k-Wave Toolbox |
On this page… |
---|
This example demonstrates how the directionality of sensor elements can give rise to artefacts in time reversal photoacoustic image reconstruction. It builds on the Sensor Element Directivity in 2D and 2D Time Reversal Reconstruction For A Line Sensor examples.
For a more detailed discussion of this example and the underlying techniques, see B. T. Cox and B. E. Treeby, "Effect of sensor directionality on photoacoustic imaging: A study using the k-Wave toolbox," in Proc. SPIE 7564, p. 75640I, 2010.
The simulation is first invoked using a rectangular binary sensor mask with omnidirectional elements in the same way as previous examples. Directionality is then added to the sensor elements by assigning an angle to the corresponding elements in an Nx by Ny matrix passed to sensor.directivity_angle
. These are assigned such that the maximum sensitivity of each sensor face faces inward.
% define a four-sided, square sensor sensor.mask = zeros(kgrid.Nx, kgrid.Ny); sensor.mask(1, :) = 1; sensor.mask(end, :) = 1; sensor.mask(:, 1) = 1; sensor.mask(:, end) = 1; % run the simulation for omnidirectional detector elements sensor_data = kspaceFirstOrder2D(kgrid, medium, source, sensor, input_args{:}); % define the directionality of the sensor elements sensor.directivity_angle = zeros(kgrid.Nx, kgrid.Ny); sensor.directivity_angle(1, :) = 0; % max sensitivity in x direction sensor.directivity_angle(end, :) = 0; % max sensitivity in x direction sensor.directivity_angle(:, 1) = pi/2; % max sensitivity in y direction sensor.directivity_angle(:, end) = pi/2; % max sensitivity in y direction % define the directivity size sensor.directivity_size = 20*kgrid.dx; % run the simulation with directional elements sensor_data_directional = kspaceFirstOrder2D(kgrid, medium, source, sensor, input_args{:});
To examine the effect of sensor directionality on time reversal image reconstruction, the sensor data recorded from both the omni-directional and directional sensor elements is used to reconstruct the initial photoacoustic pressure distribution.
% reset the initial pressure source.p0 = 0; % assign the time reversal data for the omnidirectional case sensor.time_reversal_boundary_data = sensor_data; % run the time reversal reconstruction p0_recon = kspaceFirstOrder2D(kgrid, medium, source, sensor, input_args{:}); % assign the time reversal data for the directional case sensor.time_reversal_boundary_data = sensor_data_directional; % run the time reversal reconstruction with directional elements p0_recon_directional = kspaceFirstOrder2D(kgrid, medium, source, sensor, input_args{:});
The reconstructed pressure distributions are shown below. For the omni-directional sensor, the initial pressure is reconstructed almost exactly (note, the inverse crime in which the same simulation parameters are used in both simulation and reconstruction has been committed). However, when using the directional sensor, image artefacts are introduced into the reconstruction.
3D Time Reversal Reconstruction For A Spherical Sensor | Image Reconstruction With Bandlimited Sensors |
© 2009-2014 Bradley Treeby and Ben Cox.