For a set of n random variables { X 1 , … , X n } {\displaystyle \{X_{1},\ldots ,X_{n}\}} , the dual total correlation D ( X 1 , … , X n ) {\displaystyle D(X_{1},\ldots ,X_{n})} is given by
where H ( X 1 , … , X n ) {\displaystyle H(X_{1},\ldots ,X_{n})} is the joint entropy of the variable set { X 1 , … , X n } {\displaystyle \{X_{1},\ldots ,X_{n}\}} and H ( X i ∣ ⋯ ) {\displaystyle H(X_{i}\mid \cdots )} is the conditional entropy of variable X i {\displaystyle X_{i}} , given the rest.
The dual total correlation normalized between [0,1] is simply the dual total correlation divided by its maximum value H ( X 1 , … , X n ) {\displaystyle H(X_{1},\ldots ,X_{n})} ,
Dual total correlation is non-negative and bounded above by the joint entropy H ( X 1 , … , X n ) {\displaystyle H(X_{1},\ldots ,X_{n})} .
Secondly, Dual total correlation has a close relationship with total correlation, C ( X 1 , … , X n ) {\displaystyle C(X_{1},\ldots ,X_{n})} , and can be written in terms of differences between the total correlation of the whole, and all subsets of size N − 1 {\displaystyle N-1} :7
where X = { X 1 , … , X n } {\displaystyle {\textbf {X}}=\{X_{1},\ldots ,X_{n}\}} and X − i = { X 1 , … , X i − 1 , X i + 1 , … , X n } {\displaystyle {\textbf {X}}^{-i}=\{X_{1},\ldots ,X_{i-1},X_{i+1},\ldots ,X_{n}\}}
Furthermore, the total correlation and dual total correlation are related by the following bounds:
Finally, the difference between the total correlation and the dual total correlation defines a novel measure of higher-order information-sharing: the O-information:8
The O-information (first introduced as the "enigmatic information" by James and Crutchfield9 is a signed measure that quantifies the extent to which the information in a multivariate random variable is dominated by synergistic interactions (in which case Ω ( X ) < 0 {\displaystyle \Omega ({\textbf {X}})<0} ) or redundant interactions (in which case Ω ( X ) > 0 {\displaystyle \Omega ({\textbf {X}})>0} .
Han (1978) originally defined the dual total correlation as,
However Abdallah and Plumbley (2010) showed its equivalence to the easier-to-understand form of the joint entropy minus the sum of conditional entropies via the following:
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Rosas, Fernando E.; Mediano, Pedro A. M.; Gastpar, Michael; Jensen, Henrik J. (13 September 2019). "Quantifying high-order interdependencies via multivariate extensions of the mutual information". Physical Review E. 100 (3): 032305. arXiv:1902.11239. Bibcode:2019PhRvE.100c2305R. doi:10.1103/PhysRevE.100.032305. PMID 31640038. /wiki/ArXiv_(identifier) ↩
James, Ryan G.; Ellison, Christopher J.; Crutchfield, James P. (1 September 2011). "Anatomy of a bit: Information in a time series observation". Chaos: An Interdisciplinary Journal of Nonlinear Science. 21 (3): 037109. arXiv:1105.2988. Bibcode:2011Chaos..21c7109J. doi:10.1063/1.3637494. PMID 21974672. /wiki/ArXiv_(identifier) ↩