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-> Added N-Layer PES Intensity Modelling App.
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MatBase-v1.0.1/N Layer PES Intensity Modelling/2-layer model/overlayer_calc.m
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function d_o = overlayer_calc(theta, C_m, imfp_m, I_m, C_o, imfp_o, I_o) | ||
% d_o = overlayer_calc(C_m, imfp_m, I_m, C_o, imfp_o, I_o) | ||
% Function that determines the thickness of a uniform oxide-film on an | ||
% oxidised metal surface. This is calculated from the relative | ||
% photoelectron intensity of the oxidic or the metallic component, with | ||
% respect to that of the corresponding oxide or clean metal, respectively. | ||
% This model assumes that the underlying metallic layer is an infinitely | ||
% thick slab, with a uniform oxide layer of thickness d_o on top. | ||
% | ||
% IN: | ||
% - theta: scalar of the photoelectron take-off angle. | ||
% - C_m: scalar of the volume density of metal atoms in the metal [mole / cc]. | ||
% - imfp_m: scalar of the imfp of electrons in the metal [nm]. | ||
% - I_m: scalar of the total peak area of the metal photoelectron peak. | ||
% - C_o: scalar of the volume density of metal atoms in the oxide [mole / cc]. | ||
% - imfp_o: scalar of the imfp of electrons in the oxide [nm]. | ||
% - I_o: scalar of the total peak area of the oxide photoelectron peak. | ||
% | ||
% OUT: | ||
% - d_o: thickness of the oxide in nm. | ||
|
||
%% 1 : Determination of the oxide thickness | ||
d_o = imfp_o .* sin(deg2rad(theta)) .* log(1 + (C_m.*imfp_m.*I_o) ./ (C_o.*imfp_o.*I_m)); | ||
|
||
end |
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MatBase-v1.0.1/N Layer PES Intensity Modelling/n-layer model/nlayer_pes_model.m
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MatBase-v1.0.1/N Layer PES Intensity Modelling/n-layer model/view_nlayer_pes_model.m
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function fig = view_nlayer_pes_model(pes_model, lyr_cols) | ||
% fig = view_nlayer_pes_model(pes_model) | ||
% This function plots the solutions to the 'nlayer_pes_model()' function; | ||
% the n-layered sample stack and the corresponding photoelectron | ||
% contribution from each one of the layers. The user can input the colors | ||
% for each one of the layers using the 'lyr_cols' argument; this is | ||
% convenient when you want to color-match the schematic to your own | ||
% drawings. | ||
% | ||
% IN: | ||
% - pes_model: data structure that contains all the pes model parameters and variables (from 'nlayer_pes_model()'). | ||
% - lyr_cols: Mx1 cell-vector of the [R,G,B] color of each independent layer. | ||
% | ||
% OUT: | ||
% - fig: MATLAB figure object with the ARPES data plotted. | ||
|
||
%% Default parameters | ||
def_cols = flipud(num2cell([0.25,0.25,0.25;lines(length(pes_model.lyr_mat)-1)], 2)); | ||
% -- Defining the default parameters | ||
if nargin < 2; lyr_cols = def_cols; end | ||
if isempty(lyr_cols); lyr_cols = def_cols; end | ||
|
||
%% 1 - Plotting the the model solutions | ||
% -- Range of photon energies, but a single angle | ||
if length(pes_model.hv) > 1 && length(pes_model.theta) == 1 | ||
fig{1} = view_nlayer_pes_model_vs_hv(pes_model, lyr_cols); | ||
% -- Single photon energy, but a range of angles | ||
elseif length(pes_model.hv) == 1 && length(pes_model.theta) > 1 | ||
fig{1} = view_nlayer_pes_model_vs_theta(pes_model, lyr_cols); | ||
% -- Range of photon energies and angles | ||
elseif length(pes_model.hv) > 1 && length(pes_model.theta) > 1 | ||
fig{1} = view_nlayer_pes_model_vs_hv(pes_model, lyr_cols); | ||
fig{2} = view_nlayer_pes_model_vs_theta(pes_model, lyr_cols); | ||
% -- Single values only | ||
else; fig{1} = view_nlayer_pes_model_vs_hv(pes_model, lyr_cols); | ||
end |
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MatBase-v1.0.1/N Layer PES Intensity Modelling/n-layer model/view_nlayer_pes_model_vs_hv.m
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function fig = view_nlayer_pes_model_vs_hv(pes_model, lyr_cols) | ||
% fig = view_nlayer_pes_model_vs_hv(pes_model, lyr_cols) | ||
% This function plots the solutions to the 'nlayer_pes_model()' function; | ||
% the n-layered sample stack and the corresponding photoelectron | ||
% contribution from each one of the layers. The user can input the colors | ||
% for each one of the layers using the 'lyr_cols' argument; this is | ||
% convenient when you want to color-match the schematic to your own | ||
% drawings. | ||
% | ||
% IN: | ||
% - pes_model: data structure that contains all the pes model parameters and variables (from 'nlayer_pes_model()'). | ||
% - lyr_cols: Mx1 cell-vector of the [R,G,B] color of each independent layer. | ||
% | ||
% OUT: | ||
% - fig: MATLAB figure object with the ARPES data plotted. | ||
|
||
%% Default parameters | ||
def_cols = flipud(num2cell([0.25,0.25,0.25;lines(length(pes_model.lyr_mat)-1)], 2)); | ||
% -- Defining the default parameters | ||
if nargin < 2; lyr_cols = def_cols; end | ||
if isempty(lyr_cols); lyr_cols = def_cols; end | ||
|
||
%% 1 - Plotting the the model solutions | ||
fig = figure(); | ||
fig.Position(3) = 900; | ||
fig.Position(4) = 450; | ||
%% 1.1 - Plotting the intensity profiles for each layer | ||
subplot(1,3,1); hold on; | ||
x_width = 5; | ||
bulk_thickness = 5; | ||
if pes_model.Nlyrs == 1 | ||
y_cum = cell2mat(pes_model.lyr_thick); | ||
else | ||
y_cum = cumsum(cell2mat(pes_model.lyr_thick)); | ||
y_cum(isinf(y_cum)) = y_cum(end-1) + bulk_thickness; | ||
end | ||
% -- Plotting each layer from bottom-up | ||
for i = pes_model.Nlyrs:-1:1 | ||
patch([-1, -1, 1, 1, -1].*x_width, [0, y_cum(i), y_cum(i), 0, 0].*-1,... | ||
lyr_cols{i}, 'edgecolor', [0 0 0]); | ||
end | ||
% -- Adding text for each material type | ||
for i = 1:pes_model.Nlyrs | ||
if i == 1; y_loc = 0 - 0.5*(y_cum(i) - 0); | ||
else; y_loc = -y_cum(i-1) - 0.5*(y_cum(i) - y_cum(i-1)); | ||
end | ||
if i == pes_model.Nlyrs | ||
text(0, y_loc, "(Bulk) "+string(pes_model.lyr_mat{i}),... | ||
'color', 'k', 'horizontalalignment', 'center', 'verticalalignment', 'middle', 'FontWeight','bold', 'FontSize',10); | ||
else | ||
text(0, y_loc, sprintf("(Layer %i) ",i)+string(pes_model.lyr_mat{i}),... | ||
'color', 'k', 'horizontalalignment', 'center', 'verticalalignment', 'middle', 'FontWeight','bold', 'FontSize',10); | ||
end | ||
end | ||
% - Box Styling and Axis properties | ||
ylabel('Depth From Surface [nm]', 'fontweight', 'bold'); | ||
title('Sample model stack'); | ||
axis([-x_width, x_width, -1*max(y_cum(:)), 0]); | ||
% - Formatting the axes | ||
ax = gca; | ||
% Font properties | ||
ax.FontName = 'Segoe UI'; | ||
ax.FontWeight = 'normal'; | ||
ax.FontSize = 10; | ||
% Tick properties | ||
ax.XMinorTick = 'off'; | ||
ax.YMinorTick = 'off'; | ||
ax.TickDir = 'both'; | ||
ax.XColor = [0 0 0]; | ||
ax.YColor = [0 0 0]; | ||
% Ruler properties | ||
ax.XAxisLocation = 'bottom'; % 'bottom' | 'top' | 'origin' | ||
ax.YAxisLocation = 'left'; % 'left' | 'right' | 'origin' | ||
% Box Styling properties | ||
ax.Color = [1 1 1]; | ||
ax.Box = 'off'; % 'on' | 'off' | ||
ax.LineWidth = 0.75; | ||
ax.Layer = 'Top'; | ||
%% 4.2 - Plotting the intensity profiles for each layer | ||
subplot(1,3,[2,3]); hold on; | ||
% - Filing through each layer | ||
for i = 1:pes_model.Nlyrs | ||
% -- If only one angle is given | ||
if length(pes_model.theta) == 1 | ||
plot(pes_model.hv, pes_model.lyr_ints0{i}, 'k.-', 'color', lyr_cols{i}, 'markerfacecolor', lyr_cols{i}, 'linewidth', 2.5); | ||
% -- If a range of angles are to be plotted | ||
else | ||
num_cols = length(pes_model.theta); | ||
start_col = lyr_cols{i}; | ||
end_col = lyr_cols{i} + 0.50*(1-lyr_cols{i}); | ||
colors_p = [linspace(start_col(1),end_col(1),num_cols)', linspace(start_col(2),end_col(2),num_cols)', linspace(start_col(3),end_col(3),num_cols)']; | ||
for j = 1:length(pes_model.theta) | ||
plot(pes_model.hv, pes_model.lyr_ints0{i}(j,:), 'k.-', 'color', colors_p(j,:), 'markerfacecolor', colors_p(j,:), 'linewidth', 2.5); | ||
end | ||
end | ||
leg_labels{i} = string(pes_model.lyr_mat{i})+"("+string(pes_model.lyr_cls{i})+")"; | ||
leg_cols{i} = plot(nan, 'k.-', 'color', lyr_cols{i}, 'markerfacecolor', lyr_cols{i}, 'linewidth', 2.5); | ||
end | ||
% -- Formatting the axes | ||
legend([leg_cols{:}], leg_labels, 'location', 'best'); | ||
title('Photoelectron intensities vs photon energy'); | ||
xlabel('Photon energy [eV]', 'Interpreter', 'none', 'FontWeight', 'bold'); | ||
ylabel('Relative Contribution', 'Interpreter', 'none', 'FontWeight', 'bold'); | ||
ylim([0, 1.00]); | ||
% - Formatting the axes | ||
ax = gca; | ||
% Font properties | ||
ax.FontName = 'Segoe UI'; | ||
ax.FontWeight = 'normal'; | ||
ax.FontSize = 10; | ||
% Tick properties | ||
ax.XMinorTick = 'off'; | ||
ax.YMinorTick = 'off'; | ||
ax.TickDir = 'both'; | ||
ax.XColor = [0 0 0]; | ||
ax.YColor = [0 0 0]; | ||
% Ruler properties | ||
ax.XAxisLocation = 'bottom'; % 'bottom' | 'top' | 'origin' | ||
ax.YAxisLocation = 'right'; % 'left' | 'right' | 'origin' | ||
% Box Styling properties | ||
ax.Color = [1 1 1]; | ||
ax.Box = 'off'; % 'on' | 'off' | ||
ax.LineWidth = 0.75; | ||
ax.Layer = 'Top'; |
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...ase-v1.0.1/N Layer PES Intensity Modelling/n-layer model/view_nlayer_pes_model_vs_theta.m
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function fig = view_nlayer_pes_model_vs_theta(pes_model, lyr_cols) | ||
% fig = view_nlayer_pes_model_vs_theta(pes_model, lyr_cols) | ||
% This function plots the solutions to the 'nlayer_pes_model()' function; | ||
% the n-layered sample stack and the corresponding photoelectron | ||
% contribution from each one of the layers. The user can input the colors | ||
% for each one of the layers using the 'lyr_cols' argument; this is | ||
% convenient when you want to color-match the schematic to your own | ||
% drawings. | ||
% | ||
% IN: | ||
% - pes_model: data structure that contains all the pes model parameters and variables (from 'nlayer_pes_model()'). | ||
% - lyr_cols: Mx1 cell-vector of the [R,G,B] color of each independent layer. | ||
% | ||
% OUT: | ||
% - fig: MATLAB figure object with the ARPES data plotted. | ||
|
||
%% Default parameters | ||
def_cols = flipud(num2cell([0.25,0.25,0.25;lines(length(pes_model.lyr_mat)-1)], 2)); | ||
% -- Defining the default parameters | ||
if nargin < 2; lyr_cols = def_cols; end | ||
if isempty(lyr_cols); lyr_cols = def_cols; end | ||
|
||
%% 1 - Plotting the the model solutions | ||
fig = figure(); | ||
fig.Position(3) = 900; | ||
fig.Position(4) = 450; | ||
%% 1.1 - Plotting the intensity profiles for each layer | ||
subplot(1,3,1); hold on; | ||
x_width = 5; | ||
bulk_thickness = 5; | ||
if pes_model.Nlyrs == 1 | ||
y_cum = cell2mat(pes_model.lyr_thick); | ||
else | ||
y_cum = cumsum(cell2mat(pes_model.lyr_thick)); | ||
y_cum(isinf(y_cum)) = y_cum(end-1) + bulk_thickness; | ||
end | ||
% -- Plotting each layer from bottom-up | ||
for i = pes_model.Nlyrs:-1:1 | ||
patch([-1, -1, 1, 1, -1].*x_width, [0, y_cum(i), y_cum(i), 0, 0].*-1,... | ||
lyr_cols{i}, 'edgecolor', [0 0 0]); | ||
end | ||
% -- Adding text for each material type | ||
for i = 1:pes_model.Nlyrs | ||
if i == 1; y_loc = 0 - 0.5*(y_cum(i) - 0); | ||
else; y_loc = -y_cum(i-1) - 0.5*(y_cum(i) - y_cum(i-1)); | ||
end | ||
if i == pes_model.Nlyrs | ||
text(0, y_loc, "(Bulk) "+string(pes_model.lyr_mat{i}),... | ||
'color', 'k', 'horizontalalignment', 'center', 'verticalalignment', 'middle', 'FontWeight','bold', 'FontSize',10); | ||
else | ||
text(0, y_loc, sprintf("(Layer %i) ",i)+string(pes_model.lyr_mat{i}),... | ||
'color', 'k', 'horizontalalignment', 'center', 'verticalalignment', 'middle', 'FontWeight','bold', 'FontSize',10); | ||
end | ||
end | ||
% - Box Styling and Axis properties | ||
ylabel('Depth From Surface [nm]', 'fontweight', 'bold'); | ||
title('Sample model stack'); | ||
axis([-x_width, x_width, -1*max(y_cum(:)), 0]); | ||
% - Formatting the axes | ||
ax = gca; | ||
% Font properties | ||
ax.FontName = 'Segoe UI'; | ||
ax.FontWeight = 'normal'; | ||
ax.FontSize = 10; | ||
% Tick properties | ||
ax.XMinorTick = 'off'; | ||
ax.YMinorTick = 'off'; | ||
ax.TickDir = 'both'; | ||
ax.XColor = [0 0 0]; | ||
ax.YColor = [0 0 0]; | ||
% Ruler properties | ||
ax.XAxisLocation = 'bottom'; % 'bottom' | 'top' | 'origin' | ||
ax.YAxisLocation = 'left'; % 'left' | 'right' | 'origin' | ||
% Box Styling properties | ||
ax.Color = [1 1 1]; | ||
ax.Box = 'off'; % 'on' | 'off' | ||
ax.LineWidth = 0.75; | ||
ax.Layer = 'Top'; | ||
%% 4.2 - Plotting the intensity profiles for each layer | ||
subplot(1,3,[2,3]); hold on; | ||
% - Filing through each layer | ||
for i = 1:pes_model.Nlyrs | ||
% -- If only one photon energy is given | ||
if length(pes_model.hv) == 1 | ||
plot(pes_model.theta, pes_model.lyr_ints0{i}, 'k.-', 'color', lyr_cols{i}, 'markerfacecolor', lyr_cols{i}, 'linewidth', 2.5); | ||
% -- If a range of angles are to be plotted | ||
else | ||
num_cols = length(pes_model.hv); | ||
start_col = lyr_cols{i}; | ||
end_col = lyr_cols{i} + 0.50*(1-lyr_cols{i}); | ||
colors_p = [linspace(start_col(1),end_col(1),num_cols)', linspace(start_col(2),end_col(2),num_cols)', linspace(start_col(3),end_col(3),num_cols)']; | ||
for j = 1:length(pes_model.hv) | ||
plot(pes_model.theta, pes_model.lyr_ints0{i}(:,j), 'k.-', 'color', colors_p(j,:), 'markerfacecolor', colors_p(j,:), 'linewidth', 2.5); | ||
end | ||
end | ||
leg_labels{i} = string(pes_model.lyr_mat{i})+"("+string(pes_model.lyr_cls{i})+")"; | ||
leg_cols{i} = plot(nan, 'k.-', 'color', lyr_cols{i}, 'markerfacecolor', lyr_cols{i}, 'linewidth', 2.5); | ||
end | ||
% -- Formatting the axes | ||
legend([leg_cols{:}], leg_labels, 'location', 'best'); | ||
title('Photoelectron intensities vs theta'); | ||
xlabel('Emission Angle [deg.]', 'Interpreter', 'none', 'FontWeight', 'bold'); | ||
ylabel('Relative Contribution', 'Interpreter', 'none', 'FontWeight', 'bold'); | ||
xlim([0, 90]); | ||
ylim([0, 1.00]); | ||
% - Formatting the axes | ||
ax = gca; | ||
% Font properties | ||
ax.FontName = 'Segoe UI'; | ||
ax.FontWeight = 'normal'; | ||
ax.FontSize = 10; | ||
% Tick properties | ||
ax.XMinorTick = 'off'; | ||
ax.YMinorTick = 'off'; | ||
ax.TickDir = 'both'; | ||
ax.XColor = [0 0 0]; | ||
ax.YColor = [0 0 0]; | ||
% Ruler properties | ||
ax.XAxisLocation = 'bottom'; % 'bottom' | 'top' | 'origin' | ||
ax.YAxisLocation = 'right'; % 'left' | 'right' | 'origin' | ||
% Box Styling properties | ||
ax.Color = [1 1 1]; | ||
ax.Box = 'off'; % 'on' | 'off' | ||
ax.LineWidth = 0.75; | ||
ax.Layer = 'Top'; |
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