Dark Energy from Violation of Energy Conservation
... modifications of quantum mechanics with a spontaneous stochastic collapse [4]. It has been argued by Penrose [24] that the two apparently different contexts could actually be related in a more fundamental description of quantum gravitational phenomena (for a recent development, see [25]). Finally, t ...
... modifications of quantum mechanics with a spontaneous stochastic collapse [4]. It has been argued by Penrose [24] that the two apparently different contexts could actually be related in a more fundamental description of quantum gravitational phenomena (for a recent development, see [25]). Finally, t ...
Quantum Spacetime without Observers: Ontological
... the space-time metric emerges dynamically when one evolves the canonical variables with respect to multi- ngered time. However, the initial canonical data cannot be chosen arbitrarily, but must obey certain constraints: Only for initial conditions that lie in the submanifold of phase space on which ...
... the space-time metric emerges dynamically when one evolves the canonical variables with respect to multi- ngered time. However, the initial canonical data cannot be chosen arbitrarily, but must obey certain constraints: Only for initial conditions that lie in the submanifold of phase space on which ...
Avoiding Ultraviolet Divergence by Means of Interior–Boundary
... functions that satisfy the IBC. For several models that our collaborators Jonas Lampart, Julian Schmidt, and we have studied, we have been able to prove the self-adjointness of HIBC ; these results ensure that HIBC is free of divergence problems, UV or otherwise. For suitable choice of the IBC, the ...
... functions that satisfy the IBC. For several models that our collaborators Jonas Lampart, Julian Schmidt, and we have studied, we have been able to prove the self-adjointness of HIBC ; these results ensure that HIBC is free of divergence problems, UV or otherwise. For suitable choice of the IBC, the ...
Magnetic-field-induced Anderson localization in a strongly
... presence of an arbitrarily weak disorder. The strongly anisotropic 3D gas (weakly coupled chains with a hierarchy of hopping rates t: t~) can be analyzed in the same way. In this case, the field localizes the electrons in planes or on chains, depending on its direction. Therefore, in the limit of we ...
... presence of an arbitrarily weak disorder. The strongly anisotropic 3D gas (weakly coupled chains with a hierarchy of hopping rates t: t~) can be analyzed in the same way. In this case, the field localizes the electrons in planes or on chains, depending on its direction. Therefore, in the limit of we ...
Wednesday, Mar. 26, 2014
... 3) For finite potentials, the wave function and its derivatives must be continuous. This is required because the second-order derivative term in the wave equation must be single valued. (There are exceptions to this rule when V is infinite.) 4) In order to normalize the wave functions, they must app ...
... 3) For finite potentials, the wave function and its derivatives must be continuous. This is required because the second-order derivative term in the wave equation must be single valued. (There are exceptions to this rule when V is infinite.) 4) In order to normalize the wave functions, they must app ...
The metron model - Max-Planck
... (n > 1) and wave-guide (n = 0) components. In addition, the fields must satisfy appropriate divergence gauge conditions. To lowest (cubic) interaction order, the equations for the first-harmonic constituents (n = 1) reduce to a quasi-linear eigenvalue problem, where q1 = 0, and where e1 consists of ...
... (n > 1) and wave-guide (n = 0) components. In addition, the fields must satisfy appropriate divergence gauge conditions. To lowest (cubic) interaction order, the equations for the first-harmonic constituents (n = 1) reduce to a quasi-linear eigenvalue problem, where q1 = 0, and where e1 consists of ...
The lattice structure of quantum logics
... above ones. We must prove the orthomodularity of !l only. Any of J~f, b, c E 2 split, i. e. there exist pairwise orthogonal elements b 1 , then bi = 0 and b c. such that b = bl V d, c ci V d. Let c E (b~ n Thus 2 is atomistic. Now the orthomodularity of 4 readily follows. D In the second case we als ...
... above ones. We must prove the orthomodularity of !l only. Any of J~f, b, c E 2 split, i. e. there exist pairwise orthogonal elements b 1 , then bi = 0 and b c. such that b = bl V d, c ci V d. Let c E (b~ n Thus 2 is atomistic. Now the orthomodularity of 4 readily follows. D In the second case we als ...
oscillations
... Also find the total energy at that instant. Q.19 > A ball of mass M is dropped on the floor from a height H. It undergoes elastic collision with the floor and again bounces back to the height H. Is the motion Oscillatory. Is it an SHM? In any case, find the time period of the motion of the ball Q.20 ...
... Also find the total energy at that instant. Q.19 > A ball of mass M is dropped on the floor from a height H. It undergoes elastic collision with the floor and again bounces back to the height H. Is the motion Oscillatory. Is it an SHM? In any case, find the time period of the motion of the ball Q.20 ...
The Yrast Spectra of Weakly Interacting Bose
... The properties of the non-zero angular momentum states of Bose-condensates of atoms in external traps have been addressed in several recent publications [1]. Special interest attaches to the lowest energy quantum states with a given angular momentum. Borrowing from nuclear physics terminology we sha ...
... The properties of the non-zero angular momentum states of Bose-condensates of atoms in external traps have been addressed in several recent publications [1]. Special interest attaches to the lowest energy quantum states with a given angular momentum. Borrowing from nuclear physics terminology we sha ...
PRACTICE Trig Word Problems
... 1. Write the trigonometric equation for the function with a period of 6. The function has a maximum of 3 at x = 2 and a low point of –1. 2. Write the trigonometric equation for the function with a period of 5, a low point of – 3 at x=1 and an amplitude of 7. 3. Ruby has a pulse rate of 73 beats per ...
... 1. Write the trigonometric equation for the function with a period of 6. The function has a maximum of 3 at x = 2 and a low point of –1. 2. Write the trigonometric equation for the function with a period of 5, a low point of – 3 at x=1 and an amplitude of 7. 3. Ruby has a pulse rate of 73 beats per ...
