def excite_system(mesh): sim = Sim(mesh, name='dyn') # sim.set_options(rtol=1e-10,atol=1e-14) sim.alpha = 0.04 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(np.load('m0.npy')) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.09 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, 0, 3.75e-3], name='H') sim.add(zeeman) w0 = 0.02 def time_fun(t): return np.exp(-w0 * t) hx = TimeZeeman([0, 0, 1e-5], sinc_fun, name='h') sim.add(hx, save_field=True) ts = np.linspace(0, 20000, 5001) for t in ts: sim.run_until(t) print 'sim t=%g' % t
def excite_system(mesh): sim = Sim(mesh, name="dyn") # sim.set_options(rtol=1e-10,atol=1e-14) sim.alpha = 0.04 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(np.load("m0.npy")) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.09 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, 0, 3.75e-3], name="H") sim.add(zeeman) w0 = 0.02 def time_fun(t): return np.exp(-w0 * t) hx = TimeZeeman([0, 0, 1e-5], sinc_fun, name="h") sim.add(hx, save_field=True) ts = np.linspace(0, 20000, 5001) for t in ts: sim.run_until(t) print "sim t=%g" % t
def test_dynamic(): mesh = CuboidMesh(nx=1, ny=1, nz=1) sim = Sim(mesh, name='dyn_spin', driver='slonczewski') # sim.set_options(rtol=1e-10,atol=1e-14) sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m((0.8, 0, -1)) Kx = Anisotropy(Ku=-0.05, axis=(0, 0, 1), name='Kz') sim.add(Kx) sim.p = (0, 0, 1) sim.u0 = 0.0052 sim.alpha = 0.1 ts = np.linspace(0, 1200, 401) for t in ts: sim.run_until(t) mz = sim.spin[2] alpha, K, u = 0.1, 0.05, 0.0052 print mz, u / (2 * alpha * K) ######################################################### # The system used in this test can be solved analytically, which gives that mz = u/(2*alpha*K), # where K represents the easy-plane anisotropy. ### assert abs(mz - u / (2 * alpha * K)) / mz < 5e-4
def test_dynamic(): mesh = CuboidMesh(nx=1, ny=1, nz=1) sim = Sim(mesh, name='dyn_spin', driver='slonczewski') # sim.set_options(rtol=1e-10,atol=1e-14) sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m((0.8,0,-1)) Kx = Anisotropy(Ku=-0.05, axis=(0, 0, 1), name='Kz') sim.add(Kx) sim.p = (0,0,1) sim.a_J = 0.0052 sim.alpha = 0.1 ts = np.linspace(0, 1200, 401) for t in ts: sim.run_until(t) mz = sim.spin[2] alpha, K, u = 0.1, 0.05, 0.0052 print(mz, u/(2*alpha*K)) ######################################################### # The system used in this test can be solved analytically, which gives that mz = u/(2*alpha*K), # where K represents the easy-plane anisotropy. ### assert abs(mz - u/(2*alpha*K))/mz< 5e-4
def excite_system(mesh, Hy=0): sim=Sim(mesh,name='dyn') sim.set_options(rtol=1e-10,atol=1e-12) sim.alpha = 0.04 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(np.load('m0.npy')) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.18 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0,Hy,2e-2],name='H') sim.add(zeeman) hx = TimeZeeman([0,0,1e-5], sinc_fun, name='h') sim.add(hx, save_field=True) dt = 5 steps = 2001 for i in range(steps): sim.run_until(i*dt)
def relax_system(mesh, Hy=0): sim=Sim(mesh,name='relax') sim.set_options(rtol=1e-10,atol=1e-12) sim.alpha = 0.5 sim.gamma = 1.0 sim.mu_s = 1.0 sim.do_precession = False sim.set_m(init_m) #sim.set_m(random_m) #sim.set_m(np.load('m_10000.npy')) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.18 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0,Hy,2e-2],name='H') sim.add(zeeman) sim.relax(dt=2.0, stopping_dmdt=1e-8, max_steps=10000, save_m_steps=100, save_vtk_steps=50) np.save('m0.npy',sim.spin)
def relax_system_stage2(): mesh = CuboidMesh(nx=140 , ny=140, nz=1) sim = Sim(mesh, name='dyn', driver='llg') sim.alpha = 0.1 sim.do_precession = True sim.gamma = const.gamma sim.mu_s = spatial_mu sim.set_m(np.load('skx.npy')) J = 50 * const.k_B exch = UniformExchange(J) sim.add(exch) D = 0.27 * J dmi = DMI(D) sim.add(dmi) zeeman = Zeeman(spatial_H) sim.add(zeeman) ts = np.linspace(0, 2e-9, 201) for t in ts: sim.run_until(t) sim.save_vtk() sim.save_m() print(t)
def excite_system(mesh, Hy=0): sim = Sim(mesh, name="dyn") sim.set_options(rtol=1e-10, atol=1e-12) sim.alpha = 0.04 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(np.load("m0.npy")) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.18 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, Hy, 2e-2], name="H") sim.add(zeeman) hx = TimeZeeman([0, 0, 1e-5], sinc_fun, name="h") sim.add(hx, save_field=True) dt = 5 steps = 2001 for i in range(steps): sim.run_until(i * dt)
def relax_system(mesh, Hy=0): sim = Sim(mesh, name="relax") sim.set_options(rtol=1e-10, atol=1e-12) sim.alpha = 0.5 sim.gamma = 1.0 sim.mu_s = 1.0 sim.do_precession = False sim.set_m(init_m) # sim.set_m(random_m) # sim.set_m(np.load('m_10000.npy')) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.18 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, Hy, 2e-2], name="H") sim.add(zeeman) sim.relax(dt=2.0, stopping_dmdt=1e-8, max_steps=10000, save_m_steps=100, save_vtk_steps=50) np.save("m0.npy", sim.spin)
def relax_system(mesh, Dx=0.005, Dp=0.01): mat = UnitMaterial() sim = Sim(mesh, name='test_energy') sim.set_tols(rtol=1e-10, atol=1e-12) sim.alpha = mat.alpha sim.gamma = mat.gamma sim.pins = pin_fun exch = UniformExchange(mat.J) sim.add(exch) anis = Anisotropy(Dx, axis=[1, 0, 0], name='Dx') sim.add(anis) anis2 = Anisotropy([0, 0, -Dp], name='Dp') sim.add(anis2) sim.set_m((1, 1, 1)) T = 100 ts = np.linspace(0, T, 201) for t in ts: # sim.save_vtk() sim.run_until(t) # sim.save_vtk() np.save('m0.npy', sim.spin)
def dynamic(mesh): sim = Sim(mesh, name='dyn', driver='slonczewski') # sim.set_options(rtol=1e-10,atol=1e-14) sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(np.load('m0.npy')) J = 1.0 exch = UniformExchange(J) sim.add(exch) Kx = Anisotropy(Ku=0.005, axis=(1, 0, 0), name='Kx') sim.add(Kx) sim.p = (0,0,1) sim.u0 = 0.03 sim.alpha = 0.1 ts = np.linspace(0, 1e3, 101) for t in ts: sim.run_until(t) sim.save_vtk() print t
def relax_system(mesh, Dx=0.005, Dp=0.01): mat = UnitMaterial() sim = Sim(mesh, name='test_energy') print('Created sim') sim.set_tols(rtol=1e-10, atol=1e-12) sim.alpha = mat.alpha sim.gamma = mat.gamma sim.pins = pin_fun exch = UniformExchange(mat.J) sim.add(exch) print('Added UniformExchange') anis = Anisotropy(Dx, axis=[1, 0, 0], name='Dx') sim.add(anis) print('Added Anisotropy') anis2 = Anisotropy([0, 0, -Dp], name='Dp') sim.add(anis2) print('Added Anisotropy 2') sim.set_m((1, 1, 1)) T = 100 ts = np.linspace(0, T, 201) for t in ts: # sim.save_vtk() sim.run_until(t) print('Running -', t) # sim.save_vtk() np.save('m0.npy', sim.spin)
def test_skx_num(): mesh = CuboidMesh(nx=120, ny=120, nz=1, periodicity=(True, True, False)) sim = Sim(mesh, name='skx_num') sim.set_tols(rtol=1e-6, atol=1e-6) sim.alpha = 1.0 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(init_m) sim.do_procession = False J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.09 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, 0, 5e-3]) sim.add(zeeman) sim.relax(dt=2.0, stopping_dmdt=1e-2, max_steps=1000, save_m_steps=None, save_vtk_steps=None) skn = sim.skyrmion_number() print 'skx_number', skn assert skn > -1 and skn < -0.99
def relax_system(mesh): sim = Sim(mesh, name='relax') # sim.set_options(rtol=1e-10,atol=1e-14) sim.alpha = 1.0 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(init_m) # sim.set_m(random_m) # sim.set_m(np.load('m_10000.npy')) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.09 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, 0, 3.75e-3]) sim.add(zeeman) sim.relax(dt=2.0, stopping_dmdt=1e-6, max_steps=1000, save_m_steps=100, save_vtk_steps=50) np.save('m0.npy', sim.spin)
def relax_system(mesh): sim = Sim(mesh, name='relax') sim.set_options(rtol=1e-12, atol=1e-14) sim.do_procession = False sim.alpha = 0.5 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(init_m) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.18 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, 0e-3, 2e-2], name='H') sim.add(zeeman) sim.relax(dt=2.0, stopping_dmdt=1e-8, max_steps=10000, save_m_steps=None, save_vtk_steps=100) np.save('m0.npy', sim.spin)
def relax_system_stage1(): mesh = CuboidMesh(nx=140 , ny=140, nz=1) sim = Sim(mesh, name='relax', driver='llg') #sim.set_options(dt=1e-14, gamma=const.gamma, k_B=const.k_B) sim.alpha = 0.5 sim.do_precession = False sim.gamma = const.gamma sim.mu_s = spatial_mu sim.set_m(init_m) J = 50 * const.k_B exch = UniformExchange(J) sim.add(exch) D = 0.27 * J dmi = DMI(D) sim.add(dmi) zeeman = Zeeman(spatial_H) sim.add(zeeman) sim.relax(dt=1e-14, stopping_dmdt=1e10, max_steps=1000, save_m_steps=100, save_vtk_steps=10) np.save('skx.npy', sim.spin) plot_m(mesh, 'skx.npy', comp='z')
def relax_system(mesh): sim=Sim(mesh,name='relax') sim.set_options(rtol=1e-12,atol=1e-14) sim.do_precession = False sim.alpha = 0.5 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(init_m) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.18 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0,0e-3,2e-2],name='H') sim.add(zeeman) sim.relax(dt=2.0, stopping_dmdt=1e-8, max_steps=10000, save_m_steps=None, save_vtk_steps=100) np.save('m0.npy',sim.spin)
def relax_neb(k, maxst, simname, init_im, interp, save_every=10000): """ Execute a simulation with the NEB function of the FIDIMAG code The simulations are made for a specific spring constant 'k' (a float), number of images 'init_im', interpolations between images 'interp' (an array) and a maximum of 'maxst' steps. 'simname' is the name of the simulation, to distinguish the output files. --> vtks and npys are saved in files starting with the 'simname' string """ # Prepare simulation sim = Sim(mesh, name=simname) sim.gamma = const.gamma # magnetisation in units of Bohr's magneton sim.mu_s = 2. * const.mu_B # Exchange constant in Joules: E = Sum J_{ij} S_i S_j J = 12. * const.meV exch = UniformExchange(J) sim.add(exch) # DMI constant in Joules: E = Sum D_{ij} S_i x S_j D = 2. * const.meV dmi = DMI(D, dmi_type='interfacial') sim.add(dmi) # Anisotropy along +z axis ku = Anisotropy(Ku=0.5 * const.meV, axis=[0, 0, 1], name='ku') sim.add(ku) # Initial images init_images = init_im # Number of images between each state specified before (here we need only # two, one for the states between the initial and intermediate state # and another one for the images between the intermediate and final # states). Thus, the number of interpolations must always be # equal to 'the number of initial states specified', minus one. interpolations = interp neb = NEB_Sundials(sim, init_images, interpolations=interpolations, spring=k, name=simname) neb.relax(max_steps=maxst, save_vtk_steps=save_every, save_npy_steps=save_every, stopping_dmdt=1e-2)
def test_sim_spins(do_plot=False): mesh = CuboidMesh(nx=10, ny=5, nz=1) sim = Sim(mesh, name='10spin') alpha = 0.1 gamma = 2.21e5 sim.alpha = alpha sim.gamma = gamma sim.mu_s = 1.0 sim.set_m((1, 0, 0)) print(sim.spin) H0 = 1e5 sim.add(Zeeman((0, 0, H0))) ts = np.linspace(0, 1e-9, 101) mx = [] my = [] mz = [] real_ts = [] for t in ts: sim.run_until(t) real_ts.append(sim.t) #print sim.t, abs(sim.spin_length()[0] - 1) av = sim.compute_average() mx.append(av[0]) my.append(av[1]) mz.append(av[2]) #sim.save_vtk() mz = np.array(mz) # print mz a_mx, a_my, a_mz = single_spin(alpha, gamma, H0, ts) print(sim.stat()) if do_plot: plot(real_ts, mx, my, mz, a_mx, a_my, a_mz, name='spins.pdf', title='integrating spins') print(("Max Deviation = {0}".format(np.max(np.abs(mz - a_mz))))) assert np.max(np.abs(mz - a_mz)) < 5e-7
def test_skx_num_atomistic(): """ Test the *finite spin chirality* or skyrmion number for a discrete spins simulation in a two dimensional lattice The expression is (PRL 108, 017601 (2012)) : Q = S_i \dot ( S_{i+1} X S_{j+1} ) + S_i \dot ( S_{i-1} X S_{j-1} ) which measures the chirality taking two triangles of spins per lattice site i: S_{i} , S_{i + x} , S_{i + y} and S_{i} , S_{i - x} , S_{i - y} The area of the two triangles cover a unit cell, thus the sum cover the whole area of the atomic lattice This test generate a skyrmion pointing down with unrealistic paremeters. """ mesh = CuboidMesh(nx=120, ny=120, nz=1, periodicity=(True, True, False)) sim = Sim(mesh, name='skx_num') sim.set_tols(rtol=1e-6, atol=1e-6) sim.alpha = 1.0 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(lambda pos: init_m(pos, 60, 60, 20)) sim.do_precession = False J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.09 dmi = DMI(D) sim.add(dmi) zeeman = Zeeman([0, 0, 5e-3]) sim.add(zeeman) sim.relax(dt=2.0, stopping_dmdt=1e-2, max_steps=1000, save_m_steps=None, save_vtk_steps=None) skn = sim.skyrmion_number() print('skx_number', skn) assert skn > -1 and skn < -0.99
def test_sim_pin(): mesh = CuboidMesh(nx=3, ny=2, nz=1) sim = Sim(mesh) sim.set_m((0, 0.8, 0.6)) sim.alpha = 0.1 sim.gamma = 1.0 sim.pins = pin_fun anis = Anisotropy(Ku=1.0, axis=[0, 0, 1], name='Dx') sim.add(anis) sim.run_until(1.0) assert sim.spin[0] == 0 assert sim.spin[2] != 0
def test_sim_spins(do_plot=False): mesh = CuboidMesh(nx=10, ny=5, nz=1) sim = Sim(mesh, name='10spin') alpha = 0.1 gamma = 2.21e5 sim.alpha = alpha sim.gamma = gamma sim.mu_s = 1.0 sim.set_m((1, 0, 0)) print(sim.spin) H0 = 1e5 sim.add(Zeeman((0, 0, H0))) ts = np.linspace(0, 1e-9, 101) mx = [] my = [] mz = [] real_ts = [] for t in ts: sim.run_until(t) real_ts.append(sim.t) #print sim.t, abs(sim.spin_length()[0] - 1) av = sim.compute_average() mx.append(av[0]) my.append(av[1]) mz.append(av[2]) #sim.save_vtk() mz = np.array(mz) # print mz a_mx, a_my, a_mz = single_spin(alpha, gamma, H0, ts) print(sim.stat()) if do_plot: plot(real_ts, mx, my, mz, a_mx, a_my, a_mz, name='spins.pdf', title='integrating spins') print(("Max Deviation = {0}".format( np.max(np.abs(mz - a_mz))))) assert np.max(np.abs(mz - a_mz)) < 5e-7
def relax_system(): # 1D chain of 50 spins with a lattice constant of 0.27 A mesh = CuboidMesh( nx=nx, dx=dx, unit_length=1e-9, # pbc='1d' ) # Initiate the simulation sim = Sim(mesh, name=sim_name) sim.gamma = const.gamma # magnetisation in units of Bohr's magneton sim.mu_s = 2 * const.mu_B # sim.set_options(gamma=const.gamma, k_B=const.k_B) # Initial magnetisation profile sim.set_m(init_m) # Exchange constant in Joules: E = Sum J_{ij} S_i S_j J = 12. * const.meV exch = UniformExchange(J) sim.add(exch) # DMI constant in Joules: E = Sum D_{ij} S_i x S_j D = 2. * const.meV dmi = DMI(D, dmi_type='interfacial') sim.add(dmi) # Anisotropy along +z axis ku = Anisotropy(Ku=0.5 * const.meV, axis=[0, 0, 1], name='ku') sim.add(ku) # Faster convergence sim.alpha = 0.5 sim.do_precession = False sim.relax(dt=1e-13, stopping_dmdt=0.05, max_steps=700, save_m_steps=1000, save_vtk_steps=1000) # Save the last relaxed state np.save(sim_name + '.npy', sim.spin)
def relax_system(): # 1D chain of 50 spins with a lattice constant of 0.27 A mesh = CuboidMesh(nx=nx, dx=dx, unit_length=1e-9, # pbc='1d' ) # Initiate the simulation. PBCs are specified in the mesh sim = Sim(mesh, name=sim_name) sim.gamma = const.gamma # magnetisation in units of Bohr's magneton sim.mu_s = 2. * const.mu_B # sim.set_options(gamma=const.gamma, k_B=const.k_B) # Initial magnetisation profile sim.set_m((0, 0, 1)) # Exchange constant in Joules: E = Sum J_{ij} S_i S_j J = 12. * const.meV exch = UniformExchange(J) sim.add(exch) # DMI constant in Joules: E = Sum D_{ij} S_i x S_j D = 2. * const.meV dmi = DMI(D, dmi_type='interfacial') sim.add(dmi) # Anisotropy along +z axis ku = Anisotropy(Ku=0.5 * const.meV, axis=[0, 0, 1], name='ku') sim.add(ku) # Faster convergence sim.alpha = 0.5 sim.do_precession = False sim.relax(dt=1e-13, stopping_dmdt=0.05, max_steps=700, save_m_steps=1000, save_vtk_steps=1000) # Save the last relaxed state np.save(sim_name + '.npy', sim.spin)
def relax_system(rtol=1e-10, atol=1e-12): """numerical solution""" mesh = CuboidMesh(nx=1, ny=1, nz=1) sim = Sim(mesh, name="relax") sim.set_options(rtol=rtol, atol=atol) sim.alpha = 0.5 sim.gamma = 2.21e5 sim.mu_s = 1.0 sim.set_m((1.0, 0, 0)) sim.add(Zeeman((0, 0, 1e5))) ts = np.linspace(0, 1e-9, 1001) for t in ts: sim.run_until(t)
def relax_system(rtol=1e-10, atol=1e-12): """numerical solution""" mesh = CuboidMesh(nx=1, ny=1, nz=1) sim = Sim(mesh, name='relax') sim.set_options(rtol=rtol, atol=atol) sim.alpha = 0.5 sim.gamma = 2.21e5 sim.mu_s = 1.0 sim.set_m((1.0, 0, 0)) sim.add(Zeeman((0, 0, 1e5))) ts = np.linspace(0, 1e-9, 1001) for t in ts: sim.run_until(t)
def test_sim_single_spin_vode(do_plot=False): mesh = CuboidMesh(nx=1, ny=1, nz=1) sim = Sim(mesh, name='spin') alpha = 0.1 gamma = 2.21e5 sim.alpha = alpha sim.gamma = gamma sim.mu_s = 1.0 sim.set_m((1, 0, 0)) H0 = 1e5 sim.add(Zeeman((0, 0, H0))) ts = np.linspace(0, 1e-9, 101) mx = [] my = [] mz = [] real_ts = [] for t in ts: sim.run_until(t) real_ts.append(sim.t) #print sim.t, abs(sim.spin_length()[0] - 1) mx.append(sim.spin[0]) my.append(sim.spin[1]) mz.append(sim.spin[2]) mz = np.array(mz) a_mx, a_my, a_mz = single_spin(alpha, gamma, H0, ts) print(sim.stat()) if do_plot: plot(real_ts, mx, my, mz, a_mx, a_my, a_mz) print(("Max Deviation = {0}".format( np.max(np.abs(mz - a_mz))))) assert np.max(np.abs(mz - a_mz)) < 5e-7
def test_sim_single_spin_vode(do_plot=False): mesh = CuboidMesh(nx=1, ny=1, nz=1) sim = Sim(mesh, name='spin') alpha = 0.1 gamma = 2.21e5 sim.alpha = alpha sim.gamma = gamma sim.mu_s = 1.0 sim.set_m((1, 0, 0)) H0 = 1e5 sim.add(Zeeman((0, 0, H0))) ts = np.linspace(0, 1e-9, 101) mx = [] my = [] mz = [] real_ts = [] for t in ts: sim.run_until(t) real_ts.append(sim.t) #print sim.t, abs(sim.spin_length()[0] - 1) mx.append(sim.spin[0]) my.append(sim.spin[1]) mz.append(sim.spin[2]) mz = np.array(mz) a_mx, a_my, a_mz = single_spin(alpha, gamma, H0, ts) print(sim.stat()) if do_plot: plot(real_ts, mx, my, mz, a_mx, a_my, a_mz) print(("Max Deviation = {0}".format(np.max(np.abs(mz - a_mz))))) assert np.max(np.abs(mz - a_mz)) < 5e-7
def dynamic(mesh): sim = Sim(mesh, name='dyn_spin', driver='slonczewski') # sim.set_options(rtol=1e-10,atol=1e-14) sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m((0.8, 0, -1)) Kx = Anisotropy(Ku=-0.05, axis=(0, 0, 1), name='Kz') sim.add(Kx) sim.p = (0, 0, 1) sim.u0 = 0.005 sim.alpha = 0.1 ts = np.linspace(0, 1200, 401) for t in ts: sim.run_until(t) #sim.save_vtk() print t
def dynamic(mesh): sim = Sim(mesh, name='dyn_spin', driver='slonczewski') # sim.set_options(rtol=1e-10,atol=1e-14) sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m((0.8,0,-1)) Kx = Anisotropy(Ku=-0.05, axis=(0, 0, 1), name='Kz') sim.add(Kx) sim.p = (0,0,1) sim.u0 = 0.005 sim.alpha = 0.1 ts = np.linspace(0, 1200, 401) for t in ts: sim.run_until(t) #sim.save_vtk() print t
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")
def relax_system(mesh): sim = Sim(mesh, name='relax') # sim.set_options(rtol=1e-10,atol=1e-14) sim.alpha = 1.0 sim.gamma = 1.0 sim.mu_s = 1.0 sim.set_m(init_m) # sim.set_m(random_m) # sim.set_m(np.load('m_10000.npy')) J = 1.0 exch = UniformExchange(J) sim.add(exch) Kx = Anisotropy(Ku=0.005, axis=(1, 0, 0), name='Kx') sim.add(Kx) sim.relax(dt=2.0, stopping_dmdt=1e-6, max_steps=1000, save_m_steps=100, save_vtk_steps=50) np.save('m0.npy', sim.spin)
def relax_system(mesh): sim = Sim(mesh, name='dmi_2d') sim.alpha = 0.1 sim.gamma = 1.76e11 sim.mu_s = 1e-22 J = 1e-20 exch = UniformExchange(J) sim.add(exch) dmi = DMI(0.1 * J) sim.add(dmi) sim.set_m(init_m) ts = np.linspace(0, 5e-10, 101) for t in ts: print(t) sim.run_until(t) #sim.save_vtk() return sim.spin
def relax_system(mesh): sim = Sim(mesh, name="dmi_2d") sim.alpha = 0.1 sim.gamma = 1.76e11 sim.mu_s = 1e-22 J = 1e-20 exch = UniformExchange(J) sim.add(exch) dmi = DMI(0.1 * J) sim.add(dmi) sim.set_m(init_m) ts = np.linspace(0, 5e-10, 101) for t in ts: print t sim.run_until(t) # sim.save_vtk() return sim.spin
def create_sim(): mesh = CuboidMesh(nx=121,ny=121,nz=1) sim=Sim(mesh,name='relax') sim.alpha = 1.0 sim.gamma = 0.5 sim.mu_s = mu_s sim.set_m(init_m) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.08 dmi = DMI(D) sim.add(dmi) K = 4e-3 anis=Anisotropy(K, direction=(0,0,1),name='Ku') sim.add(anis) return sim
def create_sim(): mesh = CuboidMesh(nx=121, ny=121, nz=1) sim = Sim(mesh, name='relax') sim.alpha = 1.0 sim.gamma = 0.5 sim.mu_s = mu_s sim.set_m(init_m) J = 1.0 exch = UniformExchange(J) sim.add(exch) D = 0.08 dmi = DMI(D) sim.add(dmi) K = 4e-3 anis = Anisotropy(K, direction=(0, 0, 1), name='Ku') sim.add(anis) return sim
from fidimag.atomistic import Sim from fidimag.common.cuboid_mesh import CuboidMesh from fidimag.atomistic import UniformExchange, Zeeman import fidimag.common.constant as const mesh = CuboidMesh(nx=1, ny=1, dx=1, dy=1) sim = Sim(mesh, name='relax_sk') sim.gamma = const.gamma sim.set_m((1, 0, 0)) sim.add(Zeeman((0, 0, 25.))) sim.run_until(1e-11) sim.set_tols(rtol=1e-10, atol=1e-12) sim.run_until(2e-11)
from fidimag.atomistic import Sim from fidimag.common.cuboid_mesh import CuboidMesh from fidimag.atomistic import UniformExchange, Zeeman from fidimag.atomistic import Constant # Import physical constants from fidimag const = Constant() mesh = CuboidMesh(nx=1, ny=1, dx=1, dy=1) sim = Sim(mesh, name='relax_sk') sim.gamma = const.gamma sim.set_m((1, 0, 0)) sim.add(Zeeman((0, 0, 25.))) sim.run_until(1e-11) sim.set_tols(rtol=1e-10, atol=1e-12) sim.run_until(2e-11)