Quasi-commutative property#Applied to functions

In mathematics, the quasi-commutative property is an extension or generalization of the general commutative property. This property is used in specific applications with various definitions.

Applied to matrices

Two matrices p and q are said to have the commutative property whenever

pq = qp

The quasi-commutative property in matrices is definedNeal H. McCoy. [https://www.ams.org/journals/tran/1934-036-02/S0002-9947-1934-1501746-8/S0002-9947-1934-1501746-8.pdf On quasi-commutative matrices. Transactions of the American Mathematical Society, 36(2), 327–340]. as follows. Given two non-commutable matrices x and y

xy - yx = z

satisfy the quasi-commutative property whenever z satisfies the following properties:

\begin{align}

xz &= zx \\

yz &= zy

\end{align}

An example is found in the matrix mechanics introduced by Heisenberg as a version of quantum mechanics. In this mechanics, p and q are infinite matrices corresponding respectively to the momentum and position variables of a particle. These matrices are written out at Matrix mechanics#Harmonic oscillator, and z = iħ times the infinite unit matrix, where ħ is the reduced Planck constant.

Applied to functions

A function f : X \times Y \to X is said to be {{visible anchor|quasi-commutative}}Benaloh, J., & De Mare, M. (1994, January). [http://citeseerx.ist.psu.edu/viewdoc/download?doi=10.1.1.13.8287&rep=rep1&type=pdf One-way accumulators: A decentralized alternative to digital signatures]. In Advances in Cryptology – EUROCRYPT’93 (pp. 274–285). Springer Berlin Heidelberg. if

f\left(f\left(x, y_1\right), y_2\right) = f\left(f\left(x, y_2\right), y_1\right) \qquad \text{ for all } x \in X, \; y_1, y_2 \in Y.

If f(x, y) is instead denoted by x \ast y then this can be rewritten as:

(x \ast y) \ast y_2 = \left(x \ast y_2\right) \ast y \qquad \text{ for all } x \in X, \; y, y_2 \in Y.

See also

  • {{annotated link|Commutative property}}
  • {{annotated link|Accumulator (cryptography)}}

References