def linear_phys(self,vf,dt):
"""Adds linear ramp to waveform, starts at current last
value and goes to 'vf' in 'dt'"""
if self.lastPhys == None:
msg = "The last physics value is not available\n for this waveform."
msg = msg + "\n\nProgram will be stopped."
errormsg.box('wfm.linear_phys :: ' + self.name, msg)
exit(1)
print "...linear_phys last physical value is = %f" % self.lastPhys
v0 = self.lastPhys
#One could also obtain v0 via conversion, but it is not recommended
#v0=physics.cnv(self.name+"Phys",self.last())
if dt == 0.0:
self.y[ self.y.size -1] = physics.cnv(self.name,vf)
return
N = int(math.floor(dt/self.ss))
hashbase = ''
hashbase = hashbase + self.name
hashbase = hashbase + '%.8f' % vf
hashbase = hashbase + '%.8f' % v0
hashbase = hashbase + '%.8f' % N
hashbase = hashbase + '%.8f' % dt
hashbase = hashbase + rawcalibdat( self.name )
ramphash = seqconf.ramps_dir() + 'linearPhys_' \
+ hashlib.md5( hashbase ).hexdigest()
if not os.path.exists(ramphash) or True:
print '...Making new linearPhys ramp for ' + self.name
x = numpy.linspace( v0 + (vf-v0)/N , vf , N )
ramp = physics.cnv( self.name, x )
#yramp= numpy.array([cnv(self.name,v0 + 1.0*(vf-v0)*(i+1)/N) for i in range(N)])
#if ( numpy.absolute( yramp - ramp ) > 0.0001 ).any():
# print "NOT EQUAL!"
#else:
# print "EQUAL!"
#ramp.tofile(ramphash,sep=',',format="%.4f")
else:
print '...Recycling previously calculated linearPhys ramp for ' + self.name
ramp = numpy.fromfile(ramphash,sep=',')
self.y=numpy.append(self.y, ramp)
self.lastPhys = vf
return
def linear_phys(self, vf, dt):
"""Adds linear ramp to waveform, starts at current last
value and goes to 'vf' in 'dt'"""
if self.lastPhys == None:
msg = "The last physics value is not available\n for this waveform."
msg = msg + "\n\nProgram will be stopped."
errormsg.box('wfm.linear_phys :: ' + self.name, msg)
exit(1)
print "...linear_phys last physical value is = %f" % self.lastPhys
v0 = self.lastPhys
#One could also obtain v0 via conversion, but it is not recommended
#v0=physics.cnv(self.name+"Phys",self.last())
if dt == 0.0:
self.y[self.y.size - 1] = physics.cnv(self.name, vf)
return
N = int(math.floor(dt / self.ss))
hashbase = ''
hashbase = hashbase + self.name
hashbase = hashbase + '%.8f' % vf
hashbase = hashbase + '%.8f' % v0
hashbase = hashbase + '%.8f' % N
hashbase = hashbase + '%.8f' % dt
hashbase = hashbase + rawcalibdat(self.name)
ramphash = seqconf.ramps_dir() + 'linearPhys_' \
+ hashlib.md5( hashbase ).hexdigest()
if not os.path.exists(ramphash) or True:
print '...Making new linearPhys ramp for ' + self.name
x = numpy.linspace(v0 + (vf - v0) / N, vf, N)
ramp = physics.cnv(self.name, x)
#yramp= numpy.array([cnv(self.name,v0 + 1.0*(vf-v0)*(i+1)/N) for i in range(N)])
#if ( numpy.absolute( yramp - ramp ) > 0.0001 ).any():
# print "NOT EQUAL!"
#else:
# print "EQUAL!"
#ramp.tofile(ramphash,sep=',',format="%.4f")
else:
print '...Recycling previously calculated linearPhys ramp for ' + self.name
ramp = numpy.fromfile(ramphash, sep=',')
self.y = numpy.append(self.y, ramp)
self.lastPhys = vf
return
def odt_linear(self,p0,pf,dt):
"""Adds linear ramp to waveform, starts at 'p0'
value and goes to 'pf' in 'dt'
CAREFUL: This uses OdtpowConvert and is only valid for odtpow"""
print "...ODT Linear from %.3f to %.3f" % (p0,pf)
if dt == 0.0:
self.y[ self.y.size -1] = physics.cnv('odtpow', pf)
return
else:
N = int(math.floor(dt/self.ss))
for i in range(N):
self.y=numpy.append(self.y, [ physics.cnv('odtpow', p0 + (pf-p0)*(i+1)/N )])
return
def linear(self,vf,dt,volt=-11): """Adds linear ramp to waveform, starts at current last value and goes to 'vf' in 'dt' CAREFUL: This is linear in voltage, not in phys""" #~ if 'ir' in self.name and 'pow' in self.name: #~ print "%s LINEAR: Conversion flag = %d, vf_in=%f" % (self.name, volt,vf) if volt >= -10.0 and volt <= 10.0: self.lastPhys = None vf=volt elif volt == -11: self.lastPhys = vf vf=physics.cnv(self.name,vf) #~ if 'ir' in self.name and 'pow' in self.name: #~ print "%s LINEAR: Conversion flag = %d, vf_out=%f" % (self.name, volt,vf) v0 = round(self.last(),4) if dt == 0.0: self.y[ self.y.size -1] = vf return else: N = int(math.floor(dt/self.ss)) x = numpy.linspace( 1, N, N) ramp = numpy.around(v0 + (vf-v0)*x/N, decimals=4) self.y = numpy.append( self.y, ramp ) return
def insertlin_cnv(self,vf,dt,start):
"""Inserts a linear ramp (vf,dt) at a time 'start' referenced from
the end of the current sate of the wfm.
start > 0 : appends a hold before doing the ramp
"""
self.lastPhys = vf
vf=physics.cnv(self.name,vf)
if start>0:
self.apppendhold(start-self.ss)
self.y = numpy.append(self.y,[vf])
return
elif -start > self.dt():
exc = "wfm.py: Cannot insert ramp before the beggiging of the waveform"
print exc
raise Exception(exc)
#exit(1)
elif dt > -start:
exc = "wfm.py: Ramp is too long for inserting"
print exc
raise Exception(exc)
#exit(1)
Nstart=int(math.floor(-start/self.ss))
if dt==0. :
N=0
self.y[self.y.size -1 - Nstart]=vf
else:
N=int(math.floor(dt/self.ss))
v0 = self.y[self.y.size -1 - Nstart]
for i in range(N):
self.y[self.y.size - Nstart + i] = v0 + (vf-v0)*(i+1)/N
for i in range( Nstart -N):
self.y[self.y.size - Nstart + N + i] = vf
return
def tanhRise(self,vf,dt,tau,shift):
#print "---> Initializing lattice wave : %s" % self.name
#print "convert.cnv(%.6f) = %.6f" % ( vf, cnv(self.name,vf))
#print "physics.cnv(%.6f) = %.6f" % ( vf, physics.cnv(self.name,vf))
#vf=cnv(self.name,vf)
physf = vf
vf=physics.cnv(self.name,vf)
v0=self.last()
if dt == 0.0:
self.y[ self.y.size -1] = vf
return
else:
N = int(math.floor(dt/self.ss))
print '...Making new tanhRise ramp for ' + self.name + \
' physf=%.3f, vf = %.3f, dt = %.3f, tau = %.2f, shift = %.2f' % (physf,vf, dt, tau, shift)
x=numpy.arange(dt/N,dt+dt/N,dt/N) # arange is half open: [start,stop)
#print '\t x[ 0] =',x[ 0]
#print '\t x[-1] =',x[-1]
#print '\t ss =',self.ss
#print '\tlen(x) =',x.size
#print '\t N =',N
tau = tau*dt
shift = dt/2. + shift*dt/2.
ramp= v0 + (vf-v0)* ( (1+numpy.tanh((x-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) )\
/ ( (1+numpy.tanh((dt-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) )
self.y=numpy.append(self.y, ramp)
return
def tanhRise(self, vf, dt, tau, shift):
#print "---> Initializing lattice wave : %s" % self.name
#print "convert.cnv(%.6f) = %.6f" % ( vf, cnv(self.name,vf))
#print "physics.cnv(%.6f) = %.6f" % ( vf, physics.cnv(self.name,vf))
#vf=cnv(self.name,vf)
physf = vf
vf = physics.cnv(self.name, vf)
v0 = self.last()
if dt == 0.0:
self.y[self.y.size - 1] = vf
return
else:
N = int(math.floor(dt / self.ss))
print '...Making new tanhRise ramp for ' + self.name + \
' physf=%.3f, vf = %.3f, dt = %.3f, tau = %.2f, shift = %.2f' % (physf,vf, dt, tau, shift)
x = numpy.arange(dt / N, dt + dt / N,
dt / N) # arange is half open: [start,stop)
#print '\t x[ 0] =',x[ 0]
#print '\t x[-1] =',x[-1]
#print '\t ss =',self.ss
#print '\tlen(x) =',x.size
#print '\t N =',N
tau = tau * dt
shift = dt / 2. + shift * dt / 2.
ramp= v0 + (vf-v0)* ( (1+numpy.tanh((x-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) )\
/ ( (1+numpy.tanh((dt-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) )
self.y = numpy.append(self.y, ramp)
return
def insertlin_cnv(self, vf, dt, start):
"""Inserts a linear ramp (vf,dt) at a time 'start' referenced from
the end of the current sate of the wfm.
start > 0 : appends a hold before doing the ramp
"""
self.lastPhys = vf
vf = physics.cnv(self.name, vf)
if start > 0:
self.apppendhold(start - self.ss)
self.y = numpy.append(self.y, [vf])
return
elif -start > self.dt():
exc = "wfm.py: Cannot insert ramp before the beggiging of the waveform"
print exc
raise Exception(exc)
#exit(1)
elif dt > -start:
exc = "wfm.py: Ramp is too long for inserting"
print exc
raise Exception(exc)
#exit(1)
Nstart = int(math.floor(-start / self.ss))
if dt == 0.:
N = 0
self.y[self.y.size - 1 - Nstart] = vf
else:
N = int(math.floor(dt / self.ss))
v0 = self.y[self.y.size - 1 - Nstart]
for i in range(N):
self.y[self.y.size - Nstart + i] = v0 + (vf - v0) * (i + 1) / N
for i in range(Nstart - N):
self.y[self.y.size - Nstart + N + i] = vf
return
def linear(self, vf, dt, volt=-11):
"""Adds linear ramp to waveform, starts at current last
value and goes to 'vf' in 'dt'
CAREFUL: This is linear in voltage, not in phys"""
#~ if 'ir' in self.name and 'pow' in self.name:
#~ print "%s LINEAR: Conversion flag = %d, vf_in=%f" % (self.name, volt,vf)
if volt >= -10.0 and volt <= 10.0:
self.lastPhys = None
vf = volt
elif volt == -11:
self.lastPhys = vf
vf = physics.cnv(self.name, vf)
#~ if 'ir' in self.name and 'pow' in self.name:
#~ print "%s LINEAR: Conversion flag = %d, vf_out=%f" % (self.name, volt,vf)
v0 = round(self.last(), 4)
if dt == 0.0:
self.y[self.y.size - 1] = vf
return
else:
N = int(math.floor(dt / self.ss))
x = numpy.linspace(1, N, N)
ramp = numpy.around(v0 + (vf - v0) * x / N, decimals=4)
self.y = numpy.append(self.y, ramp)
return
def follow(self, bfield, detuning):
### Levitation voltage:
###
### Vlev = slope * I + offset
###
### wherer I is the current on the bias coils
### slope and offset have been calibrated and are set below:
slope = 0.0971
offset = -2.7232
if self.ss != bfield.ss:
msg = "ERROR in HFIMG wave: step size does not match the bfield ramp!"
print msg
errormsg.box('hfimg_wave.follow', msg)
exit(1)
print "...Setting ANALOGHFIMG to follow bfield ramp"
bfieldV = numpy.copy(bfield.y)
bfieldG = physics.inv( 'bfield', bfieldV)* 6.8
hfimg0 = -1.*(100.0 + 163.7 - 1.414*bfieldG)
self.y = physics.cnv( 'analogimg', hfimg0 - detuning)
return hfimg0[-1]
def sinhRise(self, vf, dt, tau):
"""Inserts a hyperbolic-sine-like ramp to the waveform.
tau is the ramp scale, it is understood in units of dt
if tau is equal or greater to dt the ramp approaches a
linear ramp
as tau gets smaller than dt the ramp starts to deviate from
linear
a real difference starts to be seen wheh tau = dt/3
from tau=dt/20 it doesn't make a difference to keep making
tau smaller
good values to vary it are tau=dt/20, dt/5, dt/3, dt/2, dt"""
### WARNING: in general the conversion should be done for every point
### i.e. inside of the for loop below.
### This one just does it on the endpoints. It is ok because it is used
### for the magnetic field which has a mostly linear relationship between
### set voltage and current in the coils. But don't use this as an example
### for other things.
self.lastPhys = vf
vf = physics.cnv(self.name, vf)
v0 = self.last()
if dt == 0.0:
self.y[self.y.size - 1] = vf
return
else:
N = int(math.floor(dt / self.ss))
hashbase = ''
hashbase = hashbase + self.name
hashbase = hashbase + '%.8f' % vf
hashbase = hashbase + '%.8f' % v0
hashbase = hashbase + '%.8f' % N
hashbase = hashbase + '%.8f' % dt
hashbase = hashbase + '%.8f' % tau
ramphash = seqconf.ramps_dir() + 'sinhRise_' + hashlib.md5(
hashbase).hexdigest()
if not os.path.exists(ramphash) or True:
print '...Making new sinhRise ramp'
x = numpy.linspace(dt / N, dt, N)
ramp = v0 + (vf - v0) * (x / tau + (x / tau)**3.0 / 6.0) / (
dt / tau + (dt / tau)**3.0 / 6.0)
#ramp.tofile(ramphash,sep=',',format="%.4f")
else:
print '...Recycling previously calculated sinhRise ramp'
ramp = numpy.fromfile(ramphash, sep=',')
self.y = numpy.append(self.y, ramp)
return
def Evap8(self, p0, p1, t1, tau, beta, offset, t2, tau2, smoothdt, duration,scale = 1.0):
"""Evaporation ramp v8 same as v7 with scale"""
if True:
print ""
print "----- EVAPORATION RAMP Version 8-----"
if duration <=0:
return
else:
N=int(round(duration*scale/self.ss))
print '\t...Evap nsteps = ' + str(N)
ramp_phys=numpy.array([])
ramp=numpy.array([])
hashbase = ''
hashbase = hashbase + '%.s' % self.name
hashbase = hashbase + '%.8f' % self.ss
hashbase = hashbase + '%.8f' % duration
hashbase = hashbase + '%.8f' % p0
hashbase = hashbase + '%.8f' % p1
hashbase = hashbase + '%.8f' % t1
hashbase = hashbase + '%.8f' % tau
hashbase = hashbase + '%.8f' % beta
hashbase = hashbase + '%.8f' % offset
hashbase = hashbase + '%.8f' % t2
hashbase = hashbase + '%.8f' % tau2
hashbase = hashbase + '%.8f' % smoothdt
hashbase = hashbase + '%.8f' % scale
ramphash = seqconf.ramps_dir() +'Evap8_' \
+ hashlib.md5( hashbase).hexdigest()
#Here, go ahead and save the trajectory path to the report
gen.save_to_report('EVAP','ramp', ramphash+'_phys')
if not os.path.exists(ramphash) or True:
print '\t...Making new Evap8 ramp'
for xi in range(N):
t = (xi+1)*self.ss/scale
phys = evap.v6(t,p0,p1,t1,tau,beta, offset,t2,tau2,smoothdt)
volt = physics.cnv( 'odtpow', phys)
ramp_phys = numpy.append( ramp_phys, [ phys])
ramp = numpy.append( ramp, numpy.around([ volt],decimals=4))
ramp_phys.tofile(ramphash+'_phys',sep='\n',format="%.4f")
#ramp.tofile(ramphash,sep=',',format="%.4f")
else:
print '\t...Recycling previously calculated Evap8 ramp'
ramp = numpy.fromfile(ramphash,sep=',')
self.y=numpy.append(self.y,ramp)
#This returns the last value of the ramp
print ""
return evap.v6(N*self.ss/scale,p0,p1,t1,tau,beta,offset,t2,tau2,smoothdt)
def sinhRise(self,vf,dt,tau): """Inserts a hyperbolic-sine-like ramp to the waveform. tau is the ramp scale, it is understood in units of dt if tau is equal or greater to dt the ramp approaches a linear ramp as tau gets smaller than dt the ramp starts to deviate from linear a real difference starts to be seen wheh tau = dt/3 from tau=dt/20 it doesn't make a difference to keep making tau smaller good values to vary it are tau=dt/20, dt/5, dt/3, dt/2, dt""" ### WARNING: in general the conversion should be done for every point ### i.e. inside of the for loop below. ### This one just does it on the endpoints. It is ok because it is used ### for the magnetic field which has a mostly linear relationship between ### set voltage and current in the coils. But don't use this as an example ### for other things. self.lastPhys = vf vf=physics.cnv(self.name,vf) v0=self.last() if dt == 0.0: self.y[ self.y.size -1] = vf return else: N = int(math.floor(dt/self.ss)) hashbase = '' hashbase = hashbase + self.name hashbase = hashbase + '%.8f' % vf hashbase = hashbase + '%.8f' % v0 hashbase = hashbase + '%.8f' % N hashbase = hashbase + '%.8f' % dt hashbase = hashbase + '%.8f' % tau ramphash = seqconf.ramps_dir() + 'sinhRise_' + hashlib.md5(hashbase).hexdigest() if not os.path.exists(ramphash) or True: print '...Making new sinhRise ramp' x = numpy.linspace( dt/N, dt, N) ramp = v0 + (vf-v0)*(x/tau+(x/tau)**3.0/6.0)/(dt/tau+(dt/tau)**3.0/6.0) #ramp.tofile(ramphash,sep=',',format="%.4f") else: print '...Recycling previously calculated sinhRise ramp' ramp = numpy.fromfile(ramphash,sep=',') self.y=numpy.append(self.y, ramp) return
def __init__(self,name,val,stepsize,N=1,volt=-11):
"""Initialize the waveform """
self.idnum = time.time()*100
self.name = name
if volt != -11:
val=volt
else:
val=physics.cnv('odtpow', val)
self.y= numpy.array(N*[val])
self.ss=stepsize
def __init__(self, name, val, stepsize, N=1, volt=-11):
"""Initialize the waveform """
self.idnum = time.time() * 100 + 1e3 * numpy.random.randint(0, 1e8)
self.name = name
self.lastPhys = None
if volt != -11:
val = volt
else:
#print "INITIALIZING WFM: %s, val=%f, volt=%f" % (name,val,physics.cnv(self.name,val))
self.lastPhys = val
val = physics.cnv(self.name, val)
self.y = numpy.array(N * [val])
self.ss = stepsize
def __init__(self,name,val,stepsize,N=1,volt=-11): """Initialize the waveform """ self.idnum = time.time()*100 + 1e3*numpy.random.randint(0,1e8) self.name = name self.lastPhys = None if volt != -11: val=volt else: #print "INITIALIZING WFM: %s, val=%f, volt=%f" % (name,val,physics.cnv(self.name,val)) self.lastPhys = val val=physics.cnv(self.name,val) self.y= numpy.array(N*[val]) self.ss=stepsize
def tanhRise(self,vf,dt,tau,shift): #print "---> Initializing lattice wave : %s" % self.name #print "convert.cnv(%.6f) = %.6f" % ( vf, cnv(self.name,vf)) #print "physics.cnv(%.6f) = %.6f" % ( vf, physics.cnv(self.name,vf)) #vf=cnv(self.name,vf) vf=physics.cnv(self.name,vf) v0=self.last() if dt == 0.0: self.y[ self.y.size -1] = vf return else: N = int(math.floor(dt/self.ss)) print '...Making new tanhRise ramp for ' + self.name + \ ' vf = %.2f, dt = %.3f, tau = %.2f, shift = %.2f' % (vf, dt, tau, shift) x=numpy.arange(dt/N,dt,dt/N) tau = tau*dt shift = dt/2. + shift*dt/2. ramp= v0 + (vf-v0)* ( (1+numpy.tanh((x-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) )\ / ( (1+numpy.tanh((dt-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) ) self.y=numpy.append(self.y, ramp) return
def follow(self, bfield):
### Levitation voltage:
###
### Vlev = slope * I + offset
###
### wherer I is the current on the bias coils
### slope and offset have been calibrated and are set below:
## These numbers are now store in physics.py
## slope = 0.0971
## offset = -2.7232
if self.ss != bfield.ss:
msg = "ERROR in GRADIENT wave: step size does not match the bfield ramp!"
print msg
errormsg.box('gradient_wave.follow', msg)
exit(1)
print "...Setting GRADIENT to follow bfield ramp"
bfieldV = numpy.copy(bfield.y)
bfieldA = physics.inv( 'bfield', bfieldV)
#~ self.y = slope * bfieldA + offset
self.y= np.array([physics.cnv( 'gradientfield', bA) for bA in bfieldA])
def dimple_to_lattice(s, cpowend):
print "----- LATTICE LOADING RAMPS -----"
# Find out which is the longest of the ramps we are dealing with:
maxX =max( [xdomain(DL.latticeV0)[1] ,\
xdomain(DL.irpow)[1],\
xdomain(DL.grpow1)[1],\
xdomain(DL.grpow2)[1],\
xdomain(DL.grpow3)[1],\
xdomain(DL.a_s)[1]] )
print "Largest x value = %.3f ms\n" % maxX
# We define the times for which all functions will be evaluated
# MIN TIME TO DO DIGITAL EXTENSION
DIGEXTENSION = 2050.
if DL.image >= DIGEXTENSION:
Xendtime = DIGEXTENSION
else:
Xendtime = DL.image
Nnew = int(math.floor(Xendtime / DL.ss))
Xnew = numpy.arange(Xendtime / Nnew, DL.image, Xendtime / Nnew)
print "X array defined from dt:"
print "DL.ss =", DL.ss
print "x0 = ", Xnew[0]
print "xf = ", Xnew[-1]
print "xdt = ", Xnew[1] - Xnew[0]
print "%d samples" % Nnew
print 'x shape = ', Xnew.shape
# Define how we want to ramp up the lattice depth
v0_ramp, xy_v0, v0set = interpolate_ramp(DL.latticeV0)
v0 = v0_ramp(Xnew)
###########################################
#### AXIS DEFINITIONS FOR PLOTS ###
###########################################
fig = plt.figure(figsize=(4.5 * 1.05, 8. * 1.1))
ax0 = fig.add_axes([0.18, 0.76, 0.76, 0.20])
ax2 = fig.add_axes([0.18, 0.645, 0.76, 0.11])
ax3 = fig.add_axes([0.18, 0.53, 0.76, 0.11])
ax1 = fig.add_axes([0.18, 0.415, 0.76, 0.11])
ax5 = fig.add_axes([0.18, 0.30, 0.76, 0.11])
ax4 = fig.add_axes([0.18, 0.185, 0.76, 0.11])
ax6 = fig.add_axes([0.18, 0.07, 0.76, 0.11])
allax = [ax0, ax1, ax2, ax3, ax4, ax5, ax6]
for ax in allax:
ax.axvline(DL.image, linewidth=1., color='black', alpha=0.6)
lw = 1.5
labelx = -0.12
legsz = 8.
xymew = 0.5
xyms = 9
ax0.plot(Xnew, v0, 'b', lw=2.5, label='Lattice depth')
ax0.plot(xy_v0[:, 0], xy_v0[:, 1], 'x', color='blue', ms=5.)
ax0.plot(v0set[:, 0], v0set[:, 1], '.', mew=xymew, ms=xyms, color='blue')
###########################################
#### USER DEFINED RAMPS: IR, GR, and U ###
###########################################
# Define how we want to ramp up the IR power
if DIMPLE.allirpow > 0.:
ir_offset = DIMPLE.allirpow
else:
ir_offset = DIMPLE.ir1pow2
ir_ramp, xy_ir, ir = interpolate_ramp(DL.irpow, yoffset=ir_offset)
dt_ir = numpy.amax(ir[:, 0]) - numpy.amin(ir[:, 0])
N_ir = int(math.floor(dt_ir / DL.ss))
x_ir = numpy.arange(dt_ir / N_ir, dt_ir, dt_ir / N_ir)
y_ir = ir_ramp(Xnew)
if v0.size > y_ir.size:
y_ir = numpy.append(y_ir, (v0.size - y_ir.size) * [y_ir[-1]])
elif v0.size < y_ir.size:
y_ir = y_ir[0:v0.size]
if v0.size != y_ir.size:
msg = "IRPOW ERROR: number of samples in IR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
alpha_clip_range = 0.1
if (v0 > y_ir + alpha_clip_range).any():
msg = "IRPOW ERROR: not enough power to get desired lattice depth"
print msg
bad = numpy.where(v0 > y_ir + alpha_clip_range)
timefail = int(bad[0][0]) * float(DL.ss)
msg = msg + "\nFirst bad sample = %d out of %d" % (bad[0][0], v0.size)
msg = msg + "\n t = %f " % timefail
msg = msg + "\n v0 = %f " % v0[bad[0][0]]
msg = msg + "\n ir = %f " % y_ir[bad[0][0]]
print v0[bad[0][0]]
print y_ir[bad[0][0]]
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
ax0.plot(xy_ir[:, 0], xy_ir[:, 1], 'x', color='darkorange', ms=5.)
ax0.plot(ir[:, 0], ir[:, 1], '.', mew=xymew, ms=xyms, color='darkorange')
ax0.plot(Xnew, y_ir, lw=lw, color='darkorange', label='irpow')
# Define how we want to ramp up the GR power
grwfms = {}
splmrkr = ['x', '+', 'd']
ptsmrkr = ['^', 's', 'p']
for i, grramp in enumerate([(DL.grpow1, DIMPLE.gr1pow2),
(DL.grpow2, DIMPLE.gr2pow2),
(DL.grpow3, DIMPLE.gr3pow2)]):
ramppts = grramp[0]
ramp0 = grramp[1]
print 'gr' + '%d' % i + ' offset = %f' % ramp0
gr_ramp, xy_gr, gr = interpolate_ramp(ramppts, yoffset=ramp0)
dt_gr = numpy.amax(gr[:, 0]) - numpy.amin(gr[:, 0])
N_gr = int(math.floor(dt_gr / DL.ss))
x_gr = numpy.arange(dt_gr / N_gr, dt_gr, dt_gr / N_gr)
y_gr = gr_ramp(Xnew)
if DL.signal == 0:
y_gr = y_gr / 2.0
if v0.size > y_gr.size:
y_gr = numpy.append(y_gr, (v0.size - y_gr.size) * [y_gr[-1]])
elif v0.size < y_gr.size:
y_gr = y_gr[0:v0.size]
if v0.size != y_gr.size:
msg = "GRPOW ERROR: number of samples in GR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
grwfms['greenpow' + '%1d' % (i + 1)] = y_gr
ax0.plot(xy_gr[:, 0],
xy_gr[:, 1],
marker=splmrkr[i],
mec='green',
mfc='None',
ms=3.)
ax0.plot(gr[:, 0],
gr[:, 1],
marker=ptsmrkr[i],
mew=xymew,
ms=xyms / 2.,
mfc='None',
mec='green') #, label='grpow dat')
ax0.plot(Xnew, y_gr, lw=lw, color='green', label='grpow')
for grch in grwfms.keys():
print grch, " = ", grwfms[grch].shape
ax0.set_xlim(left=-10., right=ax0.get_xlim()[1] * 1.1)
plt.setp(ax0.get_xticklabels(), visible=False)
ylim = ax0.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax0.set_ylim(ylim[0] - extra, ylim[1] + extra)
ax0.grid(True)
ax0.set_ylabel('$E_{r}$', size=16, labelpad=0)
ax0.yaxis.set_label_coords(labelx, 0.5)
ax0.set_title('Lattice Loading')
ax0.legend(loc='best', numpoints=1, prop={'size': legsz * 0.8})
# Define how we want to ramp up the scattering length (control our losses)
a_s_ramp, xy_a_s, a_s = interpolate_ramp(DL.a_s)
dt_a_s = numpy.amax(a_s[:, 0]) - numpy.amin(a_s[:, 0])
N_a_s = int(math.floor(dt_a_s / DL.ss))
x_a_s = numpy.arange(dt_a_s / N_a_s, dt_a_s, dt_a_s / N_a_s)
y_a_s = a_s_ramp(Xnew)
if v0.size > y_a_s.size:
y_a_s = numpy.append(y_a_s, (v0.size - y_a_s.size) * [y_a_s[-1]])
elif v0.size < y_a_s.size:
y_a_s = y_a_s[0:v0.size]
if v0.size != y_a_s.size:
msg = "a_s ERROR: number of samples in a_s ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
ax1.plot(xy_a_s[:, 0], xy_a_s[:, 1] / 100., 'x', color='#C10087', ms=5.)
ax1.plot(a_s[:, 0],
a_s[:, 1] / 100.,
'.',
mew=xymew,
ms=xyms,
color='#C10087')
ax1.plot(Xnew,
y_a_s / 100.,
lw=lw,
color='#C10087',
label=r'$a_s\mathrm{(100 a_{0})}$')
ax1.set_ylabel(r'$a_s\mathrm{(100 a_{0})}$', size=16, labelpad=0)
ax1.yaxis.set_label_coords(labelx, 0.5)
ax1.set_xlim(ax0.get_xlim())
ylim = ax1.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax1.set_ylim(ylim[0] - extra, ylim[1] + extra)
plt.setp(ax1.get_xticklabels(), visible=False)
ax1.grid(True)
ax1.legend(loc='best', numpoints=1, prop={'size': legsz})
#######################################################################
#### CALCULATED RAMPS: ALPHA, TUNNELING, SCATTERING LENGTH, BFIELD ###
#######################################################################
alpha = (v0 / y_ir)**2.
alpha_advance = 100.
N_adv = int(math.floor(alpha_advance / DL.ss))
alpha = alpha.clip(0., 1.)
alpha_desired = numpy.copy(alpha)
if N_adv < v0.size:
alpha = alpha[N_adv:]
alpha = numpy.append(alpha, (v0.size - alpha.size) * [alpha[-1]])
else:
alpha = numpy.array(v0.size * [alpha[-1]])
#alpha = alpha.clip(0., 1.)
ax2.plot(Xnew, alpha, lw=lw, color='saddlebrown', label='alpha adv')
ax2.plot(Xnew,
alpha_desired,
':',
lw=lw,
color='saddlebrown',
label='alpha')
ax2.set_xlim(ax0.get_xlim())
ax2.set_ylim(-0.05, 1.05)
plt.setp(ax2.get_xticklabels(), visible=False)
ax2.grid()
ax2.set_ylabel('$\\alpha$', size=16, labelpad=0)
ax2.yaxis.set_label_coords(labelx, 0.5)
ax2.legend(loc='best', numpoints=1, prop={'size': legsz})
tunneling_Er = physics.inv('t_to_V0', v0)
tunneling_kHz = tunneling_Er * 29.2
ax3.plot(Xnew, tunneling_kHz, lw=lw, color='red', label='$t$ (kHz)')
ax3.set_xlim(ax0.get_xlim())
ylim = ax3.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax3.set_ylim(ylim[0] - extra, ylim[1] + extra)
plt.setp(ax3.get_xticklabels(), visible=False)
ax3.grid(True)
ax3.set_ylabel(r'$t\,\mathrm{(kHz)}$', size=16, labelpad=0)
ax3.yaxis.set_label_coords(labelx, 0.5)
ax3.legend(loc='best', numpoints=1, prop={'size': legsz})
wannierF = physics.inv('wF_to_V0', v0)
bohrRadius = 5.29e-11 #meters
lattice_spacing = 1.064e-6 / 2. #meters
bfieldG = physics.cnv('as_to_B', y_a_s)
print
print "The last value of the scattering length ramp is:"
print 'a_s =', y_a_s[-1]
print 'B =', bfieldG[-1]
print
U_over_t = y_a_s * bohrRadius / lattice_spacing * wannierF / tunneling_Er
ax4.plot(Xnew, U_over_t, lw=lw, color='k', label=r'$U/t$')
ax4.set_xlim(ax0.get_xlim())
ylim = ax4.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax4.set_ylim(ylim[0] - extra, ylim[1] + extra)
plt.setp(ax4.get_xticklabels(), visible=False)
ax4.grid(True)
ax4.set_ylabel(r'$U/t$', size=16, labelpad=0)
ax4.yaxis.set_label_coords(labelx, 0.5)
ax4.legend(loc='best', numpoints=1, prop={'size': legsz})
ax5.plot(Xnew, bfieldG, lw=lw, color='purple', label='$B$ (G)')
ax5.set_xlim(ax0.get_xlim())
ylim = ax5.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax5.set_ylim(ylim[0] - extra, ylim[1] + extra)
ax5.grid(True)
plt.setp(ax5.get_xticklabels(), visible=False)
ax5.set_ylabel(r'$B\,\mathrm{(G)}$', size=16, labelpad=0)
ax5.yaxis.set_label_coords(labelx, 0.5)
ax5.legend(loc='best', numpoints=1, prop={'size': legsz})
ax6.plot(Xnew, (tunneling_Er / U_over_t),
lw=lw,
color='#25D500',
label=r'$t^{2}/U\,(E_{r)}$')
#ax6.set_yscale('log')
ax6.set_xlim(ax0.get_xlim())
ylim = ax6.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax6.set_ylim(ylim[0] * 0.5, ylim[1])
ax6.grid(True)
ax6.set_ylabel(r'$t^{2}/U\,(E_{r)}$', size=16, labelpad=0)
ax6.yaxis.set_label_coords(labelx, 0.5)
ax6.legend(loc='best', numpoints=1, prop={'size': legsz})
ax6.set_xlabel('time (ms)')
figfile = seqconf.seqtxtout().split('.')[0] + '_latticeRamp.png'
plt.savefig(figfile, dpi=120)
#Save all ramps to a txt file for later plotting.
datfile = seqconf.seqtxtout().split('.')[0] + '_latticeRamp.dat'
allRamps = numpy.transpose(numpy.vstack((Xnew, v0, y_ir, grwfms['greenpow1'], y_a_s, alpha, alpha_desired, \
tunneling_kHz, U_over_t, bfieldG)))
header = '# Column index'
header = header + '\n#\t0\t' + 'time(ms)'
header = header + '\n#\t1\t' + 'Lattice Depth (Er)'
header = header + '\n#\t2\t' + 'Ir power (Er)'
header = header + '\n#\t3\t' + 'GR power (Er)'
header = header + '\n#\t4\t' + 'a_s (a0)'
header = header + '\n#\t5\t' + 'alpha - advance'
header = header + '\n#\t6\t' + 'alpha - desired'
header = header + '\n#\t7\t' + 'tunneling (kHz)'
header = header + '\n#\t8\t' + 'U/t'
header = header + '\n#\t9\t' + 'bfield (Gauss)'
header = header + '\n'
numpy.savetxt(datfile, allRamps)
with open(datfile, 'w') as f:
X = numpy.asarray(allRamps)
f.write(bytes(header))
format = '%.6e'
ncol = X.shape[1]
format = [
format,
] * ncol
format = ' '.join(format)
newline = '\n'
for row in X:
f.write(numpy.compat.asbytes(format % tuple(row) + newline))
shutil.copyfile(
figfile,
seqconf.savedir() + 'expseq' + seqconf.runnumber() +
'_latticeRamp.png')
shutil.copyfile(
datfile,
seqconf.savedir() + 'expseq' + seqconf.runnumber() +
'_latticeRamp.dat')
#plt.savefig( seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png', dpi=120)
#################################
#### APPEND RAMPS TO SEQUENCE ###
#################################
wfms = []
if DL.signal == 0:
print " LOCK VALUE FOR SIGNAL / NOSIGNAL "
print " before = ", DL.lock_Er
DL.lock_Er = DL.lock_Er / 1.8
print " after = \n", DL.lock_Er
for ch in ['ir1pow', 'ir2pow', 'ir3pow']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv(ch, y_ir)
if DL.lock:
endval = w.y[-1]
w.insertlin_cnv(DL.lock_Er, DL.lock_dtUP, DL.lock_t0)
elif DL.lightassist_lock:
endval = w.y[-1]
w.linear(DL.lightassist_lockpowIR, DL.lightassist_lockdtUP)
w.appendhold(DL.lightassist_t0 + DL.lightassistdt)
if DL.endvalIR >= 0.:
w.linear(DL.endvalIR, DL.lightassist_lockdtDOWN)
else:
w.linear(None, DL.lightassist_lockdtDOWN, volt=endval)
wfms.append(w)
for ch in ['greenpow1', 'greenpow2', 'greenpow3']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
correction = DIMPLE.__dict__['gr' + n + 'correct']
w.y = physics.cnv(ch, correction * grwfms[ch])
if DL.lightassist_lock:
endval = w.y[-1]
w.linear(DL.lightassist_lockpowGR, DL.lightassist_lockdtUP)
w.appendhold(DL.lightassist_t0 + DL.lightassistdt)
if DL.endvalGR >= 0.:
w.linear(DL.endvalGR, DL.lightassist_lockdtDOWN)
else:
w.linear(None, DL.lightassist_lockdtDOWN, volt=endval)
wfms.append(w)
for ch in ['lcr1', 'lcr2', 'lcr3']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
force = DL.__dict__['force_' + ch]
if force >= 0 and force <= 1:
print "...Forcing LCR%s = %f during lattice ramp" % (n, force)
w.y = physics.cnv(ch, numpy.array(alpha.size * [force]))
elif DL.signal == 0:
print "...Forcing LCR%s = 0. so that it does NOT rotate to LATTICE" % n
w.y = physics.cnv(ch, numpy.array(alpha.size * [0.0]))
else:
w.y = physics.cnv(ch, alpha)
wfms.append(w)
bfieldA = bfieldG / 6.8
##ADD field
bfield = wfm.wave('bfield', 0.0, DL.ss)
bfield.y = physics.cnv('bfield', bfieldA)
print "The last value of the bfield voltage is =", bfield.y[-1]
print
wfms.append(bfield)
##ADD gradient field
gradient = gradient_wave('gradientfield', 0.0, DL.ss, volt=0.0)
gradient.follow(bfield)
wfms.append(gradient)
buffer = 40.
s.wait(buffer)
#~ odtpow = odt.odt_wave('odtpow', cpowend, DL.ss)
#~ if DIMPLE.odt_t0 > buffer :
#~ odtpow.appendhold( DIMPLE.odt_t0 - buffer)
#~ if DIMPLE.odt_pow < 0.:
#~ odtpow.appendhold( DIMPLE.odt_dt)
#~ else:
#~ odtpow.tanhRise( DIMPLE.odt_pow, DIMPLE.odt_dt, DIMPLE.odt_tau, DIMPLE.odt_shift)
#~ if numpy.absolute(DIMPLE.odt_pow) < 0.0001:
#~ s.wait( odtpow.dt() )
#~ s.digichg('odtttl',0)
#~ s.wait(-odtpow.dt() )
#~ wfms.append(odtpow)
# RF sweep
if DL.rf == 1:
rfmod = wfm.wave('rfmod', 0., DL.ss)
rfmod.appendhold(bfield.dt() + DL.rftime)
rfmod.linear(DL.rfvoltf, DL.rfpulsedt)
wfms.append(rfmod)
if DL.round_trip == 1:
bindex = 0 # Calculate detunings using starting field
else:
bindex = -1 # Calculate detunings using field at the end of ramps
bfieldG = physics.inv('bfield', bfield.y[bindex]) * 6.8
hfimg0 = -1. * (100.0 + 163.7 - 1.414 * bfieldG)
# Find bindex for braggkill time
bindex_BK = math.floor(-DL.braggkilltime / bfield.ss)
bfieldG_BK = physics.inv('bfield', bfield.y[-1 - bindex_BK]) * 6.8
hfimg0_BK = -1. * (100.0 + 163.7 - 1.414 * bfieldG_BK)
DL.braggkill_hfimg = hfimg0_BK - DL.braggkill_hfimg
print "\n...Braggkill hfimg modification:\n"
print "\tNEW braggkill_hfimg = %.2f MHz" % DL.braggkill_hfimg
# Find bindex for bragg2kill time
bindex_B2K = math.floor(-DL.bragg2killtime / bfield.ss)
bfieldG_B2K = physics.inv('bfield', bfield.y[-1 - bindex_B2K]) * 6.8
hfimg0_B2K = -1. * (100.0 + 163.7 - 1.414 * bfieldG_B2K)
DL.bragg2kill_hfimg1 = hfimg0_B2K - DL.bragg2kill_hfimg1
DL.bragg2kill_hfimg2 = hfimg0_B2K - DL.bragg2kill_hfimg2
print "\n...Bragg2kill hfimg modification:\n"
print "\tNEW brag2gkill_hfimg1 = %.2f MHz" % DL.bragg2kill_hfimg1
print "\tNEW brag2gkill_hfimg2 = %.2f MHz" % DL.bragg2kill_hfimg2
print "\n...ANDOR:hfimg and hfimg0 will be modified in report\n"
print "\tNEW ANDOR:hfimg = %.2f MHz" % (hfimg0 - DL.imgdet)
print "\tNEW ANDOR:hfimg0 = %.2f MHz\n" % hfimg0
gen.save_to_report('ANDOR', 'hfimg', hfimg0 - DL.imgdet)
gen.save_to_report('ANDOR', 'hfimg0', hfimg0)
newANDORhfimg = hfimg0 - DL.imgdet
# THIS DEFINES THE TIME IT TAKES THE OFFSET LOCK TO SWITCH TO
# A NEW SETPOINT
hfimgdelay = 50. #ms
# Kill hfimg
if DL.probekill == 1 or DL.braggkill == 1 or DL.bragg2kill == 1 or DL.lightassist or DL.lightassist_lock:
analogimg = wfm.wave('analogimg', newANDORhfimg, DL.ss)
if DL.probekill == 1:
if (-DL.probekilltime + hfimgdelay) < DL.image:
analogimg.appendhold(bfield.dt() + DL.probekilltime -
hfimgdelay)
analogimg.linear(DL.probekill_hfimg, 0.0)
analogimg.appendhold(hfimgdelay + DL.probekilldt + 3 * DL.ss)
elif DL.braggkill == 1:
print "Setting up analogimg for braggkill"
if (-DL.braggkilltime + hfimgdelay) < DL.image:
analogimg.appendhold(bfield.dt() + DL.braggkilltime -
hfimgdelay)
analogimg.linear(DL.braggkill_hfimg, 0.0)
analogimg.appendhold(hfimgdelay + DL.braggkilldt + 3 * DL.ss)
elif DL.bragg2kill == 1:
print "Setting up analogimg for bragg2kill"
if (-DL.bragg2killtime + hfimgdelay) < DL.image:
# This sets up the detuning for the first pulse
analogimg.appendhold(bfield.dt() + DL.bragg2killtime -
hfimgdelay)
analogimg.linear(DL.bragg2kill_hfimg1, 0.0)
analogimg.appendhold(hfimgdelay + DL.bragg2killdt + 3 * DL.ss)
# Then set up the detuning for the second pulse
analogimg.linear(DL.bragg2kill_hfimg2, 0.0)
analogimg.appendhold(hfimgdelay + DL.bragg2killdt + 3 * DL.ss)
elif DL.lightassist == 1 or DL.lightassist_lock:
analogimg.appendhold(bfield.dt() - hfimgdelay)
analogimg.linear(DL.lightassist_hfimg, 0.0)
duration = DL.lightassist_lockdtUP + DL.lightassist_t0 + DL.lightassistdt + DL.lightassist_lockdtDOWN
analogimg.appendhold(hfimgdelay + duration + 3 * DL.ss)
analogimg.linear(newANDORhfimg, 0.)
analogimg.extend(10)
wfms.append(analogimg)
#analogimg = bfieldwfm.hfimg_wave('analogimg', ANDOR.hfimg, DL.ss)
#andorhfimg0 = analogimg.follow(bfield, DL.imgdet)
#wfms.append(analogimg)
# If we are doing round trip END, then mirror all the ramps
# before adding them to the sequence
if DL.round_trip == 1:
if DL.round_trip_type == 1:
maxdt = 0.
maxi = -1
for i, w in enumerate(wfms):
if w.dt() > maxdt:
maxdt = w.dt()
maxi = i
maxdt = maxdt + DL.wait_at_top / 2.
for w in wfms:
w.extend(maxdt)
if 'lcr' in w.name:
yvals = w.y
#Get the reverse of the alpha desired array
alpha_mirror = numpy.copy(alpha_desired[::-1])
#Add the wait at top part so that it has same length as yvals
if alpha_mirror.size > yvals.size:
print "Error making mirror ramp for LCR."
print "Program will exit."
exit(1)
alpha_mirror = numpy.append(
(yvals.size - alpha_mirror.size) * [alpha_mirror[0]],
alpha_mirror)
#This is how much the mirror ramp will be advanced
N_adv = int(math.floor(DL.lcr_mirror_advance / DL.ss))
if N_adv < alpha_mirror.size:
alpha_mirror = alpha_mirror[N_adv:]
alpha_mirror = numpy.append(
alpha_mirror, (yvals.size - alpha_mirror.size) *
[alpha_mirror[-1]])
else:
alpha_mirror = numpy.array(yvals.size *
[alpha_mirror[-1]])
w.y = numpy.concatenate(
(yvals, physics.cnv(w.name, alpha_mirror)))
else:
w.mirror()
w.appendhold(DL.wait_at_end)
N_adv = int(math.floor(alpha_advance / DL.ss))
alpha_desired = numpy.copy(alpha)
for wavefm in wfms:
print "%s dt = %f" % (wavefm.name, wavefm.dt())
duration = s.analogwfm_add(DL.ss, wfms)
if DL.image < DIGEXTENSION:
s.wait(duration)
else:
print "...DL.image = %f >= %.2f Digital seq extension will be used." % (
DL.image, DIGEXTENSION)
s.wait(DL.image)
### Prepare the parts of the ramps that are going to be used to mock
### the conditions for the noatoms shot
### 1. get dt = [noatoms] ms from the end of the lattice ramps.
if 'manta' in DL.camera:
noatomsdt = MANTA.noatoms
else:
noatomsdt = ANDOR.noatoms
noatomswfms = []
for wavefm in wfms:
cp = copy.deepcopy(wavefm)
cp.idnum = time.time() * 100
cp.retain_last(DL.bgRetainDT)
noatomswfms.append(cp)
### Figure out when to turn interlock back on, using alpha information
#~ if duration > DL.t0 + DL.dt:
#~ s.wait(-DL.lattice_interlock_time)
#~ if DL.use_lattice_interlock == 1:
#~ s.digichg('latticeinterlockbypass',0)
#~ else:
#~ s.digichg('latticeinterlockbypass',1)
#~ s.wait( DL.lattice_interlock_time)
#########################################
## OTHER TTL EVENTS: probekill, braggkill, rf, quick2
#########################################
# Braggkill
if DL.braggkill == 1:
print "Using Bragg Kill"
s.wait(DL.braggkilltime)
s = manta.OpenShutterBragg(s, DL.shutterdelay)
s.digichg('bragg', 1)
s.wait(DL.braggkilldt)
s.digichg('brshutter', 1) # to close shutter
s.digichg('bragg', 0)
s.wait(-DL.braggkilldt)
s.wait(-DL.braggkilltime)
if DL.bragg2kill == 1:
print "Using Bragg 2 Kill"
tcur = s.tcur
s.wait(DL.bragg2killtime)
s = manta.OpenShutterBragg(s, DL.shutterdelay)
s.digichg('bragg', 1)
s.wait(DL.bragg2killdt)
s.digichg('brshutter', 1) # to close shutter
s.digichg('bragg', 0)
s.wait(hfimgdelay + 3 * DL.ss)
s = manta.OpenShutterBragg(s, DL.shutterdelay)
s.digichg('bragg', 1)
s.wait(DL.bragg2killdt)
s.digichg('brshutter', 1) # to close shutter
s.digichg('bragg', 0)
# Revert to current time after pulses have been added in the past
s.tcur = tcur
# Probe Kill
if DL.probekill == 1:
s.wait(DL.probekilltime)
s.wait(-10)
s.digichg('prshutter', 0)
s.wait(10)
s.digichg('probe', 1)
s.wait(DL.probekilldt)
s.digichg('probe', 0)
s.digichg('prshutter', 1)
s.wait(-DL.probekilltime)
# Pulse RF
if DL.rf == 1:
s.wait(DL.rftime)
s.digichg('rfttl', 1)
s.wait(DL.rfpulsedt)
s.digichg('rfttl', 0)
s.wait(-DL.rfpulsedt)
s.wait(-DL.rftime)
# QUICK2
if DL.quick2 == 1:
s.wait(DL.quick2time)
s.digichg('quick2', 1)
s.wait(-DL.quick2time)
# Light-assisted collisions
if DL.lightassist == 1 or DL.lightassist_lock:
s.wait(-DL.lightassist_lockdtUP - DL.lightassist_t0 -
DL.lightassistdt - DL.lightassist_lockdtDOWN - 3 * DL.ss)
s.wait(DL.lightassist_lockdtUP + DL.lightassist_t0)
s.wait(-10)
s.digichg('prshutter', 0)
s.wait(10)
s.digichg('probe', DL.lightassist)
s.wait(DL.lightassistdt)
s.digichg('probe', 0)
s.digichg('prshutter', 1)
s.wait(DL.lightassist_lockdtDOWN)
s.wait(3 * DL.ss)
# After the collisions happen we still need to wait some time
# for the probe frequency to come back to the desired value
s.wait(hfimgdelay)
#########################################
## GO BACK IN TIME IF DOING ROUND-TRIP START
#########################################
if DL.round_trip == 1:
if DL.round_trip_type == 0:
s.wait(-DL.image)
s.stop_analog()
#########################################
## TURN GREEN OFF BEFORE PICTURES
#########################################
if DL.greenoff == 1:
s.wait(DL.greenoff_t0)
s.digichg('greenttl1', 0)
s.digichg('greenttl2', 0)
s.digichg('greenttl3', 0)
s.wait(-DL.greenoff_t0)
#########################################
## LATTICE LOCK WITH POSSIBILITY OF RF
#########################################
bufferdt = 5.0
lastIR = y_ir[-1]
lockwfms = []
if DL.locksmooth == 1 and DL.lock == 0:
s.wait(bufferdt)
for ch in ['ir1pow', 'ir2pow', 'ir3pow']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, lastIR,
DL.lockss) #Start value will be overrriden
w.tanhRise(DL.lock_Er, DL.lock_dtUP, 0.4, 0.2)
lockwfms.append(w)
print "...LOCKING LATTICE TO %f Er" % DL.lock_Er
print "...lastIR = %.4f" % lastIR
duration = s.analogwfm_add(DL.lockss, lockwfms)
print "...duration = %.2f" % duration
s.wait(duration)
#~ if DL.lockrf:
#~ s.digichg('rfttl',1)
#~ s.wait(DL.rfpulsedt)
#~ s.digichg('rfttl',0)
#~ s.wait(0.036)
#else:
# s.wait(bufferdt)
lockwfmscopy = []
for wavefm in lockwfms:
cp = copy.deepcopy(wavefm)
cp.idnum = time.time() * 100 + 1e3 * numpy.random.randint(0, 1e8)
lockwfmscopy.append(cp)
#########################################
## IMAGING AT LOW FIELD
#########################################
if DL.lowfieldimg == 1:
s.wait(DL.lowfieldimg_t0)
s.digichg('field', 0)
s.wait(-DL.lowfieldimg_t0)
#########################################
## TTL RELEASE FROM ODT and LATTICE
#########################################
#INDICATE WHICH CHANNELS ARE TO BE CONSIDERED FOR THE BACKGROUND
bg = [
'odtttl', 'irttl1', 'irttl2', 'irttl3', 'greenttl1', 'greenttl2',
'greenttl3'
]
bgdictPRETOF = {}
for ch in bg:
bgdictPRETOF[ch] = s.digistatus(ch)
bgdictPRETOF['tof'] = DL.tof
print "\nChannel status for pictures: PRE-TOF"
print bgdictPRETOF
print
#RELEASE FROM LATTICE
if DL.tof <= 0.:
s.wait(1.0 + ANDOR.exp)
s.digichg('greenttl1', 0)
s.digichg('greenttl2', 0)
s.digichg('greenttl3', 0)
s.digichg('irttl1', 0)
s.digichg('irttl2', 0)
s.digichg('irttl3', 0)
#RELEASE FROM IR TRAP
s.digichg('odtttl', 0)
if DL.tof <= 0.:
s.wait(-1.0 + ANDOR.exp)
print "TIME WHEN RELEASED FROM LATTICE = ", s.tcur
s.wait(DL.tof)
return s, noatomswfms, lockwfmscopy, bgdictPRETOF
def do_roundtrip(s, wfms):
""" creates roundtrips to characterize cooling in lattice.
wfms are the lattice wfms, they can be mirrored here if a mirror
ramp is desired. """
s.wait(RT.wait_at_top)
# This case is for mirrored ramps
if RT.mirror == 1:
alpha_desired = wfms[1]
wfms = wfms[0]
mirrorwfms = []
for wavefm in wfms:
cp = copy.deepcopy(wavefm)
cp.idnum = time.time() * 100
mirrorwfms.append(cp)
for w in mirrorwfms:
if 'lcr' in w.name:
yvals = w.y
# Get the reverse of the alpha desired array
alpha_mirror = numpy.copy(alpha_desired[::-1])
makeplot([w, alpha_mirror], name=w.name)
# It needs to have the same length as yvals, so append
# constant samples at the beginning if needed
if alpha_mirror.size > yvals.size:
print "Error making mirror ramp for LCR."
print "Program will exit."
exit(1)
alpha_mirror = numpy.append(
(yvals.size - alpha_mirror.size) * [alpha_mirror[0]],
alpha_mirror)
# This is how much the mirror ramp will be advanced
N_adv = int(math.floor(RT.lcr_mirror_advance / DL.ss))
if N_adv < alpha_mirror.size:
alpha_mirror = alpha_mirror[N_adv:]
alpha_mirror = numpy.append(
alpha_mirror,
(yvals.size - alpha_mirror.size) * [alpha_mirror[-1]])
else:
alpha_mirror = numpy.array(yvals.size * [alpha_mirror[-1]])
if RT.lcr_snap == 1:
alpha_mirror[alpha_mirror > 0.01] = 1.
w.y = physics.cnv(w.name, alpha_mirror)
else:
w.y = w.y[::-1]
w.appendhold(RT.wait_at_end)
wfms = mirrorwfms
# This case is for custom ramps
else:
# There need to be 10 waveforms
# 3IR, 3LCR, 3GR, BFIELD
# This follows the procedure done for the lattice ramps
Xendtime = float(RT.image)
Nnew = int(math.floor(Xendtime / DL.ss))
Xnew = numpy.arange(Xendtime / Nnew, RT.image, Xendtime / Nnew)
ir_ramp, xy_ir, ir = lattice.interpolate_ramp(RT.irpow, yoffset=0.)
y_ir = ir_ramp(Xnew)
grwfms = {}
for i, grramp in enumerate([RT.grpow1, RT.grpow2, RT.grpow3]):
gr_ramp, xy_gr, gr = lattice.interpolate_ramp(grramp, yoffset=0.)
y_gr = gr_ramp(Xnew)
grwfms['greenpow' + '%1d' % (i + 1)] = y_gr
alpha_ramp, xy_alpha, alpha = lattice.interpolate_ramp(RT.alpha,
yoffset=0.)
y_alpha = alpha_ramp(Xnew)
wfms = []
for ch in ['ir1pow', 'ir2pow', 'ir3pow']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv(ch, y_ir)
wfms.append(w)
for ch in ['greenpow1', 'greenpow2', 'greenpow3']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
correction = DIMPLE.__dict__['gr' + n + 'correct']
w.y = physics.cnv(ch, correction * grwfms[ch])
wfms.append(w)
for ch in ['lcr1', 'lcr2', 'lcr3']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
#print "Obtaining LCR waveform for ROUNDTRIP..."
w.y = physics.cnv(ch, y_alpha)
wfms.append(w)
##ADD field
bfieldG = physics.cnv('as_to_B', DL.knob05)
bfieldA = bfieldG / 6.8
bfield = wfm.wave('bfield', bfieldA, DL.ss)
bfield.extend(wfms[-1].dt())
wfms.append(bfield)
# Include ramp to zerocrossing, valid for mirror and custom cases
# Final field can be given in amps (default) or in a0
if RT.enable_zc == 1:
if isinstance(RT.zc_bias, str):
if 'a0' in RT.zc_bias:
print "Using scattering length units for final field"
scattlen = float(re.sub('a0', '', RT.zc_bias))
bfieldG = physics.cnv('as_to_B', scattlen)
bfieldA = bfieldG / 6.8
elif 'knob05' in RT.zc_bias:
print "Using knob05 as the final scattering length, amounts to no change"
bfieldG = physics.cnv('as_to_B', DL.knob05)
bfieldA = bfieldG / 6.8
else:
bfieldA = RT.zc_bias
bfieldG = bfieldA * 6.8
else:
print "Using knob05 as the final scattering length, amounts to no change"
bfieldG = physics.cnv('as_to_B', DL.knob05)
bfieldA = bfieldG / 6.8
# Set hfimg value for the given final field
hfimg0 = -1. * (100.0 + 163.7 - 1.414 * bfieldG)
print "\n...ANDOR:hfimg and hfimg0 will be modified in report\n"
print "\tNEW ANDOR:hfimg = %.2f MHz" % (hfimg0 - RT.imgdet)
print "\tNEW ANDOR:hfimg0 = %.2f MHz\n" % hfimg0
gen.save_to_report('ANDOR', 'hfimg', hfimg0 - RT.imgdet)
gen.save_to_report('ANDOR', 'hfimg0', hfimg0)
newANDORhfimg = hfimg0 - RT.imgdet
for w in wfms:
if 'bfield' in w.name:
bfieldw = w
if RT.enable_zc == 1:
if RT.zc_mirror_t0 < 0.:
dt = w.dt()
w.chop(w.dt() + RT.zc_mirror_t0)
if RT.zc_mirror_t0 > 0.:
w.appendhold(RT.zc_mirror_t0)
w.linear(bfieldA, RT.zc_mirror_rampdt)
w.appendhold(RT.zc_mirror_holddt)
for i, w in enumerate(wfms):
if 'gradientfield' in w.name:
gradientfield_i = i
print "REMOVING GRADIENT FIELD"
print len(wfms)
wfms = [w for w in wfms if w.name != 'gradientfield']
print len(wfms)
#Add gradientfield ramp to have levitation all the time
from bfieldwfm import gradient_wave
gradient = gradient_wave('gradientfield', 0.0, bfieldw.ss, volt=0.0)
gradient.follow(bfieldw)
wfms.append(gradient)
duration = s.analogwfm_add(DL.ss, wfms)
s.wait(duration)
### Prepare the parts of the ramps that are going to be used to mock
### the conditions for the noatoms shot
### 1. get dt = [noatoms] ms from the end of the lattice ramps.
if 'manta' in DL.camera:
noatomsdt = MANTA.noatoms
else:
noatomsdt = ANDOR.noatoms
noatomswfms = []
for wavefm in wfms:
cp = copy.deepcopy(wavefm)
cp.idnum = time.time() * 100
cp.retain_last(DL.bgRetainDT)
noatomswfms.append(cp)
#INDICATE WHICH CHANNELS ARE TO BE CONSIDERED FOR THE BACKGROUND
bg = [
'odtttl', 'irttl1', 'irttl2', 'irttl3', 'greenttl1', 'greenttl2',
'greenttl3'
]
bgdictPRETOF = {}
for ch in bg:
bgdictPRETOF[ch] = s.digistatus(ch)
bgdictPRETOF['tof'] = RT.tof
print "\nChannel status for pictures: PRE-TOF"
print bgdictPRETOF
print
#RELEASE FROM LATTICE
if RT.tof <= 0.:
s.wait(1.0 + ANDOR.exp)
s.digichg('greenttl1', 0)
s.digichg('greenttl2', 0)
s.digichg('greenttl3', 0)
s.digichg('irttl1', 0)
s.digichg('irttl2', 0)
s.digichg('irttl3', 0)
#RELEASE FROM IR TRAP
s.digichg('odtttl', 0)
if RT.tof <= 0.:
s.wait(-1.0 + ANDOR.exp)
print "TIME WHEN RELEASED FROM LATTICE = ", s.tcur
s.wait(RT.tof)
return s, noatomswfms, bgdictPRETOF
def dimple_to_lattice(s,cpowend):
print "----- LATTICE LOADING RAMPS -----"
dt = DL.dt
tau = DL.tau
shift = DL.shift
N0 = 0
N = int(math.floor( dt/ DL.ss))
x = numpy.arange(dt/N, dt, dt/N)
tau = tau*dt
shift = dt/2. + shift*dt/2.
# Define how we want to ramp up the lattice depth
v0_ramp, xy_v0, v0set = interpolate_ramp( DL.latticeV0)
v0 = v0_ramp(x)
#v0 = 0. + DL.latticeV0 * ( (1+numpy.tanh((x-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) )\
# / ( (1+numpy.tanh((dt-shift)/tau)) - (1+numpy.tanh((-shift)/tau)) )
NH = int(math.floor( DL.dthold/ DL.ss))
v0 = numpy.concatenate(( numpy.zeros(N0), v0, numpy.array(NH*[v0[-1]]) ))
x_v0 = numpy.arange( v0.size )
x_v0 = x_v0*DL.ss
# Number of samples to keep
NS = int(math.floor( DL.image / DL.ss))
if NS > v0.size:
x_v0 = numpy.append(x_v0, (NS-v0.size)*[x_v0[-1]])
v0 = numpy.append(v0, (NS-v0.size)*[v0[-1]])
else:
x_v0 = x_v0[:NS]
v0 = v0[:NS]
###########################################
#### AXIS DEFINITIONS FOR PLOTS ###
###########################################
fig = plt.figure( figsize=(4.5*1.05,8.*1.1))
ax0 = fig.add_axes( [0.18,0.76,0.76,0.20])
ax2 = fig.add_axes( [0.18,0.645,0.76,0.11])
ax3 = fig.add_axes( [0.18,0.53,0.76,0.11])
ax1 = fig.add_axes( [0.18,0.415,0.76,0.11])
ax5 = fig.add_axes( [0.18,0.30,0.76,0.11])
ax4 = fig.add_axes( [0.18,0.185,0.76,0.11])
ax6 = fig.add_axes( [0.18,0.07,0.76,0.11])
lw=1.5
labelx=-0.12
legsz =8.
xymew=0.5
xyms=9
ax0.plot( x_v0, v0, 'b', lw=2.5, label='Lattice depth')
ax0.plot(xy_v0[:,0],xy_v0[:,1], 'x', color='blue', ms=5.)
ax0.plot(v0set[:,0],v0set[:,1], '.', mew=xymew, ms=xyms, color='blue')
###########################################
#### USER DEFINED RAMPS: IR, GR, and U ###
###########################################
# Define how we want to ramp up the IR power
ir_ramp, xy_ir, ir = interpolate_ramp( DL.irpow, yoffset=DIMPLE.ir1pow)
dt_ir = numpy.amax( ir[:,0]) - numpy.amin( ir[:,0])
N_ir = int(math.floor( dt_ir / DL.ss ))
x_ir = numpy.arange( dt_ir/N_ir, dt_ir, dt_ir/N_ir)
#y_ir = ir_spline(x_ir)
y_ir = ir_ramp(x_ir)
if v0.size > y_ir.size:
y_ir = numpy.append(y_ir, (v0.size-y_ir.size)*[y_ir[-1]])
elif v0.size < y_ir.size:
y_ir = y_ir[0:v0.size]
if v0.size != y_ir.size:
msg = "IRPOW ERROR: number of samples in IR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
if (v0 > y_ir).any():
msg = "IRPOW ERROR: not enough power to get desired lattice depth"
print msg
bad = numpy.where( v0 > y_ir)
msg = msg + "\nFirst bad sample = %d out of %d" % (bad[0][0], v0.size)
msg = msg + "\n v0 = %f " % v0[ bad[0][0] ]
msg = msg + "\n ir = %f " % y_ir[ bad[0][0] ]
print v0[bad[0][0]]
print y_ir[bad[0][0]]
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
ax0.plot(xy_ir[:,0],xy_ir[:,1], 'x', color='darkorange', ms=5.)
ax0.plot(ir[:,0],ir[:,1], '.', mew=xymew, ms=xyms, color='darkorange')
ax0.plot(x_v0, y_ir, lw=lw, color='darkorange',label='irpow')
# Define how we want to ramp up the GR power
gr_ramp, xy_gr, gr = interpolate_ramp( DL.grpow, yoffset=DIMPLE.gr1pow)
dt_gr = numpy.amax( gr[:,0]) - numpy.amin( gr[:,0])
N_gr = int(math.floor( dt_gr / DL.ss ))
x_gr = numpy.arange( dt_gr/N_gr, dt_gr, dt_gr/N_gr)
y_gr = gr_ramp(x_gr)
if v0.size > y_gr.size:
y_gr = numpy.append(y_gr, (v0.size-y_gr.size)*[y_gr[-1]])
elif v0.size < y_gr.size:
y_gr = y_gr[0:v0.size]
if v0.size != y_gr.size:
msg = "GRPOW ERROR: number of samples in GR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
ax0.plot(xy_gr[:,0],xy_gr[:,1], 'x', color='green', ms=5.)
ax0.plot(gr[:,0],gr[:,1],'.', mew=xymew, ms=xyms, color='green')#, label='grpow dat')
ax0.plot(x_v0, y_gr, lw=lw, color='green', label='grpow')
ax0.set_xlim(left=-10., right= ax0.get_xlim()[1]*1.1)
plt.setp( ax0.get_xticklabels(), visible=False)
ylim = ax0.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax0.set_ylim( ylim[0]-extra, ylim[1]+extra )
ax0.grid(True)
ax0.set_ylabel('$E_{r}$',size=16, labelpad=0)
ax0.yaxis.set_label_coords(labelx, 0.5)
ax0.set_title('Lattice Loading')
ax0.legend(loc='best',numpoints=1,prop={'size':legsz*0.8})
# Define how we want to ramp up the scattering length (control our losses)
a_s_ramp, xy_a_s, a_s = interpolate_ramp( DL.a_s)
dt_a_s = numpy.amax( a_s[:,0]) - numpy.amin( a_s[:,0])
N_a_s = int(math.floor( dt_a_s / DL.ss ))
x_a_s = numpy.arange( dt_a_s/N_a_s, dt_a_s, dt_a_s/N_a_s)
y_a_s = a_s_ramp(x_a_s)
if v0.size > y_a_s.size:
y_a_s = numpy.append(y_a_s, (v0.size-y_a_s.size)*[y_a_s[-1]])
elif v0.size < y_a_s.size:
y_a_s = y_a_s[0:v0.size]
if v0.size != y_a_s.size:
msg = "a_s ERROR: number of samples in a_s ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
ax1.plot(xy_a_s[:,0],xy_a_s[:,1]/100., 'x', color='#C10087', ms=5.)
ax1.plot(a_s[:,0],a_s[:,1]/100., '.', mew=xymew, ms=xyms, color='#C10087')
ax1.plot(x_v0, y_a_s/100., lw=lw, color='#C10087', label=r'$a_s\mathrm{(100 a_{0})}$')
ax1.set_ylabel(r'$a_s\mathrm{(100 a_{0})}$',size=16, labelpad=0)
ax1.yaxis.set_label_coords(labelx, 0.5)
ax1.set_xlim( ax0.get_xlim())
ylim = ax1.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax1.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax1.get_xticklabels(), visible=False)
ax1.grid(True)
ax1.legend(loc='best',numpoints=1,prop={'size':legsz})
#######################################################################
#### CALCULATED RAMPS: ALPHA, TUNNELING, SCATTERING LENGTH, BFIELD ###
#######################################################################
alpha = (v0/y_ir)**2.
alpha_advance = 100.
N_adv = int(math.floor( alpha_advance / DL.ss))
alpha_desired = numpy.copy(alpha)
if N_adv < v0.size:
alpha = alpha[N_adv:]
alpha = numpy.append(alpha, (v0.size-alpha.size)*[alpha[-1]])
else:
alpha = numpy.array( v0.size*[alpha[-1]] )
ax2.plot( x_v0, alpha, lw=lw, color='saddlebrown', label='alpha adv')
ax2.plot( x_v0, alpha_desired,':', lw=lw, color='saddlebrown', label='alpha')
ax2.set_xlim( ax0.get_xlim())
ax2.set_ylim(-0.05,1.05)
plt.setp( ax2.get_xticklabels(), visible=False)
ax2.grid()
ax2.set_ylabel('$\\alpha$',size=16, labelpad=0)
ax2.yaxis.set_label_coords(labelx, 0.5)
ax2.legend(loc='best',numpoints=1,prop={'size':legsz})
tunneling_Er = physics.inv('t_to_V0', v0)
tunneling_kHz = tunneling_Er * 29.2
ax3.plot( x_v0, tunneling_kHz, lw=lw, color='red', label='$t$ (kHz)')
ax3.set_xlim( ax0.get_xlim())
ylim = ax3.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax3.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax3.get_xticklabels(), visible=False)
ax3.grid(True)
ax3.set_ylabel(r'$t\,\mathrm{(kHz)}$',size=16, labelpad=0)
ax3.yaxis.set_label_coords(labelx, 0.5)
ax3.legend(loc='best',numpoints=1,prop={'size':legsz})
wannierF = physics.inv('wF_to_V0', v0)
bohrRadius = 5.29e-11 #meters
lattice_spacing = 1.064e-6 / 2. #meters
bfieldG = physics.cnv('as_to_B', y_a_s)
U_over_t = y_a_s * bohrRadius / lattice_spacing * wannierF / tunneling_Er
ax4.plot( x_v0, U_over_t, lw=lw, color='k', label=r'$U/t$')
ax4.set_xlim( ax0.get_xlim())
ylim = ax4.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax4.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax4.get_xticklabels(), visible=False)
ax4.grid(True)
ax4.set_ylabel(r'$U/t$',size=16, labelpad=0)
ax4.yaxis.set_label_coords(labelx, 0.5)
ax4.legend(loc='best',numpoints=1,prop={'size':legsz})
ax5.plot( x_v0, bfieldG, lw=lw, color='purple', label='$B$ (G)')
ax5.set_xlim( ax0.get_xlim())
ylim = ax5.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax5.set_ylim( ylim[0]-extra, ylim[1]+extra )
ax5.grid(True)
plt.setp( ax5.get_xticklabels(), visible=False)
ax5.set_ylabel(r'$B\,\mathrm{(G)}$',size=16, labelpad=0)
ax5.yaxis.set_label_coords(labelx, 0.5)
ax5.legend(loc='best',numpoints=1,prop={'size':legsz})
ax6.plot( x_v0, (tunneling_Er / U_over_t), lw=lw, color='#25D500', label=r'$t^{2}/U\,(E_{r)}$')
#ax6.set_yscale('log')
ax6.set_xlim( ax0.get_xlim())
ylim = ax6.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax6.set_ylim( ylim[0]*0.5, ylim[1] )
ax6.grid(True)
ax6.set_ylabel(r'$t^{2}/U\,(E_{r)}$',size=16, labelpad=0)
ax6.yaxis.set_label_coords(labelx, 0.5)
ax6.legend(loc='best',numpoints=1,prop={'size':legsz})
ax6.set_xlabel('time (ms)')
figfile = seqconf.seqtxtout().split('.')[0]+'_latticeRamp.png'
plt.savefig(figfile , dpi=120 )
#Save all ramps to a txt file for later plotting.
datfile = seqconf.seqtxtout().split('.')[0]+'_latticeRamp.dat'
allRamps = numpy.transpose(numpy.vstack((x_v0, v0, y_ir, y_gr, y_a_s, alpha, alpha_desired, \
tunneling_kHz, U_over_t, bfieldG)))
header = '# Column index'
header = header + '\n#\t0\t' + 'time(ms)'
header = header + '\n#\t1\t' + 'Lattice Depth (Er)'
header = header + '\n#\t2\t' + 'Ir power (Er)'
header = header + '\n#\t3\t' + 'GR power (Er)'
header = header + '\n#\t4\t' + 'a_s (a0)'
header = header + '\n#\t5\t' + 'alpha - advance'
header = header + '\n#\t6\t' + 'alpha - desired'
header = header + '\n#\t7\t' + 'tunneling (kHz)'
header = header + '\n#\t8\t' + 'U/t'
header = header + '\n#\t9\t' + 'bfield (Gauss)'
header = header + '\n'
numpy.savetxt( datfile, allRamps)
with open(datfile, 'w') as f:
X = numpy.asarray( allRamps )
f.write(bytes(header))
format = '%.6e'
ncol = X.shape[1]
format = [format ,] *ncol
format = ' '.join(format)
newline = '\n'
for row in X:
f.write(numpy.compat.asbytes(format % tuple(row) + newline))
shutil.copyfile( figfile, seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png')
#plt.savefig( seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png', dpi=120)
#################################
#### APPEND RAMPS TO SEQUENCE ###
#################################
wfms=[]
for ch in ['ir1pow','ir2pow','ir3pow']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv( ch, y_ir )
if DL.lock:
endval = w.y[-1]
w.insertlin_cnv(DL.lock_Er, DL.lock_dtUP, DL.lock_t0 )
if DL.camera == 'manta' or DL.camera == 'both':
w.appendhold( MANTA.exp + 1.0 )
w.insertlin( endval, 0., 0.)
w.appendhold( MANTA.noatoms - MANTA.exp - 1.0)
w.insertlin_cnv(DL.lock_Er, DL.lock_dtUP, DL.lock_t0 )
elif DL.lightassist_lock:
endval = w.y[-1]
w.linear(DL.lightassist_lockpowIR, DL.lightassist_lockdtUP)
w.appendhold( DL.lightassist_t0 + DL.lightassistdt )
if DL.endvalIR >= 0.:
w.linear( DL.endvalIR, DL.lightassist_lockdtDOWN)
else:
w.linear( None, DL.lightassist_lockdtDOWN, volt=endval)
wfms.append(w)
for ch in ['greenpow1','greenpow2','greenpow3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv( ch, y_gr )
if DL.lightassist_lock:
endval = w.y[-1]
w.linear(DL.lightassist_lockpowGR, DL.lightassist_lockdtUP)
w.appendhold( DL.lightassist_t0 + DL.lightassistdt )
if DL.endvalGR >= 0.:
w.linear( DL.endvalGR, DL.lightassist_lockdtDOWN)
else:
w.linear( None, DL.lightassist_lockdtDOWN, volt=endval)
wfms.append(w)
for ch in ['lcr1','lcr2','lcr3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
force = DL.__dict__['force_'+ch]
if force >= 0 and force <=1:
print "...Forcing LCR%s = %f during lattice ramp" % (n,force)
w.y = physics.cnv( ch, numpy.array( alpha.size*[force] ) )
else:
w.y = physics.cnv( ch, alpha )
wfms.append(w)
bfieldA = bfieldG/6.8
##ADD field
bfield = wfm.wave('bfield', 0.0, DL.ss)
bfield.y = physics.cnv( 'bfield', bfieldA)
wfms.append(bfield)
##ADD gradient field
gradient = gradient_wave('gradientfield', 0.0, DL.ss,volt = 0.0)
gradient.follow(bfield)
wfms.append(gradient)
buffer = 20.
s.wait(buffer)
#~ odtpow = odt.odt_wave('odtpow', cpowend, DL.ss)
#~ if DIMPLE.odt_t0 > buffer :
#~ odtpow.appendhold( DIMPLE.odt_t0 - buffer)
#~ if DIMPLE.odt_pow < 0.:
#~ odtpow.appendhold( DIMPLE.odt_dt)
#~ else:
#~ odtpow.tanhRise( DIMPLE.odt_pow, DIMPLE.odt_dt, DIMPLE.odt_tau, DIMPLE.odt_shift)
#~ if numpy.absolute(DIMPLE.odt_pow) < 0.0001:
#~ s.wait( odtpow.dt() )
#~ s.digichg('odtttl',0)
#~ s.wait(-odtpow.dt() )
#~ wfms.append(odtpow)
# RF sweep
if DL.rf == 1:
rfmod = wfm.wave('rfmod', 0., DL.ss)
rfmod.appendhold( bfield.dt() + DL.rftime )
rfmod.linear( DL.rfvoltf, DL.rfpulsedt)
wfms.append(rfmod)
bfieldG = physics.inv( 'bfield', bfield.y[-1]) * 6.8
hfimg0 = -1.*(100.0 + 163.7 - 1.414*bfieldG)
print "...ANDOR:hfimg and hfimg0 will be modified in report\n"
print "\tNEW ANDOR:hfimg = %.2f MHz" % ( hfimg0 - DL.imgdet)
print "\tNEW ANDOR:hfimg0 = %.2f MHz\n" % hfimg0
gen.save_to_report('ANDOR','hfimg', hfimg0 - DL.imgdet)
gen.save_to_report('ANDOR','hfimg0', hfimg0)
newANDORhfimg = hfimg0 - DL.imgdet
# Kill hfimg
if DL.probekill ==1 or DL.braggkill ==1 or DL.lightassist or DL.lightassist_lock:
hfimgdelay = 50. #ms
analogimg = wfm.wave('analogimg', newANDORhfimg, DL.ss)
if DL.probekill == 1:
if (-DL.probekilltime+hfimgdelay) < DL.image:
analogimg.appendhold( bfield.dt() + DL.probekilltime - hfimgdelay)
analogimg.linear( DL.probekill_hfimg , 0.0)
analogimg.appendhold( hfimgdelay + DL.probekilldt + 3*DL.ss)
elif DL.braggkill == 1:
if (-DL.braggkilltime+hfimgdelay) < DL.image:
analogimg.appendhold( bfield.dt() + DL.braggkilltime - hfimgdelay)
analogimg.linear( DL.braggkill_hfimg , 0.0)
analogimg.appendhold( hfimgdelay + DL.braggkilldt + 3*DL.ss)
elif DL.lightassist == 1 or DL.lightassist_lock:
analogimg.appendhold( bfield.dt() - hfimgdelay)
analogimg.linear( DL.lightassist_hfimg , 0.0)
duration = DL.lightassist_lockdtUP + DL.lightassist_t0 + DL.lightassistdt + DL.lightassist_lockdtDOWN
analogimg.appendhold( hfimgdelay + duration + 3*DL.ss)
analogimg.linear( newANDORhfimg, 0.)
analogimg.extend(10)
wfms.append(analogimg)
#analogimg = bfieldwfm.hfimg_wave('analogimg', ANDOR.hfimg, DL.ss)
#andorhfimg0 = analogimg.follow(bfield, DL.imgdet)
#wfms.append(analogimg)
# If we are doing round trip END, then mirror all the ramps
# before adding them to the sequence
if DL.round_trip == 1:
if DL.round_trip_type == 1:
maxdt = 0.
maxi = -1
for i,w in enumerate(wfms):
if w.dt() > maxdt:
maxdt = w.dt()
maxi = i
maxdt = maxdt + DL.wait_at_top
for w in wfms:
w.extend(maxdt)
if 'lcr' in w.name:
yvals = w.y
alpha_mirror = numpy.copy(alpha_desired[::-1])
N_adv = int(math.floor( DL.lcr_mirror_advance / DL.ss))
if N_adv < v0.size:
alpha_mirror = alpha_mirror[N_adv:]
alpha_mirror = numpy.append(alpha_mirror, (yvals.size-alpha_mirror.size)*[alpha_mirror[-1]])
else:
alpha_mirror = numpy.array( yvals.size*[alpha_mirror[-1]] )
w.y = numpy.concatenate((yvals,physics.cnv( w.name, alpha_mirror )))
else:
w.mirror()
w.appendhold( DL.wait_at_end)
N_adv = int(math.floor( alpha_advance / DL.ss))
alpha_desired = numpy.copy(alpha)
duration = s.analogwfm_add(DL.ss,wfms)
s.wait( duration )
if DL.lock:
if DL.camera == 'manta' or DL.camera == 'both':
s.wait( - MANTA.noatoms)
### Figure out when to turn interlock back on, using alpha information
#~ if duration > DL.t0 + DL.dt:
#~ s.wait(-DL.lattice_interlock_time)
#~ if DL.use_lattice_interlock == 1:
#~ s.digichg('latticeinterlockbypass',0)
#~ else:
#~ s.digichg('latticeinterlockbypass',1)
#~ s.wait( DL.lattice_interlock_time)
return s
def dimple_to_lattice(s,cpowend):
print "----- LATTICE LOADING RAMPS -----"
dt = DL.dt
N0 = 0
N = int(math.floor( dt/ DL.ss))
x = numpy.arange(dt/N, dt, dt/N)
print "%d samples" % N
print x.shape
# Define how we want to ramp up the lattice depth
v0_ramp, xy_v0, v0set = interpolate_ramp( DL.latticeV0)
v0 = v0_ramp(x)
NH = int(math.floor( DL.dthold/ DL.ss))
v0 = numpy.concatenate(( numpy.zeros(N0), v0, numpy.array(NH*[v0[-1]]) ))
x_v0 = numpy.arange( v0.size )
x_v0 = x_v0*DL.ss
# Number of samples to keep
NS = int(math.floor( DL.image / DL.ss))
if NS > v0.size and DL.image < 2500.:
x_v0 = numpy.append(x_v0, (NS-v0.size)*[x_v0[-1]])
v0 = numpy.append(v0, (NS-v0.size)*[v0[-1]])
else:
x_v0 = x_v0[:NS]
v0 = v0[:NS]
###########################################
#### AXIS DEFINITIONS FOR PLOTS ###
###########################################
fig = plt.figure( figsize=(4.5*1.05,8.*1.1))
ax0 = fig.add_axes( [0.18,0.76,0.76,0.20])
ax2 = fig.add_axes( [0.18,0.645,0.76,0.11])
ax3 = fig.add_axes( [0.18,0.53,0.76,0.11])
ax1 = fig.add_axes( [0.18,0.415,0.76,0.11])
ax5 = fig.add_axes( [0.18,0.30,0.76,0.11])
ax4 = fig.add_axes( [0.18,0.185,0.76,0.11])
ax6 = fig.add_axes( [0.18,0.07,0.76,0.11])
lw=1.5
labelx=-0.12
legsz =8.
xymew=0.5
xyms=9
ax0.plot( x_v0, v0, 'b', lw=2.5, label='Lattice depth')
ax0.plot(xy_v0[:,0],xy_v0[:,1], 'x', color='blue', ms=5.)
ax0.plot(v0set[:,0],v0set[:,1], '.', mew=xymew, ms=xyms, color='blue')
###########################################
#### USER DEFINED RAMPS: IR, GR, and U ###
###########################################
# Define how we want to ramp up the IR power
if DIMPLE.allirpow > 0.:
ir_offset = DIMPLE.allirpow
else:
ir_offset = DIMPLE.ir1pow2
ir_ramp, xy_ir, ir = interpolate_ramp( DL.irpow, yoffset=ir_offset)
dt_ir = numpy.amax( ir[:,0]) - numpy.amin( ir[:,0])
N_ir = int(math.floor( dt_ir / DL.ss ))
x_ir = numpy.arange( dt_ir/N_ir, dt_ir, dt_ir/N_ir)
#y_ir = ir_spline(x_ir)
y_ir = ir_ramp(x_ir)
if v0.size > y_ir.size:
y_ir = numpy.append(y_ir, (v0.size-y_ir.size)*[y_ir[-1]])
elif v0.size < y_ir.size:
y_ir = y_ir[0:v0.size]
if v0.size != y_ir.size:
msg = "IRPOW ERROR: number of samples in IR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
alpha_clip_range = 0.1
if (v0 > y_ir+ alpha_clip_range).any():
msg = "IRPOW ERROR: not enough power to get desired lattice depth"
print msg
bad = numpy.where( v0 > y_ir + alpha_clip_range)
timefail = int(bad[0][0])*float(DL.ss)
msg = msg + "\nFirst bad sample = %d out of %d" % (bad[0][0], v0.size)
msg = msg + "\n t = %f " % timefail
msg = msg + "\n v0 = %f " % v0[ bad[0][0] ]
msg = msg + "\n ir = %f " % y_ir[ bad[0][0] ]
print v0[bad[0][0]]
print y_ir[bad[0][0]]
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
ax0.plot(xy_ir[:,0],xy_ir[:,1], 'x', color='darkorange', ms=5.)
ax0.plot(ir[:,0],ir[:,1], '.', mew=xymew, ms=xyms, color='darkorange')
ax0.plot(x_v0, y_ir, lw=lw, color='darkorange',label='irpow')
# Define how we want to ramp up the GR power
grwfms = {}
splmrkr = ['x','+','d']
ptsmrkr = ['^','s','p']
for i,grramp in enumerate([(DL.grpow1,DIMPLE.gr1pow2), (DL.grpow2,DIMPLE.gr2pow2), (DL.grpow3,DIMPLE.gr3pow2)]):
ramppts = grramp[0]
ramp0 = grramp[1]
print 'gr'+'%d'%i +' offset = %f' % ramp0
gr_ramp, xy_gr, gr = interpolate_ramp( ramppts, yoffset=ramp0)
dt_gr = numpy.amax( gr[:,0]) - numpy.amin( gr[:,0])
N_gr = int(math.floor( dt_gr / DL.ss ))
x_gr = numpy.arange( dt_gr/N_gr, dt_gr, dt_gr/N_gr)
y_gr = gr_ramp(x_gr)
if v0.size > y_gr.size:
y_gr = numpy.append(y_gr, (v0.size-y_gr.size)*[y_gr[-1]])
elif v0.size < y_gr.size:
y_gr = y_gr[0:v0.size]
if v0.size != y_gr.size:
msg = "GRPOW ERROR: number of samples in GR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
grwfms[ 'greenpow' + '%1d' % (i+1) ] = y_gr
ax0.plot(xy_gr[:,0],xy_gr[:,1], marker= splmrkr[i] ,mec='green', mfc='None', ms=3.)
ax0.plot(gr[:,0],gr[:,1], marker=ptsmrkr[i], mew=xymew, ms=xyms/2., mfc='None', mec='green')#, label='grpow dat')
ax0.plot(x_v0, y_gr, lw=lw, color='green', label='grpow')
for grch in grwfms.keys():
print grch, " = ", grwfms[grch].shape
ax0.set_xlim(left=-10., right= ax0.get_xlim()[1]*1.1)
plt.setp( ax0.get_xticklabels(), visible=False)
ylim = ax0.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax0.set_ylim( ylim[0]-extra, ylim[1]+extra )
ax0.grid(True)
ax0.set_ylabel('$E_{r}$',size=16, labelpad=0)
ax0.yaxis.set_label_coords(labelx, 0.5)
ax0.set_title('Lattice Loading')
ax0.legend(loc='best',numpoints=1,prop={'size':legsz*0.8})
# Define how we want to ramp up the scattering length (control our losses)
a_s_ramp, xy_a_s, a_s = interpolate_ramp( DL.a_s)
dt_a_s = numpy.amax( a_s[:,0]) - numpy.amin( a_s[:,0])
N_a_s = int(math.floor( dt_a_s / DL.ss ))
x_a_s = numpy.arange( dt_a_s/N_a_s, dt_a_s, dt_a_s/N_a_s)
y_a_s = a_s_ramp(x_a_s)
if v0.size > y_a_s.size:
y_a_s = numpy.append(y_a_s, (v0.size-y_a_s.size)*[y_a_s[-1]])
elif v0.size < y_a_s.size:
y_a_s = y_a_s[0:v0.size]
if v0.size != y_a_s.size:
msg = "a_s ERROR: number of samples in a_s ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
ax1.plot(xy_a_s[:,0],xy_a_s[:,1]/100., 'x', color='#C10087', ms=5.)
ax1.plot(a_s[:,0],a_s[:,1]/100., '.', mew=xymew, ms=xyms, color='#C10087')
ax1.plot(x_v0, y_a_s/100., lw=lw, color='#C10087', label=r'$a_s\mathrm{(100 a_{0})}$')
ax1.set_ylabel(r'$a_s\mathrm{(100 a_{0})}$',size=16, labelpad=0)
ax1.yaxis.set_label_coords(labelx, 0.5)
ax1.set_xlim( ax0.get_xlim())
ylim = ax1.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax1.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax1.get_xticklabels(), visible=False)
ax1.grid(True)
ax1.legend(loc='best',numpoints=1,prop={'size':legsz})
#######################################################################
#### CALCULATED RAMPS: ALPHA, TUNNELING, SCATTERING LENGTH, BFIELD ###
#######################################################################
alpha = (v0/y_ir)**2.
alpha_advance = 100.
N_adv = int(math.floor( alpha_advance / DL.ss))
alpha = alpha.clip(0.,1.)
alpha_desired = numpy.copy(alpha)
if N_adv < v0.size:
alpha = alpha[N_adv:]
alpha = numpy.append(alpha, (v0.size-alpha.size)*[alpha[-1]])
else:
alpha = numpy.array( v0.size*[alpha[-1]] )
#alpha = alpha.clip(0., 1.)
ax2.plot( x_v0, alpha, lw=lw, color='saddlebrown', label='alpha adv')
ax2.plot( x_v0, alpha_desired,':', lw=lw, color='saddlebrown', label='alpha')
ax2.set_xlim( ax0.get_xlim())
ax2.set_ylim(-0.05,1.05)
plt.setp( ax2.get_xticklabels(), visible=False)
ax2.grid()
ax2.set_ylabel('$\\alpha$',size=16, labelpad=0)
ax2.yaxis.set_label_coords(labelx, 0.5)
ax2.legend(loc='best',numpoints=1,prop={'size':legsz})
tunneling_Er = physics.inv('t_to_V0', v0)
tunneling_kHz = tunneling_Er * 29.2
ax3.plot( x_v0, tunneling_kHz, lw=lw, color='red', label='$t$ (kHz)')
ax3.set_xlim( ax0.get_xlim())
ylim = ax3.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax3.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax3.get_xticklabels(), visible=False)
ax3.grid(True)
ax3.set_ylabel(r'$t\,\mathrm{(kHz)}$',size=16, labelpad=0)
ax3.yaxis.set_label_coords(labelx, 0.5)
ax3.legend(loc='best',numpoints=1,prop={'size':legsz})
wannierF = physics.inv('wF_to_V0', v0)
bohrRadius = 5.29e-11 #meters
lattice_spacing = 1.064e-6 / 2. #meters
bfieldG = physics.cnv('as_to_B', y_a_s)
U_over_t = y_a_s * bohrRadius / lattice_spacing * wannierF / tunneling_Er
ax4.plot( x_v0, U_over_t, lw=lw, color='k', label=r'$U/t$')
ax4.set_xlim( ax0.get_xlim())
ylim = ax4.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax4.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax4.get_xticklabels(), visible=False)
ax4.grid(True)
ax4.set_ylabel(r'$U/t$',size=16, labelpad=0)
ax4.yaxis.set_label_coords(labelx, 0.5)
ax4.legend(loc='best',numpoints=1,prop={'size':legsz})
ax5.plot( x_v0, bfieldG, lw=lw, color='purple', label='$B$ (G)')
ax5.set_xlim( ax0.get_xlim())
ylim = ax5.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax5.set_ylim( ylim[0]-extra, ylim[1]+extra )
ax5.grid(True)
plt.setp( ax5.get_xticklabels(), visible=False)
ax5.set_ylabel(r'$B\,\mathrm{(G)}$',size=16, labelpad=0)
ax5.yaxis.set_label_coords(labelx, 0.5)
ax5.legend(loc='best',numpoints=1,prop={'size':legsz})
ax6.plot( x_v0, (tunneling_Er / U_over_t), lw=lw, color='#25D500', label=r'$t^{2}/U\,(E_{r)}$')
#ax6.set_yscale('log')
ax6.set_xlim( ax0.get_xlim())
ylim = ax6.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax6.set_ylim( ylim[0]*0.5, ylim[1] )
ax6.grid(True)
ax6.set_ylabel(r'$t^{2}/U\,(E_{r)}$',size=16, labelpad=0)
ax6.yaxis.set_label_coords(labelx, 0.5)
ax6.legend(loc='best',numpoints=1,prop={'size':legsz})
ax6.set_xlabel('time (ms)')
figfile = seqconf.seqtxtout().split('.')[0]+'_latticeRamp.png'
plt.savefig(figfile , dpi=120 )
#Save all ramps to a txt file for later plotting.
datfile = seqconf.seqtxtout().split('.')[0]+'_latticeRamp.dat'
allRamps = numpy.transpose(numpy.vstack((x_v0, v0, y_ir, grwfms['greenpow1'], y_a_s, alpha, alpha_desired, \
tunneling_kHz, U_over_t, bfieldG)))
header = '# Column index'
header = header + '\n#\t0\t' + 'time(ms)'
header = header + '\n#\t1\t' + 'Lattice Depth (Er)'
header = header + '\n#\t2\t' + 'Ir power (Er)'
header = header + '\n#\t3\t' + 'GR power (Er)'
header = header + '\n#\t4\t' + 'a_s (a0)'
header = header + '\n#\t5\t' + 'alpha - advance'
header = header + '\n#\t6\t' + 'alpha - desired'
header = header + '\n#\t7\t' + 'tunneling (kHz)'
header = header + '\n#\t8\t' + 'U/t'
header = header + '\n#\t9\t' + 'bfield (Gauss)'
header = header + '\n'
numpy.savetxt( datfile, allRamps)
with open(datfile, 'w') as f:
X = numpy.asarray( allRamps )
f.write(bytes(header))
format = '%.6e'
ncol = X.shape[1]
format = [format ,] *ncol
format = ' '.join(format)
newline = '\n'
for row in X:
f.write(numpy.compat.asbytes(format % tuple(row) + newline))
shutil.copyfile( figfile, seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png')
shutil.copyfile( datfile, seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.dat')
#plt.savefig( seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png', dpi=120)
#################################
#### APPEND RAMPS TO SEQUENCE ###
#################################
wfms=[]
for ch in ['ir1pow','ir2pow','ir3pow']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv( ch, y_ir )
wfms.append(w)
for ch in ['greenpow1','greenpow2','greenpow3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
correction = DIMPLE.__dict__['gr'+n+'correct']
w.y = physics.cnv( ch, correction * grwfms[ch] )
wfms.append(w)
for ch in ['lcr1','lcr2','lcr3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
force = DL.__dict__['force_'+ch]
if force >= 0 and force <=1:
print "...Forcing LCR%s = %f during lattice ramp" % (n,force)
w.y = physics.cnv( ch, numpy.array( alpha.size*[force] ) )
else:
w.y = physics.cnv( ch, alpha )
wfms.append(w)
bfieldA = bfieldG/6.8
##ADD field
bfield = wfm.wave('bfield', 0.0, DL.ss)
bfield.y = physics.cnv( 'bfield', bfieldA)
wfms.append(bfield)
##ADD gradient field
gradient = gradient_wave('gradientfield', 0.0, DL.ss,volt = 0.0)
gradient.follow(bfield)
wfms.append(gradient)
# RF sweep
if DL.rf == 1:
rfmod = wfm.wave('rfmod', 0., DL.ss)
rfmod.appendhold( bfield.dt() + DL.rftime )
rfmod.linear( DL.rfvoltf, DL.rfpulsedt)
wfms.append(rfmod)
#Take care of imaging frequencies, including various kill experiments
bfieldG = physics.inv( 'bfield', bfield.y[-1]) * 6.8
hfimg0 = -1.*(100.0 + 163.7 - 1.414*bfieldG)
print "...ANDOR:hfimg and hfimg0 will be modified in report\n"
print "\tNEW ANDOR:hfimg = %.2f MHz" % ( hfimg0 - DL.imgdet)
print "\tNEW ANDOR:hfimg0 = %.2f MHz\n" % hfimg0
gen.save_to_report('ANDOR','hfimg', hfimg0 - DL.imgdet)
gen.save_to_report('ANDOR','hfimg0', hfimg0)
newANDORhfimg = hfimg0 - DL.imgdet
# Kill hfimg
if DL.probekill ==1 or DL.braggkill ==1 or DL.lightassist or DL.lightassist_lock:
hfimgdelay = 50. #ms
analogimg = wfm.wave('analogimg', newANDORhfimg, DL.ss)
if DL.probekill == 1:
if (-DL.probekilltime+hfimgdelay) < DL.image:
analogimg.appendhold( bfield.dt() + DL.probekilltime - hfimgdelay)
analogimg.linear( DL.probekill_hfimg , 0.0)
analogimg.appendhold( hfimgdelay + DL.probekilldt + 3*DL.ss)
elif DL.braggkill == 1:
if (-DL.braggkilltime+hfimgdelay) < DL.image:
analogimg.appendhold( bfield.dt() + DL.braggkilltime - hfimgdelay)
analogimg.linear( DL.braggkill_hfimg , 0.0)
analogimg.appendhold( hfimgdelay + DL.braggkilldt + 3*DL.ss)
#elif DL.lightassist == 1 or DL.lightassist_lock:
# analogimg.appendhold( bfield.dt() - hfimgdelay)
# analogimg.linear( DL.lightassist_hfimg , 0.0)
# duration = DL.lightassist_lockdtUP + DL.lightassist_t0 + DL.lightassistdt + DL.lightassist_lockdtDOWN
# analogimg.appendhold( hfimgdelay + duration + 3*DL.ss)
analogimg.linear( newANDORhfimg, 0.)
analogimg.extend(10)
wfms.append(analogimg)
#analogimg = bfieldwfm.hfimg_wave('analogimg', ANDOR.hfimg, DL.ss)
#andorhfimg0 = analogimg.follow(bfield, DL.imgdet)
#wfms.append(analogimg)
# If we are doing round trip END, then mirror all the ramps
# before adding them to the sequence
if DL.round_trip == 1:
if DL.round_trip_type == 1:
maxdt = 0.
maxi = -1
for i,w in enumerate(wfms):
if w.dt() > maxdt:
maxdt = w.dt()
maxi = i
maxdt = maxdt + DL.wait_at_top / 2.
for w in wfms:
w.extend(maxdt)
if 'lcr' in w.name:
yvals = w.y
#Get the reverse of the alpha desired array
alpha_mirror = numpy.copy(alpha_desired[::-1])
#Add the wait at top part so that it has same length as yvals
if alpha_mirror.size > yvals.size:
print "Error making mirror ramp for LCR."
print "Program will exit."
exit(1)
alpha_mirror = numpy.append( (yvals.size - alpha_mirror.size)*[ alpha_mirror[0] ], alpha_mirror )
#This is how much the mirror ramp will be advanced
N_adv = int(math.floor( DL.lcr_mirror_advance / DL.ss))
if N_adv < alpha_mirror.size:
alpha_mirror = alpha_mirror[N_adv:]
alpha_mirror = numpy.append(alpha_mirror, (yvals.size-alpha_mirror.size)*[alpha_mirror[-1]])
else:
alpha_mirror = numpy.array( yvals.size*[alpha_mirror[-1]] )
w.y = numpy.concatenate((yvals,physics.cnv( w.name, alpha_mirror )))
else:
w.mirror()
w.appendhold( DL.wait_at_end)
N_adv = int(math.floor( alpha_advance / DL.ss))
alpha_desired = numpy.copy(alpha)
for wavefm in wfms:
print "%s dt = %f" % (wavefm.name, wavefm.dt())
#Wait the buffer for the lattice loading ramps before adding them
bufferdt = 20.
s.wait(bufferdt)
#Add lattice wfms
duration = s.analogwfm_add(DL.ss,wfms)
if DL.image < 2500.:
s.wait(duration)
else:
print "...DL.image = %f >= 2500. Digital seq extension will be used." % DL.image
s.wait( DL.image )
#Here give some buffer time to do lock, RF etc.
#It has to be minimum 5.0 ms
### Figure out when to turn interlock back on, using alpha information
#~ if duration > DL.t0 + DL.dt:
#~ s.wait(-DL.lattice_interlock_time)
#~ if DL.use_lattice_interlock == 1:
#~ s.digichg('latticeinterlockbypass',0)
#~ else:
#~ s.digichg('latticeinterlockbypass',1)
#~ s.wait( DL.lattice_interlock_time)
return s, y_ir[-1]
def dimple_to_lattice(s, cpowend):
print "----- LATTICE LOADING RAMPS -----"
dt = DL.dt
N0 = 0
N = int(math.floor(dt / DL.ss))
x = numpy.arange(dt / N, dt, dt / N)
print "%d samples" % N
print x.shape
# Define how we want to ramp up the lattice depth
v0_ramp, xy_v0, v0set = interpolate_ramp(DL.latticeV0)
v0 = v0_ramp(x)
NH = int(math.floor(DL.dthold / DL.ss))
v0 = numpy.concatenate((numpy.zeros(N0), v0, numpy.array(NH * [v0[-1]])))
x_v0 = numpy.arange(v0.size)
x_v0 = x_v0 * DL.ss
# Number of samples to keep
NS = int(math.floor(DL.image / DL.ss))
if NS > v0.size and DL.image < 2500.:
x_v0 = numpy.append(x_v0, (NS - v0.size) * [x_v0[-1]])
v0 = numpy.append(v0, (NS - v0.size) * [v0[-1]])
else:
x_v0 = x_v0[:NS]
v0 = v0[:NS]
###########################################
#### AXIS DEFINITIONS FOR PLOTS ###
###########################################
fig = plt.figure(figsize=(4.5 * 1.05, 8. * 1.1))
ax0 = fig.add_axes([0.18, 0.76, 0.76, 0.20])
ax2 = fig.add_axes([0.18, 0.645, 0.76, 0.11])
ax3 = fig.add_axes([0.18, 0.53, 0.76, 0.11])
ax1 = fig.add_axes([0.18, 0.415, 0.76, 0.11])
ax5 = fig.add_axes([0.18, 0.30, 0.76, 0.11])
ax4 = fig.add_axes([0.18, 0.185, 0.76, 0.11])
ax6 = fig.add_axes([0.18, 0.07, 0.76, 0.11])
lw = 1.5
labelx = -0.12
legsz = 8.
xymew = 0.5
xyms = 9
ax0.plot(x_v0, v0, 'b', lw=2.5, label='Lattice depth')
ax0.plot(xy_v0[:, 0], xy_v0[:, 1], 'x', color='blue', ms=5.)
ax0.plot(v0set[:, 0], v0set[:, 1], '.', mew=xymew, ms=xyms, color='blue')
###########################################
#### USER DEFINED RAMPS: IR, GR, and U ###
###########################################
# Define how we want to ramp up the IR power
if DIMPLE.allirpow > 0.:
ir_offset = DIMPLE.allirpow
else:
ir_offset = DIMPLE.ir1pow2
ir_ramp, xy_ir, ir = interpolate_ramp(DL.irpow, yoffset=ir_offset)
dt_ir = numpy.amax(ir[:, 0]) - numpy.amin(ir[:, 0])
N_ir = int(math.floor(dt_ir / DL.ss))
x_ir = numpy.arange(dt_ir / N_ir, dt_ir, dt_ir / N_ir)
#y_ir = ir_spline(x_ir)
y_ir = ir_ramp(x_ir)
if v0.size > y_ir.size:
y_ir = numpy.append(y_ir, (v0.size - y_ir.size) * [y_ir[-1]])
elif v0.size < y_ir.size:
y_ir = y_ir[0:v0.size]
if v0.size != y_ir.size:
msg = "IRPOW ERROR: number of samples in IR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
alpha_clip_range = 0.1
if (v0 > y_ir + alpha_clip_range).any():
msg = "IRPOW ERROR: not enough power to get desired lattice depth"
print msg
bad = numpy.where(v0 > y_ir + alpha_clip_range)
timefail = int(bad[0][0]) * float(DL.ss)
msg = msg + "\nFirst bad sample = %d out of %d" % (bad[0][0], v0.size)
msg = msg + "\n t = %f " % timefail
msg = msg + "\n v0 = %f " % v0[bad[0][0]]
msg = msg + "\n ir = %f " % y_ir[bad[0][0]]
print v0[bad[0][0]]
print y_ir[bad[0][0]]
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
ax0.plot(xy_ir[:, 0], xy_ir[:, 1], 'x', color='darkorange', ms=5.)
ax0.plot(ir[:, 0], ir[:, 1], '.', mew=xymew, ms=xyms, color='darkorange')
ax0.plot(x_v0, y_ir, lw=lw, color='darkorange', label='irpow')
# Define how we want to ramp up the GR power
grwfms = {}
splmrkr = ['x', '+', 'd']
ptsmrkr = ['^', 's', 'p']
for i, grramp in enumerate([(DL.grpow1, DIMPLE.gr1pow2),
(DL.grpow2, DIMPLE.gr2pow2),
(DL.grpow3, DIMPLE.gr3pow2)]):
ramppts = grramp[0]
ramp0 = grramp[1]
print 'gr' + '%d' % i + ' offset = %f' % ramp0
gr_ramp, xy_gr, gr = interpolate_ramp(ramppts, yoffset=ramp0)
dt_gr = numpy.amax(gr[:, 0]) - numpy.amin(gr[:, 0])
N_gr = int(math.floor(dt_gr / DL.ss))
x_gr = numpy.arange(dt_gr / N_gr, dt_gr, dt_gr / N_gr)
y_gr = gr_ramp(x_gr)
if v0.size > y_gr.size:
y_gr = numpy.append(y_gr, (v0.size - y_gr.size) * [y_gr[-1]])
elif v0.size < y_gr.size:
y_gr = y_gr[0:v0.size]
if v0.size != y_gr.size:
msg = "GRPOW ERROR: number of samples in GR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
grwfms['greenpow' + '%1d' % (i + 1)] = y_gr
ax0.plot(xy_gr[:, 0],
xy_gr[:, 1],
marker=splmrkr[i],
mec='green',
mfc='None',
ms=3.)
ax0.plot(gr[:, 0],
gr[:, 1],
marker=ptsmrkr[i],
mew=xymew,
ms=xyms / 2.,
mfc='None',
mec='green') #, label='grpow dat')
ax0.plot(x_v0, y_gr, lw=lw, color='green', label='grpow')
for grch in grwfms.keys():
print grch, " = ", grwfms[grch].shape
ax0.set_xlim(left=-10., right=ax0.get_xlim()[1] * 1.1)
plt.setp(ax0.get_xticklabels(), visible=False)
ylim = ax0.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax0.set_ylim(ylim[0] - extra, ylim[1] + extra)
ax0.grid(True)
ax0.set_ylabel('$E_{r}$', size=16, labelpad=0)
ax0.yaxis.set_label_coords(labelx, 0.5)
ax0.set_title('Lattice Loading')
ax0.legend(loc='best', numpoints=1, prop={'size': legsz * 0.8})
# Define how we want to ramp up the scattering length (control our losses)
a_s_ramp, xy_a_s, a_s = interpolate_ramp(DL.a_s)
dt_a_s = numpy.amax(a_s[:, 0]) - numpy.amin(a_s[:, 0])
N_a_s = int(math.floor(dt_a_s / DL.ss))
x_a_s = numpy.arange(dt_a_s / N_a_s, dt_a_s, dt_a_s / N_a_s)
y_a_s = a_s_ramp(x_a_s)
if v0.size > y_a_s.size:
y_a_s = numpy.append(y_a_s, (v0.size - y_a_s.size) * [y_a_s[-1]])
elif v0.size < y_a_s.size:
y_a_s = y_a_s[0:v0.size]
if v0.size != y_a_s.size:
msg = "a_s ERROR: number of samples in a_s ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR', msg)
exit(1)
ax1.plot(xy_a_s[:, 0], xy_a_s[:, 1] / 100., 'x', color='#C10087', ms=5.)
ax1.plot(a_s[:, 0],
a_s[:, 1] / 100.,
'.',
mew=xymew,
ms=xyms,
color='#C10087')
ax1.plot(x_v0,
y_a_s / 100.,
lw=lw,
color='#C10087',
label=r'$a_s\mathrm{(100 a_{0})}$')
ax1.set_ylabel(r'$a_s\mathrm{(100 a_{0})}$', size=16, labelpad=0)
ax1.yaxis.set_label_coords(labelx, 0.5)
ax1.set_xlim(ax0.get_xlim())
ylim = ax1.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax1.set_ylim(ylim[0] - extra, ylim[1] + extra)
plt.setp(ax1.get_xticklabels(), visible=False)
ax1.grid(True)
ax1.legend(loc='best', numpoints=1, prop={'size': legsz})
#######################################################################
#### CALCULATED RAMPS: ALPHA, TUNNELING, SCATTERING LENGTH, BFIELD ###
#######################################################################
alpha = (v0 / y_ir)**2.
alpha_advance = 100.
N_adv = int(math.floor(alpha_advance / DL.ss))
alpha = alpha.clip(0., 1.)
alpha_desired = numpy.copy(alpha)
if N_adv < v0.size:
alpha = alpha[N_adv:]
alpha = numpy.append(alpha, (v0.size - alpha.size) * [alpha[-1]])
else:
alpha = numpy.array(v0.size * [alpha[-1]])
#alpha = alpha.clip(0., 1.)
ax2.plot(x_v0, alpha, lw=lw, color='saddlebrown', label='alpha adv')
ax2.plot(x_v0,
alpha_desired,
':',
lw=lw,
color='saddlebrown',
label='alpha')
ax2.set_xlim(ax0.get_xlim())
ax2.set_ylim(-0.05, 1.05)
plt.setp(ax2.get_xticklabels(), visible=False)
ax2.grid()
ax2.set_ylabel('$\\alpha$', size=16, labelpad=0)
ax2.yaxis.set_label_coords(labelx, 0.5)
ax2.legend(loc='best', numpoints=1, prop={'size': legsz})
tunneling_Er = physics.inv('t_to_V0', v0)
tunneling_kHz = tunneling_Er * 29.2
ax3.plot(x_v0, tunneling_kHz, lw=lw, color='red', label='$t$ (kHz)')
ax3.set_xlim(ax0.get_xlim())
ylim = ax3.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax3.set_ylim(ylim[0] - extra, ylim[1] + extra)
plt.setp(ax3.get_xticklabels(), visible=False)
ax3.grid(True)
ax3.set_ylabel(r'$t\,\mathrm{(kHz)}$', size=16, labelpad=0)
ax3.yaxis.set_label_coords(labelx, 0.5)
ax3.legend(loc='best', numpoints=1, prop={'size': legsz})
wannierF = physics.inv('wF_to_V0', v0)
bohrRadius = 5.29e-11 #meters
lattice_spacing = 1.064e-6 / 2. #meters
bfieldG = physics.cnv('as_to_B', y_a_s)
U_over_t = y_a_s * bohrRadius / lattice_spacing * wannierF / tunneling_Er
ax4.plot(x_v0, U_over_t, lw=lw, color='k', label=r'$U/t$')
ax4.set_xlim(ax0.get_xlim())
ylim = ax4.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax4.set_ylim(ylim[0] - extra, ylim[1] + extra)
plt.setp(ax4.get_xticklabels(), visible=False)
ax4.grid(True)
ax4.set_ylabel(r'$U/t$', size=16, labelpad=0)
ax4.yaxis.set_label_coords(labelx, 0.5)
ax4.legend(loc='best', numpoints=1, prop={'size': legsz})
ax5.plot(x_v0, bfieldG, lw=lw, color='purple', label='$B$ (G)')
ax5.set_xlim(ax0.get_xlim())
ylim = ax5.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax5.set_ylim(ylim[0] - extra, ylim[1] + extra)
ax5.grid(True)
plt.setp(ax5.get_xticklabels(), visible=False)
ax5.set_ylabel(r'$B\,\mathrm{(G)}$', size=16, labelpad=0)
ax5.yaxis.set_label_coords(labelx, 0.5)
ax5.legend(loc='best', numpoints=1, prop={'size': legsz})
ax6.plot(x_v0, (tunneling_Er / U_over_t),
lw=lw,
color='#25D500',
label=r'$t^{2}/U\,(E_{r)}$')
#ax6.set_yscale('log')
ax6.set_xlim(ax0.get_xlim())
ylim = ax6.get_ylim()
extra = (ylim[1] - ylim[0]) * 0.1
ax6.set_ylim(ylim[0] * 0.5, ylim[1])
ax6.grid(True)
ax6.set_ylabel(r'$t^{2}/U\,(E_{r)}$', size=16, labelpad=0)
ax6.yaxis.set_label_coords(labelx, 0.5)
ax6.legend(loc='best', numpoints=1, prop={'size': legsz})
ax6.set_xlabel('time (ms)')
figfile = seqconf.seqtxtout().split('.')[0] + '_latticeRamp.png'
plt.savefig(figfile, dpi=120)
#Save all ramps to a txt file for later plotting.
datfile = seqconf.seqtxtout().split('.')[0] + '_latticeRamp.dat'
allRamps = numpy.transpose(numpy.vstack((x_v0, v0, y_ir, grwfms['greenpow1'], y_a_s, alpha, alpha_desired, \
tunneling_kHz, U_over_t, bfieldG)))
header = '# Column index'
header = header + '\n#\t0\t' + 'time(ms)'
header = header + '\n#\t1\t' + 'Lattice Depth (Er)'
header = header + '\n#\t2\t' + 'Ir power (Er)'
header = header + '\n#\t3\t' + 'GR power (Er)'
header = header + '\n#\t4\t' + 'a_s (a0)'
header = header + '\n#\t5\t' + 'alpha - advance'
header = header + '\n#\t6\t' + 'alpha - desired'
header = header + '\n#\t7\t' + 'tunneling (kHz)'
header = header + '\n#\t8\t' + 'U/t'
header = header + '\n#\t9\t' + 'bfield (Gauss)'
header = header + '\n'
numpy.savetxt(datfile, allRamps)
with open(datfile, 'w') as f:
X = numpy.asarray(allRamps)
f.write(bytes(header))
format = '%.6e'
ncol = X.shape[1]
format = [
format,
] * ncol
format = ' '.join(format)
newline = '\n'
for row in X:
f.write(numpy.compat.asbytes(format % tuple(row) + newline))
shutil.copyfile(
figfile,
seqconf.savedir() + 'expseq' + seqconf.runnumber() +
'_latticeRamp.png')
shutil.copyfile(
datfile,
seqconf.savedir() + 'expseq' + seqconf.runnumber() +
'_latticeRamp.dat')
#plt.savefig( seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png', dpi=120)
#################################
#### APPEND RAMPS TO SEQUENCE ###
#################################
wfms = []
for ch in ['ir1pow', 'ir2pow', 'ir3pow']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv(ch, y_ir)
wfms.append(w)
for ch in ['greenpow1', 'greenpow2', 'greenpow3']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
correction = DIMPLE.__dict__['gr' + n + 'correct']
w.y = physics.cnv(ch, correction * grwfms[ch])
wfms.append(w)
for ch in ['lcr1', 'lcr2', 'lcr3']:
n = filter(str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
force = DL.__dict__['force_' + ch]
if force >= 0 and force <= 1:
print "...Forcing LCR%s = %f during lattice ramp" % (n, force)
w.y = physics.cnv(ch, numpy.array(alpha.size * [force]))
else:
w.y = physics.cnv(ch, alpha)
wfms.append(w)
bfieldA = bfieldG / 6.8
##ADD field
bfield = wfm.wave('bfield', 0.0, DL.ss)
bfield.y = physics.cnv('bfield', bfieldA)
wfms.append(bfield)
##ADD gradient field
gradient = gradient_wave('gradientfield', 0.0, DL.ss, volt=0.0)
gradient.follow(bfield)
wfms.append(gradient)
# RF sweep
if DL.rf == 1:
rfmod = wfm.wave('rfmod', 0., DL.ss)
rfmod.appendhold(bfield.dt() + DL.rftime)
rfmod.linear(DL.rfvoltf, DL.rfpulsedt)
wfms.append(rfmod)
#Take care of imaging frequencies, including various kill experiments
bfieldG = physics.inv('bfield', bfield.y[-1]) * 6.8
hfimg0 = -1. * (100.0 + 163.7 - 1.414 * bfieldG)
print "...ANDOR:hfimg and hfimg0 will be modified in report\n"
print "\tNEW ANDOR:hfimg = %.2f MHz" % (hfimg0 - DL.imgdet)
print "\tNEW ANDOR:hfimg0 = %.2f MHz\n" % hfimg0
gen.save_to_report('ANDOR', 'hfimg', hfimg0 - DL.imgdet)
gen.save_to_report('ANDOR', 'hfimg0', hfimg0)
newANDORhfimg = hfimg0 - DL.imgdet
# Kill hfimg
if DL.probekill == 1 or DL.braggkill == 1 or DL.lightassist or DL.lightassist_lock:
hfimgdelay = 50. #ms
analogimg = wfm.wave('analogimg', newANDORhfimg, DL.ss)
if DL.probekill == 1:
if (-DL.probekilltime + hfimgdelay) < DL.image:
analogimg.appendhold(bfield.dt() + DL.probekilltime -
hfimgdelay)
analogimg.linear(DL.probekill_hfimg, 0.0)
analogimg.appendhold(hfimgdelay + DL.probekilldt + 3 * DL.ss)
elif DL.braggkill == 1:
if (-DL.braggkilltime + hfimgdelay) < DL.image:
analogimg.appendhold(bfield.dt() + DL.braggkilltime -
hfimgdelay)
analogimg.linear(DL.braggkill_hfimg, 0.0)
analogimg.appendhold(hfimgdelay + DL.braggkilldt + 3 * DL.ss)
#elif DL.lightassist == 1 or DL.lightassist_lock:
# analogimg.appendhold( bfield.dt() - hfimgdelay)
# analogimg.linear( DL.lightassist_hfimg , 0.0)
# duration = DL.lightassist_lockdtUP + DL.lightassist_t0 + DL.lightassistdt + DL.lightassist_lockdtDOWN
# analogimg.appendhold( hfimgdelay + duration + 3*DL.ss)
analogimg.linear(newANDORhfimg, 0.)
analogimg.extend(10)
wfms.append(analogimg)
#analogimg = bfieldwfm.hfimg_wave('analogimg', ANDOR.hfimg, DL.ss)
#andorhfimg0 = analogimg.follow(bfield, DL.imgdet)
#wfms.append(analogimg)
# If we are doing round trip END, then mirror all the ramps
# before adding them to the sequence
if DL.round_trip == 1:
if DL.round_trip_type == 1:
maxdt = 0.
maxi = -1
for i, w in enumerate(wfms):
if w.dt() > maxdt:
maxdt = w.dt()
maxi = i
maxdt = maxdt + DL.wait_at_top / 2.
for w in wfms:
w.extend(maxdt)
if 'lcr' in w.name:
yvals = w.y
#Get the reverse of the alpha desired array
alpha_mirror = numpy.copy(alpha_desired[::-1])
#Add the wait at top part so that it has same length as yvals
if alpha_mirror.size > yvals.size:
print "Error making mirror ramp for LCR."
print "Program will exit."
exit(1)
alpha_mirror = numpy.append(
(yvals.size - alpha_mirror.size) * [alpha_mirror[0]],
alpha_mirror)
#This is how much the mirror ramp will be advanced
N_adv = int(math.floor(DL.lcr_mirror_advance / DL.ss))
if N_adv < alpha_mirror.size:
alpha_mirror = alpha_mirror[N_adv:]
alpha_mirror = numpy.append(
alpha_mirror, (yvals.size - alpha_mirror.size) *
[alpha_mirror[-1]])
else:
alpha_mirror = numpy.array(yvals.size *
[alpha_mirror[-1]])
w.y = numpy.concatenate(
(yvals, physics.cnv(w.name, alpha_mirror)))
else:
w.mirror()
w.appendhold(DL.wait_at_end)
N_adv = int(math.floor(alpha_advance / DL.ss))
alpha_desired = numpy.copy(alpha)
for wavefm in wfms:
print "%s dt = %f" % (wavefm.name, wavefm.dt())
#Wait the buffer for the lattice loading ramps before adding them
bufferdt = 20.
s.wait(bufferdt)
#Add lattice wfms
duration = s.analogwfm_add(DL.ss, wfms)
if DL.image < 2500.:
s.wait(duration)
else:
print "...DL.image = %f >= 2500. Digital seq extension will be used." % DL.image
s.wait(DL.image)
#Here give some buffer time to do lock, RF etc.
#It has to be minimum 5.0 ms
### Figure out when to turn interlock back on, using alpha information
#~ if duration > DL.t0 + DL.dt:
#~ s.wait(-DL.lattice_interlock_time)
#~ if DL.use_lattice_interlock == 1:
#~ s.digichg('latticeinterlockbypass',0)
#~ else:
#~ s.digichg('latticeinterlockbypass',1)
#~ s.wait( DL.lattice_interlock_time)
return s, y_ir[-1]
def dimple_to_lattice(s,cpowend):
print "----- LATTICE LOADING RAMPS -----"
# Find out which is the longest of the ramps we are dealing with:
maxX =max( [xdomain(DL.latticeV0)[1] ,\
xdomain(DL.irpow)[1],\
xdomain(DL.grpow1)[1],\
xdomain(DL.grpow2)[1],\
xdomain(DL.grpow3)[1],\
xdomain(DL.a_s)[1]] )
print "Largest x value = %.3f ms\n" % maxX
# We define the times for which all functions will be evaluated
# MIN TIME TO DO DIGITAL EXTENSION
DIGEXTENSION = 2050.
if DL.image >= DIGEXTENSION:
Xendtime = DIGEXTENSION
else:
Xendtime = DL.image
Nnew = int(math.floor( Xendtime / DL.ss) )
Xnew = numpy.arange( Xendtime/Nnew, DL.image, Xendtime/Nnew )
print "X array defined from dt:"
print "DL.ss =", DL.ss
print "x0 = ",Xnew[0]
print "xf = ",Xnew[-1]
print "xdt = ",Xnew[1]-Xnew[0]
print "%d samples" % Nnew
print 'x shape = ', Xnew.shape
# Define how we want to ramp up the lattice depth
v0_ramp, xy_v0, v0set = interpolate_ramp( DL.latticeV0)
v0 = v0_ramp(Xnew)
###########################################
#### AXIS DEFINITIONS FOR PLOTS ###
###########################################
fig = plt.figure( figsize=(4.5*1.05,8.*1.1))
ax0 = fig.add_axes( [0.18,0.76,0.76,0.20])
ax2 = fig.add_axes( [0.18,0.645,0.76,0.11])
ax3 = fig.add_axes( [0.18,0.53,0.76,0.11])
ax1 = fig.add_axes( [0.18,0.415,0.76,0.11])
ax5 = fig.add_axes( [0.18,0.30,0.76,0.11])
ax4 = fig.add_axes( [0.18,0.185,0.76,0.11])
ax6 = fig.add_axes( [0.18,0.07,0.76,0.11])
allax = [ax0, ax1, ax2, ax3, ax4, ax5, ax6]
for ax in allax:
ax.axvline( DL.image, linewidth = 1., color='black', alpha=0.6)
lw=1.5
labelx=-0.12
legsz =8.
xymew=0.5
xyms=9
ax0.plot( Xnew, v0, 'b', lw=2.5, label='Lattice depth')
ax0.plot(xy_v0[:,0],xy_v0[:,1], 'x', color='blue', ms=5.)
ax0.plot(v0set[:,0],v0set[:,1], '.', mew=xymew, ms=xyms, color='blue')
###########################################
#### USER DEFINED RAMPS: IR, GR, and U ###
###########################################
# Define how we want to ramp up the IR power
if DIMPLE.allirpow > 0.:
ir_offset = DIMPLE.allirpow
else:
ir_offset = DIMPLE.ir1pow2
ir_ramp, xy_ir, ir = interpolate_ramp( DL.irpow, yoffset=ir_offset)
dt_ir = numpy.amax( ir[:,0]) - numpy.amin( ir[:,0])
N_ir = int(math.floor( dt_ir / DL.ss ))
x_ir = numpy.arange( dt_ir/N_ir, dt_ir, dt_ir/N_ir)
y_ir = ir_ramp(Xnew)
if v0.size > y_ir.size:
y_ir = numpy.append(y_ir, (v0.size-y_ir.size)*[y_ir[-1]])
elif v0.size < y_ir.size:
y_ir = y_ir[0:v0.size]
if v0.size != y_ir.size:
msg = "IRPOW ERROR: number of samples in IR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
alpha_clip_range = 0.1
if (v0 > y_ir+ alpha_clip_range).any():
msg = "IRPOW ERROR: not enough power to get desired lattice depth"
print msg
bad = numpy.where( v0 > y_ir + alpha_clip_range)
timefail = int(bad[0][0])*float(DL.ss)
msg = msg + "\nFirst bad sample = %d out of %d" % (bad[0][0], v0.size)
msg = msg + "\n t = %f " % timefail
msg = msg + "\n v0 = %f " % v0[ bad[0][0] ]
msg = msg + "\n ir = %f " % y_ir[ bad[0][0] ]
print v0[bad[0][0]]
print y_ir[bad[0][0]]
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
ax0.plot(xy_ir[:,0],xy_ir[:,1], 'x', color='darkorange', ms=5.)
ax0.plot(ir[:,0],ir[:,1], '.', mew=xymew, ms=xyms, color='darkorange')
ax0.plot(Xnew, y_ir, lw=lw, color='darkorange',label='irpow')
# Define how we want to ramp up the GR power
grwfms = {}
splmrkr = ['x','+','d']
ptsmrkr = ['^','s','p']
for i,grramp in enumerate([(DL.grpow1,DIMPLE.gr1pow2), (DL.grpow2,DIMPLE.gr2pow2), (DL.grpow3,DIMPLE.gr3pow2)]):
ramppts = grramp[0]
ramp0 = grramp[1]
print 'gr'+'%d'%i +' offset = %f' % ramp0
gr_ramp, xy_gr, gr = interpolate_ramp( ramppts, yoffset=ramp0)
dt_gr = numpy.amax( gr[:,0]) - numpy.amin( gr[:,0])
N_gr = int(math.floor( dt_gr / DL.ss ))
x_gr = numpy.arange( dt_gr/N_gr, dt_gr, dt_gr/N_gr)
y_gr = gr_ramp(Xnew)
if DL.signal == 0:
y_gr = y_gr / 2.0
if v0.size > y_gr.size:
y_gr = numpy.append(y_gr, (v0.size-y_gr.size)*[y_gr[-1]])
elif v0.size < y_gr.size:
y_gr = y_gr[0:v0.size]
if v0.size != y_gr.size:
msg = "GRPOW ERROR: number of samples in GR ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
grwfms[ 'greenpow' + '%1d' % (i+1) ] = y_gr
ax0.plot(xy_gr[:,0],xy_gr[:,1], marker= splmrkr[i] ,mec='green', mfc='None', ms=3.)
ax0.plot(gr[:,0],gr[:,1], marker=ptsmrkr[i], mew=xymew, ms=xyms/2., mfc='None', mec='green')#, label='grpow dat')
ax0.plot(Xnew, y_gr, lw=lw, color='green', label='grpow')
for grch in grwfms.keys():
print grch, " = ", grwfms[grch].shape
ax0.set_xlim(left=-10., right= ax0.get_xlim()[1]*1.1)
plt.setp( ax0.get_xticklabels(), visible=False)
ylim = ax0.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax0.set_ylim( ylim[0]-extra, ylim[1]+extra )
ax0.grid(True)
ax0.set_ylabel('$E_{r}$',size=16, labelpad=0)
ax0.yaxis.set_label_coords(labelx, 0.5)
ax0.set_title('Lattice Loading')
ax0.legend(loc='best',numpoints=1,prop={'size':legsz*0.8})
# Define how we want to ramp up the scattering length (control our losses)
a_s_ramp, xy_a_s, a_s = interpolate_ramp( DL.a_s)
dt_a_s = numpy.amax( a_s[:,0]) - numpy.amin( a_s[:,0])
N_a_s = int(math.floor( dt_a_s / DL.ss ))
x_a_s = numpy.arange( dt_a_s/N_a_s, dt_a_s, dt_a_s/N_a_s)
y_a_s = a_s_ramp(Xnew)
if v0.size > y_a_s.size:
y_a_s = numpy.append(y_a_s, (v0.size-y_a_s.size)*[y_a_s[-1]])
elif v0.size < y_a_s.size:
y_a_s = y_a_s[0:v0.size]
if v0.size != y_a_s.size:
msg = "a_s ERROR: number of samples in a_s ramp and V0 ramp does not match!"
errormsg.box('LATTICE LOADING ERROR',msg)
exit(1)
ax1.plot(xy_a_s[:,0],xy_a_s[:,1]/100., 'x', color='#C10087', ms=5.)
ax1.plot(a_s[:,0],a_s[:,1]/100., '.', mew=xymew, ms=xyms, color='#C10087')
ax1.plot(Xnew, y_a_s/100., lw=lw, color='#C10087', label=r'$a_s\mathrm{(100 a_{0})}$')
ax1.set_ylabel(r'$a_s\mathrm{(100 a_{0})}$',size=16, labelpad=0)
ax1.yaxis.set_label_coords(labelx, 0.5)
ax1.set_xlim( ax0.get_xlim())
ylim = ax1.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax1.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax1.get_xticklabels(), visible=False)
ax1.grid(True)
ax1.legend(loc='best',numpoints=1,prop={'size':legsz})
#######################################################################
#### CALCULATED RAMPS: ALPHA, TUNNELING, SCATTERING LENGTH, BFIELD ###
#######################################################################
alpha = (v0/y_ir)**2.
alpha_advance = 100.
N_adv = int(math.floor( alpha_advance / DL.ss))
alpha = alpha.clip(0.,1.)
alpha_desired = numpy.copy(alpha)
if N_adv < v0.size:
alpha = alpha[N_adv:]
alpha = numpy.append(alpha, (v0.size-alpha.size)*[alpha[-1]])
else:
alpha = numpy.array( v0.size*[alpha[-1]] )
#alpha = alpha.clip(0., 1.)
ax2.plot( Xnew, alpha, lw=lw, color='saddlebrown', label='alpha adv')
ax2.plot( Xnew, alpha_desired,':', lw=lw, color='saddlebrown', label='alpha')
ax2.set_xlim( ax0.get_xlim())
ax2.set_ylim(-0.05,1.05)
plt.setp( ax2.get_xticklabels(), visible=False)
ax2.grid()
ax2.set_ylabel('$\\alpha$',size=16, labelpad=0)
ax2.yaxis.set_label_coords(labelx, 0.5)
ax2.legend(loc='best',numpoints=1,prop={'size':legsz})
tunneling_Er = physics.inv('t_to_V0', v0)
tunneling_kHz = tunneling_Er * 29.2
ax3.plot( Xnew, tunneling_kHz, lw=lw, color='red', label='$t$ (kHz)')
ax3.set_xlim( ax0.get_xlim())
ylim = ax3.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax3.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax3.get_xticklabels(), visible=False)
ax3.grid(True)
ax3.set_ylabel(r'$t\,\mathrm{(kHz)}$',size=16, labelpad=0)
ax3.yaxis.set_label_coords(labelx, 0.5)
ax3.legend(loc='best',numpoints=1,prop={'size':legsz})
wannierF = physics.inv('wF_to_V0', v0)
bohrRadius = 5.29e-11 #meters
lattice_spacing = 1.064e-6 / 2. #meters
bfieldG = physics.cnv('as_to_B', y_a_s)
print
print "The last value of the scattering length ramp is:"
print 'a_s =', y_a_s[-1]
print 'B =', bfieldG[-1]
print
U_over_t = y_a_s * bohrRadius / lattice_spacing * wannierF / tunneling_Er
ax4.plot( Xnew, U_over_t, lw=lw, color='k', label=r'$U/t$')
ax4.set_xlim( ax0.get_xlim())
ylim = ax4.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax4.set_ylim( ylim[0]-extra, ylim[1]+extra )
plt.setp( ax4.get_xticklabels(), visible=False)
ax4.grid(True)
ax4.set_ylabel(r'$U/t$',size=16, labelpad=0)
ax4.yaxis.set_label_coords(labelx, 0.5)
ax4.legend(loc='best',numpoints=1,prop={'size':legsz})
ax5.plot( Xnew, bfieldG, lw=lw, color='purple', label='$B$ (G)')
ax5.set_xlim( ax0.get_xlim())
ylim = ax5.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax5.set_ylim( ylim[0]-extra, ylim[1]+extra )
ax5.grid(True)
plt.setp( ax5.get_xticklabels(), visible=False)
ax5.set_ylabel(r'$B\,\mathrm{(G)}$',size=16, labelpad=0)
ax5.yaxis.set_label_coords(labelx, 0.5)
ax5.legend(loc='best',numpoints=1,prop={'size':legsz})
ax6.plot( Xnew, (tunneling_Er / U_over_t), lw=lw, color='#25D500', label=r'$t^{2}/U\,(E_{r)}$')
#ax6.set_yscale('log')
ax6.set_xlim( ax0.get_xlim())
ylim = ax6.get_ylim()
extra = (ylim[1]-ylim[0])*0.1
ax6.set_ylim( ylim[0]*0.5, ylim[1] )
ax6.grid(True)
ax6.set_ylabel(r'$t^{2}/U\,(E_{r)}$',size=16, labelpad=0)
ax6.yaxis.set_label_coords(labelx, 0.5)
ax6.legend(loc='best',numpoints=1,prop={'size':legsz})
ax6.set_xlabel('time (ms)')
figfile = seqconf.seqtxtout().split('.')[0]+'_latticeRamp.png'
plt.savefig(figfile , dpi=120 )
#Save all ramps to a txt file for later plotting.
datfile = seqconf.seqtxtout().split('.')[0]+'_latticeRamp.dat'
allRamps = numpy.transpose(numpy.vstack((Xnew, v0, y_ir, grwfms['greenpow1'], y_a_s, alpha, alpha_desired, \
tunneling_kHz, U_over_t, bfieldG)))
header = '# Column index'
header = header + '\n#\t0\t' + 'time(ms)'
header = header + '\n#\t1\t' + 'Lattice Depth (Er)'
header = header + '\n#\t2\t' + 'Ir power (Er)'
header = header + '\n#\t3\t' + 'GR power (Er)'
header = header + '\n#\t4\t' + 'a_s (a0)'
header = header + '\n#\t5\t' + 'alpha - advance'
header = header + '\n#\t6\t' + 'alpha - desired'
header = header + '\n#\t7\t' + 'tunneling (kHz)'
header = header + '\n#\t8\t' + 'U/t'
header = header + '\n#\t9\t' + 'bfield (Gauss)'
header = header + '\n'
numpy.savetxt( datfile, allRamps)
with open(datfile, 'w') as f:
X = numpy.asarray( allRamps )
f.write(bytes(header))
format = '%.6e'
ncol = X.shape[1]
format = [format ,] *ncol
format = ' '.join(format)
newline = '\n'
for row in X:
f.write(numpy.compat.asbytes(format % tuple(row) + newline))
shutil.copyfile( figfile, seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png')
shutil.copyfile( datfile, seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.dat')
#plt.savefig( seqconf.savedir() + 'expseq' + seqconf.runnumber() + '_latticeRamp.png', dpi=120)
#################################
#### APPEND RAMPS TO SEQUENCE ###
#################################
wfms=[]
if DL.signal == 0:
print " LOCK VALUE FOR SIGNAL / NOSIGNAL "
print " before = ", DL.lock_Er
DL.lock_Er = DL.lock_Er / 1.8
print " after = \n", DL.lock_Er
for ch in ['ir1pow','ir2pow','ir3pow']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv( ch, y_ir )
if DL.lock:
endval = w.y[-1]
w.insertlin_cnv(DL.lock_Er, DL.lock_dtUP, DL.lock_t0 )
elif DL.lightassist_lock:
endval = w.y[-1]
w.linear(DL.lightassist_lockpowIR, DL.lightassist_lockdtUP)
w.appendhold( DL.lightassist_t0 + DL.lightassistdt )
if DL.endvalIR >= 0.:
w.linear( DL.endvalIR, DL.lightassist_lockdtDOWN)
else:
w.linear( None, DL.lightassist_lockdtDOWN, volt=endval)
wfms.append(w)
for ch in ['greenpow1','greenpow2','greenpow3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
correction = DIMPLE.__dict__['gr'+n+'correct']
w.y = physics.cnv( ch, correction * grwfms[ch] )
if DL.lightassist_lock:
endval = w.y[-1]
w.linear(DL.lightassist_lockpowGR, DL.lightassist_lockdtUP)
w.appendhold( DL.lightassist_t0 + DL.lightassistdt )
if DL.endvalGR >= 0.:
w.linear( DL.endvalGR, DL.lightassist_lockdtDOWN)
else:
w.linear( None, DL.lightassist_lockdtDOWN, volt=endval)
wfms.append(w)
for ch in ['lcr1','lcr2','lcr3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
force = DL.__dict__['force_'+ch]
if force >= 0 and force <=1:
print "...Forcing LCR%s = %f during lattice ramp" % (n,force)
w.y = physics.cnv( ch, numpy.array( alpha.size*[force] ) )
elif DL.signal == 0:
print "...Forcing LCR%s = 0. so that it does NOT rotate to LATTICE" % n
w.y = physics.cnv( ch, numpy.array( alpha.size*[0.0] ) )
else:
w.y = physics.cnv( ch, alpha )
wfms.append(w)
bfieldA = bfieldG/6.8
##ADD field
bfield = wfm.wave('bfield', 0.0, DL.ss)
bfield.y = physics.cnv( 'bfield', bfieldA)
print "The last value of the bfield voltage is =", bfield.y[-1]
print
wfms.append(bfield)
##ADD gradient field
gradient = gradient_wave('gradientfield', 0.0, DL.ss,volt = 0.0)
gradient.follow(bfield)
wfms.append(gradient)
buffer = 40.
s.wait(buffer)
#~ odtpow = odt.odt_wave('odtpow', cpowend, DL.ss)
#~ if DIMPLE.odt_t0 > buffer :
#~ odtpow.appendhold( DIMPLE.odt_t0 - buffer)
#~ if DIMPLE.odt_pow < 0.:
#~ odtpow.appendhold( DIMPLE.odt_dt)
#~ else:
#~ odtpow.tanhRise( DIMPLE.odt_pow, DIMPLE.odt_dt, DIMPLE.odt_tau, DIMPLE.odt_shift)
#~ if numpy.absolute(DIMPLE.odt_pow) < 0.0001:
#~ s.wait( odtpow.dt() )
#~ s.digichg('odtttl',0)
#~ s.wait(-odtpow.dt() )
#~ wfms.append(odtpow)
# RF sweep
if DL.rf == 1:
rfmod = wfm.wave('rfmod', 0., DL.ss)
rfmod.appendhold( bfield.dt() + DL.rftime )
rfmod.linear( DL.rfvoltf, DL.rfpulsedt)
wfms.append(rfmod)
if DL.round_trip == 1:
bindex = 0 # Calculate detunings using starting field
else:
bindex = -1 # Calculate detunings using field at the end of ramps
bfieldG = physics.inv( 'bfield', bfield.y[bindex]) * 6.8
hfimg0 = -1.*(100.0 + 163.7 - 1.414*bfieldG)
# Find bindex for braggkill time
bindex_BK = math.floor(-DL.braggkilltime / bfield.ss)
bfieldG_BK = physics.inv( 'bfield', bfield.y[-1-bindex_BK]) * 6.8
hfimg0_BK = -1.*(100.0 + 163.7 - 1.414*bfieldG_BK)
DL.braggkill_hfimg = hfimg0_BK - DL.braggkill_hfimg
print "\n...Braggkill hfimg modification:\n"
print "\tNEW braggkill_hfimg = %.2f MHz" % DL.braggkill_hfimg
# Find bindex for bragg2kill time
bindex_B2K = math.floor(-DL.bragg2killtime / bfield.ss)
bfieldG_B2K = physics.inv( 'bfield', bfield.y[-1-bindex_B2K]) * 6.8
hfimg0_B2K = -1.*(100.0 + 163.7 - 1.414*bfieldG_B2K)
DL.bragg2kill_hfimg1 = hfimg0_B2K - DL.bragg2kill_hfimg1
DL.bragg2kill_hfimg2 = hfimg0_B2K - DL.bragg2kill_hfimg2
print "\n...Bragg2kill hfimg modification:\n"
print "\tNEW brag2gkill_hfimg1 = %.2f MHz" % DL.bragg2kill_hfimg1
print "\tNEW brag2gkill_hfimg2 = %.2f MHz" % DL.bragg2kill_hfimg2
print "\n...ANDOR:hfimg and hfimg0 will be modified in report\n"
print "\tNEW ANDOR:hfimg = %.2f MHz" % ( hfimg0 - DL.imgdet)
print "\tNEW ANDOR:hfimg0 = %.2f MHz\n" % hfimg0
gen.save_to_report('ANDOR','hfimg', hfimg0 - DL.imgdet)
gen.save_to_report('ANDOR','hfimg0', hfimg0)
newANDORhfimg = hfimg0 - DL.imgdet
# THIS DEFINES THE TIME IT TAKES THE OFFSET LOCK TO SWITCH TO
# A NEW SETPOINT
hfimgdelay = 50. #ms
# Kill hfimg
if DL.probekill ==1 or DL.braggkill ==1 or DL.bragg2kill==1 or DL.lightassist or DL.lightassist_lock:
analogimg = wfm.wave('analogimg', newANDORhfimg, DL.ss)
if DL.probekill == 1:
if (-DL.probekilltime+hfimgdelay) < DL.image:
analogimg.appendhold( bfield.dt() + DL.probekilltime - hfimgdelay)
analogimg.linear( DL.probekill_hfimg , 0.0)
analogimg.appendhold( hfimgdelay + DL.probekilldt + 3*DL.ss)
elif DL.braggkill == 1:
print "Setting up analogimg for braggkill"
if (-DL.braggkilltime+hfimgdelay) < DL.image:
analogimg.appendhold( bfield.dt() + DL.braggkilltime - hfimgdelay)
analogimg.linear( DL.braggkill_hfimg , 0.0)
analogimg.appendhold( hfimgdelay + DL.braggkilldt + 3*DL.ss)
elif DL.bragg2kill == 1:
print "Setting up analogimg for bragg2kill"
if (-DL.bragg2killtime+hfimgdelay) < DL.image:
# This sets up the detuning for the first pulse
analogimg.appendhold( bfield.dt() + DL.bragg2killtime - hfimgdelay)
analogimg.linear( DL.bragg2kill_hfimg1 , 0.0)
analogimg.appendhold( hfimgdelay + DL.bragg2killdt + 3*DL.ss)
# Then set up the detuning for the second pulse
analogimg.linear( DL.bragg2kill_hfimg2 , 0.0)
analogimg.appendhold( hfimgdelay + DL.bragg2killdt + 3*DL.ss)
elif DL.lightassist == 1 or DL.lightassist_lock:
analogimg.appendhold( bfield.dt() - hfimgdelay)
analogimg.linear( DL.lightassist_hfimg , 0.0)
duration = DL.lightassist_lockdtUP + DL.lightassist_t0 + DL.lightassistdt + DL.lightassist_lockdtDOWN
analogimg.appendhold( hfimgdelay + duration + 3*DL.ss)
analogimg.linear( newANDORhfimg, 0.)
analogimg.extend(10)
wfms.append(analogimg)
#analogimg = bfieldwfm.hfimg_wave('analogimg', ANDOR.hfimg, DL.ss)
#andorhfimg0 = analogimg.follow(bfield, DL.imgdet)
#wfms.append(analogimg)
# If we are doing round trip END, then mirror all the ramps
# before adding them to the sequence
if DL.round_trip == 1:
if DL.round_trip_type == 1:
maxdt = 0.
maxi = -1
for i,w in enumerate(wfms):
if w.dt() > maxdt:
maxdt = w.dt()
maxi = i
maxdt = maxdt + DL.wait_at_top / 2.
for w in wfms:
w.extend(maxdt)
if 'lcr' in w.name:
yvals = w.y
#Get the reverse of the alpha desired array
alpha_mirror = numpy.copy(alpha_desired[::-1])
#Add the wait at top part so that it has same length as yvals
if alpha_mirror.size > yvals.size:
print "Error making mirror ramp for LCR."
print "Program will exit."
exit(1)
alpha_mirror = numpy.append( (yvals.size - alpha_mirror.size)*[ alpha_mirror[0] ], alpha_mirror )
#This is how much the mirror ramp will be advanced
N_adv = int(math.floor( DL.lcr_mirror_advance / DL.ss))
if N_adv < alpha_mirror.size:
alpha_mirror = alpha_mirror[N_adv:]
alpha_mirror = numpy.append(alpha_mirror, (yvals.size-alpha_mirror.size)*[alpha_mirror[-1]])
else:
alpha_mirror = numpy.array( yvals.size*[alpha_mirror[-1]] )
w.y = numpy.concatenate((yvals,physics.cnv( w.name, alpha_mirror )))
else:
w.mirror()
w.appendhold( DL.wait_at_end)
N_adv = int(math.floor( alpha_advance / DL.ss))
alpha_desired = numpy.copy(alpha)
for wavefm in wfms:
print "%s dt = %f" % (wavefm.name, wavefm.dt())
duration = s.analogwfm_add(DL.ss,wfms)
if DL.image < DIGEXTENSION:
s.wait(duration)
else:
print "...DL.image = %f >= %.2f Digital seq extension will be used." % (DL.image, DIGEXTENSION)
s.wait( DL.image )
### Prepare the parts of the ramps that are going to be used to mock
### the conditions for the noatoms shot
### 1. get dt = [noatoms] ms from the end of the lattice ramps.
if 'manta' in DL.camera:
noatomsdt = MANTA.noatoms
else:
noatomsdt = ANDOR.noatoms
noatomswfms = []
for wavefm in wfms:
cp = copy.deepcopy( wavefm )
cp.idnum = time.time()*100
cp.retain_last( DL.bgRetainDT )
noatomswfms.append( cp )
### Figure out when to turn interlock back on, using alpha information
#~ if duration > DL.t0 + DL.dt:
#~ s.wait(-DL.lattice_interlock_time)
#~ if DL.use_lattice_interlock == 1:
#~ s.digichg('latticeinterlockbypass',0)
#~ else:
#~ s.digichg('latticeinterlockbypass',1)
#~ s.wait( DL.lattice_interlock_time)
#########################################
## OTHER TTL EVENTS: probekill, braggkill, rf, quick2
#########################################
# Braggkill
if DL.braggkill == 1:
print "Using Bragg Kill"
s.wait( DL.braggkilltime)
s = manta.OpenShutterBragg(s,DL.shutterdelay)
s.digichg('bragg',1)
s.wait( DL.braggkilldt)
s.digichg('brshutter',1) # to close shutter
s.digichg('bragg',0)
s.wait( -DL.braggkilldt)
s.wait( -DL.braggkilltime )
if DL.bragg2kill == 1:
print "Using Bragg 2 Kill"
tcur = s.tcur
s.wait( DL.bragg2killtime )
s = manta.OpenShutterBragg(s,DL.shutterdelay)
s.digichg('bragg',1)
s.wait( DL.bragg2killdt)
s.digichg('brshutter',1) # to close shutter
s.digichg('bragg',0)
s.wait( hfimgdelay + 3*DL.ss )
s = manta.OpenShutterBragg(s,DL.shutterdelay)
s.digichg('bragg',1)
s.wait( DL.bragg2killdt)
s.digichg('brshutter',1) # to close shutter
s.digichg('bragg',0)
# Revert to current time after pulses have been added in the past
s.tcur = tcur
# Probe Kill
if DL.probekill == 1:
s.wait(DL.probekilltime)
s.wait(-10)
s.digichg('prshutter',0)
s.wait(10)
s.digichg('probe',1)
s.wait(DL.probekilldt)
s.digichg('probe',0)
s.digichg('prshutter',1)
s.wait(-DL.probekilltime)
# Pulse RF
if DL.rf == 1:
s.wait(DL.rftime)
s.digichg('rfttl',1)
s.wait(DL.rfpulsedt)
s.digichg('rfttl',0)
s.wait(-DL.rfpulsedt)
s.wait(-DL.rftime)
# QUICK2
if DL.quick2 == 1:
s.wait( DL.quick2time)
s.digichg('quick2',1)
s.wait(-DL.quick2time)
# Light-assisted collisions
if DL.lightassist == 1 or DL.lightassist_lock:
s.wait( -DL.lightassist_lockdtUP -DL.lightassist_t0 -DL.lightassistdt -DL.lightassist_lockdtDOWN - 3*DL.ss)
s.wait(DL.lightassist_lockdtUP + DL.lightassist_t0)
s.wait(-10)
s.digichg('prshutter',0)
s.wait(10)
s.digichg('probe', DL.lightassist)
s.wait(DL.lightassistdt)
s.digichg('probe',0)
s.digichg('prshutter',1)
s.wait(DL.lightassist_lockdtDOWN)
s.wait(3*DL.ss)
# After the collisions happen we still need to wait some time
# for the probe frequency to come back to the desired value
s.wait(hfimgdelay)
#########################################
## GO BACK IN TIME IF DOING ROUND-TRIP START
#########################################
if DL.round_trip == 1:
if DL.round_trip_type == 0:
s.wait( -DL.image )
s.stop_analog()
#########################################
## TURN GREEN OFF BEFORE PICTURES
#########################################
if DL.greenoff == 1:
s.wait( DL.greenoff_t0 )
s.digichg('greenttl1', 0)
s.digichg('greenttl2', 0)
s.digichg('greenttl3', 0)
s.wait(-DL.greenoff_t0 )
#########################################
## LATTICE LOCK WITH POSSIBILITY OF RF
#########################################
bufferdt = 5.0
lastIR = y_ir[-1]
lockwfms=[]
if DL.locksmooth == 1 and DL.lock == 0:
s.wait(bufferdt)
for ch in ['ir1pow','ir2pow','ir3pow']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, lastIR, DL.lockss) #Start value will be overrriden
w.tanhRise( DL.lock_Er, DL.lock_dtUP, 0.4,0.2)
lockwfms.append(w)
print "...LOCKING LATTICE TO %f Er" % DL.lock_Er
print "...lastIR = %.4f" % lastIR
duration = s.analogwfm_add(DL.lockss,lockwfms)
print "...duration = %.2f" % duration
s.wait(duration)
#~ if DL.lockrf:
#~ s.digichg('rfttl',1)
#~ s.wait(DL.rfpulsedt)
#~ s.digichg('rfttl',0)
#~ s.wait(0.036)
#else:
# s.wait(bufferdt)
lockwfmscopy = []
for wavefm in lockwfms:
cp = copy.deepcopy( wavefm )
cp.idnum = time.time()*100 + 1e3*numpy.random.randint(0,1e8)
lockwfmscopy.append( cp )
#########################################
## IMAGING AT LOW FIELD
#########################################
if DL.lowfieldimg == 1:
s.wait(DL.lowfieldimg_t0)
s.digichg('field',0)
s.wait(-DL.lowfieldimg_t0)
#########################################
## TTL RELEASE FROM ODT and LATTICE
#########################################
#INDICATE WHICH CHANNELS ARE TO BE CONSIDERED FOR THE BACKGROUND
bg = ['odtttl','irttl1','irttl2','irttl3','greenttl1','greenttl2','greenttl3']
bgdictPRETOF={}
for ch in bg:
bgdictPRETOF[ch] = s.digistatus(ch)
bgdictPRETOF['tof'] = DL.tof
print "\nChannel status for pictures: PRE-TOF"
print bgdictPRETOF
print
#RELEASE FROM LATTICE
if DL.tof <= 0.:
s.wait(1.0+ANDOR.exp)
s.digichg('greenttl1',0)
s.digichg('greenttl2',0)
s.digichg('greenttl3',0)
s.digichg('irttl1',0)
s.digichg('irttl2',0)
s.digichg('irttl3',0)
#RELEASE FROM IR TRAP
s.digichg('odtttl',0)
if DL.tof <= 0.:
s.wait(-1.0+ANDOR.exp)
print "TIME WHEN RELEASED FROM LATTICE = ",s.tcur
s.wait(DL.tof)
return s, noatomswfms, lockwfmscopy, bgdictPRETOF
def do_roundtrip( s, wfms ):
""" creates roundtrips to characterize cooling in lattice.
wfms are the lattice wfms, they can be mirrored here if a mirror
ramp is desired. """
s.wait( RT.wait_at_top)
# This case is for mirrored ramps
if RT.mirror == 1 :
alpha_desired = wfms[1]
wfms = wfms[0]
mirrorwfms = []
for wavefm in wfms:
cp = copy.deepcopy( wavefm )
cp.idnum = time.time()*100
mirrorwfms.append( cp )
for w in mirrorwfms:
if 'lcr' in w.name:
yvals = w.y
# Get the reverse of the alpha desired array
alpha_mirror = numpy.copy(alpha_desired[::-1])
makeplot( [w, alpha_mirror], name=w.name )
# It needs to have the same length as yvals, so append
# constant samples at the beginning if needed
if alpha_mirror.size > yvals.size:
print "Error making mirror ramp for LCR."
print "Program will exit."
exit(1)
alpha_mirror = numpy.append( (yvals.size - alpha_mirror.size)*[ alpha_mirror[0] ], alpha_mirror )
# This is how much the mirror ramp will be advanced
N_adv = int(math.floor( RT.lcr_mirror_advance / DL.ss))
if N_adv < alpha_mirror.size:
alpha_mirror = alpha_mirror[N_adv:]
alpha_mirror = numpy.append(alpha_mirror, (yvals.size-alpha_mirror.size)*[alpha_mirror[-1]])
else:
alpha_mirror = numpy.array( yvals.size*[alpha_mirror[-1]] )
if RT.lcr_snap == 1:
alpha_mirror[ alpha_mirror > 0.01 ] = 1.
w.y = physics.cnv( w.name, alpha_mirror)
else:
w.y = w.y[::-1]
w.appendhold( RT.wait_at_end)
wfms = mirrorwfms
# This case is for custom ramps
else:
# There need to be 10 waveforms
# 3IR, 3LCR, 3GR, BFIELD
# This follows the procedure done for the lattice ramps
Xendtime = float( RT.image )
Nnew = int(math.floor( Xendtime / DL.ss) )
Xnew = numpy.arange( Xendtime/Nnew, RT.image, Xendtime/Nnew )
ir_ramp, xy_ir, ir = lattice.interpolate_ramp( RT.irpow, yoffset=0.)
y_ir = ir_ramp(Xnew)
grwfms = {}
for i,grramp in enumerate([RT.grpow1, RT.grpow2, RT.grpow3]):
gr_ramp, xy_gr, gr = lattice.interpolate_ramp( grramp, yoffset=0.)
y_gr = gr_ramp(Xnew)
grwfms[ 'greenpow' + '%1d' % (i+1) ] = y_gr
alpha_ramp, xy_alpha, alpha = lattice.interpolate_ramp( RT.alpha, yoffset=0. )
y_alpha = alpha_ramp(Xnew)
wfms = []
for ch in ['ir1pow', 'ir2pow', 'ir3pow']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
w.y = physics.cnv( ch, y_ir )
wfms.append(w)
for ch in ['greenpow1','greenpow2','greenpow3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
correction = DIMPLE.__dict__['gr'+n+'correct']
w.y = physics.cnv( ch, correction * grwfms[ch] )
wfms.append(w)
for ch in ['lcr1','lcr2','lcr3']:
n = filter( str.isdigit, ch)[0]
w = wfm.wave(ch, 0.0, DL.ss) #Start value will be overrriden
print "Obtaining LCR waveform for ROUNDTRIP..."
print y_alpha
w.y = physics.cnv( ch, y_alpha )
wfms.append(w)
##ADD field
bfieldG = physics.cnv('as_to_B', DL.knob05)
bfieldA = bfieldG/6.8
bfield = wfm.wave('bfield', bfieldA, DL.ss)
bfield.extend( wfms[-1].dt() )
wfms.append(bfield)
# Include ramp to zerocrossing, valid for mirror and custom cases
# Final field can be given in amps (default) or in a0
if RT.enable_zc == 1 :
if isinstance(RT.zc_bias, str):
if 'a0' in RT.zc_bias:
print "Using scattering length units for final field"
scattlen = float(re.sub('a0','', RT.zc_bias))
bfieldG = physics.cnv('as_to_B', scattlen)
bfieldA = bfieldG/6.8
elif 'knob05' in RT.zc_bias:
print "Using knob05 as the final scattering length, amounts to no change"
bfieldG = physics.cnv('as_to_B', DL.knob05)
bfieldA = bfieldG/6.8
else:
bfieldA = RT.zc_bias
bfieldG = bfieldA*6.8
else:
print "Using knob05 as the final scattering length, amounts to no change"
bfieldG = physics.cnv('as_to_B', DL.knob05)
bfieldA = bfieldG/6.8
# Set hfimg value for the given final field
hfimg0 = -1.*(100.0 + 163.7 - 1.414*bfieldG)
print "\n...ANDOR:hfimg and hfimg0 will be modified in report\n"
print "\tNEW ANDOR:hfimg = %.2f MHz" % ( hfimg0 - RT.imgdet)
print "\tNEW ANDOR:hfimg0 = %.2f MHz\n" % hfimg0
gen.save_to_report('ANDOR','hfimg', hfimg0 - RT.imgdet)
gen.save_to_report('ANDOR','hfimg0', hfimg0)
newANDORhfimg = hfimg0 - RT.imgdet
for w in wfms:
if 'bfield' in w.name:
bfieldw = w
if RT.enable_zc == 1 :
if RT.zc_mirror_t0 < 0.:
dt = w.dt()
w.chop( w.dt() + RT.zc_mirror_t0 )
if RT.zc_mirror_t0 > 0.:
w.appendhold( RT.zc_mirror_t0 )
w.linear( bfieldA, RT.zc_mirror_rampdt)
w.appendhold( RT.zc_mirror_holddt )
for i,w in enumerate(wfms):
if 'gradientfield' in w.name:
gradientfield_i = i
print "REMOVING GRADIENT FIELD"
print len(wfms)
wfms = [ w for w in wfms if w.name != 'gradientfield' ]
print len(wfms)
#Add gradientfield ramp to have levitation all the time
from bfieldwfm import gradient_wave
gradient = gradient_wave('gradientfield', 0.0, bfieldw.ss,volt = 0.0)
gradient.follow( bfieldw)
wfms.append(gradient)
duration = s.analogwfm_add(DL.ss,wfms)
s.wait(duration)
### Prepare the parts of the ramps that are going to be used to mock
### the conditions for the noatoms shot
### 1. get dt = [noatoms] ms from the end of the lattice ramps.
if 'manta' in DL.camera:
noatomsdt = MANTA.noatoms
else:
noatomsdt = ANDOR.noatoms
noatomswfms = []
for wavefm in wfms:
cp = copy.deepcopy( wavefm )
cp.idnum = time.time()*100
cp.retain_last( DL.bgRetainDT )
noatomswfms.append( cp )
#INDICATE WHICH CHANNELS ARE TO BE CONSIDERED FOR THE BACKGROUND
bg = ['odtttl','irttl1','irttl2','irttl3','greenttl1','greenttl2','greenttl3']
bgdictPRETOF={}
for ch in bg:
bgdictPRETOF[ch] = s.digistatus(ch)
bgdictPRETOF['tof'] = RT.tof
print "\nChannel status for pictures: PRE-TOF"
print bgdictPRETOF
print
#RELEASE FROM LATTICE
if RT.tof <= 0.:
s.wait(1.0+ANDOR.exp)
s.digichg('greenttl1',0)
s.digichg('greenttl2',0)
s.digichg('greenttl3',0)
s.digichg('irttl1',0)
s.digichg('irttl2',0)
s.digichg('irttl3',0)
#RELEASE FROM IR TRAP
s.digichg('odtttl',0)
if RT.tof <= 0.:
s.wait(-1.0+ANDOR.exp)
print "TIME WHEN RELEASED FROM LATTICE = ",s.tcur
s.wait(RT.tof)
return s, noatomswfms, bgdictPRETOF