Explore: Schrödinger Equation

The Schrödinger equation is a partial differential equation that governs the wave function of a non-relativistic quantum-mechanical system. Its discovery

(one-dimensional) nonlinear Schrödinger equation (NLSE) is a nonlinear variation of the Schrödinger equation. It is a classical field equation whose principal applications

The Schrödinger–Newton equation, sometimes referred to as the Newton–Schrödinger or Schrödinger–Poisson equation, is a nonlinear modification of the Schrödinger

Schrödinger equation, an equation that provides a way to calculate the wave function of a system and how it changes dynamically in time. Schrödinger coined

The Dirac equation of relativistic quantum theory improves these solutions (see below). The solution of the Schrödinger equation (wave equation) for the

solution to the many-body Schrödinger equation as the solution to free particles in presence of some unknown interacting parts. Equations that include operators

introduced here from the subsequent, but more familiar, Schrödinger picture. According to Schrödinger's equation, the quantum state at time t {\displaystyle t}

mechanics". Schrödinger subsequently showed that the two approaches were equivalent. In 1926, Schrödinger published the famous wave equation now named after

the WKB approximation. The Schrödinger equation was published in 1926. The first person to apply the Schrödinger equation to a problem that involved tunneling

Klein–Gordon equation (Klein–Fock–Gordon equation or sometimes Klein–Gordon–Fock equation) is a relativistic wave equation, related to the Schrödinger equation. It