Exemplo n.º 1
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def bragg_lumapi(args):

    num_periods = args.num_periods  # Number of Periods for Bragg Grating
    length = args.length  # Length of each segment of BG, Period = Length * 2
    num_wavelengths = args.num_wavelengths  # Number of wavelengths to sweep
    wl_lower = args.wl_lower  # Lower wavelength bound
    wl_upper = args.wl_upper  # Upper wavelength bound
    num_modes = args.num_modes  # Number of Modes
    mesh = args.mesh  # Number of mesh points
    width1 = args.width1  # Width of first core block
    width2 = args.width2  # Width of second core block
    thickness = args.thickness  # Thicnkess of the core
    modesolver = MSLumerical  # Which modesolver to use
    t = [
    ]  # Array that holds the transmission coefficients for different wavelengths

    eme = LumEME(num_periods=num_periods)

    for wavelength in np.linspace(wl_lower, wl_upper, num_wavelengths):

        eme.reset()

        mode_solver1 = modesolver(
            wavelength * 1e-6,
            width1 * 1e-6,
            thickness * 1e-6,
            mesh=mesh,
            num_modes=num_modes,
            mode=eme.mode,
            eme_modes=True,
        )  # First half of bragg grating

        mode_solver2 = modesolver(
            wavelength * 1e-6,
            width2 * 1e-6,
            thickness * 1e-6,
            mesh=mesh,
            num_modes=num_modes,
            mode=eme.mode,
            eme_modes=True,
        )  # Second half of bragg grating

        eme.add_layer(
            Layer(mode_solver1, num_modes, wavelength * 1e-6,
                  length * 1e-6))  # First half of bragg grating
        eme.add_layer(
            Layer(mode_solver2, num_modes, wavelength * 1e-6,
                  length * 1e-6))  # Second half of bragg grating

        eme.propagate()  # propagate at given wavelength

        t.append(np.abs((eme.s_parameters()
                         ))[0, 0,
                            num_modes]**2)  # Grab the transmission coefficient

    return t
Exemplo n.º 2
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def taper_lumerical(print_s=True, start=0, finish=10):

    # This dictionary stores the information used by the benchmark scripts
    taper_lumerical_dict = {"density": [], "time": [], "s_params": []}

    # Cross sectional parameters (computational complexity determined here)
    ModeSolver = MSLumerical  # Choose a modesolver object that will calculate the 2D field profile
    mesh = 128  # Mesh density of 2D field profiles
    num_modes = 1

    # Geometric parameters
    width1 = 0.8e-6  # Width of left waveguide
    thickness1 = 0.3e-6  # Thickness of left waveguide
    width2 = 0.25e-6  # Width of right waveguide
    thickness2 = 0.15e-6  # Thickness of right waveguide
    wavelength = 1.55e-6  # Wavelength of light (m)
    length = 10e-6  # Length of the waveguides
    # taper_density = 10  # How many divisions in the taper where eigenmodes will be calculated
    taper_length = 2e-6  # The length of the taper

    wg_length = 0.5 * (length - taper_length
                       )  # Length of each division in the taper

    eme = LumEME(
    )  # Choose either a normal eme or a periodic eme (PeriodicEME())
    for taper_density in range(start, finish):

        # Ensure a new eme each iteration
        eme.reset()

        # first layer is a straight waveguide
        mode1 = ModeSolver(wl=wavelength,
                           width=width1,
                           thickness=thickness1,
                           mesh=mesh,
                           num_modes=num_modes,
                           mode=eme.mode)
        straight1 = Layer(mode1, num_modes, wavelength, wg_length)
        eme.add_layer(straight1)

        # create the discrete taper with a fine enough taper density to approximate a continuous linear taper
        widths = np.linspace(width1, width2, taper_density)
        thicknesses = np.linspace(thickness1, thickness2, taper_density)
        taper_length_per = taper_length / taper_density if taper_density else None

        # add the taper layers
        for i in range(taper_density):
            solver = ModeSolver(wl=wavelength,
                                width=widths[i],
                                thickness=thicknesses[i],
                                mesh=mesh,
                                num_modes=num_modes,
                                mode=eme.mode)
            taper_layer = Layer(solver, num_modes, wavelength,
                                taper_length_per)
            eme.add_layer(taper_layer)

        # last layer is a straight waveguide of smaller geometry
        mode2 = ModeSolver(wl=wavelength,
                           width=width2,
                           thickness=thickness2,
                           mesh=mesh,
                           num_modes=num_modes,
                           mode=eme.mode)
        straight2 = Layer(mode2, num_modes, wavelength, wg_length)
        eme.add_layer(straight2)

        # eme.draw()  # Look at our simulation geometry

        t1 = time.time()
        eme.propagate()  # Run the eme
        t2 = time.time()
        taper_lumerical_dict["time"].append(t2 - t1)
        taper_lumerical_dict["density"].append(taper_density)
        taper_lumerical_dict["s_params"].append(eme.s_parameters())

        if print_s:
            print(taper_density, ": ",
                  np.abs(eme.s_parameters()))  # Extract s_parameters

    return taper_lumerical_dict
Exemplo n.º 3
0
    wavelength,
    mode=eme.mode,
    thickness=thickness,
    core_index=core_index,
    cladding_index=cladding_index,
    cladding_width=8e-6,
    cladding_thickness=8e-6,
    num_modes=num_modes_input,
    mesh=mesh,
    x=x,
    y=x,
    polygons=polygons[:],
    PML=PML,
)

eme.add_layer(Layer(input_channel, num_modes_input, wavelength, input_length))

# Create taper into MMI
for i in range(input_taper_num_steps):
    polygons = []
    for out in range(num_inputs):
        starting_center = -0.5 * (num_inputs - 1) * (input_gap + input_width)
        n_input = np.ones(mesh) * cladding_index
        center = starting_center + out * (input_gap + input_width)
        width = input_width + (input_taper_width -
                               input_width) * (i / input_taper_num_steps)
        left_edge = center - 0.5 * width
        right_edge = center + 0.5 * width
        n_input = np.where((left_edge <= x) * (x <= right_edge), core_index,
                           n_input)
Exemplo n.º 4
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mesh = 128  # Number of mesh points in each xy dimension

eme = LumEME()  # Choose either a normal eme or a periodic eme (PeriodicEME())

# first layer is a straight waveguide
mode1 = MSLumerical1D(
    wavelength,
    width1,
    thickness1,
    num_modes=3,
    cladding_width=10e-6,
    cladding_thickness=10e-6,
    mesh=mesh,
    mode=eme.mode,
)
straight1 = Layer(mode1, 3, wavelength, length)
eme.add_layer(straight1)

# create the discrete taper with a fine enough taper density to approximate a continuous linear taper
widths = taper_func(width1, width2, taper_density)
thicknesses = np.linspace(thickness1, thickness2, taper_density)
taper_length_per = taper_length / taper_density

# add the taper layers
for i in range(taper_density):
    num_modes = num_modes_first_half if i < taper_density / 2.0 else num_modes_second_half
    solver = MSLumerical1D(
        wavelength,
        widths[i],
        thicknesses[i],
        num_modes=num_modes,
Exemplo n.º 5
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        0.22e-6,
        mesh=mesh,
        num_modes=num_modes,
        lumapi_location="/Applications/Lumerical v202.app/Contents/API/Python",
    )  # First half of bragg grating

    mode_solver2 = modesolver(
        wavelength * 1e-6,
        0.54e-6,
        0.22e-6,
        mesh=mesh,
        num_modes=num_modes,
        lumapi_location="/Applications/Lumerical v202.app/Contents/API/Python",
    )  # Second half of bragg grating

    layer1 = Layer(mode_solver1, num_modes, wavelength * 1e-6,
                   length * 1e-6)  # First half of bragg grating
    layer2 = Layer(mode_solver2, num_modes, wavelength * 1e-6,
                   length * 1e-6)  # Second half of bragg grating

    eme = PeriodicEME(
        [layer1, layer2], num_periods
    )  # Periodic EME will save computational time for repeated geometry

    # eme.draw() # Draw the structure

    eme.propagate()  # propagate at given wavelength

    t.append(np.abs((eme.s_parameters()
                     )[0, 0,
                       num_modes])**2)  # Grab the transmission coefficient