List of equations in quantum mechanics
This article summarizes equations in the theory of quantum mechanics.
Wavefunctions
A fundamental physical constant occurring in quantum mechanics is the Planck constant, h. A common abbreviation is, also known as the reduced Planck constant or Dirac constant.| Quantity | symbol/s | Defining equation | SI unit | Dimension |
| Wavefunction | ψ, Ψ | To solve from the Schrödinger equation | varies with situation and number of particles | |
| Wavefunction probability density | ρ | m−3 | −3 | |
| Wavefunction probability current | j | Non-relativistic, no external field: star * is complex conjugate | m−2⋅s−1 | −1 −2 |
The general form of wavefunction for a system of particles, each with position ri and z-component of spin sz i. Sums are over the discrete variable sz, integrals over continuous positions r.
For clarity and brevity, the coordinates are collected into tuples, the indices label the particles. Following are general mathematical results, used in calculations.
| Property or effect | Nomenclature | Equation |
| Wavefunction for N particles in 3d | r = sz = | In function notation: in bra–ket notation: for non-interacting particles: |
| Position-momentum Fourier transform |
| |
| General probability distribution | Vj = volume particle may occupy,P = Probability that particle 1 has position r1 in volume V1 with spin sz1 and particle 2 has position r2 in volume V2 with spin sz2, etc. | |
| General normalization condition |
Equations
Wave–particle duality and time evolution
| Property or effect | Nomenclature | Equation |
| Planck–Einstein equation and de Broglie wavelength relations | P = is the four-momentum,K = is the four-wavevector,E = energy of particleω = 2πf is the angular frequency and frequency of the particleħ = h/2π are the Planck constantsc = speed of light | |
| Schrödinger equation | Ψ = wavefunction of the systemĤ = Hamiltonian operator,E = energy eigenvalue of systemi is the imaginary unitt = time | General time-dependent case: Time-independent case: |
| Heisenberg equation | Â = operator of an observable property
| |
| Time evolution in Heisenberg picture | m = mass,V = potential energy, r = position,p = momentum, of a particle. | For momentum and position; |
Non-relativistic time-independent Schrödinger equation
Summarized below are the various forms the Hamiltonian takes, with the corresponding Schrödinger equations and forms of wavefunction solutions. Notice in the case of one spatial dimension, for one particle, the partial derivative reduces to an ordinary derivative.| One particle | N particles | |
| One dimension | where the position of particle n is xn. | |
| One dimension | ||
| One dimension | There is a further restriction — the solution must not grow at infinity, so that it has either a finite L2-norm or a slowly diverging norm : | for non-interacting particles |
| Three dimensions | where the position of the particle is r =. | where the position of particle n is r n =, and the Laplacian for particle n using the corresponding position coordinates is |
| Three dimensions | ||
| Three dimensions | for non-interacting particles |
Non-relativistic time-dependent Schrödinger equation
Again, summarized below are the various forms the Hamiltonian takes, with the corresponding Schrödinger equations and forms of solutions.| One particle | N particles | |
| One dimension | where the position of particle n is xn. | |
| One dimension | ||
| One dimension | ||
| Three dimensions | ||
| Three dimensions | This last equation is in a very high dimension, so the solutions are not easy to visualize. | |
| Three dimensions |
Photoemission
| Property/Effect | Nomenclature | Equation |
| Photoelectric equation | Kmax = Maximum kinetic energy of ejected electron h = Planck constantf = frequency of incident photons φ, Φ = Work function of the material the photons are incident on | |
| Threshold frequency and Work function | φ, Φ = Work function of the material the photons are incident on f0, ν0 = Threshold frequency | Can only be found by experiment. The De Broglie relations give the relation between them: |
| Photon momentum | p = momentum of photon f = frequency of photon λ = wavelength of photon | The De Broglie relations give: |
Quantum uncertainty
| Property or effect | Nomenclature | Equation |
| Heisenberg's uncertainty principles | n = number of photonsφ = wave phase | Position–momentum Energy-time Number-phase |
| Dispersion of observable | A = observables | |
| General uncertainty relation | A, B = observables |
| Property or effect | Equation |
| Density of states | |
| Fermi–Dirac distribution | whereP = probability of energy Eig = degeneracy of energy Ei μ = chemical potential |
| Bose–Einstein distribution |
Angular momentum
| Property or effect | Nomenclature | Equation |
| Angular momentum quantum numbers | s = spin quantum numberms = spin magnetic quantum numberℓ = Azimuthal quantum numbermℓ = azimuthal magnetic quantum numberj = total angular momentum quantum numbermj = total angular momentum magnetic quantum number | Spin: Orbital: Total: |
| Angular momentum magnitudes | angular momementa:S = Spin,L = orbital,J = total | Spin magnitude: Orbital magnitude: Total magnitude: |
| Angular momentum components | Spin: Orbital: |
; Magnetic moments :
In what follows, B is an applied external magnetic field and the quantum numbers above are used.
| Property or effect | Nomenclature | Equation |
| orbital magnetic dipole moment | e = electron chargeme = electron rest massL = electron orbital angular momentumg = orbital Landé g-factorμB = Bohr magneton | z-component: |
| spin magnetic dipole moment | S = electron spin angular momentumgs = spin Landé g-factor | z-component: |
| dipole moment potential | U = potential energy of dipole in field |
Hydrogen atom
| Property or effect | Nomenclature | Equation |
| Energy level | En = energy eigenvaluen = principal quantum numbere = electron chargeme = electron rest massε0 = permittivity of free spaceh = Planck constant | |
| Spectrum | λ = wavelength of emitted photon, during electronic transition from Ei to Ej |