Quantum Strategies V 82, N 5
... U1 , U3 , and F is. Since U3 U2 U1 jHl cannot equal both jHl and jT l, at least one of the players can improve his expected payoff by changing his strategy while the other does not. Thus sfU2 g, fU1 , U3 gd cannot be an equilibrium, for any U1 , U2 , U3 , so PQ penny flipover has no (quantum, quantu ...
... U1 , U3 , and F is. Since U3 U2 U1 jHl cannot equal both jHl and jT l, at least one of the players can improve his expected payoff by changing his strategy while the other does not. Thus sfU2 g, fU1 , U3 gd cannot be an equilibrium, for any U1 , U2 , U3 , so PQ penny flipover has no (quantum, quantu ...
Mixed, pure, and entangled quantum states. Density matrix
... Göran Johansson, Thilo Bauch, Jonas Bylander Chalmers, MC2 September 24, 2013 The density operator or density matrix is a more general way of describing the state of a quantum system than that provided by the wave function or state vector. It allows us to describe situations where the state vector ...
... Göran Johansson, Thilo Bauch, Jonas Bylander Chalmers, MC2 September 24, 2013 The density operator or density matrix is a more general way of describing the state of a quantum system than that provided by the wave function or state vector. It allows us to describe situations where the state vector ...
Bounding the quantum dimension with contextuality Linköping University Post Print
... measurement a sequence. This difference to the standard version does not matter at this point (since the observables in any row or column commute), but it will become important below. The PM inequality is of special interest for our program since it is violated up to the algebraic maximum with four- ...
... measurement a sequence. This difference to the standard version does not matter at this point (since the observables in any row or column commute), but it will become important below. The PM inequality is of special interest for our program since it is violated up to the algebraic maximum with four- ...
Available PDF download
... assigns to any oriented edge e in M an element Ā(e) of SU(2) (a ‘holonomy’) such that Ā(e−1 ) = [Ā(e)]−1 ; and, if the end point of e1 is the starting point of e2 , then Ā(e1 ◦ e2 ) = Ā(e1 ) · Ā(e2 ). Clearly, every smooth connection A is a generalized connection. In fact, the space A of smoot ...
... assigns to any oriented edge e in M an element Ā(e) of SU(2) (a ‘holonomy’) such that Ā(e−1 ) = [Ā(e)]−1 ; and, if the end point of e1 is the starting point of e2 , then Ā(e1 ◦ e2 ) = Ā(e1 ) · Ā(e2 ). Clearly, every smooth connection A is a generalized connection. In fact, the space A of smoot ...
- Philsci
... unresolvable and a species of “twentieth century medieval metaphysics” from which it is best to abstain. He sides with Reichenbach in maintaining that the ontology we adopt, be it of objects, events, or whatever, rests on convenience, convention or superfluous metaphysics, and that science itself fo ...
... unresolvable and a species of “twentieth century medieval metaphysics” from which it is best to abstain. He sides with Reichenbach in maintaining that the ontology we adopt, be it of objects, events, or whatever, rests on convenience, convention or superfluous metaphysics, and that science itself fo ...
1203.3054v2
... We conclude with a discussion on possible applications of our results and implications for generalizing quantum mechanics by introducing nonlinear time evolution laws for pure states. ...
... We conclude with a discussion on possible applications of our results and implications for generalizing quantum mechanics by introducing nonlinear time evolution laws for pure states. ...
here
... Ak j are the components of A in this basis, they may be written as entries in a matrix, with Ak j occupying the slot in the kth row and jth column. The vector that makes up the first column Ak1 is the ‘image’ of e1 (i.e. coefficients in the linear combination appearing in A|e1 i), the second column ...
... Ak j are the components of A in this basis, they may be written as entries in a matrix, with Ak j occupying the slot in the kth row and jth column. The vector that makes up the first column Ak1 is the ‘image’ of e1 (i.e. coefficients in the linear combination appearing in A|e1 i), the second column ...
Quantum Manipulation of Ultracold Atoms and Photons
... (magnon), that can be mapped onto a photon with high efficiency [8,9]. In such a system we have recently demonstrated phase-coherent transfer of a single magnon from one ensemble to another via an optical resonator serving as a quantum bus that in the ideal case is only virtually populated [10]. Par ...
... (magnon), that can be mapped onto a photon with high efficiency [8,9]. In such a system we have recently demonstrated phase-coherent transfer of a single magnon from one ensemble to another via an optical resonator serving as a quantum bus that in the ideal case is only virtually populated [10]. Par ...
