def doRamseyRun(hspace, params, dec):
tdelay = np.linspace(0,5000,500)
YR = np.zeros([len(tdelay),hspace.dimensions], np.complex64)
pop = np.zeros([len(tdelay),hspace.dimensions], np.complex64)
widgets = [progbar.Percentage(), ' ', progbar.Bar(),' ', progbar.ETA()]
pbar = progbar.ProgressBar(widgets=widgets).start()
for i in range(len(tdelay)):
pulseseq = sim.PulseSequence( [ \
sim.Rcar(params, pi/2, 0), \
sim.Delay(params, tdelay[i]), \
sim.Rcar(params, pi/2, pi/2) \
] )
data = qc.simulateevolution(pulseseq, params, dec)
YR[i,:] = data.YR[-1,:]
pbar.update(int(1.*(i+1)*100/(len(tdelay))))
data1 = sim.database(tdelay, YR, hspace, pulseseq=None, statesvalid = False)
data1.tracedpopulation(0)
[fitfun, par] = doRamseyFit(data1)
return data1, fitfun, par
def test_heating_detailed(figNum):
NumberOfIons = 1
NumberofPhonons = 10
hspace = sim.hspace(NumberOfIons, 2, NumberofPhonons, 0)
params = sim.parameters(hspace)
dec = sim.decoherence(params)
# since data.RhoPNAll doesn't save phonons, we'll have to simulate sequentially
numRuns = 5
phonons = np.zeros(numRuns)
dec.doRandNtimes = 1
dec.dict['heating'] = True
dec.progbar = False
params.progbar = False
params.heatingrate = 250
maxDelay = 1000
pulseseq = sim.PulseSequence( [ \
sim.Delay(params, maxDelay), \
] )
widgets = [progbar.Percentage(), ' ', progbar.Bar(), ' ', progbar.ETA()]
pbar = progbar.ProgressBar(widgets=widgets).start()
for i in range(numRuns):
data = qc.simulateevolution(pulseseq, params, dec)
phonons[i] = qc.indexToState(np.nonzero(data.Yend)[0][0], hspace)[0]
pbar.update(int(1. * (i + 1) * 100 / numRuns))
epsilon = np.abs(maxDelay / params.heatingrate - np.mean(phonons))
return epsilon < 2 * np.std(phonons) # allow 2 sigma deviation
def test_dephasing_detailed(figNum):
NumberOfIons = 1
NumberofPhonons = 0
hspace = sim.hspace(NumberOfIons, 2, NumberofPhonons, 0)
params = sim.parameters(hspace)
dec = sim.decoherence(params)
params.coherenceTime = 1000
params.correlationTime = 0.1
dec.doRandNtimes = 20
dec.dict['dephase'] = True
dec.progbar = False
params.stepsize = 10
params.ODEtimestep = 1
params.detuning = 2 * pi * 0.01 #kHz
params.progbar = False
#dec.doPP = True
#params.use_servers(['local'])
#dec.doPPprintstats = False
tdelay = np.linspace(0, 1000, 100)
YR = np.zeros([len(tdelay), hspace.dimensions], np.complex64)
pop = np.zeros([len(tdelay), hspace.dimensions], np.complex64)
widgets = [progbar.Percentage(), ' ', progbar.Bar(), ' ', progbar.ETA()]
pbar = progbar.ProgressBar(widgets=widgets).start()
for i in range(len(tdelay)):
pulseseq = sim.PulseSequence( [ \
sim.Rcar(params, pi/2, 0), \
sim.Delay(params, tdelay[i]), \
sim.Rcar(params, pi/2, pi/2) \
] )
data = qc.simulateevolution(pulseseq, params, dec)
YR[i, :] = data.YR[-1, :]
pbar.update(int(1. * (i + 1) * 100 / (len(tdelay))))
data1 = sim.database(tdelay, YR, hspace, pulseseq=None, statesvalid=False)
data1.tracedpopulation(figNum)
# fitting part
p0 = [0.5, params.detuning, pi / 2, 0.5, params.coherenceTime]
fitfun = lambda p, x: p[0] * np.cos(p[1] * x + p[2]) * np.exp(-np.log(
2) * (x / p[4])**2) + p[3]
errfun = lambda p, x, y: y - fitfun(p, x)
x = data1.T
y = data1.YR[:, 0]
par, covmat, infodict, mesg, ier = leastsq(errfun,
p0,
args=(x, y),
full_output=True)
epsilon = 100 # with 20 iterations allow 100us offset in coherence time
#print(par)
return data1
def parity(data, params):
''' check the parity of the pi/2 MS gate.
must run expMS first. call: parity(data.Yend) '''
phase = np.linspace(0, 2 * pi, 20)
params.y0 = data.Yend
P_PMT = data.P_PMT
parity = np.zeros(len(phase))
params.printpulse = False
dec = sim.decoherence(params)
widgets = [progbar.Percentage(), ' ', progbar.Bar(), ' ', progbar.ETA()]
pbar = progbar.ProgressBar(widgets=widgets).start()
for i in range(len(phase)):
pulseseq = sim.PulseSequence([sim.Rcar(params, pi / 2, phase[i], -1)])
data = qc.simulateevolution(pulseseq, params, dec)
data.tracedpopulation(0)
parity[i] = data.YtrN[-1, 0] + data.YtrN[-1, 3] - data.YtrN[
-1, 1] - data.YtrN[-1, 2]
pbar.update(int(1. * (i + 1) * 100 / (len(phase))))
def sinefunc(x, a, b):
return -a * np.sin(2 * x) + b
[p, pcov] = spop.curve_fit(sinefunc, phase, parity)
population = P_PMT[-1, 0] + P_PMT[-1, -1]
coherence = abs(p[0])
fidelity = (population + coherence) / 2
xphase = np.linspace(0, 2 * pi, 200)
parityfit = sinefunc(xphase, p[0], p[1])
pl.plot(phase, parity, '.', xphase, parityfit, '-')
pl.xlabel('phase [rad]')
pl.ylabel('parity')
pl.show()
print "population = ", population
print "coherence contrast = ", coherence
print "fidelity = ", fidelity
return phase, parity, pulseseq
def calculateGateFidelityProcTomo(self, ErrorBars=False, ind=None):
''' use proctomo to convert error of gate to fidelity '''
#print "Using ProcTomo to calculate gate fidelity. This may take a while ..."
if ind != None:
indreal = [ind]
if ErrorBars:
indreal = [ind, ind, ind]
elif not ErrorBars:
indreal = [self.error0]
else:
indreal = [self.error0, self.error0max, self.error0min]
result = []
for ind in indreal:
if self.noisetype == 'all':
for noisetype in self.dec.dict_params_static.keys():
self.setNoiseAmp(noisetype, ind)
else:
self.setNoiseAmp(self.noisetype, ind)
if not self.verbose:
widgets = [
progressbar.Percentage(), ' ',
progressbar.Bar(), ' ',
progressbar.ETA()
]
pbar = progressbar.ProgressBar(widgets=widgets).start()
else:
pbar = None
pos = self.gates[0] # only do it once, for now
newpulseseq = sim.PulseSequence(
[copy.deepcopy(self.pulseseq[pos])])
self.pulseseq[pos].UtrAll = []
newpulseseq[0].use_ideal = False
ScanObj = ips.ScanParameter_in_Sequence(
newpulseseq,
self.params,
self.dec,
np.arange(12**self.params.hspace.nuions),
type='ProcTomo',
verbose=self.verbose,
doPP=True,
use_ideal=True,
pbar=pbar)
ScanObj.runScan(batchsize=40)
data_proctom = ScanObj.output_dict['qstates_camera']
chi = proctom.proctomo(data_proctom, 100)
chiId = qproc.Unitary2Chi(newpulseseq[0].Uidtr.conjugate())
result.append(U.jozsafid(chiId, chi))
#print "PT:"
#print np.around(chiId,3)
#print np.around(chi,3) # TEMP
if ind != None and ErrorBars:
result.sort()
result.append(result[0])
result.remove(result[0])
if not ErrorBars:
print self._printGatetype(self.gatetype), ":", np.around(
result[0], 4)
return [result[0], result[0], result[0]]
else:
print self._printGatetype(
self.gatetype) + " : %0.4f + %0.4f - %0.4f" % (np.around(
result[0],
4), np.around(result[1] - result[0],
4), np.around(result[0] - result[2], 4))
return result
hspace = sim.hspace(NumberOfIons,2,NumberofPhonons,0)
hspace.initial_state("thermal", nBar=0.5)
params = sim.parameters(hspace)
dec = sim.decoherence(params)
params.stepsize = 600
detuning = np.arange(-1.2*params.omz, 1.2*params.omz, params.omz/300)
#dets1 = np.arange(-1.1*params.omz, -0.9*params.omz, 2*pi*0.001)
#detc = np.arange(-2*pi*0.1, 2*pi*0.1, 2*pi*0.001)
#dets2 = np.arange(0.9*params.omz, 1.1*params.omz, 2*pi*0.001)
#detuning = np.hstack([ dets1, detc, dets2 ])
YR = np.zeros([len(detuning),hspace.dimensions], np.complex128)
widgets = [progbar.Percentage(), ' ', progbar.Bar(),' ', progbar.ETA()]
pbar = progbar.ProgressBar(widgets=widgets).start()
for i in range(len(detuning)):
params.detuning = detuning[i]
pulseseq = sim.PulseSequence( [ \
sim.Rcar(params, pi/params.eta[0], 0), \
] )
data = qc.simulateevolution(pulseseq, params, dec)
YR[i,:] = data.YR[-1,:]
pbar.update(int(1.*(i+1)*100/(len(detuning))))
data1 = sim.database(detuning, YR, hspace, pulseseq=None, statesvalid = False)
#data1.displaypopulation(1)
data1.tracedpopulation(0)
def simulateevolutionOnce(pulseseq, params, dec):
""" a wrapper for simulationCore, to do randomizing internally
by making changes to parameters and collecting the results """
if dec.doSQL:
sequel.insertSimToDB(pulseseq, params, dec)
# the same time array as in simulationCore
totaltime = pulseseq.totaltime
T = np.append(np.arange(0, totaltime, params.stepsize), totaltime)
if dec.doRandNtimes == 0:
data = simulationCore(pulseseq, params, dec)
else:
k = 0
### addressing error
if dec.dict['all'] or dec.dict['addressing']:
params.set_addressing()
for i in range(len(pulseseq)):
pulseseq[i].targetion = params.addressing[pulseseq[i].ion]
# save the variables we're going to change
addressing_saved = np.copy(params.addressing)
if dec.doPP:
job_server = pp.Server( \
ncpus = params.ppcpus,
ppservers = params.ppservers,
secret = params.ppsecret)
if dec.params.pplog:
### job_server's logger
job_server.logger.setLevel(logging.DEBUG)
# create file handler which logs even debug messages
fh = logging.FileHandler('pp.log')
fh.setLevel(logging.DEBUG)
# create formatter and add it to the handlers
formatter = logging.Formatter(
'%(asctime)s - %(name)s - %(levelname)s - %(message)s')
fh.setFormatter(formatter)
# add the handlers to logger
job_server.logger.addHandler(fh)
#######
if dec.doPPprintstats:
print "Starting PP with", job_server.get_ncpus(), \
"local workers and", params.ppservers
if dec.progbar:
widgets = [
progbar.Percentage(), ' ',
progbar.Bar(), ' ',
progbar.ETA()
]
pbar = progbar.ProgressBar(widgets=widgets).start()
# for now we store all param permutations, but be careful this could get very large!
if dec.doPP:
params_list = []
pulseseq_list = []
dec_list = []
data = None
pulseseq_orig = copy.deepcopy(pulseseq)
while k < dec.doRandNtimes:
#######################
### randomize the parameters
### initialization error
if dec.dict['all'] or dec.dict['initerr']:
rn = np.random.uniform()
r_qubit = int(
np.floor(np.random.uniform(0, params.hspace.nuions)))
if rn < params.stateiniterr * params.hspace.nuions:
#print " init error on ion ", r_qubit
params.addressing[:, r_qubit] = 0
# propagate addressing matrix to the pulses
for i in range(len(pulseseq)):
pulseseq[i].targetion = params.addressing[pulseseq[i].ion]
### spectator mode coupling, as initialized intensity shift
if dec.dict['all'] or dec.dict['specmode']:
rn = 1 + np.random.normal(scale=params.specmodecoupling)
params.addressing = params.addressing * rn
for i in range(len(pulseseq)):
pulseseq[i].targetion = params.addressing[pulseseq[i].ion]
### dephasing as offset in the pulse phase
if dec.dict['phaseoffset']:
phasenoise = np.random.normal(scale=params.phaseOffset,
size=len(pulseseq))
for i in range(len(pulseseq)):
pulseseq[i].phase = pulseseq_orig[i].phase + phasenoise[i]
### dephasing
if dec.dict['all'] or dec.dict['dephase']:
dec.calcDephasing(T, params.stepsize)
if len(pulseseq) != 0:
### spontaneous decay
if dec.dict['all'] or dec.dict['spontdecay']:
stepsize = min(params.stepsize,
pulseseq.totaltime / len(pulseseq))
dec.calcSpontaneousDecay(T, stepsize, dec.params.lifetime,
params.hspace.nuions)
### heating
if dec.dict['all'] or dec.dict['heating']:
stepsize = min(params.stepsize,
pulseseq.totaltime / len(pulseseq))
dec.calcHeating(T, stepsize, dec.params.heatingrate)
### intensity fluct
if dec.dict['all'] or dec.dict['intensity']:
stepsize = min(params.stepsize,
pulseseq.totaltime / len(pulseseq))
dec.calcIntensFluct(T, stepsize, dec.params.intensityfluct)
#######################
### do it
if not dec.doPP:
data1 = simulationCore(pulseseq, params, dec)
else:
pulseseq_list.append(copy.deepcopy(pulseseq))
params_list.append(copy.deepcopy(params))
dec_list.append(copy.deepcopy(dec))
#######################
### collect the results
# may have to adjust shape of result vector
if not dec.doPP:
if k == 0:
data = data1
else:
try:
data += data1
except ValueError:
print "adding data failed, abandoning this instance"
continue
### initialization error
# restore variables and increment counter
if dec.dict['all'] or dec.dict['initerr'] or dec.dict['specmode']:
params.addressing = np.copy(addressing_saved)
k += 1
### update progressbar
if dec.progbar and (not dec.doPP):
pbar.update(int(1. * k * 100 / (dec.doRandNtimes)))
if dec.doPP:
jobcounter = 0
runs = range(dec.doRandNtimes)
for m in range(
int(np.ceil(dec.doRandNtimes / float(dec.doRandBatch)))):
if m < dec.doRandNtimes:
batch = runs[m * dec.doRandBatch:m * dec.doRandBatch +
dec.doRandBatch]
else:
batch = runs[m * doRandBatch:]
jobs = [job_server.submit(simulationCore, \
args=(pulseseq_list[i], params_list[i], dec_list[i]), \
depfuncs=(), \
modules=('numpy','scipy', 'PyTIQC.core.simtools', \
'PyTIQC.core.qmtools', 'PyTIQC.core.sequel', \
'PyTIQC.tools.progressbar') ) \
for i in batch ]
for job in jobs:
data1 = job()
if data1 == None:
print "simulationCore failed, continuing"
continue
if dec.progbar:
jobcounter += 1
pbar.update(
int(1. * jobcounter * 100 / (dec.doRandNtimes)))
if not data:
data = data1
else:
try:
data += data1
except ValueError:
print "adding data failed, abandoning this instance"
continue
if params.savedata:
saveRun(pulseseq,
params,
dec,
data,
params.savedataname,
clear=False)
# print pp stats
if dec.doPPprintstats:
print "PP server active: ", job_server.get_active_nodes()
job_server.print_stats()
#job_server.logger.removeHandler(fh)
if dec.params.pplog: logging.shutdown()
job_server.destroy()
# do averaging
data.mean(k)
return data
def simulationCore(pulseseq, params, dec):
""" heart of the computation process.
input: pulse sequence, parameters (includes hilbert space def), and decoherence object.
output: a database object containing the time evolution of states.
"""
np = numpy
splg = scipy.linalg
pi = np.pi
qmtools = PyTIQC.core.qmtools
simtools = PyTIQC.core.simtools
# make list of times and state vector
totaltime = pulseseq.totaltime
T = np.append(np.arange(0, totaltime, params.stepsize), totaltime)
Y = np.zeros((len(T), len(params.y0)), np.complex128)
Y[0, :] = params.y0
# initialize indices and temp vars
p0 = 0 # p0 is index to current pulse
t0 = 0 # t0 is index to current time (in data list T)
# tlen is amount of time to compute evolution
ycur = np.mat(Y[0, :]).T # convert to matrix to use *
tcur = 0
pcur = -1
Ucur = 1
# construct the time-dependent omrabi factors
for pulse in pulseseq.seqqc:
pulse.maketimedep(params.shape, params.doMSshapingCorr)
# initialize the hamiltonian and noise objects
ht = qmtools.Hamilton()
ns = qmtools.Noise()
# pre-fetch the noise dictionary
if dec.doRandNtimes > 0:
noise_dict = ns.Noise(params, dec)
noise_total = [[noise_dict['none'][0]], [noise_dict['none'][1]],
[noise_dict['none'][2]]]
for key, [mult, add, uni] in noise_dict.iteritems():
if (dec.dict['all'] or dec.dict[key]): # and not pulse.use_ideal:
noise_total[0].append(mult)
noise_total[1].append(add)
noise_total[2].append(uni)
noise_mult = ns.prodFunctions(noise_total[0])
noise_add = ns.sumFunctions(noise_total[1])
noise_uni = ns.sumFunctions(noise_total[2])
projtimes = np.union1d(T[np.nonzero(dec.heatingV)],
T[np.nonzero(dec.spontdecayV)])
else:
noise_mult = lambda t: 1
noise_add = lambda t: params.hspace.operator_dict['zero']
noise_uni = lambda t: params.hspace.operator_dict['zero']
projtimes = np.array([])
# storage of hidden ions
hiddenions = np.zeros_like(params.addressing[-1])
hiddenionsErr = np.ones_like(params.addressing[-1])
hiddenionsCount = 0
# a classical register to store intermediate measurements
classical_reg = []
if totaltime == 0:
#set Y=y0 if no time for evolution
Y[0, :] = params.y0
else:
### time evolution starts here
while (tcur < totaltime):
### new pulse starts here
pulse = pulseseq.seqqc[p0]
if pcur != p0:
pcur = p0
HTsaved = None
if params.printpulse:
print "Pulse ", p0, ":", pulse
if params.progbar and pulseseq.seqqc[p0].type != 'M':
widgets = [
progressbar.Percentage(), ' ',
progressbar.Bar(), ' ',
progressbar.ETA()
]
pbar = progressbar.ProgressBar(widgets=widgets).start()
#################
# check for hiding. modify hiding matrix, then treat as delay
nuions = params.hspace.nuions
if pulse.type == "H":
hiddenionsCount += 1
if pulse.hide:
hiddenions[nuions - pulse.ion -
1] = params.addressing[-1][pulse.ion]
else:
hiddenions[nuions - pulse.ion - 1] = 0
hiddenionsErr[nuions - pulse.ion -
1] *= params.hidingerr
else:
pulse.targetion[np.nonzero(hiddenions)] = 0
if dec.dict['all'] or dec.dict['hiding']:
# with some probability some ions are "lost" after unhiding
rn = np.random.uniform( size= \
len(np.nonzero(hiddenionsErr-1)[0]) )
for ith, ind in enumerate(
np.nonzero(hiddenionsErr - 1)[0]):
if rn[ith] > hiddenionsErr[np.nonzero(
hiddenionsErr - 1)[0][ith]]:
pulse.targetion[ind] = 0
else:
pulse.targetion = \
np.copy(params.addressing[pulse.ion])
pulse.calculateIdealUnitary(
params,
np.nonzero(hiddenions[::-1])[0])
# check for meas-init. measure and do projection, then treat as delay.
if pulse.type == "I":
if (dec.dict['all'] or dec.dict['hiding']) \
and pulse.incl_hidingerr:
reg = pulse.measure(np.asarray(ycur))
reg[1] += hiddenionsCount * params.hidingMeaserr
reg[0] -= hiddenionsCount * params.hidingMeaserr
classical_reg.append(reg)
else:
classical_reg.append(pulse.measure(np.asarray(ycur)))
Uproj = pulse.Uinit()
U = np.mat(Uproj)
ynew = U * ycur
ynew = ynew / np.sqrt(np.sum(np.power(abs(ynew), 2)))
ycur = ynew
#################
# check for Uideal and skip time evolution if yes
if pulse.use_ideal:
ynew = np.dot(pulse.Uid, ycur)
ycur = ynew
tcur = pulse.endtime
# save data and advance pulse
t0 = np.searchsorted(T, tcur)
if tcur == T[t0]:
Y[t0, :] = np.asarray(ynew.T)
else:
T = np.insert(T, t0, tcur)
[Yn1, Yn2] = np.array_split(Y, [t0])
if len(Yn2) != 0:
Y = np.concatenate([Yn1, np.asarray(ynew.T), Yn2],
axis=0)
else:
Y = np.concatenate([Yn1, np.asarray(ynew.T)], axis=0)
t0 = t0 + 1
p0 = p0 + 1
#################
#### Unitary evolutions
elif not pulse.dotimedepPulse and not params.dotimedep:
assert tcur >= pulse.starttime \
and tcur <= pulse.endtime \
and abs(pulse.starttime + pulse.duration - pulse.endtime) < 0.001 \
and pulse.duration >= 0, \
"Pulse timing not consistent; missing copy.deepcopy?"
tlen = min(
[pulseseq.seqqc[p0].endtime - tcur, T[t0 + 1] - tcur])
[HT, lqc] = ht.Hamiltonian(pulse,
params,
LDApprox=params.LDapproximation)
if not pulse.use_ideal:
HT = noise_mult(tcur) * HT + noise_add(tcur)
lqc = noise_mult(tcur) * lqc + np.diag(noise_add(tcur))
Ugate = splg.expm2(-1j * tlen * HT)
Ulqc1 = np.diag(np.exp(-1j * tcur * lqc))
Ulqc2 = np.diag(np.exp(-1j * (-tlen - tcur) * lqc))
U = np.mat(Ulqc2) * np.mat(Ugate) * np.mat(Ulqc1)
ynew = U * ycur
# normalize in case of jump operators for spontdecay and heating
ynew = ynew / np.sqrt(np.sum(np.power(abs(ynew), 2)))
Ucur = U * Ucur
# extra check for projective unitary (spontdecay, heating)
if dec.doRandNtimes > 0 and np.sum(noise_uni(tcur)) != 0 \
and not pulse.use_ideal:
U = np.mat(noise_uni(tcur))
ynew = U * ycur
ynew = ynew / np.sqrt(np.sum(np.power(abs(ynew), 2)))
ycur = ynew
if abs(ynew[-1])**2 > 0.25:
print "Warning: further heating will exceed phonon space"
ycur = ynew
tcur = tcur + tlen
# if reached data-point, store data and advance time
datasaved = False
if tcur == T[t0 + 1]:
Y[t0 + 1, :] = np.asarray(ynew.T)
t0 = t0 + 1
datasaved = True
if params.printpulse and params.progbar and pulseseq.seqqc[
p0].type != 'M':
pbar.update(int(1.*(tcur-pulseseq.seqqc[p0].starttime)*100 \
/(pulseseq.seqqc[p0].duration)))
# if pulse ended, advance to next pulse (if both then do both)
if tcur == pulseseq.seqqc[p0].endtime:
pulseseq.seqqc[p0].U = np.copy(np.asarray(Ucur))
# save current data if not already saved
if not datasaved:
T = np.insert(T, t0 + 1, tcur)
[Yn1, Yn2] = np.array_split(Y, [t0 + 1])
Y = np.concatenate([Yn1, np.asarray(ynew.T), Yn2],
axis=0)
t0 = t0 + 1
# advance to next pulse
p0 = p0 + 1
Ucur = 1
#################
#### Time-dependent HT: ODE solving
else:
# choose time step depending on detuning
if pulseseq.seqqc[p0].detuning > 2 * pi * 2:
stepduration = min(
2 / (pulseseq.seqqc[p0].detuning / (2 * pi)), 1)
else:
stepduration = params.ODEtimestep
# for MS pulse, check and modify omrabi due to hiding
if pulse.type == "M" and params.doMShidecorr:
nuions = len(pulse.targetion)
activeions = len(np.nonzero(pulse.targetion)[0])
omc_fac = params.MShidecorr[activeions, nuions]
if omc_fac == -1:
print "MS w/ hiding correction factor invalid, ignoring"
else:
pulse.omrabi_b = params.omc_ms * omc_fac
pulse.omrabi_r = params.omc_ms * omc_fac
# set up time-dep Hamiltonian
if pulse.dobichro:
HTblue = ht.Hamiltonian_timedep_complete(
pulse.targetion,
pulse.omrabi_bt,
pulse.phase_light + pulse.phase_rb,
pulse.detuning_b,
params.omz,
params.eta,
params.hspace,
LDApprox=params.LDapproximation)
HTred = ht.Hamiltonian_timedep_complete(
pulse.targetion,
pulse.omrabi_rt,
pulse.phase_light - pulse.phase_rb,
pulse.detuning_r,
params.omz,
params.eta,
params.hspace,
LDApprox=params.LDapproximation)
HTorig = lambda t: HTblue(t) + HTred(t)
else:
HTorig = ht.Hamiltonian_timedep_complete(
pulse.targetion,
pulse.omrabi_t,
pulse.phase,
pulse.detuning,
params.omz,
params.eta,
params.hspace,
LDApprox=params.LDapproximation)
HT = lambda t: noise_mult(t) * HTorig(t) + noise_add(t)
psidot = lambda t, psi: -1j * np.dot(HT(t), psi)
# ycur needs to be cast as a 1d array
solver = qmtools.SEsolver(params.solver)
Tloc = np.array([0.])
Yloc = np.zeros(
[1, len(np.asarray(ycur))]
) # this is to get the dimensions right, but make sure to remove the first row of 0's
if params.progbar:
widgets = [
progressbar.Percentage(), ' ',
progressbar.Bar(), ' ',
progressbar.ETA()
]
pbar = progressbar.ProgressBar(widgets=widgets).start()
else:
pbar = None
# ODE solver
# variable aliases for convenience
pstarttime = pulseseq.seqqc[p0].starttime
pendtime = pulseseq.seqqc[p0].endtime
# first calculate the expected number of datapoints
testtime = np.arange(tcur, pendtime, stepduration)
testtime = np.append(np.delete(testtime, 0), pendtime)
# extra check for projective unitary (spontdecay, heating)
projtimes_cur = projtimes[np.intersect1d( \
np.nonzero(projtimes<pendtime)[0], \
np.nonzero(projtimes>pstarttime)[0]) ]
for tproj in projtimes_cur:
ms_ode = solver(HT, tcur, tproj, stepduration, np.ravel(ycur), \
pbar, pstarttime, pendtime)
Tloc = np.append(Tloc, np.delete(ms_ode.time, 0))
Yloc = np.append(Yloc,
np.delete(ms_ode.y.transpose(), 0,
axis=0),
axis=0)
tcur = tproj
ycur = Yloc[-1, :].T
if dec.doRandNtimes > 0 and np.sum(noise_uni(tcur)) != 0 \
and not pulse.use_ideal:
U = noise_uni(tcur)
ynew = np.dot(U, ycur)
ynew = ynew / np.sqrt(np.sum(np.power(abs(ynew), 2)))
ycur = ynew
if abs(ynew[-1])**2 > 0.25:
print "Warning: further heating will exceed phonon space"
Yloc[-1, :] = np.asarray(ynew.T)
ms_ode = solver(HT, tcur, pendtime, stepduration, np.ravel(ycur), \
pbar, pstarttime, pendtime)
Tloc = np.append(Tloc, np.delete(ms_ode.time, 0))
Yloc = np.append(Yloc,
np.delete(ms_ode.y.transpose(), 0, axis=0),
axis=0)
Tloc = np.delete(Tloc, 0)
Yloc = np.delete(Yloc, 0, axis=0)
# check the length w.r.t. expected length of T vector and remove extras
while len(Tloc) > len(testtime):
for i in range(len(testtime)):
if testtime[i] != Tloc[i]:
Tloc = np.delete(Tloc, i)
Yloc = np.delete(Yloc, i, axis=0)
break
if not params.saveallpoints:
Tloc = [Tloc[-1]]
Yloc = np.array([Yloc[-1]])
# now we put the result into original result array
# first, update the current time and state
tcur = Tloc[-1]
ycur = np.mat(Yloc[-1, :]).T
# find the end of the pulse in the original T list
t1 = np.nonzero(T >= tcur)[0][0]
# only replace point if it's already been calculated
if T[t1] == tcur:
tend = t1 + 1
else: # T[t1] > tcur
tend = t1
# replace the overlapping times in T with Tloc
[Tnew1,
Tnew2] = np.array_split(np.delete(T, range(t0 + 1, tend)),
[t0 + 1])
Tnew = np.concatenate([Tnew1, Tloc, Tnew2])
# mirror with Y and Yloc
[Ynew1, Ynew2
] = np.array_split(np.delete(Y, range(t0 + 1, tend), axis=0),
[t0 + 1])
# seems that concatenate doesn't work on 2d arrays if they're empty
if len(Ynew2) == 0:
Ynew = np.concatenate([Ynew1, Yloc], axis=0)
else:
Ynew = np.concatenate([Ynew1, Yloc, Ynew2], axis=0)
T = Tnew
Y = Ynew
p0 = p0 + 1
t0 = np.nonzero(T >= tcur)[0][0]
data = simtools.database(T,
Y,
params.hspace,
pulseseq,
register=classical_reg)
data.creationtime = params.savedataname # timestamp the data
if dec.doSQL:
sequel.insertJobToDB(data)
# get rid of lambda functions in order to send results back through pp
for pulse in pulseseq.seqqc:
pulse.omrabi_t = 0
pulse.omrabi_bt = 0
pulse.omrabi_rt = 0
return data
