The chromatic symmetric function is a symmetric function invariant of graphs studied in algebraic graph theory, a branch of mathematics. It is the weight generating function for proper graph colorings, and was originally introduced by Richard Stanley as a generalization of the chromatic polynomial of a graph.[1]
For a finite graph G = ( V , E ) {\displaystyle G=(V,E)} with vertex set V = { v 1 , v 2 , … , v n } {\displaystyle V=\{v_{1},v_{2},\ldots ,v_{n}\}} , a vertex coloring is a function κ : V → C {\displaystyle \kappa :V\to C} where C {\displaystyle C} is a set of colors. A vertex coloring is called proper if all adjacent vertices are assigned distinct colors (i.e., { i , j } ∈ E ⟹ κ ( i ) ≠ κ ( j ) {\displaystyle \{i,j\}\in E\implies \kappa (i)\neq \kappa (j)} ). The chromatic symmetric function denoted X G ( x 1 , x 2 , … ) {\displaystyle X_{G}(x_{1},x_{2},\ldots )} is defined to be the weight generating function of proper vertex colorings of G {\displaystyle G} :[1][2] X G ( x 1 , x 2 , … ) := ∑ κ : V → N proper x κ ( v 1 ) x κ ( v 2 ) ⋯ x κ ( v n ) {\displaystyle X_{G}(x_{1},x_{2},\ldots ):=\sum _{\underset {\text{proper}}{\kappa :V\to \mathbb {N} }}x_{\kappa (v_{1})}x_{\kappa (v_{2})}\cdots x_{\kappa (v_{n})}}
For λ {\displaystyle \lambda } a partition, let m λ {\displaystyle m_{\lambda }} be the monomial symmetric polynomial associated to λ {\displaystyle \lambda } .
Consider the complete graph K n {\displaystyle K_{n}} on n {\displaystyle n} vertices:
Thus, X K n ( x 1 , … , x n ) = n ! x 1 ⋯ x n = n ! m ( 1 , … , 1 ) {\displaystyle X_{K_{n}}(x_{1},\ldots ,x_{n})=n!x_{1}\cdots x_{n}=n!m_{(1,\ldots ,1)}}
Consider the path graph P 3 {\displaystyle P_{3}} of length 3 {\displaystyle 3} :
Altogether, the chromatic symmetric function of P 3 {\displaystyle P_{3}} is then given by:[2] X P 3 ( x 1 , x 2 , x 3 ) = 6 x 1 x 2 x 3 + x 1 2 x 2 + x 1 x 2 2 + x 1 2 x 3 + x 1 x 3 2 + x 2 2 x 3 + x 2 x 3 2 = 6 m ( 1 , 1 , 1 ) + m ( 1 , 2 ) {\displaystyle X_{P_{3}}(x_{1},x_{2},x_{3})=6x_{1}x_{2}x_{3}+x_{1}^{2}x_{2}+x_{1}x_{2}^{2}+x_{1}^{2}x_{3}+x_{1}x_{3}^{2}+x_{2}^{2}x_{3}+x_{2}x_{3}^{2}=6m_{(1,1,1)}+m_{(1,2)}}
There are a number of outstanding questions regarding the chromatic symmetric function which have received substantial attention in the literature surrounding them.
For a partition λ {\displaystyle \lambda } , let e λ {\displaystyle e_{\lambda }} be the elementary symmetric function associated to λ {\displaystyle \lambda } .
A partially ordered set P {\displaystyle P} is called ( 3 + 1 ) {\displaystyle (3+1)} -free if it does not contain a subposet isomorphic to the direct sum of the 3 {\displaystyle 3} element chain and the 1 {\displaystyle 1} element chain. The incomparability graph inc ( P ) {\displaystyle {\text{inc}}(P)} of a poset P {\displaystyle P} is the graph with vertices given by the elements of P {\displaystyle P} which includes an edge between two vertices if and only if their corresponding elements in P {\displaystyle P} are incomparable.
Conjecture (Stanley–Stembridge) Let G {\displaystyle G} be the incomparability graph of a ( 3 + 1 ) {\textstyle (3+1)} -free poset, then X G {\textstyle X_{G}} is e {\displaystyle e} -positive.[1]
A weaker positivity result is known for the case of expansions into the basis of Schur functions.
Theorem (Gasharov) Let G {\displaystyle G} be the incomparability graph of a ( 3 + 1 ) {\textstyle (3+1)} -free poset, then X G {\textstyle X_{G}} is s {\displaystyle s} -positive.[3]
In the proof of the theorem above, there is a combinatorial formula for the coefficients of the Schur expansion given in terms of P {\displaystyle P} -tableaux which are a generalization of semistandard Young tableaux instead labelled with the elements of P {\displaystyle P} .
There are a number of generalizations of the chromatic symmetric function: