hamiltonian operator उदाहरण वाक्य
उदाहरण वाक्य
- The continuous and discrete spectra of physical systems can be modeled in functional analysis as different parts in the Hamiltonian operator.
- One particularly important representation, is that in which the transformed Hamiltonian operator \ hat { H }'_ 0 is diagonalized.
- By contrast, in quantum mechanics, terms have to be introduced artificially into the Hamiltonian operator to achieve agreement with experimental observations.
- Thus the symmetry group of the two particle Hamiltonian operator is the superset of the symmetry groups of the Hamiltonian operators of individual particles.
- Thus the symmetry group of the two particle Hamiltonian operator is the superset of the symmetry groups of the Hamiltonian operators of individual particles.
- In the Schr�dinger equation for this system of one negative and one positive particle, the atomic orbitals are the eigenstates of the Hamiltonian operator for the energy.
- Thus, what we think about as time evolution of any physical system is just a gauge transformation, similar to that of kernel of the Hamiltonian operator.
- To demonstrate this, they picking up on Fermi's trick which allows to identify an arbitrary wavefunction as a stationary state for some Hamiltonian operator.
- where \ hat { H } is the Hamiltonian operator, and is the Hamiltonian represented in coordinate space ( as is the case in the derivation above ).
- where is the wavefunction of the system, is the quantum Hamiltonian operator, rather than a function as in classical mechanics, and is the Planck constant divided by 2.