def get_trace(self, channel):
"""Get a trace.
Args:
channel (int): Which channel to get.
Returns:
(ValueArray[s]): Time axis.
(ValueArray[V]): Voltage axis.
"""
word_length = 2
yield self.write(':WAV:SOUR CHAN{}'.format(channel))
yield self.write(':WAV:MSBF')
yield self.write(':SING')
preamble_raw = yield self.query(':WAV:PRE?')
preamble = parse_preamble(preamble_raw)
yield self.write(':WAV:FORM WORD')
yield self.write(':WAV:DATA?')
wave_bin = yield self.read_raw()
wave_raw = parse_binary_waveform(wave_bin, word_length=word_length)
y_incriment = preamble['y_incriment']
y_origin = preamble['y_origin']
y_reference = preamble['y_reference']
wave_volts = ((wave_raw - y_reference) * y_incriment) + y_origin
x_incriment = preamble['x_incriment']
x_origin = preamble['x_origin']
num_points = preamble['num_points']
time_s = np.linspace(x_origin,
x_origin + (num_points - 1) * x_incriment,
num_points)
returnValue((time_s * U.Unit('s'), wave_volts * U.Unit('V')))
def dep_coupling_factor_no_s(eta_c, N, d):
"""Coupling factor for two qubits, ignoring the self-inductance adjustment
Args:
eta_c (float): Coupling efficiency, i.e. the ratio M/L where M is the
mutual inductance and L is the self inductance.
N (int): Number of qubits you wish to couple to a single qubit.
d (np.ndarray): Structured data array, with named columns.
Returns (float):
The dimensionless part of the qubit-qubit coupling. Multiply by omega_LC
to get a coupling frequency.
The qubit-qubit coupling is written
J / hbar = [s (eta_c / N) (R_K / (8 pi Z_LC)) <0|phi|1>^2] omega_LC
The part in [..] is the "coupling factor", a dimensionless parameter. The s
factor is defined as (1 - M^2 / (L1 L2))^-1 and is near unity, so we ignore
it.
See the annealer-handbook for a full development of the coupling strength
formula.
"""
Z_LC = d['Z_LC'] * U.Unit(LABELS['Z_LC'][1])
f_LC = d['f_LC'] * U.Unit(LABELS['f_LC'][1])
phi_10 = d['phi_10']
return (eta_c / N) * (R_K / (8 * np.pi * Z_LC)) * phi_10**2
def handleUnitConversion(self):
""" Note that we only do unit conversion for the (shared) X-axis. """
import labrad.units as U
newUnit = str(self.xAxisUnitsLE.text()).strip()
currentUnit = U.Unit(self.xAxisCurrentUnit)
originalUnit = U.Unit(self.variables[0][0][1])
if not newUnit:
newUnit = self.variables[0][0][1]
# if we change units, convert old data
if newUnit != self.xAxisCurrentUnit:
try:
conversion = currentUnit.conversionTupleTo(newUnit)
self.data[:, 0] = (self.data[:, 0] +
conversion[1]) * conversion[0]
if self.xAxisZero is not None:
self.xAxisZero = (self.xAxisZero +
conversion[1]) * conversion[0]
self.xAxisCurrentUnit = newUnit
for figure in self.figures.values():
figure.axes[0].set_xlabel(
'%s [%s]' %
(self.variables[0][0][0], self.xAxisCurrentUnit))
self.dirtyPlots = True
except TypeError:
pass
# run new data through conversion
if self.newData is not None and self.newData.shape[0] > 0:
conversion = originalUnit.conversionTupleTo(self.xAxisCurrentUnit)
self.newData[:, 0] = (self.newData[:, 0] +
conversion[1]) * conversion[0]
def T1_us(d, M):
f_LC = d['f_LC'][0] * U.Unit(LABELS['f_LC'][1])
Z_LC = d['Z_LC'][0] * U.Unit(LABELS['Z_LC'][1])
f_10 = d['f_10'][0] * U.Unit(LABELS['f_LC'][1])
phi_10 = d['phi_10'][0]
R = 50 * Ohm
Q = 4 * np.pi * (R / R_K) * (Z_LC /
(2 * np.pi * f_LC * M))**2 / (phi_10**2)
return (Q / (2 * np.pi * f_10))['us']
def testInfNan(self):
ms = units.Unit('ms')
GHz = units.Unit('GHz')
MHz = units.Unit('MHz')
self.assertEquals(float('inf') * GHz, float('inf') * MHz)
self.assertNotEqual(float('inf') * GHz, float('inf') * ms)
self.assertNotEqual(float('inf') * GHz, -float('inf') * GHz)
self.assertNotEqual(float('nan') * GHz, float('nan') * GHz)
self.assertNotEqual(float('nan') * GHz, float('nan') * ms)
def testArithmetic(self):
m = units.Unit('m')
kg = units.Unit('kg')
self.assertEquals(units.Value(5.0, None)*m, 5.0*m)
# addition
self.assertEquals(1.0*kg + 0.0, 1.0*kg)
self.assertNotEquals(1.0*kg, None)
def testTypeConversions(self):
m = units.Unit('m')
V = units.Unit('V')
GHz = units.Unit('GHz')
x1 = 1.0 * m
x2 = 5j * V
a = np.arange(10) * 1.0
va = units.ValueArray(np.arange(10) * 1.0, 'GHz')
# Unit times number
self.assertIsInstance(1.0 * m, units.Value)
self.assertIsInstance(1 * m, units.Value)
self.assertIsInstance(m * 1.0, units.Value)
self.assertIsInstance(m * 1, units.Value)
# Value times value or number
self.assertIsInstance(x1 * x1, units.Value)
self.assertIsInstance(x1 * 5, units.Value)
self.assertIsInstance(0 * x1, units.Value)
# Unit times complex
self.assertIsInstance((1 + 1j) * V, units.Complex)
self.assertIsInstance(V * (1 + 1j), units.Complex)
# Value times Complex/complex
self.assertIsInstance(x1 * 1j, units.Complex)
self.assertIsInstance(1j * x1, units.Complex)
self.assertIsInstance(x2 * x1, units.Complex)
self.assertIsInstance(x1 * x2, units.Complex)
# Unit/Value/ValueArray times array
self.assertIsInstance(x1 * a, units.ValueArray)
self.assertIsInstance(x2 * a, units.ValueArray)
self.assertIsInstance(GHz * a, units.ValueArray)
self.assertIsInstance(va * a, units.ValueArray)
# Unit/Value/ValueArray times ValueArray
self.assertIsInstance(x1 * va, units.ValueArray)
self.assertIsInstance(x2 * va, units.ValueArray)
self.assertIsInstance(GHz * va, units.ValueArray)
self.assertIsInstance(va * va, units.ValueArray)
# array times ?
self.assertIsInstance(a * x1, units.ValueArray)
self.assertIsInstance(a * x2, units.ValueArray)
self.assertIsInstance(a * GHz, units.ValueArray)
self.assertIsInstance(a * va, units.ValueArray)
# ValueArray times ?
self.assertIsInstance(va * x1, units.ValueArray)
self.assertIsInstance(va * x2, units.ValueArray)
self.assertIsInstance(va * GHz, units.ValueArray)
self.assertIsInstance(va * a, units.ValueArray)
def testDimensionless(self):
ns = units.Unit('ns')
GHz = units.Unit('GHz')
self.assertTrue(isinstance((5 * ns) * (5 * GHz), float))
self.assertTrue(hasattr((5 * ns) * (5 * GHz), 'inUnitsOf'))
self.assertTrue(((5 * ns) * (5 * GHz)).isDimensionless())
self.assertTrue((5 * ns) * (5 * GHz) < 50)
self.assertTrue(
isinstance(units.WithUnit(5.0, ''), units.DimensionlessFloat))
self.assertTrue((5 * ns * 5j * GHz) == 25j)
self.assertTrue((5 * ns * 5j * GHz).isDimensionless())
def dep_tunnelling_time_times_f_LC(which, d):
"""Tunneling time normalized to f_LC
Args:
d (np.ndarray): Structured data array with named columns.
Returns (float):
Tunneling time multiplied by f_LC.
"""
f_LC = d['f_LC'] * U.Unit(LABELS['f_LC'][1])
Z_LC = d['Z_LC'] * U.Unit(LABELS['Z_LC'][1])
phi_well = d[which]
phi_barrier = d['phi_max']
return tunnel_time_times_f_LC(f_LC, Z_LC, phi_well, phi_barrier, d['beta'],
d['phi_x'])
def testPickling(self):
ns = units.Unit('ns')
GHz = units.Unit('GHz')
blank = units.Unit('')
def round_trip(obj):
return pickle.loads(pickle.dumps(obj))
self.assertEqual(round_trip(5 * GHz), 5 * GHz) # Value
self.assertEqual(round_trip(GHz), GHz) # Unit
self.assertTrue((round_trip(np.arange(5) * ns) == np.arange(5) *
ns).all()) # array
self.assertEqual(round_trip(5 * GHz * ns), 5) # Dimensionless
self.assertIsInstance(round_trip(3 * blank), type(
3 * blank)) # Don't loose dimensionless type
def testArithmetic(self):
m = units.Unit('m')
kg = units.Unit('kg')
km = units.Unit('km')
#self.assertEqual(units.Value(5.0, None)*m, 5.0*m)
# addition
self.assertEqual(1.0 * kg + 0.0, 1.0 * kg)
with self.assertRaises(TypeError):
_ = 1.0 * kg + 1.0 * m
with self.assertRaises(TypeError):
_ = 1.0 * kg + 2.0
self.assertAlmostEqual(1.0 * km / m + 5.0, 1005)
self.assertNotEqual(1.0 * kg, None)
def dep_number_of_states(which, d):
"""Number of states in a well
Args:
which (string): 'phi_left' or 'phi_right', indicating which well to
analyze.
d (np.ndarray): Structured data array with named columns.
Returns (float):
Number of states in the well.
"""
f_LC = d['f_LC'] * U.Unit(LABELS['f_LC'][1])
Z_LC = d['Z_LC'] * U.Unit(LABELS['Z_LC'][1])
phi = d[which]
return number_of_states(f_LC, Z_LC, phi, d['phi_max'], d['phi_x'],
d['beta'])
def horiz_position(self, position=None):
horiz_scale = yield self.horiz_scale()
if position is not None:
pos = position * horiz_scale
yield self.write(':TIM:POS {}'.format(-pos['s']))
resp = yield self.query(':TIM:POS?')
returnValue(-float(resp) * U.Unit('s') / horiz_scale)
def testComplex(self):
V = units.Unit('V')
self.assertTrue(1j * V != 1.0 * V)
self.assertTrue(1j * V == 1.0j * V)
self.assertTrue(1.0 * V == (1 + 0j) * V)
with self.assertRaises(TypeError):
_ = 1.0j * V < 2j * V
def testComparison(self):
s = units.Unit('s')
ms = units.Unit('ms')
kg = units.Unit('kg')
self.assertTrue(1 * s > 10 * ms, '1*s > 10*ms')
self.assertTrue(1 * s >= 10 * ms, '1*s >= 10*ms')
self.assertTrue(1 * s < 10000 * ms, '1*s > 10000*ms')
self.assertTrue(1 * s <= 10000 * ms, '1*s >= 10000*ms')
self.assertTrue(10 * ms < 1 * s, '10*ms < 1*s')
self.assertTrue(10 * ms <= 1 * s, '10*ms <= 1*s')
self.assertTrue(10000 * ms > 1 * s, '10000*ms < 1*s')
self.assertTrue(10000 * ms >= 1 * s, '10000*ms <= 1*s')
with self.assertRaises(TypeError):
nogood = 1 * s > 1 * kg
self.assertFalse(1 * s == 1 * kg)
self.assertTrue(0 * s == 0)
self.assertTrue(4 * s > 0)
with self.assertRaises(TypeError):
_ = 4 * s > 1
def __le__(self, other):
# this method is a bit funky. The <= relationship determines
# which types are allowed to be coerced in flattening. If the
# other type is also a value, we allow this if we have a unit,
# or the other value does not. In other words, the only case
# disallowed is the case where we have no unit but the other
# type does. This prevents the unit from getting lost in the coercion.
if type(other) == TAny:
return True
if type(self) != type(other):
return False
# If other is 'v', then any variant of 'v' is allowed. For example, if
# we are 'v[]' or 'v[Hz]', we are allowed to pass to a setting
# advertising 'v'.
if other.unit is None:
return True
if self.unit is None:
msg = "Unreachable: no python object should get %s as type"%(self,)
raise TypeError(msg)
# We have a unit, and the other guy has a unit, so make sure our units
# are compatible.
return U.Unit(self.unit).isCompatible(U.Unit(other.unit))
def sampling_rate(self, c, samplingRate=None):
"""
Set or get the sampling rate.
Accepts:
samplingRate: sampling rate in samples per unit time, or
as a number assuming S/s units.
Returns:
samplingRate: sampling rate in samples per unit time.
"""
if samplingRate is None:
if 'samplingRate' not in c:
# Assume a sampling rate of 1 GS/s.
c['samplingRate'] = 1000000000
else:
if isinstance(samplingRate, units.Value):
samplingRate = samplingRate['S/s']
rates = (1000000000, 500000000, 250000000)
samplingRate = max(
[rate for rate in rates if samplingRate >= rate])
c['samplingRate'] = samplingRate
self.configure_clock_reference(c)
return c['samplingRate'] * units.Unit('S/s')
def testNegativePowers(self):
self.assertEqual(str(units.Unit('1/s')), 's^-1')
self.assertEqual(str(units.Unit('1/s^1/2')), 's^-1/2')
def test_string_unit(self):
ts = units.Unit('tshirt/s')
self.assertEqual((1 * ts)['tshirt/h'], 3600.0)
self.assertEqual(str(ts), 'tshirt/s')
def test_non_SI(self):
units.addNonSI('count', True)
x = 5 * units.Unit('kcount')
self.assertTrue(x['count'] == 5000.0)
self.assertTrue(x.inBaseUnits() == 5000.0 * units.Unit('count'))
self.assertTrue((x**2).unit == units.Unit('kcount^2'))
def testNone(self):
with self.assertRaises(Exception):
units.Unit(None)
with self.assertRaises(TypeError):
None * units.Unit('MHz')
def testUnitPowers(self):
self.assertTrue(units.Unit('ns')**2 == units.Unit('ns^2'))
def testBaseUnitPowers(self):
x = Value(1, 'ns^2')
self.assertTrue(x.unit.base_unit == units.Unit('s^2'))
self.assertTrue(x.inBaseUnits() == Value(1e-18, 's^2'))
def testInUnitsOf(self):
s = units.Unit('s')
ms = units.Unit('ms')
self.assertTrue((1 * s).inUnitsOf(ms) == 1000 * ms)
self.assertTrue((1 * s).inUnitsOf('ms') == 1000 * ms)
def testUnitCreation(self):
self.assertIsInstance(
units.Unit('test0', 1.0, units.hplanck / (2 * units.e)),
units.Unit)
self.assertTrue(
(units.Unit('phi0')**2).isCompatible(units.Unit('phi0^2')))
### END NODE INFO
"""
from datetime import datetime
import math
from twisted.python import log
from twisted.internet.defer import inlineCallbacks, returnValue
from labrad import types as T, util, units as U
from labrad.server import setting
from labrad.gpib import GPIBManagedServer, GPIBDeviceWrapper
import labrad.units as units
import numpy as np
Ohm, K, s = [U.Unit(s) for s in ['Ohm', 'K', 's']]
READ_ORDER = [1, 2, 1, 3, 1, 4, 1, 5]
#N_CHANNELS = 5
DEFAULT_SETTLE_TIME = 8*s
DEFAULT, FUNCTION, INTERPOLATION, VRHOPPING = range(4)
# These functions suck.
def res2temp(r):
try:
return units.K * ((math.log(r) - 6.02) / 1.76) ** (-1/.345)
except Exception:
return units.K*0.0
def temp2res(t):
try:
import matplotlib
matplotlib.use('Qt4Agg')
import matplotlib.pyplot as plt
import functools
import numpy as np
import scipy.interpolate as interpolate
import scipy.optimize as opt
import itertools
import labrad
import labrad.units as U
from labrad.units import Value, ValueArray as VA
us, GHz, Ohm, pH = (U.Unit(s) for s in ['us', 'GHz', 'Ohm', 'pH'])
# Physical constants
pi = np.pi
PHI_0 = Value(2E-15, 'V*s')
HBAR = Value(1.05E-34, 'J*s')
R_K = Value(25.8E3, 'Ohm')
# Data management
NUM_BETAS = 10
NUM_PHI_POINTS = 200
DATA_NAMES = [
'Z_LC', 'beta', 'f_LC', 'phi_x', 'f_10', 'f_21', 'phi_left', 'phi_right',
'phi_max', 'phi_10', '|0>', '|1>'
def testAngle(self):
rad = units.Unit('rad')
self.assertTrue(rad.is_angle)
self.assertTrue(rad.isAngle())
x = units.Unit('rad*m/s')
self.assertFalse(x.is_angle)
def dep(d):
f_LC = d['f_LC'] * U.Unit(LABELS['f_LC'][1])
t = dep_tunnelling_time_times_f_LC(d)
return t
def well_freq(d):
f_LC = d['f_LC'] * U.Unit(LABELS['f_LC'][1])
Z_LC = d['Z_LC'] * U.Unit(LABELS['Z_LC'][1])
betas = d['beta']
f_well = f_LC * well_frequency_over_f_LC(d['phi_left'], betas)
return f_well[LABELS['f_LC'][1]] / d['f_LC']
