hamiltonian operator वाक्य
उदाहरण वाक्य
मोबाइल
- Someone enlighten me by dialing 0 on the Hamiltonian operator.
- Using a suitable Hamiltonian operator corresponding to the system.
- Because the crystal has translational symmetry, this operator commutes with the Hamiltonian operator.
- Manipulating, we have the " Trace formula " for the exponential of the Hamiltonian operator satisfying
- The Hamiltonian operators in the Schr�dinger picture are one approach to forming the differential equations for.
- Where " i " times the time derivative is the Hamiltonian operator in quantum mechanics.
- The Fock operator is an effective one-electron Hamiltonian operator being the sum of two terms.
- One of the Feynman's path integral formulation uses a Lagrangian rather than a Hamiltonian operator.
- And each time a Hamiltonian operator acts it does so by adding a new edge at the vertex.
- The eigenfunctions of the Hamiltonian operator are stationary states of the quantum mechanical system, each with a corresponding energy.
- 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.
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