| from sympy.core.numbers import Float |
| from sympy.core.singleton import S |
| from sympy.functions.combinatorial.factorials import factorial |
| from sympy.functions.elementary.exponential import exp |
| from sympy.functions.elementary.miscellaneous import sqrt |
| from sympy.functions.special.polynomials import assoc_laguerre |
| from sympy.functions.special.spherical_harmonics import Ynm |
|
|
|
|
| def R_nl(n, l, r, Z=1): |
| """ |
| Returns the Hydrogen radial wavefunction R_{nl}. |
| |
| Parameters |
| ========== |
| |
| n : integer |
| Principal Quantum Number which is |
| an integer with possible values as 1, 2, 3, 4,... |
| l : integer |
| ``l`` is the Angular Momentum Quantum Number with |
| values ranging from 0 to ``n-1``. |
| r : |
| Radial coordinate. |
| Z : |
| Atomic number (1 for Hydrogen, 2 for Helium, ...) |
| |
| Everything is in Hartree atomic units. |
| |
| Examples |
| ======== |
| |
| >>> from sympy.physics.hydrogen import R_nl |
| >>> from sympy.abc import r, Z |
| >>> R_nl(1, 0, r, Z) |
| 2*sqrt(Z**3)*exp(-Z*r) |
| >>> R_nl(2, 0, r, Z) |
| sqrt(2)*(-Z*r + 2)*sqrt(Z**3)*exp(-Z*r/2)/4 |
| >>> R_nl(2, 1, r, Z) |
| sqrt(6)*Z*r*sqrt(Z**3)*exp(-Z*r/2)/12 |
| |
| For Hydrogen atom, you can just use the default value of Z=1: |
| |
| >>> R_nl(1, 0, r) |
| 2*exp(-r) |
| >>> R_nl(2, 0, r) |
| sqrt(2)*(2 - r)*exp(-r/2)/4 |
| >>> R_nl(3, 0, r) |
| 2*sqrt(3)*(2*r**2/9 - 2*r + 3)*exp(-r/3)/27 |
| |
| For Silver atom, you would use Z=47: |
| |
| >>> R_nl(1, 0, r, Z=47) |
| 94*sqrt(47)*exp(-47*r) |
| >>> R_nl(2, 0, r, Z=47) |
| 47*sqrt(94)*(2 - 47*r)*exp(-47*r/2)/4 |
| >>> R_nl(3, 0, r, Z=47) |
| 94*sqrt(141)*(4418*r**2/9 - 94*r + 3)*exp(-47*r/3)/27 |
| |
| The normalization of the radial wavefunction is: |
| |
| >>> from sympy import integrate, oo |
| >>> integrate(R_nl(1, 0, r)**2 * r**2, (r, 0, oo)) |
| 1 |
| >>> integrate(R_nl(2, 0, r)**2 * r**2, (r, 0, oo)) |
| 1 |
| >>> integrate(R_nl(2, 1, r)**2 * r**2, (r, 0, oo)) |
| 1 |
| |
| It holds for any atomic number: |
| |
| >>> integrate(R_nl(1, 0, r, Z=2)**2 * r**2, (r, 0, oo)) |
| 1 |
| >>> integrate(R_nl(2, 0, r, Z=3)**2 * r**2, (r, 0, oo)) |
| 1 |
| >>> integrate(R_nl(2, 1, r, Z=4)**2 * r**2, (r, 0, oo)) |
| 1 |
| |
| """ |
| |
| n, l, r, Z = map(S, [n, l, r, Z]) |
| |
| n_r = n - l - 1 |
| |
| a = 1/Z |
| r0 = 2 * r / (n * a) |
| |
| C = sqrt((S(2)/(n*a))**3 * factorial(n_r) / (2*n*factorial(n + l))) |
| |
| |
| |
| return C * r0**l * assoc_laguerre(n_r, 2*l + 1, r0).expand() * exp(-r0/2) |
|
|
|
|
| def Psi_nlm(n, l, m, r, phi, theta, Z=1): |
| """ |
| Returns the Hydrogen wave function psi_{nlm}. It's the product of |
| the radial wavefunction R_{nl} and the spherical harmonic Y_{l}^{m}. |
| |
| Parameters |
| ========== |
| |
| n : integer |
| Principal Quantum Number which is |
| an integer with possible values as 1, 2, 3, 4,... |
| l : integer |
| ``l`` is the Angular Momentum Quantum Number with |
| values ranging from 0 to ``n-1``. |
| m : integer |
| ``m`` is the Magnetic Quantum Number with values |
| ranging from ``-l`` to ``l``. |
| r : |
| radial coordinate |
| phi : |
| azimuthal angle |
| theta : |
| polar angle |
| Z : |
| atomic number (1 for Hydrogen, 2 for Helium, ...) |
| |
| Everything is in Hartree atomic units. |
| |
| Examples |
| ======== |
| |
| >>> from sympy.physics.hydrogen import Psi_nlm |
| >>> from sympy import Symbol |
| >>> r=Symbol("r", positive=True) |
| >>> phi=Symbol("phi", real=True) |
| >>> theta=Symbol("theta", real=True) |
| >>> Z=Symbol("Z", positive=True, integer=True, nonzero=True) |
| >>> Psi_nlm(1,0,0,r,phi,theta,Z) |
| Z**(3/2)*exp(-Z*r)/sqrt(pi) |
| >>> Psi_nlm(2,1,1,r,phi,theta,Z) |
| -Z**(5/2)*r*exp(I*phi)*exp(-Z*r/2)*sin(theta)/(8*sqrt(pi)) |
| |
| Integrating the absolute square of a hydrogen wavefunction psi_{nlm} |
| over the whole space leads 1. |
| |
| The normalization of the hydrogen wavefunctions Psi_nlm is: |
| |
| >>> from sympy import integrate, conjugate, pi, oo, sin |
| >>> wf=Psi_nlm(2,1,1,r,phi,theta,Z) |
| >>> abs_sqrd=wf*conjugate(wf) |
| >>> jacobi=r**2*sin(theta) |
| >>> integrate(abs_sqrd*jacobi, (r,0,oo), (phi,0,2*pi), (theta,0,pi)) |
| 1 |
| """ |
|
|
| |
| n, l, m, r, phi, theta, Z = map(S, [n, l, m, r, phi, theta, Z]) |
| |
| if n.is_integer and n < 1: |
| raise ValueError("'n' must be positive integer") |
| if l.is_integer and not (n > l): |
| raise ValueError("'n' must be greater than 'l'") |
| if m.is_integer and not (abs(m) <= l): |
| raise ValueError("|'m'| must be less or equal 'l'") |
| |
| return R_nl(n, l, r, Z)*Ynm(l, m, theta, phi).expand(func=True) |
|
|
|
|
| def E_nl(n, Z=1): |
| """ |
| Returns the energy of the state (n, l) in Hartree atomic units. |
| |
| The energy does not depend on "l". |
| |
| Parameters |
| ========== |
| |
| n : integer |
| Principal Quantum Number which is |
| an integer with possible values as 1, 2, 3, 4,... |
| Z : |
| Atomic number (1 for Hydrogen, 2 for Helium, ...) |
| |
| Examples |
| ======== |
| |
| >>> from sympy.physics.hydrogen import E_nl |
| >>> from sympy.abc import n, Z |
| >>> E_nl(n, Z) |
| -Z**2/(2*n**2) |
| >>> E_nl(1) |
| -1/2 |
| >>> E_nl(2) |
| -1/8 |
| >>> E_nl(3) |
| -1/18 |
| >>> E_nl(3, 47) |
| -2209/18 |
| |
| """ |
| n, Z = S(n), S(Z) |
| if n.is_integer and (n < 1): |
| raise ValueError("'n' must be positive integer") |
| return -Z**2/(2*n**2) |
|
|
|
|
| def E_nl_dirac(n, l, spin_up=True, Z=1, c=Float("137.035999037")): |
| """ |
| Returns the relativistic energy of the state (n, l, spin) in Hartree atomic |
| units. |
| |
| The energy is calculated from the Dirac equation. The rest mass energy is |
| *not* included. |
| |
| Parameters |
| ========== |
| |
| n : integer |
| Principal Quantum Number which is |
| an integer with possible values as 1, 2, 3, 4,... |
| l : integer |
| ``l`` is the Angular Momentum Quantum Number with |
| values ranging from 0 to ``n-1``. |
| spin_up : |
| True if the electron spin is up (default), otherwise down |
| Z : |
| Atomic number (1 for Hydrogen, 2 for Helium, ...) |
| c : |
| Speed of light in atomic units. Default value is 137.035999037, |
| taken from https://arxiv.org/abs/1012.3627 |
| |
| Examples |
| ======== |
| |
| >>> from sympy.physics.hydrogen import E_nl_dirac |
| >>> E_nl_dirac(1, 0) |
| -0.500006656595360 |
| |
| >>> E_nl_dirac(2, 0) |
| -0.125002080189006 |
| >>> E_nl_dirac(2, 1) |
| -0.125000416028342 |
| >>> E_nl_dirac(2, 1, False) |
| -0.125002080189006 |
| |
| >>> E_nl_dirac(3, 0) |
| -0.0555562951740285 |
| >>> E_nl_dirac(3, 1) |
| -0.0555558020932949 |
| >>> E_nl_dirac(3, 1, False) |
| -0.0555562951740285 |
| >>> E_nl_dirac(3, 2) |
| -0.0555556377366884 |
| >>> E_nl_dirac(3, 2, False) |
| -0.0555558020932949 |
| |
| """ |
| n, l, Z, c = map(S, [n, l, Z, c]) |
| if not (l >= 0): |
| raise ValueError("'l' must be positive or zero") |
| if not (n > l): |
| raise ValueError("'n' must be greater than 'l'") |
| if (l == 0 and spin_up is False): |
| raise ValueError("Spin must be up for l==0.") |
| |
| if spin_up: |
| skappa = -l - 1 |
| else: |
| skappa = -l |
| beta = sqrt(skappa**2 - Z**2/c**2) |
| return c**2/sqrt(1 + Z**2/(n + skappa + beta)**2/c**2) - c**2 |
|
|