Beispiel #1
0
def get_D_square_min(atoms_now,
                     atoms_old,
                     i_now,
                     j_now,
                     delta_plus_epsilon=None):
    """
    Calculate the D^2_min norm of Falk and Langer
    """
    nat = len(atoms_now)
    assert len(atoms_now) == len(atoms_old)

    pos_now = atoms_now.positions
    pos_old = atoms_old.positions

    # Compute current and old distance vectors. Note that current distance
    # vectors cannot be taken from the neighbor calculation, because neighbors
    # are calculated from the sheared cell while these distance need to come
    # from the unsheared cell. Taking the distance from the unsheared cell
    # make periodic boundary conditions (and flipping of cell) a lot easier.
    dr_now = mic(pos_now[i_now] - pos_now[j_now], atoms_now.cell)
    dr_old = mic(pos_old[i_now] - pos_old[j_now], atoms_old.cell)

    # Sanity check: Shape needs to be identical!
    assert dr_now.shape == dr_old.shape

    if delta_plus_epsilon is None:
        # Get minimum strain tensor
        delta_plus_epsilon = get_delta_plus_epsilon(nat, i_now, dr_now, dr_old)

    # Spread epsilon out for each neighbor index
    delta_plus_epsilon_n = delta_plus_epsilon[i_now]

    # Compute D^2_min
    d_sq_n = np.sum((dr_now - np.sum(
        delta_plus_epsilon_n.reshape(-1, 3, 3) * dr_old.reshape(-1, 1, 3),
        axis=2))**2,
                    axis=1)

    # For each atom, sum over all neighbors
    d_sq = np.bincount(i_now, weights=d_sq_n)

    return delta_plus_epsilon, d_sq
Beispiel #2
0
def get_D_square_min(atoms_now, atoms_old, i_now, j_now, delta_plus_epsilon=None):
    """
    Calculate the D^2_min norm of Falk and Langer
    """
    nat = len(atoms_now)
    assert len(atoms_now) == len(atoms_old)

    pos_now = atoms_now.positions
    pos_old = atoms_old.positions

    # Compute current and old distance vectors. Note that current distance
    # vectors cannot be taken from the neighbor calculation, because neighbors
    # are calculated from the sheared cell while these distance need to come
    # from the unsheared cell. Taking the distance from the unsheared cell
    # make periodic boundary conditions (and flipping of cell) a lot easier.
    dr_now = mic(pos_now[i_now] - pos_now[j_now], atoms_now.cell)
    dr_old = mic(pos_old[i_now] - pos_old[j_now], atoms_old.cell)

    # Sanity check: Shape needs to be identical!
    assert dr_now.shape == dr_old.shape

    if delta_plus_epsilon is None:
        # Get minimum strain tensor
        delta_plus_epsilon = get_delta_plus_epsilon(nat, i_now, dr_now, dr_old)

    # Spread epsilon out for each neighbor index
    delta_plus_epsilon_n = delta_plus_epsilon[i_now]

    # Compute D^2_min
    d_sq_n = np.sum(
        (
        dr_now-
        np.sum(delta_plus_epsilon_n.reshape(-1,3,3)*dr_old.reshape(-1,1,3),
               axis=2)
        )**2,
        axis=1)

    # For each atom, sum over all neighbors
    d_sq = np.bincount(i_now, weights=d_sq_n)

    return delta_plus_epsilon, d_sq
Beispiel #3
0
    def test_neighbor_list(self):
        a = io.read('aC.cfg')
        an = native.from_atoms(a)
        nl = native.Neighbors(100)
        nl.request_interaction_range(5.0)

        i, j, abs_dr_no_vec = nl.get_neighbors(an)
        i, j, dr, abs_dr = nl.get_neighbors(an, vec=True)

        self.assertTrue(np.all(np.abs(abs_dr_no_vec-abs_dr) < 1e-12))

        r = a.get_positions()
        dr_direct = mic(r[i]-r[j], a.cell)

        abs_dr_from_dr = np.sqrt(np.sum(dr*dr, axis=1))
        abs_dr_direct = np.sqrt(np.sum(dr_direct*dr_direct, axis=1))

        self.assertTrue(np.all(np.abs(abs_dr-abs_dr_from_dr) < 1e-12))
        self.assertTrue(np.all(np.abs(abs_dr-abs_dr_direct) < 1e-12))

        self.assertTrue(np.all(np.abs(dr-dr_direct) < 1e-12))