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% ACCELERATE_GRADIENTS use the Nesterov's Accelerated Gradient method
%
% cache = accelerate_gradients(self, par, cache, iter)
%
% ** self structure containing inputs: e.g. current reconstruction results, data, mask, positions, pixel size, ..
% ** par structure containing parameters for the engines
% ** cache structure with precalculated values to avoid unnecessary overhead
% ** iter number of the current iteration
%
% returns:
% ** self updated structure containing inputs
% ** cache structure with precalculated values - stores the previous accelerated gradients updates
%
% Academic License Agreement
%
% Source Code
%
% Introduction
% This license agreement sets forth the terms and conditions under which the PAUL SCHERRER INSTITUT (PSI), CH-5232 Villigen-PSI, Switzerland (hereafter "LICENSOR")
% will grant you (hereafter "LICENSEE") a royalty-free, non-exclusive license for academic, non-commercial purposes only (hereafter "LICENSE") to use the cSAXS
% ptychography MATLAB package computer software program and associated documentation furnished hereunder (hereafter "PROGRAM").
%
% Terms and Conditions of the LICENSE
% 1. LICENSOR grants to LICENSEE a royalty-free, non-exclusive license to use the PROGRAM for academic, non-commercial purposes, upon the terms and conditions
% hereinafter set out and until termination of this license as set forth below.
% 2. LICENSEE acknowledges that the PROGRAM is a research tool still in the development stage. The PROGRAM is provided without any related services, improvements
% or warranties from LICENSOR and that the LICENSE is entered into in order to enable others to utilize the PROGRAM in their academic activities. It is the
% LICENSEEs responsibility to ensure its proper use and the correctness of the results.
% 3. THE PROGRAM IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, FITNESS FOR
% A PARTICULAR PURPOSE AND NONINFRINGEMENT OF ANY PATENTS, COPYRIGHTS, TRADEMARKS OR OTHER RIGHTS. IN NO EVENT SHALL THE LICENSOR, THE AUTHORS OR THE COPYRIGHT
% HOLDERS BE LIABLE FOR ANY CLAIM, DIRECT, INDIRECT OR CONSEQUENTIAL DAMAGES OR OTHER LIABILITY ARISING FROM, OUT OF OR IN CONNECTION WITH THE PROGRAM OR THE USE
% OF THE PROGRAM OR OTHER DEALINGS IN THE PROGRAM.
% 4. LICENSEE agrees that it will use the PROGRAM and any modifications, improvements, or derivatives of PROGRAM that LICENSEE may create (collectively,
% "IMPROVEMENTS") solely for academic, non-commercial purposes and that any copy of PROGRAM or derivatives thereof shall be distributed only under the same
% license as PROGRAM. The terms "academic, non-commercial", as used in this Agreement, mean academic or other scholarly research which (a) is not undertaken for
% profit, or (b) is not intended to produce works, services, or data for commercial use, or (c) is neither conducted, nor funded, by a person or an entity engaged
% in the commercial use, application or exploitation of works similar to the PROGRAM.
% 5. LICENSEE agrees that it shall make the following acknowledgement in any publication resulting from the use of the PROGRAM or any translation of the code into
% another computing language:
% "Data processing was carried out using the cSAXS ptychography MATLAB package developed by the Science IT and the coherent X-ray scattering (CXS) groups, Paul
% Scherrer Institut, Switzerland."
%
% Additionally, any publication using the package, or any translation of the code into another computing language should cite for difference map:
% P. Thibault, M. Dierolf, A. Menzel, O. Bunk, C. David, F. Pfeiffer, High-resolution scanning X-ray diffraction microscopy, Science 321, 379382 (2008).
% (doi: 10.1126/science.1158573),
% for mixed coherent modes:
% P. Thibault and A. Menzel, Reconstructing state mixtures from diffraction measurements, Nature 494, 6871 (2013). (doi: 10.1038/nature11806),
% for LSQ-ML method
% M. Odstrcil, A. Menzel, M.G. Sicairos, Iterative least-squares solver for generalized maximum-likelihood ptychography, Optics Express, 2018
% for OPRP method
% M. Odstrcil, P. Baksh, S. A. Boden, R. Card, J. E. Chad, J. G. Frey, W. S. Brocklesby, "Ptychographic coherent diffractive imaging with orthogonal probe relaxation." Optics express 24.8 (2016): 8360-8369
% and/or for multislice:
% E. H. R. Tsai, I. Usov, A. Diaz, A. Menzel, and M. Guizar-Sicairos, X-ray ptychography with extended depth of field, Opt. Express 24, 2908929108 (2016).
% 6. Except for the above-mentioned acknowledgment, LICENSEE shall not use the PROGRAM title or the names or logos of LICENSOR, nor any adaptation thereof, nor the
% names of any of its employees or laboratories, in any advertising, promotional or sales material without prior written consent obtained from LICENSOR in each case.
% 7. Ownership of all rights, including copyright in the PROGRAM and in any material associated therewith, shall at all times remain with LICENSOR, and LICENSEE
% agrees to preserve same. LICENSEE agrees not to use any portion of the PROGRAM or of any IMPROVEMENTS in any machine-readable form outside the PROGRAM, nor to
% make any copies except for its internal use, without prior written consent of LICENSOR. LICENSEE agrees to place the following copyright notice on any such copies:
% © All rights reserved. PAUL SCHERRER INSTITUT, Switzerland, Laboratory for Macromolecules and Bioimaging, 2017.
% 8. The LICENSE shall not be construed to confer any rights upon LICENSEE by implication or otherwise except as specifically set forth herein.
% 9. DISCLAIMER: LICENSEE shall be aware that Phase Focus Limited of Sheffield, UK has an international portfolio of patents and pending applications which relate
% to ptychography and that the PROGRAM may be capable of being used in circumstances which may fall within the claims of one or more of the Phase Focus patents,
% in particular of patent with international application number PCT/GB2005/001464. The LICENSOR explicitly declares not to indemnify the users of the software
% in case Phase Focus or any other third party will open a legal action against the LICENSEE due to the use of the program.
% 10. This Agreement shall be governed by the material laws of Switzerland and any dispute arising out of this Agreement or use of the PROGRAM shall be brought before
% the courts of Zürich, Switzerland.
%
function [self,cache] = accelerate_gradients(self, par, cache, iter)
%% accelerated gradients extension, tries to look ahead in direction of the last update
if iter == par.accelerated_gradients_start
cache.object_prev = {self.object, self.object};
cache.probe_prev = {self.probe, self.probe};
for ii = 1:length(cache.illum_sum_0)
cache.update_weights{ii} = cache.illum_sum_0{ii}.^2 ./ (cache.illum_sum_0{ii}.^2 + 0.1*cache.MAX_ILLUM(ii)^2);
end
elseif iter > par.accelerated_gradients_start
object_start = max(par.object_change_start, par.accelerated_gradients_start);
probe_start = max(par.probe_change_start, par.accelerated_gradients_start);
cache.object_prev{1} = cache.object_prev{2};
cache.object_prev{2} = self.object;
cache.probe_prev{1} = cache.probe_prev{2};
cache.probe_prev{2} = self.probe;
% accelerate the object reconstructions
if iter > par.object_change_start
beta = (iter-object_start+1)/(iter-object_start+3);
for ii = 1:size(self.object,1)
for layer = 1:size(self.object,2)
if ii == 1 && utils.verbose() > 3
plotting.smart_figure(555)
update = cache.update_weights{ii}.* (self.object{ii,layer} - cache.object_prev{1}{ii,layer});
plotting.imagesc3D(update)
title('Acceleration step in the Nesterov method')
axis xy off
utils.verbose(0, 'Norm of accelerated gradient = %g', math.norm2(update) )
drawnow
end
self.object{ii,layer} = self.object{ii,layer} + ...
beta*cache.update_weights{ii}.*(self.object{ii,layer} - cache.object_prev{1}{ii,layer});
end
end
end
% accelerate only the first OPR mode of the probe
if iter > par.probe_change_start
beta = (iter-probe_start+1)/(iter-probe_start+3);
for ii = 1:numel(self.probe)
self.probe{ii}(:,:,:,1) = self.probe{ii}(:,:,:,1) + ...
beta.*(self.probe{ii}(:,:,:,1) - cache.probe_prev{1}{ii}(:,:,:,1));
end
end
end
end