2.6. Dispersion Coefficients Near Surfaces

In this tutorial we reproduce the results depicted in Figure 5 from J. Block and S. Scheel “van der Waals interaction potential between Rydberg atoms near surfaces” Phys. Rev. A 96, 062509 (2017). We calculate the van der Waals \(C_6\)-coefficient between two Rubidium Rydberg atoms that are equidistantly placed in front of a perfect mirror (i.e. in horizontal alignment in front of a perfectly conducting plate). One finds that the relevant length scale is interatomic distance devided by distance from surface and that for decreasing surface distance the \(C_6\) coefficient is significantly reduced.

As described in the introduction, we start our code with some preparations and load the necessary modules.

%matplotlib inline

# Arrays
import numpy as np

# Plotting
import matplotlib.pyplot as plt

# Operating system interfaces
import os

# pairinteraction :-)
from pairinteraction import pireal as pi

# Create cache for matrix elements
if not os.path.exists("./cache"):
    os.makedirs("./cache")
cache = pi.MatrixElementCache("./cache")

The plate lies in the \(xy\)-plane with the surface at \(z = 0\). The atoms lie in the \(xz\)-plane with \(z>0\).

We can set the angle between the interatomic axis and the z-axis theta and the center of mass distance from the surface distance_surface. distance_atom defines the interatomic distances for which the pair potential is plotted. The units of the respective quantities are given as comments.

Be careful: theta = np.pi/2 corresponds to horizontal alignment of the two atoms with respect to the surface. For different angles, large interatomic distances distance_atom might lead to one of the atoms being placed inside the plate. Make sure that distance_surface is larger than distance_atom*np.cos(theta)/2

theta = np.pi/2 # rad
distance_atoms = 10 # µm
distance_surface = np.linspace(distance_atoms*np.abs(np.cos(theta))/2, 2*distance_atoms,30) # µm

Next we define the state that we are interested in using pairinteraction’s StateOne class . As shown in Figures 4 and 5 of Phys. Rev. A 96, 062509 (2017) we expect changes of about 50% for the \(C_6\) coefficient of the \(|69s_{1/2},m_j=1/2;72s_{1/2},m_j=1/2\rangle\) pair state of Rubidium, so this provides a good example.

We set up the one-atom system using restrictions of energy, main quantum number n and angular momentum l. This is done by means of the restrict... functions in SystemOne.

state_one1 = pi.StateOne("Rb", 69, 0, 0.5, 0.5)
state_one2 = pi.StateOne("Rb", 72, 0, 0.5, 0.5)

# Set up one-atom system
system_one = pi.SystemOne(state_one1.getSpecies(), cache)
system_one.restrictEnergy(min(state_one1.getEnergy(),state_one2.getEnergy()) - 30, \
                          max(state_one1.getEnergy(),state_one2.getEnergy()) + 30)
system_one.restrictN(min(state_one1.getN(),state_one2.getN()) - 3, \
                     max(state_one1.getN(),state_one2.getN()) + 3)
system_one.restrictL(min(state_one1.getL(),state_one2.getL()) - 1, \
                     max(state_one1.getL(),state_one2.getL()) + 1)

The pair state state_two is created from the one atom states state_one1 and state_one2 using the StateTwo class.

From the previously set up system_one we define system_two using SystemTwo class. This class also contains methods set.. to set angle, distance, surface distance and to enableGreenTensor in order implement a surface.

# Set up pair state
state_two = pi.StateTwo(state_one1, state_one2)

# Set up two-atom system
system_two = pi.SystemTwo(system_one, system_one, cache)
system_two.restrictEnergy(state_two.getEnergy() - 3, state_two.getEnergy() + 3)

system_two.setAngle(theta)
system_two.setDistance(distance_atoms)
system_two.setSurfaceDistance(distance_surface[0])
system_two.enableGreenTensor(True)
system_two.buildInteraction()

We calculate the \(C_6\) coefficients. The energyshift is given by the difference between the interaction energy at given surface_distance and the unperturbed energy of the two atom state state_two.getEnergy(). The \(C_6\) coefficient is then given by the product of energyshift and distance_atoms**6.

idx is the index of the two atom state. The command getOverlap(state_two, 0, -theta, 0) rotates the quantisation axis of state_two by theta around the y-axis. The rotation is given by the Euler angles (0, -theta, 0) in zyz convention. The negative sign of theta is needed because the Euler angles used by pairinteraction represent a rotation of the coordinate system. Thus, the quantisation axis has to be rotated by the inverse angle.

# Calculate C6 coefficients
C6 = []
for d in distance_surface:
    system_two.setSurfaceDistance(d)
    system_two.diagonalize()
    idx = np.argmax(system_two.getOverlap(state_two, 0, -theta, 0))
    energyshift = system_two.getHamiltonian().diagonal()[idx]-state_two.getEnergy()
    C6.append(energyshift*distance_atoms**6)
# Plot results
plt.plot(distance_surface/distance_atoms, np.abs(C6))
plt.xlim(min(distance_surface/distance_atoms), max(distance_surface/distance_atoms))
plt.xlabel("distance to surface / interatomic distance")
plt.ylabel("|C$_6$| (GHz $\mu m^6$)");
_images/vdw_near_surface_12_0.png