コード例 #1
0
    def fromDataFolder(folder, wantedSBs, keepErrors=False, negateNIR=True):
        """
        Create a fan compiler by passing the data path. Handles looping through the
        folder's sub-folders to find
        :param folder: The folder to search through. Alternatively, if it's a
        list/iterable, iterate through that instead. Useful if external code is
        directly removing sets of data.
        :return:
        """
        comp = FanCompiler(wantedSBs, keepErrors, negateNIR)
        # If it's a string, assume it's a single path that wants to be searached
        if isinstance(folder, str):
            wantFolders = hsg.natural_glob(folder, "*")
        else:
            # Otherwise, assume they've passed an iterable to search through
            wantFolders = folder

        for nirFolder in wantFolders:
            if "skip" in nirFolder.lower(): continue
            laserParams, rawData = hsg.hsg_combine_qwp_sweep(nirFolder,
                                                             save=False,
                                                             verbose=False,
                                                             loadNorm=False)

            _, fitDict = hsg.proc_n_fit_qwp_data(rawData,
                                                 laserParams,
                                                 vertAnaDir="VAna"
                                                 in nirFolder,
                                                 series=nirFolder)
            comp.addSet(fitDict)
        return comp
コード例 #2
0
def fan_generator(file,
                  observedSidebands,
                  crystalAngle,
                  saveFileName,
                  save_results=False,
                  Plot=True):
    '''
    This is a split off from fan_n_Tmat that just handles the fan. Apparently
    some of the fan creation stops scripts from running so to avoid that we're
    seperating the creation of the fan into this.

    :param file: String of folder name containing 4 polarimetry scans
    :param observedSidebands: np array of observed sidebands. Data will be
        cropped such that these sidebands are included in everything.
    :param crystalAngle: (Float) Angle of the sample from the 010 crystal face
    :saveFileName: Str of what you want to call the text files to be saved
    :save_results: Boolean controls if the fan diagram png is saved.

    Returns:
    :f: This is a fan object. I'm not really sure how to mess with these in
        greater depth.
    '''
    # Make a list of folders for the fan data
    datasets = hsg.natural_glob(file, "*")

    # FanCompiler class keeps alpha and gamma data together for different pols
    fanData = FanCompiler(observedSidebands)

    for data in datasets:
        laserParams, rawData = hsg.hsg_combine_qwp_sweep(data)
        _, fitDict = hsg.proc_n_fit_qwp_data(rawData,
                                             vertAnaDir=False,
                                             laserParams=laserParams,
                                             wantedSbs=observedSidebands)
        # Add the new alpha and gamma sets to the fan class
        fanData.addSet(fitDict)

    alphaData, gammaData, _ = fanData.build()

    from PyQt5 import QtWidgets
    app = QtWidgets.QApplication([])

    # interpolate so we have alpha and gamma for all excitation pols
    resampledAlpha, resampledGamma = jonesToFans(observedSidebands, J)

    # And create the fan
    f = FanDiagram(resampledAlpha, resampledGamma)
    # And show the fann
    if Plot:
        f.show()
        app.exec_()

    # ToDo: Add code for making the fans look nicer

    # You can save the fan with
    if save_results:
        f.export(saveFileName + "_fanDiagram.png")

    return f
コード例 #3
0
def J_T_proc(file,
             observedSidebands,
             crystalAngle,
             saveFileName,
             save_results=False,
             Plot=False):
    """
    This function will take a folder of polarimetry scans and produce
    DOP, alpha/gamma, J and T matrices, and Matrix Relations This is the same
    as fan_n_Tmat but doesn't create the fan itself. Otherwise creates pretty
    much everything one would need.

    :param file: String of folder name containing 4 polarimetry scans
    :param observedSidebands: np array of observed sidebands. Data will be
        cropped such that these sidebands are included in everything.
    :param crystalAngle: (Float) Angle of the sample from the 010 crystal face
    :saveFileName: Str of what you want to call the text files to be saved
    :save_results: Boolean controls if things are saved to txt files.
        Currently saves DOP, alpha, gamma, J matrix, T matrix, Fan, and Matrix
        Relations
    :Plot: Boolean controls if plots of matrix relations are displayed

    :return: DOP,alpha,gamma,J matrix, T matrix, Matrix Relations
    """

    # Make a list of folders for the fan data
    datasets = hsg.natural_glob(file, "*")

    # FanCompiler class keeps alpha and gamma data together for different pols
    fanData = FanCompiler(observedSidebands)

    # Initialize arrays for DOP
    dop00 = np.array([])
    dop45 = np.array([])
    dop90 = np.array([])
    dopn45 = np.array([])

    for data in datasets:
        laserParams, rawData = hsg.hsg_combine_qwp_sweep(data)
        try:
            _, fitDict = hsg.proc_n_fit_qwp_data(rawData,
                                                 vertAnaDir=False,
                                                 laserParams=laserParams,
                                                 wantedSbs=observedSidebands)
            # Add the new alpha and gamma sets to the fan class
        except IndexError:
            print('incorrect number of files in data folder ', data)
            print('proceeding without fourier analysis')
            _, fitDict = hsg.proc_n_fit_qwp_data(rawData,
                                                 vertAnaDir=False,
                                                 laserParams=laserParams,
                                                 wantedSbs=observedSidebands,
                                                 fourier=False)
        # Add the new alpha and gamma sets to the fan class
        fanData.addSet(fitDict)

        # Get Stoke Parameters
        s0 = fitDict['S0']
        s1 = fitDict['S1']
        s2 = fitDict['S2']
        s3 = fitDict['S3']

        # Trims the Stoke Parameters down to remove any sidebands beyond observedSidebands
        # This does mean that it won't calculate the DOP for any extra sidebands, even if
        # the software detected them.

        while s0[-1, 0] > observedSidebands[-1]:
            s0 = s0[:-1, :]
            s1 = s1[:-1, :]
            s2 = s2[:-1, :]
            s3 = s3[:-1, :]

        # This actually calculates the DOP and DOP error
        dop = s0
        dop[1:, 1] = np.sqrt((s1[1:, 1])**2 + (s2[1:, 1])**2 +
                             (s3[1:, 1])**2) / s0[1:, 1]
        dop[1:,
            2] = np.sqrt((s1[1:, 1]**2) * (s1[1:, 2]**2) / (s0[1:, 1]**2) /
                         ((s1[1:, 1])**2 + (s2[1:, 1])**2 + (s3[1:, 1])**2) +
                         (s2[1:, 1]**2) * (s2[1:, 2]**2) / (s0[1:, 1]**2) /
                         ((s1[1:, 1])**2 + (s2[1:, 1])**2 + (s3[1:, 1])**2) +
                         (s3[1:, 1]**2) * (s3[1:, 2]**2) / (s0[1:, 1]**2) /
                         ((s1[1:, 1])**2 + (s2[1:, 1])**2 +
                          (s3[1:, 1])**2)) + (
                              (s1[1:, 1])**2 + (s2[1:, 1])**2 +
                              (s3[1:, 1])**2) * s0[1:, 2]**2 / s0[1:, 1]**4

        # Save according to alpha. This will break if you use an alpha not in the usual
        #   0,45,90,-45 range.
        if laserParams['lAlpha'] == 00:
            dop00 = dop[1:, :]
        if laserParams['lAlpha'] == 45:
            dop45 = dop[1:, :]
        if laserParams['lAlpha'] == 90:
            dop90 = dop[1:, :]
        if laserParams['lAlpha'] == -45:
            dopn45 = dop[1:, :]

    # Put into appropriate form for saving
    #totdop = [dop00,dop45[:,1:],dop90[:,1:],dopn45[:,1:]]
    #totdop = np.hstack(totdop)

    # Saves as txt file with columns, SB Order, 00 DOP and error, 45 DOP and error,
    # 90 DOP and error, -45 DOP and error
    # if save_results:
    #     np.savetxt(saveFileName + "_DOP.txt", totdop, delimiter=',', header=
    #         'SB Order, 00 DOP, 00 DOP Error, 45 DOP, 45 DOP Error, 90 DOP, 90 DOP Error, -45 DOP, -45 DOP Error')

    # Building the fan compiler causes it to make  2D np arrays with the alpha and
    # gamma angles where each column is a different alpha_NIR excitation
    alphaData, gammaData, _ = fanData.build()

    # save the alpha and gamma results
    if save_results:
        fanData.buildAndSave(saveFileName + "_{}.txt")

    # Now we need to calculate the Jones matrices.
    J = findJ(alphaData, gammaData)

    # Get the T matrix:
    T = makeT(J, crystalAngle)

    # and save the matrices
    if save_results:
        saveT(J, observedSidebands, "{}_JMatrix.txt".format(saveFileName))
        saveT(T, observedSidebands, "{}_TMatrix.txt".format(saveFileName))

    # And to look at the ratios of the T matrix directly:
    if Plot:
        pg.figure("Magnitudes")
        pg.plot(observedSidebands,
                np.abs(T[0, 0, :] / T[1, 1, :]),
                'o-',
                label="T++/T--")
        pg.plot(observedSidebands,
                np.abs(T[0, 1, :] / T[1, 0, :]),
                'o-',
                label="T+-/T-+")

        pg.figure("Angles")
        pg.plot(observedSidebands,
                np.angle(T[0, 0, :] / T[1, 1, :], deg=True),
                'o-',
                label="T++/T--")
        pg.plot(observedSidebands,
                np.angle(T[0, 1, :] / T[1, 0, :], deg=True),
                'o-',
                label="T+-/T-+")

        pg.show()

    # Ok this is sort of a quick way to get what I want for Origin plotting
    # the relevant T matrix values
    #
    # ToDo: Format the text files to fit with the standards of other txt files

    tmag = np.transpose(
        np.array([
            observedSidebands,
            np.abs(T[0, 0, :] / T[1, 1, :]),
            np.abs(T[0, 1, :] / T[1, 0, :])
        ]))
    tang = np.transpose(
        np.array([
            observedSidebands,
            np.angle(T[0, 0, :] / T[1, 1, :], deg=True),
            np.angle(T[0, 1, :] / T[1, 0, :], deg=True)
        ]))

    if save_results:
        np.savetxt(saveFileName + "_{}.txt".format("TmatrixMag"),
                   tmag,
                   delimiter=',',
                   header='SB Order, |T++/T--|, |T+-/T-+|')
        np.savetxt(saveFileName + "_{}.txt".format("TmatrixAng"),
                   tang,
                   delimiter=',',
                   header='SB Order, Angle(T++/T--), Angle(T+-/T-+)')

    return alphaData, gammaData, J, T, tmag, tang