Cubic harmonic

Cubic harmonics

In fields like computational chemistry and solid-state and condensed matter physics the so-called atomic orbitals, or spin-orbitals, as they appear in textbooks[1][2][3] on quantum physics, are often partially replaced by cubic harmonics for a number of reasons.

Introduction

The l(l+1) hydrogen-like atomic orbitals with principal quantum number n and angular momentum quantum number l are often expressed as

\psi_{nlm}(\bold{r}) = R_{nl}(r) Y_l^m(\theta,\varphi)

in which the R_{nl}(r) is the radial part of the wave function and Y_l^m(\theta,\varphi) is the angular dependent part. The Y_l^m(\theta,\varphi) are the spherical harmonics, which are solutions of the angular momentum operator. The spherical harmonics are representations of functions of the full rotation group SO(3)[4] with rotational symmetry. In many fields of physics and chemistry these spherical harmonics are replaced by cubic harmonics because the rotational symmetry of the atom and its environment are distorted or because cubic harmonics offer computational benefits.

Symmetry and coordinate system

In many cases, especially in chemistry and solid-state and condensed-matter physics, the system under investigation doesn't have rotational symmetry. Often it has some kind of lower symmetry, with a special point group representation, or it has no spatial symmetry at all. Biological and biochemical systems, like amino acids and enzymes often belong to low molecular symmetry point groups. The solid crystals of the elements often belong to the space groups and point groups with high symmetry. (Cubic harmonics representations are often listed and referenced in point group tables.) The system has at least a fixed orientation in three-dimensional Euclidean space. Therefore the coordinate system that is used in such cases is most often a Cartesian coordinate system instead of a spherical coordinate system. In a Cartesian coordinate system the atomic orbitals are often expressed as

\psi_{nlc}(\bold{r}) = R_{nl}(r) X_{lc}(\bold{r})

with the cubic harmonics,[5][6][7] X_{lc}(\bold{r}), as a basis set. LCAO and MO calculations in computational chemistry or tight binding calculations in solid-state physics use cubic harmonics as an atomic orbital basis. The indices lc are denoting some kind of Cartesian representation.

Basis transformations

For the representations of the spherical harmonics a spherical coordinate system is chosen with a principal axis in the z-direction. For the cubic harmonics this axis is also the most convenient choice. For states of higher angular momentum quantum number l and a higher dimension of l(l+1) the number of possible rotations or basis transformations in Hilbert space grows and so does the number of possible orthogonal representations that can be constructed on the basis of the l(l+1)-dimensional spherical harmonics basis set. There is more freedom to choose a representation that fits the point group symmetry of the problem. The cubic representations that are listed in the table are a result of the transformations, which are 45° 2D rotations and a 90° rotation to the real axis if necessary, like

X_{lc}(\bold{r}) = Y_l^0
X_{lc'}(\bold{r}) = \frac{1}{i^{n_{c'}}\sqrt{2}}\left(Y_l^m - Y_l^{-m}\right)
X_{lc''}(\bold{r}) = \frac{1}{i^{n_{c''}}\sqrt{2}}\left(Y_l^m + Y_l^{-m}\right)

A substantial number of the spherical harmonics are listed in the Table of spherical harmonics.

Computational benefits

Ferricyanide ion, used to make 'Turnbull's blue' with an octahedrically surrounded central Fe3+-ion.

First of all, the cubic harmonics are real functions, while spherical harmonics are complex functions. The complex numbers are two-dimensional with a real part and an imaginary part. Complex numbers offer very handsome and effective tools to tackle mathematical problems analytically but they are not very effective when they are used for numerical calculations. Skipping the imaginary part saves half the calculational effort in summations, a factor of four in multiplications and often factors of eight or even more when it comes to computations involving matrices.

The cubic harmonics often fit the symmetry of the potential or surrounding of an atom. A common surrounding of atoms in solids and chemical complexes is an octahedral surrounding with an octahedral cubic point group symmetry. The representations of the cubic harmonics often have a high symmetry and multiplicity so operations like integrations can be reduced to a limited, or irreducible, part of the domain of the function that has to be evaluated. A problem with the 48-fold octahedral Oh symmetry can be calculated much faster if one limits a calculation, like an integration, to the irreducible part of the domain of the function.

Table of cubic harmonics

The s-orbitals

The s-orbitals only have a radial part.

\psi_{n00}(\bold{r}) = R_{n0}(r) Y_0^0
s = X_{00} = Y_0^0 = \frac{1}{\sqrt{4\pi}}
n=1 2 3 4 5 6 7
Rn0

The p-orbitals

The three p-orbitals are atomic orbitals with an angular momentum quantum number ℓ = 1. The cubic harmonic expression of the p-orbitals

p_z = N_1^c \frac{z}{r} = Y_1^0
p_x = N_1^c \frac{x}{r} = \frac{1}{\sqrt{2}} \left(Y_1^{-1}-Y_1^1\right)
p_y = N_1^c \frac{y}{r} = \frac{i}{\sqrt{2}} \left(Y_1^{-1}+Y_1^1\right)

with

N_1^c = \left(\frac{3}{4\pi}\right)^{1/2}
pz px py

The d-orbitals

The five d-orbitals are atomic orbitals with an angular momentum quantum number ℓ = 2. The angular part of the d-orbitals are often expressed like

\psi_{n2c}(\bold{r}) = R_{n2}(r) X_{2c}(\bold{r})

The angular part of the d-orbitals are the cubic harmonics X_{2c}(\bold{r})

d_{z^2} = N_2^c \frac{3z^2 - r^2}{2r^2\sqrt{3}} = Y_2^0
d_{xz} = N_2^c \frac{xz}{r^2} = \frac{1}{\sqrt{2}} \left(Y_2^{-1}-Y_2^1\right)
d_{yz} = N_2^c \frac{yz}{r^2} = \frac{i}{\sqrt{2}} \left(Y_2^{-1}+Y_2^1\right)
d_{xy} = N_2^c \frac{xy}{r^2} = \frac{i}{\sqrt{2}} \left(Y_2^{-2}-Y_2^2\right)
d_{x^2-y^2} = N_2^c \frac{x^2 - y^2}{2r^2} = \frac{1}{\sqrt{2}} \left(Y_2^{-2}+Y_2^2\right)

with

N_2^c = \left(\frac{15}{4\pi}\right)^{1/2}
dz2 dxz dyz dxy dx2-y2

The f-orbitals

The seven f-orbitals are atomic orbitals with an angular momentum quantum number ℓ = 3. often expressed like

\psi_{n3c}(\bold{r}) = R_{n3}(r) X_{3c}(\bold{r})

The angular part of the f-orbitals are the cubic harmonics X_{3c}(\bold{r}). In many cases different linear combinations of spherical harmonics are chosen to construct a cubic f-orbital basis set.

f_{z^3} = N_3^c \frac{z (2 z^2 - 3 x^2 - 3 y^2)}{2 r^3 \sqrt{15}} = Y_3^0
f_{xz^2} = N_3^c \frac{x (4 z^2 - x^2 - y^2)}{2 r^3 \sqrt{10}} = \frac{1}{\sqrt{2}}\left(Y_3^{-1}-Y_3^1\right)
f_{yz^2} = N_3^c \frac{y (4 z^2 - x^2 - y^2)}{r^3 \sqrt{10}} = \frac{i}{\sqrt{2}}\left(Y_3^{-1}+Y_3^1\right)
f_{xyz} = N_3^c \frac{xyz}{r^3} = \frac{i}{\sqrt{2}}\left(Y_3^{-2}-Y_3^2\right)
f_{z(x^2-y^2)} = N_3^c \frac{z \left( x^2 - y^2 \right)}{2 r^3} = \frac{1}{\sqrt{2}}\left(Y_3^{-2}+Y_3^2\right)
f_{x(x^2-3y^2)} = N_3^c \frac{x \left( x^2 - 3 y^2 \right)}{2 r^3 \sqrt{6}} = \frac{1}{\sqrt{2}}\left(Y_3^{-3}-Y_3^3\right)
f_{y(3x^2-y^2)} = N_3^c \frac{y \left( 3 x^2 - y^2 \right)}{2 r^3 \sqrt{6}} = \frac{i}{\sqrt{2}}\left(Y_3^{-3}+Y_3^3\right)

with

N_3^c = \left(\frac{105}{4\pi}\right)^{1/2}
fz3 fxz2 fyz2 fxyz fz(x2-y2) fx(x2-3y2) fy(3x2-y2)

See also

References

  1. ↑ Albert Messiah (1999). Quantum Mechanics. Dover Publications. ISBN 0-486-40924-4.
  2. ↑ Stephen Gasiorowicz (1974). Quantum Physics. Wiley & Sons. ISBN 0-471-29281-8.
  3. ↑ Eugen Merzbacher (1961). Quantum Mechanics. Wiley & Sons. ISBN 0-471-59670-1.
  4. ↑ D. M. Brink & G. R. Satchler (1993). Angular Momentum. Oxford University Press. ISBN 0-19-851759-9.
  5. ↑ R. McWeeny (1978). Methods of Molecular Quantum Mechanics. Academic Press. ISBN 0-12-486552-6.
  6. ↑ J. Muggli (1972). "Cubic harmonics as linear combinations of spherical harmonics". Zeitschrift für Angewandte Mathematik und Physik (Springer-Verlag) 23 (2): 311–317. Bibcode:1972ZaMP...23..311M. doi:10.1007/BF01593094.
  7. ↑ T. Kwiatkowski, S. Olszewski, A. Wierzbicki (1977). "Cubic harmonics in Cartesian coordinates". International Journal of Quantum Chemistry 11: 21. doi:10.1002/qua.560110104.
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