Quantum Probabilistic Dyadic Second-Order Logic⋆
... the set of states ΣH to the set of set of states ΣH0 , given by A(|ψi) for every |ψi ∈ H. An action is any such function A : H → H0 induced on state spaces by some linear map A : ΣH → ΣH0 . We can also define composition, tensor product and adjoint of actions in a natural way via composition, tensor ...
... the set of states ΣH to the set of set of states ΣH0 , given by A(|ψi) for every |ψi ∈ H. An action is any such function A : H → H0 induced on state spaces by some linear map A : ΣH → ΣH0 . We can also define composition, tensor product and adjoint of actions in a natural way via composition, tensor ...
Synchronistic Phenomena as Entanglement
... ‘meaningful coincidences’, correlations not produced by causal interaction of the kind physicists know and apply successfully but mediated by correspondences of sense and meaning. In fact, it is a common feature of paranormal phenomena that they are prima facie disturbing, unfitting, unlikely incide ...
... ‘meaningful coincidences’, correlations not produced by causal interaction of the kind physicists know and apply successfully but mediated by correspondences of sense and meaning. In fact, it is a common feature of paranormal phenomena that they are prima facie disturbing, unfitting, unlikely incide ...
Complete Axiomatizations for Quantum Actions
... (the ones satisfying the property). Our axiomatization in terms of quantum frames extends the older work on relational semantics for orthologic (based on orthoframes2 ) to the full (orthomodular) quantum logic, and beyond. One of the main problems of orthoframes (as shown in [15]) was that orthomodu ...
... (the ones satisfying the property). Our axiomatization in terms of quantum frames extends the older work on relational semantics for orthologic (based on orthoframes2 ) to the full (orthomodular) quantum logic, and beyond. One of the main problems of orthoframes (as shown in [15]) was that orthomodu ...
- Natural Sciences Publishing
... which corresponds to the absolute value of the sum of negative eigenvalues of ρ̂ TA [38] , and which vanishes for unentangled states, N(ρ ) does not increase under local operations and classical communications (LOCC), i.e., it is an entanglement monotone [39], and as such it can be used to quantify ...
... which corresponds to the absolute value of the sum of negative eigenvalues of ρ̂ TA [38] , and which vanishes for unentangled states, N(ρ ) does not increase under local operations and classical communications (LOCC), i.e., it is an entanglement monotone [39], and as such it can be used to quantify ...
Unitary quantum theory as a formal framework for a
... below, its identification with the recordable time of human experience is an interpretative assumption. As noted by physicists from Schrödinger onward, unitary time evolution turns any separable physical state |U> = |A> |B> into an entangled state |U> = |A B>, where “entangled” simply means “not ...
... below, its identification with the recordable time of human experience is an interpretative assumption. As noted by physicists from Schrödinger onward, unitary time evolution turns any separable physical state |U> = |A> |B> into an entangled state |U> = |A B>, where “entangled” simply means “not ...
Square-root measurement for quantum
... As mentioned earlier, a signal detector is described by a POVM. It is, however, difficult to obtain a closed-form analytical expression of the optimal POVM directly from the necessary and sufficient conditions of Bayes strategy in general. Fortunately, we can take an alternative approach, that is, w ...
... As mentioned earlier, a signal detector is described by a POVM. It is, however, difficult to obtain a closed-form analytical expression of the optimal POVM directly from the necessary and sufficient conditions of Bayes strategy in general. Fortunately, we can take an alternative approach, that is, w ...
