示例#1
0
    def __init__(self, power, FWHM_ps, center_wavelength_nm,
                 time_window_ps = 10., frep_MHz = 100., NPTS = 2**10, 
                 GDD = 0, TOD = 0, chirp2 = 0, chirp3 = 0,
                 power_is_avg = False):
        """Generate sinc pulse A(t) = sqrt(peak_power[W]) * sin(t/T0)/(t/T0)
        centered at wavelength center_wavelength_nm (nm).
        The width is given by FWHM_ps, which is the full-width-at-half-maximum 
        in picoseconds. T0 is equal th FWHM/3.7909885.
        time_window_ps sets temporal grid size. Optional GDD and TOD are
        in ps^2 and ps^3."""
        Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
        # make sure we weren't passed mks units        
        assert (center_wavelength_nm > 1.0) 
        assert (time_window_ps > 1.0 )                
        self.set_center_wavelength_nm(center_wavelength_nm)        
        self.set_time_window_ps(time_window_ps)

        T0_ps = FWHM_ps/3.7909885
        ### Generate pulse
        if not power_is_avg:
            # numpy.sinc is sin(pi*x)/(pi*x), so we divide by pi
            self.set_AT( np.sqrt(power) * np.sinc(self.T_ps/(T0_ps*np.pi)) ) 
        else:
            self.set_AT( 1 / np.sinc(np.pi * self.T_ps/(T0_ps*np.pi)) )
            self.set_AT(self.AT * np.sqrt( power / ( frep_MHz*1.0e6 * self.calc_epp()) ))
        
        self.chirp_pulse_W(GDD, TOD)
        self.chirp_pulse_T(chirp2, chirp3, T0_ps)   
示例#2
0
    def __init__(self, power, FWHM_ps, center_wavelength_nm,
                 time_window_ps = 10., frep_MHz = 100., NPTS = 2**10, 
                 GDD = 0, TOD = 0, chirp2 = 0, chirp3 = 0,
                 power_is_avg = False):
        """Generate sinc pulse A(t) = sqrt(peak_power[W]) * sin(t/T0)/(t/T0)
        centered at wavelength center_wavelength_nm (nm).
        The width is given by FWHM_ps, which is the full-width-at-half-maximum 
        in picoseconds. T0 is equal th FWHM/3.7909885.
        time_window_ps sets temporal grid size. Optional GDD and TOD are
        in ps^2 and ps^3."""
        Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
        # make sure we weren't passed mks units        
        assert (center_wavelength_nm > 1.0) 
        assert (time_window_ps > 1.0 )                
        self.set_center_wavelength_nm(center_wavelength_nm)        
        self.set_time_window_ps(time_window_ps)

        T0_ps = FWHM_ps/3.7909885
        ### Generate pulse
        if not power_is_avg:
            # numpy.sinc is sin(pi*x)/(pi*x), so we divide by pi
            self.set_AT( np.sqrt(power) * np.sinc(self.T_ps/(T0_ps*np.pi)) ) 
        else:
            self.set_AT( 1 / np.sinc(np.pi * self.T_ps/(T0_ps*np.pi)) )
            self.set_AT(self.AT * np.sqrt( power / ( frep_MHz*1.0e6 * self.calc_epp()) ))
        
        self.chirp_pulse_W(GDD, TOD)
        self.chirp_pulse_T(chirp2, chirp3, T0_ps)   
示例#3
0
    def __init__(self, avg_power, center_wavelength_nm, time_window_ps = 10.0,
                 NPTS = 2**8,offset_from_center_THz = None):
        Pulse.__init__(self, n = NPTS)
        # make sure we weren't passed mks units
        assert (center_wavelength_nm > 1.0) 
        assert (time_window_ps > 1.0 )        

        if offset_from_center_THz is None:            
            self.set_center_wavelength_nm(center_wavelength_nm)
            self.set_time_window_ps(time_window_ps)        
         
            # Set the time domain to be CW, which should give us a delta function in
            # frequency. Then normalize that delta function (in frequency space) to
            # the average power. Note that frep does not factor in here.
            self.set_AT(np.ones(self.NPTS,))
            self.set_AW(self.AW * np.sqrt(avg_power) / sum(abs(self.AW)) )
        else:
            dF = 1.0/time_window_ps
            n_offset = np.round( offset_from_center_THz/dF)      
            
            center_THz = self._c_nmps/center_wavelength_nm -\
                                    n_offset * dF
            center_nm = self._c_nmps / center_THz
            self.set_time_window_ps(time_window_ps)
        
            self.set_center_wavelength_nm(center_nm)
            aws = np.zeros((self.NPTS, ))
            aws[int(self.NPTS/2.0) + int(n_offset)  ] = 1.0 *np.sqrt(avg_power)
            self.set_AW(aws)
示例#4
0
 def __init__(self, power, T0_ps, center_wavelength_nm,
              time_window_ps = 10., frep_MHz = 100., NPTS = 2**10, 
              GDD = 0, TOD = 0, chirp2 = 0, chirp3 = 0,
              power_is_avg = False):
     """Generate a squared-hyperbolic secant "sech" pulse 
              A(t) = sqrt(P0 [W]) * sech(t/T0 [ps])
     centered at wavelength center_wavelength_nm (nm).
     time_window (ps) sets temporal grid size. 
     
     Optional GDD and TOD are in ps^2 and ps^3.
       
     Note: The full-width-at-half-maximum (FWHM) is given by 
              T0_ps * 1.76   
     """
     Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
     # make sure we weren't passed mks units        
     assert (center_wavelength_nm > 1.0) 
     assert (time_window_ps > 1.0 )                
     self.set_center_wavelength_nm(center_wavelength_nm)        
     self.set_time_window_ps(time_window_ps)
                     
     ### Generate pulse
     if not power_is_avg:
         # from https://www.rp-photonics.com/sech2_shaped_pulses.html
         self.set_AT( np.sqrt(power)/np.cosh(self.T_ps/T0_ps) )
     else:
         self.set_AT( 1 / np.cosh(self.T_ps/T0_ps) )
         self.set_AT(self.AT * np.sqrt( power / ( frep_MHz*1.0e6 * self.calc_epp()) ))
     
     self.chirp_pulse_W(GDD, TOD)
     self.chirp_pulse_T(chirp2, chirp3, T0_ps)            
示例#5
0
    def __init__(self, power, T0_ps, center_wavelength_nm,
                 time_window_ps = 10., frep_MHz = 100., NPTS = 2**10, 
                 GDD = 0, TOD = 0, chirp2 = 0, chirp3 = 0,
                 power_is_avg = False):
        """Generate Gaussian pulse A(t) = sqrt(peak_power[W]) * 
            exp( -(t/T0 [ps])^2 / 2 ) centered at wavelength 
            center_wavelength_nm (nm). time_window (ps) sets temporal grid
            size. Optional GDD and TOD are in ps^2 and ps^3.
        
        Note: For this definition of a Gaussian pulse, T0_ps is the 
              full-width-at-half-maximum (FWHM) of the pulse.
        """

        Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
        # make sure we weren't passed mks units        
        assert (center_wavelength_nm > 1.0) 
        assert (time_window_ps > 1.0 )        
        self.set_center_wavelength_nm(center_wavelength_nm)
        self.set_time_window_ps(time_window_ps)        
        
        GDD = GDD
        TOD = TOD
        
        # from https://www.rp-photonics.com/gaussian_pulses.html
        self.set_AT( np.sqrt(power) * np.exp(-2.77*0.5*self.T_ps**2/(T0_ps**2)) ) # input field (W^0.5) 
        if power_is_avg:            
            self.set_AT(self.AT * np.sqrt( power / ( frep_MHz*1.0e6 * self.calc_epp()) ))
        self.chirp_pulse_W(GDD, TOD)
        self.chirp_pulse_T(chirp2, chirp3, T0_ps)
示例#6
0
    def __init__(self, avg_power, center_wavelength_nm, time_window_ps = 10.0,
                 NPTS = 2**8,offset_from_center_THz = None):
        Pulse.__init__(self, n = NPTS)
        # make sure we weren't passed mks units
        assert (center_wavelength_nm > 1.0) 
        assert (time_window_ps > 1.0 )        

        if offset_from_center_THz is None:            
            self.set_center_wavelength_nm(center_wavelength_nm)
            self.set_time_window_ps(time_window_ps)        
         
            # Set the time domain to be CW, which should give us a delta function in
            # frequency. Then normalize that delta function (in frequency space) to
            # the average power. Note that frep does not factor in here.
            self.set_AT(np.ones(self.NPTS,))
            self.set_AW(self.AW * np.sqrt(avg_power) / sum(abs(self.AW)) )
        else:
            dF = 1.0/time_window_ps
            n_offset = np.round( offset_from_center_THz/dF)      
            
            center_THz = self._c_nmps/center_wavelength_nm -\
                                    n_offset * dF
            center_nm = self._c_nmps / center_THz
            self.set_time_window_ps(time_window_ps)
        
            self.set_center_wavelength_nm(center_nm)
            aws = np.zeros((self.NPTS, ))
            aws[int(self.NPTS/2.0) + int(n_offset)  ] = 1.0 *np.sqrt(avg_power)
            self.set_AW(aws)
示例#7
0
 def __init__(self, center_wavelength_nm, time_window_ps = 10., NPTS = 2**8,
              frep_MHz = None):
     Pulse.__init__(self, n = NPTS, frep_MHz = frep_MHz)
     self.set_center_wavelength_nm(center_wavelength_nm)
     self.set_time_window_ps(time_window_ps)        
     
     self.set_AW( 1e-30 * np.ones(self.NPTS) * np.exp(1j * 2 * np.pi *
              1j * np.random.rand(self.NPTS)))
示例#8
0
 def __init__(self, center_wavelength_nm, time_window_ps = 10., NPTS = 2**8,
              frep_MHz = None):
     Pulse.__init__(self, n = NPTS, frep_MHz = frep_MHz)
     self.set_center_wavelength_nm(center_wavelength_nm)
     self.set_time_window_ps(time_window_ps)        
     
     self.set_AW( 1e-30 * np.ones(self.NPTS) * np.exp(1j * 2 * np.pi *
              1j * np.random.rand(self.NPTS)))
示例#9
0
    def __init__(self, time_window_ps, center_wavelength_nm, power,frep_MHz = 100., NPTS = 2**10,
                 power_is_avg = False,
                 fileloc = '',
                 flip_phase = True):
        """Generate pulse from FROG data. Grid is centered at wavelength
        center_wavelength_nm (nm), but pulse properties are loaded from data
        file. If flip_phase is true, all phase is multiplied by -1 [useful
        for correcting direction of time ambiguity]. time_window (ps) sets 
        temporal grid size. 
        
        power sets the pulse energy:
        if power_is_epp is True  then the number is pulse energy [J] 
        if power_is_epp is False then the power is average power [W], and 
        is multiplied by frep to calculate pulse energy"""
        Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
        try:
            self.fileloc   = fileloc
            # make sure we weren't passed mks units
            assert (center_wavelength_nm > 1.0) 
            assert (time_window_ps > 1.0 )
            self.set_time_window_ps(time_window_ps)
            self.set_center_wavelength_nm(center_wavelength_nm) # reference wavelength (nm)                         
            
            # power -> EPP
            if power_is_avg:
                power = power / self.frep_mks
            
            # Read in retrieved FROG trace
            frog_data = np.genfromtxt(self.fileloc)
            wavelengths = frog_data[:,0]# (nm)
            intensity   = frog_data[:,1]# (arb. units)
            phase       = frog_data[:,2]# (radians)

            if flip_phase:
                phase = -1 * phase
                            
            pulse_envelope = interp1d(wavelengths, intensity, kind='linear',
                                      bounds_error=False,fill_value=0)
            phase_envelope = interp1d(wavelengths, phase, kind='linear', 
                                      bounds_error=False,fill_value=0)
                                      
            gridded_intensity   = pulse_envelope(self.wl_nm)
            gridded_phase       = phase_envelope(self.wl_nm)

            # Calculate time domain complex electric field A
            self.set_AW(gridded_intensity*np.exp(1j*gridded_phase))
            # Calculate normalization factor  to achieve requested 
            # pulse energy
            e_scale = np.sqrt(power / self.calc_epp() )
            self.set_AT(self.AT * e_scale )

        except IOError:
            print ('File not found.' )
示例#10
0
    def __init__(self, time_window_ps, center_wavelength_nm, power,frep_MHz = 100., NPTS = 2**10,
                 power_is_avg = False,
                 fileloc = '',
                 flip_phase = True):
        """Generate pulse from FROG data. Grid is centered at wavelength
        center_wavelength_nm (nm), but pulse properties are loaded from data
        file. If flip_phase is true, all phase is multiplied by -1 [useful
        for correcting direction of time ambiguity]. time_window (ps) sets 
        temporal grid size. 
        
        power sets the pulse energy:
        if power_is_epp is True  then the number is pulse energy [J] 
        if power_is_epp is False then the power is average power [W], and 
        is multiplied by frep to calculate pulse energy"""
        Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
        try:
            self.fileloc   = fileloc
            # make sure we weren't passed mks units
            assert (center_wavelength_nm > 1.0) 
            assert (time_window_ps > 1.0 )
            self.set_time_window_ps(time_window_ps)
            self.set_center_wavelength_nm(center_wavelength_nm) # reference wavelength (nm)                         
            
            # power -> EPP
            if power_is_avg:
                power = power / self.frep_mks
            
            # Read in retrieved FROG trace
            frog_data = np.genfromtxt(self.fileloc)
            wavelengths = frog_data[:,0]# (nm)
            intensity   = frog_data[:,1]# (arb. units)
            phase       = frog_data[:,2]# (radians)

            if flip_phase:
                phase = -1 * phase
                            
            pulse_envelope = interp1d(wavelengths, intensity, kind='linear',
                                      bounds_error=False,fill_value=0)
            phase_envelope = interp1d(wavelengths, phase, kind='linear', 
                                      bounds_error=False,fill_value=0)
                                      
            gridded_intensity   = pulse_envelope(self.wl_nm)
            gridded_phase       = phase_envelope(self.wl_nm)

            # Calculate time domain complex electric field A
            self.set_AW(gridded_intensity*np.exp(1j*gridded_phase))
            # Calculate normalization factor  to achieve requested 
            # pulse energy
            e_scale = np.sqrt(power / self.calc_epp() )
            self.set_AT(self.AT * e_scale )

        except IOError:
            print 'File not found.'
示例#11
0
 def filter(self, pulse_in, band, fiber, output_power=None):
     self.band0 = band / (2 * np.sqrt(np.log(2)))
     pulse_out = Pulse()
     pulse_out.clone_pulse(pulse_in)
     self.setup_fftw(pulse_in, fiber, output_power, raman_plots=False)
     self.T_BP = np.exp(-(self.wl_nm - self.center_wavelength_nm)**2 / 2 /
                        self.band0**2)
     pulse_out.set_AW(pulse_out.AW * self.T_BP)
     return pulse_out
示例#12
0
    def __init__(self, power, T0_ps, center_wavelength_nm,
                 time_window_ps = 10., frep_MHz = 100., NPTS = 2**10, 
                 GDD = 0, TOD = 0, chirp2 = 0, chirp3 = 0,
                 power_is_avg = False):
        """Generate Gaussian pulse A(t) = sqrt(peak_power[W]) * 
            exp( -(t/T0 [ps])^2 / 2 ) centered at wavelength 
            center_wavelength_nm (nm). time_window (ps) sets temporal grid
            size. Optional GDD and TOD are in ps^2 and ps^3."""

        Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
        # make sure we weren't passed mks units        
        assert (center_wavelength_nm > 1.0) 
        assert (time_window_ps > 1.0 )        
        self.set_center_wavelength_nm(center_wavelength_nm)
        self.set_time_window_ps(time_window_ps)        
        
        GDD = GDD
        TOD = TOD
                   
        self.set_AT( np.sqrt(power) * np.exp(-2.77*self.T_ps**2/(T0_ps**2)) ) # input field (W^0.5) 
        if power_is_avg:            
            self.set_AT(self.AT * np.sqrt( power / ( frep_MHz*1.0e6 * self.calc_epp()) ))
        self.chirp_pulse_W(GDD, TOD)
        self.chirp_pulse_T(chirp2, chirp3, T0_ps)
示例#13
0
 def __init__(self, power, T0_ps, center_wavelength_nm,
              time_window_ps = 10., frep_MHz = 100., NPTS = 2**10, 
              GDD = 0, TOD = 0, chirp2 = 0, chirp3 = 0,
              power_is_avg = False):
     """Generate sech pulse A(t) = sqrt(P0 [W]) * sech(t/T0 [ps])
     centered at wavelength center_wavelength_nm (nm).
     time_window (ps) sets temporal grid size. Optional GDD and TOD are
     in ps^2 and ps^3."""
     Pulse.__init__(self, frep_MHz = frep_MHz, n = NPTS)
     # make sure we weren't passed mks units        
     assert (center_wavelength_nm > 1.0) 
     assert (time_window_ps > 1.0 )                
     self.set_center_wavelength_nm(center_wavelength_nm)        
     self.set_time_window_ps(time_window_ps)
                     
     ### Generate pulse
     if not power_is_avg:
         self.set_AT( np.sqrt(power)/np.cosh(self.T_ps/T0_ps) )
     else:
         self.set_AT( 1 / np.cosh(self.T_ps/T0_ps) )
         self.set_AT(self.AT * np.sqrt( power / ( frep_MHz*1.0e6 * self.calc_epp()) ))
     
     self.chirp_pulse_W(GDD, TOD)
     self.chirp_pulse_T(chirp2, chirp3, T0_ps)            
示例#14
0
    def get_run(self, run_num=None, z_num=None):
        """ Return tuple of (pump, signal, idler) pulses for run # n at z index
        z_num . By default, returns last z step of last run."""
        if run_num is None:
            run_num = self.run_ctr - 1
        if run_num < 0 or run_num >= self.run_ctr:
            raise IndexError(str(run_num) + ' not a valid run index.')
        if z_num is None:
            z_num = -1

        run = self.root_name + '/run' + str(run_num)

        # Read in and generate pump pulse
        pump_field = self.tables_file.get_node(run + '/pump')[:, z_num]
        pump_Twind = self.tables_file.get_node(run + '/pump_Twind')[0]
        pump_center = self.tables_file.get_node(run + '/pump_center_nm')[0]
        p = Pulse()
        p.set_NPTS(len(pump_field))
        p.set_center_wavelength_nm(pump_center)
        p.set_time_window_ps(pump_Twind)
        p.set_AW(pump_field)
        p.set_frep_MHz(self.frep_Hz * 1.0e-6)

        # Read in and generate signal pulse
        sgnl_field = self.tables_file.get_node(run + '/sgnl')[:, z_num]
        sgnl_Twind = self.tables_file.get_node(run + '/sgnl_Twind')[0]
        sgnl_center = self.tables_file.get_node(run + '/sgnl_center_nm')[0]
        s = Pulse()
        s.set_NPTS(len(sgnl_field))
        s.set_center_wavelength_nm(sgnl_center)
        s.set_time_window_ps(sgnl_Twind)
        s.set_AW(sgnl_field)
        s.set_frep_MHz(self.frep_Hz * 1.0e-6)

        # Read in and generate idler pulse
        idlr_field = self.tables_file.get_node(run + '/idlr')[:, z_num]
        idlr_Twind = self.tables_file.get_node(run + '/idlr_Twind')[0]
        idlr_center = self.tables_file.get_node(run + '/idlr_center_nm')[0]
        i = Pulse()
        i.set_NPTS(len(idlr_field))
        i.set_center_wavelength_nm(idlr_center)
        i.set_time_window_ps(idlr_Twind)
        i.set_AW(idlr_field)
        i.set_frep_MHz(self.frep_Hz * 1.0e-6)

        return (p, s, i)
示例#15
0
    def get_run(self, run_num = None, z_num = None):
        """ Return tuple of (pump, signal, idler) pulses for run # n at z index
        z_num . By default, returns last z step of last run."""
        if run_num is None:
            run_num = self.run_ctr - 1
        if run_num < 0 or run_num >= self.run_ctr:
            raise IndexError(str(run_num)+' not a valid run index.')
        if z_num is None:
            z_num = -1
            
        run = self.root_name+'/run'+str(run_num)
        
        # Read in and generate pump pulse
        pump_field  = self.tables_file.get_node(run+'/pump')[:,z_num]
        pump_Twind  = self.tables_file.get_node(run+'/pump_Twind')[0]
        pump_center = self.tables_file.get_node(run+'/pump_center_nm')[0]
        p = Pulse()
        p.set_NPTS(len(pump_field))
        p.set_center_wavelength_nm(pump_center)
        p.set_time_window_ps(pump_Twind)
        p.set_AW(pump_field)
        p.set_frep_MHz(self.frep_Hz * 1.0e-6)
        
        # Read in and generate signal pulse
        sgnl_field  = self.tables_file.get_node(run+'/sgnl')[:,z_num]
        sgnl_Twind  = self.tables_file.get_node(run+'/sgnl_Twind')[0]
        sgnl_center = self.tables_file.get_node(run+'/sgnl_center_nm')[0]
        s = Pulse()
        s.set_NPTS(len(sgnl_field))
        s.set_center_wavelength_nm(sgnl_center)
        s.set_time_window_ps(sgnl_Twind)
        s.set_AW(sgnl_field)
        s.set_frep_MHz(self.frep_Hz * 1.0e-6)

        # Read in and generate idler pulse
        idlr_field  = self.tables_file.get_node(run+'/idlr')[:,z_num]
        idlr_Twind  = self.tables_file.get_node(run+'/idlr_Twind')[0]
        idlr_center = self.tables_file.get_node(run+'/idlr_center_nm')[0]
        i = Pulse()
        i.set_NPTS(len(idlr_field))
        i.set_center_wavelength_nm(idlr_center)
        i.set_time_window_ps(idlr_Twind)
        i.set_AW(idlr_field)
        i.set_frep_MHz(self.frep_Hz * 1.0e-6)
        
        return (p, s, i)
示例#16
0
    def propagate(self,
                  pulse_in,
                  fiber,
                  n_steps,
                  output_power=None,
                  reload_fiber_each_step=False):
        """
        This is the main user-facing function that allows a pulse to be 
        propagated along a fiber (or other nonlinear medium). 
        
        Parameters
        ----------
        
        pulse_in : pulse object
            this is an instance of the :class:`pynlo.light.PulseBase.Pulse` class.
        
        fiber : fiber object
            this is an instance of the :class:`pynlo.media.fibers.fiber.FiberInstance` class.
        
        n_steps : int
            the number of steps requested in the integrator output. Note: the RK4IP integrator
            uses an adaptive step size. It should pick the correct step size automatically,
            so setting n_steps should not affect the accuracy, just the number of points that
            are returned by this funciton.
        
        output_power : 
            This parameter is a mystery
    
        reload_fiber_each_step : boolean
            This flag determines if the fiber parameters should be reloaded every step. It is 
            necessary if the fiber dispersion or gamma changes along the fiber length. 
            :func:`pynlo.media.fibers.fiber.FiberInstance.set_dispersion_function` and 
            :func:`pynlo.media.fibers.fiber.FiberInstance.set_dispersion_function` should be used
            to specify how the dispersion and gamma change with the fiber length
        
        
        Returns
        -------
        z_positions : array of float
            an array of z-positions along the fiber (in meters)
        
        AW : 2D array of complex128
            A 2D numpy array corresponding to the intensities in each *frequency* bin for each
            step in the z-direction of the fiber. 
        
        AT : 2D array of complex128
            A 2D numpy array corresponding to the intensities in each *time* bin for each
            step in the z-direction of the fiber. 
        
        pulse_out : PulseBase object
            the pulse after it has propagated through the fiber. This object is suitable for propagation 
            through the next fiber!
        """

        n_steps = int(n_steps)

        # Copy parameters from pulse and fiber into class-wide variables
        z_positions = np.linspace(0, fiber.length, n_steps + 1)
        if n_steps == 1:
            delta_z = fiber.length
        else:
            delta_z = z_positions[1] - z_positions[0]

        AW = np.complex64(np.zeros((pulse_in.NPTS, n_steps)))
        AT = np.complex64(np.copy(AW))

        #print ("Pulse energy before", fiber.fibertype,":", \
        #      1e9 * pulse_in.calc_epp(), 'nJ' )

        pulse_out = Pulse()
        pulse_out.clone_pulse(pulse_in)
        self.setup_fftw(pulse_in, fiber, output_power, raman_plots=False)
        self.load_fiber_parameters(pulse_in, fiber, output_power)

        for i in range(n_steps):
            #print ("Step:", i, "Distance remaining:", fiber.length * (1 - np.float(i)/n_steps) )

            if reload_fiber_each_step:
                self.load_fiber_parameters(pulse_in,
                                           fiber,
                                           output_power,
                                           z=i * delta_z)

            self.integrate_over_dz(delta_z)
            AW[:, i] = self.conditional_ifftshift(self.FFT_t_2(self.A))
            AT[:, i] = self.conditional_ifftshift(self.A)
            pulse_out.set_AT(self.conditional_ifftshift(self.A))
            #print ("Pulse energy after:", \
            #  1e9 * pulse_out.calc_epp(), 'nJ' )
        pulse_out.set_AT(self.conditional_ifftshift(self.A))

        #print ( "Pulse energy after", fiber.fibertype,":", \
        #      1e9 * pulse_out.calc_epp(), 'nJ' )
        #        print "alpha out:",self.alpha
        self.cleanup()
        return z_positions, AW, AT, pulse_out
示例#17
0
roundtrip = 20

for i in range(roundtrip):
    print('正在运行第%s次循环,共%s循环' % (i + 1, roundtrip))
    Et_1.append(evol.propagate(Et_8[i], Fiber1, n_steps=Steps)[3])
    #    PulseTemp = Pulse()
    #    PulseTemp.clone_pulse(Et)
    #    PulseTemp.set_AT(Et_1[i])
    Et_2.append(evol.filter(Et_1[i], band, Fiber1))
    Et_3.append(evol.propagate(Et_2[i], Fiber2, n_steps=Steps)[3])
    Et_4.append(evol.propagate(Et_3[i], FiberYsfLo, n_steps=Steps)[3])
    Et_5.append(evol.propagate(Et_4[i], Fiber3, n_steps=Steps)[3])
    # NALM
    #clock
    Eclock0 = Pulse()
    Eclock0.clone_pulse(Et_5[i])
    Eclock0.set_AT(np.sqrt(CRatio) * Eclock0.AT)
    Eclock1 = evol.propagate(Eclock0, FiberSmf1, n_steps=Steps)[3]
    Eclock2 = evol.propagate(Eclock1, FiberYsfHi, n_steps=Steps)[3]
    Eclock3 = evol.propagate(Eclock2, FiberSmf2, n_steps=Steps)[3]
    #anclock
    Eanclock0 = Pulse()
    Eanclock0.clone_pulse(Et_5[i])
    Eanclock0.set_AT(1j * np.sqrt(1 - CRatio) * Eanclock0.AT)
    Eanclock1 = evol.propagate(Eanclock0, FiberSmf2, n_steps=Steps)[3]
    Eanclock2 = evol.propagate(Eanclock1, FiberYsfHi, n_steps=Steps)[3]
    Eanclock3 = evol.propagate(Eanclock2, FiberSmf1, n_steps=Steps)[3]

    E6 = Pulse()
    E6.clone_pulse(Et_5[i])