Baryons in O (4) and Vibron Model
... states which can be removed by means of the two auxiliary conditions ∂ µ1 Ψµ1 ...µK = 0, and γ µ1 Ψµ1 ...µK = 0. That these conditions do not serve the above purpose, was demonstrated in Ref. [5]. There, the first auxiliary condition was shown to solely test consistency with the mass-shell relation ...
... states which can be removed by means of the two auxiliary conditions ∂ µ1 Ψµ1 ...µK = 0, and γ µ1 Ψµ1 ...µK = 0. That these conditions do not serve the above purpose, was demonstrated in Ref. [5]. There, the first auxiliary condition was shown to solely test consistency with the mass-shell relation ...
Analogue gravity from field theory normal modes?
... that if the Lagrangian contains non-trivial second derivatives you should not be too surprised to see terms beyond the d’Alembertian showing up in the linearized equations of motion. Specific examples of this in special cases are already known: for example, this happens in the acoustic geometry when ...
... that if the Lagrangian contains non-trivial second derivatives you should not be too surprised to see terms beyond the d’Alembertian showing up in the linearized equations of motion. Specific examples of this in special cases are already known: for example, this happens in the acoustic geometry when ...
algunos resultados asociados a problemas
... particle disappears upon reaching a wall and then appears at the other end must be considered. This type of movement (which is very unusual because the particle is not actually trapped between the two walls) corresponds to that of a quantum particle described by the Hamiltonian operator under period ...
... particle disappears upon reaching a wall and then appears at the other end must be considered. This type of movement (which is very unusual because the particle is not actually trapped between the two walls) corresponds to that of a quantum particle described by the Hamiltonian operator under period ...
A Note on Shor`s Quantum Algorithm for Prime Factorization
... algorithm for finding the order r of an element x (mod n) instead of giving a quantum computer algorithm for factoring n directly. The indirect algorithm is feasible because factorization can be reduced to finding the order of an element by using randomization[2]. We now briefly give this reduction. ...
... algorithm for finding the order r of an element x (mod n) instead of giving a quantum computer algorithm for factoring n directly. The indirect algorithm is feasible because factorization can be reduced to finding the order of an element by using randomization[2]. We now briefly give this reduction. ...
Nature of the cosmic ray power law exponents
... have computed power law indices for bosons and fermions in very good agreement with data. • A second order phase transition is shown to occur leading to the observed knee in the spectrum and the estimate of the cross-over energy is satisfactory. • Our prediction of the critical index for electron/fe ...
... have computed power law indices for bosons and fermions in very good agreement with data. • A second order phase transition is shown to occur leading to the observed knee in the spectrum and the estimate of the cross-over energy is satisfactory. • Our prediction of the critical index for electron/fe ...
THE HVZ THEOREM FOR N
... of the discrete Schrödinger operators under very weak assumptions on the behavior of magnetic and electric potentials at infinity. For the discrete Schrödinger operators, associated with the Hamiltonians of systems of three quantum particles moving on lattice interacting via zerorange attractive p ...
... of the discrete Schrödinger operators under very weak assumptions on the behavior of magnetic and electric potentials at infinity. For the discrete Schrödinger operators, associated with the Hamiltonians of systems of three quantum particles moving on lattice interacting via zerorange attractive p ...
Heuristic Optimisation in Design and Analysis
... but other schemes are possible. We need to create photons that with an electric field oscillating in the desired magnetic plane. One way to do this is by passing light through an appropriate ...
... but other schemes are possible. We need to create photons that with an electric field oscillating in the desired magnetic plane. One way to do this is by passing light through an appropriate ...
Homework No. 07 (Spring 2015) PHYS 530A: Quantum Mechanics II
... Table 1: Isospin assignments for particles. ...
... Table 1: Isospin assignments for particles. ...
Full text in PDF - ndl nano
... the grid. Here N i denotes a number of nodes in the i direction. The finite-difference equations were obtained using Euler-Lagrange equations from the discretized Lagrangian of the system, which ensured the Hermiticity of the corresponding matrix constructed on bonds with material parameters determi ...
... the grid. Here N i denotes a number of nodes in the i direction. The finite-difference equations were obtained using Euler-Lagrange equations from the discretized Lagrangian of the system, which ensured the Hermiticity of the corresponding matrix constructed on bonds with material parameters determi ...
Evolution without evolution, and without ambiguities
... classical dynamics, there is no need to assume any underlying motion: both time and motion are explained in terms of motionless entanglement contained in the state of the universe. This elegant model leading to an “evolution without evolution” [5] has promising features, such as its compatibility wi ...
... classical dynamics, there is no need to assume any underlying motion: both time and motion are explained in terms of motionless entanglement contained in the state of the universe. This elegant model leading to an “evolution without evolution” [5] has promising features, such as its compatibility wi ...
Representations of Lorentz and Poincaré groups
... better suited for a relativistic theory) can be represented by a group of unitary8 symmetry operators acting on the Hilbert state space. Correspondingly, the algebra of infinitesimal generators (in the case of a continuous symmetry) is represented by an algebra of Hermitian operators. In the case of ...
... better suited for a relativistic theory) can be represented by a group of unitary8 symmetry operators acting on the Hilbert state space. Correspondingly, the algebra of infinitesimal generators (in the case of a continuous symmetry) is represented by an algebra of Hermitian operators. In the case of ...
Posterior distributions on certain parameter spaces obtained by using group theoretic methods adopted from quantum physics
... For example, the rotation group in three-dimensional Euclidean space is not transitive. A point on a given sphere cannot be changed to a point on a sphere of a different radius by a rotation. However, the unit two-sphere is a homogeneous space for the rotation group. Let G be a transitive transforma ...
... For example, the rotation group in three-dimensional Euclidean space is not transitive. A point on a given sphere cannot be changed to a point on a sphere of a different radius by a rotation. However, the unit two-sphere is a homogeneous space for the rotation group. Let G be a transitive transforma ...
A Chemical Approach to Molecular Spin Qubits: Decoherence and
... Section a: Extended Synopsis of the scientific proposal (max. 5 pages) All electronics “runs on quantum mechanics”, from semiconductors and lasers to giant-magnetoresistancebased hard drives and memories. A number of spectacular technologies even depend very explicitly of quantum effects, from medic ...
... Section a: Extended Synopsis of the scientific proposal (max. 5 pages) All electronics “runs on quantum mechanics”, from semiconductors and lasers to giant-magnetoresistancebased hard drives and memories. A number of spectacular technologies even depend very explicitly of quantum effects, from medic ...