123456789101112131415161718192021222324252627282930313233343536373839404142434445464748495051525354555657585960616263646566676869707172737475767778798081828384858687888990919293949596979899100101102103104105106107108109110111112113114115116117118119120121122123124125126127128129130131132133134135136137138139140141142143144145146147148149150151152153154155156157158159160161162163164165166167168169170171172173174175176177178179180181182183184185186187188189190191192193194195196197198199200201202203204205206207208209210211212213214215216217218219220221222223224225226227228229230231232233234235236237238239240241242243244245246247248249250251252253254255256257258259260261262263264265266267268269270271272273274275276277278279280281282283284285286287288289290291292293294295296297298299300301302303304305306307308309310311312313314315316317318319320321322323324325326327328329330331332333334335336337338339340341342343344345346347348349350351352353354355356357358359360361362363364365366367368369370371372373374375376377378379380381382383384385386387388389390391392393394395396397398399400401402403404405406407408409410411412413414415416417418419420421422423424425426427428429430431432433434435436437438439440441442443444445446447448449450451452453454455456457458459460461462463464465466467468469470471472473474475476477478479480481482483484485486487488489490491492493494495496497498499500501502503504505506507508509510511512513514515516517518519520521522523524525526527528529530531532533534535536537538539540541542543544545546547548549550551552553554555556557558559560561562563564565566567568569570571572573574575576577578579580581582583584585586587588589590591592593594595596597598599600601602603604605606607608609610611612613614615616617618619620621622623624625626627628629630631632633634635636637638639640641642643644645646647648649650651652653654655656657658659660661662663664665666667668669670671672673674675676677678679680681682683684685686687688689690691692693694695696697698699700701702703704705706707708709710711712713714715716717718719720721722723724725726727728729730731732733734735736737738739740741742743744745746747748749750751752753754755756757758759760761762763764765766767768769770771772773774775776777778779780781782783784785786787788789790791792793794795796797798799800801802803804805806807808809810811812813814815816817818819820821822823824825826827828829830831832833834835836837838839840841842843844845846847848849850851852853854855856857858859860861862863864865866867868869870871872873874875876877878879880881882883884885886887888889890891892893894895896897898899900901902903904905906907908909910911912913914915916917918919920921922923924925926927928929930931932933934935936937938939940941942943944945946947948949950951952953954955956957958959960961962963964965966967968969970971972973974975976977978979980981982983984985986987988989990991992993994995996997998999100010011002100310041005100610071008100910101011101210131014101510161017101810191020102110221023102410251026102710281029103010311032103310341035103610371038103910401041104210431044104510461047104810491050105110521053105410551056105710581059106010611062106310641065106610671068106910701071107210731074107510761077107810791080108110821083108410851086108710881089109010911092109310941095109610971098109911001101110211031104110511061107110811091110111111121113111411151116111711181119112011211122112311241125112611271128112911301131113211331134113511361137113811391140114111421143114411451146114711481149115011511152115311541155115611571158115911601161116211631164116511661167116811691170117111721173117411751176117711781179118011811182118311841185118611871188118911901191119211931194119511961197119811991200120112021203120412051206120712081209121012111212121312141215121612171218121912201221122212231224122512261227122812291230123112321233123412351236123712381239124012411242124312441245124612471248124912501251125212531254125512561257125812591260126112621263126412651266126712681269127012711272127312741275127612771278127912801281128212831284128512861287128812891290129112921293129412951296129712981299130013011302130313041305130613071308130913101311131213131314131513161317131813191320132113221323132413251326132713281329133013311332133313341335133613371338133913401341134213431344134513461347134813491350135113521353135413551356135713581359136013611362136313641365136613671368136913701371137213731374137513761377137813791380138113821383138413851386138713881389139013911392139313941395139613971398139914001401140214031404140514061407140814091410141114121413141414151416141714181419142014211422142314241425142614271428142914301431143214331434143514361437143814391440144114421443144414451446144714481449145014511452145314541455145614571458145914601461146214631464146514661467146814691470147114721473147414751476147714781479148014811482148314841485148614871488148914901491149214931494149514961497149814991500150115021503150415051506150715081509151015111512151315141515151615171518151915201521152215231524152515261527152815291530153115321533153415351536153715381539154015411542154315441545154615471548154915501551155215531554155515561557155815591560156115621563156415651566156715681569157015711572157315741575157615771578157915801581158215831584158515861587158815891590159115921593159415951596159715981599160016011602160316041605160616071608160916101611161216131614161516161617161816191620162116221623162416251626162716281629163016311632163316341635163616371638163916401641164216431644164516461647164816491650165116521653165416551656165716581659166016611662166316641665166616671668166916701671167216731674167516761677167816791680168116821683168416851686168716881689169016911692169316941695169616971698169917001701170217031704170517061707170817091710171117121713171417151716171717181719172017211722172317241725172617271728172917301731173217331734173517361737173817391740174117421743174417451746174717481749175017511752175317541755175617571758175917601761176217631764176517661767176817691770177117721773177417751776177717781779178017811782178317841785178617871788178917901791179217931794179517961797179817991800180118021803180418051806180718081809181018111812181318141815181618171818181918201821182218231824182518261827182818291830183118321833183418351836183718381839184018411842184318441845184618471848184918501851185218531854185518561857185818591860186118621863186418651866186718681869187018711872187318741875187618771878187918801881188218831884188518861887188818891890189118921893189418951896189718981899190019011902190319041905190619071908190919101911191219131914191519161917191819191920192119221923192419251926192719281929193019311932193319341935193619371938193919401941194219431944194519461947194819491950195119521953195419551956195719581959196019611962196319641965196619671968196919701971197219731974197519761977197819791980198119821983198419851986198719881989199019911992199319941995199619971998199920002001200220032004200520062007200820092010201120122013201420152016201720182019202020212022202320242025202620272028202920302031203220332034203520362037203820392040204120422043204420452046204720482049205020512052205320542055205620572058205920602061206220632064206520662067206820692070207120722073207420752076207720782079208020812082208320842085208620872088208920902091209220932094209520962097209820992100210121022103210421052106210721082109211021112112211321142115211621172118211921202121212221232124212521262127212821292130213121322133213421352136213721382139214021412142214321442145214621472148214921502151215221532154215521562157215821592160216121622163216421652166216721682169217021712172217321742175217621772178217921802181218221832184218521862187218821892190219121922193219421952196219721982199220022012202220322042205220622072208220922102211221222132214221522162217221822192220222122222223222422252226222722282229223022312232223322342235223622372238223922402241224222432244224522462247224822492250225122522253225422552256225722582259226022612262226322642265226622672268226922702271227222732274227522762277227822792280228122822283228422852286228722882289229022912292229322942295229622972298229923002301230223032304230523062307230823092310231123122313231423152316231723182319232023212322232323242325232623272328232923302331233223332334233523362337233823392340234123422343234423452346234723482349235023512352235323542355235623572358235923602361236223632364236523662367236823692370237123722373237423752376237723782379238023812382238323842385238623872388238923902391239223932394239523962397239823992400240124022403240424052406240724082409241024112412241324142415241624172418241924202421242224232424242524262427242824292430243124322433243424352436243724382439244024412442244324442445244624472448244924502451245224532454245524562457245824592460246124622463246424652466246724682469247024712472247324742475247624772478247924802481248224832484248524862487248824892490249124922493249424952496249724982499250025012502250325042505250625072508250925102511251225132514251525162517251825192520252125222523252425252526252725282529253025312532253325342535253625372538253925402541254225432544254525462547254825492550255125522553255425552556255725582559256025612562256325642565256625672568256925702571257225732574257525762577257825792580258125822583258425852586258725882589259025912592259325942595259625972598259926002601260226032604260526062607260826092610261126122613261426152616261726182619262026212622262326242625262626272628262926302631263226332634263526362637263826392640264126422643264426452646264726482649265026512652265326542655265626572658265926602661266226632664266526662667266826692670267126722673267426752676267726782679268026812682268326842685268626872688268926902691269226932694269526962697269826992700270127022703270427052706270727082709271027112712271327142715271627172718271927202721272227232724272527262727272827292730273127322733273427352736273727382739274027412742274327442745274627472748274927502751275227532754275527562757275827592760276127622763276427652766 |
- from PyQt5.QtCore import *
- import numpy as np
- import scipy.signal as signal
- import pylab
- import sys
- import scipy
- import copy
- import struct
- from scipy.io.matlab import mio
- from numpy import pi
- from math import floor
- import matplotlib as mpl
- from matplotlib.ticker import FuncFormatter
- import matplotlib.font_manager as fm
- import matplotlib.pyplot as plt
- import matplotlib.ticker
- from matplotlib.ticker import MaxNLocator
-
- import multiprocessing
- import itertools
-
- import akvo.tressel.adapt as adapt
- #import akvo.tressel.cadapt as adapt # cython for more faster
- import akvo.tressel.decay as decay
- import akvo.tressel.pca as pca
- import akvo.tressel.rotate as rotate
- import akvo.tressel.cmaps as cmaps
- import akvo.tressel.harmonic as harmonic
-
- import cmocean # colormaps for geophysical data
- plt.register_cmap(name='viridis', cmap=cmaps.viridis)
- plt.register_cmap(name='inferno', cmap=cmaps.inferno)
- plt.register_cmap(name='inferno_r', cmap=cmaps.inferno_r)
-
- plt.register_cmap(name='magma', cmap=cmaps.magma)
- plt.register_cmap(name='magma_r', cmap=cmaps.magma_r)
-
-
- def xxloadGMRBinaryFID( rawfname, info ):
- """ Reads a single binary GMR file and fills into DATADICT
- """
-
- #################################################################################
- # figure out key data indices
- # Pulse
- nps = (int)((info["prePulseDelay"])*info["samp"])
- npul = (int)(self.pulseLength[0]*self.samp) #+ 100
-
- # Data
- nds = nps+npul+(int)((self.deadTime)*self.samp); # indice pulse 1 data starts
- nd1 = (int)(1.*self.samp) # samples in first pulse
-
- invGain = 1./self.RxGain
- invCGain = self.CurrentGain
-
- pulse = "Pulse 1"
- chan = self.DATADICT[pulse]["chan"]
- rchan = self.DATADICT[pulse]["rchan"]
-
- rawFile = open( rawfname, 'rb')
-
- T = N_samp * self.dt
- TIMES = np.arange(0, T, self.dt) - .0002 # small offset in GMR DAQ?
-
- for ipm in range(self.nPulseMoments):
- buf1 = rawFile.read(4)
- buf2 = rawFile.read(4)
-
- N_chan = struct.unpack('>i', buf1 )[0]
- N_samp = struct.unpack('>i', buf2 )[0]
-
- DATA = np.zeros([N_samp, N_chan+1])
- for ichan in range(N_chan):
- DATADUMP = rawFile.read(4*N_samp)
- for irec in range(N_samp):
- DATA[irec,ichan] = struct.unpack('>f', DATADUMP[irec*4:irec*4+4])[0]
-
- return DATA, TIMES
-
- class SNMRDataProcessor(QObject):
- """ Revised class for preprocessing sNMR Data.
- Derived types can read GMR files
- """
- def __init__(self):
- QObject.__init__(self)
- self.numberOfMoments = 0
- self.numberOfPulsesPerMoment = 0
- self.pulseType = "NONE"
- self.transFreq = 0
- self.pulseLength = np.zeros(1)
- self.nPulseMoments = 0
- self.dt = 0
-
- def mfreqz(self, b,a=1):
- """ Plots the frequency response of a filter specified with a and b weights
- """
- import scipy.signal as signal
- pylab.figure(124)
- w,h = signal.freqz(b,a)
- w /= max(w)
- w *= .5/self.dt
- h_dB = 20 * pylab.log10 (abs(h))
- pylab.subplot(211)
- #pylab.plot(w/max(w),h_dB)
- pylab.plot(w,h_dB)
- pylab.ylim(-150, 5)
- pylab.ylabel('Magnitude (dB)')
- #pylab.xlabel(r'Normalized Frequency (x$\pi$rad/sample)')
- pylab.xlabel(r'Hz')
- pylab.title(r'Frequency response')
- pylab.subplot(212)
- h_Phase = pylab.unwrap(pylab.arctan2(pylab.imag(h), pylab.real(h)))
- #pylab.plot(w/max(w),h_Phase)
- pylab.plot(w,h_Phase)
- pylab.ylabel('Phase (radians)')
- pylab.xlabel(r'Hz')
- #pylab.xlabel(r'Normalized Frequency (x$\pi$rad/sample)')
- pylab.title(r'Phase response')
- pylab.subplots_adjust(hspace=0.5)
-
- def mfreqz2(self, b, a, canvas):
- "for analysing filt-filt"
- import scipy.signal as signal
- canvas.reAx2(False,False)
-
- canvas.ax1.tick_params(axis='both', which='major', labelsize=8)
- canvas.ax2.tick_params(axis='both', which='major', labelsize=8)
- #canvas.ax2.tick_params(axis='both', which='minor', labelsize=6)
-
- #pylab.figure(124)
- w,h = signal.freqz(b,a)
- w /= max(w)
- w *= .5/self.dt
- h_dB = 20 * pylab.log10(abs(h*h) + 1e-16)
- #ab.subplot(211)
- #pylab.plot(w/max(w),h_dB)
- canvas.ax1.plot(w,h_dB)
- canvas.ax1.set_ylim(-150, 5)
- canvas.ax1.set_ylabel('Magnitude [db]', fontsize=8)
- #pylab.xlabel(r'Normalized Frequency (x$\pi$rad/sample)')
- canvas.ax1.set_xlabel(r'[Hz]', fontsize=8)
- canvas.ax1.set_title(r'Frequency response', fontsize=8)
- canvas.ax1.grid(True)
-
- tt = np.arange(0, .02, self.dt)
- impulse = signal.dimpulse((self.filt_z, self.filt_p, self.filt_k, self.dt), t=tt)
- #impulse = signal.dstep((self.filt_z, self.filt_p, self.filt_k, self.dt), t=tt)
- #print impulse
- #for ii in range(len(impulse[1])):
- impulse_dB = 20.*np.log10(np.abs(np.array(impulse[1][0])))
- #canvas.ax2.plot(np.array(impulse[0]), impulse_dB)
- canvas.ax2.plot(np.array(impulse[0]), impulse[1][0])
- #h_Phase = pylab.unwrap(pylab.arctan2(pylab.imag(h), pylab.real(h)))
- #canvas.ax2.plot(w,h_Phase)
- canvas.ax2.set_ylabel('response [%]', fontsize=8)
- canvas.ax2.set_xlabel(r'time [s]', fontsize=8)
- canvas.ax2.set_title(r'impulse response', fontsize=8)
- #canvas.ax2.grid(True)
- canvas.draw()
- # search for last
- return impulse #[np.where(impulse[1][0] > .01)[-1]]
-
-
- class GMRDataProcessor(SNMRDataProcessor):
-
- # slots
- progressTrigger = pyqtSignal("int")
- doneTrigger = pyqtSignal()
- enableDSPTrigger = pyqtSignal()
- updateProcTrigger = pyqtSignal()
-
- def __init__(self):
-
- SNMRDataProcessor.__init__(self)
- self.maxBusV = 0.
- self.samp = 50000. # sampling frequency
- self.dt = 2e-5 # sampling rate
- self.deadTime = .0055 # instrument dead time before measurement
- self.prePulseDelay = 0.05 # delay before pulse
- self.windead = 0. # FD window filter dead time
- self.pulseType = -1
- self.transFreq = -1
- self.maxBusV = -1
- self.pulseLength = -1
- self.interpulseDelay = -1 # for T2, Spin Echo
- self.repetitionDelay = -1 # delay between first pulse
- self.nPulseMoments = -1 # Number of pulse moments per stack
- self.TuneCapacitance = -1 # tuning capac in uF
- self.nTransVersion = -1 # Transmitter version
- self.nDAQVersion = -1 # DAQ software version
- self.nInterleaves = -1 # num interleaves
- # self.nReceiveChannels = 4 # Num receive channels
-
- self.RotatedAmplitude = False
- # self.DATA = np.zeros(1) # Numpy array to hold all data, dimensions resized based on experiment
- # self.PULSES = np.zeros(1) # Numpy array to hold all data, dimensions resized based on experiment
-
- def Print(self):
- print ("pulse type", self.pulseType)
- print ("maxBusV", self.maxBusV)
- print ("inner pulse delay", self.interpulseDelay)
- print ("tuning capacitance", self.TuneCapacitance)
- print ("sampling rate", self.samp)
- print ("dt", self.dt)
- print ("dead time", self.deadTime)
- print ("pre pulse delay", self.prePulseDelay)
- print ("number of pulse moments", self.nPulseMoments)
- print ("pulse Length", self.pulseLength)
- print ("trans freq", self.transFreq)
-
- def readHeaderFile(self, FileName):
-
- HEADER = np.loadtxt(FileName)
-
- pulseTypeDict = {
- 1 : lambda: "FID",
- 2 : lambda: "T1",
- 3 : lambda: "SPINECHO",
- 4 : lambda: "4PhaseT1"
- }
-
- pulseLengthDict = {
- 1 : lambda x: np.ones(1) * x,
- 2 : lambda x: np.ones(2) * x,
- 3 : lambda x: np.array([x, 2.*x]),
- 4 : lambda x: np.ones(2) * x
- }
-
- self.pulseType = pulseTypeDict.get((int)(HEADER[0]))()
- self.transFreq = HEADER[1]
- self.maxBusV = HEADER[2]
- self.pulseLength = pulseLengthDict.get((int)(HEADER[0]))(1e-3*HEADER[3])
- self.interpulseDelay = 1e-3*HEADER[4] # for T2, Spin Echo
- self.repetitionDelay = HEADER[5] # delay between first pulse
- self.nPulseMoments = (int)(HEADER[6]) # Number of pulse moments per stack
- self.TuneCapacitance = HEADER[7] # tuning capacitance in uF
- self.nTransVersion = HEADER[8] # Transmitter version
- self.nDAQVersion = HEADER[9] # DAQ software version
- self.nInterleaves = HEADER[10] # num interleaves
-
- self.gain()
-
- # default
- self.samp = 50000. # sampling frequency
- self.dt = 2e-5 # sampling rate
-
- # newer header files contain 64 entries
- if self.nDAQVersion >= 2:
- #self.deadtime = HEADER[11]
- #self.unknown = HEADER[12]
- #self.PreAmpGain = HEADER[13]
- self.samp = HEADER[14] # sampling frequency
- self.dt = 1./self.samp # sampling rate
- self.deadTime = .0055 # instrument dead time before measurement
- self.prePulseDelay = 0.05 # delay before pulse
- #exit()
-
- def gain(self):
-
- #######################################################
- # Circuit gain
- # From MRSMatlab
- w = 2*np.pi*self.transFreq
- # 1e6 due to uF of reported capacitance
- L_coil = 1e6/(self.TuneCapacitance*(w**2))
- R_coil = 1.
- Z1_in = .5 + 1j*.5*w
- Z2_in = 1./(1j*w*.000001616)
- Z_eq_inv = (1./Z1_in) + (1./Z2_in)
- Zeq = 1./Z_eq_inv
- Zsource = R_coil + 1j*w*L_coil
- voltage_in = Zeq / (Zsource + Zeq)
- self.circuitGain = np.abs(voltage_in)
- self.circuitPhase_deg = (180/np.pi)+np.angle(voltage_in)
- circuitImpedance_ohms = np.abs(Zsource + Zeq)
-
- ######################################################
- # PreAmp gain
- if self.nTransVersion == 4:
- self.PreAmpGain = 1000.
- elif self.nTransVersion == 1 or self.nTransVersion == 2 or self.nTransVersion == 3 or self.nTransVersion == 6:
- self.PreAmpGain = 500.
- else:
- print ("unsupported transmitter version")
- exit(1)
-
- # Total Receiver Gain
- self.RxGain = self.circuitGain * self.PreAmpGain
-
- #####################################################
- # Current gain
- if floor(self.nDAQVersion) == 1:
- self.CurrentGain = 150.
- elif floor(self.nDAQVersion) == 2:
- self.CurrentGain = 180.
-
- def updateProgress(self):
- pass
-
- def TDSmartStack(self, outlierTest, MADcutoff, canvas):
- #print("Line 300 in mrsurvey")
- Stack = {}
- # align for stacking and modulate
- for pulse in self.DATADICT["PULSES"]:
- stack = np.zeros(( len(self.DATADICT[pulse]["chan"]), self.DATADICT["nPulseMoments"],\
- len(self.DATADICT["stacks"]), len(self.DATADICT[pulse]["TIMES"]) ))
- for ipm in range(self.DATADICT["nPulseMoments"]):
- istack = 0
- for sstack in self.DATADICT["stacks"]:
- if self.pulseType == "FID" or pulse == "Pulse 2":
- if floor(self.nDAQVersion) < 2:
- mod = 1
- else:
- mod = (-1.)**(ipm%2) * (-1.)**(sstack%2)
- elif self.pulseType == "T1":
- #mod = (-1.)**(sstack%2)
- #mod = (-1)**(ipm%2) * (-1)**(sstack%2)
- #mod = (-1)**(ipm%2) * (-1.**(((sstack-1)/2)%2))
- #print("mod", mod, ipm, sstack, (-1.)**(ipm%2), -1.0**(((sstack-1)/2)%2 ))
- #mod = (-1.)**((ipm+1)%2) * (-1.**(((sstack)/2)%2))
- #mod = (-1.)**((ipm-1)%2) * (-1.)**((sstack-1)%2)
- #mod = 1 # (-1.**(((sstack-1)/2)%2))
-
- # These two give great noise estimate
- #qcycler = np.array([1,-1,-1,1])
- #scycler = np.array([1,-1,1,-1])
-
- qcycler = np.array([ 1, 1])
- scycler = np.array([ 1, 1])
- mod = qcycler.take([ipm], mode='wrap')*scycler.take([sstack], mode='wrap')
- #mod = (-1.)**(ipm%2) * (-1.)**(sstack%2)
- elif self.pulseType == "4PhaseT1":
- mod = (-1.)**(ipm%2) * (-1.**(((sstack-1)/2)%2))
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
- stack[ichan,ipm,istack,:] += mod*self.DATADICT[pulse][chan][ipm][sstack]
- ichan += 1
- istack += 1
- Stack[pulse] = stack
-
- #########################################
- # simple stack and plot of simple stack #
- #########################################
- canvas.reAxH2(np.shape(stack)[0], False, False)
- axes = canvas.fig.axes
- SimpleStack = {}
- VarStack = {}
- for pulse in self.DATADICT["PULSES"]:
- SimpleStack[pulse] = {}
- VarStack[pulse] = {}
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
- SimpleStack[pulse][chan] = 1e9*np.average( Stack[pulse][ichan], 1 )
- VarStack[pulse][chan] = 1e9*np.std( Stack[pulse][ichan], 1 )
- ax1 = axes[ 2*ichan ]
- #ax1.get_yaxis().get_major_formatter().set_useOffset(False)
-
- y_formatter = matplotlib.ticker.ScalarFormatter(useOffset=False)
- ax1.yaxis.set_major_formatter(y_formatter)
-
- ax1.plot( 1e3*self.DATADICT[pulse]["TIMES"], np.average( SimpleStack[pulse][chan], 0 )) #, color='darkblue' )
- ax1.set_title("Ch." + str(chan) + ": avg FID", fontsize=8)
- ax1.set_xlabel(r"time (ms)", fontsize=8)
-
- if ichan == 0:
- ax1.set_ylabel(r"signal [nV]", fontsize=8)
- else:
- plt.setp(ax1.get_yticklabels(), visible=False)
- plt.setp(ax1.get_yaxis().get_offset_text(), visible=False)
- # if ichan == 1:
- # canvas.ax2.plot( 1e3*self.DATADICT[pulse]["TIMES"], np.average( SimpleStack[pulse][chan], 0 ), color='darkblue' )
- # canvas.ax2.set_title("Ch." + str(chan) + ": total average FID", fontsize=8)
- # canvas.ax2.set_xlabel(r"time [ms]", fontsize=8)
- # if ichan == 2:
- # canvas.ax3.plot( 1e3*self.DATADICT[pulse]["TIMES"], np.average( SimpleStack[pulse][chan], 0 ), color='darkblue' )
- # canvas.ax3.set_title("Ch." + str(chan) + ": total average FID", fontsize=8)
- # canvas.ax3.set_xlabel(r"time [ms]", fontsize=8)
- # if ichan == 3:
- # canvas.ax4.plot( 1e3*self.DATADICT[pulse]["TIMES"], np.average( SimpleStack[pulse][chan], 0 ), color='darkblue' )
- # canvas.ax4.set_title("Ch." + str(chan) + ": total average FID", fontsize=8)
- # canvas.ax4.set_xlabel(r"time [ms]", fontsize=8)
- ichan += 1
-
- #########################
- # Oulier rejectig stack #
- #########################
- if outlierTest == "MAD":
- MADStack = {}
- VarStack = {}
- #1.4826 is assumption of gaussian noise
- madstack = np.zeros(( len(self.DATADICT[pulse]["chan"]),\
- self.DATADICT["nPulseMoments"], len(self.DATADICT[pulse]["TIMES"]) ))
- varstack = np.zeros(( len(self.DATADICT[pulse]["chan"]),\
- self.DATADICT["nPulseMoments"], len(self.DATADICT[pulse]["TIMES"]) ))
- for pulse in self.DATADICT["PULSES"]:
- MADStack[pulse] = {}
- VarStack[pulse] = {}
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
- ax1 = axes[ 2*ichan ]
- for ipm in range(self.DATADICT["nPulseMoments"]):
- # # brutal loop over time, can this be vectorized?
- # for it in range(len(self.DATADICT[pulse]["TIMES"])):
- # x = 1e9 *Stack[pulse][ichan,ipm,:,it]
- # MAD = 1.4826 * np.median( np.abs(x-np.median(x)) )
- # good = 0
- # for istack in self.DATADICT["stacks"]:
- # if (np.abs(x[istack-1]-np.median(x))) / MAD < 2:
- # good += 1
- # madstack[ ichan, ipm, it ] += x[istack-1]
- # else:
- # pass
- # madstack[ichan, ipm, it] /= good
- # percent = int(1e2* (float)(ipm) / (float)(self.DATADICT["nPulseMoments"]) )
- # self.progressTrigger.emit(percent)
-
- # Vectorized version of above...much, much faster
- x = 1e9*copy.deepcopy(Stack[pulse][ichan][ipm,:,:]) # stack and time indices
- tile_med = np.tile( np.median(x, axis=0), (np.shape(x)[0],1))
- MAD = MADcutoff * np.median(np.abs(x - tile_med), axis=0)
- tile_MAD = np.tile( MAD, (np.shape(x)[0],1))
- good = np.abs(x-tile_med)/tile_MAD < 2. # 1.4826 # 2
-
- madstack[ichan][ipm] = copy.deepcopy( np.ma.masked_array(x, good != True).mean(axis=0) )
- varstack[ichan][ipm] = copy.deepcopy( np.ma.masked_array(x, good != True).std(axis=0) )
-
- # reporting
- percent = int(1e2* (float)((ipm)+ichan*self.DATADICT["nPulseMoments"]) /
- (float)(self.DATADICT["nPulseMoments"] * len(self.DATADICT[pulse]["chan"])))
- self.progressTrigger.emit(percent)
-
- ax1.plot( 1e3*self.DATADICT[pulse]["TIMES"], np.average( madstack[ichan], 0 ))# , color='darkred')
-
- MADStack[pulse][chan] = madstack[ichan]
- VarStack[pulse][chan] = varstack[ichan]
- ichan += 1
-
- self.DATADICT["stack"] = MADStack
-
- else:
- self.DATADICT["stack"] = SimpleStack
-
- #########################################
- # Plot Fourier Transform representation #
- #########################################
-
- # canvas.fig.subplots_adjust(right=0.8)
- # cbar_ax = canvas.fig.add_axes([0.85, 0.1, 0.015, 0.355])
- # cbar_ax.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
- im2 = []
- im1 = []
- for pulse in self.DATADICT["PULSES"]:
- ichan = 0
- axes = canvas.fig.axes
- vvmin = 1e10
- vvmax = 0
- for chan in self.DATADICT[pulse]["chan"]:
- ax1 = axes[2*ichan ]
- ax2 = axes[2*ichan+1] # TODO fix hard coded number
- if outlierTest == "MAD":
- X = np.fft.rfft( MADStack[pulse][chan][0,:] )
- nu = np.fft.fftfreq(len( MADStack[pulse][chan][0,:]), d=self.dt)
- else:
- X = np.fft.rfft( SimpleStack[pulse][chan][0,:] )
- nu = np.fft.fftfreq(len( SimpleStack[pulse][chan][0,:]), d=self.dt)
-
- nu = nu[0:len(X)]
- nu[-1] = np.abs(nu[-1])
- df = nu[1] - nu[0]
- of = 0
-
- istart = int((self.transFreq-50.)/df)
- iend = int((self.transFreq+50.)/df)
- of = nu[istart]
-
- def freqlabel(xxx, pos):
- return '%1.0f' %(of + xxx*df)
- formatter = FuncFormatter(freqlabel)
-
- SFFT = np.zeros( (self.DATADICT["nPulseMoments"], len(X)), dtype=np.complex64 )
- SFFT[0,:] = X
- for ipm in range(1, self.DATADICT["nPulseMoments"]):
- if outlierTest == "MAD":
- SFFT[ipm,:] = np.fft.rfft( MADStack[pulse][chan][ipm,:] )
- else:
- SFFT[ipm,:] = np.fft.rfft( SimpleStack[pulse][chan][ipm,:] )
-
- # convert to dB and add colorbars
- #db = 20.*np.log10(np.abs(SFFT[:,istart:iend]))
- db = (np.abs(SFFT[:,istart:iend]))
- #db = (np.real(SFFT[:,istart:iend]))
- #dbr = (np.real(SFFT[:,istart:iend]))
- #db = (np.imag(SFFT[:,istart:iend]))
-
- vvmin = min(vvmin, np.min(db) + 1e-16 )
- vvmax = max(vvmax, np.max(db) + 1e-16 )
- im2.append(ax2.matshow( db, aspect='auto', cmap=cmocean.cm.ice, vmin=vvmin, vmax=vvmax))
- #im1.append(ax1.matshow( dbr, aspect='auto')) #, vmin=vvmin, vmax=vvmax))
- #im2.append(ax2.matshow( db, aspect='auto', vmin=vvmin, vmax=vvmax))
- #im2 = ax2.matshow( db, aspect='auto', cmap=cmocean.cm.ice, vmin=vvmin, vmax=vvmax)
- if ichan == 0:
- ax2.set_ylabel(r"$q$ (A $\cdot$ s)", fontsize=8)
- else:
- #ax2.yaxis.set_ticklabels([])
- plt.setp(ax2.get_yticklabels(), visible=False)
-
- ax2.xaxis.set_major_formatter(formatter)
- ax2.xaxis.set_ticks_position('bottom')
- ax2.xaxis.set_major_locator(MaxNLocator(3))
-
- y_formatter = matplotlib.ticker.ScalarFormatter(useOffset=False)
- ax2.yaxis.set_major_formatter(y_formatter)
-
-
- #if chan == self.DATADICT[pulse]["chan"][-1]:
- #cb2 = canvas.fig.colorbar(im2, cax=cbar_ax, format='%1.0e')
-
- #cb2 = canvas.fig.colorbar(im2[0], ax=ax2, format='%1.0e', orientation='horizontal')
- #cb2 = canvas.fig.colorbar(im2, ax=ax2, format='%1.0e', orientation='horizontal')
- #cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- #cb2.set_label("signal (dB)", fontsize=8)
-
- ichan += 1
-
-
- canvas.fig.subplots_adjust(hspace=.1, wspace=.05, left=.075, right=.95 )#left=None, bottom=None, right=None, top=None, wspace=None, hspace=None)
-
- #cb1 = canvas.fig.colorbar(im, ax=axes[0::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30)
- #cb1.ax.tick_params(axis='both', which='major', labelsize=8)
- #cb1.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
-
- cb2 = canvas.fig.colorbar(im2[-1], ax=axes[1::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30)
- cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- cb2.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
-
- #canvas.fig.tight_layout()
- canvas.draw()
- self.doneTrigger.emit()
-
- #def harmonicModel(self, nF, nK, f0, f1, plot, canvas):
-
- def harmonicModel(self, nF, \
- f0, f0K1, f0KN, f0Ks, f0ns, \
- f1, f1K1, f1KN, f1Ks, \
- plot, canvas):
- """ nF = number of base frequencies, must be 1 or 2
- f0 = first base frequency
- f0K1 = first harmonic to model for first base frequency
- f0KN = last harmonic to model for the first base frequency
- f0Ks = subharmonic spacing, set to 1 for no subharmonics.
- f0Ns = number of segments for f0
- f1 = second base frequency
- f1K1 = first harmonic to model for second base frequency
- f1KN = last harmonic to model for the second base frequency
- f1Ks = subharmonic spacing for the second base frequency, set to 1 for no subharmonics.
- plot = should Akvo plot the results
- canvas = mpl plotting axis
- """
- if plot:
- canvas.reAx2()
- canvas.ax1.set_ylabel(r"signal [nV]", fontsize=8)
- canvas.ax2.set_xlabel(r"time [s]", fontsize=8)
- canvas.ax2.set_ylabel(r"signal [nV]", fontsize=8)
-
- # Data
- iFID = 0
-
- # stores previous f0 as starting point in non-linear search
- f0p = {}
- f1p = {}
- for pulse in self.DATADICT["PULSES"]:
- for rchan in self.DATADICT[pulse]["rchan"]:
- f0p[rchan] = f0
- f1p[rchan] = f1+1e-1
- for chan in self.DATADICT[pulse]["chan"]:
- f0p[chan] = f0
- f1p[chan] = f1+1e-1
-
- for pulse in self.DATADICT["PULSES"]:
- Nseg = int( np.floor(len( self.DATADICT[pulse]["TIMES"] ) / f0ns) )
- for istack in self.DATADICT["stacks"]:
- for ipm in range(self.DATADICT["nPulseMoments"]):
- if plot:
- canvas.softClear()
- mmax = 0
- for ichan in self.DATADICT[pulse]["rchan"]:
- canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack], alpha=.5)
- mmax = max( mmax, np.max(1e9*self.DATADICT[pulse][ichan][ipm][istack]))
- for ichan in self.DATADICT[pulse]["chan"]:
- canvas.ax2.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack], alpha=.5)
- mmax = max( mmax, np.max(1e9*self.DATADICT[pulse][ichan][ipm][istack]))
- canvas.ax1.set_prop_cycle(None)
- canvas.ax2.set_prop_cycle(None)
- canvas.ax1.set_ylim(-mmax, mmax)
- for ichan in self.DATADICT[pulse]["rchan"]:
- if nF == 1:
- for iseg in range(f0ns):
- if iseg < f0ns-1:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg], f0p[ichan] = \
- harmonic.minHarmonic( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg], \
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg:(iseg+1)*Nseg], \
- f0p[ichan], f0K1, f0KN, f0Ks )
- else:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::], f0p[ichan] = \
- harmonic.minHarmonic( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::], \
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg::], \
- f0p[ichan], f0K1, f0KN, f0Ks )
- elif nF == 2:
- for iseg in range(f0ns):
- if iseg < f0ns-1:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg], f0p[ichan], f1p[ichan] = \
- harmonic.minHarmonic2( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg],\
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg:(iseg+1)*Nseg], \
- f0p[ichan], f0K1, f0KN, f0Ks, \
- f1p[ichan], f1K1, f1KN, f1Ks )
- else:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::], f0p[ichan], f1p[ichan] = \
- harmonic.minHarmonic2( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::],\
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg::], \
- f0p[ichan], f0K1, f0KN, f0Ks, \
- f1p[ichan], f1K1, f1KN, f1Ks )
- # plot
- if plot:
- canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack], \
- label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " rchan=" + str(ichan))
-
- for ichan in self.DATADICT[pulse]["chan"]:
-
- if nF == 1:
- for iseg in range(f0ns):
- if iseg < f0ns-1:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg], f0p[ichan] = \
- harmonic.minHarmonic( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg],
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg:(iseg+1)*Nseg], \
- f0p[ichan], f0K1, f0KN, f0Ks )
- else:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::], f0p[ichan] = \
- harmonic.minHarmonic( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::],
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg::], \
- f0p[ichan], f0K1, f0KN, f0Ks )
-
- elif nF == 2:
- for iseg in range(f0ns):
- if iseg < f0ns-1:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg], f0p[ichan], f1p[ichan] = \
- harmonic.minHarmonic2( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg:(iseg+1)*Nseg],\
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg:(iseg+1)*Nseg], \
- f0p[ichan], f0K1, f0KN, f0Ks, \
- f1p[ichan], f1K1, f1KN, f1Ks )
- else:
- self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::], f0p[ichan], f1p[ichan] = \
- harmonic.minHarmonic2( self.DATADICT[pulse][ichan][ipm][istack][iseg*Nseg::],\
- self.samp, self.DATADICT[pulse]["TIMES"][iseg*Nseg::], \
- f0p[ichan], f0K1, f0KN, f0Ks, \
- f1p[ichan], f1K1, f1KN, f1Ks )
-
- # plot
- if plot:
- canvas.ax2.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack], \
- label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " chan=" + str(ichan))
-
- if plot:
- canvas.ax1.legend(prop={'size':6}, loc='upper right')
- canvas.ax2.legend(prop={'size':6}, loc='upper right')
- canvas.draw()
-
- percent = (int)(1e2*((ipm+istack*self.nPulseMoments)/(self.nPulseMoments*len(self.DATADICT["stacks"]))))
- self.progressTrigger.emit(percent)
- iFID += 1
-
- self.doneTrigger.emit()
- self.updateProcTrigger.emit()
- self.doneTrigger.emit()
-
- def FDSmartStack(self, outlierTest, MADcutoff, canvas):
-
- print("FFT stuff")
- self.dataCubeFFT()
-
- Stack = {}
- # align phase cycling for stacking and modulate
- for pulse in self.DATADICT["PULSES"]:
- stack = np.zeros(( len(self.DATADICT[pulse]["chan"]), \
- self.DATADICT["nPulseMoments"],\
- len(self.DATADICT["stacks"]),\
- len(self.DATADICT[pulse][self.DATADICT[pulse]["chan"][0] ]["FFT"]["nu"])//2 + 1),\
- dtype=np.complex )
- for ipm in range(self.DATADICT["nPulseMoments"]):
- istack = 0
- for sstack in self.DATADICT["stacks"]:
- if self.pulseType == "FID" or pulse == "Pulse 2":
- mod = (-1)**(ipm%2) * (-1)**(sstack%2)
- elif self.pulseType == "4PhaseT1":
- mod = (-1)**(ipm%2) * (-1)**(((sstack-1)/2)%2)
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
- #stack[ichan,ipm,istack,:] += mod*self.DATADICT[pulse][chan][ipm][sstack]
- stack[ichan,ipm,istack,:] += mod*self.DATADICT[pulse][chan]["FFT"][sstack][ipm,:]
- ichan += 1
- istack += 1
- Stack[pulse] = stack
-
- #########################################
- # simple stack and plot of simple stack #
- ########################################https://faculty.apps.utah.edu/#
- canvas.reAxH2(np.shape(stack)[0], False, False)
- axes = canvas.fig.axes
- SimpleStack = {}
- VarStack = {}
- for pulse in self.DATADICT["PULSES"]:
- SimpleStack[pulse] = {}
- VarStack[pulse] = {}
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
- SimpleStack[pulse][chan] = 1e9*np.average( Stack[pulse][ichan], 1 )
- VarStack[pulse][chan] = 1e9*np.std( Stack[pulse][ichan], 1 )
- ax1 = axes[ 2*ichan ]
- #ax1.get_yaxis().get_major_formatter().set_useOffset(False)
-
- y_formatter = matplotlib.ticker.ScalarFormatter(useOffset=False)
- ax1.yaxis.set_major_formatter(y_formatter)
-
- #ax1.plot( 1e3*self.DATADICT[pulse][chan]["FFT"]["nu"][0:len(SimpleStack[pulse][chan])], np.average(SimpleStack[pulse][chan], 0 )) #, color='darkblue' )
- #ax1.pcolor( np.real(SimpleStack[pulse][chan]) ) #, color='darkblue' )
- ax1.matshow( np.real(SimpleStack[pulse][chan]), aspect='auto') #, color='darkblue' )
- ax1.set_title("Ch." + str(chan) + ": avg FID", fontsize=8)
- ax1.set_xlabel(r"time (ms)", fontsize=8)
-
- if ichan == 0:
- ax1.set_ylabel(r"signal [nV]", fontsize=8)
- else:
- plt.setp(ax1.get_yticklabels(), visible=False)
- plt.setp(ax1.get_yaxis().get_offset_text(), visible=False)
- ichan += 1
-
- #########################
- # Oulier rejectig stack #
- #########################
- if outlierTest == "MAD":
- MADStack = {}
- VarStack = {}
- #1.4826 is assumption of gaussian noise
- madstack = np.zeros(( len(self.DATADICT[pulse]["chan"]),\
- self.DATADICT["nPulseMoments"],\
- len(self.DATADICT[pulse][self.DATADICT[pulse]["chan"][0] ]["FFT"]["nu"])//2 + 1))
- varstack = np.zeros(( len(self.DATADICT[pulse]["chan"]),\
- self.DATADICT["nPulseMoments"],\
- len(self.DATADICT[pulse][self.DATADICT[pulse]["chan"][0] ]["FFT"]["nu"])//2 + 1))
- for pulse in self.DATADICT["PULSES"]:
- MADStack[pulse] = {}
- VarStack[pulse] = {}
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
- ax1 = axes[ 2*ichan ]
- for ipm in range(self.DATADICT["nPulseMoments"]):
- # # brutal loop over time, can this be vectorized?
- # for it in range(len(self.DATADICT[pulse]["TIMES"])):
- # x = 1e9 *Stack[pulse][ichan,ipm,:,it]
- # MAD = 1.4826 * np.median( np.abs(x-np.median(x)) )
- # good = 0
- # for istack in self.DATADICT["stacks"]:
- # if (np.abs(x[istack-1]-np.median(x))) / MAD < 2:
- # good += 1
- # madstack[ ichan, ipm, it ] += x[istack-1]
- # else:
- # pass
- # madstack[ichan, ipm, it] /= good
- # percent = int(1e2* (float)(ipm) / (float)(self.DATADICT["nPulseMoments"]) )
- # self.progressTrigger.emit(percent)
-
- # Vectorized version of above...much, much faster
- x = 1e9*copy.deepcopy(Stack[pulse][ichan][ipm,:,:]) # stack and time indices
- tile_med = np.tile( np.median(x, axis=0), (np.shape(x)[0],1))
- MAD = MADcutoff * np.median(np.abs(x - tile_med), axis=0)
- tile_MAD = np.tile( MAD, (np.shape(x)[0],1))
- good = np.abs(x-tile_med)/tile_MAD < 2. # 1.4826 # 2
-
- madstack[ichan][ipm] = copy.deepcopy( np.ma.masked_array(x, good != True).mean(axis=0) )
- varstack[ichan][ipm] = copy.deepcopy( np.ma.masked_array(x, good != True).std(axis=0) )
-
- # reporting
- percent = int(1e2* (float)((ipm)+ichan*self.DATADICT["nPulseMoments"]) /
- (float)(self.DATADICT["nPulseMoments"] * len(self.DATADICT[pulse]["chan"])))
- self.progressTrigger.emit(percent)
-
- ax2 = axes[2*ichan+1] # TODO fix hard coded number
- #ax1.plot( 1e3*self.DATADICT[pulse]["TIMES"], np.average( madstack[ichan], 0 ))# , color='darkred')
- MADStack[pulse][chan] = madstack[ichan]
- VarStack[pulse][chan] = varstack[ichan]
- ax2.matshow( np.real(MADStack[pulse][chan]), aspect='auto') #, color='darkblue' )
- ichan += 1
-
- self.DATADICT["stack"] = MADStack
-
- else:
- self.DATADICT["stack"] = SimpleStack
-
- # #########################################
- # # Plot Fourier Transform representation #
- # #########################################
- #
- # # canvas.fig.subplots_adjust(right=0.8)
- # # cbar_ax = canvas.fig.add_axes([0.85, 0.1, 0.015, 0.355])
- # # cbar_ax.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
- # im2 = []
- # im1 = []
- # for pulse in self.DATADICT["PULSES"]:
- # ichan = 0
- # axes = canvas.fig.axes
- # vvmin = 1e10
- # vvmax = 0
- # for chan in self.DATADICT[pulse]["chan"]:
- # ax1 = axes[2*ichan ]
- # ax2 = axes[2*ichan+1] # TODO fix hard coded number
- # if outlierTest == "MAD":
- # X = np.fft.rfft( MADStack[pulse][chan][0,:] )
- # nu = np.fft.fftfreq(len( MADStack[pulse][chan][0,:]), d=self.dt)
- # else:
- # X = np.fft.rfft( SimpleStack[pulse][chan][0,:] )
- # nu = np.fft.fftfreq(len( SimpleStack[pulse][chan][0,:]), d=self.dt)
- #
- # nu = nu[0:len(X)]
- # nu[-1] = np.abs(nu[-1])
- # df = nu[1] - nu[0]
- # of = 0
- #
- # istart = int((self.transFreq-50.)/df)
- # iend = int((self.transFreq+50.)/df)
- # of = nu[istart]
- #
- # def freqlabel(xxx, pos):
- # return '%1.0f' %(of + xxx*df)
- # formatter = FuncFormatter(freqlabel)
- #
- # SFFT = np.zeros( (self.DATADICT["nPulseMoments"], len(X)), dtype=np.complex64 )
- # SFFT[0,:] = X
- # for ipm in range(1, self.DATADICT["nPulseMoments"]):
- # if outlierTest == "MAD":
- # SFFT[ipm,:] = np.fft.rfft( MADStack[pulse][chan][ipm,:] )
- # else:
- # SFFT[ipm,:] = np.fft.rfft( SimpleStack[pulse][chan][ipm,:] )
- #
- # # convert to dB and add colorbars
- # #db = 20.*np.log10(np.abs(SFFT[:,istart:iend]))
- # db = (np.abs(SFFT[:,istart:iend]))
- # #db = (np.real(SFFT[:,istart:iend]))
- # #dbr = (np.real(SFFT[:,istart:iend]))
- # #db = (np.imag(SFFT[:,istart:iend]))
- #
- # vvmin = min(vvmin, np.min (db))
- # vvmax = max(vvmax, np.max (db))
- # im2.append(ax2.matshow( db, aspect='auto', cmap=cmocean.cm.ice, vmin=vvmin, vmax=vvmax))
- # #im1.append(ax1.matshow( dbr, aspect='auto')) #, vmin=vvmin, vmax=vvmax))
- # #im2.append(ax2.matshow( db, aspect='auto', vmin=vvmin, vmax=vvmax))
- # #im2 = ax2.matshow( db, aspect='auto', cmap=cmocean.cm.ice, vmin=vvmin, vmax=vvmax)
- # if ichan == 0:
- # ax2.set_ylabel(r"$q$ (A $\cdot$ s)", fontsize=8)
- # else:
- # #ax2.yaxis.set_ticklabels([])
- # plt.setp(ax2.get_yticklabels(), visible=False)
- #
- # ax2.xaxis.set_major_formatter(formatter)
- # ax2.xaxis.set_ticks_position('bottom')
- # ax2.xaxis.set_major_locator(MaxNLocator(3))
- #
- # y_formatter = matplotlib.ticker.ScalarFormatter(useOffset=False)
- # ax2.yaxis.set_major_formatter(y_formatter)
- #
- #
- # #if chan == self.DATADICT[pulse]["chan"][-1]:
- # #cb2 = canvas.fig.colorbar(im2, cax=cbar_ax, format='%1.0e')
- #
- # #cb2 = canvas.fig.colorbar(im2[0], ax=ax2, format='%1.0e', orientation='horizontal')
- # #cb2 = canvas.fig.colorbar(im2, ax=ax2, format='%1.0e', orientation='horizontal')
- # #cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- # #cb2.set_label("signal (dB)", fontsize=8)
- #
- # ichan += 1
- #
- #
- # canvas.fig.subplots_adjust(hspace=.1, wspace=.05, left=.075, right=.95 )#left=None, bottom=None, right=None, top=None, wspace=None, hspace=None)
- #
- # #cb1 = canvas.fig.colorbar(im, ax=axes[0::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30)
- # #cb1.ax.tick_params(axis='both', which='major', labelsize=8)
- # #cb1.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
- #
- # cb2 = canvas.fig.colorbar(im2[-1], ax=axes[1::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30)
- # cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- # cb2.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
-
- #canvas.fig.tight_layout()
- canvas.draw()
- self.doneTrigger.emit()
-
-
- def sumData(self, canvas, fred):
- chans = copy.deepcopy(self.DATADICT[self.DATADICT["PULSES"][0]]["chan"]) #= np.array( ( self.DATADICT[pulse]["chan"][0], ) )
- nchan = len(chans)
- # Sum permutations of two channel combos
- for ich in range(nchan-1):
- for ch in chans[ich+1:]:
- chsum = chans[ich] + "+" + ch
- for pulse in self.DATADICT["PULSES"]:
- self.DATADICT[pulse][chsum] = {}
- for ipm in range(self.DATADICT["nPulseMoments"]):
- self.DATADICT[pulse][chsum][ipm] = {}
- for istack in self.DATADICT["stacks"]:
- self.DATADICT[pulse][chsum][ipm][istack] = self.DATADICT[pulse][chans[ich]][ipm][istack] - self.DATADICT[pulse][ch][ipm][istack]
- if chsum == "1+2":
- #self.DATADICT[pulse]["rchan"].pop()
- #self.DATADICT[pulse]["rchan"].pop()
- self.DATADICT[pulse]["chan"].append(chsum)
-
- # Sum all channels
- sumall = False
- if sumall:
- chsum = ""
- for ch in chans:
- chsum += ch + "+"
- chsum = chsum[0:-1] # remove last "+"
-
- for pulse in self.DATADICT["PULSES"]:
- self.DATADICT[pulse][chsum] = {}
- for ipm in range(self.DATADICT["nPulseMoments"]):
- self.DATADICT[pulse][chsum][ipm] = {}
- for istack in self.DATADICT["stacks"]:
- self.DATADICT[pulse][chsum][ipm][istack] = copy.deepcopy(self.DATADICT[pulse][chans[0]][ipm][istack])
- for ch in chans[1:]:
- self.DATADICT[pulse][chsum][ipm][istack] += self.DATADICT[pulse][ch][ipm][istack]
- self.DATADICT[pulse]["chan"].append(chsum)
-
- # if nchan > 2:
- # for ch in chans:
- # chsum += ch
- # for ch2 in chans[1::]:
- # for pulse in self.DATADICT["PULSES"]:
- # self.DATADICT[pulse][chsum] = {}
- # for istack in self.DATADICT["stacks"]:
- # self.DATADICT[pulse][chsum][ipm][istack] = self.DATADICT[pulse][chans[ich]][ipm][istack] + self.DATADICT[pulse][ch][ipm][istack]
- self.doneTrigger.emit()
-
- def quadDet(self, clip, method, loss, canvas):
-
- from scipy import signal
- self.RotatedAmplitude = True
-
- wL = self.transFreq * 2*np.pi
- vL = self.transFreq
- #T = 50
- dt = self.dt
- #DT = 0.01
-
- CA = {} # corrected amplitude
- IP = {} # instantaneous phase
- NR = {} # Noise residual
- RE = {} # Real channel
- IM = {} # Imaginary channel
-
- # global maximums for plotting
- CAmax = {}
- NRmax = {}
- REmax = {}
- IMmax = {}
- E0,phi,df,T2 = 100.,0,0,.2
- first = False
- self.sigma = {}
- for pulse in self.DATADICT["PULSES"]:
- CA[pulse] = {}
- IP[pulse] = {}
- NR[pulse] = {}
- RE[pulse] = {}
- IM[pulse] = {}
- CAmax[pulse] = 0
- NRmax[pulse] = 0
- REmax[pulse] = 0
- IMmax[pulse] = 0
- ichan = 0
- self.sigma[pulse] = {}
- for chan in self.DATADICT[pulse]["chan"]:
- CA[pulse][chan] = np.zeros( (self.DATADICT["nPulseMoments"], len(self.DATADICT[pulse]["TIMES"])-clip ) )
- IP[pulse][chan] = np.zeros( (self.DATADICT["nPulseMoments"], len(self.DATADICT[pulse]["TIMES"])-clip ) )
- NR[pulse][chan] = np.zeros( (self.DATADICT["nPulseMoments"], len(self.DATADICT[pulse]["TIMES"])-clip ) )
- RE[pulse][chan] = np.zeros( (self.DATADICT["nPulseMoments"], len(self.DATADICT[pulse]["TIMES"])-clip ) )
- IM[pulse][chan] = np.zeros( (self.DATADICT["nPulseMoments"], len(self.DATADICT[pulse]["TIMES"])-clip ) )
- for ipm in range(0, self.DATADICT["nPulseMoments"]):
- #t = self.DATADICT[pulse]["TIMES"] - self.DATADICT[pulse]["PULSE_TIMES"][-1]
- xn = self.DATADICT["stack"][pulse][chan][ipm,:]
- ht = signal.hilbert(xn)*np.exp(-1j*wL*self.DATADICT[pulse]["TIMES"])
- #############################################################
- # Quadrature signal
- RE[pulse][chan][ipm,:] = np.real(ht[clip::])
- IM[pulse][chan][ipm,:] = np.imag(ht[clip::])
- REmax[pulse] = max(REmax[pulse], np.max(np.real(ht[clip::])))
- IMmax[pulse] = max(IMmax[pulse], np.max(np.imag(ht[clip::])))
- #############################################################
- # Instantaneous phase
- IP[pulse][chan][ipm,:] = np.angle(ht)[clip::]
- #############################################################
- # Rotated amplitude
- #if ipm != 0:
- # [success, E0, df, phi, T2] = decay.quadratureDetect2( ht.real, ht.imag, self.DATADICT[pulse]["TIMES"], (E0,phi,df,T2))
- #[success, E0, df, phi, T2] = decay.quadratureDetect( ht.real, ht.imag, self.DATADICT[pulse]["TIMES"] )
- #else:
- [success, E0, df, phi, T2] = decay.quadratureDetect2( ht.real, ht.imag, self.DATADICT[pulse]["TIMES"], method, loss)
- #[success, E0, df, phi, T2] = decay.quadratureDetect2( ht.real, ht.imag, self.DATADICT[pulse]["TIMES"], (E0,phi,df,T2))
- #[success, E0, df, phi, T2] = decay.quadratureDetect( ht.real, ht.imag, self.DATADICT[pulse]["TIMES"] )
- #print("success", success, "E0", E0, "phi", phi, "df", df, "T2", T2)
-
- D = self.RotateAmplitude( ht.real, ht.imag, phi, df, self.DATADICT[pulse]["TIMES"] )
- CA[pulse][chan][ipm,:] = D.imag[clip::] # amplitude data
- NR[pulse][chan][ipm,:] = D.real[clip::] # noise data
- CAmax[pulse] = max(CAmax[pulse], np.max(D.imag[clip::]) )
- NRmax[pulse] = max(NRmax[pulse], np.max(D.real[clip::]) )
- self.sigma[pulse][chan] = np.std(NR[pulse][chan])
- # reporting
- percent = int(1e2* (float)((ipm)+ichan*self.DATADICT["nPulseMoments"]) /
- (float)(self.DATADICT["nPulseMoments"] * len(self.DATADICT[pulse]["chan"])))
- self.progressTrigger.emit(percent)
- ichan += 1
-
- self.DATADICT["CA"] = CA
- self.DATADICT["IP"] = IP
- self.DATADICT["NR"] = NR
- self.DATADICT["RE"] = RE
- self.DATADICT["IM"] = IM
-
- self.DATADICT["CAmax"] = CAmax
- self.DATADICT["NRmax"] = NRmax
- self.DATADICT["REmax"] = REmax
- self.DATADICT["IMmax"] = IMmax
-
- self.doneTrigger.emit()
-
- def plotQuadDet(self, clip, phase, canvas):
-
- canvas.reAxH2( len(self.DATADICT[ self.DATADICT["PULSES"][0] ]["chan"] ), False, False)
-
- ###############
- # Plot on GUI #
- ###############
- dcmap = cmocean.cm.curl_r #"seismic_r" #cmocean.cm.balance_r #"RdBu" #YlGn" # "coolwarm_r" # diverging
- canvas.reAxH2( len(self.DATADICT[ self.DATADICT["PULSES"][0] ]["chan"] ), False, False)
- for pulse in self.DATADICT["PULSES"]:
- ichan = 0
- axes = canvas.fig.axes
- mmaxr = 0.
- mmaxi = 0.
- if clip > 0:
- time_sp = 1e3 * (self.DATADICT[pulse]["TIMES"][clip-1::] - self.DATADICT[pulse]["PULSE_TIMES"][-1] )
- else:
- time_sp = 1e3 * (self.DATADICT[pulse]["TIMES"] - self.DATADICT[pulse]["PULSE_TIMES"][-1] )
-
- QQ = np.average(self.DATADICT[pulse]["Q"], axis=1 )
-
- for chan in self.DATADICT[pulse]["chan"]:
- ax1 = axes[2*ichan ]
- ax2 = axes[2*ichan+1] # TODO fix hard coded number
- if phase == 0: # Re Im
- im1 = ax1.pcolormesh( time_sp, QQ, self.DATADICT["RE"][pulse][chan], cmap=dcmap, rasterized=True,\
- vmin=-self.DATADICT["REmax"][pulse] , vmax=self.DATADICT["REmax"][pulse] )
- im2 = ax2.pcolormesh( time_sp, QQ, self.DATADICT["IM"][pulse][chan], cmap=dcmap, rasterized=True,\
- vmin=-self.DATADICT["IMmax"][pulse], vmax=self.DATADICT["IMmax"][pulse] )
- if phase == 1: # Amp phase
- im1 = ax1.pcolormesh( time_sp, QQ, self.DATADICT["CA"][pulse][chan], cmap=dcmap, rasterized=True,
- vmin=-self.DATADICT["CAmax"][pulse] , vmax=self.DATADICT["CAmax"][pulse] )
- im2 = ax2.pcolormesh( time_sp, QQ, self.DATADICT["IP"][pulse][chan], cmap=cmocean.cm.phase, rasterized=True,\
- vmin=-np.pi, vmax=np.pi)
- if phase == 2: # CA NR
- im1 = ax1.pcolormesh( time_sp, QQ, self.DATADICT["CA"][pulse][chan], cmap=dcmap, rasterized=True,\
- vmin=-self.DATADICT["CAmax"][pulse] , vmax=self.DATADICT["CAmax"][pulse] )
- im2 = ax2.pcolormesh( time_sp, QQ, self.DATADICT["NR"][pulse][chan], cmap=dcmap, rasterized=True,\
- vmin=-self.DATADICT["NRmax"][pulse] , vmax=self.DATADICT["NRmax"][pulse] )
- # cb2 = canvas.fig.colorbar(im2, ax=ax2, format='%1.0e')
- # cb2.set_label("Noise residual (nV)", fontsize=8)
- # cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- # cb1 = canvas.fig.colorbar(im1, ax=ax1, format='%1.0e')
- # cb1.set_label("Phased amplitude (nV)", fontsize=8)
- # cb1.ax.tick_params(axis='both', which='major', labelsize=8)
-
- # cb2 = canvas.fig.colorbar(im2, ax=ax2, format="%1.0e")
- # cb2.set_label("Phase (rad)", fontsize=8)
- # cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- # cb1 = canvas.fig.colorbar(im1, ax=ax1, format="%1.0e")
- # cb1.set_label("FID (nV)", fontsize=8)
- # cb1.ax.tick_params(axis='both', which='major', labelsize=8)
-
- # if you save these as pdf or eps, there are artefacts
- # for cbar in [cb1,cb2]:
- # #cbar.solids.set_rasterized(True)
- # cbar.solids.set_edgecolor("face")
-
- # reporting
- percent = int(1e2* (float)(ichan)/len(self.DATADICT[pulse]["chan"]))
- self.progressTrigger.emit(percent)
-
- if ichan == 0:
- ax1.set_ylabel(r"$q$ ( $\mathrm{A}\cdot\mathrm{s}$)", fontsize=8)
- ax2.set_ylabel(r"$q$ ( $\mathrm{A}\cdot\mathrm{s}$)", fontsize=8)
- else:
- #ax2.yaxis.set_ticklabels([])
- #ax1.yaxis.set_ticklabels([])
- plt.setp(ax1.get_yticklabels(), visible=False)
- plt.setp(ax2.get_yticklabels(), visible=False)
- ichan += 1
-
- ax1.set_yscale('log')
- ax2.set_yscale('log')
-
- plt.setp(ax1.get_xticklabels(), visible=False)
-
- ax1.set_ylim( np.min(QQ), np.max(QQ) )
- ax2.set_ylim( np.min(QQ), np.max(QQ) )
-
- ax1.set_xlim( np.min(time_sp), np.max(time_sp) )
- ax2.set_xlim( np.min(time_sp), np.max(time_sp) )
-
- #ax2.set_xlabel(r"Time since end of pulse (ms)", fontsize=8)
- ax2.set_xlabel(r"Time (ms)", fontsize=8)
-
- canvas.fig.subplots_adjust(hspace=.15, wspace=.05, left=.075, right=.95, bottom=.1, top=.95 )#left=None, bottom=None, right=None, top=None, wspace=None, hspace=None)
- tick_locator = MaxNLocator(nbins=3)
-
- cb1 = canvas.fig.colorbar(im1, ax=axes[0::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30)
- cb1.ax.tick_params(axis='both', which='major', labelsize=8)
- cb1.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
- cb1.locator = tick_locator
- cb1.update_ticks()
-
- tick_locator2 = MaxNLocator(nbins=3)
- cb2 = canvas.fig.colorbar(im2, ax=axes[1::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30, pad=.2)
- cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- cb2.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
-
-
- cb2.locator = tick_locator2
- cb2.update_ticks()
-
- canvas.draw()
- self.doneTrigger.emit()
-
- def RotateAmplitude(self, X, Y, zeta, df, t):
- V = X + 1j*Y
- return np.abs(V) * np.exp( 1j * ( np.angle(V) - zeta - 2.*np.pi*df*t ) )
-
- def gateIntegrate( self, gpd, clip, canvas ):
- """ Gate integrate the real, imaginary, phased, and noise residual channels
- """
-
- self.gated = True
- self.GATED = {}
-
- for pulse in self.DATADICT["PULSES"]:
- QQ = np.average(self.DATADICT[pulse]["Q"], axis=1 )
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
- self.GATED[chan] = {}
- for ipm in range(0, self.DATADICT["nPulseMoments"]):
-
- # Time since pulse rather than since record starts...
- #if clip > 0:
- # time_sp = 1e3 * (self.DATADICT[pulse]["TIMES"][clip:] - self.DATADICT[pulse]["PULSE_TIMES"][-1] )
- #else:
- time_sp = 1e3 * (self.DATADICT[pulse]["TIMES"] - self.DATADICT[pulse]["PULSE_TIMES"][-1] )
-
- #GT, GD, GTT, sig_stack, isum = rotate.gateIntegrate( self.DATADICT["CA"][pulse][chan][ipm,:], time_sp, gpd, self.sigma[pulse][chan], 1.5 )
- #GT2, GP, GTT, sig_stack_err, isum = rotate.gateIntegrate( self.DATADICT["NR"][pulse][chan][ipm,:], time_sp, gpd, self.sigma[pulse][chan], 1.5 )
-
- GT, GCA, GTT, sig_stack, isum = rotate.gateIntegrate( self.DATADICT["CA"][pulse][chan][ipm], time_sp, gpd, self.sigma[pulse][chan], 1.5 )
- GT, GNR, GTT, sig_stack, isum = rotate.gateIntegrate( self.DATADICT["NR"][pulse][chan][ipm], time_sp, gpd, self.sigma[pulse][chan], 1.5 )
- GT, GRE, GTT, sig_stack, isum = rotate.gateIntegrate( self.DATADICT["RE"][pulse][chan][ipm], time_sp, gpd, self.sigma[pulse][chan], 1.5 )
- GT, GIM, GTT, sig_stack, isum = rotate.gateIntegrate( self.DATADICT["IM"][pulse][chan][ipm], time_sp, gpd, self.sigma[pulse][chan], 1.5 )
- GT, GIP, GTT, sig_stack, isum = rotate.gateIntegrate( self.DATADICT["IP"][pulse][chan][ipm], time_sp, gpd, self.sigma[pulse][chan], 1.5 )
-
- if ipm == 0:
- # self.GATED[chan]["DATA"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)) )
- # self.GATED[chan]["ERR"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)) )
- # self.GATED[chan]["SIGMA"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)) )
- self.GATED[chan]["CA"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)-clip) )
- self.GATED[chan]["NR"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)-clip) )
- self.GATED[chan]["RE"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)-clip) )
- self.GATED[chan]["IM"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)-clip) )
- self.GATED[chan]["IP"] = np.zeros( ( self.DATADICT["nPulseMoments"], len(GT)-clip) )
- self.GATED[chan]["isum"] = isum
-
- #self.GATED[chan]["DATA"][ipm] = GD.real
- self.GATEDABSCISSA = GT[clip:]
- self.GATEDWINDOW = GTT[clip:]
- #self.GATED[chan]["SIGMA"][ipm] = sig_stack #_err # GP.real
- #self.GATED[chan]["ERR"][ipm] = GP.real
-
- self.GATED[chan]["CA"][ipm] = GCA.real[clip:]
- self.GATED[chan]["NR"][ipm] = GNR.real[clip:]
- self.GATED[chan]["RE"][ipm] = GRE.real[clip:]
- self.GATED[chan]["IM"][ipm] = GIM.real[clip:]
- self.GATED[chan]["IP"][ipm] = GIP.real[clip:]
-
- percent = int(1e2* (float)((ipm)+ichan*self.DATADICT["nPulseMoments"]) /
- (float)(self.DATADICT["nPulseMoments"] * len(self.DATADICT[pulse]["chan"])))
- self.progressTrigger.emit(percent)
-
- self.GATED[chan]["GTT"] = GTT[clip:]
- self.GATED[chan]["GT"] = GT[clip:]
- self.GATED[chan]["QQ"] = QQ
- ichan += 1
- self.doneTrigger.emit()
-
- def bootstrap_resample(self, X, n=None):
- # from http://nbviewer.jupyter.org/gist/aflaxman/6871948
- """ Bootstrap resample an array_like
- Parameters
- ----------
- X : array_like
- data to resample
- n : int, optional
- length of resampled array, equal to len(X) if n==None
- Results
- -------
- returns X_resamples
- """
- if n == None:
- n = len(X)
-
- resample_i = np.floor(np.random.rand(n)*len(X)).astype(int)
- return X[resample_i]
-
- def bootstrap_sigma(self, pulse, chan):
-
- # bootstrap resample
- nt = len(self.GATED[chan]["GT"])
- nb = 5000
- XS = np.zeros( (nb, nt) )
- for ii in range(nb):
- for it in range(nt):
- if self.GATED[chan]["isum"][it] < 8:
- XS[ii, it] = self.sigma[pulse][chan]
- else:
-
- if it == 0:
- X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it], self.GATED[chan]["NR"][:,it+1], \
- self.GATED[chan]["NR"][:,it+2], self.GATED[chan]["NR"][:,it+3] ) ), n=nt )
- elif it == 1:
- X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it-1], self.GATED[chan]["NR"][:,it], \
- self.GATED[chan]["NR"][:,it+1], self.GATED[chan]["NR"][:,it+2] ) ), n=nt )
- elif it == nt-2:
- X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it+1], self.GATED[chan]["NR"][:,it], \
- self.GATED[chan]["NR"][:,it-1], self.GATED[chan]["NR"][:,it-2] ) ), n=nt )
- elif it == nt-1:
- X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it], self.GATED[chan]["NR"][:,it-1], \
- self.GATED[chan]["NR"][:,it-2], self.GATED[chan]["NR"][:,it-3] ) ), n=nt )
- else:
- X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it-2] , self.GATED[chan]["NR"][:,it-1], \
- self.GATED[chan]["NR"][:,it], self.GATED[chan]["NR"][:,it+1], self.GATED[chan]["NR"][:,it+2] )), n=nt )
- XS[ii,it] = np.std(X)
- return XS
-
- def plotGateIntegrate( self, gpd, clip, phase, canvas ):
- """ Plot the gate integration
- """
-
- canvas.reAxH2( len(self.DATADICT[ self.DATADICT["PULSES"][0] ]["chan"] ), False, False)
- axes = canvas.fig.axes
- cmap = cmocean.cm.balance_r
-
- # Calculate maximum for plotting...TODO move into loop above
- vmax1 = 0
- vmax2 = 0
- for pulse in self.DATADICT["PULSES"]:
- for chan in self.DATADICT[pulse]["chan"]:
- if phase == 0:
- vmax1 = max(vmax1, np.max(np.abs(self.GATED[chan]["RE"])))
- vmax2 = max(vmax2, np.max(np.abs(self.GATED[chan]["IM"])))
- elif phase == 1:
- vmax1 = max(vmax1, np.max(np.abs(self.GATED[chan]["CA"])))
- vmax2 = np.pi
- elif phase == 2:
- vmax1 = max(vmax1, np.max(np.abs(self.GATED[chan]["CA"])))
- vmax2 = max(vmax2, np.max(np.abs(self.GATED[chan]["NR"])))
-
-
- for pulse in self.DATADICT["PULSES"]:
- ichan = 0
- for chan in self.DATADICT[pulse]["chan"]:
-
- ax1 = axes[2*ichan ]
- ax2 = axes[2*ichan+1]
-
- if phase == 0:
- im1 = ax1.pcolormesh(self.GATED[chan]["GTT"], self.GATED[chan]["QQ"], self.GATED[chan]["RE"], cmap=cmap, vmin=-vmax1, vmax=vmax1)
- im2 = ax2.pcolormesh(self.GATED[chan]["GTT"], self.GATED[chan]["QQ"], self.GATED[chan]["IM"], cmap=cmap, vmin=-vmax2, vmax=vmax2)
- elif phase == 1:
- im1 = ax1.pcolormesh(self.GATED[chan]["GTT"], self.GATED[chan]["QQ"], self.GATED[chan]["CA"], cmap=cmap, vmin=-vmax1, vmax=vmax1)
- im2 = ax2.pcolormesh(self.GATED[chan]["GTT"], self.GATED[chan]["QQ"], self.GATED[chan]["IP"], cmap=cmocean.cm.phase, vmin=-vmax2, vmax=vmax2)
- elif phase == 2:
- im1 = ax1.pcolormesh(self.GATED[chan]["GTT"], self.GATED[chan]["QQ"], self.GATED[chan]["CA"], cmap=cmap, vmin=-vmax1, vmax=vmax1)
- XS = self.bootstrap_sigma(pulse, chan)
- #im2 = ax2.pcolormesh(self.GATED[chan]["GTT"], self.GATED[chan]["QQ"], self.GATED[chan]["NR"], cmap=cmap, vmin=-vmax2, vmax=vmax2)
- # bootstrap resample
- # nt = len(self.GATED[chan]["GT"])
- # nb = 5000
- # XS = np.zeros( (nb, nt) )
- # for ii in range(nb):
- # #XS = []
- # for it in range(nt):
- # if self.GATED[chan]["isum"][it] < 8:
- # XS[ii, it] = self.sigma[pulse][chan]
- # else:
- # if it == 0:
- # X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it], self.GATED[chan]["NR"][:,it+1], \
- # self.GATED[chan]["NR"][:,it+2], self.GATED[chan]["NR"][:,it+3] ) ), n=nt )
- # if it == 1:
- # X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it-1], self.GATED[chan]["NR"][:,it], \
- # self.GATED[chan]["NR"][:,it+1], self.GATED[chan]["NR"][:,it+2] ) ), n=nt )
- # elif it == nt-2:
- # X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it+1], self.GATED[chan]["NR"][:,it], \
- # self.GATED[chan]["NR"][:,it-1], self.GATED[chan]["NR"][:,it-2] ) ), n=nt )
- # elif it == nt-1:
- # X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it], self.GATED[chan]["NR"][:,it-1], \
- # self.GATED[chan]["NR"][:,it-2], self.GATED[chan]["NR"][:,it-3] ) ), n=nt )
- # else:
- # X = self.bootstrap_resample( np.concatenate( (self.GATED[chan]["NR"][:,it-2] , self.GATED[chan]["NR"][:,it-1], \
- # self.GATED[chan]["NR"][:,it], self.GATED[chan]["NR"][:,it+1], self.GATED[chan]["NR"][:,it+2] )), n=nt )
- # XS[ii,it] = np.std(X)
- #if ii == 0:
- # ax2.plot( self.GATED[chan]["GT"], XS[ii], '-', linewidth=1, markersize=4, alpha=.5, color='lightgrey', label = "bootstrap sim" )
- #else:
- # ax2.plot( self.GATED[chan]["GT"], XS[ii], '-', linewidth=1, markersize=4, alpha=.5, color='lightgrey' )
- ax2.plot( self.GATED[chan]["GT"], np.std(self.GATED[chan]["NR"], axis=0), color='darkgrey', linewidth=2, label="gate std" )
- ax2.plot( np.tile(self.GATED[chan]["GT"], (5000,1) ), XS, '.', color='lightgrey', linewidth=1, alpha=.5 )
- ax2.plot( self.GATED[chan]["GT"], np.average(XS, axis=0), color='black', linewidth=2, label="bootstrap avg." )
- ax2.plot( self.GATED[chan]["GT"], np.median(XS, axis=0), color='black', linewidth=2, label="bootstrap med." )
- ax2.legend()
-
- im1.set_edgecolor('face')
- if phase != 2:
- im2.set_edgecolor('face')
-
-
- plt.setp(ax1.get_xticklabels(), visible=False)
-
- ax1.set_ylim( np.min(self.GATED[chan]["QQ"]), np.max(self.GATED[chan]["QQ"]) )
-
- if phase != 2:
- ax2.set_ylim( np.min(self.GATED[chan]["QQ"]), np.max(self.GATED[chan]["QQ"]) )
-
- ax1.set_xlim( np.min(self.GATED[chan]["GTT"]), np.max(self.GATED[chan]["GTT"]) )
- ax2.set_xlim( np.min(self.GATED[chan]["GTT"]), np.max(self.GATED[chan]["GTT"]) )
-
- ax1.set_yscale('log')
- ax2.set_yscale('log')
-
- qlabs = np.append(np.concatenate( ( self.GATED[chan]["QQ"][0:1], self.GATED[chan]["QQ"][9::10] )), self.GATED[chan]["QQ"][-1] )
- ax1.yaxis.set_ticks( qlabs ) # np.append(np.concatenate( (QQ[0:1],QQ[9::10] )), QQ[-1] ) )
- if phase != 2:
- ax2.yaxis.set_ticks( qlabs ) #np.append(np.concatenate( (QQ[0:1],QQ[9::10] )), QQ[-1] ) )
- #formatter = matplotlib.ticker.LogFormatter(10, labelOnlyBase=False)
- formatter = matplotlib.ticker.FuncFormatter(lambda x, pos: str((round(x,1))))
-
- ax1.yaxis.set_major_formatter(formatter) #matplotlib.ticker.FormatStrFormatter('%d.1'))
- ax2.yaxis.set_major_formatter(formatter) #matplotlib.ticker.FormatStrFormatter('%d.1'))
-
- ax1.xaxis.set_major_formatter(formatter) #matplotlib.ticker.FormatStrFormatter('%d.1'))
- ax2.xaxis.set_major_formatter(formatter) #matplotlib.ticker.FormatStrFormatter('%d.1'))
-
- ax1.set_xscale('log')
- ax2.set_xscale('log')
-
- if ichan == 0:
- ax1.set_ylabel(r"$q$ ( $\mathrm{A}\cdot\mathrm{s}$)", fontsize=8)
- if phase == 2:
- ax2.set_ylabel(r"noise est. (nV)", fontsize=8)
- else:
- ax2.set_ylabel(r"$q$ ( $\mathrm{A}\cdot\mathrm{s}$)", fontsize=8)
- else:
- plt.setp(ax1.get_yticklabels(), visible=False)
- plt.setp(ax2.get_yticklabels(), visible=False)
-
- ax2.set_xlabel(r"$t-\tau_p$ (ms)", fontsize=8)
- ichan += 1
-
- #canvas.fig.subplots_adjust(hspace=.1, wspace=.05, left=.075, right=.925 )#left=None, bottom=None, right=None, top=None, wspace=None, hspace=None)
- #canvas.fig.tight_layout()
- #canvas.draw()
- canvas.fig.subplots_adjust(hspace=.15, wspace=.05, left=.075, right=.95, bottom=.1, top=.95 )#left=None, bottom=None, right=None, top=None, wspace=None, hspace=None)
- tick_locator = MaxNLocator(nbins=5)
-
- cb1 = canvas.fig.colorbar(im1, ax=axes[0::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30)
- cb1.ax.tick_params(axis='both', which='major', labelsize=8)
- cb1.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
- cb1.locator = tick_locator
- cb1.update_ticks()
-
- if phase != 2:
- cb2 = canvas.fig.colorbar(im2, ax=axes[1::2], format='%1.0e', orientation='horizontal', shrink=.35, aspect=30, pad=.2)
- cb2.ax.tick_params(axis='both', which='major', labelsize=8)
- cb2.set_label("$\mathcal{V}_N$ (nV)", fontsize=8)
-
- cb2.locator = tick_locator
- cb2.update_ticks()
-
- canvas.draw()
- self.doneTrigger.emit()
-
-
- def FDSmartStack(self, cv, canvas):
- from matplotlib.colors import LogNorm
- from matplotlib.ticker import MaxNLocator
- """
- Currently this stacks 4-phase second pulse data only, we need to generalise
- """
-
- try:
- canvas.fig.clear()
- except:
- pass
-
-
- self.dataCubeFFT( )
-
- # canvas.ax1 = canvas.fig.add_axes([.1, .1, .8, .8])
- canvas.ax1 = canvas.fig.add_axes([.1, .1, .2, .8])
- canvas.ax2 = canvas.fig.add_axes([.325, .1, .2, .8])
- canvas.ax3 = canvas.fig.add_axes([.55, .1, .2, .8])
- canvas.ax4 = canvas.fig.add_axes([.815, .1, .05, .8]) #cb
- canvas.ax1.tick_params(axis='both', which='major', labelsize=8)
- canvas.ax2.tick_params(axis='both', which='major', labelsize=8)
- canvas.ax3.tick_params(axis='both', which='major', labelsize=8)
- canvas.ax4.tick_params(axis='both', which='major', labelsize=8)
- canvas.ax1.set_ylabel("pulse index", fontsize=8)
- canvas.ax1.set_xlabel(r"$\omega$ bin", fontsize=8)
- canvas.ax2.set_xlabel(r"$\omega$ bin", fontsize=8)
- canvas.ax3.set_xlabel(r"$\omega$ bin", fontsize=8)
- canvas.ax2.yaxis.set_ticklabels([])
- canvas.ax3.yaxis.set_ticklabels([])
-
- #canvas.ax1.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
-
- # # Look at pulses
- # for pulse in self.DATADICT["PULSES"]:
- # for istack in self.DATADICT["stacks"]:
- # for ipm in range(0,3):
- # canvas.ax1.plot( self.DATADICT[pulse]["CURRENT"][ipm][istack] , label="istack "+str(istack) + " ipm=" + str(ipm) + pulse )
- # canvas.draw()
-
- # Create Container for stacks
-
-
- # sandbox determine pulse sequence again
- for pulse in self.DATADICT["PULSES"]:
- for ichan in self.DATADICT[pulse]["chan"]:
- #for ipm in range(10,11):
- CONTAINER = {}
- CONTAINER["Cycle 1"] = [] # These are actually subtracted cycles... v+ - v
- CONTAINER["Cycle 2"] = []
- for istack in self.DATADICT["stacks"]:
- #canvas.ax1.clear()
- ipm = 8
- #for ipm in range(self.DATADICT["nPulseMoments"]):
- #canvas.ax1.matshow( np.real(self.DATADICT[pulse][ichan]["FFT"][istack]), aspect='auto' )
- #canvas.draw()
- if not istack%4%4:
- # phase cycle 4, aligned with 1 after sub
- CONTAINER["Cycle 1"].append(-self.DATADICT[pulse][ichan]["FFT"][istack])
- #canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], -self.DATADICT[pulse][ichan][ipm][istack], label="istack "+str(istack)+ " " + pulse )
- elif not istack%4%3:
- # phase cycle 3, aligned with 2 after sub
- CONTAINER["Cycle 2"].append(-self.DATADICT[pulse][ichan]["FFT"][istack])
- #canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], -self.DATADICT[pulse][ichan][ipm][istack], label="istack "+str(istack)+ " " + pulse )
- elif not istack%4%2:
- # phase cycle 2
- CONTAINER["Cycle 2"].append( self.DATADICT[pulse][ichan]["FFT"][istack])
- #canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], self.DATADICT[pulse][ichan][ipm][istack], label="istack "+str(istack)+ " " + pulse )
- else:
- # phase cycle 1
- CONTAINER["Cycle 1"].append( self.DATADICT[pulse][ichan]["FFT"][istack])
- #canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], self.DATADICT[pulse][ichan][ipm][istack], label="istack "+str(istack)+ " " + pulse )
- #canvas.ax1.matshow(np.array(np.average(self.DATADICT[pulse][ichan]["FFT"]), axis=2), aspect='auto' )
- #canvas.ax1.plot( self.DATADICT[pulse]["PULSE_TIMES"], self.DATADICT[pulse]["CURRENT"][ipm][istack] , color='black', label="istack "+str(istack) )
- #canvas.ax1.plot( self.DATADICT[pulse]["CURRENT"][ipm][istack] , label="istack "+str(istack) + " iFID" + str(iFID) )
- #canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], self.DATADICT[pulse][ichan][ipm][istack], label="istack "+str(istack)+ " " + pulse )
-
- #canvas.ax1.legend(prop={'size':6})
- #canvas.draw()
-
- # Boostrap
- # stack.
- #scipy.random.shuffle(x)
-
-
-
- # Stack and calculate the pooled variance (http://en.wikipedia.org/wiki/Pooled_variance)
- """ All this phase cycling wreaks havoc on a normal calculation of std. and variance. Instead, we resort to calculating
- a pooled variance. In this assumption is that the precision of the measurment is constant. This is a poor choice for
- any type of moving sensor.
- """
- # if a window filter has been applied
- #self.WINDOW
- #self.IWindowStart
- #self.iWindowEnd
- #self.FFTtimes
- CONTAINER = .5*(np.array(CONTAINER["Cycle 2"]) - np.array(CONTAINER["Cycle 1"]))
- print ("container shape", np.shape( CONTAINER), self.iWindowStart+1, self.iWindowEnd-1)
- dmin = np.min(np.abs(np.average(np.array(CONTAINER)[:,:,self.iWindowStart+1:self.iWindowEnd-1], axis=0)))
- dmax = np.max(np.abs(np.average(np.array(CONTAINER)[:,:,self.iWindowStart+1:self.iWindowEnd-1], axis=0)))
- mn = canvas.ax1.matshow( 20.*np.log10(np.abs(np.average(np.array(CONTAINER)[:,:, self.iWindowStart+1:self.iWindowEnd-1], axis=0))), aspect='auto', vmin=-120, vmax=-40)
- #mn = canvas.ax1.matshow(20.*np.log10(XA[:,istart:iend+1]), aspect='auto', vmax=-40, vmin=-120) #, norm=LogNorm())
- canvas.ax2.matshow( 20*np.log10(np.std(np.real(np.array(CONTAINER)[:,:,self.iWindowStart+1:self.iWindowEnd-1]), axis=0)), aspect='auto', vmin=-120, vmax=-40)
- canvas.ax3.matshow( 20*np.log10(np.std(np.imag(np.array(CONTAINER)[:,:,self.iWindowStart+1:self.iWindowEnd-1]), axis=0)), aspect='auto', vmin=-120, vmax=-40)
- #canvas.ax1.legend(prop={'size':6})
-
- cb1 = mpl.colorbar.Colorbar(canvas.ax4, mn)
- cb1.ax.tick_params(labelsize=8)
- cb1.set_label("power [dB]", fontsize=8)
- canvas.ax1.xaxis.set_major_locator(MaxNLocator(4))
- canvas.ax2.xaxis.set_major_locator(MaxNLocator(4))
- canvas.ax3.xaxis.set_major_locator(MaxNLocator(4))
- canvas.draw()
-
- self.doneTrigger.emit()
-
- def effectivePulseMoment(self, cv, canvas):
-
- canvas.reAxH(2)
- nstack = len(self.DATADICT["stacks"])
- canvas.ax1.set_yscale('log')
-
- for pulse in self.DATADICT["PULSES"]:
- self.DATADICT[pulse]["qeff"] = {}
- self.DATADICT[pulse]["q_nu"] = {}
- for ipm in range(self.DATADICT["nPulseMoments"]):
- self.DATADICT[pulse]["qeff"][ipm] = {}
- self.DATADICT[pulse]["q_nu"][ipm] = {}
- #canvas.ax1.clear()
- #scolours = np.array( ( np.linspace(0.8,0.4,len(self.DATADICT["stacks"])), \
- # np.linspace(0.0,0.6,len(self.DATADICT["stacks"])), \
- # np.linspace(0.6,0.0,len(self.DATADICT["stacks"])) )
- # ).T
-
- #scolours = plt.cm.Spectral(np.linspace(0,1,len(self.DATADICT["stacks"])))
- #scolours = plt.cm.Blues(np.linspace(0,1,1.5*len(self.DATADICT["stacks"])))
- scolours = cmocean.cm.ice(np.linspace(0,1,1.5*len(self.DATADICT["stacks"])))
- iistack = 0
- for istack in self.DATADICT["stacks"]:
- #self.DATADICT[pulse]["PULSE_TIMES"]
- x = self.DATADICT[pulse]["CURRENT"][ipm][istack]
- X = np.fft.rfft(x)
- v = np.fft.fftfreq(len(x), self.dt)
- v = v[0:len(X)]
- v[-1] = np.abs(v[-1])
- # calculate effective current/moment
- I0 = np.abs(X)/len(X)
- qeff = I0 * (self.DATADICT[pulse]["PULSE_TIMES"][-1]-self.DATADICT[pulse]["PULSE_TIMES"][0])
- canvas.ax1.set_title(r"pulse moment index " +str(ipm), fontsize=10)
- canvas.ax1.set_xlabel(r"$\nu$ [Hz]", fontsize=8)
- canvas.ax1.set_ylabel(r"$q_{eff}$ [A$\cdot$sec]", fontsize=8)
- canvas.ax1.plot(v, qeff, color=scolours[iistack] ) # eff current
- self.DATADICT[pulse]["qeff"][ipm][istack] = qeff
- self.DATADICT[pulse]["q_nu"][ipm][istack] = v
- iistack += 1
- canvas.draw()
-
- percent = int(1e2* (float)((istack)+ipm*self.DATADICT["nPulseMoments"]) /
- (float)(len(self.DATADICT["PULSES"])*self.DATADICT["nPulseMoments"]*nstack))
- self.progressTrigger.emit(percent)
-
- canvas.draw()
-
-
- self.plotQeffNu(cv, canvas.ax2)
- canvas.draw()
- self.doneTrigger.emit()
-
- def plotQeffNu(self, cv, ax):
-
- ####################################
- # TODO label fid1 and fid2, and make a legend, and colour by pulse
- nstack = len(self.DATADICT["stacks"])
- iFID = 0
- for pulse in self.DATADICT["PULSES"]:
- self.DATADICT[pulse]["Q"] = np.zeros( (self.DATADICT["nPulseMoments"], len(self.DATADICT["stacks"])) )
- ilabel = True
- for ipm in range(self.DATADICT["nPulseMoments"]):
- #scolours = np.array([0.,0.,1.])
- scolours = cmocean.cm.ice(np.linspace(0,1,1.5*len(self.DATADICT["stacks"])))
- #scolours = plt.cm.Spectral(np.linspace(0,1,len(self.DATADICT["stacks"])))
- #scolours = plt.cm.Spectral(np.linspace(0,1,len(self.DATADICT["stacks"])))
- istack = 0
- for stack in self.DATADICT["stacks"]:
- # find index
- icv = int (round(cv / self.DATADICT[pulse]["q_nu"][ipm][stack][1]))
- self.DATADICT[pulse]["Q"][ipm,istack] = self.DATADICT[pulse]["qeff"][ipm][stack][icv]
- if ilabel:
- ax.scatter(ipm, self.DATADICT[pulse]["qeff"][ipm][stack][icv], facecolors='none', edgecolors=scolours[istack], label=(str(pulse)))
- ilabel = False
- else:
- ax.scatter(ipm, self.DATADICT[pulse]["qeff"][ipm][stack][icv], facecolors='none', edgecolors=scolours[istack])
- #scolours += np.array((0,1./(nstack+1),-1/(nstack+1.)))
-
- percent = int(1e2* (float)((istack)+ipm*self.DATADICT["nPulseMoments"]) /
- (float)(len(self.DATADICT["PULSES"])*self.DATADICT["nPulseMoments"]*nstack))
- self.progressTrigger.emit(percent)
- istack += 1
- iFID += 1
- ax.set_xlabel(r"pulse moment index", fontsize=8)
- ax.set_ylabel(r"$q_{eff}$ [A$\cdot$sec]", fontsize=8)
- ax.set_yscale('log')
- ax.set_xlim(0, ax.get_xlim()[1])
- ax.legend(loc='upper right', scatterpoints = 1, prop={'size':6})
-
- def enableDSP(self):
- self.enableDSPTrigger.emit()
-
- def adaptiveFilter(self, M, flambda, truncate, mu, PCA, canvas):
-
- canvas.reAx2(shx=False, shy=False)
- # ax1 is top plot of filter taps
- # ax2 is bottom plot of conditioned signal
-
- if truncate:
- itrunc =(int) ( round( 1e-3*truncate*self.samp ) )
-
- print( "adaptive filter size", 1e3*self.dt*M, " [ms]" )
-
- Filt = adapt.AdaptiveFilter(flambda)
- H = {}
- for pulse in self.DATADICT["PULSES"]:
- H[pulse] = {}
- for ichan in self.DATADICT[pulse]["chan"]:
- H[pulse][ichan] = np.zeros(M)
-
- iFID = 0
- # original ordering...
- #for pulse in self.DATADICT["PULSES"]:
- # for ipm in range(self.DATADICT["nPulseMoments"]):
- # for istack in self.DATADICT["stacks"]:
- # This order makes more sense, same as data collection, verify
- for istack in self.DATADICT["stacks"]:
- for ipm in range(self.DATADICT["nPulseMoments"]):
- for pulse in self.DATADICT["PULSES"]:
- canvas.softClear()
- mmax = 0
- for ichan in self.DATADICT[pulse]["chan"]:
- canvas.ax2.plot( self.DATADICT[pulse]["TIMES"], 1e9* self.DATADICT[pulse][ichan][ipm][istack], alpha=.5)
- mmax = max(mmax, np.max(1e9*self.DATADICT[pulse][ichan][ipm][istack]))
- canvas.ax2.set_ylim(-mmax, mmax)
- canvas.ax2.set_prop_cycle(None)
-
- for ichan in self.DATADICT[pulse]["chan"]:
- #H = np.zeros(M)
- RX = []
- for irchan in self.DATADICT[pulse]["rchan"]:
- RX.append(self.DATADICT[pulse][irchan][ipm][istack][::-1])
- if all(H[pulse][ichan]) == 0:
- # call twice to reconcile filter wind-up
- [e,H[pulse][ichan]] = Filt.adapt_filt_Ref( self.DATADICT[pulse][ichan][ipm][istack][::-1],\
- RX,\
- M, mu, PCA, flambda, H[pulse][ichan])
- [e,H[pulse][ichan]] = Filt.adapt_filt_Ref( self.DATADICT[pulse][ichan][ipm][istack][::-1],\
- RX,\
- M, mu, PCA, flambda, H[pulse][ichan])
- else:
- [e,H[pulse][ichan]] = Filt.adapt_filt_Ref( self.DATADICT[pulse][ichan][ipm][istack][::-1],\
- RX,\
- M, mu, PCA, flambda, H[pulse][ichan])
- # replace
- if truncate:
- canvas.ax2.plot( self.DATADICT[pulse]["TIMES"][0:itrunc], 1e9* e[::-1][0:itrunc],\
- label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " ichan=" + str(ichan))
- self.DATADICT[pulse][ichan][ipm][istack] = e[::-1][0:itrunc]
- else:
- canvas.ax2.plot( self.DATADICT[pulse]["TIMES"], 1e9* e[::-1],\
- label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " ichan=" + str(ichan))
- self.DATADICT[pulse][ichan][ipm][istack] = e[::-1]
-
- canvas.ax1.plot( H[pulse][ichan] ) # , label="taps")
- canvas.ax2.legend(prop={'size':6}, loc='upper right')
- #canvas.ax2.legend(prop={'size':6}, loc='upper right')
-
- canvas.ax2.set_xlabel(r"time [s]", fontsize=8)
- canvas.ax2.set_ylabel(r"signal [nV]", fontsize=8)
-
- canvas.ax1.set_xlabel(r"filter index", fontsize=8)
- canvas.ax1.set_ylabel(r"scale factor", fontsize=8)
-
- canvas.draw()
-
- # truncate the reference channels too, in case you still need them for something.
- # Otherwise they are no longer aligned with the data
- for rchan in self.DATADICT[pulse]["rchan"]:
- if truncate:
- self.DATADICT[pulse][rchan][ipm][istack] = self.DATADICT[pulse][rchan][ipm][istack][0:itrunc]
-
- #percent = (int)(1e2*((float)(iFID*self.DATADICT["nPulseMoments"]+(ipm))/( len(self.DATADICT["PULSES"])*self.nPulseMoments)))
- percent = (int)(1e2*((float)(istack*self.DATADICT["nPulseMoments"]+(ipm))/( len(self.DATADICT["PULSES"])*self.nPulseMoments*(len(self.DATADICT["stacks"])+1) )))
- self.progressTrigger.emit(percent)
-
- # # why is this loop here, istack is not part of rest?
- # for istack in self.DATADICT["stacks"]:
- # if truncate:
- # self.DATADICT[pulse]["TIMES"] = self.DATADICT[pulse]["TIMES"][0:itrunc]
- # percent = (int)(1e2*((float)(iFID*self.DATADICT["nPulseMoments"]+(ipm))/( len(self.DATADICT["PULSES"])*self.nPulseMoments)))
- # self.progressTrigger.emit(percent)
- # iFID += 1
-
- if truncate:
- self.DATADICT[pulse]["TIMES"] = self.DATADICT[pulse]["TIMES"][0:itrunc]
-
- self.doneTrigger.emit()
- self.updateProcTrigger.emit()
-
- #self.plotFT(canvas)
-
- def plotFT(self, canvas, istart=0, iend=0):
-
- try:
- canvas.fig.clear()
- except:
- pass
-
- canvas.ax1 = canvas.fig.add_axes([.1, .1, .65, .8])
- canvas.ax1c = canvas.fig.add_axes([.8, .1, .05, .8])
- canvas.ax1.tick_params(axis='both', which='major', labelsize=8)
-
- for pulse in self.DATADICT["PULSES"]:
- for istack in self.DATADICT["stacks"]:
- for ichan in self.DATADICT[pulse]["chan"]:
- # FFT of stack
- XA = np.zeros((self.DATADICT["nPulseMoments"] , len(self.DATADICT[pulse][ichan][0][istack])/2+1))
- nu = np.fft.fftfreq(self.DATADICT[pulse][ichan][0][istack].size, d=self.dt)
- nu[-1] *= -1
- df = nu[1]
- of = 0
- if istart:
- of = nu[istart]
- def freqlabel(x, pos):
- return '%1.0f' %(of + x*df)
- formatter = FuncFormatter(freqlabel)
- canvas.ax1.clear()
- for ipm in range(self.DATADICT["nPulseMoments"]):
- X = np.fft.rfft(self.DATADICT[pulse][ichan][ipm][istack])
- XA[ipm,:] = np.abs(X)
- if istart:
- mn = canvas.ax1.matshow(20.*np.log10(XA[:,istart:iend+1]), aspect='auto', vmax=-40, vmin=-120) #, norm=LogNorm())
- else:
- mn = canvas.ax1.matshow(20.*np.log10(XA), aspect='auto', vmax=-40, vmin=-120) #, norm=LogNorm())
- smin = np.min(20.*np.log10(XA))
- smax = np.max(20.*np.log10(XA))
- canvas.ax1.xaxis.set_major_formatter(formatter)
- cb1 = mpl.colorbar.Colorbar(canvas.ax1c, mn)
- cb1.ax.tick_params(labelsize=8)
- cb1.set_label("signal [dB]", fontsize=8)
- canvas.ax1.set_xlabel(r"$\nu$ [Hz]", fontsize=10)
- canvas.ax1.set_ylabel(r"$q_{index}$", fontsize=10)
- canvas.draw()
-
- def plotFT(self, canvas, istart=0, iend=0):
-
- try:
- canvas.fig.clear()
- except:
- pass
-
- canvas.ax1 = canvas.fig.add_axes([.1, .1, .65, .8])
- canvas.ax1c = canvas.fig.add_axes([.8, .1, .05, .8])
- canvas.ax1.tick_params(axis='both', which='major', labelsize=8)
-
- for pulse in self.DATADICT["PULSES"]:
- for istack in self.DATADICT["stacks"]:
- for ichan in self.DATADICT[pulse]["chan"]:
- # FFT of stack
- XA = np.zeros((self.DATADICT["nPulseMoments"] , len(self.DATADICT[pulse][ichan][0][istack])//2+1))
- nu = np.fft.fftfreq(self.DATADICT[pulse][ichan][0][istack].size, d=self.dt)
- nu[-1] *= -1
- df = nu[1]
- of = 0
- if istart:
- of = nu[istart]
- def freqlabel(x, pos):
- return '%1.0f' %(of + x*df)
- formatter = FuncFormatter(freqlabel)
- canvas.ax1.clear()
- for ipm in range(self.DATADICT["nPulseMoments"]):
- X = np.fft.rfft(self.DATADICT[pulse][ichan][ipm][istack])
- XA[ipm,:] = np.abs(X)
- if istart:
- mn = canvas.ax1.matshow(20.*np.log10(XA[:,istart:iend+1]), aspect='auto', vmax=-40, vmin=-120, cmap='viridis') #, norm=LogNorm())
- else:
- mn = canvas.ax1.matshow(20.*np.log10(XA), aspect='auto', vmax=-40, vmin=-120, cmap='viridis') #, norm=LogNorm())
- canvas.ax1.xaxis.set_major_formatter(formatter)
- cb1 = mpl.colorbar.Colorbar(canvas.ax1c, mn)
- cb1.ax.tick_params(labelsize=8)
- cb1.set_label("signal [dB]", fontsize=8)
- canvas.ax1.set_xlabel(r"$\nu$ [Hz]", fontsize=10)
- canvas.ax1.set_ylabel(r"$q_{index}$", fontsize=10)
- canvas.draw()
-
-
- def dataCubeFFT(self):
- """
- Performs FFT on entire cube of DATA, and REFERENCE channels, but not pulse currents,
- Results are saved to a new field in the data structure
-
- The GMR varies phase as a function of pulse moment index, so that the first pusle moment is zero phase,
- the second is pi/2 the third is zero. This method corrects for this, so that all pulse moments are in phase.
-
- Technically we may not want to do this, if there is some system response that this cycles away, and we lose track of
- how many of each cycle we have, could this be problomatic? I think it will come out in the wash as we keep track of the
- rest of the phase cycles. Holy phase cycling batman.
- """
- for pulse in self.DATADICT["PULSES"]:
- for ichan in np.append(self.DATADICT[pulse]["chan"], self.DATADICT[pulse]["rchan"]):
- # FFT of stack
- self.DATADICT[pulse][ichan]["FFT"] = {}
- self.DATADICT[pulse][ichan]["FFT"]["nu"] = np.fft.fftfreq(self.DATADICT[pulse][ichan][0][self.DATADICT["stacks"][0]].size, d=self.dt)
- self.DATADICT[pulse][ichan]["FFT"]["nu"][-1] *= -1
- for istack in self.DATADICT["stacks"]:
- self.DATADICT[pulse][ichan]["FFT"][istack] = np.zeros((self.DATADICT["nPulseMoments"] , len(self.DATADICT[pulse][ichan][0][istack])//2+1), dtype=complex)
- for ipm in range(self.DATADICT["nPulseMoments"]):
- # Mod works for FID pulse sequences, TODO generalize this for 4 phase T1, etc..
- mod = (-1)**(ipm%2) * (-1)**(istack%2)
- self.DATADICT[pulse][ichan]["FFT"][istack][ipm,:] = np.fft.rfft( self.DATADICT[pulse][ichan][ipm][istack] )
- #if ipm%2:
- # odd, phase cycled from previous
- # self.DATADICT[pulse][ichan]["FFT"][istack][ipm,:] = np.fft.rfft(-self.DATADICT[pulse][ichan][ipm][istack])
- #else:
- # even, we define as zero phase, first pulse moment has this
- # self.DATADICT[pulse][ichan]["FFT"][istack][ipm,:] = np.fft.rfft(self.DATADICT[pulse][ichan][ipm][istack])
-
- def adaptiveFilterFD(self, ftype, band, centre, canvas):
-
- try:
- canvas.fig.clear()
- except:
- pass
-
- canvas.ax1 = canvas.fig.add_axes([.1, .5, .7, .4])
- canvas.ax1c = canvas.fig.add_axes([.85, .5, .05, .4])
- canvas.ax1.tick_params(axis='both', which='major', labelsize=8)
- #canvas.ax1.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
-
- canvas.ax2 = canvas.fig.add_axes([.1, .05, .7, .4])
- canvas.ax2c = canvas.fig.add_axes([.85, .05, .05, .4])
- canvas.ax2.tick_params(axis='both', which='major', labelsize=8)
- #canvas.ax2.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
-
- self.dataCubeFFT()
-
- Filt = adapt.AdaptiveFilter(0.)
- for pulse in self.DATADICT["PULSES"]:
- # Compute window function and dimensions
- [WINDOW, nd, wstart, wend, dead] = self.computeWindow(pulse, band, centre, ftype)
- for istack in self.DATADICT["stacks"]:
- for ichan in self.DATADICT[pulse]["chan"]:
- # FFT of stack
- nd = len(self.DATADICT[pulse][ichan][0][istack])
- XX = np.zeros((self.DATADICT["nPulseMoments"] , len(self.DATADICT[pulse][ichan][0][istack])//2+1), dtype=complex)
- nu = np.fft.fftfreq(self.DATADICT[pulse][ichan][0][istack].size, d=self.dt)
- nu[-1] *= -1
- #nu = self.DATADICT[pulse][ichan]["FFT"]["nu"]
- def freqlabel(x, pos):
- return '%1.0f' %((wstart)*nu[1] + x*nu[1])
- formatter = FuncFormatter(freqlabel)
- canvas.ax1.clear()
- for ipm in range(self.DATADICT["nPulseMoments"]):
- X = np.fft.rfft(self.DATADICT[pulse][ichan][ipm][istack])
- XX[ipm,:] = X
-
- XX = XX*WINDOW
- XX = XX[:,wstart:wend]
- smin = np.min(20.*np.log10(np.abs(XX)))
- smax = np.max(20.*np.log10(np.abs(XX)))
- #if smin != smin:
- smax = -40
- smin = -120
- mn = canvas.ax1.matshow(20.*np.log10(np.abs(XX)), aspect='auto', vmin=smin, vmax=smax) #, norm=LogNorm())
-
- canvas.ax1.xaxis.set_major_formatter(formatter)
- cb1 = mpl.colorbar.Colorbar(canvas.ax1c, mn)
-
- RX = []
- for ichan in self.DATADICT[pulse]["rchan"]:
- R = np.zeros((self.DATADICT["nPulseMoments"] , len(self.DATADICT[pulse][ichan][0][istack])//2+1), dtype=complex)
- for ipm in range(self.DATADICT["nPulseMoments"]):
- R[ipm,:] = np.fft.rfft(self.DATADICT[pulse][ichan][ipm][istack])
- RX.append(R[:,wstart:wend])
- XC = Filt.transferFunctionFFT(XX, RX)
-
- # TODO inverse FFT, but we need to map back to origional matrix size
- #for ichan in self.DATADICT[pulse]["chan"]:
- # for ipm in range(self.DATADICT["nPulseMoments"]):
- # self.DATADICT[pulse][ichan][ipm][istack] = np.fft.irfft(XC[] , nd)
- mc = canvas.ax2.matshow(20.*np.log10(np.abs(XC)), aspect='auto', vmin=smin, vmax=smax) #, norm=LogNorm())
- cb2 = mpl.colorbar.Colorbar(canvas.ax2c, mc)
- cmin = np.min(20.*np.log10(np.abs(XC)))
- cmax = np.max(20.*np.log10(np.abs(XC)))
- canvas.ax2.xaxis.set_major_formatter(formatter)
- #canvas.ax2.colorbar(mn)
- canvas.draw()
-
- ##############################3
- # TODO inverse FFT to get the damn data back!!!
- # self.progressTrigger.emit(percent)
- # #label = "iFID="+str(iFID) + " ipm=" + str(ipm) + " istack=" + str(istack) + " ichan=" + str(ichan))
- self.doneTrigger.emit()
-
-
- def findSpikes(self, x, width, threshold, rollOn):
- import scipy.ndimage as im
- spikes = np.zeros( len(x) )
- med = im.median_filter(x, width,mode='nearest')
- std = np.std(x)
- spikes = (np.abs(x-med) > threshold * std)
- return np.array(np.where(spikes[rollOn::])) + rollOn
-
- # def despike(self, width, threshold, itype, rollOn, win, canvas):
- # from scipy import interpolate
- # """ This was a stab at a despike filter. Better results were achieved using the SmartStack approach
- # """
- # try:
- # canvas.fig.clear()
- # except:
- # pass
- #
- # canvas.ax1 = canvas.fig.add_axes([.125,.1,.725,.8])
- # canvas.ax1.tick_params(axis='both', which='major', labelsize=8)
- # canvas.ax1.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
- # iFID = 0
- # for pulse in self.DATADICT["PULSES"]:
- # for ipm in range(self.DATADICT["nPulseMoments"]):
- # for istack in self.DATADICT["stacks"]:
- # canvas.ax1.clear()
- # for ichan in np.append(self.DATADICT[pulse]["chan"], self.DATADICT[pulse]["rchan"]):
- # x = self.findSpikes(self.DATADICT[pulse][ichan][ipm][istack], width, threshold, rollOn)
- # canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], self.DATADICT[pulse][ichan][ipm][istack],
- # label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " ichan=" + str(ichan))
- # canvas.ax1.plot( self.DATADICT[pulse]["TIMES"][x], self.DATADICT[pulse][ichan][ipm][istack][x], '.', color='red' , markersize=6 )
- #
- # FIXED = np.zeros(len(x[0]))
- # ii = 0
- # for spike in np.array(x[0]).tolist():
- # f = interpolate.interp1d(np.delete(self.DATADICT[pulse]["TIMES"][spike-win/2:spike+win/2], x[0]-(spike-win/2)), \
- # np.delete(self.DATADICT[pulse][ichan][ipm][istack][spike-win/2:spike+win/2], x[0]-(spike-win/2)), itype)
- # FIXED[ii] = f(self.DATADICT[pulse]["TIMES"][spike])
- # ii += 1
- # canvas.ax1.plot( self.DATADICT[pulse]["TIMES"][x[0]] , FIXED, '.', color='black' , markersize=4 )
- # self.DATADICT[pulse][ichan][ipm][istack][x[0]] = FIXED
- #
- # canvas.ax1.legend(prop={'size':6})
- # canvas.draw()
- # percent = (int)(1e2*((float)(iFID*self.DATADICT["nPulseMoments"]+(ipm))/( len(self.DATADICT["PULSES"])*self.nPulseMoments)))
- # self.progressTrigger.emit(percent)
- # iFID += 1
- # self.doneTrigger.emit()
-
- def designFilter(self, cf, PB, SB, gpass, gstop, ftype, canvas):
- ''' cf is central frequency
- pb is pass band
- sb is stop band
- '''
- TS = (cf) / (.5/self.dt)
- PB = PB / (.5/self.dt) # 1/2 width pass band Muddy Creek
- SB = SB / (.5/self.dt) # 1/2 width stop band Muddy Creek
- # if butterworth
- #[bord, wn] = signal.buttord([TS-PB,TS+PB], [TS-SB,TS+SB], 1e-1, 5.)
- if ftype=="Butterworth":
- [bord, wn] = signal.buttord([TS-PB,TS+PB], [TS-SB,TS+SB], gpass, gstop)
- [self.filt_b, self.filt_a] = signal.butter(bord, wn, btype='bandpass', output='ba')
- [self.filt_z, self.filt_p, self.filt_k] = signal.butter(bord, wn, btype='band', output='zpk')
- elif ftype == "Chebychev Type II":
- [bord, wn] = signal.cheb2ord([TS-PB,TS+PB], [TS-SB,TS+SB], gpass, gstop)
- [self.filt_b, self.filt_a] = signal.cheby2(bord, gstop, wn, btype='bandpass', output='ba')
- [self.filt_z, self.filt_p, self.filt_k] = signal.cheby2(bord, gstop, wn, btype='band', output='zpk')
- elif ftype == "Elliptic":
- [bord, wn] = signal.ellipord([TS-PB,TS+PB], [TS-SB,TS+SB], gpass, gstop)
- [self.filt_b, self.filt_a] = signal.ellip(bord, gpass, gstop, wn, btype='bandpass', output='ba')
- [self.filt_z, self.filt_p, self.filt_k] = signal.ellip(bord, gpass, gstop, wn, btype='band', output='zpk')
-
- # if cheby2
- impulse = self.mfreqz2(self.filt_b, self.filt_a, canvas)
- self.fe = -5
- for it in range(len(impulse[0])):
- if abs(impulse[1][0][it][0]) >= .1 * gpass:# gpass:
- self.fe = impulse[0][it]
-
- canvas.draw()
- return [bord, self.fe]
-
- def downsample(self, truncate, dec, plot=False, canvas=None):
- """ Downsamples and truncates the raw signal.
- Args
- truncate (float) : the length of the signal to truncate to
- dec (int) : the decimation factor, 1 results in no downsampling
- plot (bool) : perform plots
- canvas : MPL axis for plotting
- """
-
- if plot:
- canvas.reAx2()
- canvas.ax1.set_ylabel(r"signal [nV]", fontsize=8)
- canvas.ax2.set_xlabel(r"time [s]", fontsize=8)
- canvas.ax2.set_ylabel(r"signal [nV]", fontsize=8)
-
- self.samp /= dec
- self.dt = 1./self.samp
-
- iFID = 0
- for pulse in self.DATADICT["PULSES"]:
- RSTIMES = self.DATADICT[pulse]["TIMES"][::dec]
- if truncate:
- itrunc = (int)( 1e-3*truncate*self.samp )
- RSTIMES = RSTIMES[0:itrunc]
- for ipm in range(self.DATADICT["nPulseMoments"]):
- for istack in self.DATADICT["stacks"]:
- if plot:
- canvas.softClear()
- for ichan in np.append(self.DATADICT[pulse]["chan"], self.DATADICT[pulse]["rchan"]):
- # trim off indices that don't divide evenly
- ndi = np.shape(self.DATADICT[pulse][ichan][ipm][istack])[0]%dec
- if ndi:
- #[self.DATADICT[pulse][ichan][ipm][istack], RSTIMES] = signal.resample(self.DATADICT[pulse][ichan][ipm][istack][0:-ndi],\
- # len(self.DATADICT[pulse][ichan][ipm][istack][0:-ndi])//dec,\
- # self.DATADICT[pulse]["TIMES"][0:-ndi], window='hamm')
- self.DATADICT[pulse][ichan][ipm][istack] = signal.decimate(self.DATADICT[pulse][ichan][ipm][istack], dec, n=None, ftype='iir', zero_phase=True)
- else:
- #[self.DATADICT[pulse][ichan][ipm][istack], RSTIMES] = signal.resample(self.DATADICT[pulse][ichan][ipm][istack],\
- # len(self.DATADICT[pulse][ichan][ipm][istack])//dec,\
- # self.DATADICT[pulse]["TIMES"], window='hamm')
- self.DATADICT[pulse][ichan][ipm][istack] = signal.decimate(self.DATADICT[pulse][ichan][ipm][istack], dec, n=None, ftype='iir', zero_phase=True)
- if truncate:
- self.DATADICT[pulse][ichan][ipm][istack] = self.DATADICT[pulse][ichan][ipm][istack][0:itrunc]
-
- if plot:
- for ichan in self.DATADICT[pulse]["chan"]:
- canvas.ax2.plot( RSTIMES, 1e9*self.DATADICT[pulse][ichan][ipm][istack], \
- label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " ichan=" + str(ichan))
- for ichan in self.DATADICT[pulse]["rchan"]:
- canvas.ax1.plot( RSTIMES, 1e9*self.DATADICT[pulse][ichan][ipm][istack], \
- label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " ichan=" + str(ichan))
- canvas.ax1.legend(prop={'size':6}, loc='upper right')
- canvas.ax2.legend(prop={'size':6}, loc='upper right')
- canvas.draw()
- percent = (int)(1e2*((float)(iFID*self.DATADICT["nPulseMoments"]+(ipm))/( len(self.DATADICT["PULSES"])*self.nPulseMoments)))
- self.progressTrigger.emit(percent)
- iFID += 1
- self.DATADICT[pulse]["TIMES"] = RSTIMES
-
- #####################################
- # resample pulse data
- for pulse in self.DATADICT["PULSES"]:
- for ipm in range(self.DATADICT["nPulseMoments"]):
- for istack in self.DATADICT["stacks"]:
- ndi = np.shape(self.DATADICT[pulse]["CURRENT"][ipm][istack])[0]%dec
- if ndi:
- [self.DATADICT[pulse]["CURRENT"][ipm][istack], RSPTIMES] = signal.resample(self.DATADICT[pulse]["CURRENT"][ipm][istack][0:-ndi],\
- len(self.DATADICT[pulse]["CURRENT"][ipm][istack][0:-ndi])//dec,\
- self.DATADICT[pulse]["PULSE_TIMES"][0:-ndi], window='hamm')
- else:
- [self.DATADICT[pulse]["CURRENT"][ipm][istack], RSPTIMES] = signal.resample(self.DATADICT[pulse]["CURRENT"][ipm][istack],\
- len(self.DATADICT[pulse]["CURRENT"][ipm][istack])//dec,\
- self.DATADICT[pulse]["PULSE_TIMES"], window='hamm')
- self.DATADICT[pulse]["PULSE_TIMES"] = RSPTIMES
- self.doneTrigger.emit()
- self.updateProcTrigger.emit()
-
- def computeWindow(self, pulse, band, centre, ftype, canvas=None):
-
- # Compute window
- nd = len(self.DATADICT[pulse][self.DATADICT[pulse]["chan"][0]][0][self.DATADICT["stacks"][0]])
- fft1 = np.fft.rfft(self.DATADICT[pulse][self.DATADICT[pulse]["chan"][0]][0][self.DATADICT["stacks"][0]])
- freqs = np.fft.fftfreq(nd, self.dt)
- df = freqs[1] - freqs[0]
- N = int((round)(band/df))
-
- if ftype == "Hamming":
- window = np.hamming(N)
- elif ftype == "Hanning":
- window = np.hanning(N)
- elif ftype == "Rectangular":
- window = np.ones(N)
- elif ftype == "Flat top":
- window = signal.flattop(N)
- else:
- print ("in windowFilter, window type undefined")
-
- WINDOW = np.zeros(len(fft1))
- ifreq = int(round(centre/df))
- istart = ifreq-len(window)//2
- iend = 0
- if N%2:
- WINDOW[ifreq-N//2:ifreq+N//2+1] = window
- iend = ifreq+N//2+1
- else:
- WINDOW[ifreq-N//2:ifreq+N//2] = window
- iend = ifreq+N//2
-
- self.WINDOW = WINDOW
- self.iWindowStart = istart
- self.iWindowEnd = iend
- self.FFTtimes = nd
-
- fft1 = np.fft.irfft(WINDOW)
- # calculate dead time
- self.windead = 0.
- for ift in np.arange(100,0,-1):
- #print( ift, fft1[ift] )
- if fft1[ift] > .001:
- #print ("DEAD TIME", 1e3*self.DATADICT[pulse]["TIMES"][ift] - 1e3*self.DATADICT[pulse]["TIMES"][0] )
- dead = 1e3*self.DATADICT[pulse]["TIMES"][ift] - 1e3*self.DATADICT[pulse]["TIMES"][0]
- self.windead = self.DATADICT[pulse]["TIMES"][ift] - self.DATADICT[pulse]["TIMES"][0]
- break
-
- if canvas != None:
- canvas.fig.clear()
- canvas.ax1 = canvas.fig.add_axes([.1, .6, .75, .35])
- canvas.ax2 = canvas.fig.add_axes([.1, .1, .75, .35])
- canvas.ax1.plot(WINDOW)
- canvas.ax2.plot( 1e3* self.DATADICT[pulse]["TIMES"][0:100] - 1e3*self.DATADICT[pulse]["TIMES"][0], fft1[0:100] )
- canvas.ax2.set_xlabel("time (ms)")
- canvas.ax2.set_title("IFFT")
- canvas.draw()
-
- return [WINDOW, nd, istart, iend, dead]
-
- def windowFilter(self, ftype, band, centre, canvas):
-
- ###############################
- # Window Filter (Ormsby filter http://www.xsgeo.com/course/filt.htm)
- # apply window
- iFID = 0
- for pulse in self.DATADICT["PULSES"]:
- [WINDOW, nd, istart, iend,dead] = self.computeWindow(pulse, band, centre, ftype)
- for istack in self.DATADICT["stacks"]:
- for ipm in range(self.DATADICT["nPulseMoments"]):
- for ichan in np.append(self.DATADICT[pulse]["chan"], self.DATADICT[pulse]["rchan"]):
- fft = np.fft.rfft( self.DATADICT[pulse][ichan][ipm][istack] )
- fft *= WINDOW
- self.DATADICT[pulse][ichan][ipm][istack] = np.fft.irfft(fft , nd)
-
- percent = (int)(1e2*((float)(iFID*self.DATADICT["nPulseMoments"]+(ipm))/(len(self.DATADICT["PULSES"])*self.nPulseMoments)))
- self.progressTrigger.emit(percent)
- iFID += 1
-
- self.plotFT(canvas, istart, iend)
- self.doneTrigger.emit()
-
- def bandpassFilter(self, canvas, blank, plot=True):
-
- if plot:
- canvas.reAx2()
- canvas.ax1.set_ylabel(r"signal [nV]", fontsize=8)
- canvas.ax2.set_xlabel(r"time [s]", fontsize=8)
- canvas.ax2.set_ylabel(r"signal [nV]", fontsize=8)
-
- ife = (int)( max(self.fe, self.windead) * self.samp )
- # Data
- iFID = 0
- for pulse in self.DATADICT["PULSES"]:
- self.DATADICT[pulse]["TIMES"] = self.DATADICT[pulse]["TIMES"][ife:-ife]
- for ipm in range(self.DATADICT["nPulseMoments"]):
- for istack in self.DATADICT["stacks"]:
- if plot:
- canvas.softClear()
- mmax = 0
- for ichan in self.DATADICT[pulse]["rchan"]:
- canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack][ife:-ife], alpha=.5)
- mmax = max( mmax, np.max(1e9*self.DATADICT[pulse][ichan][ipm][istack][ife:-ife]))
- for ichan in self.DATADICT[pulse]["chan"]:
- canvas.ax2.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack][ife:-ife], alpha=.5)
- mmax = max( mmax, np.max(1e9*self.DATADICT[pulse][ichan][ipm][istack][ife:-ife]))
- canvas.ax2.set_prop_cycle(None)
- canvas.ax1.set_prop_cycle(None)
- canvas.ax1.set_ylim(-mmax, mmax)
-
- for ichan in self.DATADICT[pulse]["rchan"]:
- # reflect signal back on itself to reduce gibbs effects on early times
- #nr = len( self.DATADICT[pulse][ichan][ipm][istack] ) - 1 + ife
- #refl = np.append( -1*self.DATADICT[pulse][ichan][ipm][istack][::-1][0:-1], self.DATADICT[pulse][ichan][ipm][istack] )
- #reflfilt = signal.filtfilt( self.filt_b, self.filt_a, refl )
- #self.DATADICT[pulse][ichan][ipm][istack] = reflfilt[nr:-ife]
-
- # don't reflect
- self.DATADICT[pulse][ichan][ipm][istack] = \
- signal.filtfilt(self.filt_b, self.filt_a, self.DATADICT[pulse][ichan][ipm][istack])[ife:-ife]
-
- # plot
- if plot:
- canvas.ax1.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack], \
- label = pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " rchan=" + str(ichan))
-
- for ichan in self.DATADICT[pulse]["chan"]:
- # reflect signal back on itself to reduce gibbs effects on early times
- #nr = len( self.DATADICT[pulse][ichan][ipm][istack] ) - 1 + ife
- #refl = np.append( -1*self.DATADICT[pulse][ichan][ipm][istack][::-1][0:-1], self.DATADICT[pulse][ichan][ipm][istack] )
- #reflfilt = signal.filtfilt( self.filt_b, self.filt_a, refl )
- #self.DATADICT[pulse][ichan][ipm][istack] = reflfilt[nr:-ife]
-
- # don't reflect
- self.DATADICT[pulse][ichan][ipm][istack] = \
- scipy.signal.filtfilt(self.filt_b, self.filt_a, self.DATADICT[pulse][ichan][ipm][istack])[ife:-ife]
-
- # plot
- if plot:
- canvas.ax2.plot( self.DATADICT[pulse]["TIMES"], 1e9*self.DATADICT[pulse][ichan][ipm][istack], \
- label = "data " + pulse + " ipm=" + str(ipm) + " istack=" + str(istack) + " chan=" + str(ichan))
-
- if plot:
- canvas.ax1.legend(prop={'size':6}, loc='upper right')
- canvas.ax2.legend(prop={'size':6}, loc='upper right')
- canvas.draw()
-
- percent = (int)(1e2*((float)(iFID*self.DATADICT["nPulseMoments"]+(ipm))/(len(self.DATADICT["PULSES"])*self.nPulseMoments)))
- self.progressTrigger.emit(percent)
- iFID += 1
- self.doneTrigger.emit()
- self.updateProcTrigger.emit()
-
- def loadGMRBinaryFID( self, rawfname, istack ):
- """ Reads a single binary GMR file and fills into DATADICT
- """
-
- #################################################################################
- # figure out key data indices
- # Pulse
- nps = (int)((self.prePulseDelay)*self.samp)
- npul = (int)(self.pulseLength[0]*self.samp) #+ 100
-
- # Data
- nds = nps+npul+(int)((self.deadTime)*self.samp); # indice pulse 1 data starts
- nd1 = (int)(1.*self.samp) # samples in first pulse
-
- invGain = 1./self.RxGain
- invCGain = self.CurrentGain
-
- pulse = "Pulse 1"
- chan = self.DATADICT[pulse]["chan"]
- rchan = self.DATADICT[pulse]["rchan"]
-
- rawFile = open( rawfname, 'rb')
-
- for ipm in range(self.nPulseMoments):
- buf1 = rawFile.read(4)
- buf2 = rawFile.read(4)
-
- N_chan = struct.unpack('>i', buf1 )[0]
- N_samp = struct.unpack('>i', buf2 )[0]
-
- T = N_samp * self.dt
- TIMES = np.arange(0, T, self.dt) - .0002 # small offset in GMR DAQ?
-
- DATA = np.zeros([N_samp, N_chan+1])
- for ichan in range(N_chan):
- DATADUMP = rawFile.read(4*N_samp)
- for irec in range(N_samp):
- DATA[irec,ichan] = struct.unpack('>f', DATADUMP[irec*4:irec*4+4])[0]
-
- # Save into Data Cube
- for ichan in chan:
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:,eval(ichan)+3][nds:nds+nd1] * invGain
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
- self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] = DATA[:,1][nps:nps+npul] * invCGain
- self.DATADICT["Pulse 1"]["PULSE_TIMES"] = TIMES[nps:nps+npul]
-
- # reference channels?
- for ichan in rchan:
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:,eval(ichan)+3][nds:nds+nd1] * invGain
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
-
- def loadGMRASCIIFID( self, rawfname, istack ):
- """Based on the geoMRI instrument manufactured by VistaClara. Imports
- a suite of raw .lvm files with the following format (on one line)
-
- time(s) DC_Bus/100(V) Current+/75(A) Curr-/75(A) Voltage+/200(V) \
- Ch1(V) Ch2(V) Ch3(V) Ch4(V)
-
- Sampling rate is assumed at 50 kHz
- """
- import pandas as pd
- #################################################################################
- # figure out key data indices
- # Pulse
- nps = (int)((self.prePulseDelay)*self.samp)
- npul = (int)(self.pulseLength[0]*self.samp) #+ 100
-
- # Data
- nds = nps+npul+(int)((self.deadTime)*self.samp); # indice pulse 1 data starts
- nd1 = (int)(1.*self.samp) - nds # samples in first pulse
- ndr = (int)(1.*self.samp) # samples in record
-
- invGain = 1./self.RxGain
- invCGain = self.CurrentGain
-
- pulse = "Pulse 1"
- chan = self.DATADICT[pulse]["chan"]
- rchan = self.DATADICT[pulse]["rchan"]
-
- T = 1.5 #N_samp * self.dt
- TIMES = np.arange(0, T, self.dt) - .0002 # small offset in GMR DAQ?
-
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
- self.DATADICT["Pulse 1"]["PULSE_TIMES"] = TIMES[nps:nps+npul]
-
- # pandas is much faster than numpy for io
- #DATA = np.loadtxt(rawfname)
- DATA = pd.read_csv(rawfname, header=None, sep="\t").values
- for ipm in range(self.nPulseMoments):
- for ichan in np.append(chan,rchan):
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:, eval(ichan)+4][nds:(nds+nd1)] * invGain
- self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] = DATA[:,2][nps:nps+npul] * invCGain
- nds += ndr
- nps += ndr
-
- def loadGMRASCIIT1( self, rawfname, istack ):
- """Based on the geoMRI instrument manufactured by VistaClara. Imports
- a suite of raw .lvm files with the following format (on one line)
-
- time(s) DC_Bus/100(V) Current+/75(A) Curr-/75(A) Voltage+/200(V) \
- Ch1(V) Ch2(V) Ch3(V) Ch4(V)
-
- Sampling rate is assumed at 50 kHz
- """
- import pandas as pd
- #################################################################################
- # figure out key data indices
- # Pulse
- nps = (int)((self.prePulseDelay)*self.samp)
- npul = (int)(self.pulseLength[0]*self.samp) #+ 100
-
- # phase cycling
- # Older T1 GMR data had a curious phase cycling
- npc = 2 #(int)( self.samp / self.transFreq / 6 )
- #print("npc", npc)
-
- # Data
- nds = nps+npul+(int)((self.deadTime)*self.samp); # indice pulse 1 data starts
- nd1 = (int)( (self.interpulseDelay) * self.samp) - nds # samples in first pulse
- ndr = (int)( (self.interpulseDelay) * self.samp) # samples in record
-
- invGain = 1./self.RxGain
- invCGain = self.CurrentGain
-
- pulse = "Pulse 1"
- chan = self.DATADICT[pulse]["chan"]
- rchan = self.DATADICT[pulse]["rchan"]
-
- T = 1.5 #N_samp * self.dt
- TIMES = np.arange(0, T, self.dt) - .0002 # small offset in GMR DAQ?
-
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
- self.DATADICT["Pulse 1"]["PULSE_TIMES"] = TIMES[nps:nps+npul]
-
- # pandas is much faster than numpy for io
- #DATA = np.loadtxt(rawfname)
- DATA = pd.read_csv(rawfname, header=None, sep="\t").values
- for ipm in range(self.nPulseMoments):
- for ichan in np.append(chan,rchan):
- if ipm%2:
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:, eval(ichan)+4][(nds+npc):(nds+nd1+npc)] * invGain
- #self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:, eval(ichan)+4][nds:(nds+nd1)] * invGain
- self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] = DATA[:,2][nps+npc:nps+npul+npc] * invCGain
- else:
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:, eval(ichan)+4][nds:(nds+nd1)] * invGain
- self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] = DATA[:,2][nps:nps+npul] * invCGain
- nds += ndr
- nps += ndr
-
- def loadFIDData(self, base, procStacks, chanin, rchanin, FIDProc, canvas, deadTime, plot):
- '''
- Loads a GMR FID dataset, reads binary and ASCII format files
- '''
-
- canvas.reAx3(True,False)
-
- chan = []
- for ch in chanin:
- chan.append(str(ch))
-
- rchan = []
- for ch in rchanin:
- rchan.append(str(ch))
-
- self.deadTime = deadTime # instrument dead time before measurement
- self.samp = 50000. # in case this is a reproc, these might have
- self.dt = 1./self.samp # changed
-
-
- #################################################################################
- # Data structures
- PULSES = [FIDProc]
- PULSES = ["Pulse 1"]
-
- self.DATADICT = {}
- self.DATADICT["nPulseMoments"] = self.nPulseMoments
- self.DATADICT["stacks"] = procStacks
- self.DATADICT["PULSES"] = PULSES
- for pulse in PULSES:
- self.DATADICT[pulse] = {}
- self.DATADICT[pulse]["chan"] = chan # TODO these should not be a subet of pulse! for GMR all
- self.DATADICT[pulse]["rchan"] = rchan # data are consistent
- self.DATADICT[pulse]["CURRENT"] = {}
- for ichan in np.append(chan,rchan):
- self.DATADICT[pulse][ichan] = {}
- for ipm in range(self.nPulseMoments):
- self.DATADICT[pulse][ichan][ipm] = {}
- self.DATADICT[pulse]["CURRENT"][ipm] = {}
- for istack in procStacks:
- self.DATADICT[pulse][ichan][ipm][istack] = np.zeros(3)
- self.DATADICT[pulse]["CURRENT"][ipm][istack] = np.zeros(3)
-
- ##############################################
- # Read in binary (.lvm) data
- iistack = 0
- for istack in procStacks:
- if self.nDAQVersion <= 1.0:
- try:
- self.loadGMRASCIIFID( base + "_" + str(istack), istack )
- except:
- self.loadGMRASCIIFID( base + "_" + str(istack) + ".lvm", istack )
- elif self.nDAQVersion < 2.3:
- self.loadGMRASCIIFID( base + "_" + str(istack), istack )
- else:
- self.loadGMRBinaryFID( base + "_" + str(istack) + ".lvm", istack )
-
- if plot:
- for ipm in range(self.nPulseMoments):
- canvas.softClear()
-
- for ichan in chan:
- canvas.ax1.plot(self.DATADICT["Pulse 1"]["PULSE_TIMES"], self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] , color='black')
- canvas.ax3.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID data ch. "+str(ichan)) #, color='blue')
-
- for ichan in rchan:
- canvas.ax2.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID ref ch. "+str(ichan)) #, color='blue')
-
- canvas.ax3.legend(prop={'size':6}, loc='upper right')
- canvas.ax2.legend(prop={'size':6}, loc='upper right')
-
- canvas.ax1.set_title("stack "+str(istack)+" pulse index " + str(ipm), fontsize=8)
- canvas.ax1.set_ylabel("Current [A]", fontsize=8)
- canvas.ax1.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
-
- canvas.ax2.set_ylabel("RAW signal [V]", fontsize=8)
- canvas.ax3.set_ylabel("RAW signal [V]", fontsize=8)
- canvas.ax2.tick_params(axis='both', which='major', labelsize=8)
- canvas.ax2.tick_params(axis='both', which='minor', labelsize=6)
- canvas.ax2.set_xlabel("time [s]", fontsize=8)
- canvas.draw()
-
- percent = (int) (1e2*((float)((iistack*self.nPulseMoments+ipm+1)) / (len(procStacks)*self.nPulseMoments)))
- self.progressTrigger.emit(percent)
- iistack += 1
-
- # percent = (int) (1e2*((float)((iistack*self.nPulseMoments+ipm+1)) / (len(procStacks)*self.nPulseMoments)))
- # self.progressTrigger.emit(percent)
- # iistack += 1
-
- self.enableDSP()
- self.doneTrigger.emit()
-
- def loadT1Data(self, base, procStacks, chanin, rchanin, FIDProc, canvas, deadTime, plot):
- '''
- Loads a GMR T1 dataset, reads binary and ASCII format files
- '''
-
- canvas.reAx3(True,False)
-
- chan = []
- for ch in chanin:
- chan.append(str(ch))
-
- rchan = []
- for ch in rchanin:
- rchan.append(str(ch))
-
- # not in any headers but this has changed, NOT the place to do this. MOVE
- #self.prePulseDelay = 0.01 # delay before pulse
- self.deadTime = deadTime # instrument dead time before measurement
- self.samp = 50000. # in case this is a reproc, these might have
- self.dt = 1./self.samp # changed
-
-
- #################################################################################
- # Data structures
- PULSES = [FIDProc]
-
- self.DATADICT = {}
- self.DATADICT["nPulseMoments"] = self.nPulseMoments
- self.DATADICT["stacks"] = procStacks
- self.DATADICT["PULSES"] = PULSES
- for pulse in PULSES:
- self.DATADICT[pulse] = {}
- self.DATADICT[pulse]["chan"] = chan # TODO these should not be a subet of pulse! for GMR all
- self.DATADICT[pulse]["rchan"] = rchan # data are consistent
- self.DATADICT[pulse]["CURRENT"] = {}
- for ichan in np.append(chan,rchan):
- self.DATADICT[pulse][ichan] = {}
- for ipm in range(self.nPulseMoments):
- self.DATADICT[pulse][ichan][ipm] = {}
- self.DATADICT[pulse]["CURRENT"][ipm] = {}
- for istack in procStacks:
- self.DATADICT[pulse][ichan][ipm][istack] = np.zeros(3)
- self.DATADICT[pulse]["CURRENT"][ipm][istack] = np.zeros(3)
-
- ##############################################
- # Read in binary (.lvm) data
- iistack = 0
- fnames = []
- for istack in procStacks:
- if self.nDAQVersion < 2.3:
- #rawfname = base + "_" + str(istack)
- #self.loadGMRASCIIFID( base + "_" + str(istack), istack )
- self.loadGMRASCIIT1( base + "_" + str(istack), istack )
- else:
- self.loadGMRBinaryFID( base + "_" + str(istack) + ".lvm", istack )
- #fnames.append( base + "_" + str(istack) + ".lvm" )
-
- percent = (int) (1e2*((float)((iistack*self.nPulseMoments+ipm+1)) / (len(procStacks)*self.nPulseMoments)))
- self.progressTrigger.emit(percent)
- iistack += 1
-
- # multiprocessing load data
- #info = {}
- #info["prePulseDelay"] = self.prePulseDelay
- #info["samp"] = self.samp
- #with multiprocessing.Pool() as pool:
- # results = pool.starmap( xxloadGMRBinaryFID, ( fnames, zip(itertools.repeat(info)) ) )
- # Plotting
-
- if plot:
- iistack = 0
- for istack in procStacks:
- #for ipm in range(0,7,1):
- for ipm in range(self.nPulseMoments):
- canvas.ax1.clear()
- canvas.ax2.clear()
- canvas.ax3.clear()
- #canvas.fig.patch.set_facecolor('blue')
- for ichan in chan:
- canvas.ax1.plot(self.DATADICT["Pulse 1"]["PULSE_TIMES"], self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] , color='black')
- canvas.ax3.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID data ch. "+str(ichan)) #, color='blue')
-
- for ichan in rchan:
- canvas.ax2.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID ref ch. "+str(ichan)) #, color='blue')
-
- canvas.ax3.legend(prop={'size':6}, loc='upper right')
- canvas.ax2.legend(prop={'size':6}, loc='upper right')
-
- canvas.ax1.set_title("stack "+str(istack)+" pulse index " + str(ipm), fontsize=8)
- canvas.ax1.set_xlabel("time [s]", fontsize=8)
- canvas.ax1.set_ylabel("Current [A]", fontsize=8)
- canvas.ax1.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
-
- canvas.ax2.set_ylabel("RAW signal [V]", fontsize=8)
- canvas.ax2.tick_params(axis='both', which='major', labelsize=8)
- canvas.ax2.tick_params(axis='both', which='minor', labelsize=6)
- canvas.ax2.set_xlabel("time [s]", fontsize=8)
- canvas.ax2.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
- canvas.ax3.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
- canvas.draw()
- #canvas.draw()
-
- percent = (int) (1e2*((float)((iistack*self.nPulseMoments+ipm+1)) / (len(procStacks)*self.nPulseMoments)))
- self.progressTrigger.emit(percent)
- iistack += 1
-
- self.enableDSP()
- self.doneTrigger.emit()
-
- def load4PhaseT1Data(self, base, procStacks, chan, rchan, FIDProc, canvas, deadTime, plot):
-
- """
- Designed to load GMR 4-phase data which use the following convention for phase cycles
- P1 P2
- Stack 1 -> 0 0 <-- <--
- Stack 2 -> 0 pi/2 | <-- <--
- Stack 3 -> pi/2 0 <-- | <--
- Stack 4 -> pi/2 pi/2 <-- <--
- The cycle is determined by stack indice. Walbrecker proposes for pulse2 data (Stack2 - Stack1) / 2
- equivalently (Stack 4 - Stack3) will yield the same voltage response wrt. the second pulse.
- Alternatively Stack 4 can be converted to be aligned with Stack 1 by negating, and Stack 3 Can be aligned with Stack 2 by negating
- Then there are just the two phase cycles that can be stacked like normal.
- Unfortunately, we need to stack each cycle first, then perform corrections for phase cycling. The reason for this is that otherwise,
- the entire point is lost, as the signal that is desired to be cancelled out may not be balanced evenly across the stacks. That is to say,
- if there is an uneven number of a certain phase cycle.
-
- We could, I suppose impose this condition, but I think I would rather not?
- + more samples for std. deviation calculation
- + single spikes will have less residual effect
- - can no longer do normality tests etc. and remove data that are suspect.
- - requires a dumb stack, and may also require removal of entire stacks of data
-
- Additonally, the GMR varies phase as a function of pulse moment index, so that the first pusle moment is zero phase, the second is pi/2 the third is zero ...
- This however, is altered by the above convention. It gets a little complicated...
- """
-
- import struct
- canvas.reAx3()
-
- # not in any headers but this has changed, NOT the place to do this. MOVE
- self.prePulseDelay = 0.01 # delay before pulse
- self.deadTime = deadTime # instrument dead time before measurement
- self.samp = 50000. # in case this is a reproc, these might have
- self.dt = 1./self.samp # changed
- invGain = 1./self.RxGain
- invCGain = self.CurrentGain
-
- #################################################################################
- # figure out key data indices
- # Pulse
- nps = (int)((self.prePulseDelay)*self.samp)
- nps2 = (int)((self.prePulseDelay+self.interpulseDelay)*self.samp)
- npul = (int)(self.pulseLength[0]*self.samp) #+ 100
- np2 = (int)(self.pulseLength[1]*self.samp) #+ 100
-
- # Data
- nds = nps+npul+(int)((self.deadTime)*self.samp); # indice pulse 1 data starts
- nd1 = (int)((self.interpulseDelay)*self.samp) # samples in first pulse
-
- nd2s = nps+npul+nd1+(int)((self.deadTime)*self.samp); # indice pulse 2 data starts
- nd2 = (int)((1.)*self.samp) # samples in first pulse
- nd1 -= (int)((.028)*self.samp) + nps # some time to get ready for next pulse
-
- #################################################################################
- # Data structures
- PULSES = [FIDProc]
- if FIDProc == "Both":
- PULSES = ["Pulse 1","Pulse 2"]
-
- self.DATADICT = {}
- self.DATADICT["nPulseMoments"] = self.nPulseMoments
- self.DATADICT["stacks"] = procStacks
- self.DATADICT["PULSES"] = PULSES
- for pulse in PULSES:
- self.DATADICT[pulse] = {}
- self.DATADICT[pulse]["chan"] = chan
- self.DATADICT[pulse]["rchan"] = rchan
- self.DATADICT[pulse]["CURRENT"] = {}
- for ichan in np.append(chan,rchan):
- self.DATADICT[pulse][ichan] = {}
- for ipm in range(self.nPulseMoments):
- self.DATADICT[pulse][ichan][ipm] = {}
- self.DATADICT[pulse]["CURRENT"][ipm] = {}
- for istack in procStacks:
- self.DATADICT[pulse][ichan][ipm][istack] = np.zeros(3)
- self.DATADICT[pulse]["CURRENT"][ipm][istack] = np.zeros(3)
-
- ##############################################
- # Read in binary data
- iistack = 0
- for istack in procStacks:
- rawFile = open(base + "_" + str(istack) + ".lvm", 'rb')
- for ipm in range(self.nPulseMoments):
-
- N_chan = struct.unpack('>i', rawFile.read(4))[0]
- N_samp = struct.unpack('>i', rawFile.read(4))[0]
-
- T = N_samp * self.dt
- TIMES = np.arange(0, T, self.dt) - .0002 # small offset in GMR DAQ?
-
- DATA = np.zeros([N_samp, N_chan+1])
- for ichan in range(N_chan):
- DATADUMP = rawFile.read(4*N_samp)
- for irec in range(N_samp):
- DATA[irec,ichan] = struct.unpack('>f', DATADUMP[irec*4:irec*4+4])[0]
- if plot:
- #canvas.ax1.clear()
- #canvas.ax2.clear()
- canvas.softClear()
- li = np.shape( DATA[:,4][nd2s:nd2s+nd2] )[0]
-
- ######################################
- # save into DATA cube
- # TODO, changing iFID to 'Pulse 1' or 'Pulse 2'
- for ichan in chan:
- if FIDProc == "Pulse 1":
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:,ichan+3][nds:nds+nd1] * invGain
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
- self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] = DATA[:,1][nps:nps+npul] * invCGain
- self.DATADICT["Pulse 1"]["PULSE_TIMES"] = TIMES[nps:nps+npul]
- if plot:
- canvas.ax3.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID data ch. "+str(ichan)) #, color='blue')
- canvas.ax1.plot(self.DATADICT["Pulse 1"]["PULSE_TIMES"], self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] , color='black')
- elif FIDProc == "Pulse 2":
- print("TODO fix y scale")
- self.DATADICT["Pulse 2"][ichan][ipm][istack] = DATA[:,ichan+3][nd2s:nd2s+nd2] *invGain
- self.DATADICT["Pulse 2"]["TIMES"] = TIMES[nd2s:nd2s+nd2]
- self.DATADICT["Pulse 2"]["CURRENT"][ipm][istack] = DATA[:,1][nps2:nps2+np2] * invCGain
- self.DATADICT["Pulse 2"]["PULSE_TIMES"] = TIMES[nps2:nps2+np2]
- if plot:
- canvas.ax3.plot(self.DATADICT["Pulse 2"]["TIMES"], self.DATADICT["Pulse 2"][ichan][ipm][istack], label="Pulse 2 FID data ch. "+str(ichan)) #, color='blue')
- canvas.ax1.plot( self.DATADICT["Pulse 2"]["PULSE_TIMES"], self.DATADICT["Pulse 2"]["CURRENT"][ipm][istack], color='black' )
- else:
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:,ichan+3][nds:nds+nd1] * invGain
- self.DATADICT["Pulse 2"][ichan][ipm][istack] = DATA[:,ichan+3][nd2s:nd2s+nd2] * invGain
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
- self.DATADICT["Pulse 2"]["TIMES"] = TIMES[nd2s:nd2s+nd2]
- self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] = DATA[:,1][nps:nps+npul] * invCGain
- self.DATADICT["Pulse 1"]["PULSE_TIMES"] = TIMES[nps:nps+npul]
- self.DATADICT["Pulse 2"]["CURRENT"][ipm][istack] = DATA[:,1][nps2:nps2+np2] * invCGain
- self.DATADICT["Pulse 2"]["PULSE_TIMES"] = TIMES[nps2:nps2+np2]
- if plot:
- canvas.ax3.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID data ch. "+str(ichan)) #, color='blue')
- canvas.ax3.plot(self.DATADICT["Pulse 2"]["TIMES"], self.DATADICT["Pulse 2"][ichan][ipm][istack], label="Pulse 2 FID data ch. "+str(ichan)) #, color='blue')
- canvas.ax1.plot( self.DATADICT["Pulse 1"]["PULSE_TIMES"], self.DATADICT["Pulse 1"]["CURRENT"][ipm][istack] , color='black' )
- canvas.ax1.plot( self.DATADICT["Pulse 2"]["PULSE_TIMES"], self.DATADICT["Pulse 2"]["CURRENT"][ipm][istack] , color='black')
-
- for ichan in rchan:
- if FIDProc == "Pulse 1":
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:,ichan+3][nds:nds+nd1] * invGain
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
- if plot:
- canvas.ax2.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID ref ch. "+str(ichan)) #, color='blue')
- elif FIDProc == "Pulse 2":
- self.DATADICT["Pulse 2"][ichan][ipm][istack] = DATA[:,ichan+3][nd2s:nd2s+nd2] * invGain
- self.DATADICT["Pulse 2"]["TIMES"] = TIMES[nd2s:nd2s+nd2]
- if plot:
- canvas.ax2.plot(self.DATADICT["Pulse 2"]["TIMES"], self.DATADICT["Pulse 2"][ichan][ipm][istack], label="Pulse 2 FID ref ch. "+str(ichan)) #, color='blue')
- else:
- self.DATADICT["Pulse 1"][ichan][ipm][istack] = DATA[:,ichan+3][nds:nds+nd1] * invGain
- self.DATADICT["Pulse 2"][ichan][ipm][istack] = DATA[:,ichan+3][nd2s:nd2s+nd2] * invGain
- self.DATADICT["Pulse 1"]["TIMES"] = TIMES[nds:nds+nd1]
- self.DATADICT["Pulse 2"]["TIMES"] = TIMES[nd2s:nd2s+nd2]
- if plot:
- canvas.ax2.plot(self.DATADICT["Pulse 1"]["TIMES"], self.DATADICT["Pulse 1"][ichan][ipm][istack], label="Pulse 1 FID ref ch. "+str(ichan)) #, color='blue')
- canvas.ax2.plot(self.DATADICT["Pulse 2"]["TIMES"], self.DATADICT["Pulse 2"][ichan][ipm][istack], label="Pulse 2 FID ref ch. "+str(ichan)) #, color='blue')
-
- if plot:
- canvas.ax3.legend(prop={'size':6}, loc='upper right')
- canvas.ax2.legend(prop={'size':6}, loc='upper right')
- canvas.ax1.set_title("stack "+str(istack)+" pulse index " + str(ipm), fontsize=8)
- canvas.ax1.set_xlabel("time [s]", fontsize=8)
- canvas.ax3.set_ylabel("RAW signal [V]", fontsize=8)
- canvas.ax2.set_ylabel("RAW signal [V]", fontsize=8)
- canvas.ax1.set_ylabel("Current [A]", fontsize=8)
- #canvas.ax2.tick_params(axis='both', which='major', labelsize=8)
- #canvas.ax2.tick_params(axis='both', which='minor', labelsize=6)
- #canvas.ax2.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
- #canvas.ax1.ticklabel_format(style='sci', scilimits=(0,0), axis='y')
-
- canvas.draw()
-
- # update GUI of where we are
- percent = (int) (1e2*((float)((iistack*self.nPulseMoments+ipm+1)) / (len(procStacks)*self.nPulseMoments)))
- self.progressTrigger.emit(percent)
- iistack += 1
-
- self.enableDSP()
- self.doneTrigger.emit()
-
-
- if __name__ == "__main__":
-
- if len(sys.argv) < 4:
- print( "mrsurvey path/to/header <stack1> <stackN> ")
- exit()
-
- GMR = GMRDataProcessor()
- GMR.readHeaderFile(sys.argv[1])
- GMR.Print()
-
- if GMR.pulseType == "FID":
- GMR.loadFIDData(sys.argv[1], sys.argv[2], sys.argv[3], 5)
-
- if GMR.pulseType == "4PhaseT1":
- GMR.load4PhaseT1Data(sys.argv[1], sys.argv[2], sys.argv[3], 5)
-
- pylab.show()
|