On the Motion of Solids in Modified Quantum Mechanics.
... presence of the 3 independent spatial directions. The numeric values correspond to N m = 1g. The expectation values ( 0 )and ( P ) move along classical trajectories apart from a certain stochastic spread around them. This anomalous Brownian motion of the centre-ofmass is, however, completely unobser ...
... presence of the 3 independent spatial directions. The numeric values correspond to N m = 1g. The expectation values ( 0 )and ( P ) move along classical trajectories apart from a certain stochastic spread around them. This anomalous Brownian motion of the centre-ofmass is, however, completely unobser ...
Chapter_9 - Experimental Elementary Particle Physics Group
... However, the fact that a set of points possesses a non-positive-definite line element does not imply that the set degenerates into a featureless point (which is fortunate, considering that the spacetime we inhabit is characterized by just such a line element). It simply implies that we need to apply ...
... However, the fact that a set of points possesses a non-positive-definite line element does not imply that the set degenerates into a featureless point (which is fortunate, considering that the spacetime we inhabit is characterized by just such a line element). It simply implies that we need to apply ...
Lokal fulltext - Chalmers tekniska högskola
... the best of worlds, the results will agree with one another, and if they do not, it forces theory (if the measurement is correct) to change, expanding the scientific knowledge of humanity. In some cases, the distance between theory and experiments is too vast to be overcome in the near future. For e ...
... the best of worlds, the results will agree with one another, and if they do not, it forces theory (if the measurement is correct) to change, expanding the scientific knowledge of humanity. In some cases, the distance between theory and experiments is too vast to be overcome in the near future. For e ...
The Semiclassical Electron in a Magnetic Field and Lattice. Some
... (1) isolated point (a critical point of our foliation), (2) closed curve in R3 (a curve homotopic to zero in T 3 ), (3) periodic nonclosed curve in R3 (a curve, closed in T 3 , but nonhomotopic to zero), (4) nonperiodic nonclosed curve in R3 (such a curve in T 3 has a closure which is generically 2- ...
... (1) isolated point (a critical point of our foliation), (2) closed curve in R3 (a curve homotopic to zero in T 3 ), (3) periodic nonclosed curve in R3 (a curve, closed in T 3 , but nonhomotopic to zero), (4) nonperiodic nonclosed curve in R3 (such a curve in T 3 has a closure which is generically 2- ...
Plentiful Nothingness: The Void in Modern Art and Modern Science
... Yakov Zeldovich (1967): Virtual particles bubbling out of the vacuum of quantum field theory contribute to the cosmological constant Λ • zero-point energy of a harmonic oscillator (vacuum = ground state) E= ...
... Yakov Zeldovich (1967): Virtual particles bubbling out of the vacuum of quantum field theory contribute to the cosmological constant Λ • zero-point energy of a harmonic oscillator (vacuum = ground state) E= ...
Pseudoholomorphic Curves and Mirror Symmetry
... by string theories. This helps to address one major difficulty in string theory — the fact that the theory cannot single out a unique manifold to model the “real world”. If different manifolds give rise to the same physics, then this should not be too much of a concern. Having been first proposed by ...
... by string theories. This helps to address one major difficulty in string theory — the fact that the theory cannot single out a unique manifold to model the “real world”. If different manifolds give rise to the same physics, then this should not be too much of a concern. Having been first proposed by ...
The British Journal for the Philosophy of Science
... as ' disturbance of phenomena by observation ', Le. against the use of the concept of vexed nature. The reason is plain : such phrases imply the assertion of the objective existence of a reality hidden, for the time being, behind the appearances ; of a nature Hbera existing while we are not acting u ...
... as ' disturbance of phenomena by observation ', Le. against the use of the concept of vexed nature. The reason is plain : such phrases imply the assertion of the objective existence of a reality hidden, for the time being, behind the appearances ; of a nature Hbera existing while we are not acting u ...
- Philsci
... field to create a radiative process that transfers energy from an emitter to an absorber. As noted in Cramer (1986), the original version of the Transactional Interpretation (TI) already has basic compatibility with relativity in virtue of the fact that the realization of a transaction occurs with r ...
... field to create a radiative process that transfers energy from an emitter to an absorber. As noted in Cramer (1986), the original version of the Transactional Interpretation (TI) already has basic compatibility with relativity in virtue of the fact that the realization of a transaction occurs with r ...
... Closed-orbit theory is a semiclassical method for calculating photoabsorption cross sections. This method is based on the observation that to calculate this cross section it is only necessary to obtain the Green’s function for points near the nucleus when the initial state is compact. Thus in a semi ...
Compactness and Symmetry in Quantum Logic 1 Introduction
... H and T , the other with faces h and t. Let E be the experiment of flipping the first coin, so that E = {H, T }; let F be the experiment of flipping the second coin, so that F = {h, t}. We have then a very simple semi-classical test space with X = {H, T, h, t} and A = {E, F } = {{H, T }, {h, t}}. We ...
... H and T , the other with faces h and t. Let E be the experiment of flipping the first coin, so that E = {H, T }; let F be the experiment of flipping the second coin, so that F = {h, t}. We have then a very simple semi-classical test space with X = {H, T, h, t} and A = {E, F } = {{H, T }, {h, t}}. We ...
STRONG-FIELD PHENOMENA IN ATOMS QUASICLASSICAL
... functions X J± can be considered as a product of two factors. The first of them includes the pre-exponential factor and the first exponent on the right-hand side of Eq. (6). This part reminds closely the field-free quasiclassical wave functions [1]. On the other hand, the second exponent on the righ ...
... functions X J± can be considered as a product of two factors. The first of them includes the pre-exponential factor and the first exponent on the right-hand side of Eq. (6). This part reminds closely the field-free quasiclassical wave functions [1]. On the other hand, the second exponent on the righ ...
Structure, Individuality and Quantum Gravity
... other physical events in a general-relativistic theory of matter and/or nongravitational fields. This is the purport of the “hole argument” (see [54] and earlier references therein). The points of space-time have quiddity as such, but only gain haecceity (to the extent that they do) from the propert ...
... other physical events in a general-relativistic theory of matter and/or nongravitational fields. This is the purport of the “hole argument” (see [54] and earlier references therein). The points of space-time have quiddity as such, but only gain haecceity (to the extent that they do) from the propert ...
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... strings take on different properties depending on their modes of vibration, just as the strings of a violin produce different notes depending on how they are played. To string theorists, the whole universe is a boisterous symphony performed upon these strings. It’s a lovely idea. Lovelier yet, strin ...
... strings take on different properties depending on their modes of vibration, just as the strings of a violin produce different notes depending on how they are played. To string theorists, the whole universe is a boisterous symphony performed upon these strings. It’s a lovely idea. Lovelier yet, strin ...
