of that size, and its weight is then the sum of the weights of the clusters. These observations will be used in deriving the cumulant and Ursell expansions.

Define a cluster as any labeled subset. Define a graph as any set of clusters. Let the weight of a set of clusters be the sum of the weights of the clusters in the set. Let the weight of any graph be the product of the weights of the clusters in the graph. Let the weight of a set of graphs be the sum of the weights of the graphs. Let the number of vertices of a cluster be the number of objects in the cluster. Let the number of vertices of the graph be the sum of the numbers of vertices of the clusters in the graph. The structure composition theorem leads directly to the Linked Cluster Theorem.

. Linked Cluster Theorem. Let tex2html_wrap_inline13433 represent the set of all graphs on k vertices. Let tex2html_wrap_inline13293 be the set of all clusters on k vertices. Let the weight of any set of graphs be the sum of the weights of the graphs in the set, and let the weight of any graph be the product of the weights of the clusters in the graph. Represent the weight of a graph g as tex2html_wrap_inline13443. Let the weight of the empty graph be 0. Then
equation994

Proof: The coefficient of tex2html_wrap_inline13445 on the left hand side may be taken as the sum of the weights of all graphs on N vertices, so the left hand side is the generating function for the sum of the weights of all graphs on N vertices. The generating function of the uniform structure is tex2html_wrap_inline13353. By the structure composition theorem the generating function for the compound structure consisting of the uniform structure of tex2html_wrap_inline13355 structures is tex2html_wrap_inline13455. Let tex2html_wrap_inline13457 be the weight associated with a subset of size k. Make the identification indicated above the theorem of labeled subset and cluster. Then tex2html_wrap_inline13457 is the weight of the set of all clusters of size k. The function tex2html_wrap_inline13465 is then the generating function tex2html_wrap_inline13467 just defined. Make the identification of uniform structure of clusters and graph to find that the right side is immediately another expression for the generating function given by the left side. QED.

We may rewrite the linked cluster theorem in symbols more easily read directly. Let G(N) be any graph on N vertices, tex2html_wrap_inline13473 be any connected graph on N vertices and W(G) be the weight of any graph G. We then have that the linked cluster theorem is
equation1007
The weights of clusters may be any desired functions, and the rule stating that the weight of a graph made up of clusters is the product of the weights of the clusters immediately yields the Ursell development of 3.5 with sum of the weights of the graphs on vertices, the W(G(N)) here, being the tex2html_wrap_inline13483 there. A proper choice for the weights of the clusters immediately leads to the cumulant expansion theorem we have already discussed, as is proven next.

: Cumulant expansion theorem. See section 3.3

: Let the labels of the vertices in equation 3.20 range over a set tex2html_wrap_inline13485, and set x=1 in that equation. Let tex2html_wrap_inline13489 be any labeling of an m-vertex cluster consisting of tex2html_wrap_inline13243 labels 1, tex2html_wrap_inline13391tex2html_wrap_inline13499 k labels k. Define tex2html_wrap_inline13505 by tex2html_wrap_inline13507, where tex2html_wrap_inline13239 is an argument consisting of tex2html_wrap_inline13243tex2html_wrap_inline13245's, etc. Since an m vertex cluster may be labeled with tex2html_wrap_inline13243 1's, tex2html_wrap_inline13391tex2html_wrap_inline13499 k's in tex2html_wrap_inline13527 ways we find that the expression tex2html_wrap_inline13529 of equation 3.20, is tex2html_wrap_inline13531. Now, with the choice of the u given after equation 3.5, the right side of equation 3.20 becomes the right side of equation 3.5, and similarly for the left sides of these equations, thus showing that the cumulant expansion theorem follows as a special case of the linked cluster theorem, with the weights of the clusters given by special sums of products of averages of the variables that the labels of the cluster vertices represent. QED.

To summarize, in this section we have shown that the cumulant expansion, and the various cluster theorems are simply re-namings of a theorem about labeled partitions.


nextuppreviouscontents
Next:Factorization propertyUp:Information correlationcumulants, clusters, Previous:The Ursell functionspartitions,
David Wolf

Tue Mar 25 08:11:49 CST 1997