Associated Legendre function/Related Articles: Difference between revisions
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imported>Jitse Niesen (add {{r|Orthogonal polynomials}}) |
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==Other related topics== | ==Other related topics== | ||
{{r|Legendre function}} | {{r|Legendre function}} | ||
{{r|Legendre polynomials}} | |||
{{r|Spherical harmonics}} | {{r|Spherical harmonics}} | ||
{{r|Angular momentum (quantum)}} | {{r|Angular momentum (quantum)}} | ||
{{r|Adrien-Marie Legendre}} | {{r|Adrien-Marie Legendre}} | ||
==Articles related by keyphrases (Bot populated)== | |||
{{r|Adrien-Marie Legendre}} | |||
{{r|Legendre polynomials}} | |||
{{r|Sturm-Liouville theory}} | |||
{{r|Angular momentum (quantum)}} | |||
Latest revision as of 16:00, 13 July 2024
- See also changes related to Associated Legendre function, or pages that link to Associated Legendre function or to this page or whose text contains "Associated Legendre function".
Parent topics
- Hypergeometric function [r]: Add brief definition or description
- Orthogonal polynomials [r]: Add brief definition or description
- Legendre function [r]: Add brief definition or description
- Legendre polynomials [r]: Orthogonal polynomials in the variable −1 ≤ x ≤ 1 and weight function w(x) = 1. [e]
- Spherical harmonics [r]: A series of harmonic basis functions that can be used to describe the boundary of objects with spherical topology. [e]
- Angular momentum (quantum) [r]: A vector operator of which the three components have well-defined commutation relations. [e]
- Adrien-Marie Legendre [r]: (1752 – 1833) important French mathematician whose name lives on in the Legendre polynomials and associated Legendre functions. [e]
- Adrien-Marie Legendre [r]: (1752 – 1833) important French mathematician whose name lives on in the Legendre polynomials and associated Legendre functions. [e]
- Legendre polynomials [r]: Orthogonal polynomials in the variable −1 ≤ x ≤ 1 and weight function w(x) = 1. [e]
- Sturm-Liouville theory [r]: A special second order linear ordinary differential equation. [e]
- Angular momentum (quantum) [r]: A vector operator of which the three components have well-defined commutation relations. [e]