Numerov animation
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numerov-2-ani.py
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66
numerov-2-ani.py
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import pylab as pl
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import numpy as np
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import matplotlib.animation as animation
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iterations = 60000 # iterations for approximation
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step = 0.0001 # step size for x
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step_sqrd = pow(step, 2) # square of step size
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n = 2
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epsilon = (n * np.pi) ** 2 / (12 ** 2) # energy level, should be integer n+1/2 for good solutions
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psi = 0.0 # initial value of wave function
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potential = 0.0 # initial value of the potential energy function
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pos = -1 * (iterations - 2) * step # initial value of the position
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potential_past_2 = 0 # epsilon + pos - 2 * step # k_0, potential energy at two steps before current
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potential_past_1 = 0 # epsilon + pos - step # k_1, potential energy at one step before current
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amplitude = 0.1 # initial amplitude of wave function
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psi_past_2 = 0 # y_0, wave function at two steps before current
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psi_past_1 = amplitude # amplitude # y_1, wave function at one step before current
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x_out = [] # list to store x values for plotting
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y_out = [] # list to store y values for plotting
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count = -1 * iterations + 2 # counter for the loop
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fig, ax = pl.subplots()
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ax.set_xlim(-6, 6)
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ax.set_ylim(-1, 1)
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line, = ax.plot(x_out, y_out, label=f'epsilon = {epsilon}')
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def update(frame):
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global pos, potential_past_1, psi_past_1, potential_past_2, psi_past_2, ax
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# Numerov integration loop
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# count += 1
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for i in range(0, 1000, 1):
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pos += step
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potential = epsilon
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# potential = epsilon # potential energy function
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b = step_sqrd / 12 # constant used for Numerov
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# Numerov method to calculate psi at current step
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psi = ((2 * (1 - 5 * b * potential_past_1) * psi_past_1 - (1 + b * potential_past_2) * psi_past_2)
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/ (1 + b * potential))
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# Save for plotting
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x_out.append(pos)
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y_out.append(psi)
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# Shift for next iteration
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psi_past_2 = psi_past_1
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psi_past_1 = psi
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potential_past_2 = potential_past_1
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potential_past_1 = potential
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ax.set_xlim(min(x_out), max(x_out))
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ax.set_ylim(min(y_out), max(y_out))
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line.set_data(x_out, y_out)
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return line,
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# Plot
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ani = animation.FuncAnimation(fig, update, frames=np.arange((-1 * iterations + 2) // 1000, (iterations + 2) // 1000),
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blit=True, repeat=False)
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pl.show()
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64
numerov-ani.py
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numerov-ani.py
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import pylab as pl
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import numpy as np
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import matplotlib.animation as animation
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iterations = 60000 # iterations for approximation
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step = 0.0001 # step size for x
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step_sqrd = pow(step, 2) # square of step size
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epsilon = 2.5 # energy level, should be integer n+1/2 for good solutions
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psi = 0.0 # initial value of wave function
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potential = 0.0 # initial value of the potential energy function
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pos = -1 * (iterations - 2) * step # initial value of the position
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potential_past_2 = epsilon + pos - 2 * step # k_0, potential energy at two steps before current
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potential_past_1 = epsilon + pos - step # k_1, potential energy at one step before current
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amplitude = 0.1 # initial amplitude of wave function
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psi_past_2 = 0 # y_0, wave function at two steps before current
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psi_past_1 = amplitude # y_1, wave function at one step before current
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x_out = [] # list to store x values for plotting
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y_out = [] # list to store y values for plotting
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count = -1 * iterations + 2 # counter for the loop
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fig, ax = pl.subplots()
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ax.set_xlim(-6, 6)
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ax.set_ylim(-1, 1)
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line, = ax.plot(x_out, y_out, label=f'epsilon = {epsilon}')
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def update(frame):
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global pos, potential_past_1, psi_past_1, potential_past_2, psi_past_2, ax
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# Numerov integration loop
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# count += 1
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for i in range(0, 1000, 1):
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pos += step
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potential = 2 * epsilon - pow(pos, 2) # potential energy function
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b = step_sqrd / 12 # constant used for Numerov
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# Numerov method to calculate psi at current step
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psi = ((2 * (1 - 5 * b * potential_past_1) * psi_past_1 - (1 + b * potential_past_2) * psi_past_2)
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/ (1 + b * potential))
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# Save for plotting
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x_out.append(pos)
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y_out.append(psi)
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# Shift for next iteration
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psi_past_2 = psi_past_1
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psi_past_1 = psi
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potential_past_2 = potential_past_1
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potential_past_1 = potential
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ax.set_xlim(min(x_out), max(x_out))
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ax.set_ylim(min(y_out), max(y_out))
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line.set_data(x_out, y_out)
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return line,
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# Plot
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ani = animation.FuncAnimation(fig, update, frames=np.arange((-1 * iterations + 2) // 1000, (iterations - 2) // 1000),
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blit=True, repeat=False)
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pl.show()
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65
numerov-animation.py
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65
numerov-animation.py
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import numpy as np
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import matplotlib.pyplot as plt
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import matplotlib.animation as animation
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iterations = 60000 # iterations for approximation
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step = 0.0001 # step size for x
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step_sqrd = pow(step, 2) # square of step size
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epsilon = 2.5 # energy level, should be integer n+1/2 for good solutions
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psi = 0.0 # initial value of wave function
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potential = 0.0 # initial value of the potential energy function
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pos = -1 * (iterations - 2) * step # initial value of the position
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potential_past_2 = epsilon + pos - 2 * step # k_0, potential energy at two steps before current
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potential_past_1 = epsilon + pos - step # k_1, potential energy at one step before current
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amplitude = 0.1 # initial amplitude of wave function
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psi_past_2 = 0 # y_0, wave function at two steps before current
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psi_past_1 = amplitude # y_1, wave function at one step before current
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x_out = [] # list to store x values for plotting
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y_out = [] # list to store y values for plotting
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fig, ax = plt.subplots()
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line, = ax.plot([], [], label=f'epsilon = {epsilon}')
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ax.set_xlim(-1, 1)
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ax.set_ylim(-1, 1)
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ax.set_xlabel("x")
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ax.set_ylabel("y")
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ax.set_title("Schrodinger Eqn in Harmonic Potential")
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ax.legend(loc=1)
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def init():
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line.set_data([], [])
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return line,
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def update(frame):
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global pos, potential, psi, potential_past_2, potential_past_1, psi_past_2, psi_past_1
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for i in range(frame * 1000, (frame * 1000) + 1000):
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print(i)
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pos += step
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potential = 2 * epsilon - pow(pos, 2) # potential energy function
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b = step_sqrd / 12 # constant used for Numerov
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# Numerov method to calculate psi at current step
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psi = ((2 * (1 - 5 * b * potential_past_1) * psi_past_1 - (1 + b * potential_past_2) * psi_past_2)
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/ (1 + b * potential))
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# Save for plotting
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x_out.append(pos)
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y_out.append(psi)
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# Shift for next iteration
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psi_past_2 = psi_past_1
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psi_past_1 = psi
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potential_past_2 = potential_past_1
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potential_past_1 = potential
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line.set_data(x_out, y_out)
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return line,
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ani = animation.FuncAnimation(fig, update, frames=np.arange(0, (iterations - 2)), init_func=init, blit=True)
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plt.show()
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60
numerov-thing.py
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60
numerov-thing.py
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@ -0,0 +1,60 @@
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import pylab as lab
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import numpy as np
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iterations = 60000 # iterations for approximation
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step = 0.0001 # step size for x
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step_sqrd = pow(step, 2) # square of step size
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well_width = 2
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# try values 1, 2, and 3 for various solutions
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n = 1
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epsilon = (n * np.pi) ** 2 / (well_width ** 2) # energy level, should be integer n+1/2 for good solutions
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psi = 0.0 # initial value of wave function
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potential = 0.0 # initial value of the potential energy function
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pos = -1 * (iterations - 2) * step # initial value of the position
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potential_past_2 = epsilon + pos - 2 * step # k_0, potential energy at two steps before current
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potential_past_1 = epsilon + pos - step # k_1, potential energy at one step before current
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amplitude = 0.1 # initial amplitude of wave function
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psi_past_2 = 0 # y_0, wave function at two steps before current
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psi_past_1 = amplitude # y_1, wave function at one step before current
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x_out = [] # list to store x values for plotting
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y_out = [] # list to store y values for plotting
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count = -1 * iterations + 2 # counter for the loop
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# Numerov integration loop
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while count < iterations - 2:
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count += 1
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pos += step
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# close enough to infinity :)
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potential = 100000000
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if abs(pos) < well_width / 2:
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potential = epsilon # potential energy function
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b = step_sqrd / 12 # constant used for Numerov
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# Numerov method to calculate psi at current step
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psi = ((2 * (1 - 5 * b * potential_past_1) * psi_past_1 - (1 + b * potential_past_2) * psi_past_2)
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/ (1 + b * potential))
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# Save for plotting
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x_out.append(pos)
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y_out.append(psi)
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# Shift for next iteration
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psi_past_2 = psi_past_1
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psi_past_1 = psi
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potential_past_2 = potential_past_1
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potential_past_1 = potential
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# Plot
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lab.figure(1)
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lab.plot(x_out, y_out, label=f'epsilon = {epsilon}')
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lab.xlabel("x")
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lab.ylabel("y")
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lab.title("Schrodinger Eqn in Harmonic Potential")
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lab.legend(loc=1)
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lab.show()
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