Quantum-like model of unconscious–conscious dynamics
... and instruments. We illustrate our approach with the model of bistable perception of a particular ambiguous figure, the Schröder stair. This is a concrete model for unconscious and conscious processing of information and their interaction. The starting point of our quantum-like journey was the obser ...
... and instruments. We illustrate our approach with the model of bistable perception of a particular ambiguous figure, the Schröder stair. This is a concrete model for unconscious and conscious processing of information and their interaction. The starting point of our quantum-like journey was the obser ...
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... In this paper, we also consider the issue of causality at the Planck scale in the framework of causal sets, although our results do not promote this aspect as decisively as in [12]. In our opinion, the very concept of causality makes sense in the quasi-classical limit, in relation with the fact that ...
... In this paper, we also consider the issue of causality at the Planck scale in the framework of causal sets, although our results do not promote this aspect as decisively as in [12]. In our opinion, the very concept of causality makes sense in the quasi-classical limit, in relation with the fact that ...
Characterizing the Performance Effect of Trials and Rotations in
... of single-qubit rotations that can be done on a Bloch sphere, but we can implement a finite subset on a physical computer. A major cost in some of the QPE approaches arises when algorithms must decompose arbitary rotations—especially precise small rotations—into a sequence of physical operations. De ...
... of single-qubit rotations that can be done on a Bloch sphere, but we can implement a finite subset on a physical computer. A major cost in some of the QPE approaches arises when algorithms must decompose arbitary rotations—especially precise small rotations—into a sequence of physical operations. De ...
... an expression which is easily amenable to a probabilistic interpretation.We consider CN endowed with the already mentioned inner product 〈X, Y〉J = Y*JX, for any X ,Y ∈ CN, and respective J-norm ∥X∥J = X*JX. The matrix A + B gives the possible dynamical states of each bosonic particle. Some considera ...
Detected-jump-error-correcting quantum codes - IAP TU
... For some special cases it is also possible to design a passive error-correcting quantum code 关8 –10兴. Such a passive quantum code relies on a subspace of the Hilbert space which is not affected by any errors at all. In this situation the unitary recovery operation is the identity operation so that a ...
... For some special cases it is also possible to design a passive error-correcting quantum code 关8 –10兴. Such a passive quantum code relies on a subspace of the Hilbert space which is not affected by any errors at all. In this situation the unitary recovery operation is the identity operation so that a ...
Introductory Quantum Optics Section 1. Single photon physics
... Here ω denotes the frequency and k denotes the wave vector of the photon. In the following, we discuss the generation of entanglement and look at recent linear optics experiments with single photons. These experiments were designed to test the foundations of quantum mechanics or aim at finding imple ...
... Here ω denotes the frequency and k denotes the wave vector of the photon. In the following, we discuss the generation of entanglement and look at recent linear optics experiments with single photons. These experiments were designed to test the foundations of quantum mechanics or aim at finding imple ...
Heisenberg`s original derivation of the uncertainty principle and its
... The problem of mathematically characterizing all the physically realizable quantum measurements is reduced to the problem as to which instruments are physically realizable13. To settle this problem, standard models of measuring processes were introduced in ref. 16 as follows. A measuring process for ...
... The problem of mathematically characterizing all the physically realizable quantum measurements is reduced to the problem as to which instruments are physically realizable13. To settle this problem, standard models of measuring processes were introduced in ref. 16 as follows. A measuring process for ...
Phys. Rev. Lett. 98, 070602
... heat bath to the kinetic energy does not destroy such a phase. However, for strong dissipation the gap becomes very small, and the topological phase may be too delicate to observe or use at reasonable temperatures. If the heat bath is coupled to the classical state of each plaquette, the topological ...
... heat bath to the kinetic energy does not destroy such a phase. However, for strong dissipation the gap becomes very small, and the topological phase may be too delicate to observe or use at reasonable temperatures. If the heat bath is coupled to the classical state of each plaquette, the topological ...
Lower Bounds for Quantum Search and Derandomization
... Here αk is a complex number, called the amplitude of state |ki. If we observe |φi we will see one and only one |ki. The probability of seeing one specific |ki is given by |αk |2 . Hence we must have P ...
... Here αk is a complex number, called the amplitude of state |ki. If we observe |φi we will see one and only one |ki. The probability of seeing one specific |ki is given by |αk |2 . Hence we must have P ...
Experimental quantum teleportation articles
... reappearing at some distant location. An object to be teleported can be fully characterized by its properties, which in classical physics can be determined by measurement. To make a copy of that object at a distant location one does not need the original parts and pieces— all that is needed is to se ...
... reappearing at some distant location. An object to be teleported can be fully characterized by its properties, which in classical physics can be determined by measurement. To make a copy of that object at a distant location one does not need the original parts and pieces— all that is needed is to se ...
