def test_base_rate(self):
# All binary combinaisons for V and H.
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
base_rates = []
# Add the uniform base rate, i.e. all parameters of the model are set to 0.
base_rates.append(self.model.get_base_rate())
# Add the base rate where visible biases are the ones from the model.
base_rates.append(self.model.get_base_rate('c'))
# Add the base rate where hidden biases are the ones from the model.
base_rates.append(self.model.get_base_rate('b')) # Not implemented
for base_rate, anneable_params in base_rates:
base_rate_lnZ = base_rate.compute_lnZ().eval().astype(
config.floatX)
brute_force_lnZ = logsumexp(-base_rate.E(V, H)).eval()
assert_almost_equal(brute_force_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=6)
theano_lnZ = logsumexp(-base_rate.free_energy(V), axis=0).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=6)
theano_lnZ = logsumexp(-base_rate.marginalize_over_v(H)).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=6)
def test_base_rate(self):
# All binary combinaisons for V and H_z
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
# Construct Hz, a subset of H, using np.NaN as padding.
Hz = []
for z in range(1, self.hidden_size + 1):
hz = np.array(H[::2**(self.hidden_size - z)])
hz[:, z:] = np.NaN
Hz.extend(hz)
Hz = np.array(Hz)
assert_equal(len(Hz), np.sum(2**(np.arange(self.hidden_size) + 1)))
assert_true(len(Hz) < self.hidden_size * 2**self.hidden_size)
base_rates = []
# Add the uniform base rate, i.e. all parameters of the model are set to 0.
base_rates.append(self.model.get_base_rate())
# Add the base rate where visible biases are the ones from the model.
base_rates.append(self.model.get_base_rate('c'))
# Add the base rate where hidden biases are the ones from the model.
# base_rates.append(self.model.get_base_rate('b')) # Not implemented
for base_rate, anneable_params in base_rates:
base_rate_lnZ = base_rate.compute_lnZ().eval().astype(
config.floatX)
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
lnZ = theano.function([v, h, z], logsumexp(-base_rate.E(v, h, z)))
energies = []
for z in range(1, self.hidden_size + 1):
hz = np.array(H[::2**(self.hidden_size - z)])
energies.append(lnZ(V, hz, z))
brute_force_lnZ = logsumexp(np.array(energies)).eval()
assert_almost_equal(brute_force_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=6)
theano_lnZ = logsumexp(-base_rate.free_energy(V), axis=0).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=6)
theano_lnZ = logsumexp(-base_rate.marginalize_over_v_z(Hz)).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=6)
def test_compute_lnZ(self):
v = T.matrix('v')
h = T.matrix('h')
lnZ = theano.function([v, h], logsumexp(-self.model.E(v, h)))
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
lnZ_using_free_energy = theano.function([v], logsumexp(-self.model.free_energy(v)))
assert_equal(lnZ_using_free_energy(V), lnZ(V, H))
lnZ_using_marginalize_over_v = theano.function([h], logsumexp(-self.model.marginalize_over_v(h)))
assert_almost_equal(lnZ_using_marginalize_over_v(H), lnZ(V, H), decimal=6)
def test_compute_lnZ(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
lnZ = theano.function([v, h, z], logsumexp(-self.model.E(v, h, z)))
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
energies = []
for z in range(1, self.hidden_size + 1):
hz = np.array(H[::2**(self.hidden_size - z)])
energies.append(lnZ(V, hz, z))
lnZ = logsumexp(np.array(energies)).eval()
lnZ_using_free_energy = theano.function(
[v], logsumexp(-self.model.free_energy(v)))
assert_almost_equal(lnZ_using_free_energy(V), lnZ, decimal=6)
h = T.matrix('h')
z = T.iscalar('z')
lnZ_using_marginalize_over_v = theano.function(
[h, z], logsumexp(self.model.marginalize_over_v(h, z)))
energies = []
for z in range(1, self.hidden_size + 1):
hz = np.array(H[::2**(self.hidden_size - z)])
energies.append(lnZ_using_marginalize_over_v(hz, z))
assert_almost_equal(logsumexp(np.array(energies)).eval(),
lnZ,
decimal=6)
# Construct Hz, a subset of H, using np.NaN as padding.
Hz = []
for z in range(1, self.hidden_size + 1):
hz = np.array(H[::2**(self.hidden_size - z)])
hz[:, z:] = np.NaN
Hz.extend(hz)
Hz = np.array(Hz)
assert_equal(len(Hz), np.sum(2**(np.arange(self.hidden_size) + 1)))
assert_true(len(Hz) < self.hidden_size * 2**self.hidden_size)
lnZ_using_marginalize_over_v_z = theano.function(
[h], logsumexp(-self.model.marginalize_over_v_z(h)))
assert_almost_equal(lnZ_using_marginalize_over_v_z(Hz), lnZ, decimal=6)
def test_compute_lnZ(self):
v = T.matrix('v')
z = T.iscalar('z')
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
#H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
# We simulate having an infinite number of hidden units by adding lot of hidden units with parameters set to 0.
nb_hidden_units_to_add = 10000
model = iRBM(input_size=self.model.input_size,
hidden_size=self.model.hidden_size + nb_hidden_units_to_add,
beta=self.model.beta.get_value())
model.W.set_value(np.r_[self.model.W.get_value(), np.zeros((nb_hidden_units_to_add, model.input_size), dtype=theano.config.floatX)])
model.b.set_value(np.r_[self.model.b.get_value(), np.zeros((nb_hidden_units_to_add,), dtype=theano.config.floatX)])
model.c.set_value(self.model.c.get_value())
v = T.matrix('v')
z = T.iscalar('z')
F_vz = theano.function([v, z], model.F(v, z))
energies = []
for z in range(1, model.hidden_size+1):
energies.append(F_vz(V, z))
lnZ = logsumexp(-np.array(energies)).eval()
lnZ_using_free_energy = theano.function([v], logsumexp(-self.model.free_energy(v)))
assert_almost_equal(lnZ_using_free_energy(V), lnZ, decimal=5) # decimal=5 needed for float32
def test_verify_AIS(self):
model = oRBM(input_size=self.input_size,
hidden_size=self.hidden_size,
beta=self.beta)
model.W.set_value(self.W)
model.b.set_value(self.b)
model.c.set_value(self.c)
# Brute force
print "Computing lnZ using brute force (i.e. summing the free energy of all posible $v$)..."
V = theano.shared(
value=cartesian([(0, 1)] * self.input_size, dtype=config.floatX))
brute_force_lnZ = logsumexp(-model.free_energy(V), 0)
f_brute_force_lnZ = theano.function([], brute_force_lnZ)
params_bak = [param.get_value() for param in model.parameters]
print "Approximating lnZ using AIS..."
import time
start = time.time()
try:
ais_working_dir = tempfile.mkdtemp()
result = compute_AIS(model,
M=self.nb_samples,
betas=self.betas,
seed=1234,
ais_working_dir=ais_working_dir,
force=True)
logcummean_Z, logcumstd_Z_down, logcumstd_Z_up = result[
'logcummean_Z'], result['logcumstd_Z_down'], result[
'logcumstd_Z_up']
std_lnZ = result['std_lnZ']
print "{0} sec".format(time.time() - start)
import pylab as plt
plt.gca().set_xmargin(0.1)
plt.errorbar(range(1, self.nb_samples + 1),
logcummean_Z,
yerr=[std_lnZ, std_lnZ],
fmt='or')
plt.errorbar(range(1, self.nb_samples + 1),
logcummean_Z,
yerr=[logcumstd_Z_down, logcumstd_Z_up],
fmt='ob')
plt.plot([1, self.nb_samples], [f_brute_force_lnZ()] * 2, '--g')
plt.ticklabel_format(useOffset=False, axis='y')
plt.show()
AIS_logZ = logcummean_Z[-1]
assert_array_equal(params_bak[0], model.W.get_value())
assert_array_equal(params_bak[1], model.b.get_value())
assert_array_equal(params_bak[2], model.c.get_value())
print np.abs(AIS_logZ - f_brute_force_lnZ())
assert_almost_equal(AIS_logZ, f_brute_force_lnZ(), decimal=2)
finally:
shutil.rmtree(ais_working_dir)
def test_base_rate(self):
# All binary combinaisons for V and H_z
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
# Construct Hz, a subset of H, using np.NaN as padding.
Hz = []
for z in range(1, self.hidden_size+1):
hz = np.array(H[::2**(self.hidden_size-z)])
hz[:, z:] = np.NaN
Hz.extend(hz)
Hz = np.array(Hz)
assert_equal(len(Hz), np.sum(2**(np.arange(self.hidden_size)+1)))
assert_true(len(Hz) < self.hidden_size * 2**self.hidden_size)
base_rates = []
# Add the uniform base rate, i.e. all parameters of the model are set to 0.
base_rates.append(self.model.get_base_rate())
# Add the base rate where visible biases are the ones from the model.
base_rates.append(self.model.get_base_rate('c'))
# Add the base rate where hidden biases are the ones from the model.
# base_rates.append(self.model.get_base_rate('b')) # Not implemented
for base_rate, anneable_params in base_rates:
base_rate_lnZ = base_rate.compute_lnZ().eval().astype(config.floatX)
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
lnZ = theano.function([v, h, z], logsumexp(-base_rate.E(v, h, z)))
energies = []
for z in range(1, self.hidden_size+1):
hz = np.array(H[::2**(self.hidden_size-z)])
energies.append(lnZ(V, hz, z))
brute_force_lnZ = logsumexp(np.array(energies)).eval()
assert_almost_equal(brute_force_lnZ.astype(config.floatX), base_rate_lnZ, decimal=6)
theano_lnZ = logsumexp(-base_rate.free_energy(V), axis=0).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX), base_rate_lnZ, decimal=6)
theano_lnZ = logsumexp(-base_rate.marginalize_over_v_z(Hz)).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX), base_rate_lnZ, decimal=6)
def test_compute_lnZ(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
lnZ = theano.function([v, h, z], logsumexp(-self.model.E(v, h, z)))
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
energies = []
for z in range(1, self.hidden_size+1):
hz = np.array(H[::2**(self.hidden_size-z)])
energies.append(lnZ(V, hz, z))
lnZ = logsumexp(np.array(energies)).eval()
lnZ_using_free_energy = theano.function([v], logsumexp(-self.model.free_energy(v)))
assert_almost_equal(lnZ_using_free_energy(V), lnZ, decimal=6)
h = T.matrix('h')
z = T.iscalar('z')
lnZ_using_marginalize_over_v = theano.function([h, z], logsumexp(self.model.marginalize_over_v(h, z)))
energies = []
for z in range(1, self.hidden_size+1):
hz = np.array(H[::2**(self.hidden_size-z)])
energies.append(lnZ_using_marginalize_over_v(hz, z))
assert_almost_equal(logsumexp(np.array(energies)).eval(), lnZ, decimal=6)
# Construct Hz, a subset of H, using np.NaN as padding.
Hz = []
for z in range(1, self.hidden_size+1):
hz = np.array(H[::2**(self.hidden_size-z)])
hz[:, z:] = np.NaN
Hz.extend(hz)
Hz = np.array(Hz)
assert_equal(len(Hz), np.sum(2**(np.arange(self.hidden_size)+1)))
assert_true(len(Hz) < self.hidden_size * 2**self.hidden_size)
lnZ_using_marginalize_over_v_z = theano.function([h], logsumexp(-self.model.marginalize_over_v_z(h)))
assert_almost_equal(lnZ_using_marginalize_over_v_z(Hz), lnZ, decimal=6)
def test_free_energy(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
logsumexp_E = theano.function([v, h, z],
-logsumexp(-self.model.E(v, h, z)))
F_vz = theano.function([v, z], self.model.F(v, z))
rng = np.random.RandomState(42)
v1 = (rng.rand(1, self.input_size) > 0.5).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
# Check the free energy F(v, z) is correct.
for z in range(1, self.hidden_size + 1):
h = np.array(H[::2**(self.hidden_size - z)])
free_energy_vz = logsumexp_E(v1, h, z)
assert_almost_equal(F_vz(v1, z), free_energy_vz, decimal=6)
# We now check that free energy F(v) assumes an infinite number of hidden units.
# To do so, we create another model that has an infinite (read a lot) number of hidden units with parameters set to 0.
nb_hidden_units_to_add = 10000
model = iRBM(input_size=self.model.input_size,
hidden_size=self.model.hidden_size +
nb_hidden_units_to_add,
beta=self.model.beta.get_value())
model.W.set_value(np.r_[self.model.W.get_value(),
np.zeros(
(nb_hidden_units_to_add, model.input_size),
dtype=theano.config.floatX)])
model.b.set_value(
np.r_[self.model.b.get_value(),
np.zeros(
(nb_hidden_units_to_add, ), dtype=theano.config.floatX)])
model.c.set_value(self.model.c.get_value())
v = T.matrix('v')
z = T.iscalar('z')
F_vz = theano.function([v, z], model.F(v, z))
free_energies_vz = []
for z in range(1, model.hidden_size + 1):
free_energies_vz.append(F_vz(v1, z))
Fv = -logsumexp(-np.array(free_energies_vz)).eval()
v = T.matrix('v')
free_energy = theano.function([v], self.model.free_energy(v))
assert_array_almost_equal(free_energy(v1), [Fv],
decimal=5) # decimal=5 needed for float32
v2 = np.tile(v1, (self.batch_size, 1))
assert_array_almost_equal(free_energy(v2), [Fv] * self.batch_size,
decimal=5) # decimal=5 needed for float32
def test_base_rate(self):
# All binary combinaisons for V and H_z
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
#H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
base_rates = []
# Add the uniform base rate, i.e. all parameters of the model are set to 0.
base_rates.append(self.model.get_base_rate())
# Add the base rate where visible biases are the ones from the model.
base_rates.append(self.model.get_base_rate('c'))
# Add the base rate where hidden biases are the ones from the model.
# base_rates.append(self.model.get_base_rate('b')) # Not implemented
for base_rate, anneable_params in base_rates:
print base_rate
base_rate_lnZ = base_rate.compute_lnZ().eval().astype(
config.floatX)
# We simulate having an infinite number of hidden units by adding lot of hidden units with parameters set to 0.
nb_hidden_units_to_add = 10000
model = iRBM(input_size=base_rate.input_size,
hidden_size=base_rate.hidden_size +
nb_hidden_units_to_add,
beta=base_rate.beta.get_value())
model.W = T.join(
0, base_rate.W,
np.zeros((nb_hidden_units_to_add, model.input_size),
dtype=theano.config.floatX))
model.b = T.join(
0, base_rate.b,
np.zeros((nb_hidden_units_to_add, ),
dtype=theano.config.floatX))
model.c = base_rate.c
v = T.matrix('v')
z = T.iscalar('z')
F_vz = theano.function([v, z], model.F(v, z))
energies = []
for z in range(1, model.hidden_size + 1):
energies.append(F_vz(V, z))
brute_force_lnZ = logsumexp(-np.array(energies)).eval()
assert_almost_equal(brute_force_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=5)
theano_lnZ = logsumexp(-base_rate.free_energy(V), axis=0).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX),
base_rate_lnZ,
decimal=6)
def test_marginalize_over_v(self):
v = T.matrix('v')
h = T.matrix('h')
E = theano.function([v, h], -logsumexp(-self.model.E(v, h)))
h1 = np.random.rand(1, self.hidden_size).astype(config.floatX)
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
expected_energy = E(V, h1)
h = T.matrix('h')
marginalize_over_v = theano.function([h], self.model.marginalize_over_v(h))
assert_array_almost_equal(marginalize_over_v(h1), [expected_energy])
h2 = np.tile(h1, (self.batch_size, 1))
assert_array_almost_equal(marginalize_over_v(h2), [expected_energy]*self.batch_size)
def test_free_energy(self):
v = T.matrix('v')
h = T.matrix('h')
logsumexp_E = theano.function([v, h], -logsumexp(-self.model.E(v, h)))
v1 = np.random.rand(1, self.input_size).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
Fv = logsumexp_E(v1, H) # Marginalization over $\bh$
v = T.matrix('v')
free_energy = theano.function([v], self.model.free_energy(v))
assert_array_almost_equal(free_energy(v1), [Fv])
v2 = np.tile(v1, (self.batch_size, 1))
assert_array_almost_equal(free_energy(v2), [Fv]*self.batch_size)
def test_free_energy(self):
v = T.matrix('v')
h = T.matrix('h')
logsumexp_E = theano.function([v, h], -logsumexp(-self.model.E(v, h)))
v1 = np.random.rand(1, self.input_size).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
Fv = logsumexp_E(v1, H) # Marginalization over $\bh$
v = T.matrix('v')
free_energy = theano.function([v], self.model.free_energy(v))
assert_array_almost_equal(free_energy(v1), [Fv])
v2 = np.tile(v1, (self.batch_size, 1))
assert_array_almost_equal(free_energy(v2), [Fv] * self.batch_size)
def test_base_rate(self):
# All binary combinaisons for V and H.
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
base_rates = []
# Add the uniform base rate, i.e. all parameters of the model are set to 0.
base_rates.append(self.model.get_base_rate())
# Add the base rate where visible biases are the ones from the model.
base_rates.append(self.model.get_base_rate('c'))
# Add the base rate where hidden biases are the ones from the model.
base_rates.append(self.model.get_base_rate('b')) # Not implemented
for base_rate, anneable_params in base_rates:
base_rate_lnZ = base_rate.compute_lnZ().eval().astype(config.floatX)
brute_force_lnZ = logsumexp(-base_rate.E(V, H)).eval()
assert_almost_equal(brute_force_lnZ.astype(config.floatX), base_rate_lnZ, decimal=6)
theano_lnZ = logsumexp(-base_rate.free_energy(V), axis=0).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX), base_rate_lnZ, decimal=6)
theano_lnZ = logsumexp(-base_rate.marginalize_over_v(H)).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX), base_rate_lnZ, decimal=6)
def test_verify_AIS(self):
model = iRBM(input_size=self.input_size,
hidden_size=self.hidden_size,
beta=self.beta)
model.W.set_value(self.W)
model.b.set_value(self.b)
model.c.set_value(self.c)
# Brute force
print "Computing lnZ using brute force (i.e. summing the free energy of all posible $v$)..."
V = theano.shared(value=cartesian([(0, 1)] * self.input_size, dtype=config.floatX))
brute_force_lnZ = logsumexp(-model.free_energy(V), 0)
f_brute_force_lnZ = theano.function([], brute_force_lnZ)
params_bak = [param.get_value() for param in model.parameters]
print "Approximating lnZ using AIS..."
import time
start = time.time()
try:
ais_working_dir = tempfile.mkdtemp()
result = compute_AIS(model, M=self.nb_samples, betas=self.betas, seed=1234, ais_working_dir=ais_working_dir, force=True)
logcummean_Z, logcumstd_Z_down, logcumstd_Z_up = result['logcummean_Z'], result['logcumstd_Z_down'], result['logcumstd_Z_up']
std_lnZ = result['std_lnZ']
print "{0} sec".format(time.time() - start)
import pylab as plt
plt.gca().set_xmargin(0.1)
plt.errorbar(range(1, self.nb_samples+1), logcummean_Z, yerr=[std_lnZ, std_lnZ], fmt='or')
plt.errorbar(range(1, self.nb_samples+1), logcummean_Z, yerr=[logcumstd_Z_down, logcumstd_Z_up], fmt='ob')
plt.plot([1, self.nb_samples], [f_brute_force_lnZ()]*2, '--g')
plt.ticklabel_format(useOffset=False, axis='y')
plt.show()
AIS_logZ = logcummean_Z[-1]
assert_array_equal(params_bak[0], model.W.get_value())
assert_array_equal(params_bak[1], model.b.get_value())
assert_array_equal(params_bak[2], model.c.get_value())
print np.abs(AIS_logZ - f_brute_force_lnZ())
assert_almost_equal(AIS_logZ, f_brute_force_lnZ(), decimal=2)
finally:
shutil.rmtree(ais_working_dir)
def test_free_energy(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
logsumexp_E = theano.function([v, h, z], -logsumexp(-self.model.E(v, h, z)))
F_vz = theano.function([v, z], self.model.F(v, z))
rng = np.random.RandomState(42)
v1 = (rng.rand(1, self.input_size) > 0.5).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
# Check the free energy F(v, z) is correct.
for z in range(1, self.hidden_size+1):
h = np.array(H[::2**(self.hidden_size-z)])
free_energy_vz = logsumexp_E(v1, h, z)
assert_almost_equal(F_vz(v1, z), free_energy_vz, decimal=6)
# We now check that free energy F(v) assumes an infinite number of hidden units.
# To do so, we create another model that has an infinite (read a lot) number of hidden units with parameters set to 0.
nb_hidden_units_to_add = 10000
model = iRBM(input_size=self.model.input_size,
hidden_size=self.model.hidden_size + nb_hidden_units_to_add,
beta=self.model.beta.get_value())
model.W.set_value(np.r_[self.model.W.get_value(), np.zeros((nb_hidden_units_to_add, model.input_size), dtype=theano.config.floatX)])
model.b.set_value(np.r_[self.model.b.get_value(), np.zeros((nb_hidden_units_to_add,), dtype=theano.config.floatX)])
model.c.set_value(self.model.c.get_value())
v = T.matrix('v')
z = T.iscalar('z')
F_vz = theano.function([v, z], model.F(v, z))
free_energies_vz = []
for z in range(1, model.hidden_size+1):
free_energies_vz.append(F_vz(v1, z))
Fv = -logsumexp(-np.array(free_energies_vz)).eval()
v = T.matrix('v')
free_energy = theano.function([v], self.model.free_energy(v))
assert_array_almost_equal(free_energy(v1), [Fv], decimal=5) # decimal=5 needed for float32
v2 = np.tile(v1, (self.batch_size, 1))
assert_array_almost_equal(free_energy(v2), [Fv]*self.batch_size, decimal=5) # decimal=5 needed for float32
def test_sample_z_given_v(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
E = theano.function([v, h, z], logsumexp(-self.model.E(v, h, z)))
v1 = np.random.rand(1, self.input_size).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
energies = []
for z in range(1, self.hidden_size + 1):
h = np.array(H[::2**(self.hidden_size - z)])
energies.append(E(v1, h, z))
probs = T.nnet.softmax(T.stack(energies))
expected_icdf = T.cumsum(probs[:, ::-1], axis=1)[:, ::-1].eval()
# Test inverse cdf
v = T.matrix('v')
icdf_z_given_v = theano.function([v], self.model.icdf_z_given_v(v))
assert_array_almost_equal(icdf_z_given_v(v1), expected_icdf)
batch_size = 500000
self.model.batch_size = batch_size
sample_zmask_given_v = theano.function(
[v], self.model.sample_zmask_given_v(v))
v2 = np.tile(v1, (self.model.batch_size, 1))
#theano.printing.pydotprint(sample_zmask_given_v)
z_mask = sample_zmask_given_v(v2)
# First hidden units should always be considered i.e. z_mask[:, 0] == 1
assert_equal(np.sum(z_mask[:, 0] == 0, axis=0), 0)
# Test that sampled masks are as expected i.e. equal expected_icdf
freq_per_z = np.sum(z_mask, axis=0) / self.model.batch_size
assert_array_almost_equal(
freq_per_z,
expected_icdf[0],
decimal=3,
err_msg=
"Tested using MC sampling, rerun it to be certain that is an error or increase 'batch_size'."
)
def test_base_rate(self):
# All binary combinaisons for V and H_z
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
#H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
base_rates = []
# Add the uniform base rate, i.e. all parameters of the model are set to 0.
base_rates.append(self.model.get_base_rate())
# Add the base rate where visible biases are the ones from the model.
base_rates.append(self.model.get_base_rate('c'))
# Add the base rate where hidden biases are the ones from the model.
# base_rates.append(self.model.get_base_rate('b')) # Not implemented
for base_rate, anneable_params in base_rates:
print base_rate
base_rate_lnZ = base_rate.compute_lnZ().eval().astype(config.floatX)
# We simulate having an infinite number of hidden units by adding lot of hidden units with parameters set to 0.
nb_hidden_units_to_add = 10000
model = iRBM(input_size=base_rate.input_size,
hidden_size=base_rate.hidden_size + nb_hidden_units_to_add,
beta=base_rate.beta.get_value())
model.W = T.join(0, base_rate.W, np.zeros((nb_hidden_units_to_add, model.input_size), dtype=theano.config.floatX))
model.b = T.join(0, base_rate.b, np.zeros((nb_hidden_units_to_add,), dtype=theano.config.floatX))
model.c = base_rate.c
v = T.matrix('v')
z = T.iscalar('z')
F_vz = theano.function([v, z], model.F(v, z))
energies = []
for z in range(1, model.hidden_size+1):
energies.append(F_vz(V, z))
brute_force_lnZ = logsumexp(-np.array(energies)).eval()
assert_almost_equal(brute_force_lnZ.astype(config.floatX), base_rate_lnZ, decimal=5)
theano_lnZ = logsumexp(-base_rate.free_energy(V), axis=0).eval()
assert_almost_equal(theano_lnZ.astype(config.floatX), base_rate_lnZ, decimal=6)
def test_free_energy(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
logsumexp_E = theano.function([v, h, z], -logsumexp(-self.model.E(v, h, z)))
v1 = np.random.rand(1, self.input_size).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
energies = []
for z in range(1, self.hidden_size+1):
h = np.array(H[::2**(self.hidden_size-z)])
energies.append(logsumexp_E(v1, h, z))
Fv = -logsumexp(-np.array(energies)).eval()
v = T.matrix('v')
free_energy = theano.function([v], self.model.free_energy(v))
assert_array_almost_equal(free_energy(v1), [Fv])
v2 = np.tile(v1, (self.batch_size, 1))
assert_array_almost_equal(free_energy(v2), [Fv]*self.batch_size)
def test_compute_lnZ(self):
v = T.matrix('v')
z = T.iscalar('z')
V = cartesian([(0, 1)] * self.input_size, dtype=config.floatX)
#H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
# We simulate having an infinite number of hidden units by adding lot of hidden units with parameters set to 0.
nb_hidden_units_to_add = 10000
model = iRBM(input_size=self.model.input_size,
hidden_size=self.model.hidden_size +
nb_hidden_units_to_add,
beta=self.model.beta.get_value())
model.W.set_value(np.r_[self.model.W.get_value(),
np.zeros(
(nb_hidden_units_to_add, model.input_size),
dtype=theano.config.floatX)])
model.b.set_value(
np.r_[self.model.b.get_value(),
np.zeros(
(nb_hidden_units_to_add, ), dtype=theano.config.floatX)])
model.c.set_value(self.model.c.get_value())
v = T.matrix('v')
z = T.iscalar('z')
F_vz = theano.function([v, z], model.F(v, z))
energies = []
for z in range(1, model.hidden_size + 1):
energies.append(F_vz(V, z))
lnZ = logsumexp(-np.array(energies)).eval()
lnZ_using_free_energy = theano.function(
[v], logsumexp(-self.model.free_energy(v)))
assert_almost_equal(lnZ_using_free_energy(V), lnZ,
decimal=5) # decimal=5 needed for float32
def test_free_energy(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
logsumexp_E = theano.function([v, h, z],
-logsumexp(-self.model.E(v, h, z)))
v1 = np.random.rand(1, self.input_size).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
energies = []
for z in range(1, self.hidden_size + 1):
h = np.array(H[::2**(self.hidden_size - z)])
energies.append(logsumexp_E(v1, h, z))
Fv = -logsumexp(-np.array(energies)).eval()
v = T.matrix('v')
free_energy = theano.function([v], self.model.free_energy(v))
assert_array_almost_equal(free_energy(v1), [Fv])
v2 = np.tile(v1, (self.batch_size, 1))
assert_array_almost_equal(free_energy(v2), [Fv] * self.batch_size)
def test_sample_z_given_v(self):
v = T.matrix('v')
h = T.matrix('h')
z = T.iscalar('z')
E = theano.function([v, h, z], logsumexp(-self.model.E(v, h, z)))
v1 = np.random.rand(1, self.input_size).astype(config.floatX)
H = cartesian([(0, 1)] * self.hidden_size, dtype=config.floatX)
energies = []
for z in range(1, self.hidden_size+1):
h = np.array(H[::2**(self.hidden_size-z)])
energies.append(E(v1, h, z))
probs = T.nnet.softmax(T.stack(energies))
expected_icdf = T.cumsum(probs[:, ::-1], axis=1)[:, ::-1].eval()
# Test inverse cdf
v = T.matrix('v')
icdf_z_given_v = theano.function([v], self.model.icdf_z_given_v(v))
assert_array_almost_equal(icdf_z_given_v(v1), expected_icdf)
batch_size = 500000
self.model.batch_size = batch_size
sample_zmask_given_v = theano.function([v], self.model.sample_zmask_given_v(v))
v2 = np.tile(v1, (self.model.batch_size, 1))
#theano.printing.pydotprint(sample_zmask_given_v)
z_mask = sample_zmask_given_v(v2)
# First hidden units should always be considered i.e. z_mask[:, 0] == 1
assert_equal(np.sum(z_mask[:, 0] == 0, axis=0), 0)
# Test that sampled masks are as expected i.e. equal expected_icdf
freq_per_z = np.sum(z_mask, axis=0) / self.model.batch_size
assert_array_almost_equal(freq_per_z, expected_icdf[0], decimal=3, err_msg="Tested using MC sampling, rerun it to be certain that is an error or increase 'batch_size'.")
