A proof that measured data and equations of quantum mechanics
... time intervals a detection result, consisting of 0 (for no detection) or 1 (for detection), so a record contains LK bits. Depending on judgments made about correlations from time interval to time interval and detector to detector, these LK bits may constitute LK quantum outcomes, or one quantum outc ...
... time intervals a detection result, consisting of 0 (for no detection) or 1 (for detection), so a record contains LK bits. Depending on judgments made about correlations from time interval to time interval and detector to detector, these LK bits may constitute LK quantum outcomes, or one quantum outc ...
The Uncertainty Principle
... where ℏ = h/2π, h denotes Planck's constant, and boldface type is used to represent matrices. The new theory scored spectacular empirical success by encompassing nearly all spectroscopic data known at the time, especially after the concept of the electron spin was included in the theoretical framewo ...
... where ℏ = h/2π, h denotes Planck's constant, and boldface type is used to represent matrices. The new theory scored spectacular empirical success by encompassing nearly all spectroscopic data known at the time, especially after the concept of the electron spin was included in the theoretical framewo ...
Renormalization
... One might be tempted to conclude from this that a phenomenological description is simply not possible beyond the delta function approximation. After all, if the underlying theory is known, one can always compute the corrections without any approximation, and it might be argued that the inconsistenci ...
... One might be tempted to conclude from this that a phenomenological description is simply not possible beyond the delta function approximation. After all, if the underlying theory is known, one can always compute the corrections without any approximation, and it might be argued that the inconsistenci ...
Conformal field theory for inhomogeneous one
... taken to be constant throughout the system. However, in many experimental contexts, such as quantum gases in trapping potentials and in several out-of-equilibrium situations, systems are strongly inhomogeneous. We show here that the powerful CFT methods can be extended to deal with such 1D situation ...
... taken to be constant throughout the system. However, in many experimental contexts, such as quantum gases in trapping potentials and in several out-of-equilibrium situations, systems are strongly inhomogeneous. We show here that the powerful CFT methods can be extended to deal with such 1D situation ...
Quantum Computation with Molecular Nanomagnets
... The key point here is that it is demonstrated that any unitary operation on n-qubits can be implemented by a sequence of single-qubit and CNOT gates. Equivalent universality can be proved with other sets of elementary operations of one- and two-qubit gates [1]. This is an important result that sugge ...
... The key point here is that it is demonstrated that any unitary operation on n-qubits can be implemented by a sequence of single-qubit and CNOT gates. Equivalent universality can be proved with other sets of elementary operations of one- and two-qubit gates [1]. This is an important result that sugge ...
Fast Equivalence-checking for Quantum Circuits
... Quantum circuits often operate on quantum states that contain exponentially large superpositions, making quantum simulation, as well as circuit design and analysis on conventional computers very challenging. To this end, a layered software architecture for quantum computing design tools was outlined ...
... Quantum circuits often operate on quantum states that contain exponentially large superpositions, making quantum simulation, as well as circuit design and analysis on conventional computers very challenging. To this end, a layered software architecture for quantum computing design tools was outlined ...
Quantum Mechanics as Quantum Information
... Our foremost task should be to go to each and every axiom of quantum theory and give it an information theoretic justification if we can. Only when we are finished picking off all the terms (or combinations of terms) that can be interpreted as subjective information will we be in a position to make ...
... Our foremost task should be to go to each and every axiom of quantum theory and give it an information theoretic justification if we can. Only when we are finished picking off all the terms (or combinations of terms) that can be interpreted as subjective information will we be in a position to make ...
Introduction to ”Topological Geometrodynamics: an Overview
... time of about half decade [K1]. The basic vision and its relationship to existing theories is now rather well understood. 1. Space-times are representable as 4-surfaces in the 8-dimensional imbedding space H = M 4 × CP2 , where M 4 is 4-dimensional (4-D) Minkowski space and CP2 is 4-D complex projec ...
... time of about half decade [K1]. The basic vision and its relationship to existing theories is now rather well understood. 1. Space-times are representable as 4-surfaces in the 8-dimensional imbedding space H = M 4 × CP2 , where M 4 is 4-dimensional (4-D) Minkowski space and CP2 is 4-D complex projec ...
Holographic quantum error-correcting code
... 2n-perfectway state rs at di↵erent length scales in a-- scale so into that four SA /subsets log(L) A, where L D. pairs may be possible by using tensors w length of A. Such distributionsB,ofC,EPR D e structures or placing the so-called disentanglers at each layer of a MERA circu However such simple c ...
... 2n-perfectway state rs at di↵erent length scales in a-- scale so into that four SA /subsets log(L) A, where L D. pairs may be possible by using tensors w length of A. Such distributionsB,ofC,EPR D e structures or placing the so-called disentanglers at each layer of a MERA circu However such simple c ...