
Quantum gravity without gravitons in a superfluid quantum space.
... justify the compression of space's quanta (ς ) into virtual photons (γς ) within the absorptionemission mechanism. On the right the possible mechanism corresponding to spin½, where the system returns in the same state after a rotation of 720° in the toroidal direction σ1 , while each space's quantum ...
... justify the compression of space's quanta (ς ) into virtual photons (γς ) within the absorptionemission mechanism. On the right the possible mechanism corresponding to spin½, where the system returns in the same state after a rotation of 720° in the toroidal direction σ1 , while each space's quantum ...
Full Text
... Schrödinger equation, the uncertainty principle, and the Pauli Exclusion Principle. Almost all the test questions include visualizations. The QPVI consists of 25 questions and a student selects the correct response of given five choices. In addition, a student is asked to explain his/her answers wit ...
... Schrödinger equation, the uncertainty principle, and the Pauli Exclusion Principle. Almost all the test questions include visualizations. The QPVI consists of 25 questions and a student selects the correct response of given five choices. In addition, a student is asked to explain his/her answers wit ...
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... This approach unified with special relativity is the modem quantum field theory. So we still have a space-time framework in which fields evolve (by some wave equation); these fields interact with our instrument of measure exchanging energy in a discrete way. The vectors for this energy exchange are ...
... This approach unified with special relativity is the modem quantum field theory. So we still have a space-time framework in which fields evolve (by some wave equation); these fields interact with our instrument of measure exchanging energy in a discrete way. The vectors for this energy exchange are ...
Quantum error correction
... the possible states are exactly the same as the ones in table 2. Further steps are the same as the ones from bit–flip correction. If the rate of error without error correction is p than after error correction the error is of order p2 . The circuit of the error correcting code is shown in figure 4. U ...
... the possible states are exactly the same as the ones in table 2. Further steps are the same as the ones from bit–flip correction. If the rate of error without error correction is p than after error correction the error is of order p2 . The circuit of the error correcting code is shown in figure 4. U ...
W. Pauli - Fisica Fundamental
... circumstances which are closely connected with the regularities of the complex structure of spectra. For instance, the ground state of the alkaline earths in which the two valence electrons are equivalent corresponds to a singlet S-term, while in those stationary states of the atom which belong to t ...
... circumstances which are closely connected with the regularities of the complex structure of spectra. For instance, the ground state of the alkaline earths in which the two valence electrons are equivalent corresponds to a singlet S-term, while in those stationary states of the atom which belong to t ...
Quantum networks with trapped ions
... angle. The coherent transfer of quantum information requires a particular optical mode to be selected as the photonic qubit, and coupling of the material qubit to all other modes must be suppressed. In the deterministic approach, this selection is achieved through a highquality cavity which enhances ...
... angle. The coherent transfer of quantum information requires a particular optical mode to be selected as the photonic qubit, and coupling of the material qubit to all other modes must be suppressed. In the deterministic approach, this selection is achieved through a highquality cavity which enhances ...
Introduction to Quantum Information
... key idea was that probabilities depend on what you know; if we acquire additional information then this modifies the probabilities. Today such reasoning is uncontentious and forms part of the prevailing paradigm in much of probability theory (Jeffreys, 1939; Box and Tiao 1973; Bretthorst 1988; Lee 1 ...
... key idea was that probabilities depend on what you know; if we acquire additional information then this modifies the probabilities. Today such reasoning is uncontentious and forms part of the prevailing paradigm in much of probability theory (Jeffreys, 1939; Box and Tiao 1973; Bretthorst 1988; Lee 1 ...
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... new interesting questions arise now due to the good tunability of the experiments with optical lattices. In particular, it becomes possible to study time-dependent processes such as driven quantum phase transitions [1]. A theoretical understanding of such phenomena is challenging, since the characte ...
... new interesting questions arise now due to the good tunability of the experiments with optical lattices. In particular, it becomes possible to study time-dependent processes such as driven quantum phase transitions [1]. A theoretical understanding of such phenomena is challenging, since the characte ...
A Landau-Ginzburg model, flat coordinates and a mirror theorem for
... isomorphic to QA : the fonction F (the Landau-Ginzburg model) yields a mirror partner of the small quantum cohomology F2 . The explicit construction of the quantum differential system QB associated with the LandauGinzburg model of F2 is interesting for several reasons: • first, it brings to light so ...
... isomorphic to QA : the fonction F (the Landau-Ginzburg model) yields a mirror partner of the small quantum cohomology F2 . The explicit construction of the quantum differential system QB associated with the LandauGinzburg model of F2 is interesting for several reasons: • first, it brings to light so ...
Quantum computing
Quantum computing studies theoretical computation systems (quantum computers) that make direct use of quantum-mechanical phenomena, such as superposition and entanglement, to perform operations on data. Quantum computers are different from digital computers based on transistors. Whereas digital computers require data to be encoded into binary digits (bits), each of which is always in one of two definite states (0 or 1), quantum computation uses quantum bits (qubits), which can be in superpositions of states. A quantum Turing machine is a theoretical model of such a computer, and is also known as the universal quantum computer. Quantum computers share theoretical similarities with non-deterministic and probabilistic computers. The field of quantum computing was initiated by the work of Yuri Manin in 1980, Richard Feynman in 1982, and David Deutsch in 1985. A quantum computer with spins as quantum bits was also formulated for use as a quantum space–time in 1968.As of 2015, the development of actual quantum computers is still in its infancy, but experiments have been carried out in which quantum computational operations were executed on a very small number of quantum bits. Both practical and theoretical research continues, and many national governments and military agencies are funding quantum computing research in an effort to develop quantum computers for civilian, business, trade, and national security purposes, such as cryptanalysis.Large-scale quantum computers will be able to solve certain problems much more quickly than any classical computers that use even the best currently known algorithms, like integer factorization using Shor's algorithm or the simulation of quantum many-body systems. There exist quantum algorithms, such as Simon's algorithm, that run faster than any possible probabilistic classical algorithm.Given sufficient computational resources, however, a classical computer could be made to simulate any quantum algorithm, as quantum computation does not violate the Church–Turing thesis.