Loading csst_mci_sim/CTI/CTI.pydeleted 100644 → 0 +0 −177 Original line number Diff line number Diff line """ Charge Transfer Inefficiency ============================ This file contains a simple class to run a CDM03 CTI model developed by Alex Short (ESA). This now contains both the official CDM03 and a new version that allows different trap parameters in parallel and serial direction. :requires: NumPy :requires: CDM03 (FORTRAN code, f2py -c -m cdm03bidir cdm03bidir.f90) :version: 0.35 """ import numpy as np #CDM03bidir class CDM03bidir(): """ Class to run CDM03 CTI model, class Fortran routine to perform the actual CDM03 calculations. :param settings: input parameters :type settings: dict :param data: input data to be radiated :type data: ndarray :param log: instance to Python logging :type log: logging instance """ def __init__(self, settings, data, log=None): """ Class constructor. :param settings: input parameters :type settings: dict :param data: input data to be radiated :type data: ndarray :param log: instance to Python logging :type log: logging instance """ self.data = data self.values = dict(quads=(0,1,2,3), xsize=2048, ysize=2066, dob=0.0, rdose=8.0e9) self.values.update(settings) self.log = log self._setupLogger() #default CDM03 settings self.params = dict(beta_p=0.6, beta_s=0.6, fwc=200000., vth=1.168e7, vg=6.e-11, t=20.48e-3, sfwc=730000., svg=1.0e-10, st=5.0e-6, parallel=1., serial=0.0) #update with inputs self.params.update(self.values) #read in trap information trapdata = np.loadtxt(self.values['dir_path']+self.values['paralleltrapfile']) if trapdata.ndim > 1: self.nt_p = trapdata[:, 0] self.sigma_p = trapdata[:, 1] self.taur_p = trapdata[:, 2] else: #only one trap species self.nt_p = [trapdata[0],] self.sigma_p = [trapdata[1],] self.taur_p = [trapdata[2],] trapdata = np.loadtxt(self.values['dir_path']+self.values['serialtrapfile']) if trapdata.ndim > 1: self.nt_s = trapdata[:, 0] self.sigma_s = trapdata[:, 1] self.taur_s = trapdata[:, 2] else: #only one trap species self.nt_s = [trapdata[0],] self.sigma_s = [trapdata[1],] self.taur_s = [trapdata[2],] #scale thibaut's values if 'thibaut' in self.values['parallelTrapfile']: self.nt_p /= 0.576 #thibaut's values traps / pixel self.sigma_p *= 1.e4 #thibaut's values in m**2 if 'thibaut' in self.values['serialTrapfile']: self.nt_s *= 0.576 #thibaut's values traps / pixel #should be division? self.sigma_s *= 1.e4 #thibaut's values in m**2 def _setupLogger(self): """ Set up the logger. """ self.logger = True # if self.log is None: # self.logger = False def applyRadiationDamage(self, data, iquadrant=0): """ Apply radian damage based on FORTRAN CDM03 model. The method assumes that input data covers only a single quadrant defined by the iquadrant integer. :param data: imaging data to which the CDM03 model will be applied to. :type data: ndarray :param iquandrant: number of the quadrant to process :type iquandrant: int cdm03 - Function signature:: sout = cdm03(sinp,iflip,jflip,dob,rdose,in_nt,in_sigma,in_tr,[xdim,ydim,zdim]) Required arguments: sinp : input rank-2 array('d') with bounds (xdim,ydim) iflip : input int jflip : input int dob : input float rdose : input float in_nt : input rank-1 array('d') with bounds (zdim) in_sigma : input rank-1 array('d') with bounds (zdim) in_tr : input rank-1 array('d') with bounds (zdim) Optional arguments: xdim := shape(sinp,0) input int ydim := shape(sinp,1) input int zdim := len(in_nt) input int Return objects: sout : rank-2 array('d') with bounds (xdim,ydim) .. Note:: Because Python/NumPy arrays are different row/column based, one needs to be extra careful here. NumPy.asfortranarray will be called to get an array laid out in Fortran order in memory. Before returning the array will be laid out in memory in C-style (row-major order). :return: image that has been run through the CDM03 model :rtype: ndarray """"" #return data iflip = iquadrant / 2 jflip = iquadrant % 2 params = [self.params['beta_p'], self.params['beta_s'], self.params['fwc'], self.params['vth'], self.params['vg'], self.params['t'], self.params['sfwc'], self.params['svg'], self.params['st'], self.params['parallel'], self.params['serial']] if self.logger: self.log.info('nt_p=' + str(self.nt_p)) self.log.info('nt_s=' + str(self.nt_s)) self.log.info('sigma_p= ' + str(self.sigma_p)) self.log.info('sigma_s= ' + str(self.sigma_s)) self.log.info('taur_p= ' + str(self.taur_p)) self.log.info('taur_s= ' + str(self.taur_s)) self.log.info('dob=%f' % self.values['dob']) self.log.info('rdose=%e' % self.values['rdose']) self.log.info('xsize=%i' % data.shape[1]) self.log.info('ysize=%i' % data.shape[0]) self.log.info('quadrant=%i' % iquadrant) self.log.info('iflip=%i' % iflip) self.log.info('jflip=%i' % jflip) ################################################################################# ###modify #sys.path.append('../so') # from ifs_so.cdm03.cpython-38-x86_64-linux-gnu import cdm03bidir # import cdm03bidir from .mci_so import cdm03bidir CTIed = cdm03bidir.cdm03(np.asfortranarray(data), jflip, iflip, self.values['dob'], self.values['rdose'], self.nt_p, self.sigma_p, self.taur_p, self.nt_s, self.sigma_s, self.taur_s, params, [data.shape[0], data.shape[1], len(self.nt_p), len(self.nt_s), len(self.params)]) return np.asanyarray(CTIed) ################################################################################################################# ################################################################################################################# Loading
csst_mci_sim/CTI/CTI.pydeleted 100644 → 0 +0 −177 Original line number Diff line number Diff line """ Charge Transfer Inefficiency ============================ This file contains a simple class to run a CDM03 CTI model developed by Alex Short (ESA). This now contains both the official CDM03 and a new version that allows different trap parameters in parallel and serial direction. :requires: NumPy :requires: CDM03 (FORTRAN code, f2py -c -m cdm03bidir cdm03bidir.f90) :version: 0.35 """ import numpy as np #CDM03bidir class CDM03bidir(): """ Class to run CDM03 CTI model, class Fortran routine to perform the actual CDM03 calculations. :param settings: input parameters :type settings: dict :param data: input data to be radiated :type data: ndarray :param log: instance to Python logging :type log: logging instance """ def __init__(self, settings, data, log=None): """ Class constructor. :param settings: input parameters :type settings: dict :param data: input data to be radiated :type data: ndarray :param log: instance to Python logging :type log: logging instance """ self.data = data self.values = dict(quads=(0,1,2,3), xsize=2048, ysize=2066, dob=0.0, rdose=8.0e9) self.values.update(settings) self.log = log self._setupLogger() #default CDM03 settings self.params = dict(beta_p=0.6, beta_s=0.6, fwc=200000., vth=1.168e7, vg=6.e-11, t=20.48e-3, sfwc=730000., svg=1.0e-10, st=5.0e-6, parallel=1., serial=0.0) #update with inputs self.params.update(self.values) #read in trap information trapdata = np.loadtxt(self.values['dir_path']+self.values['paralleltrapfile']) if trapdata.ndim > 1: self.nt_p = trapdata[:, 0] self.sigma_p = trapdata[:, 1] self.taur_p = trapdata[:, 2] else: #only one trap species self.nt_p = [trapdata[0],] self.sigma_p = [trapdata[1],] self.taur_p = [trapdata[2],] trapdata = np.loadtxt(self.values['dir_path']+self.values['serialtrapfile']) if trapdata.ndim > 1: self.nt_s = trapdata[:, 0] self.sigma_s = trapdata[:, 1] self.taur_s = trapdata[:, 2] else: #only one trap species self.nt_s = [trapdata[0],] self.sigma_s = [trapdata[1],] self.taur_s = [trapdata[2],] #scale thibaut's values if 'thibaut' in self.values['parallelTrapfile']: self.nt_p /= 0.576 #thibaut's values traps / pixel self.sigma_p *= 1.e4 #thibaut's values in m**2 if 'thibaut' in self.values['serialTrapfile']: self.nt_s *= 0.576 #thibaut's values traps / pixel #should be division? self.sigma_s *= 1.e4 #thibaut's values in m**2 def _setupLogger(self): """ Set up the logger. """ self.logger = True # if self.log is None: # self.logger = False def applyRadiationDamage(self, data, iquadrant=0): """ Apply radian damage based on FORTRAN CDM03 model. The method assumes that input data covers only a single quadrant defined by the iquadrant integer. :param data: imaging data to which the CDM03 model will be applied to. :type data: ndarray :param iquandrant: number of the quadrant to process :type iquandrant: int cdm03 - Function signature:: sout = cdm03(sinp,iflip,jflip,dob,rdose,in_nt,in_sigma,in_tr,[xdim,ydim,zdim]) Required arguments: sinp : input rank-2 array('d') with bounds (xdim,ydim) iflip : input int jflip : input int dob : input float rdose : input float in_nt : input rank-1 array('d') with bounds (zdim) in_sigma : input rank-1 array('d') with bounds (zdim) in_tr : input rank-1 array('d') with bounds (zdim) Optional arguments: xdim := shape(sinp,0) input int ydim := shape(sinp,1) input int zdim := len(in_nt) input int Return objects: sout : rank-2 array('d') with bounds (xdim,ydim) .. Note:: Because Python/NumPy arrays are different row/column based, one needs to be extra careful here. NumPy.asfortranarray will be called to get an array laid out in Fortran order in memory. Before returning the array will be laid out in memory in C-style (row-major order). :return: image that has been run through the CDM03 model :rtype: ndarray """"" #return data iflip = iquadrant / 2 jflip = iquadrant % 2 params = [self.params['beta_p'], self.params['beta_s'], self.params['fwc'], self.params['vth'], self.params['vg'], self.params['t'], self.params['sfwc'], self.params['svg'], self.params['st'], self.params['parallel'], self.params['serial']] if self.logger: self.log.info('nt_p=' + str(self.nt_p)) self.log.info('nt_s=' + str(self.nt_s)) self.log.info('sigma_p= ' + str(self.sigma_p)) self.log.info('sigma_s= ' + str(self.sigma_s)) self.log.info('taur_p= ' + str(self.taur_p)) self.log.info('taur_s= ' + str(self.taur_s)) self.log.info('dob=%f' % self.values['dob']) self.log.info('rdose=%e' % self.values['rdose']) self.log.info('xsize=%i' % data.shape[1]) self.log.info('ysize=%i' % data.shape[0]) self.log.info('quadrant=%i' % iquadrant) self.log.info('iflip=%i' % iflip) self.log.info('jflip=%i' % jflip) ################################################################################# ###modify #sys.path.append('../so') # from ifs_so.cdm03.cpython-38-x86_64-linux-gnu import cdm03bidir # import cdm03bidir from .mci_so import cdm03bidir CTIed = cdm03bidir.cdm03(np.asfortranarray(data), jflip, iflip, self.values['dob'], self.values['rdose'], self.nt_p, self.sigma_p, self.taur_p, self.nt_s, self.sigma_s, self.taur_s, params, [data.shape[0], data.shape[1], len(self.nt_p), len(self.nt_s), len(self.params)]) return np.asanyarray(CTIed) ################################################################################################################# #################################################################################################################