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We introduce a useful and rather simple classes of BKP tau functions which which we shall shall call easy tau functions. We consider the large BKP hiearchy related to $O(2infty +1)$ which was introduced in cite{KvdLbispec} (which is closely related to the DKP $O(2infty) $hierarchy introduced in cite{JM}). Actually easy tau functions of the small BKP was already considered in cite{HLO}, here we are more interested in the large BKP and also the mixed small-large BKP tau functions cite{KvdLbispec}. Tau functions under consideration are equal to sums over partitions and to multi-integrals. In this way they may be appliciable in models of random partitions and models of random matrices. Here in the part II we consider multi-intergals and series of $N$-ply integrals in $N$. Relations to matrix models is explained. This paper may be viewed as a developement of the the paper by J.van de Leur cite{L1} related to orthogonal and symplectic ensembles of random matrices.
Designing shared neural architecture plays an important role in multi-task learning. The challenge is that finding an optimal sharing scheme heavily relies on the expert knowledge and is not scalable to a large number of diverse tasks. Inspired by th
It is shown that the hodograph solutions of the dispersionless coupled KdV (dcKdV) hierarchies describe critical and degenerate critical points of a scalar function which obeys the Euler-Poisson-Darboux equation. Singular sectors of each dcKdV hierar
In this paper we investigate integrable models from the perspective of information theory, exhibiting various connections. We begin by showing that compressible hydrodynamics for a one-dimesional isentropic fluid, with an appropriately motivated info
The paper begins with a review of the well known Novikovs equations and corresponding finite KdV hierarchies. For a positive integer $N$ we give an explicit description of the $N$-th Novikovs equation and its first integrals. Its finite KdV hierarchy
We consider systems of ordinary differential equations (ODEs) of the form ${cal B}{mathbf K}=0$, where $cal B$ is a Hamiltonian operator of a completely integrable partial differential equation (PDE) hierarchy, and ${mathbf K}=(K,L)^T$. Such systems,