1985
DOI: 10.1063/1.526621
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Some properties of hyperspherical harmonics

Abstract: A general formula is given for the canonical decomposition of a homogeneous polynomial of order λ in m variables into a sum of harmonic polynomials. This formula, which involves successive applications of the generalized Laplace operator, is proved in the Appendix. It is shown that the group-theoretical method for constructing irreducible Cartesian tensors follows from the general formula for canonical decomposition. The relationship between harmonic polynomials and hyperspherical harmonics is discussed, and a… Show more

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Cited by 64 publications
(70 citation statements)
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“…This equation can be treated perturbatively for small following the procedure in Sec. IV and by introducing the hyperspherical harmonics Y m l ( θ), which obey the eigenvalue equation [28] …”
Section: Intrinsically Spherical Growth and Rapid Rougheningmentioning
confidence: 99%
“…This equation can be treated perturbatively for small following the procedure in Sec. IV and by introducing the hyperspherical harmonics Y m l ( θ), which obey the eigenvalue equation [28] …”
Section: Intrinsically Spherical Growth and Rapid Rougheningmentioning
confidence: 99%
“…However, the projection method allows one to obtain analytic results only for a limited set of functions having simple functional forms so that necessary integrals can be calculated analytically. We present here an alternative, differential approach, which generalizes earlier results by Sack [13] (who dealt with multipole expansions for the special case of two-center functions) as well as by Avery [14] and Wen and Avery [15] (who dealt with bicenter expansions using the vector differentiation technique in three dimensions [14] and m dimensions [15] for the special case of scalar functions). Our general results for the multipole expansion of T jm (a 1 , a 2 , .…”
Section: Introductionmentioning
confidence: 93%
“…Taking into account (14), the general equation (8) for the function (12) may be written (after some rearrangements of summation indices) as (15) where the differential operator  is defined by (16) Taking into account the known identity we obtain the multipole expansion for the function (12) in the following final form: (17) where the coefficients B are defined by (18) Note that the  -operator (16) commutes with the Ñ 2 -operator because  originates from Ñ-operators (see (8) and (A.2)). Thus, we can write the operator  ( j ) ll′ (r 1 ) in (18) before the sum over the index k.…”
Section: Multipole Expansion Of Two-center Functions Of the Form F (Rmentioning
confidence: 99%
“…Note that those were not conventional harmonics as defined in [8,12] but the set of harmonics labeled by the individual angular momenta quantum numbers of particles [14]. The expression for CMC was then extracted from the series by using some specific gauge convention (eqs.…”
Section: Discussionmentioning
confidence: 99%
“…In order to calculate this integral we note that the Gegenbauer polynomial in (47) is proportional to the scalar product of six-dimensional hyperspherical harmonics [8,12],…”
Section: The Hyperspherical Expansion Of the Multipole Coeffi-cientsmentioning
confidence: 99%