Abstract
In this paper, we first introduce and study the quantum (K-1, K-2)-Gross Laplacian denoted Delta(QG)(K-1, K-2). Then, we prove that Delta(QG)(K-1, K-2) is a well defined and linear continuous operator acting on the space of continuous operators and has a quantum stochastic integral. Finally, we give an explicit solution of the quantum heat equation associated with Delta(QG)(K-1, K-2). Then, under some positive conditions, we give an integral representation of this solution.