Stephen J. Wills
University College Cork
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Featured researches published by Stephen J. Wills.
Bulletin of The London Mathematical Society | 2001
J. Martin Lindsay; Stephen J. Wills
The quantum stochastic differential equation dk t = k t ∘ θ α β d Λ β α ( t ) is considered on a unital C *-algebra, with separable noise dimension space. Necessary conditions on the matrix of bounded linear maps θ for the existence of a completely positive contractive solution are shown to be sufficient. It is known that for completely positive contraction processes, k satisfies such an equation if and only if k is a regular Markovian cocycle. ‘Feller’ refers to an invariance condition analogous to probabilistic terminology if the algebra is thought of as a non-commutative topological space.
arXiv: Functional Analysis | 2007
J. Martin Lindsay; Stephen J. Wills
A recent characterisation of Fock-adapted contraction operator stochastic cocycles on a Hilbert space, in terms of their associated semigroups, yields a general principle for the construction of such cocycles by approximation of their stochastic generators. This leads to new existence results for quantum stochastic differential equations. We also give necessary and sufficient conditions for a cocycle to satisfy such an equation.
Journal of The London Mathematical Society-second Series | 2003
J. Martin Lindsay; Stephen J. Wills
When a Fock-adapted Feller cocycle on a C*-algebra is regular, completely positive and contractive, it possesses a stochastic generator that is necessarily completely bounded. Necessary and sufficient conditions are given, in the form of a sequence of identities, for a completely bounded map to generate a weakly multiplicative cocycle. These are derived from a product formula for iterated quantum stochastic integrals. Under two alternative assumptions, one of which covers all previously considered cases, the first identity in the sequence is shown to imply the rest.
arXiv: Functional Analysis | 2006
J. Martin Lindsay; Stephen J. Wills
A new method for the construction of Fock-adapted quantum stochastic operator cocycles is outlined, and its use is illustrated by application to a number of examples arising in physics and probability. The construction uses the Trotter-Kato theorem and a recent characterisation of such cocycles in terms of an associated family of contraction semigroups.
Mathematische Annalen | 2001
Debashish Goswami; J. Martin Lindsay; Stephen J. Wills
Abstract. Completely positive Markovian cocycles on a von Neumann algebra, adapted to a Fock filtration, are realised as conjugations of
Proceedings of the Conference | 2003
J. Martin Lindsay; Stephen J. Wills
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Annales De L Institut Henri Poincare-probabilites Et Statistiques | 2015
Alexander C. R. Belton; Stephen J. Wills
-homomorphic Markovian cocycles. The conjugating processes are affiliated to the algebra, and are governed by quantum stochastic differential equations whose coefficients evolve according to the
Journal of Functional Analysis | 2000
J. Martin Lindsay; Stephen J. Wills
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Probability Theory and Related Fields | 2000
J. Martin Lindsay; Stephen J. Wills
-homomorphic process. Some perturbation theory for quantum stochastic flows is developed in order to achieve the above Stinespring decomposition.
Journal of Functional Analysis | 2003
Franco Fagnola; Stephen J. Wills
where σ is the Fock space shift semigroup and s is the map between matrix spaces M(F;A)b and M(F ;A)b (defined below) induced by js. Regularity for the cocycle means that its associated semigroups are norm continuous. If j is completely positive and contractive then it has a CB stochastic generator in the following sense: there is a completely bounded operator θ from A into the matrix space M(k;A)b such that j satisfies the Evans-Hudson equation djt = jt ◦ θ β dΛα(t), in which [θ β ] is the matrix of components of θ with respect to the basis of k used for defining the matrix of quantum stochastic integrators [Λβ ]. Furthermore, if j is ∗-homomorphic then the quantum Ito formula implies that θ satisfies θ(a∗a) = θ(a)∗(a⊗ Ik) + (a ∗ ⊗ Ik)θ(a) + θ(a) (Ih ⊗ P )θ(a), (0.2)