示例#1
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def excite_system(mesh):

    sim = Sim(mesh, name='dyn', driver='sllg')
    sim.set_options(dt=1e-14, gamma=const.gamma, k_B=const.k_B)
    sim.driver.alpha = 0.1
    sim.mu_s = const.mu_s_1
    sim.T = temperature_gradient

    sim.set_m(np.load("m0.npy"))

    J = 50.0 * const.k_B
    exch = UniformExchange(J)
    sim.add(exch)

    D = 0.5 * J
    dmi = DMI(D)
    sim.add(dmi)

    Hz = 0.2 * J / const.mu_s_1
    zeeman = Zeeman([0, 0, Hz])
    sim.add(zeeman)

    dt = 2e-14 * 50  # 1e-12
    ts = np.linspace(0, 1000 * dt, 501)
    for t in ts:
        sim.run_until(t)
        sim.save_vtk()
        sim.save_m()
        print 'sim t=%g' % t
示例#2
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def excite_system(T=0.1, H=0.15):

    mesh = CuboidMesh(nx=28 * 3, ny=16 * 5, nz=1, pbc='2d')

    sim = Sim(mesh, name='dyn', driver='sllg')
    sim.set_options(dt=1e-14, gamma=const.gamma, k_B=const.k_B)
    sim.alpha = 0.1
    sim.mu_s = const.mu_s_1

    sim.set_m(random_m)

    J = 50 * const.k_B
    exch = UniformExchange(J)
    sim.add(exch)

    D = 0.5 * J
    dmi = DMI(D)
    sim.add(dmi)

    Hz = H * J / const.mu_s_1
    zeeman = Zeeman([0, 0, Hz])
    sim.add(zeeman)

    sim.T = J / const.k_B * T

    ts = np.linspace(0, 5e-11, 51)
    for t in ts:
        sim.run_until(t)
        # sim.save_vtk()

    np.save('m.npy', sim.spin)
    plot_m(mesh, 'm.npy', comp='z')
示例#3
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def excite_system(mesh):

    sim = Sim(mesh, name='dyn', driver='sllg')
    sim.set_options(dt=1e-14, gamma=const.gamma, k_B=const.k_B)
    sim.alpha = 0.1
    sim.mu_s = const.mu_s_1
    sim.T = temperature_gradient

    sim.set_m(np.load("m0.npy"))

    J = 50.0 * const.k_B
    exch = UniformExchange(J)
    sim.add(exch)

    D = 0.5 * J
    dmi = DMI(D)
    sim.add(dmi)

    Hz = 0.2 * J / const.mu_s_1
    zeeman = Zeeman([0, 0, Hz])
    sim.add(zeeman)

    dt = 2e-14 * 50  # 1e-12
    ts = np.linspace(0, 1000 * dt, 501)
    for t in ts:
        sim.run_until(t)
        sim.save_vtk()
        sim.save_m()
        print 'sim t=%g' % t
示例#4
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def single_spin(alpha=0.01):

    mat = Material()

    mesh = CuboidMesh(nx=1, ny=1, nz=1)

    sim = Sim(mesh, driver='sllg')
    sim.alpha = alpha
    sim.gamma = mat.gamma
    sim.mu_s = mat.mu_s
    sim.T = 10000

    sim.set_m((1, 1, 1))

    #sim.add(Zeeman(1,(0, 0, 1)))

    anis = Anisotropy(mat.K, direction=(0, 0, 1))
    sim.add(anis)

    dt = 0.5e-12
    ts = np.linspace(0, 1000 * dt, 1001)

    sx = []
    sy = []
    for t in ts:
        sim.run_until(t)
        sx.append(sim.spin[0])
        sy.append(sim.spin[1])
        print(t)

    plt.plot(sx, sy)
    plt.xlabel("$S_x$")
    plt.ylabel("$S_y$")
    plt.grid()
    plt.axis((-0.9, 0.9, -0.9, 0.9))
    plt.axes().set_aspect('equal')

    plt.savefig("macrospin.pdf")
示例#5
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def single_spin(alpha=0.01):

    mat = Material()

    mesh = CuboidMesh(nx=1, ny=1, nz=1)

    sim = Sim(mesh, driver='sllg')
    sim.alpha = alpha
    sim.gamma = mat.gamma
    sim.mu_s = mat.mu_s
    sim.T = 10000

    sim.set_m((1, 1, 1))

    #sim.add(Zeeman(1,(0, 0, 1)))

    anis = Anisotropy(mat.K, direction=(0, 0, 1))
    sim.add(anis)

    dt = 0.5e-12
    ts = np.linspace(0, 1000 * dt, 1001)

    sx = []
    sy = []
    for t in ts:
        sim.run_until(t)
        sx.append(sim.spin[0])
        sy.append(sim.spin[1])
        print(t)

    plt.plot(sx, sy)
    plt.xlabel("$S_x$")
    plt.ylabel("$S_y$")
    plt.grid()
    plt.axis((-0.9, 0.9, -0.9, 0.9))
    plt.axes().set_aspect('equal')

    plt.savefig("macrospin.pdf")