Malliavin calculus on the Clifford algebra
Takayoshi Watanabe
TL;DR
The paper develops Malliavin calculus on the Clifford algebra to extend stochastic-analytic techniques to fermionic (non-commutative) settings. By constructing an anti-symmetric derivation $\,\mathcal{D}$ and divergence $\,\delta$ that obey canonical anti-commutation, it builds a Clark-Ocone-type formula within the Itô-Clifford framework and analyzes key functional-analytic inequalities. It demonstrates that while concentration results resemble the classical case, the logarithmic Sobolev inequality is weaker, and a fourth-moment theorem does not guarantee distributional convergence for Clifford chaos, highlighting intrinsic differences from Brownian (bosonic) theory. The work also discusses limitations due to the non-Leibniz nature of the anti-symmetric derivation and outlines avenues for future extensions, including non-causal calculus and Lévy-area-like representations.
Abstract
We deal with Malliavin calculus on the $L^2$ space of the $W^*$-algebra generated by fermion fields (the Clifford algebra). First, we verify the product formula for multiple integrals in Itô-Clifford calculus, which is Itô calculus on the Clifford algebra. Using this product formula, we can define the derivation operator and the divergence operator. Anti-symmetric Malliavin calculus thus constructed has properties similar to those of usual Malliavin calculus. The derivation operator and the divergence operator satisfy the canonical anti-commutation relations, and the divergence operator serves as an extension of the Itô-Clifford stochastic integral, satisfying the Clark-Ocone formula. Subsequently, using this calculus, we consider the concentration inequality, the logarithmic Sobolev inequality, and the fourth-moment theorem. As for the logarithmic Sobolev inequality, only a weaker result is obtained. On the other hand, as for the concentration inequality, we obtain results that are almost similar to those of the usual case; moreover, the results concerning the fourth-moment theorem imply that, unlike in the case of the usual Brownian motion, convergence in distribution cannot be deduced from the convergence of the fourth moment.
