hamiltonian operator उदाहरण वाक्य
उदाहरण वाक्य
- This yields to a Hamiltonian whose eigenvalues are the square of the imaginary part of the Riemann zeros, and also the functional determinant of this Hamiltonian operator is just the Riemann Xi function.
- In RS theory one considers an unperturbed Hamiltonian operator \ hat { H } _ { 0 }, to which a small ( often external ) perturbation \ hat { V } is added:
- To apply the Schr�dinger equation, the Hamiltonian operator is set up for the system, accounting for the kinetic and potential energy of the particles constituting the system, then inserted into the Schr�dinger equation.
- This means that the state at a slightly later time differs from the state at the current time by the result of acting with the Hamiltonian operator ( multiplied by the negative imaginary unit, ).
- As an application, we consider the Schr�dinger equation, or equivalently, the Hamiltonian operator " H " models the total energy observable of a quantum mechanical system "'S " '.
- "Fractional quantum oscillator " introduced by Nick Laskin ( see, Ref . [ 2 ] ) is the fractional quantum mechanical model with the Hamiltonian operator H _ { \ alpha, \ beta } defined as
- The tensor product factorization is only possible if the orbital and spin angular momenta of the particle are separable in the Hamiltonian operator underlying the system's dynamics ( in other words, the Hamiltonian can be split into the sum of orbital and spin terms ).
- The Lagrangian approach with field interpretation of is the subject of QFT rather than RQM : Feynman's path integral formulation uses invariant Lagrangians rather than Hamiltonian operators, since the latter can become extremely complicated, see ( for example ) S . Weinberg ( 1995 ).
- Solving the latter in any particular case requires specifying the Hamiltonian operator, which includes a generic part related to kinetic energy and specific part related to how the particle ( s ) potential energy can be expected to change as a function of position and / or time.
- A very important aspect of the Hamiltonian operator is that it only acts at vertices ( a consequence of this is that Thiemann's Hamiltonian operator, like Ashtekar's operator, annihilates non-intersecting loops except now it is not just formal and has rigorous mathematical meaning ).