Field and gauge theories
... Formulation of QFT – Path Integrals Amplitude to propagate from state A to B in time T governed by exp[-i H T], specifically the matrix element between A and B Path integral breaks down the propagation into infinitesimal elements between complete sets of states Feynman diagrams handy for keep ...
... Formulation of QFT – Path Integrals Amplitude to propagate from state A to B in time T governed by exp[-i H T], specifically the matrix element between A and B Path integral breaks down the propagation into infinitesimal elements between complete sets of states Feynman diagrams handy for keep ...
Part 3: Quantum numbers and orbitals
... the orbit of an electron, Bohr used one quantum number, n = 1, 2, 3 ……which designated 2 things: ...
... the orbit of an electron, Bohr used one quantum number, n = 1, 2, 3 ……which designated 2 things: ...
n-1 - KAIST
... Ψ should be single valued, continuous as a function of Θ and Φ: the wave meets itself as Θ and Φ cycle around the origin ← with quantum numbers ...
... Ψ should be single valued, continuous as a function of Θ and Φ: the wave meets itself as Θ and Φ cycle around the origin ← with quantum numbers ...
A quantum mechanical model for the rate of return
... case of stock markets with price limit rule: the rate of return in a trading day can not exceed a fixed limit ±q% (for example, in most Chinese stock markets q = 10). By choosing 1% as a ‘quantum’ for the rate of return, the set of all the possible values of R is L = {−q, −q+1, ... , q−1, q}. 2. A F ...
... case of stock markets with price limit rule: the rate of return in a trading day can not exceed a fixed limit ±q% (for example, in most Chinese stock markets q = 10). By choosing 1% as a ‘quantum’ for the rate of return, the set of all the possible values of R is L = {−q, −q+1, ... , q−1, q}. 2. A F ...
Pretest for Uncertainty Principle Part 1
... 3. Suppose at time t=0, the position space wavefunction for a particle is not given explicitly but its momentum space wavefunction is given. Is it possible to determine the uncertainty in the position of the particle at time t=0 without knowing the Hamiltonian of the system? Explain. ...
... 3. Suppose at time t=0, the position space wavefunction for a particle is not given explicitly but its momentum space wavefunction is given. Is it possible to determine the uncertainty in the position of the particle at time t=0 without knowing the Hamiltonian of the system? Explain. ...
Quantum computing
... complete basis hidden in the long sequence of data, we need to find this basis dimension and location satisfying our computational needs. After this, assuming that we have successfully divided long data sequence into snapshots of the basis vector, we should be able to connect individual parts by a u ...
... complete basis hidden in the long sequence of data, we need to find this basis dimension and location satisfying our computational needs. After this, assuming that we have successfully divided long data sequence into snapshots of the basis vector, we should be able to connect individual parts by a u ...
Optics, Light and Lasers: The Practical Approach to RIAO/OPTILAS
... in mesoscopic transport and the underlying physical principles. This is very helpful and absolutely necessary, since he explains a field that is growing fast and in which some conceptual questions are still being discussed. What makes this remarkable as a textbook is that it treats topics as diverse ...
... in mesoscopic transport and the underlying physical principles. This is very helpful and absolutely necessary, since he explains a field that is growing fast and in which some conceptual questions are still being discussed. What makes this remarkable as a textbook is that it treats topics as diverse ...
A Signed Particle Formulation of Non
... dp′ dx′ fW (x′ ; p′ ; t′ )Γ(x′ ; p; p′ )e t′ θ(t − t′ )δ(x′ − x(t′ ))θD (x′ ), dt′ ...
... dp′ dx′ fW (x′ ; p′ ; t′ )Γ(x′ ; p; p′ )e t′ θ(t − t′ )δ(x′ − x(t′ ))θD (x′ ), dt′ ...
Physical Chemistry II
... 1.9 The Heisenberg Uncertainty Principle States That the Position and the Momentum of a Particle Cannot be Speci ed Simultaneously with Unlimited Precision • The act of locating the electron leads to a change in its momentum • As such, the Heisenberg Uncertainty Principle states, ...
... 1.9 The Heisenberg Uncertainty Principle States That the Position and the Momentum of a Particle Cannot be Speci ed Simultaneously with Unlimited Precision • The act of locating the electron leads to a change in its momentum • As such, the Heisenberg Uncertainty Principle states, ...
leading quantum correction to the newtonian potential
... it has not been possible to combine general relativity with quantum mechanics to form a satisfactory theory of quantum gravity. One of the problems, among others, is that general relativity does not fit the present paradigm for a fundamental theory; that of a renormalizable quantum field theory. Alt ...
... it has not been possible to combine general relativity with quantum mechanics to form a satisfactory theory of quantum gravity. One of the problems, among others, is that general relativity does not fit the present paradigm for a fundamental theory; that of a renormalizable quantum field theory. Alt ...
Greco1 - INFN - Torino Personal pages
... We can see that ideal Hydro can be satisfied only if f=feq , on the other hand the underlying hypothesis of Hydro is that the mean free path is so small that the f(x,p)is always at equilibrium during the evolution. Similarly ∂T , for f≠feq and one can do the expansion in terms of transport ...
... We can see that ideal Hydro can be satisfied only if f=feq , on the other hand the underlying hypothesis of Hydro is that the mean free path is so small that the f(x,p)is always at equilibrium during the evolution. Similarly ∂T , for f≠feq and one can do the expansion in terms of transport ...