# Difference between revisions of "Schrödinger equation"

Ulf Rehmann (talk | contribs) m (moved Schroedinger equation to Schrödinger equation over redirect: accented title) |
m (Completed rendering of article in TeX. Corrected errors in mathematical formulas.) |
||

Line 1: | Line 1: | ||

− | A fundamental equation in quantum mechanics that determines, together with corresponding additional conditions, a wave function | + | A fundamental equation in quantum mechanics that determines, together with corresponding additional conditions, a wave function $ \psi(t,\mathbf{q}) $ characterizing the state of a quantum system. For a non-relativistic system of spin-less particles, it was formulated by E. Schrödinger in 1926. It has the form |

+ | $$ | ||

+ | i \hbar \frac{\partial}{\partial t} [\psi(t,\mathbf{q})] = \hat{H} \psi(t,\mathbf{q}), | ||

+ | $$ | ||

+ | where $ \hat{H} = H(\hat{\mathbf{p}},\hat{\mathbf{r}}) $ is the [[Hamilton operator|Hamiltonian operator]] constructed by the following general rule: In the classical Hamiltonian function $ H(\mathbf{p},\mathbf{r}) $, the particle momenta $ \mathbf{p} $ and their coordinates $ \mathbf{r} $ are replaced by operators that have, respectively, the following form in the coordinate representation $ \mathbf{q} = (r_{1},\ldots,r_{N}) $ and in the momentum representation $ \mathbf{p} = (p_{1},\ldots,p_{N}) $: | ||

+ | $$ | ||

+ | \hat{p}_{i} = \frac{\hbar}{i} \frac{\partial}{\partial r_{i}} \quad \text{and} \quad \hat{r}_{i} = r_{i}; \qquad \hat{p}_{i} = p_{i} \quad \text{and} \quad \hat{r}_{i} = - \frac{\hbar}{i} \frac{\partial}{\partial p_{i}}; \qquad i \in \{ 1,\ldots,N \}. | ||

+ | $$ | ||

+ | For charged particles in an electromagnetic field, characterized by a vector potential $ \mathbf{A}(t,\mathbf{r}) $, the quantity $ \mathbf{p} $ is replaced by $ \mathbf{p} + \dfrac{e}{c} \mathbf{A}(t,\mathbf{r}) $. In these representations, the Schrödinger equation is a partial differential equation. For example, for particles in the potential field $ U(\mathbf{r}) $, the equation becomes | ||

+ | $$ | ||

+ | i \hbar \frac{\partial}{\partial t} [\psi(t,\mathbf{r})] = - \frac{\hbar^{2}}{2 m} {\Delta \psi}(t,\mathbf{r}) + U(\mathbf{r}) \psi(t,\mathbf{r}). | ||

+ | $$ | ||

− | + | Discrete representations are possible, in which the function $ \psi $ is a multi-component function and the operator $ \hat{H} $ has the form of a matrix. If a wave function is defined in the space of occupation numbers, then the operator $ \hat{H} $ is represented by some combinations of [[Creation operators|creation]] and [[Annihilation operators|annihilation operators]] (i.e., the second quantization representation). | |

− | + | The generalization of the Schrödinger equation to the case of a non-relativistic particle with spin $ \dfrac{1}{2} $ (a two-component wave-function $ \psi(t,\mathbf{r}) $) is called the '''Pauli equation''' (1927); to the case of a relativistic particle with spin $ \dfrac{1}{2} $ (a four-component wave-function $ \psi $) — the [[Dirac equation|'''Dirac equation''']] (1928); to the case of a relativistic particle with spin $ 0 $ — the [[Klein–Gordon equation|'''Klein–Gordon equation''']] (1926); to the case of a relativistic particle with spin $ 1 $ (the wave-function $ \psi $ is a vector) — the '''Proca equation''' (1936); etc. | |

− | + | The solution of the Schrödinger equation is defined in the class of functions that satisfy the normalization condition $ \langle \psi(t,\mathbf{q}),\psi(t,\mathbf{q}) \rangle = 1 $ for all $ t $ (the angled brackets mean an integration or a summation over all values of $ \mathbf{q} $). To find the solution, it is necessary to formulate initial and boundary conditions, corresponding to the character of the problem under consideration. The most characteristic among such problems are: | |

− | + | # The stationary Schrödinger equation and the determination of admissible values of the energy of the system. Assuming that $ \psi(t,\mathbf{q}) = \phi(\mathbf{q}) e^{- i E t / \hbar} $, and requiring in conformity with the normalization condition and the condition of absence of flows at infinity that the wave function and its gradients vanish when $ \| \mathbf{r} \| \to \infty $, one obtains an equation for the eigenvalues $ E_{n} $ and eigenfunctions $ \phi_{n} $ of the Hamiltonian operator: $$ \hat{H} {\phi_{n}}(\mathbf{q}) = E_{n} {\phi_{n}}(\mathbf{q}). $$ Characteristic examples of the exact solution to this problem are: The eigenfunctions and energy levels for a harmonic oscillator, a hydrogen atom, etc. | |

+ | # The quantum-mechanical scattering problem. The Schrödinger equation is solved under boundary conditions that correspond at a large distance from the scattering center (described by a potential $ U(\mathbf{r}) $) to the plane waves falling on it and the spherical waves arising from it. Taking into consideration this boundary condition, the Schrödinger equation can be written as an integral equation, the first iteration of which with respect to the term containing $ U(\mathbf{r}) $ corresponds to the so-called '''Born approximation'''. This equation is also called the '''Lippman–Schwinger equation'''. | ||

+ | # The case where the Hamiltonian of the system depends on time, $ H = {H_{0}}(\mathbf{p},\mathbf{r}) + U(t,\mathbf{p},\mathbf{r}) $, is usually considered in the framework of '''time-dependent perturbation theory'''. This is a theory of quantum transition, the determination of the system’s reaction to an external perturbation (dynamic susceptibility) and characteristics of relaxation processes. | ||

− | + | To solve the Schrödinger equation, one usually applies approximate methods, regular methods (different types of perturbation theories), variational methods, etc. | |

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

− | |||

====References==== | ====References==== | ||

− | |||

+ | <table> | ||

+ | <TR><TD valign="top">[1]</TD><TD valign="top"> | ||

+ | A. Messiah, “Quantum mechanics”, '''1''', North-Holland (1961).</TD></TR> | ||

+ | <TR><TD valign="top">[2]</TD><TD valign="top"> | ||

+ | L.D. Landau, E.M. Lifshitz, “Quantum mechanics”, Pergamon (1965). (Translated from Russian)</TD></TR> | ||

+ | <TR><TD valign="top">[3]</TD><TD valign="top"> | ||

+ | L.I. Schiff, “Quantum mechanics”, McGraw-Hill (1955).</TD></TR> | ||

+ | </table> | ||

+ | ====Comments==== | ||

− | |||

A comprehensive treatise on the mathematics of the Schrödinger equation is [[#References|[a4]]]. | A comprehensive treatise on the mathematics of the Schrödinger equation is [[#References|[a4]]]. | ||

====References==== | ====References==== | ||

− | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> | + | |

+ | <table> | ||

+ | <TR><TD valign="top">[a1]</TD><TD valign="top"> | ||

+ | R.P. Feynman, R.B. Leighton, M. Sands, “The Feynman lectures on physics”, '''III''', Addison-Wesley (1965).</TD></TR> | ||

+ | <TR><TD valign="top">[a2]</TD><TD valign="top"> | ||

+ | S. Gasiorowicz, “Quantum physics”, Wiley (1974).</TD></TR> | ||

+ | <TR><TD valign="top">[a3]</TD><TD valign="top"> | ||

+ | J.M. Lévy-Lehlond, “Quantics-rudiments of quantum physics”, North-Holland (1990). (Translated from French)</TD></TR> | ||

+ | <TR><TD valign="top">[a4]</TD><TD valign="top"> | ||

+ | F.A. Berezin, M.A. Shubin, “The Schrödinger equation”, Kluwer (1991). (Translated from Russian)</TD></TR> | ||

+ | </table> |

## Latest revision as of 09:15, 14 December 2016

A fundamental equation in quantum mechanics that determines, together with corresponding additional conditions, a wave function $ \psi(t,\mathbf{q}) $ characterizing the state of a quantum system. For a non-relativistic system of spin-less particles, it was formulated by E. Schrödinger in 1926. It has the form $$ i \hbar \frac{\partial}{\partial t} [\psi(t,\mathbf{q})] = \hat{H} \psi(t,\mathbf{q}), $$ where $ \hat{H} = H(\hat{\mathbf{p}},\hat{\mathbf{r}}) $ is the Hamiltonian operator constructed by the following general rule: In the classical Hamiltonian function $ H(\mathbf{p},\mathbf{r}) $, the particle momenta $ \mathbf{p} $ and their coordinates $ \mathbf{r} $ are replaced by operators that have, respectively, the following form in the coordinate representation $ \mathbf{q} = (r_{1},\ldots,r_{N}) $ and in the momentum representation $ \mathbf{p} = (p_{1},\ldots,p_{N}) $: $$ \hat{p}_{i} = \frac{\hbar}{i} \frac{\partial}{\partial r_{i}} \quad \text{and} \quad \hat{r}_{i} = r_{i}; \qquad \hat{p}_{i} = p_{i} \quad \text{and} \quad \hat{r}_{i} = - \frac{\hbar}{i} \frac{\partial}{\partial p_{i}}; \qquad i \in \{ 1,\ldots,N \}. $$ For charged particles in an electromagnetic field, characterized by a vector potential $ \mathbf{A}(t,\mathbf{r}) $, the quantity $ \mathbf{p} $ is replaced by $ \mathbf{p} + \dfrac{e}{c} \mathbf{A}(t,\mathbf{r}) $. In these representations, the Schrödinger equation is a partial differential equation. For example, for particles in the potential field $ U(\mathbf{r}) $, the equation becomes $$ i \hbar \frac{\partial}{\partial t} [\psi(t,\mathbf{r})] = - \frac{\hbar^{2}}{2 m} {\Delta \psi}(t,\mathbf{r}) + U(\mathbf{r}) \psi(t,\mathbf{r}). $$

Discrete representations are possible, in which the function $ \psi $ is a multi-component function and the operator $ \hat{H} $ has the form of a matrix. If a wave function is defined in the space of occupation numbers, then the operator $ \hat{H} $ is represented by some combinations of creation and annihilation operators (i.e., the second quantization representation).

The generalization of the Schrödinger equation to the case of a non-relativistic particle with spin $ \dfrac{1}{2} $ (a two-component wave-function $ \psi(t,\mathbf{r}) $) is called the **Pauli equation** (1927); to the case of a relativistic particle with spin $ \dfrac{1}{2} $ (a four-component wave-function $ \psi $) — the **Dirac equation** (1928); to the case of a relativistic particle with spin $ 0 $ — the **Klein–Gordon equation** (1926); to the case of a relativistic particle with spin $ 1 $ (the wave-function $ \psi $ is a vector) — the **Proca equation** (1936); etc.

The solution of the Schrödinger equation is defined in the class of functions that satisfy the normalization condition $ \langle \psi(t,\mathbf{q}),\psi(t,\mathbf{q}) \rangle = 1 $ for all $ t $ (the angled brackets mean an integration or a summation over all values of $ \mathbf{q} $). To find the solution, it is necessary to formulate initial and boundary conditions, corresponding to the character of the problem under consideration. The most characteristic among such problems are:

- The stationary Schrödinger equation and the determination of admissible values of the energy of the system. Assuming that $ \psi(t,\mathbf{q}) = \phi(\mathbf{q}) e^{- i E t / \hbar} $, and requiring in conformity with the normalization condition and the condition of absence of flows at infinity that the wave function and its gradients vanish when $ \| \mathbf{r} \| \to \infty $, one obtains an equation for the eigenvalues $ E_{n} $ and eigenfunctions $ \phi_{n} $ of the Hamiltonian operator: $$ \hat{H} {\phi_{n}}(\mathbf{q}) = E_{n} {\phi_{n}}(\mathbf{q}). $$ Characteristic examples of the exact solution to this problem are: The eigenfunctions and energy levels for a harmonic oscillator, a hydrogen atom, etc.
- The quantum-mechanical scattering problem. The Schrödinger equation is solved under boundary conditions that correspond at a large distance from the scattering center (described by a potential $ U(\mathbf{r}) $) to the plane waves falling on it and the spherical waves arising from it. Taking into consideration this boundary condition, the Schrödinger equation can be written as an integral equation, the first iteration of which with respect to the term containing $ U(\mathbf{r}) $ corresponds to the so-called
**Born approximation**. This equation is also called the**Lippman–Schwinger equation**. - The case where the Hamiltonian of the system depends on time, $ H = {H_{0}}(\mathbf{p},\mathbf{r}) + U(t,\mathbf{p},\mathbf{r}) $, is usually considered in the framework of
**time-dependent perturbation theory**. This is a theory of quantum transition, the determination of the system’s reaction to an external perturbation (dynamic susceptibility) and characteristics of relaxation processes.

To solve the Schrödinger equation, one usually applies approximate methods, regular methods (different types of perturbation theories), variational methods, etc.

#### References

[1] |
A. Messiah, “Quantum mechanics”, 1, North-Holland (1961). |

[2] | L.D. Landau, E.M. Lifshitz, “Quantum mechanics”, Pergamon (1965). (Translated from Russian) |

[3] | L.I. Schiff, “Quantum mechanics”, McGraw-Hill (1955). |

#### Comments

A comprehensive treatise on the mathematics of the Schrödinger equation is [a4].

#### References

[a1] |
R.P. Feynman, R.B. Leighton, M. Sands, “The Feynman lectures on physics”, III, Addison-Wesley (1965). |

[a2] | S. Gasiorowicz, “Quantum physics”, Wiley (1974). |

[a3] | J.M. Lévy-Lehlond, “Quantics-rudiments of quantum physics”, North-Holland (1990). (Translated from French) |

[a4] | F.A. Berezin, M.A. Shubin, “The Schrödinger equation”, Kluwer (1991). (Translated from Russian) |

**How to Cite This Entry:**

Schrödinger equation.

*Encyclopedia of Mathematics.*URL: http://encyclopediaofmath.org/index.php?title=Schr%C3%B6dinger_equation&oldid=23522