def test2(self):
"neutron"
# creating instances
from mcni import neutron
n = neutron(r=(0,0,0), v=(0,0,3000))
n = neutron(r=(0,0,0), v=(0,0,3000), time=1000.)
n = neutron(r=(0,0,0), v=(0,0,3000), time=1000., prob=10.)
n = neutron(r=(0,0,0), v=(0,0,3000), s=(0,1), time=1000., prob=10.)
# printing
print n
print n.state
print n.state.velocity
# setting values
n.state.position = mcni.position(1,2,3)
self.assertEqual(tuple(n.state.position), (1,2,3))
n.state.velocity = mcni.velocity(1,2,3)
self.assertEqual(tuple(n.state.velocity), (1,2,3))
n.state.spin = mcni.spin(1,0)
self.assertEqual(n.state.spin.s1, 1)
self.assertEqual(n.state.spin.s2, 0)
n.time = 999
self.assertEqual(n.time, 999)
n.probability = 888
self.assertEqual(n.probability, 888)
return
def test2(self):
"neutron"
# creating instances
from mcni import neutron
n = neutron(r=(0, 0, 0), v=(0, 0, 3000))
n = neutron(r=(0, 0, 0), v=(0, 0, 3000), time=1000.)
n = neutron(r=(0, 0, 0), v=(0, 0, 3000), time=1000., prob=10.)
n = neutron(r=(0, 0, 0),
v=(0, 0, 3000),
s=(0, 1),
time=1000.,
prob=10.)
# printing
print n
print n.state
print n.state.velocity
# setting values
n.state.position = mcni.position(1, 2, 3)
self.assertEqual(tuple(n.state.position), (1, 2, 3))
n.state.velocity = mcni.velocity(1, 2, 3)
self.assertEqual(tuple(n.state.velocity), (1, 2, 3))
n.state.spin = mcni.spin(1, 0)
self.assertEqual(n.state.spin.s1, 1)
self.assertEqual(n.state.spin.s2, 0)
n.time = 999
self.assertEqual(n.time, 999)
n.probability = 888
self.assertEqual(n.probability, 888)
return
def test_pass_through_guide():
"""
Test several cases where neutrons pass through the guide
"""
guide_length = 16
guide_exit_height = 2.0
guide = Guide('test guide', 3, 3, 2, guide_exit_height, guide_length)
# neutron straight through at origin
result = do_process(guide, neutron(r=(0., 0., 0.), v=(0.0, 0.0, 0.5)))
# the neutron should be at the same place propagated along the +Z axis
np.testing.assert_equal([0., 0., guide_length], result[0:3])
# make sure the velocity does not change
np.testing.assert_equal([0., 0., 0.5], result[3:6])
# the time should be the same as t = d/v
np.testing.assert_equal(guide_length / 0.5, result[8])
# probability shouldn't change since there are no reflections
np.testing.assert_equal(1.0, result[9])
# neutron angled at the upper back guide exit from the origin
vmag = 0.5
angle = np.arctan((0.5 * guide_exit_height) / guide_length)
result = do_process(
guide,
neutron(r=(0., 0., 0.),
v=(0.0, vmag * np.sin(angle), vmag * np.cos(angle))))
np.testing.assert_equal([0.0, 0.5 * guide_exit_height, guide_length],
result[0:3])
np.testing.assert_equal(1.0, result[9])
def __init__(self,
name,
xmin=0,
xmax=0,
ymin=0,
ymax=0,
radius=0,
cut=0,
width=0,
height=0,
**kwargs):
"""
Initialize this Slit component.
The slit is at z==0.
Setting radius to non-zero switches this slit from being rectangular to
a circle centered on x,y==0,0.
Parameters:
name (str): the name of this component
xmin (m): the smallest value of x that still passes a rectangular slit
xmax (m): the largest value of x that still passes a rectangular slit
ymin (m): the smallest value of y that still passes a rectangular slit
ymax (m): the largest value of y that still passes a rectangular slit
radius (m): the largest distance on x-y from 0,0 that still passes a
circular slit
cut: the smallest neutron weight that can penetrate the slit
width (m): sets xmin and xmax to a width centered on x==0
height (m): sets ymin and ymax to a width centered on y==0
"""
super().__init__(__class__, **kwargs)
self.name = name
# Check and process the arguments.
if width > 0:
xmax = width / 2
xmin = -xmax
if height > 0:
ymax = height / 2
ymin = -ymax
if not (xmin or xmax or ymin or ymax or radius):
raise ValueError("a slit must have some extent")
# Note the configuration of the slit.
self.propagate_params = (np.array(
[xmin, xmax, ymin, ymax, radius * radius, cut]), )
# Aim neutrons toward the slit to cause JIT compilation.
import mcni
neutrons = mcni.neutron_buffer(2)
# first neutron passes through
neutrons[0] = mcni.neutron(r=(0, 0, -1), v=(0, 0, 1), prob=1, time=0)
# second neutron is absorbed
x_edge = radius if radius > 0 else xmax
neutrons[1] = mcni.neutron(r=(x_edge * 2, 0, -1),
v=(0, 0, 1),
prob=1,
time=0)
self.process(neutrons)
def help_test_slit_beamstop(component, passes):
# Where the neutron is when it reaches the component.
xs_arrived = np.arange(-9, 10) # 19
ys_arrived = np.arange(-9, 10) # 19
# How the neutron position is different before it reaches the component.
dxs = np.arange(-3, 4) # 7
dys = np.arange(-3, 4) # 7
# Try various neutron weights.
ws = deque(np.arange(0.2, 1.1, 0.2))
# Pattern of weights should be irregular against geometry of test data.
assert gcd(len(ws), prod(map(len, [xs_arrived, ys_arrived, dxs, dys]))) == 1
# Fill a neutron buffer with a range of neutrons that approach the plane of
# the component.
neutrons_start = []
neutrons_end_expected = []
(any_pass, any_fail) = (False, False)
for x_arrived in xs_arrived:
for y_arrived in ys_arrived:
for dx in dxs:
for dy in dys:
# Construct an incoming neutron 2m before.
distance = sqrt(sum([2, pow(dx, 2), pow(dy, 2)]))
position_start = [x_arrived + dx, y_arrived + dy, -2]
velocity = [n / distance for n in [-dx, -dy, 2]] # 1 m/s
w = ws[0]
ws.rotate() # A different weight for the next neutron.
neutrons_start.append(neutron(
r=position_start, v=velocity, prob=w))
if passes(x_arrived, y_arrived, w):
# Construct a neutron expected from the component.
position_arrived = [x_arrived, y_arrived, 0]
neutrons_end_expected.append(neutron(
r=position_arrived, v=velocity, prob=w,
time=distance))
any_pass = True
else:
any_fail = True
assert any_pass and any_fail
neutrons_end_expected = neutron_buffer_from_array(neutrons_end_expected)
# Propagate the neutrons.
neutrons_buffer = neutron_buffer_from_array(neutrons_start)
component.process(neutrons_buffer)
# Compare the actual neutrons with the expectation.
tolerance = 1e-6 if get_numpy_floattype() == np.float32 else 1e-15
assert np.allclose(neutrons_as_npyarr(neutrons_buffer),
neutrons_as_npyarr(neutrons_end_expected),
atol=tolerance)
def test1(self):
'mccomponents.sample.samplecomponent'
import mcni
neutron = mcni.neutron( r = (0,0,0), v = (0,0,3000), time = 0, prob = 1 )
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource('source', neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent( 'Ni', 'sampleassemblies/Ni/sampleassembly.xml' )
instrument = mcni.instrument( [component1, component2] )
geometer = mcni.geometer()
geometer.register( component1, (0,0,0), (0,0,0) )
geometer.register( component2, (0,0,1), (0,0,0) )
neutrons = mcni.neutron_buffer( 1 )
from mcni.pyre_support.ConsoleNeutronTracer import ConsoleNeutronTracer
tracer = ConsoleNeutronTracer()
mcni.simulate(
instrument, geometer, neutrons,
multiple_scattering=True,
tracer = tracer
)
return
def test3(self):
'''create pure python representation of a homogeneous scatterer with
composite kernel. render the c++ computation engine of that kernel.
'''
#shape
from mccomposite.geometry import primitives
shape = primitives.block( (1,1,1) )
#kernel
nprinter = NeutronPrinter( )
#composite kernel
composite_kernel = hs.compositeKernel()
composite_kernel.addElement( nprinter )
#scatterer
scatterer = hs.homogeneousScatterer(
shape, composite_kernel)
#render the c++ representation
cscatterer = hs.scattererEngine( scatterer )
for i in range(10):
ev = mcni.neutron( r = (0,0,-5), v = (0,0,1) )
cscatterer.scatter(ev)
continue
return
def test2(self):
'shape positioning: rotated sphere'
# source
from mcni.components.MonochromaticSource import MonochromaticSource
import mcni
neutron = mcni.neutron(r=(0,0,-1), v=(0,0,1000), prob=1)
source = MonochromaticSource('s', neutron, dx=0.10, dy=0.09, dE=0)
# sample
from mccomponents.sample import samplecomponent
scatterer = samplecomponent('sa', 'sphere-rotated-arbitrarily/sampleassembly.xml' )
# neutrons
N = 1000
neutrons = mcni.neutron_buffer(N)
neutrons = source.process(neutrons)
# find neutrons out of target
arr = neutrons.to_npyarr()
x,y,z = arr[:, :3].T
missing = x*x+y*y>0.05*0.05
# print "missed:", missing.sum()
# print neutrons
scatterer.process(neutrons)
# print neutrons
arr = neutrons.to_npyarr()
x,y,z = arr[:, :3].T
assert (z[missing] < -.9).all()
hit = arr[np.logical_not(missing), :3]
x,y,z = hit.T
assert (z > -.1).all()
assert np.isclose(np.abs(x*x+y*y+z*z), 0.05*0.05).all()
return
def test1(self):
'mccomponents.sample.samplecomponent isotropic kernel, multiple-scattering'
import mcni
neutron = mcni.neutron(r=(0, 0, 0), v=(0, 0, 3000), time=0, prob=1)
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource('source', neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent(
'Al', 'sampleassemblies/Al-isotropickernel/sampleassembly.xml')
instrument = mcni.instrument([component1, component2])
geometer = mcni.geometer()
geometer.register(component1, (0, 0, 0), (0, 0, 0))
geometer.register(component2, (0, 0, 1), (0, 0, 0))
N0 = 1
neutrons = mcni.neutron_buffer(N0)
mcni.simulate(instrument, geometer, neutrons, multiple_scattering=True)
N = len(neutrons)
for i in range(N):
neutron = neutrons[i]
print neutron
continue
return
def test1(self):
'mccomponents.sample.samplecomponent: IsotropicKernel'
import mcni
neutron = mcni.neutron( r = (0,0,0), v = (0,0,3000), time = 0, prob = 1 )
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource('source', neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent( 'Al', 'sampleassemblies/Al-isotropickernel/sampleassembly.xml' )
instrument = mcni.instrument( [component1, component2] )
geometer = mcni.geometer()
geometer.register( component1, (0,0,0), (0,0,0) )
geometer.register( component2, (0,0,1), (0,0,0) )
N0 = 1000
neutrons = mcni.neutron_buffer(N0)
mcni.simulate( instrument, geometer, neutrons )
N = len(neutrons)
for i in range(10):
neutron = neutrons[i]
print neutron
continue
# N should be about 2/3 of N0. this is determined by
# the mc weights in Al-isotropic-kernel-plate-scatterer.xml
self.assert_( N < 0.72*N0 and N > 0.6*N0)
return
def test(self):
"wrap SNS_source_r1"
from mcstas2 import componentfactory
factory = componentfactory(category, componentname)
component = factory(
"component",
S_filename="source_sct521_bu_17_1.dat",
width=0.1,
height=0.12,
dist=2.5,
xw=0.1,
yh=0.12,
Emin=50,
Emax=70,
)
import mcni
neutrons = mcni.neutron_buffer(5)
for i in range(5):
neutrons[i] = mcni.neutron(r=(0, 0, -1), v=(0, 0, 3000), time=0, prob=1)
continue
component.process(neutrons)
print neutrons
return
def test1(self):
'mccomponents.sample.samplecomponent isotropic kernel, multiple-scattering'
import mcni
neutron = mcni.neutron( r = (0,0,0), v = (0,0,3000), time = 0, prob = 1 )
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource('source', neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent( 'Al', 'sampleassemblies/Al-isotropickernel/sampleassembly.xml' )
instrument = mcni.instrument( [component1, component2] )
geometer = mcni.geometer()
geometer.register( component1, (0,0,0), (0,0,0) )
geometer.register( component2, (0,0,1), (0,0,0) )
N0 = 1
neutrons = mcni.neutron_buffer(N0)
mcni.simulate( instrument, geometer, neutrons, multiple_scattering=True)
N = len(neutrons)
for i in range(N):
neutron = neutrons[i]
print neutron
continue
return
def test1(self):
'detector hierarchy from xml'
from instrument.nixml import parse_file
instrument = parse_file('ARCS.xml')
import instrument.geometers as ig
instrument.geometer.changeRequestCoordinateSystem(
ig.coordinateSystem(coordinate_system))
assignLocalGeometers(instrument, coordinate_system=coordinate_system)
detectorSystem = instrument.getDetectorSystem()
tofparams = 0, 10e-3, 1e-4
detectorSystem.tofparams = tofparams
dims = getDetectorHierarchyDimensions(instrument)
dims = [dim for name, dim in dims]
mca = md.eventModeMCA(outfilename, dims)
detectorSystem.mca = mca
cds = mh.scattererEngine(detectorSystem,
coordinate_system=coordinate_system)
for i in range(nevents):
if i % 1000 == 0: print i
ev = mcni.neutron(r=(0, 0, 0), v=(2000, 1500, 0))
cds.scatter(ev)
continue
instrument.geometer = instrument.global_geometer
return
def process(self, neutrons):
import mcni
for i in range(len(neutrons)):
info.log("loop #%d" % i)
neutrons[i] = mcni.neutron( r = ( 0,0,0 ), v = (0,0,random.random()) )
continue
return neutrons
def test3(self):
'''create pure python representation of a homogeneous scatterer with
composite kernel. render the c++ computation engine of that kernel.
'''
#shape
from mccomposite.geometry import primitives
shape = primitives.block((1, 1, 1))
#kernel
nprinter = NeutronPrinter()
#composite kernel
composite_kernel = hs.compositeKernel()
composite_kernel.addElement(nprinter)
#scatterer
scatterer = hs.homogeneousScatterer(shape, composite_kernel)
#render the c++ representation
cscatterer = hs.scattererEngine(scatterer)
for i in range(10):
ev = mcni.neutron(r=(0, 0, -5), v=(0, 0, 1))
cscatterer.scatter(ev)
continue
return
def test3(self):
'neutron_storage.Storage: wrap-reading (nread>ntotal)'
path = 'test-storage-3'
if os.path.exists(path):
os.remove( path )
from mcni.neutron_storage.Storage import Storage
#open storage for writing
s = Storage( path, 'w' )
#create neutrons
import mcni
neutrons = mcni.neutron_buffer( 7 )
for i in range(7):
neutrons[i] = mcni.neutron( v = (i,0,0) )
#write
s.write( neutrons )
# flush
del s
#open the storage for reading
sr = Storage( path, 'r', packetsize=10)
neutrons = sr.read()
self.assertEqual( len(neutrons), 10 )
self.assertAlmostEqual( neutrons[5].state.velocity[0] , 5 )
self.assertAlmostEqual( neutrons[9].state.velocity[0] , 2 )
neutrons = sr.read()
self.assertAlmostEqual( neutrons[0].state.velocity[0] , 3 )
return
def test(self):
'neutron_storage.Storage: write and then read'
path = 'test-storage'
if os.path.exists(path):
os.remove( path )
from mcni.neutron_storage.Storage import Storage
#open storage for writing
s = Storage( path, 'w' )
#create neutrons
import mcni
neutrons = mcni.neutron_buffer( 7 )
neutrons[5] = mcni.neutron( v = (8,9,10) )
#write neutrons
s.write( neutrons )
#delete the storage to make sure it flushes all neutrons
del s
#open the storage for reading
sr = Storage( path, 'r')
neutrons = sr.read()
self.assertEqual( len(neutrons), 7 )
self.assertAlmostEqual( neutrons[5].state.velocity[0] , 8 )
return
def test5(self):
'neutron_storage.Storage: wrap-reading (nread>>ntotal)'
path = 'test-storage-4'
if os.path.exists(path):
os.remove( path )
from mcni.neutron_storage.Storage import Storage
#open storage for writing
s = Storage( path, 'w' )
#create neutrons
import mcni
neutrons = mcni.neutron_buffer( 5 )
for i in range(5):
neutrons[i] = mcni.neutron( v = (i,0,0) )
#write
s.write( neutrons )
# flush
del s
#open the storage for reading
sr = Storage( path, 'r')
neutrons = sr.read(100)
self.assertEqual( len(neutrons), 100 )
self.assertAlmostEqual( neutrons[3].state.velocity[0] , 3 )
self.assertAlmostEqual( neutrons[4].state.velocity[0] , 4 )
self.assertAlmostEqual( neutrons[6].state.velocity[0] , 1 )
self.assertAlmostEqual( neutrons[7].state.velocity[0] , 2 )
return
def test1(self):
'NDMonitor'
from mcni.components.NDMonitor import NDMonitor, Axis
xaxis = Axis(
name='x',
expression='x',
bins=100,
range=(0, 1000.),
unit='meter',
)
m = NDMonitor('abc', [xaxis])
N = 100
from mcni import neutron_buffer, neutron
b = neutron_buffer(N)
for i in range(N):
b[i] = neutron()
continue
m.process(b)
self.assertEqual(m.histogram.I[0], N)
self.assertEqual(m.histogram.E2[0], N)
self.assertEqual(m.histogram.I[1], 0.)
self.assertEqual(m.histogram.E2[1], 0.)
if interactive:
from histogram.plotter import defaultPlotter as plotter
plotter.plot(m.histogram)
return
def test1(self):
'detector hierarchy from xml'
from instrument.nixml import parse_file
instrument = parse_file( 'ARCS.xml' )
import instrument.geometers as ig
instrument.geometer.changeRequestCoordinateSystem(
ig.coordinateSystem( coordinate_system ) )
assignLocalGeometers( instrument, coordinate_system = coordinate_system )
detectorSystem = instrument.getDetectorSystem()
tofparams = 0, 10e-3, 1e-4
detectorSystem.tofparams = tofparams
dims = getDetectorHierarchyDimensions( instrument )
dims = [ dim for name, dim in dims ]
mca = md.eventModeMCA( outfilename, dims )
detectorSystem.mca = mca
cds = mh.scattererEngine( detectorSystem, coordinate_system = coordinate_system )
for i in range(nevents):
if i%1000 == 0: print i
ev = mcni.neutron( r = (0,0,0), v = (1500,0,2000) )
cds.scatter(ev)
continue
instrument.geometer = instrument.global_geometer
return
def __init__(
self,
name,
xwidth,
yheight,
zthickness,
mu,
sigma,
):
"""
Initialize the isotropicbox component.
Parameters:
name (str): the name of this component
xwidth (m): width
yheight (m): height
zthickness (m): thickness
mu (1/m): inverse absorption length
sigma (1/m): inverse scattering length
"""
self.name = name
self.propagate_params = (np.array(
[xwidth, yheight, zthickness, mu, sigma]), )
# Aim neutrons toward the sample to cause JIT compilation.
import mcni
neutrons = mcni.neutron_buffer(1)
neutrons[0] = mcni.neutron(r=(0, 0, -1), v=(0, 0, 1), prob=1, time=0)
self.process(neutrons)
def test1(self):
'complex. pack, detector, pixel hierarchy'
mca = md.eventModeMCA(
outfilename,
(npacks, ndetsperpack, npixelsperdet,) )
cylinder = operations.subtract( primitives.cylinder( sample2det * 1.1, detlength ),
primitives.cylinder( sample2det * 0.9, detlength ) )
ds = md.detectorSystem( cylinder, tofparams, mca )
pack0 = makepack()
packs = [pack0]
for i in range(1, npacks):
packs.append( mccomposite.scatterercopy( pack0, id = i ) )
continue
for i in range( npacks ):
z = 0 * meter
angle = (i-packindexat0)* 5./180 * N.pi
x = sample2det * math.cos(angle)
y = sample2det * math.sin(angle)
ds.addElement( packs[i], (x,y,z) )
continue
cds = mh.scattererEngine( ds, coordinate_system = "InstrumentScientist" )
for i in range(nevents):
if i%1000 == 0: print i
ev = mcni.neutron( r = (-L1,0,0), v = (vi,0,0) )
cds.scatter(ev)
continue
return
def process(self, neutrons):
import mcni
for i in range(len(neutrons)):
neutrons[i] = mcni.neutron(r=(1, 2, 3), v=(1, 2, 3))
continue
return neutrons
def __init__(
self, name,
w1, h1, w2, h2, l,
R0=0.99, Qc=0.0219, alpha=6.07, m=2, W=0.003):
"""
Initialize this Guide component.
The guide is centered on the z-axis with the entrance at z=0.
Parameters:
name (str): the name of this component
w1 (m): width at the guide entry
h1 (m): height at the guide entry
w2 (m): width at the guide exit
h2 (m): height at the guide exit
l (m): length of guide
R0: low-angle reflectivity
Qc: critical scattering vector
alpha: slope of reflectivity
m: m-value of material (0 is complete absorption)
W: width of supermirror cutoff
"""
self.name = name
ww = .5*(w2-w1); hh = .5*(h2 - h1)
hw1 = 0.5*w1; hh1 = 0.5*h1
self._params = (
float(ww), float(hh), float(hw1), float(hh1), float(l),
float(R0), float(Qc), float(alpha), float(m), float(W),
)
import mcni
neutrons = mcni.neutron_buffer(1)
neutrons[0] = mcni.neutron(r=(0,0,0), v=(0,0,1000), prob=1, time=0)
self.process(neutrons)
def test(self):
E_Q = "Q*Q/3."
S_Q = "1"
Qmin = 0; Qmax = 10
absorption_coefficient = scattering_coefficient = 1.
kernel = mccomponentsbp.create_E_Q_Kernel(
E_Q, S_Q,
Qmin, Qmax,
absorption_coefficient,
scattering_coefficient,
)
ei = 500 # meV
from mcni.utils import conversion
vil = conversion.e2v(ei)
vi = (0,0,vil)
import numpy.linalg as nl
import numpy as np
for i in range(10):
event = mcni.neutron(
r = (0,0,0), v = vi,
prob = 1, time = 0 )
kernel.scatter( event );
vf = np.array(event.state.velocity)
diffv = vi - vf
Q = conversion.v2k(nl.norm(diffv))
ef = conversion.v2e(nl.norm(vf))
E = ei - ef
# print E, Q, event
E1 = eval(E_Q)
self.assertAlmostEqual(E, E1)
continue
return
def test_copy(self):
'''copy'''
print "This test creates two identical blocks, each of which "\
"does not interact with neutrons. They print the info "\
"about the neutrons passing thru them, however. "\
"This test then send one neutron through these two "\
"blocks, so we should see two printings of neutron info, "\
"differing only on time-of-flight."
# create a shape
from mccomposite.geometry import primitives
smallblock = primitives.block((1, 1, 1))
#create pure python representation of scatterer composite
composite1 = mccomposite.composite(smallblock)
import UseNeutronPrinter2
nprinter = UseNeutronPrinter2.NeutronPrinter(smallblock)
composite1.addElement(nprinter)
#create a copy
copy = Copy.Copy(composite1)
#create a larget composite
largeblock = primitives.block((1, 1, 2))
composite = mccomposite.composite(largeblock)
composite.addElement(composite1, (0, 0, -0.5))
#composite.addElement( nprinter, (0,0,-0.5) )
composite.addElement(copy, (0, 0, +0.5))
#render the c++ representation
ccomposite = mccomposite.scattererEngine(composite)
ev = mcni.neutron(r=(0, 0, -5), v=(0, 0, 1))
ccomposite.scatter(ev)
return
def test2(self):
'shape positioning: cylinder with axis along beam'
# source
from mcni.components.MonochromaticSource import MonochromaticSource
import mcni
neutron = mcni.neutron(r=(0,0,-1), v=(0,0,1000), prob=1)
source = MonochromaticSource('s', neutron, dx=0.09, dy=0.09, dE=0)
# sample
from mccomponents.sample import samplecomponent
scatterer = samplecomponent('sa', 'cyl-along-beam/sampleassembly.xml' )
# neutrons
N = 1000
neutrons = mcni.neutron_buffer(N)
neutrons = source.process(neutrons)
# find neutrons out of target
arr = neutrons.to_npyarr()
x,y,z = arr[:, :3].T
missing = x*x+y*y > 0.04**2
# print neutrons
scatterer.process(neutrons)
# print neutrons
arr = neutrons.to_npyarr()
x,y,z = arr[:, :3].T
assert (z[missing] < -.9).all()
hit = arr[np.logical_not(missing), :3]
x,y,z = hit.T
assert (z > -.1).all()
assert (np.isclose((x*x + y*y)**.5, 0.04) | np.isclose(np.abs(z), 0.005)).all()
return
def test_scatterercopy(self):
'''scatterercopy'''
# create a weird shape
from mccomposite.geometry import primitives
shape = primitives.block( (1,1,1) )
#create pure python representation of scatterer composite
composite1 = mccomposite.composite( shape )
nprinter = NeutronPrinter( shape )
composite1.addElement( nprinter )
#create a copy
copy = mccomposite.scatterercopy( composite1 )
#create a larget composite
shape = primitives.block( (1,1,2) )
composite = mccomposite.composite( shape )
composite.addElement( composite1, (0,0,-0.5) )
composite.addElement( copy, (0,0,+0.5) )
#render the c++ representation
ccomposite = mccomposite.scattererEngine( composite )
ev = mcni.neutron( r = (0,0,-5), v = (0,0,1) )
ccomposite.scatter(ev)
return
def test(self):
"wrap Single_crystal"
from mcstas2 import componentfactory
factory = componentfactory(category, componentname)
component = factory('component',
xwidth=0.01,
yheight=0.01,
zthick=0.01,
delta_d_d=1e-4,
mosaic=5,
ax=3.8186,
ay=0,
az=0,
bx=0,
by=3.8843,
bz=0,
cx=0,
cy=0,
cz=11.6777,
reflections="YBaCuO.lau")
import mcni
neutrons = mcni.neutron_buffer(5)
for i in range(5):
neutrons[i] = mcni.neutron(r=(0, 0, -1),
v=(0, 0, 3000),
time=0,
prob=1)
continue
component.process(neutrons)
print neutrons
return
def test1(self):
'shape positioning: plate perp to beam'
# source
from mcni.components.MonochromaticSource import MonochromaticSource
import mcni
neutron = mcni.neutron(r=(0,0,-1), v=(0,0,1000), prob=1)
source = MonochromaticSource('s', neutron, dx=0.07, dy=0.09, dE=0)
# sample
from mccomponents.sample import samplecomponent
scatterer = samplecomponent('sa', 'plate/sampleassembly.xml' )
# neutrons
N = 1000
neutrons = mcni.neutron_buffer(N)
neutrons = source.process(neutrons)
# find neutrons out of target
arr = neutrons.to_npyarr()
x,y,z = arr[:, :3].T
missing = (x>0.03) | (x<-0.03) | (y>0.04) | (y<-0.04)
# print neutrons
scatterer.process(neutrons)
# print neutrons
arr = neutrons.to_npyarr()
x,y,z = arr[:, :3].T
assert (z[missing] < -.9).all()
hit = arr[np.logical_not(missing), :3]
x,y,z = hit.T
assert (z > -.1).all()
assert (np.isclose(np.abs(x), 0.03) | np.isclose(np.abs(y), 0.04) | np.isclose(np.abs(z), 0.005)).all()
return
def test1(self):
'NDMonitor'
from mcni.components.NDMonitor import NDMonitor, Axis
xaxis = Axis(
name = 'x', expression='x',
bins = 100, range=(0, 1000.),
unit = 'meter',
)
m = NDMonitor('abc', [xaxis])
N = 100
from mcni import neutron_buffer, neutron
b = neutron_buffer(N)
for i in range(N):
b[i] = neutron()
continue
m.process(b)
self.assertEqual(m.histogram.I[0], N)
self.assertEqual(m.histogram.E2[0], N)
self.assertEqual(m.histogram.I[1], 0.)
self.assertEqual(m.histogram.E2[1], 0.)
if interactive:
from histogram.plotter import defaultPlotter as plotter
plotter.plot(m.histogram)
return
def test1(self):
'Neutrons_from above'
rq = lambda Q: np.exp(-Q * Q / 25)
s = Sample('sample', 5, 5, rq)
from mcni import neutron_buffer, neutron
N = 8
nb = neutron_buffer(N)
t = 1.
for i in range(N):
vi = np.array((0, -(i + 1) * 100, (i + 1) * 100))
ri = -vi * t
nb[i] = neutron(r=ri, v=vi, s=(0, 0), time=0., prob=1.)
continue
nb2 = s.process(nb)
for i, (n, n2) in enumerate(zip(nb, nb2)):
# print "input:", n
# print "output:", n2
vf = np.array((0, (i + 1) * 100, (i + 1) * 100))
np.allclose(vf, n2.state.velocity)
np.allclose([0, 0, 0], n2.state.position)
np.isclose(n2.time, 1.)
vy = vf[1]
Q = np.abs(vy * 2) * conv.V2K
np.isclose(rq(Q), n2.probability)
return
def test(self):
"wrap SNS_source_r1"
from mcstas2 import componentfactory
factory = componentfactory(category, componentname)
component = factory(
'component',
S_filename="source_sct521_bu_17_1.dat",
width=0.1,
height=0.12,
dist=2.5,
xw=0.1,
yh=0.12,
Emin=50,
Emax=70,
)
import mcni
neutrons = mcni.neutron_buffer(5)
for i in range(5):
neutrons[i] = mcni.neutron(r=(0, 0, -1),
v=(0, 0, 3000),
time=0,
prob=1)
continue
component.process(neutrons)
print neutrons
return
def testCompositeScatteringKernel(self):
'CompositeScatteringKernel'
shape = mccompositebp.Block(1,1,1)
from neutron_printer3 import cKernel as Printer
printer = Printer( )
kernels = mccomponentsbp.pointer_vector_Kernel(0)
kernels.append( printer )
weights = mccomponentsbp.vector_double(0)
weights.append(1.)
rotmats = mccomponentsbp.vector_rotmat(0)
rotmat = mcnibp.RotationMatrix_double(1,0,0, 0,1,0, 0,0,1)
rotmats.append(rotmat)
average=False
kernelcomposite = mccomponentsbp.CompositeScatteringKernel(
kernels, weights, rotmats, average)
mcweights = mccomponentsbp.MCWeights_AbsorptionScatteringTransmission()
scatterer = mccomponentsbp.HomogeneousNeutronScatterer(
shape, kernelcomposite, mcweights )
for i in range(10):
ev = mcni.neutron( r = (0,0,-5), v = (0,0,1) )
scatterer.scatter(ev)
continue
return
def testCompositeScatteringKernel(self):
'CompositeScatteringKernel'
shape = mccompositebp.Block(1, 1, 1)
from neutron_printer3 import cKernel as Printer
printer = Printer()
kernels = mccomponentsbp.pointer_vector_Kernel(0)
kernels.append(printer)
weights = mccomponentsbp.vector_double(0)
weights.append(1.)
average = False
kernelcomposite = mccomponentsbp.CompositeScatteringKernel(
kernels, weights, average)
mcweights = mccomponentsbp.MCWeights_AbsorptionScatteringTransmission()
scatterer = mccomponentsbp.HomogeneousNeutronScatterer(
shape, kernelcomposite, mcweights)
for i in range(10):
ev = mcni.neutron(r=(0, 0, -5), v=(0, 0, 1))
scatterer.scatter(ev)
continue
return
def _init():
neutrons = mcni.neutron_buffer(ntotneutrons)
for i in range(ntotneutrons):
neutrons[i] = mcni.neutron(
r = (0,0,i),
)
continue
from mcni.utils import mpiutil
global mpirank
mpirank = mpiutil.rank
mpisize = mpiutil.world.size
if mpisize != 3:
raise RuntimeError, __doc__
import os
channel = 1000
if mpirank == 0:
if os.path.exists(neutron_storage_path):
os.remove(neutron_storage_path)
from mcni.neutron_storage.Storage import Storage
storage = Storage(neutron_storage_path, 'w')
storage.write(neutrons)
del storage
for i in range(1, mpisize):
mpiutil.send(0, i, channel)
continue
else:
mpiutil.receive(0, channel)
def test_copy(self):
'''copy'''
print "This test creates two identical blocks, each of which "\
"does not interact with neutrons. They print the info "\
"about the neutrons passing thru them, however. "\
"This test then send one neutron through these two "\
"blocks, so we should see two printings of neutron info, "\
"differing only on time-of-flight."
# create a shape
from mccomposite.geometry import primitives
smallblock = primitives.block( (1,1,1) )
#create pure python representation of scatterer composite
composite1 = mccomposite.composite( smallblock )
import UseNeutronPrinter2
nprinter = UseNeutronPrinter2.NeutronPrinter( smallblock )
composite1.addElement( nprinter )
#create a copy
copy = Copy.Copy( composite1 )
#create a larget composite
largeblock = primitives.block( (1,1,2) )
composite = mccomposite.composite( largeblock )
composite.addElement( composite1, (0,0,-0.5) )
#composite.addElement( nprinter, (0,0,-0.5) )
composite.addElement( copy, (0,0,+0.5) )
#render the c++ representation
ccomposite = mccomposite.scattererEngine( composite )
ev = mcni.neutron( r = (0,0,-5), v = (0,0,1) )
ccomposite.scatter(ev)
return
def test1a(self):
from sampleassembly.saxml import parse_file
import os
dir, filename = os.path.split(sampleassembly_xml)
save = os.path.abspath(os.curdir)
os.chdir(dir)
sa = parse_file( filename )
from mccomponents.sample.sampleassembly_support \
import sampleassembly2compositescatterer, \
findkernelsfromxmls
scatterercomposite = findkernelsfromxmls(
sampleassembly2compositescatterer( sa ) )
import mccomponents.homogeneous_scatterer as hs
engine = hs.scattererEngine( scatterercomposite )
os.chdir(save)
for i in range(1000):
ev = mcni.neutron( r = (0,0,-5), v = (0,0,3000) )
engine.scatter( ev )
# print ev
continue
return
def test1a(self):
from sampleassembly.saxml import parse_file
import os
dir, filename = os.path.split(sampleassembly_xml)
save = os.path.abspath(os.curdir)
os.chdir(dir)
sa = parse_file(filename)
from mccomponents.sample.sampleassembly_support \
import sampleassembly2compositescatterer, \
findkernelsfromxmls
scatterercomposite = findkernelsfromxmls(
sampleassembly2compositescatterer(sa))
import mccomponents.homogeneous_scatterer as hs
engine = hs.scattererEngine(scatterercomposite)
os.chdir(save)
for i in range(10):
ev = mcni.neutron(r=(0, 0, -5), v=(0, 0, 3000))
engine.scatter(ev)
print ev
continue
return
def test_scatterercopy(self):
'''scatterercopy'''
# create a weird shape
from mccomposite.geometry import primitives
shape = primitives.block((1, 1, 1))
#create pure python representation of scatterer composite
composite1 = mccomposite.composite(shape)
nprinter = NeutronPrinter(shape)
composite1.addElement(nprinter)
#create a copy
copy = mccomposite.scatterercopy(composite1)
#create a larget composite
shape = primitives.block((1, 1, 2))
composite = mccomposite.composite(shape)
composite.addElement(composite1, (0, 0, -0.5))
composite.addElement(copy, (0, 0, +0.5))
#render the c++ representation
ccomposite = mccomposite.scattererEngine(composite)
ev = mcni.neutron(r=(0, 0, -5), v=(0, 0, 1))
ccomposite.scatter(ev)
return
def test1(self):
'mccomponents.sample.samplecomponent: IsotropicKernel'
import mcni
neutron = mcni.neutron( r = (0,0,0), v = (0,0,3000), time = 0, prob = 1 )
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource('source', neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent( 'Al', 'sampleassemblies/Al-isotropickernel/sampleassembly.xml' )
instrument = mcni.instrument( [component1, component2] )
geometer = mcni.geometer()
geometer.register( component1, (0,0,0), (0,0,0) )
geometer.register( component2, (0,0,1), (0,0,0) )
N0 = 1000
neutrons = mcni.neutron_buffer(N0)
mcni.simulate( instrument, geometer, neutrons )
N = len(neutrons)
for i in range(10):
neutron = neutrons[i]
print neutron
continue
# N should be about 2/3 of N0. this is determined by
# the mc weights in Al-isotropic-kernel-plate-scatterer.xml
self.assert_( N < 0.72*N0 and N > 0.6*N0)
return
def test_expected_exits(position_x, velocity_z):
"""
Check that neutrons exit the guide at the expected angle, etc.
"""
import math
# set up simple guide
guide_length = 16
guide = Guide('test guide', 3, 3, 2, 2, guide_length)
guide_angle = math.atan(((3 - 2) / 2) / guide_length)
# set up particle
position = np.array([position_x, -1, 0], dtype=float)
velocity = np.array([0, 1, velocity_z], dtype=float)
# determine expected angle from z-axis of exit assuming two reflections
angle_expected = math.atan(velocity[1] / velocity[2])
for i in range(0, 2):
offset_from_normal = math.pi / 2 - angle_expected - guide_angle
angle_expected = math.pi - angle_expected - 2 * offset_from_normal
# propagate particle through guide
result = do_process(guide, [neutron(position, velocity)])
(position, velocity, duration) = (result[0:3], result[3:6], result[8])
angle_actual = math.atan(velocity[1] / velocity[2])
path_length = duration * np.linalg.norm(velocity)
# check outcome
assert np.isclose(position_x, position[0])
assert np.isclose(guide_length, position[2])
assert np.isclose(angle_expected, angle_actual)
assert guide_length < path_length < guide_length * 1.1
def test(self):
"wrap Fermi_chop2"
from mcstas2 import componentfactory
factory = componentfactory(category, componentname)
component = factory('component',
len=0.10,
w=0.06,
nu=600,
delta=0.0,
tc=0.0,
ymin=-0.03,
ymax=0.03,
nchan=32,
bw=0.00035,
blader=0.5801)
import mcni
neutrons = mcni.neutron_buffer(5)
for i in range(5):
neutrons[i] = mcni.neutron(r=(0, 0, -1),
v=(0, 0, 3000),
time=0,
prob=1)
continue
component.process(neutrons)
print neutrons
return
def test1(self):
'mccomponents.sample.samplecomponent'
import mcni
neutron = mcni.neutron( r = (0,0,0), v = (0,0,4149.48), time = 0, prob = 1 )
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource('source', neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent( 'V-constantE', 'sampleassemblies/V-constantE/sampleassembly.xml' )
instrument = mcni.instrument( [component1, component2] )
geometer = mcni.geometer()
geometer.register( component1, (0,0,0), (0,0,0) )
geometer.register( component2, (0,0,1), (0,0,0) )
neutrons = mcni.neutron_buffer( 1 )
from mcni.pyre_support.ConsoleNeutronTracer import ConsoleNeutronTracer
tracer = ConsoleNeutronTracer()
mcni.simulate(
instrument, geometer, neutrons,
multiple_scattering=True,
tracer = tracer
)
return
def _init():
neutrons = mcni.neutron_buffer(ntotneutrons)
for i in range(ntotneutrons):
neutrons[i] = mcni.neutron(r=(0, 0, i), )
continue
from mcni.utils import mpiutil
global mpirank
mpirank = mpiutil.rank
mpisize = mpiutil.world.size
if mpisize != 3:
raise RuntimeError, __doc__
import os
channel = 1000
if mpirank == 0:
if os.path.exists(neutron_storage_path):
os.remove(neutron_storage_path)
from mcni.neutron_storage.Storage import Storage
storage = Storage(neutron_storage_path, 'w')
storage.write(neutrons)
del storage
for i in range(1, mpisize):
mpiutil.send(0, i, channel)
continue
else:
mpiutil.receive(0, channel)
def test1(self):
from mccomponents.sample.sansmodel import sansspheremodel_kernel
scale=1.0e-6
radius=60.0 #A
contrast=1.0 #A-2
background=0 #cm-1
absorption_cross_section = 0
scattering_cross_section = 1
Qmin = 0
Qmax = 10
k = sansspheremodel_kernel(
scale, radius, contrast, background,
absorption_cross_section, scattering_cross_section,
Qmin, Qmax)
from mccomponents.sample import scattererEngine
kengine = scattererEngine( k )
print dir(kengine)
n = mcni.neutron( r = (0,0,0), v = (0,0,3000) )
kengine.scatter( n )
print n
return
def test(self):
"wrap Channeled_guide"
from mcstas2 import componentfactory
factory = componentfactory(category, componentname)
component = factory('component',
w1=-0.1,
h1=0.12,
w2=0.02,
h2=0.02,
l=2.0,
R0=0.99,
Qcx=0.021,
Qcy=0.021,
alphax=6.07,
alphay=6.07,
W=0.003,
k=1,
d=0.0005,
mx=1,
my=1)
import mcni
neutrons = mcni.neutron_buffer(5)
for i in range(5):
neutrons[i] = mcni.neutron(r=(0, 0, -1),
v=(0, 0, 3000),
time=0,
prob=1)
continue
component.process(neutrons)
print neutrons
return
def test1(self):
'mccomponents.sample.samplecomponent: DGSSXResKernel'
import mcni
neutron = mcni.neutron( r = (0,0,0), v = (0,0,3000), time = 0, prob = 1 )
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource('source', neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent( 'Al', 'sampleassemblies/Al-DGSSXResKernel/sampleassembly.xml' )
instrument = mcni.instrument( [component1, component2] )
geometer = mcni.geometer()
geometer.register( component1, (0,0,0), (0,0,0) )
geometer.register( component2, (0,0,6), (0,0,0) )
N0 = 10
neutrons = mcni.neutron_buffer(N0)
mcni.simulate( instrument, geometer, neutrons )
N = len(neutrons)
for i in range(10):
neutron = neutrons[i]
# print neutron
self.assert_(np.allclose(neutron.state.velocity, [3000, 0, 0], atol=20))
continue
return
def test(self):
"wrap TOF_monitor2"
from mcstas2 import componentfactory
factory = componentfactory(category, componentname)
component = factory(
'component',
nchan=100,
xmin=-0.1,
xmax=0.1,
ymin=-0.1,
ymax=0.1,
tmin=0.0,
tmax=0.00005,
filename="tof.dat",
)
import mcni
neutrons = mcni.neutron_buffer(5)
for i in range(5):
neutrons[i] = mcni.neutron(r=(0, 0, -1),
v=(0, 0, 3000),
time=0,
prob=1)
continue
component.process(neutrons)
print neutrons
return
def test7(self):
"neutron buffer: set element"
from mcni import neutron_buffer, neutron
b1 = neutron_buffer(1)
n = neutron(r=(0,10,0))
b1[0] = n
self.assertEqual(b1[0].state.position[1], 10)
return
def test7(self):
"neutron buffer: set element"
from mcni import neutron_buffer, neutron
b1 = neutron_buffer(1)
n = neutron(r=(0, 10, 0))
b1[0] = n
self.assertEqual(b1[0].state.position[1], 10)
return
def test3(self):
'MonochromaticSource - energy spread'
# source component
from mcni.components.MonochromaticSource import MonochromaticSource
from mcni import neutron_buffer, neutron
neutron0 = neutron(v=(0, 0, 3000), r=(0.3, 0.4, 1.5))
dx = 0.1
dy = 0.8
dE = 5
s = MonochromaticSource("name", neutron0, dx=0, dy=0, dE=dE)
# neutron buffer
N = 100000
b = neutron_buffer(N)
# process
s.process(b)
#
E0 = neutron0.energy()
#
n_in_onesigma = 0
n_in_twosigma = 1
for n in b:
E = n.energy()
# print n
# print E, E0
# not always true but usually true
self.assertNotEqual(E, E0)
#
if abs(E - E0) < dE:
n_in_onesigma += 1
if abs(E - E0) < 2 * dE:
n_in_twosigma += 1
self.assertEqual(
tuple(n.state.position),
tuple(neutron0.state.position),
)
self.assertEqual(
n.time,
neutron0.time,
)
self.assertEqual(
n.probability,
neutron0.probability,
)
continue
self.assert_(abs(n_in_onesigma * 1. / N - 0.68) < 0.01)
self.assert_(abs(n_in_twosigma * 1. / N - 0.95) < 0.01)
return
def test(self):
"wrap IQE_monitor"
from mcstas2 import componentfactory
category = 'monitors'
componentname = 'IQE_monitor'
factory = componentfactory(category, componentname)
Qmin = 0
Qmax = 13.
nQ = 130
Emin = -50
Emax = 50.
nE = 100
component = factory(
'component',
Ei=Ei,
Qmin=Qmin,
Qmax=Qmax,
nQ=nQ,
Emin=Emin,
Emax=Emax,
nE=nE,
max_angle_out_of_plane=30,
min_angle_out_of_plane=-30,
max_angle_in_plane=120,
min_angle_in_plane=-30,
)
scatterer = makeScatterer()
import mcni
N = 10000
neutrons = mcni.neutron_buffer(N)
for i in range(N):
neutron = mcni.neutron(r=(0, 0, 0), v=(0, 0, vi), time=0, prob=1)
scatterer.scatter(neutron)
neutrons[i] = neutron
#print neutrons[i]
continue
component.process(neutrons)
hist = get_histogram(component)
import os
f = os.path.basename(__file__)
filename = 'IQE-%s.h5' % f
if os.path.exists(filename): os.remove(filename)
import histogram.hdf as hh
hh.dump(hist, filename, '/', 'c')
if self.interactive:
from histogram.plotter import defaultPlotter
defaultPlotter.plot(hist)
return
def process(self, neutrons):
n0 = neutrons[0]
from mcni import neutron
self.neutron = neutron(
r=n0.state.position, v=n0.state.velocity,
s=(n0.state.spin.s1,n0.state.spin.s2),
time=n0.time,
prob=n0.probability,
)
return
def testHomogeneousNeutronScatterer(self):
'HomogeneousNeutronScatterer'
shape = mccompositebp.Cylinder(0.025/2., 0.01)
tof=0.001; pressure=10*101325
pixel = mccomponentsbp.DGSSXResPixel(tof, pressure, shape)
ev = mcni.neutron( r = (0,0,-3), v = (0,0,3000) )
pixel.scatter(ev)
print ev.probability
return
def test(self):
kernel = mccomponentsbp.IsotropicKernel(1,1)
for i in range(10):
event = mcni.neutron( r = (0,0,0), v = (0,0,3000), prob = 1, time = 0 )
kernel.scatter( event );
print event
continue
return
def test2(self):
"mccomponents.sample.samplecomponent: E_vQ_Kernel - discontinued dispersion surface"
import mcni
from mcni.utils import conversion
ei = 60
vil = conversion.e2v(ei)
vi = (0, 0, vil)
neutron = mcni.neutron(r=(0, 0, 0), v=vi, time=0, prob=1)
from mcni.components.MonochromaticSource import MonochromaticSource
component1 = MonochromaticSource("source", neutron)
from mccomponents.sample import samplecomponent
component2 = samplecomponent("Al", "sampleassemblies/Al-E_vQ_withdiscontinuity-kernel/sampleassembly.xml")
E_Q = "np.where(Qx*Qx+Qy*Qy+Qz*Qz>30, 25, 15)" # in sampleassemblies/Al-E_vQ-kernel/Al-scatterer.xml
instrument = mcni.instrument([component1, component2])
geometer = mcni.geometer()
geometer.register(component1, (0, 0, 0), (0, 0, 0))
geometer.register(component2, (0, 0, 1), (0, 0, 0))
N0 = 10000
neutrons = mcni.neutron_buffer(N0)
mcni.simulate(instrument, geometer, neutrons)
N = len(neutrons)
import numpy.linalg as nl
import numpy as np
from math import sin
N_noscatt = 0
for i in range(N):
neutron = neutrons[i]
vf = np.array(neutron.state.velocity)
diffv = vi - vf
# no scattering is fine
if np.linalg.norm(diffv) < 1e-12:
N_noscatt += 1
continue
Q = conversion.V2K * diffv
Qx, Qy, Qz = Q
ef = conversion.v2e(nl.norm(vf))
E = ei - ef
# print E, Q, neutron
E1 = eval(E_Q)
self.assertAlmostEqual(E, E1)
continue
print "\n* percentage of no scattering (Q happen to be at a singular point):", N_noscatt * 100.0 / N, "%"
return
