Exercise Eigenvalues

import time

import matplotlib.pyplot as plt
import numpy as np
import scipy.linalg as scl
import scipy.sparse as scsp

def get_dimension(dim):
    # converts short notion (only 1 int or 1 tuple for two times same index) into 2-tuple
    # INPUT : 2-tuple, 1-tuple or int
    # OUTPUT: 2-tuple
    if str(type(dim)) == "<class 'tuple'>":
        try:
            n = dim[1]
        except:
            n = dim[0]
        m = dim[0]
    else:
        m = dim
        n = dim
    return (m, n)


# Test function:
print(get_dimension((2, 3)), "should be: (2, 3)")
print(get_dimension(2), "should be: (2, 2)")
print(get_dimension((2)), "should be: (2, 2)")

def Create_random_matrix(dim, data_type="real"):
    # Returns a real or complex matrix with uniform or wide range distribution
    # INPUT :- dim:  number or 1-tuple or 2- tuple
    #        - data_type: "real or complex"
    #        - distribution "uniform" in [0,1) or "wide_range" in (-10^10, 10^10), approximated log distributed
    # OUTPUT: Matrix of dimension dim with real or complex entries

    dim = get_dimension(dim)

    A = np.random.random(dim)
    if data_type == "complex":
        A = A + 1j * np.random.random()
    if data_type == "symmetric":
        A = A + A.T
    if data_type == "diag_dominant":
        row_sum = np.sum(A, axis=1)
        A = A + A.T
        for i in range(dim[0]):
            A[i, i] = row_sum[i] + 0.5
    return A


# test function
A = Create_random_matrix(2, "complex")
print(A)
B = Create_random_matrix((2, 1))
print(B)

# Some index manipulations, used later
def index_2d_to_1d(i, j, n):
    """
    Convert 2D index to 1D index
    Input:
        i is the row index
        j is the column index
        n is the number of columns
    Output:
        1D index
    """
    return i * n + j


def index_1d_to_2d(index, n):
    """
    Convert 1D index to 2D index
    Input:
        index is the 1D index
        n is the number of columns
    Output:
        2D index
    """
    return (index // n, index % n)

def laplace_matrix_square(n):
    """
    returns the Laplace operator discretized on a grid of n*n points
    Input:
        n is the number of points in each dimension
    Output:
        A is the Laplace matrix
    """
    A = np.zeros((n * n, n * n), dtype=float)
    for i in range(n):
        for j in range(n):
            # inside the domain
            A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j, n)] = -4.0
            if i > 0 and j > 0 and i < n - 1 and j < n - 1:
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i - 1, j, n)] = 1.0
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i + 1, j, n)] = 1.0
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j - 1, n)] = 1.0
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j + 1, n)] = 1.0
                continue
            ## on the boundary
            # top boundary
            if i == 0:
                if j == 0:  # top left corner
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i + 1, j, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j + 1, n)] = 1

                elif j == n - 1:  # top right corner
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i + 1, j, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j - 1, n)] = 1

                else:
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i + 1, j, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j - 1, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j + 1, n)] = 1
                continue
            # bottom boundary

            if i == n - 1:
                if j == 0:  # bottom left corner
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i - 1, j, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j + 1, n)] = 1
                    continue
                elif j == n - 1:  # bottom right corner
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i - 1, j, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j - 1, n)] = 1
                    continue
                else:
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i - 1, j, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j - 1, n)] = 1
                    A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j + 1, n)] = 1
                    continue
            # left boundary
            if j == 0:
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i - 1, j, n)] = 1
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i + 1, j, n)] = 1
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j + 1, n)] = 1
            # right boundary
            if j == n - 1:
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i - 1, j, n)] = 1
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i + 1, j, n)] = 1
                A[index_2d_to_1d(i, j, n), index_2d_to_1d(i, j - 1, n)] = 1

    return A / n**2

n = 5
A = laplace_matrix_square(n)
plt.matshow(A)
plt.colorbar()

def plot_eigenfunctions(A, n_max=6):  # just another helper function, skip
    plot_row = n_max // 3 + np.min([n_max % 3, 1])
    print(plot_row)
    fig, ax = plt.subplots(plot_row, 3, figsize=(15, 5 * plot_row))
    n = int(np.sqrt(A.shape[0]))

    for i in range(n_max):
        B = np.zeros((n, n))
        for j in range(n**2):
            coords = index_1d_to_2d(j, n)
            B[coords[0], coords[1]] = A[j, i]
        # plot
        row = i // 3
        col = i % 3
        im = ax[row, col].matshow(B)
        ax[row, col].set_title("Eigenfunction " + str(i + 1))
        fig.colorbar(im, ax=ax[row, col])
    plt.show()

n = 100
A = laplace_matrix_square(n)
eigenvalues = np.ones(n**2)
eigenvectors = np.zeros((n**2, n**2))
# HERE your Code
eigenvalues, eigenvectors = np.linalg.eigh(A)  # scl.eig(A)
mask = np.argsort(eigenvalues)
eigenvalues = eigenvalues[mask[::-1]]
eigenvectors = eigenvectors[:, mask[::-1]]


print("Eigenvalues: \n", np.real(eigenvalues))
plot_eigenfunctions(eigenvectors)

test_capacity = True

n = 4
times = []
while test_capacity:
    time_start = time.time()
    A = laplace_matrix_square(n)
    eigenvalues, eigenvectors = scl.eig(A)
    time_end = time.time()
    times.append(time_end - time_start)
    if (time_end - time_start) > 10:
        test_capacity = False
    n = n * 2
n_Max = n // 2
print("What??? Only " + str(n_Max))

sizes = np.arange(2, len(times) + 2, 1)
plt.title("Time to calculate eigenvalues")
plt.plot(2 ** (sizes), times)

def Householder_matrix(v):
    # Create Matrix Q_v as described above.
    # INPUT: v 1d-array or 2d-array with one column or one row
    # OUPUT: Q Householdermatrix of v

    v = v.copy()  # do not overwrite original matrix
    n = len(v)
    v = v.reshape(
        (n)
    )  # reshape, because tensorprod gives different results for (n) and (n,1) dimension

    if np.linalg.norm(v) == 0:
        return np.eye(n)
    # modify first component
    if v[0] == 0:
        sign = 1
    else:
        sign = v[0] / np.abs(v[0])
    v[0] += sign * np.linalg.norm(v)  # linalg.norm calculates the l2 norm of a vector
    v = v / np.linalg.norm(v)
    # calc Q
    Q = np.eye(n) - 2.0 * np.tensordot(
        v, np.conj(v), axes=0
    )  # tensorprod does w w^T multiplication
    return Q

fig, ax = plt.subplots(1, 3, figsize=(15, 5))

# test case 1
print("test case 1")
v = Create_random_matrix((4, 1))
print("v=\n", v)
Q = Householder_matrix(v)
im = ax[0].matshow(np.abs(Q))
ax[0].set_title("Case 1: |Q_v| ")
fig.colorbar(im, ax=ax[0])
# check errors
error_sym = np.max(np.abs(Q - np.conj(Q.T)))
error_id = np.max(np.abs(Q @ Q - np.eye(v.shape[0])))
error_refl = np.max(np.abs((Q @ v)[1:]))
print("maximal error: |Q-Q^*| = \t", error_sym)
print("maximal error: |QQ-id|=\t", error_id)
print("zero after reflection |Qv|=\t", error_refl)
assert error_sym < 1e-10
assert error_id < 1e-10
assert error_refl < 1e-10

# test case 2
print("\ntest case 2")
v = Create_random_matrix((4, 1))
v[0:2] = np.array([0, 0]).reshape((2, 1))
print("\n\n\nv_2=\n", v)
Q = Householder_matrix(v)
im = ax[1].matshow(np.abs(Q))
ax[1].set_title("Case 2: |Q_v2|")
fig.colorbar(im, ax=ax[1])

print("maximal error: |Q-Q^*| = \t", np.max(np.abs(Q - np.conj(Q.T))))
print("maximal error |QQ-id|=\t", np.max(np.abs(Q @ Q - np.eye(v.shape[0]))))
print("2nd column ofQ under diagonal: \t", Q[2:, 1], "should be zero")
assert np.max(np.abs(Q[2:, 1])) <= 1e-10

# test case 3
print("\ntest case 3")
v = np.zeros(4)
Q = Householder_matrix(v)
im = ax[2].matshow(np.abs(Q))
ax[2].set_title("Case 3: |Q_v3|")
fig.colorbar(im, ax=ax)
print("\n\nv_3= \n", v)
print("maximal error Q-id=\t", np.max(np.abs(Q - np.eye(4))))

x = np.array([1, 2, 2])
A = np.random.rand(3, 3)
A[:, 0] = x
print(f"A:\n{A}")
P1 = Householder_matrix(x)
print(P1 @ A)
# print(f"P1.T * A * P1:\n{P1.T @ A @ P1}")
# # # print(f"Iteration 1:\n{}")
# # # print(f"Iteration 2:\n{Householder_matrix(A[:, 0]) @ A}")
# print(f"Hessenberg:\n{scl.hessenberg(A)}")

def Hessenberg_form(A):
    # This function calculates the Hessenberg form via Housholder transformations of a complex matrix.
    # The entries of the inputmatrix will be overwritten by the Hessenbergform.
    # INPUT : real/complex squared Matrix A
    # OUTPUT: transfomation matrix

    n = A.shape[0]
    # store full transformation in matrix
    Q_res = np.eye(n, dtype=A.dtype)
    H = A.copy()
    # A = Q_res @ A
    # for k in range(n):
    #     Q[:, k] = Householder_matrix(A[k:, k])

    # HERE your code|
    return np.conj(Q_res.T)

# Test your implementation
fig, ax = plt.subplots(1, 2, figsize=(10, 5))
A = Create_random_matrix(5)
ax[0].matshow(A)
ax[0].set_title("A before")
B = A.copy()
Q = Hessenberg_form(A)
im = ax[1].matshow(A)
ax[1].set_title("A in Hessenbergform")
fig.colorbar(im, ax=ax)
plt.show()
print("maximal error of Q*AQ-A_h\t", np.max(np.abs(np.conj(Q.T) @ B @ Q - A)))

n = 5
A = laplace_matrix_square(n)
Hessenberg_form(A)


plt.matshow(A)
plt.title("A in Hessenbergform")
plt.colorbar()
plt.show()

def Givens_rotation(v):
    # This function calculates a rotation matrix,
    # such that the lower component of a 2-dimensional vector is 0
    # This is the complex version
    # INPUT : 2-dimensional vector
    # OUTPUT: 2x2-matrix

    v = v.copy()  # not overwrite the matrix elements
    v = v.reshape((2))  # such that entries are callable
    Q = np.eye(2)
    # HERE your code
    return Q

v = Create_random_matrix((2, 1))
print("v=\n", v)
Q = Givens_rotation(v)
print("Q=\n", Q)
print("Qv = \n", Q @ v)

def QR_decomposition_Hess(A):
    # This function calculates the QR decomposition of a matrix in Hessenberg form and store the values of R in A
    # INPUT : A, nxn matrix in Hessenberg form
    # OUTPUT: Q*, nxn matrix, orthogonal

    n = A.shape[0]
    Q_res = np.eye(n, dtype=A.dtype)

    # HERE your Code

    return np.conj(Q_res.T)

# test your function
fig, ax = plt.subplots(1, 3, figsize=(15, 5))

A = laplace_matrix_square(5)
Q_1 = Hessenberg_form(A)
B = A.copy()
# original matrix
ax[0].matshow(np.abs(A))
ax[0].set_title("A in Hessenberg form")

Q_2 = QR_decomposition_Hess(A)
# Q
ax[1].matshow(np.abs(Q_2))
ax[1].set_title("Q")
# R
im = ax[2].matshow(np.abs(A))
ax[2].set_title("R")
fig.colorbar(im, ax=ax)
error_qr = np.max(np.abs(Q_2 @ A - B))
print("maximal error |QR-A|: \t", error_qr)
assert error_qr < 1e-10

def QR_iteration_slow(A, eps=1e-6, max_Iterations=10000):
    # This function iterates the basic QR algorithm, until either the entries on the first sub diagonal
    # are small enough or Max iter reached The matrix A will be overwritten.
    # INPUT : - A: squared Matrix in hessenberg form
    #         - eps: if no diag entry changes more than eps, than the algorithm is converged
    #         - max_iterations: If this number is reached, it aborts the iteration and gives a warning
    # OUTPUT: - Q, nxn Matrix, similarity transformation
    #         - Iter : number of Iterations

    # define values, for the computation

    n = A.shape[0]
    Iter = 0
    error_ev = 1
    diagvals = np.diag(A).copy()
    Q_res = np.eye(n)

    # start QR iteration
    while error_ev > eps and Iter < max_Iterations:
        Iter += 1

        # HERE your code

        # preparation for next iteration
        error_ev = np.max(np.abs(diagvals - np.diag(A)))
        diagvals = np.diag(A).copy()

    if Iter == max_Iterations:
        print("Warning: Algorithm may not converged.")
    return Q_res, Iter

# test your code directly with our example
# your result is comopared to result, that python calculates
A = laplace_matrix_square(5)
Q_Hess = Hessenberg_form(A)

B = A.copy()
Q, Iter = QR_iteration_slow(A, max_Iterations=10000)
plt.matshow(A)
plt.title("A in Schur form")
plt.colorbar()
plt.show()

w, v = np.linalg.eig(A)
print("Iterations:\t\t\t", Iter)
print("eigenvalues\t\t", np.diag(A))
print("true eigenvalues:\t", np.sort(w))
error_eigenval = np.max(np.abs(np.sort(w) - np.sort(np.diag(A))))
print("Max error of eigenvalues:\t", error_eigenval)

test_capacity = False

n = 4
times = []
while test_capacity:
    print(n)
    time_start = time.time()

    A = laplace_matrix_square(n)
    Hessenberg_form(A)
    Q, iter = QR_iteration_slow(A)
    time_end = time.time()
    times.append(time_end - time_start)
    if (time_end - time_start) > 10:
        test_capacity = False
    n = n * 2
n_Max_selfwritten = n // 2
print(
    "Our self written code is just "
    + str(n_Max // n_Max_selfwritten)
    + " times slower."
)

# prepare experiment:
n = 8
A = Create_random_matrix(n, "diag_dominant")

# for comparison:
w, v = np.linalg.eig(A.copy())
w = np.sort(w)
Q_Hess = Hessenberg_form(A)

max_Iterations = 20
convergence_eigenvals = {}  # dict
B = A.copy()
improvement_diag = np.zeros((n, max_Iterations))
for j in range(max_Iterations):
    Q, Iter = QR_iteration_slow(B, max_Iterations=2)
    improvement_diag[:, j] = np.sort(np.diag(B.copy()))


# plot over iterations
fig, ax = plt.subplots()
fig.suptitle("Convergence of eigenvalues")
ax.plot(np.arange(max_Iterations), improvement_diag.T)
ax.hlines(w, xmin=0, xmax=max_Iterations, colors="k", linestyles="dashed")
ax.set_xlabel("iterations")
ax.set_ylabel("eigenvalues")

# ax.set_xscale("log")
plt.show()

def evaluate_shift(A, shift_type="Zero"):
    # This function returns different types of shifts.
    # INPUT : A: submatrix of size 2x2
    #       : Type of shift(Zero, Rayleigh, Wilkinson(?))
    # OUTPUT: a number which approximates an eigenvalue.
    if shift_type == "Zero":
        return 0
    # HERE your code

    else:
        print("Warning: No valid shift type, no shift used")
        return 0

# test the shifts, that were suggested above
A = Create_random_matrix(2)
print(A)
sigma1 = evaluate_shift(A)
print("No shift:\n sigma =", sigma1)
sigma2 = evaluate_shift(A, "Rayleigh")
print("Raiyleigh shift:\n sigma=", sigma2)
sigma3 = evaluate_shift(A, "Wilkinson")
print("Wilkonson shift:\n sigma=", sigma3)
w, v = np.linalg.eig(A)
print("compare to eigenvalues:", w)
print("No valid input:\n")
sigma5 = evaluate_shift(A, "blabla")

def QR_iteration_shift(
    A, eps=1e-6, max_Iterations=10000, shift="Zero", suppress_warning=False
):
    # This function iterates the QR algorithm using shifts and a first glance of deflation.
    # I titerates, until either Max iter reached or
    # the values on the diagonal are
    # converged. The matrix A will be overwritten.
    # INPUT : - A: squared Matrix in hessenberg form
    #         - eps: if no diag entry changes more than eps, than the algorithm is converged
    #         - max_iterations: If this number is reached, it aborts the iteration and gives a warning
    #         - shift: accelerate convergence, types: Zero, Wilkinson, Francis, Rayleigh, None,
    #                 if None Wilkinson or Francis will be selected
    # OUTPUT: - Q, nxn Matrix, similarity transformation
    #         - Iter : number of Iterations

    # define values, for the computation
    n = A.shape[0]
    Iter = 0
    error_ev = 1
    diagvals = np.diag(A).copy()
    Q_res = np.eye(n, dtype=A.dtype)

    # start QR iteration
    while error_ev > eps and Iter < max_Iterations:
        # print(Iter, min_pos_not_converged, max_pos_not_converged)

        # evaluate shifts

        # HERE your code

        # QR iteration including shifts

        # HERE your code

        Iter += 1
        # preparation for next iteration
        error_ev = np.max(np.abs(diagvals - np.diag(A)))
        indices_not_converged = np.where(np.abs(diagvals - np.diag(A)) > eps)[0]
        if len(indices_not_converged) == 0:
            break

        diagvals = np.diag(A).copy()

    if not suppress_warning and Iter == max_Iterations:
        print("Warning: Algorithm may not converged.")
    return Q_res, Iter

n = 5
A = Create_random_matrix(n, "diag_dominant")
Q_Hess = Hessenberg_form(A)
w, v = np.linalg.eig(A)
B = A.copy()
Q, Iter = QR_iteration_shift(A, max_Iterations=10000, shift="Rayleigh")
eigenvalues = np.diag(A)
mask = np.argsort(eigenvalues)
eigenvalues = eigenvalues[mask[::-1]]
eigenvectors = eigenvectors[:, mask[::-1]]

plt.matshow(A)
plt.title("check result visually")
plt.colorbar()
plt.show()


print("Iterations:\t\t\t", Iter)

print("true eigenvalues:\t", w)
print("eigenvalues\t\t", eigenvalues)
error_eigenval = np.max(np.abs(np.sort(w) - np.sort(eigenvalues)))
print("Max error of eigenvalues:\t", error_eigenval)

# prepare experiment:
n = 15
A = Create_random_matrix(n, "diag_dominant")
# for comparison:
w, v = np.linalg.eig(A.copy())
w = np.sort(w)
Q_Hess = Hessenberg_form(A)
# HERE: modify the following list of shifts
list_shifts = ["Zero"]
print("shifts", "  iterartions", " error eigenvalues")
for shift in list_shifts:
    B = A.copy()
    Q, Iter = QR_iteration_shift(B, max_Iterations=10000, shift=shift)
    eigenvalues = np.sort(np.diag(B))
    error_eigenval = np.max(np.abs(w - eigenvalues))
    print(shift, Iter, error_eigenval)

# prepare experiment:
n = 15
A = Create_random_matrix(n, "diag_dominant")

# for comparison:
w, v = np.linalg.eig(A.copy())
w = np.sort(w)
Q_Hess = Hessenberg_form(A)

# HERE modify the list of shifts
list_shifts = ["Zero"]
print("shifts", "  iterartions", " error eigenvalues")

max_Iterations = 100
convergence_eigenvals = {}  # dict
for i, shift in enumerate(list_shifts):
    B = A.copy()
    improvement_diag = np.zeros((n, max_Iterations))
    for j in range(max_Iterations):
        Q, Iter = QR_iteration_shift(
            B, max_Iterations=2, shift=shift, suppress_warning=True
        )
        improvement_diag[:, j] = np.sort(np.diag(B.copy()))
    convergence_eigenvals[shift] = improvement_diag


############
# plotting #
############


# plot over iterations
fig, ax = plt.subplots(1, len(list_shifts), figsize=(5 * len(list_shifts), 5))
fig.suptitle("Convergence of eigenvalues")
try:
    for i, shift in enumerate(list_shifts):
        ax[i].plot(np.arange(max_Iterations), convergence_eigenvals[shift].T)
        ax[i].hlines(w, xmin=0, xmax=max_Iterations, colors="k", linestyles="dashed")
        ax[i].set_xlabel("iterations")
        ax[i].set_ylabel("eigenvalues")
        ax[i].set_title(shift)
        ax[i].set_xscale("log")
    plt.show()
except TypeError:
    pass

fig, ax = plt.subplots(
    1, len(list_shifts), figsize=(5 * len(list_shifts), 5), sharey=True
)
fig.suptitle("Error of eigenvalues")
try:
    for i, shift in enumerate(list_shifts):
        for j in [0, 4, 8, 12, 14]:
            ax[i].plot(
                np.arange(max_Iterations),
                np.abs(convergence_eigenvals[shift][j, :] - w[j]),
                label=str(np.round(w[j], 2)),
            )
        ax[i].hlines(
            1e-6,
            xmin=0,
            xmax=max_Iterations,
            colors="k",
            linestyles="dashed",
            label="eps",
        )
        ax[i].set_xlabel("iterations")
        ax[i].set_ylabel("eigenvalues")
        ax[i].set_title(shift)
        ax[i].set_xscale("log")
        ax[i].set_yscale("log")
        ax[i].legend()

    plt.show()
except TypeError:
    pass

def Deflation(A, eps=1e-10):
    # returns list with indices, at which  the subdiag of A is zero or neglectable
    # INPUT : -A ,nxn matrix
    #         - eps, a relativ threashold indicating, if an entry vanishes
    # OUTPUT: list of columns of the entries on the first subdiagonal, that vanish

    # get values of diag and subdiag
    diag = np.abs(np.diag(A)).copy()
    subdiag = np.abs(np.diag(A, k=-1)).copy()
    # values, at which deflation makes sense
    compare_value = eps * (diag[:-1] + diag[1:])
    # indexarray to return the positions
    n = len(subdiag)
    positions = np.arange(n)
    # checks, if deflation should be applied,
    pos_zeros_long = np.where(subdiag < compare_value, positions, -1)
    # just give the values of the deflation
    pos_zeros = pos_zeros_long[pos_zeros_long > -1]
    return pos_zeros

A = Create_random_matrix(5)

A[2, 1] = 0
plt.matshow(np.abs(A))
plt.colorbar()
plt.plot(1, 2, "rs")
plt.show()
x = Deflation(A)
print("Deflations in column", x, "(red point)")

def Split(A, col_zeros, offset=0):
    # this function splits a matrix into smaller matrices at the position of vanishing elements, such that
    # QR iteration gives the same result. It ignores 1 dimensional blocks in the complex case and 2 dim, real
    # blocks, if the eigenvalues of this block are complex
    # INPUT : - A: nxn matrix
    #         - col_zeros: list with the columns of the subdiagonal, which vanish
    #         - offset: the row (and the column) from the position of the original matrix
    # OUTPUT: list of tuples with first part is the submatrix and the second the offset

    lst = []
    n = A.shape[0]
    recent_zero = 0
    # switch from column to row entries of the zeros
    row_zeros = [i + 1 for i in col_zeros]

    for i in range(len(col_zeros)):
        if row_zeros[i] - recent_zero > 1:  # can't be eigenvalue block
            lst.append(
                (
                    A[recent_zero : row_zeros[i], recent_zero : row_zeros[i]],
                    recent_zero + offset,
                )
            )
        recent_zero = row_zeros[i]

    # last block of matrix
    if n - recent_zero > 1:
        lst.append((A[recent_zero:, recent_zero:], recent_zero + offset))

    return lst

import matplotlib.patches as patches

# insert postions ,where the splitting will take place
pos_zeros = [0, 2, 5]
print("Assume zeros at positions :", pos_zeros)
A = Create_random_matrix(7)
for i in pos_zeros:
    A[i + 1, i] = 0

# plot original matrix
plt.matshow(np.abs(A))
# plot zeros (red dots)
for i in pos_zeros:
    plt.plot(i, i + 1, "rs")

# plot frame around submatrices
rect0 = patches.Rectangle(
    (-0.5, -0.5), 1, 1, linewidth=6, edgecolor="b", facecolor="none"
)
rect1 = patches.Rectangle(
    (0.5, 0.5), 2, 2, linewidth=4, edgecolor="k", facecolor="none"
)
rect2 = patches.Rectangle(
    (2.5, 2.5), 3, 3, linewidth=4, edgecolor="k", facecolor="none"
)
rect3 = patches.Rectangle(
    (5.5, 5.5), 1, 1, linewidth=6, edgecolor="b", facecolor="none"
)
ax = plt.gca()
ax.add_patch(rect0)
ax.add_patch(rect1)
ax.add_patch(rect2)
ax.add_patch(rect3)
plt.title("A")
plt.colorbar()
plt.show()

print(" red dots are set to 0, blue boxes are eigenvalues. The two black boxes remain.")
# split the matrix in submatrices
lst = Split(A, pos_zeros)
# plot submatrices
fig, ax = plt.subplots(1, 2, figsize=(10, 5))
for i, mat in enumerate(lst):
    im = ax[i].matshow(np.abs(mat[0]))
    ax[i].set_title("submatrix " + str(i + 1) + " at column " + str(mat[1]))
plt.colorbar(im, ax=ax)
plt.show()

def QR_iteration(
    A,
    eps=1e-6,
    max_Iterations=10000,
    shift="None",
    check_deflation=True,
    eps_deflation=1e-10,
):
    # This function iterates the QR algorithm, until either Max iter reached, the values on the diagonal
    # converged or you could deflate the matrix. The matrix A will be overwritten.
    # INPUT : - A: squared Matrix in hessenberg form
    #         - eps: if no diag entry changes more than eps, than the algorithm is converged
    #         - max_iterations: If this number is reached, it aborts the iteration and gives a warning
    #         - shift: accelerate convergence, types: Zero, Wilkinson, Francis, Rayleigh, None,
    #                 if None Wilkinson or Francis will be selected
    #         - check_deflation: checks, if one can deflate the matrix
    #         - eps_deflation: threshhold for deflation
    # OUTPUT: - Q, nxn Matrix, similarity transformation
    #         - positions of the vanishing entries for the deflation
    #         - Iter : number of Iterations

    # define values, for the computation
    if shift == "None":
        shift = "Zero"

    n = A.shape[0]
    Iter = 0
    error_ev = 1
    diagvals = np.diag(A).copy()
    Q_res = np.eye(n, dtype=A.dtype)
    pos_zeros = []

    # start QR iteration
    while error_ev > eps and Iter < max_Iterations:
        # evaluate shifts
        sigma = np.real(evaluate_shift(A[-2:, -2:], shift))

        # QR iteration
        A[:, :] = A - sigma * np.eye(n, dtype=A.dtype)
        Q_2 = QR_decomposition_Hess(A)
        A[:, :] = A @ Q_2 + sigma * np.eye(n, dtype=A.dtype)
        Q_res[:, :] = Q_res @ Q_2
        if check_deflation:
            pos_zeros = Deflation(A, eps_deflation)
            if len(pos_zeros) > 0:
                break
        Iter += 1
        # preparation for next iteration
        error_ev = np.max(np.abs(diagvals - np.diag(A)))
        diagvals = np.diag(A).copy()

    if Iter == max_Iterations:
        print("Warning: Algorithm may not converged.")
    return Q_res, pos_zeros, Iter

def eigenvalue_QR(
    A, shift="None", eps_deflation=1e-10, eps_convergence=1e-6, max_Iterations=1000
):
    # calculates the eigenvalues and eigenvectors of matrix A using deflation and the QR iteration method
    # INPUT : - A squared Matrix
    #         - shift, eps_deflation, eps_convergence, max_Iterations see QR_iteration
    # OUTPUT: - eigenvalues
    #         - Q similarity transformation, it contains the eigenvectors if A is normal

    Q_res = Hessenberg_form(A)
    zero_pos = Deflation(A, eps_deflation)

    matrixList = Split(A, zero_pos)

    while matrixList != []:  # iterate until no matrix in the list
        B = matrixList[0][0]
        n_start = matrixList[0][1]
        n = B.shape[0]
        Q, pos_zeros, steps = QR_iteration(
            B,
            eps=eps_convergence,
            max_Iterations=max_Iterations,
            shift=shift,
            eps_deflation=eps_deflation,
        )

        if steps < max_Iterations:
            splitted_matrices = Split(B, pos_zeros, offset=n_start)
            matrixList += splitted_matrices

        matrixList.pop(0)  # remove matrix B from list
        Q_res[:, n_start : n_start + n] = Q_res[:, n_start : n_start + n] @ Q
    return np.diag(A), Q_res

A = Create_random_matrix(5, "diag_dominant")
# HERE your code

# enter HERE the type of shift you implemented
shifts = ["Zero"]
# the following is a dictionary of functions,
# prepare every function in such a way, that it only takes a matrix as input
# use lambda functions as helpers (see next line)
algorithms_slow = {"slow QR": lambda A: QR_iteration_slow(A)}
algorithms_shift = {
    "QR_shift" + shift: lambda A: QR_iteration(A, shift=shift) for shift in shifts
}
algorithms_deflation = {
    "QR_deflation with " + shift: lambda A: QR_iteration(
        A, shift=shift, check_deflation=True
    )
    for shift in shifts
}
algortihms_python = {"python": lambda A: np.linalg.eig(A)}
# add all dictionaries to one
algortigms = {
    **algorithms_slow,
    **algorithms_shift,
    **algorithms_deflation,
    **algortihms_python,
}
max_size = 7
times = {alg: np.zeros(max_size - 3) for alg in algortigms.keys()}
for i in range(3, max_size):
    A = laplace_matrix_square(i)
    Q = Hessenberg_form(A)
    for alg in algortigms:
        start = time.time()
        algortigms[alg](A.copy())
        end = time.time()
        times[alg][i - 3] = end - start

for alg in algortigms:
    plt.plot(times[alg], label=alg)
plt.legend()
plt.yscale("log")

test_all_implementations = False
shifts = ["Zero"]
n_shifts = len(shifts)
algorithms_shift = {
    "QR_shift" + shifts[i]: lambda A: QR_iteration(
        A,
        shift=shifts[i],
    )
    for i in range(n_shifts)
}
algorithms_deflation = {
    "QR_deflation with " + shifts[i]: lambda A: QR_iteration(
        A, shift=shifts[i], check_deflation=True
    )
    for i in range(n_shifts)
}
algortihms_python = {
    "python_np": lambda A: np.linalg.eig(A),
    "python_scipy": lambda A: scl.eig(A),
}
algortigms = {**algorithms_shift, **algorithms_deflation, **algortihms_python}
max_size = 7
times = {alg: np.zeros(max_size - 3) for alg in algortigms.keys()}
if test_all_implementations:
    for i in range(3, max_size):
        A = laplace_matrix_square(i)
        B = A.copy()
        for alg in algortigms:
            if "shift" in alg:
                start = time.time()
                Q = Hessenberg_form(B)
            else:
                start = time.time()
            algortigms[alg](B)
            end = time.time()
            times[alg][i - 3] = end - start
plt.figure()
for alg in algortigms:
    plt.plot(times[alg], label=alg)
plt.legend()
plt.yscale("log")

test_all_implementations = False
shifts = ["Zero"]
n_shifts = len(shifts)
algorithms_shift = {
    "QR_shift" + shifts[i]: lambda A: QR_iteration(
        A,
        shift=shifts[i],
    )
    for i in range(n_shifts)
}
algorithms_deflation = {
    "QR_deflation with " + shifts[i]: lambda A: QR_iteration(
        A, shift=shifts[i], check_deflation=True
    )
    for i in range(n_shifts)
}
algortihms_python = {"python": lambda A: np.linalg.eig(A)}
algortigms = {**algorithms_shift, **algorithms_deflation, **algortihms_python}
max_size = 6
times = {alg: np.zeros(max_size - 3) for alg in algortigms.keys()}
repetitions = 100
if test_all_implementations:
    for i in range(3, max_size):
        for j in range(repetitions):  # average over different random matrices
            A = Create_random_matrix(i * i, "diag_dominant")
            for alg in algortigms:
                B = A.copy()  # all algortigms use the same random matrix
                if "shift" in alg:
                    start = time.time()
                    Q = Hessenberg_form(B)
                else:
                    start = time.time()
                algortigms[alg](B)
                end = time.time()
                times[alg][i - 3] += end - start
plt.figure()
for alg in algortigms:
    plt.plot(times[alg] / repetitions, label=alg)
plt.legend()
plt.yscale("log")