Multipole expansion explained

A multipole expansion is a mathematical series representing a function that depends on angles—usually the two angles used in the spherical coordinate system (the polar and azimuthal angles) for three-dimensional Euclidean space,

\R ^{3} . Similarly to Taylor series, multipole expansions are useful because oftentimes only the first few terms are needed to provide a good approximation of the original function. The function being expanded may be real- or complex-valued and is defined either on \R ^{3} , or less often on \R ^{n} for some other

Multipole expansions are used frequently in the study of electromagnetic and gravitational fields, where the fields at distant points are given in terms of sources in a small region. The multipole expansion with angles is often combined with an expansion in radius. Such a combination gives an expansion describing a function throughout three-dimensional space.^[1]

The multipole expansion is expressed as a sum of terms with progressively finer angular features (moments). The first (the zeroth-order) term is called the monopole moment, the second (the first-order) term is called the dipole moment, the third (the second-order) the quadrupole moment, the fourth (third-order) term is called the octupole moment, and so on. Given the limitation of Greek numeral prefixes, terms of higher order are conventionally named by adding "-pole" to the number of poles—e.g., 32-pole (rarely dotriacontapole or triacontadipole) and 64-pole (rarely tetrahexacontapole or hexacontatetrapole).^{[2] [3] [4]} A multipole moment usually involves powers (or inverse powers) of the distance to the origin, as well as some angular dependence.

In principle, a multipole expansion provides an exact description of the potential, and generally converges under two conditions: (1) if the sources (e.g. charges) are localized close to the origin and the point at which the potential is observed is far from the origin; or (2) the reverse, i.e., if the sources are located far from the origin and the potential is observed close to the origin. In the first (more common) case, the coefficients of the series expansion are called exterior multipole moments or simply multipole moments whereas, in the second case, they are called interior multipole moments.

Expansion in spherical harmonics

Most commonly, the series is written as a sum of spherical harmonics. Thus, we might write a function

f(\theta,\varphi) as the sum$$f(\backslash theta,\backslash varphi)\; =\; \backslash sum\_^\backslash infty\backslash ,\; \backslash sum\_^\backslash ell\backslash ,\; C^m\_\backslash ell\backslash ,\; Y^m\_\backslash ell(\backslash theta,\backslash varphi)$$where Y ^{m} _{\ell(\theta,\varphi)} are the standard spherical harmonics, and C ^{m} _{\ell} are constant coefficients which depend on the function. The term C ^{0} _{0} represents the monopole; C ^{1} _{1} represent the dipole; and so on. Equivalently, the series is also frequently written^[5] as$$f(\backslash theta,\backslash varphi)\; =\; C\; +\; C\_i\; n^i\; +\; C\_n^i\; n^j\; +\; C\_n^i\; n^j\; n^k\; +\; C\_n^i\; n^j\; n^k\; n^\backslash ell\; +\; \backslash cdots$$where the n ^{i} represent the components of a unit vector in the direction given by the angles \theta and \varphi , and indices are implicitly summed. Here, the term C is the monopole; C _{i} is a set of three numbers representing the dipole; and so on.

In the above expansions, the coefficients may be real or complex. If the function being expressed as a multipole expansion is real, however, the coefficients must satisfy certain properties. In the spherical harmonic expansion, we must have$$C\_\backslash ell^\; =\; (-1)^m\; C^\_\backslash ell\; \backslash ,\; .$$In the multi-vector expansion, each coefficient must be real:$$C\; =\; C^\backslash ast;\backslash \; C\_i\; =\; C\_i^\backslash ast;\backslash \; C\_\; =\; C\_^\backslash ast;\backslash \; C\_\; =\; C\_^\backslash ast;\backslash \; \backslash ldots$$

While expansions of scalar functions are by far the most common application of multipole expansions, they may also be generalized to describe tensors of arbitrary rank.^[6] This finds use in multipole expansions of the vector potential in electromagnetism, or the metric perturbation in the description of gravitational waves.

For describing functions of three dimensions, away from the coordinate origin, the coefficients of the multipole expansion can be written as functions of the distance to the origin,

r —most frequently, as a Laurent series in powers of r . For example, to describe the electromagnetic potential, V , from a source in a small region near the origin, the coefficients may be written as:$$V(r,\backslash theta,\backslash varphi)\; =\; \backslash sum\_^\backslash infty\backslash ,\; \backslash sum\_^\backslash ell\; C^m\_\backslash ell(r)\backslash ,\; Y^m\_\backslash ell(\backslash theta,\backslash varphi)=\; \backslash sum\_^\backslash infty\backslash ,\; \backslash sum\_^\backslash infty\backslash ,\; \backslash sum\_^\backslash ell\; \backslash frac\backslash ,\; Y^m\_\backslash ell(\backslash theta,\backslash varphi)\; .$$

Applications

Multipole expansions are widely used in problems involving gravitational fields of systems of masses, electric and magnetic fields of charge and current distributions, and the propagation of electromagnetic waves. A classic example is the calculation of the exterior multipole moments of atomic nuclei from their interaction energies with the interior multipoles of the electronic orbitals. The multipole moments of the nuclei report on the distribution of charges within the nucleus and, thus, on the shape of the nucleus. Truncation of the multipole expansion to its first non-zero term is often useful for theoretical calculations.

Multipole expansions are also useful in numerical simulations, and form the basis of the fast multipole method of Greengard and Rokhlin, a general technique for efficient computation of energies and forces in systems of interacting particles. The basic idea is to decompose the particles into groups; particles within a group interact normally (i.e., by the full potential), whereas the energies and forces between groups of particles are calculated from their multipole moments. The efficiency of the fast multipole method is generally similar to that of Ewald summation, but is superior if the particles are clustered, i.e. the system has large density fluctuations.

Multipole expansion of a potential outside an electrostatic charge distribution

Consider a discrete charge distribution consisting of point charges with position vectors . We assume the charges to be clustered around the origin, so that for all i:, where has some finite value. The potential, due to the charge distribution, at a point outside the charge distribution, i.e.,, can be expanded in powers of . Two ways of making this expansion can be found in the literature: The first is a Taylor series in the Cartesian coordinates,, and, while the second is in terms of spherical harmonics which depend on spherical polar coordinates. The Cartesian approach has the advantage that no prior knowledge of Legendre functions, spherical harmonics, etc., is required. Its disadvantage is that the derivations are fairly cumbersome (in fact a large part of it is the implicit rederivation of the Legendre expansion of, which was done once and for all by Legendre in the 1780s). Also it is difficult to give a closed expression for a general term of the multipole expansion - usually only the first few terms are given followed by an ellipsis.

Expansion in Cartesian coordinates

Assume for convenience. The Taylor expansion of around the origin can be written as$$v(\backslash mathbf-\; \backslash mathbf)\; =\; v(\backslash mathbf)\; -\; \backslash sum\_\; r\_\backslash alpha\; v\_\backslash alpha(\backslash mathbf)\; +\backslash frac\; \backslash sum\_\backslash sum\_\; r\_\backslash alpha\; r\_\backslash beta\; v\_(\backslash mathbf)-\; \backslash cdots\; +\; \backslash cdots$$with Taylor coefficients$$v\_\backslash alpha(\backslash mathbf)\; \backslash equiv\backslash left(\backslash frac\backslash right)\_\; \backslash quad\backslash text\; \backslash quadv\_(\backslash mathbf)\; \backslash equiv\backslash left(\backslash frac\backslash right)\_\; .$$If satisfies the Laplace equation, then by the above expansion we have$$\backslash left(\backslash nabla^2\; v(\backslash mathbf-\; \backslash mathbf)\backslash right)\_\; =\; \backslash sum\_\; v\_(\backslash mathbf)\; =\; 0,$$and the expansion can be rewritten in terms of the components of a traceless Cartesian second rank tensor:$$\backslash sum\_\backslash sum\_\; r\_\backslash alpha\; r\_\backslash beta\; v\_(\backslash mathbf)=\; \backslash frac\; \backslash sum\_\backslash sum\_\; \backslash left(3r\_\backslash alpha\; r\_\backslash beta\; -\; \backslash delta\_\; r^2\backslash right)\; v\_(\backslash mathbf),$$where is the Kronecker delta and . Removing the trace is common, because it takes the rotationally invariant out of the second rank tensor.

Example

Consider now the following form of :$$v(\backslash mathbf-\; \backslash mathbf)\; \backslash equiv\; \backslash frac$$

.Then by direct differentiation it follows that$$v(\backslash mathbf)\; =\; \backslash frac,\backslash quad\; v\_\backslash alpha(\backslash mathbf)=\; -\backslash frac,\backslash quad\; \backslash hbox\backslash quad\; v\_(\backslash mathbf)\; =\; \backslash frac\; .$$Define a monopole, dipole, and (traceless) quadrupole by, respectively,$$q\_\backslash mathrm\; \backslash equiv\; \backslash sum\_^N\; q\_i,\; \backslash quad\; P\_\backslash alpha\; \backslash equiv\backslash sum\_^N\; q\_i\; r\_,\; \backslash quad\; \backslash text\backslash quad\; Q\_\; \backslash equiv\; \backslash sum\_^N\; q\_i\; (3r\_\; r\_\; -\; \backslash delta\_\; r\_i^2),$$and we obtain finally the first few terms of the multipole expansion of the total potential, which is the sum of the Coulomb potentials of the separate charges:^[7]

This expansion of the potential of a discrete charge distribution is very similar to the one in real solid harmonics given below. The main difference is that the present one is in terms of linearly dependent quantities, for$$\backslash sum\_\; v\_\; =\; 0\; \backslash quad\; \backslash hbox\; \backslash quad\; \backslash sum\_\; Q\_\; =\; 0\; .$$

Note:If the charge distribution consists of two charges of opposite sign which are an infinitesimal distance apart, so that, it is easily shown that the dominant term in the expansion is$$V(\backslash mathbf)\; =\; \backslash frac\; (\backslash mathbf\backslash cdot\backslash mathbf),$$the electric dipolar potential field.

Spherical form

The potential at a point outside the charge distribution, i.e., can be expanded by the Laplace expansion:$$V(\backslash mathbf)\; \backslash equiv\; \backslash sum\_^N\; \backslash frac=\backslash frac\; \backslash sum\_^\backslash infty\; \backslash sum\_^(-1)^m\; I^\_\backslash ell(\backslash mathbf)\; \backslash sum\_^N\; q\_i\; R^m\_\backslash ell(\backslash mathbf\_i),$$where

I ^{- m} _{\ell} ( R ) is an irregular solid harmonic (defined below as a spherical harmonic function divided by R ^{\ell+1} ) and R ^{m} _{\ell} ( r ) is a regular solid harmonic (a spherical harmonic times). We define the spherical multipole moment of the charge distribution as follows$$Q^m\_\backslash ell\; \backslash equiv\; \backslash sum\_^N\; q\_i\; R^m\_\backslash ell(\backslash mathbf\_i),\backslash quad\backslash \; -\backslash ell\; \backslash le\; m\; \backslash le\; \backslash ell.$$Note that a multipole moment is solely determined by the charge distribution (the positions and magnitudes of the N charges).

A spherical harmonic depends on the unit vector

\hat{R} . (A unit vector is determined by two spherical polar angles.) Thus, by definition, the irregular solid harmonics can be written as$$I^m\_(\backslash mathbf)\; \backslash equiv\; \backslash sqrt\; \backslash frac$$so that the multipole expansion of the field at the point outside the charge distribution is given by

This expansion is completely general in that it gives a closed form for all terms, not just for the first few. It shows that the spherical multipole moments appear as coefficients in the expansion of the potential.

It is of interest to consider the first few terms in real form, which are the only terms commonly found in undergraduate textbooks.Since the summand of the m summation is invariant under a unitary transformation of both factors simultaneously and since transformation of complex spherical harmonics to real form is by a unitary transformation, we can simply substitute real irregular solid harmonics and real multipole moments. The term becomes$$V\_(\backslash mathbf)\; =\backslash frac\; \backslash quad\backslash hbox\backslash quad\; q\_\backslash mathrm\backslash equiv\backslash sum\_^N\; q\_i.$$This is in fact Coulomb's law again. For the term we introduce$$\backslash mathbf\; =\; (R\_x,\; R\_y,\; R\_z),\backslash quad\; \backslash mathbf\; =\; (P\_x,\; P\_y,\; P\_z)\backslash quad\backslash hbox\backslash quad\; P\_\backslash alpha\; \backslash equiv\; \backslash sum\_^N\; q\_i\; r\_,\; \backslash quad\; \backslash alpha=x,y,z.$$Then$$V\_(\backslash mathbf)\; =\backslash frac\; (R\_x\; P\_x\; +R\_y\; P\_y\; +\; R\_z\; P\_z)\; =\; \backslash frac\; =\backslash frac.$$This term is identical to the one found in Cartesian form.

In order to write the term, we have to introduce shorthand notations for the five real components of the quadrupole moment and the real spherical harmonics. Notations of the type$$Q\_\; \backslash equiv\; \backslash sum\_^N\; q\_i\backslash ;\; \backslash frac(3z\_i^2\; -\; r\_i^2),$$can be found in the literature. Clearly the real notation becomes awkward very soon, exhibiting the usefulness of the complex notation.

Interaction of two non-overlapping charge distributions

Consider two sets of point charges, one set clustered around a point and one set clustered around a point . Think for example of two molecules, and recall that a molecule by definition consists of electrons (negative point charges) and nuclei (positive point charges). The total electrostatic interaction energy between the two distributions is$$U\_\; =\; \backslash sum\_\; \backslash sum\_\; \backslash frac.$$This energy can be expanded in a power series in the inverse distance of and .This expansion is known as the multipole expansion of U_AB.

In order to derive this multipole expansion, we write, which is a vector pointing from towards . Note that$$\backslash mathbf\_+\backslash mathbf\_+\backslash mathbf\_+\backslash mathbf\_\; =\; 0\backslash quad\; \backslash iff\; \backslash quad\backslash mathbf\_\; =\; \backslash mathbf\_-\backslash mathbf\_+\backslash mathbf\_\; .$$We assume that the two distributions do not overlap:$$|\backslash mathbf\_|\; >\; |\backslash mathbf\_-\backslash mathbf\_|\; \backslash text\; i,j.$$Under this condition we may apply the Laplace expansion in the following form$$\backslash frac$$

= \frac =\sum_^\infty \sum_^L \, (-1)^M I_L^(\mathbf_)\;R^M_L(\mathbf_ - \mathbf_),where I ^{M} _{L} and R ^{M} _{L} are irregular and regular solid harmonics, respectively. The translation of the regular solid harmonic gives a finite expansion,$$R^M\_L(\backslash mathbf\_-\backslash mathbf\_)\; =\; \backslash sum\_^L\; (-1)^\; \backslash binom^\backslash times\; \backslash sum\_^\; R^\_(\backslash mathbf\_)R^\_(\backslash mathbf\_)\backslash ;\backslash langle\; \backslash ell\_A,\; m\_A;\; L-\backslash ell\_A,\; M-m\_A\backslash mid\; L\; M\; \backslash rangle,$$where the quantity between pointed brackets is a Clebsch–Gordan coefficient. Further we used$$R^\_(-\backslash mathbf)\; =\; (-1)^\; R^\_(\backslash mathbf)\; .$$Use of the definition of spherical multipoles and covering of the summation ranges in a somewhat different order (which is only allowed for an infinite range of) gives finally

This is the multipole expansion of the interaction energy of two non-overlapping charge distributions which are a distance R_AB apart. Since$$I\_^(\backslash mathbf\_)\; \backslash equiv\; \backslash left[\backslash frac\{4\backslash pi\}\{2\backslash ell\_A+2\backslash ell\_B+1\}\backslash right]^\backslash ;\backslash frac,$$this expansion is manifestly in powers of . The function is a normalized spherical harmonic.

Molecular moments

All atoms and molecules (except S-state atoms) have one or more non-vanishing permanent multipole moments. Different definitions can be found in the literature, but the following definition in spherical form has the advantage that it is contained in one general equation. Because it is in complex form it has as the further advantage that it is easier to manipulate in calculations than its real counterpart.

We consider a molecule consisting of N particles (electrons and nuclei) with charges eZ_i. (Electrons have a Z-value of −1, while for nuclei it is the atomic number). Particle i has spherical polar coordinates r_i, θ_i, and φ_i and Cartesian coordinates x_i, y_i, and z_i.The (complex) electrostatic multipole operator is$$Q^m\_\backslash ell\; \backslash equiv\; \backslash sum\_^N\; e\; Z\_i\; \backslash ;\; R^m\_(\backslash mathbf\_i),$$where

R ^{m} _{\ell} ( r _{i)} is a regular solid harmonic function in Racah's normalization (also known as Schmidt's semi-normalization).If the molecule has total normalized wave function Ψ (depending on the coordinates of electrons and nuclei), then the multipole moment of order \ell of the molecule is given by the expectation (expected) value:$$M^m\_\backslash ell\; \backslash equiv\; \backslash langle\; \backslash Psi\; \backslash mid\; Q^m\_\backslash ell\; \backslash mid\; \backslash Psi\; \backslash rangle.$$If the molecule has certain point group symmetry, then this is reflected in the wave function: Ψ transforms according to a certain irreducible representation λ of the group ("Ψ has symmetry type λ"). This has the consequence that selection rules hold for the expectation value of the multipole operator, or in other words, that the expectation value may vanish because of symmetry. A well-known example of this is the fact that molecules with an inversion center do not carry a dipole (the expectation values of Q ^{m} _{1} vanish for . For a molecule without symmetry, no selection rules are operative and such a molecule will have non-vanishing multipoles of any order (it will carry a dipole and simultaneously a quadrupole, octupole, hexadecapole, etc.).

The lowest explicit forms of the regular solid harmonics (with the Condon-Shortley phase) give:$$M^0\_0\; =\; \backslash sum\_^N\; e\; Z\_i,$$(the total charge of the molecule). The (complex) dipole components are:$$M^1\_1\; =\; -\; \backslash tfrac\; \backslash sum\_^N\; e\; Z\_i\; \backslash langle\; \backslash Psi\; |\; x\_i+iy\_i\; |\; \backslash Psi\; \backslash rangle\backslash quad\; \backslash hbox\; \backslash quadM^\_\; =\; \backslash tfrac\; \backslash sum\_^N\; e\; Z\_i\; \backslash langle\; \backslash Psi\; |\; x\_i\; -\; iy\_i\; |\; \backslash Psi\; \backslash rangle.$$$$M^0\_1\; =\; \backslash sum\_^N\; e\; Z\_i\; \backslash langle\; \backslash Psi\; |\; z\_i\; |\; \backslash Psi\; \backslash rangle.$$

Note that by a simple linear combination one can transform the complex multipole operators to real ones. The real multipole operators are of cosine type

C ^{m} _{\ell} or sine type S ^{m} _{\ell} . A few of the lowest ones are:

Note on conventions

The definition of the complex molecular multipole moment given above is the complex conjugate of the definition given in this article, which follows the definition of the standard textbook on classical electrodynamics by Jackson,^[7] except for the normalization. Moreover, in the classical definition of Jackson the equivalent of the N-particle quantum mechanical expectation value is an integral over a one-particle charge distribution. Remember that in the case of a one-particle quantum mechanical system the expectation value is nothing but an integral over the charge distribution (modulus of wavefunction squared), so that the definition of this article is a quantum mechanical N-particle generalization of Jackson's definition.

The definition in this article agrees with, among others, the one of Fano and Racah^[8] and Brink and Satchler.^[9]

Examples

There are many types of multipole moments, since there are many types of potentials and many ways of approximating a potential by a series expansion, depending on the coordinates and the symmetry of the charge distribution. The most common expansions include:

• Axial multipole moments of a potential;
• Spherical multipole moments of a potential; and
• Cylindrical multipole moments of a potential

Examples of potentials include the electric potential, the magnetic potential and the gravitational potential of point sources. An example of a potential is the electric potential of an infinite line charge.

General mathematical properties

Multipole moments in mathematics and mathematical physics form an orthogonal basis for the decomposition of a function, based on the response of a field to point sources that are brought infinitely close to each other. These can be thought of as arranged in various geometrical shapes, or, in the sense of distribution theory, as directional derivatives.

Multipole expansions are related to the underlying rotational symmetry of the physical laws and their associated differential equations. Even though the source terms (such as the masses, charges, or currents) may not be symmetrical, one can expand them in terms of irreducible representations of the rotational symmetry group, which leads to spherical harmonics and related sets of orthogonal functions. One uses the technique of separation of variables to extract the corresponding solutions for the radial dependencies.

In practice, many fields can be well approximated with a finite number of multipole moments (although an infinite number may be required to reconstruct a field exactly). A typical application is to approximate the field of a localized charge distribution by its monopole and dipole terms. Problems solved once for a given order of multipole moment may be linearly combined to create a final approximate solution for a given source.

See also

• Barnes–Hut simulation
• Fast multipole method
• Laplace expansion
• Legendre polynomials
• Quadrupole magnets are used in particle accelerators
• Solid harmonics
• Toroidal moment
• Dynamic toroidal dipole

References

1. Book: Edmonds, A. R. . Angular Momentum in Quantum Mechanics . 1960 . registration . Princeton University Press. 9780691079127 .
2. Book: Auzinsh. Marcis. Budker. Dmitry. Rochester. Simon. Optically polarized atoms : understanding light-atom interactions. 2010. New York. Oxford. 9780199565122. 100.
3. Okumura. Mitchio. Chan. Man-Chor. Oka. Takeshi. High-resolution infrared spectroscopy of solid hydrogen: The tetrahexacontapole-induced transitions. Physical Review Letters. 2 January 1989. 62. 1. 32–35. 10.1103/PhysRevLett.62.32. 10039541. 1989PhRvL..62...32O.
4. Ikeda. Hiroaki. Suzuki. Michi-To. Arita. Ryotaro. Takimoto. Tetsuya. Shibauchi. Takasada. Matsuda. Yuji. Emergent rank-5 nematic order in URu2Si2. Nature Physics. 3 June 2012. 8. 7. 528–533. 10.1038/nphys2330. 1204.4016. 2012NatPh...8..528I. 119108102 .
5. Book: Thompson, William J. . Angular Momentum . John Wiley & Sons, Inc..
6. Thorne . Kip S. . Reviews of Modern Physics . Multipole Expansions of Gravitational Radiation . April 1980 . 52 . 2 . 299–339 . 10.1103/RevModPhys.52.299 . 1980RvMP...52..299T.
7. Book: Jackson. John David. Classical electrodynamics. 1975. Wiley. New York. 047143132X. 2d. registration.
8. U. Fano and G. Racah, Irreducible Tensorial Sets, Academic Press, New York (1959). p. 31
9. D. M. Brink and G. R. Satchler, Angular Momentum, 2nd edition, Clarendon Press, Oxford, UK (1968). p. 64. See also footnote on p. 90.