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1Bhabha Atomic Research Centre, Mumbai, India
National Facility for Neutron Beam Research 2
Neutrons for Condensed Matter Resarch 4
Single Crystal Diffractometer 6
Powder Diffractometer-1 8
Powder Diffractometer-2 10
Powder Diffractometer-3 12
Polarized Neutron Spectrometer 14
High-Q Diffractometer 16
Small-Angle Neutron Scattering Diffractometer 18
Double Crystal based SANS Instrument 20
Polarized Neutron Reflectometer 22
Spin Echo and Polarized Small Angle Neutron Scattering Instrument 24
Triple Axis Spectrometer 26
Quasi Elastic Neutron Spectrometer 28
Filter Detector Spectrometer 30
Neutron Radiography Facility 32
Neutron Detectors 34
Sample Environment Facilities 37
Contact Scientists 38
C o n t e n t s
2 Bhabha Atomic Research Centre, Mumbai, India
Neutron scattering at Trombay started
with the facility at Apsara reactor
(1 MW) in 1956, and then continued
with CIRUS (40 MW), which became
available in 1960 and then with the
present reactor Dhruva. Dhruva is a
100 MW natural uranium reactor with
peak thermal neutron flux of 1.8x1014
neutrons cm -2 s-1, tailor-made for
neutron scattering experiments with
tangential beam holes, through-tube,
provision for separate moderators for
cold and hot neutrons, guide-tube, etc.
Advanced instruments, fully automatic
in instrument control and data
acquisition modes have been installed
on various beam ports. State of the art
technology was used to design and
fabricate the spectrometers. 1-D and
2-D position sensitive detectors (PSD),
and associated electronics have also
been developed indigenously.
National Facility for Neutron Beam
Research (NFNBR) has been created as
a part of the Solid State Physics
Division (SSPD) during early nineties
to cater to the needs of the Indian
scientific community in the field of
neutron beam research. Scientists from
BARC, other DAE units, universities and
national laboratories are welcome to
use this facility through collaborative
reseach projects with SSPD scientists.
Many of these collaborations are being
supported by UGC-DAE Consortium
for Scientific Research, Board of
Research in Nuclear Sciences (BRNS)
and other agencies.
NationalFacility for
Neutron BeamResearch
International collaboration between neutron
beam research at BARC and other countries is
over four decades old. The first such
agreement was the “Indian-Philippines-IAEA
Agrement” signed during sixties, under
which BARC-built neutron instrument was
installed at Phillipines, and their scientists
were trained to use it. A more recent example
is the installation of a neutron spectrometer
at Bangladesh through IAEA in nineties.
Scientists from Phillipines, Korea, Indonesia,
Bangladesh, Vietnam, Malaysia and Egypt
have visited BARC to work on the neutron
instruments. A neutron instrument was
installed at the spallation neutron source at
Rutherford Appleton Laboratory in UK.
Scientists from SSPD avail advanced sources at UK, USA, Germany, France, Switzerland, Japan and other countries to carry
out front line research, and keep themselves up to date in this field.
Fig. 1. A panoramic view of CIRUS and DHRUVA reactors at BARC
3Bhabha Atomic Research Centre, Mumbai, India
General layout in the reactor hall and the guide-tube laboratory is shown in Fig. 2. There are four spectrometers at the
tangential beam lines, three at the ends of the through tube, two at the beam lines looking at the hot source, and four
instruments in the guide laboratory.
The present-day facilities include, single-crystal and powder diffractometers, polarization analysis spectrometer, Hi-Q
diffractometer, triple-axis & filter-detector spectrometers, quasi-elastic scattering spectrometer, all installed in the reactor
hall, and two small-angle scattering instruments, spin-echo spectrometer and reflectometer in the guide-tube laboratory.
80 K ice based cold neutron source and graphite at 1800 K hot source are under advanced stages of development.
Fig. 2. A layout of the neutron scattering instruments at Dhruva reactor
Fig. 3. A view of neutron scattering facilities inside the Dhruva reactor hall
4 Bhabha Atomic Research Centre, Mumbai, India
Neutrons forCondensed
MatterResearch
The existence of a neutral particle
similar to the mass of a proton, was
hypothesized by Rutherford in 1920
and this was proved by the discovery
of neutron by J. Chadwick, a student
of Rutherford, in 1932. Since its
discovery, neutrons have been used
as a great probe for research in
condensed matter.
Due to its various special properties,
neutrons provide an insight about the
microscopic structures and dynamics
in a wide class of materials. When get
scattered by the materials, neutrons
can not only tell about the position of
an atom in that material but also
atomic movement with time.
Particle nature
• Mass = 1.67x10-27 Kg
• Spin = 1/2 Acts as a tiny magnet
• Magnetic moment = -1.913 μN
• Velocity [2200m/s for thermal
neutrons of energy 25 meV]
Neutron’s properties which make all these possible
. Wave-particle duality
. Compatible wavelength with the inter-atomic distances for thermal
neutrons
. Compatible energy with atomic excitation energies
. Deep penetration due to the charge neutrality
. Scattering contrasts between neighbouring elements in the periodic table
. Isotope specific scattering and absorption
. Magnetic moment and thus can interact with magnetic materials
. Simple interaction with nuclei (isotropic s-wave scattering). No angular
dependence of scattering amplitude for nuclear scattering unlike in the case
of x-ray.
Wave nature
• Diffraction and interference
pattern
• Measurable wavelength
• Measurable scattering length
5Bhabha Atomic Research Centre, Mumbai, India
Unlike for x-rays, the neutron
scattering power of elements
varies in a zigzag fashion with
respect to the atomic mass. Due
to this special property, neutron
can differentiate neighbouring
elements in a material and even
sees differently the different
isotopes of an element.
Neutrons also allow to probe
light atoms that are barely visible
with x-rays. The scattering
length of neutron for a few
isotopes of some elements
are negative. Hydrogen has a
negative scattering length
( -3.739 fm) while Deuterium
possess a positive scattering
length (6.671fm). Suitable
combination of materials with positive and negative scattering length can be used to tune the neutron scattering contrast.
Contrast matching experiments are used to obtain multi-level structures.
As the neutron does not carry any
electric charge, the neutron has no
electrostatic interaction with the
electron cloud of an atom. For this
reason, the neutron has a higher
penetration power comparable to
x-ray or electrons.
Neutron has a spin ½ and is sensitive
to the magnetic fields created by
unpaired electrons. In the magnetic
materials, the order in magnetic
structures and the interactions can be
obtained using neutron scattering.
6 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole no. T1011
Monochromator Cu220
Wavelength 0.995
Scattering angle 0 o < 2θ < 90o
Flux at sample 5x105 n/cm2/sec
Detector BF3
Counter
The instrument is used to study a high
precision 3-dimensional structure of
materials, where hydrogen plays a
major role in either the stereochemistry
or the physical properties of the
materials. These include hydrates,
biomolecules, ferro-electrics, electro-
optic materials, etc.
The single crystal diffractometer is
located at T1011 beam line of the
Dhruva reactor. The crystal is rotated
about three Eulerian axes χ, φ and ω,and the detector is rotated about the
2θ axis. These four axes meet at a point,which is the centre of the sample
crystal. The χ circle is mounted on theω axis, while the φ circle is mountedon the χ-axis as shown in Figure.The crystal is mounted on the φ-axis.The geometry of axes mounting
enables any reciprocal lattice point to
be brought into the equatorial plane
of the diffractometer.
Single CrystalNeutron
Diffractometer
This Four Circle Eulerian geometrybased Single Crystal NeutronDiffractometer is used forthe studies on hydrogen-bondedcrystal structures.
Å
7Bhabha Atomic Research Centre, Mumbai, India
Selected examples
. Hydrogen bonding studies in bis(glycinium) oxalate
Fig.1. Showing the short hydrogen bond between glycinium and oxalate moiety
Single-crystal neutrondiffraction investigation ofbis(glycinium) oxalate wasundertaken in order to studyits hydrogen bondingnetwork, particularly the veryshort hydrogen bondbetween the glycinum andoxalate ions, indicated by theX-ray diffraction study. Thenon-existence of any phasetransition in these crystals wasattributed to the fact that theshort hydrogen bond inbis(glycinium) oxalate is asymmetric in nature, with no hydrogen disorder (Fig. 1). The potential energy landscape for theabove-mentioned H atom was found to have a single minimum closer to the glycinium ion. IR and Raman investigations ofthe title complex supported the above result.
Some references:
1. R. Chitra and R. R Choudhury, Acta Cryst. B 63, 497 (2007).2. R.Chitra, R.R. Choudhury and M.Ramanadham, Appl. Phys. A 74 (suppl.), S1576 (2002).3. R.R. Choudhury, R.Chitra and M.Ramanadham, Appl. Phys. A 74 (suppl.), S1667 (2002).
. Thiourea doped ammoniun dihydrogen phosphate
Fig. 2. Packing of the thiourea dopeddihydrogen phosphate
Thiourea Doped ADP (TADP) exhibits nonlinear optical property and thesecond harmonic generation efficiency of these crystals is three timesthat of pure ADP crystal. The single crystal neutron diffraction (Fig. 2)study of TADP gave cell parameters (a=b=7.531(3)Å,c=7.544(5)Å),which were found to be significantly greater from that of pure ADP atRT (a=b=7.502(1)Å,c=7.546(1)Å). This indicates that the dopantconcentration in the crystals is small but enough to bring changes in theoverall average structure. There is a significant lengthening of N-H—Ohydrogen bond in the Thiourea Doped ADP crystal.
8 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole No. TT1015
Monochromator Si (422)
Monochromatortake –offangle (2θ
M) 60°
Wavelength 1.094 Å
Detector One linear He3
PSD, covers 30°in one PSDsetting
(Sin θ/λ )max 0.64 Å-1
Flux at sample 5x105 n/ cm2/sec
Scattering angle 5o < 2θ < 90o
Resolution (Δd/d) 1 %
The diffractometer is extensively used
for studying crystal and magnetic
structures in a large variety of systems.
These studies include titanates and
zirconates showing ferro/anti-
ferro-electric properties, alloys of
transition metals, rare-earths and
actinides (UCu2Ge
2, ErFe
2D
x etc.)
showing exotic magnetic properties,
ferrites exhibiting disordered
magnetic ordering, manganites
showing CMR behaviour, and
cobaltates showing coexistence of
ferro- and antiferromagnetism, etc.
PowderDiffractometer-1
This instrument is installed atThrough-tube beam hole no TT1015and has been used to carry out medium-resolution powder diffractionmeasurements on a variety ofmagnetic and nonmagnetic systems.
S.K. Paranjpe and Y. D. Dande, Pramana-J. Phys. 32, 793 (1989).S.K. Paranjpe and S. M. Yusuf, Neutron News 13, 36 (2002).
9Bhabha Atomic Research Centre, Mumbai, India
Neutron powder diffraction patterns of CaTiO3 (CT)
and Sr1-x
CaxTiO
3 (SCT) with x = 0.04 and 0.50. For
the CT and SCT (x=0.50) samples, superlattice linesare observed.
Temperature variation of I531
/ I006
for Sr1-x
CaxTiO
3 (SCT) with
x = 0.06 and 0.12. The antiferrodistortive phase transition isobserved around 300 K and 375 K for x = 0.06 and 0.12,respectively.
Some references:
1. V. G. Sathe et al., J. Phys.-Cond. Matter 10, 4045 (1998).2. R. Ranjan et al., J. Phys.-Cond. Matter 11, 2233 (1999).3. P. Raj et al., Phil. Mag. B 79, 1185 (1999).4. A. Das et al., J. Magn. Magn. Mat. 237, 41 (2001) .5. S. M. Yusuf et al., Phys. Rev. B 68, 104421(2003).
Selected examples
. Mixed Ferrites: Disordered Magnetic Systems: Magnetic ordering in Zn0.5
Co0.5
FeCrO4
The evolution of themagnetic structure factorwith temperature for (a)the (220) reflection and(b) the (222) reflectionfor Zn
0.5Co
0.5FeCrO
4.
Solid curves: The Brillouinfunctions
Difference neutron diffraction patterns at 40,20, and 15 K with respect to 200 K forZn
0.5Co
0.5FeCrO
4 showing the buildup of the
diffuse hump at ~20 K around a Q-value wherethe (200) Bragg peak is expected.
. Structural phase transition in ferroelectric materials
10 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole no. T1013
Monochromator Ge (331)
Wavelength 1.249 Å
Beam size 4.0 cm x1.5 cm
Flux at sample 8.5x105 n/cm2/sec
Scattering angle 4o < 2θ < 140o
Q range 0.4 – 9.4 Å-1
Δd/d ~ 0.8 %
Detector 5 PSDs (to beupgradedto 15 PSDs)
Sampleenvironment 10 – 300 K
PowderDiffractometer-2
This Powder diffractometeris a conventional medium resolutionneutron diffractometer. It is mainly used tostudy stuctural and magnatic ordering inpolycrystalline materials.
Powder diffractometer is a multi-PSD
based instrument covering Q-range
up to 9.4 Å-1. This instrument is being
extensively used by researchers all over
the country to study structural and
dimensional magnetic materials,
molecular magnetic materials and also
in studies of local structure
determination from disordered
crystalline systems.
magnetic transitions in alloys and
compounds. It has been used for
structural studies of a number of CMR
materials, ferro-electric materials, high
Tc materials, SOFC materials, low
11Bhabha Atomic Research Centre, Mumbai, India
Selected examples
. Low temperature structural phase transitions in NaNbO3
Material engineering of alkaline niobates like potassium sodium niobate and lithium sodium niobate with ultralarge piezo
response comparable to PZT have evoked considerable interest as the next generation eco-friendly lead free piezo ceramics
required for applications as transducers in cell phones, medical implants, etc. The end member NaNbO3 has an antiferroelectric
(AFE) structure at room temperature and exhibits an unusual complex sequence of temperature and pressure driven
structural phase transitions which are not clearly understood. Accurate characterization of the phase diagram of NaNbO3 is
essential for the design of new sodium niobate based ceramics required for applications. Powder neutron diffraction
studies have been used to understand the complex sequence of low temperature phase transitions of NaNbO3 in the
temperature range between 12 and 350 K. Our studies present unambiguous evidence for the presence of the ferroelectric
(R3c) phase (FE) of NaNbO3 coexisting with an antiferroelectric phase (Pbcm) over a wide range of temperatures. (S.K.
Mishra et al., (2007).
The physical properties in charge ordered manganites are influenced by magnetic
field, pressure, and substitution effects. Here we study the effect of change in
ionic radii on the magnetic structure and its influence on the measured physical
properties. The figure shows a section of the neutron diffraction pattern of
La0.5
Ca0.5-x
SrxMnO
3 at 15 K. With increase in Sr concentration the magnetic
structure evolves from a CE-type antiferromagnet to ferromagnet with an
intermediate A-type antiferromagnetic structure. The magnetic structure
influences the magnetic and transport properties .
Some references:
1. S.K. Mishra et al., Phys. Rev. B 76, 024110 (2007).
2. I. Dhiman et al., Solid State Communications 141, 160 (2007).
3. S. Taran et al., J. Phys. Cond. Matter (in press).
4. Brajendra Singh et al., J. Appl. Phys. 101, 09G518 (2007).
5. S. N. Achary et al., J. Alloys and Compounds 438, 274 (2007).
Structure of NaNbO3
913 K (PE)300 K (AFE) 12 K (FE)
. Evolution of magnetic structures in charge ordered manganites
12 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole no. TT1015
Monochromator Bent perfect Si
Wavelength 1.48 Å(standard)
Beam size 15 × 25 mm2
Flux at sample 7×107 n/cm2/sec
Scattering angle 6 – 123O
Q range 0.4 – 7.4 Å-1
(1.48 Å)
Δd/d ~ 0.3%
Detector 4 Linear 3HePSDs (to beupgraded to12 nos.)
PowderDiffractometer-3
This diffractometer, installed recently,with focusing monochromator,is expected to be widely used in thearea of chemical and magnetic structuresof novel materials.
This powder diffractometer developed
and installed by UGC-DAE
Consortium for Scientific Research, is
a multi-PSD high throughput
diffractometer. It employs a bent
perfect crystal monochromator at a
take-off angle of 90
degrees and it is
designed for a
highly focused
neutron beam of
about 15 x 25 mm2
in size. This would
enable high flux
at sample position
and also use of
small samples
(~1 cc in volume).
The resolutions obtained are up to
Δd/d ~ 0.3%.
The monochromator can be rotated or
flipped to give a range of wavelengths
from 1.1 to 2.3 Å. The sample
environment consists of a 4 K CCR for
standard measurements as a function
of temperature and a cryogen-free
7 Tesla magnet with VTI for in-field
measurements down to 1.4 K. An
oscillating radial collimator (under
installation) will be used to suppress
extraneous contributions from the
magnet and CCR shrouds. The data
acquisition system, developed locally,
has an input for up to 16 PSDs and
the software enables recording various
sequences of measurements with
respect to incident neutron flux and
sample temperature.
13Bhabha Atomic Research Centre, Mumbai, India
. Monochromator Rocking Curve and Beam Profiles
Rocking curve of bent perfect Si monochromator at a take-off angle of 90º
and λ = 1.48 Å. Figures on right show the horizontal and vertical beamprofiles measured at sample position.
Some references:
1. A.V. Pimpale, B.A. Dasannacharya, V. Siruguri, P.D. Babu, P.S. Goyal, Nucl. Instrum. Meth.A481 (2002) 615
2. S. Patnaik et al (unpublished)
. Neutron diffraction pattern of YMnO3 taken at room temperature [2] at λ = 1.48 Å.
14 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole No. T1009
Wavelength 1.201 Å
Beam polarization 98.83%
Flipper RF flipper /DC flipper
Flux at sample 3.6x105
n/cm2/sec
Scattering angle 0o < 2θ < 120o
Analyzer efficiency 97.36% /99.89%
Detector BF3 counter
Available T range 1.5 – 300 K
Available H 1.2 kOe
The polarized neutron spectrometer (PNS) is used for magnetic
scattering studies. This spectrometer can be used in different
modes, such as (a) diffraction mode (2-axis configuration), (b)
polarization analysis mode (3–axis configuration in scattering
geometry), and depolarization mode (3-axis configuration in
transmission geometry). The instrument has been used for
studying mixed ferrites, 3d-based alloys, uranium / thorium /
cerium based intermetallic compounds, amorphous magnets,
CMR perovskites, quasi 1-D spin chain compounds, etc.
PolarizedNeutron
Spectrometer
This PNS instrument is installedat the end of the tangential beamhole No. T1009. The spectrometeris used for magnetic correlation studies.
S. M. Yusuf and L. Madhav Rao, Neutron News 8, 12 (1997).S. M. Yusuf and L. Madhav Rao, Pramana- J. Phys. 47, 171 (1996).
15Bhabha Atomic Research Centre, Mumbai, India
Selected examples
. Magnetic and Electronic Phase Transitions-Ionic Size Effect in (La1-x
Dyx)0.7
Ca0.3
MnO3
CMR Perovskites
Increasing Dy concentration drives the system first into a local cantedferromagnetic (LCF) state with a reduced metal-insulator transition temperature(for x = 0.114 and 0.243) and then (for x = 0.347) to an “insulating”cluster-spin glass state .
. Neutron Depolarization Study on CMR Perovskites (Nd1-x
Tbx)0.55
Sr0.45
MnO3
Some References:
1. S. M. Yusuf, L. Madhav Rao and P. Raj, Phys. Rev. B 53, 28 (1996).2. S. M. Yusuf et al., Solid State Commun. 112, 207 (1999).3. S. M. Yusuf, M. Sahana, K. Dorr, U.K. Röbler and K. H. Müller, Phys. Rev. B 66, 064414 (2002).4. S. M. Yusuf et al., Phys. Rev. B 68, 104421 (2003).5. S. M. Yusuf et al., J. Magn. Magn. Mater. 272-276, 1288 (2004).
The crossover from long-range to short-range magnetic ordering in the CMR perovskites is studied by complementaryneutron scattering techniques. A canted ferromagnetic state for x < 0.5 with large domains (> 1000 nm), ferromagnetic-like spin clusters of ~ 100 nm size for 0.5< x < 0.6 and only short range correlation of ~ 5 nm for x > 0.6 compositions havebeen observed.
16 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole no. HS1019
Monochromator Cu (220): λ = 0.783ÅCu (111): λ = 1.278Å
Flux at sample 2x106 (λ = 1.278 Å(n/cm2/sec) 3x105 (λ = 0.783 Å)
Sample size 40 mm high &5-10 mm dia
Scattering angle 3o < 2θ < 140o
Detector 10 (1-d PSDs)at 5 positions
Q range 0.3 – 15 Å-1
ΔQ/Q 2.5 %
Hi-Q diffractometer is a multi-
PSD based instrument covering
Q-range up to 15 Å-1. It has been used
for structural studies of a number of
molecular fluids, chalcogenide
glasses,borate glasses, phosphate
High - QDiffractrometer
This High-Q diffractometer is a conventionalneutron powder diffractometer with highQmax (=15 Å-1) with λ = 0.783 Å and isused mainly to understand short rangeorder in glasses, liquids and disorderedcrystals.
glasses, tellurite glasses, sulphide
glasses, amorphous carbon and also
in studies of local structure
determination from disordered
crystalline systems. This diffractometer
has also been used to study high
pressure structural phase transitions
in α-Resorcinol, NbO2F etc., using a
home made piston cylinder type
pressure cell using EN45 steel as the
cell material.
17Bhabha Atomic Research Centre, Mumbai, India
Selected examples
. H-bonded simple alcohols
Simple alcohols like CD3OD, t-butanol
and 2-propanol show intermediate
range order characterized by
a pre-peak which is due to molecular
clusters (mainly hexamer) through
H-bond association. On the other
hand 1-propanol does not show any
pre-peak and the H-bonded
association of the molecules lead to
open chain clusters instead of closed
cyclic chain clusters. The main reason
is that the first group of alcohols all
have methane like structure where as
1-propanol is a linear molecule. The
top right hand side figure shows
schematic of the cyclic chain clusters
. Rare earth phosphate glasses: Radioactive waste storage materials
T(r) shown for R=Ce glass showing
the P-O, R-O & O-O distances. PO4
tetrahedra are the basic building blocks in
these glasses
Glasses with general formula 0.1La2O
3 - 0.1R
2O
3 - 0.05Al
2O
3 – 0.75P
2O
5 are candidates of radioactive waste storage
materials as they are chemically durable and pouring temperatures are low. Some phosphate glasses have low leachingrates compared to the alternative borosilicate glasses. We found that these glasses have mainly PO
4 tetrahedral units. R-O
co-ordination is about 6 to 8. A 3D-hand built model is displayed with the intention of confirming the feasibility ofconstructing a continuous random network. Some of these glasses are found to be good candidates as UV filters anda patent has been obtained for the same.
Some References:
1. A.G. Shikerkar et al., J. Non-Cryst. Solids. 270, 234 (2000).2. A.K. Karmakar et al., Phys. Lett. A 253, 207 (1999).3. P.P. Nath et al., Z. naturforschungs 56a, 825 (2001).4. A. Sahoo et al., Pramana – J. Phys. 63, 183 (2004).5. Keka R. Chakraborty et al., Pramana – J. Phys. 63, 245 (2004).
n 2-propanol whereas the bottom one shows open chain clusters in 1-propanol.
18 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam port Guide G1
λ* (guide cut-off) 2.2 Å
Monochromator BeO Filterat 77 K
λcut-off 4.7 Å
λaverage 5.2 Å
(Δλ/λ) ~15 %
Flux at sample 2.2×105 n/cm2/sec
Source slit (S1) 3 cm × 2 cm
Sample slit (S2) 1.5 cm × 1 cm
Distance S1 & S2 2 m
Angular divergence ± 0.5o
Detector (D) linear He3-PSD
Distance S2 & D 1.85 m
Q range 0.017 – 0.35 Å-1
The SANS diffractometer is widely
used to investigate the structure(shape and size) of different kinds of
mesoscopic systems such as micellarsolutions, magnetic fluids, protein
solutions and colloidal suspensions.
Small-angleNeutron
ScatteringDiffractometer
This SANS diffractometer isinstalled at the end of one ofthe guides. The diffractometeris suitable for studies ofinhomogeneities of the sizesin the range 10 – 200 Å.
This is a conventional slit-geometry SANS diffractometer. It makes use of BeOfilter as a monochrometer. The beam passes through two slits S1 and S2 before
it is incident on the sample. The angular distribution of neutrons scattered by thesample is recorded using a 1-m linear positive sensitive detector.
V.K. Aswal and P.S. Goyal, Current Science 79, 947 (2000)
19Bhabha Atomic Research Centre, Mumbai, India
Selected examples
. Protein crystallization in aqueous salt solutionThe process of proteincrystallization is of interestfrom both scientific andbiological aspects.Structural evolution amongprotein macromolecules isan important step inunderstanding the processthat the system isundergoing duringcrystallization. It has beenobserved that the effect ofsalt concentration as well
as that of different salts on protein crystallization is markedly different (Fig. 1). SANS data suggest that difference in thecrystallization on varying concentration/type of salt is related to the differences in structures in these samples in terms of thepopulations of monomers and dimmers (Fig. 2). Higher-mers are not observed as they are formed in very small numberstowards the process that leads to crystallization.
. Tuning gelation of block copolymer/surfactant mixed systemsS e l f - a s s e m b l ybehavior of theP E O - P P O - P E Obased triblockcopolymers havebeen studied quiteextensively in viewof their richs t r u c t u r a lp o l y m o r p h i s mand numerousapplications in theindustries. In manyapplications, they
are used in combinations with ionic surfactants like SDS, CTAB etc. Fig. 4 shows lower (T1) and upper (T2) meltingtemperature of cubic gels formed by 25% of block copolymer (EO)20(PO)70(EO)20 solutions as a function of SDS concentration.The gel phase can be tuned by the ratio of the two components. Contrast variation SANS studies show that the blockcopolymer and SDS form mixed micelles comprising a uniform distribution of the respective molecules (Fig. 4).
Some references
1. V.K. Aswal and P.S. Goyal, Phys. Rev. E 6161616161, 2947 (2000).2. J. Sharma, V.K. Aswal, P.S. Goyal and H. Bohidar, Macromolecules 3434343434, 5215 (2001).3. J. Haldar, V.K. Aswal, P.S. Goyal and S. Bhattacharya, Angew. Chem. Int. Ed. 4040404040, 1228 (2001).4. S. Chodankar and V.K. Aswal, , , , , Phys. Rev. E 7272727272, 041931 (2005).5. R. Ganguly et al., J. Phys. Chem. B 110110110110110, 9843 (2006).
Fig. 4Fig. 4Fig. 4Fig. 4Fig. 4Fig. 3Fig. 3Fig. 3Fig. 3Fig. 3
Fig. 1Fig. 1Fig. 1Fig. 1Fig. 1 Fig. 2Fig. 2Fig. 2Fig. 2Fig. 2
20 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam port Guide G1
Monochromator Si(111)
Wavelength (λ) 3.12 Å
(Δλ/λ) ~1 %
Flux at sample 500 n/cm2/sec
Analyser Si(111)
Q range 0.0003-0.0173 Å-1
Real space 200 - 10000 Åresolution
Detector BF3 Counter
This facility is widely used toinvestigate the mesoscopicinhomogeneties in ceramics,metallurgical alloys, naturallyoccuring porous media like rock etc.
In this kind of double crystal basedinstruments, unlike pinholecollimation instruments, thecollimation is performed in thereciprocal space only and theresolution in wave vector transfer Q isindependent of the beam crosssection. Because of the non-dispersive setting of both the crystals,the width of the rocking curve isindependent of the divergenceof the incoming beam.
DoubleCrystal based
SANSInstrument
This is a double crystal based mediumresolution small-angle neutron scatteringinstrument built and commissioned at theguide tube laboratory. The instrumentconsists of a non-dispersive (1, -1) setting of(111) reflections of silicon single crystals withsample between the two crystals.
S. Mazumder, D. Sen, T. Saravanan and P. R.Vijayaraghavan,J. Neutron Research 9, 9, 9, 9, 9, 39 (2001)
21Bhabha Atomic Research Centre, Mumbai, India
Selected examples
. Effect of pore structure on low frequency dielectric response in ZrO2-8 %Y2O3 ceramic compact
Yttria stabilized zirconia is
a potential candidate forsolid oxide fuel cell
applications. SANS data forZrO2-8 % Y2O3 pellet
samples with identicalporosity but prepared from
finer and coarser grain areshown (left). Scattering
experiments have beencarried out for
two different samplethicknesses in order to
correct for multiple scattering. The real and the imaginary components of the dielectric response forthese samples are depicted (right). The variation in the dielectric response has been explained by a pore
structure dependent interfacial polarization, ion hopping and conduction.
. Carbide precipitates in solution quenched PH 13-8 Mo stainless steelPH13-8 Mo, because of itshigh strength andtoughness, coupled with
good corrosion resistance, isoften used in aircraft, nuclear
reactor, petrochemical plantsand many other challenging
applications. SANS data fromsolution quenched (from
1000oC) sample for twodifferent sample thickness
are shown (left). Theestimated single scattering profile is also shown in the inset. TEM (left inset) shows the presence block like precipitates. The
size distribution of the parallelepiped block precipitates, estimated from SANS, is shown (right).
Some references
1. D. Sen, S. Mazumder and S. Tarafdar; J. Mat. Sci 3737373737, 941 (2002).2. S. Mazumder et al. Phys. Rev. Lett. 9393939393, 255704 (2004); S. Mazumder, et al Phys. Rev. B 7272727272, 224208 (2005).3. D Sen, T. Mahata, A K Patra, S Mazumder and B P Sharma; J. Phys.: Condens. Matter 1616161616, 6229 (2004).4. D. Sen et al. Mat. Sci. & Eng A 397397397397397, 370 (2005); J. Mittra et al. Scripta Materilia 5151515151, 349 (2004).5. A.K. Patra, S. Nair, A.K. Tyagi, D. Sen, S. Mazumder, S. Ramanathan; J. Alloys and Comp. 403403403403403, 288 (2005).
22 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Monochromator Si(113)
Wavelength 2.5 Å
ΔQ/Q 0.141 - 0.411
Polarizer FeCo/TiZrsupermirror
Flux at sample 104 n/cm2/sec
D.C. flipper 92 %efficiency
Detector linear He3 PSD
Reflectivity 1 – 10-4
The reflectometer uses a linear position sensitive detector, which helpsto collect the off-specular reflectivity data in addition to specular
reflectivity data from the thin film samples, in a single setting.
This facility has been widely used for structural and magneticcharacterization of thin film samples, using specular and off-specular
techniques.
Reflectivity is intrinsically sensitive to the difference of the refractiveindex (or contrast) across any interface. For the case of specular
reflection, the intensity of the reflected beam is related to the depthdependence of the index of refraction averaged over the lateral
dimensions of the sample. Polarized neutron reflectometry is a uniquetechnique to study the depth profile of magnetic moment in multilayer.
Off-specular or diffuse neutron reflectivity is a widely used techniqueto understand surface (interface) morphology.
PolarizedNeutron
Reflectometer
The polarized neutron reflectometeris located in Guide Tube laboratory.The reflectometer has been designed forvertical sample geometry. It utilizes ahighly collimated monochromatic:polarized or unpolarized beamof neutrons.
Saibal Basu and Surendra Singh, J. Neutron Research 1414141414, 109 (2006).
23Bhabha Atomic Research Centre, Mumbai, India
Selected examples
. Investigation of interface magnetic moment in Fe/Ge multilayer
Metal-semiconductor interfaces display transport and magnetic properties which strongly depend on interface quality viz.roughness, alloying at interfaces, and magnetic moment at interface. Polarized neutron reflectivity data on Fe/Ge multilayers(left and right) have been used to clearly demonstrate that there is overall reduction in magnetic moment of Fe atoms as wellas asymmetry of moments at the Fe/Ge interfaces.
. Corrosion-induced morphology in Ni Film: a study in off-specular reflectometry
The microscopic fractal morphology of corrosion front at the exposed air-film interface of a Ni film as well as the morphologyof an interface buried below the affected surface layer have been used to determine off-specular neutron reflectivity (right)and specular neutron reflectometry (left) in unpolarized mode. Differences in morphology, of a hidden interface vis-à-visthe exposed surface under corrosion (middle), at microscopic length-scales have been quantified in terms of fractaldimension of these two surfaces.
Some references
1. Surendra Singh, Saibal Basu, M. Vedpathak, R. H. Kodama, R. Chitra and Y. Goud, Appl. Surf. Sci. 240240240240240,251 (2005).
2. Surendra Singh, Saibal Basu, A.K. Poswal and M. Gupta, Solid State Comm. 136136136136136, 400 (2005).3. Surendra Singh and Saibal Basu, Surf. Sci. 600600600600600, 493 (2006).4. Surendra Singh, S.K. Ghosh, Saibal Basu, M. Gupta, P. Mishra and A.K. Grover, Electrochem. & Solid State Lett.
99999, J5 (2006).5. Surendra Singh, Saibal Basu, Mukul Gupta, Mahesh Vedpathak, and R.H. Kodama, J. Appl. Phys. 101101101101101,
33913 (2007).
24 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam port Guide G2
λ∗ (guide cut-off) 3.1 Å
Monochromator BeO Filter (77 K)
λcut-off 4.7 Å
λaverage 5.2 Å
(Δλ/λ) ~15 %
Flux at sample ~105 n/cm2/sec
Detector (D) linear He3-PSD
Real space length 20-400 Åscale
Q range (SANS) 0.015 – 0.3 Å-1
Spin Echoand
Polarized SANSInstrument
This instrument consistsof two arms,i) Spin echo andii) polarised neutronssmall angle scattering.
The spin echo technique is used tostudy stochastic dynamics of polymers,
macromolecules etc. BeO filterproduces a quasi-monochromatic
neutron beam. A focusing soller-typemulti-segment supermirror based
polarizer and analyzer are used topolarize and analyze the neutrons.
Similar π and π/2 flippers are used tochange the direction of neutron
polarization. A multilayer copper wiresolenoid is used as guide field to
initiate Larmor precession of theneutrons. A 3He detector is used to
detect the neutrons. The maximumq-range is 1 Å-1. Dynamical systems
of real space correlations of about10 Å and a time scale of 1 ns can be
investigated.
The small angle scattering instrument is a slit geometry configuration, using BeO
filter cooled at liquid nitrogen temperature. The incident neutrons are polarizedusing a multi-segment soller type
supermirror polarizer (Co/Ti coatedwith anti-reflecting Gd coating). The
distance between the sample and thedetector is 2.21 m which may be
increased to about 3 m. This setup canbe used to investigate shape and size
of different mesoscopic systems likemicellar solutions, proteins and the
study of magnetic inhomogeneties.
25Bhabha Atomic Research Centre, Mumbai, India
Some references
1. S. L. Chaplot, R. Mittal, Prabhatasree Goel, Appl. Phys. A7474747474 (suppl). S280 (2002).2. S. L. Chaplot, R. Mittal, K. N. Prabhatasree, Neutron spin echo spectroscopy, eds. F. Mezei, C. Pappas and T.
Gutberlet (Springer verlag, Berlin 2003) p 48.
Selected examples
. Surfactants in aqueous solution
Surfactants are amphiphilic molecules with water repelling and water loving ends, they self-assemble to form micelles inaqueous solutions. SANS data on 0.2 M micellar solution of anionic surfactant Sodium Dodecyl Sulphate prepared in D2Oare shown. SANS distribution shows a correlation peak at Qmax ~ 0.07 Å
-1, which is due to a peak in the interparticlestructure factor S(Q). This corresponds to average distance (~2π/Qmax) between micelles of about 90 Å.
. Cobalt precipitates in Copper annealed at 560O CSmall angle neutronscattering studies on diluteCu alloy with 0.8 at %Co havebeen carried out. Cobalt formsprecipitates whose sizesdepend on reaction kinetics.The sample studied wassolution treated at 950OC for3 hrs in a vertical furnace inargon atmosphere, followedby rapid quench into waterat room temperature andannealed at 560OC for 80minutes.
26 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole no. T1007
Monochromator Cu(111)
ΔE range 3 – 200 meV
Q range 1 – 10 Å-1
lncident 0.6 – 2.3 Åwavelength range
Flux at sample 106 n/cm2/sec
Analyzer PG(0002)
Filter PG
Scattering angle 10o – 100o
Detector BF3 Counter
Triple AxisSpectrometer
This instrument is used tostudy inelastic Neutron Scatteringfrom single crystals andpolycrystalline samples.
This instrument has been successfullyemployed for measurement of phonondispersion curves, phonon density ofstates, crystal field excitations andquasielastic scattering.
The geometry of the triple axisspectrometer allows measurements ofthe scattering function S(Q,E) in singlecrystals at well defined values ofmomentum transfer Q and energytransfer E.
Principal components of thisinstrument are:
(i) Monochromator that producesthe mono-energetic neutronbeam.
(ii) Positional spectrometer that setsthe angles φ and ψ.
(iii) Analyzer that measures theoutgoing energy.
Various arms of the spectrometer canbe moved at angular speeds of severaldegrees/ minute by means of wormgear assemblies.
The shielding wedges of the monochromator shield are lifted automatically toallow for continuous variation of the monochromator settings.
S.L. Chaplot, R. Mukhopadhyay, P.R. Vijayaraghavan, A.S. Deshpande andK.R. Rao, Pramana - J. Phys. 3333333333, 595 (1989).
27Bhabha Atomic Research Centre, Mumbai, India
Selected examples. Al2SiO5: Andalusite, a polymorph having five-coordinated aluminiumAl2SiO5 exists in threepolymorphic forms: sillimanite,
andalusite and kyanite with onealuminium in tetrahedral, five-
coordination and octahedralcoordination respectively. These
display unique phase transitionswith pressure and temperature
and the phase diagram hasextensive applications in
geophysics. Experiments on allthree phases validated a
transferable interatomic potentialto explain vibrational and
thermodynamic properties of these polymorphs. (Left) Polyhedral representation of andalusite crystal structure with AlO6octahedra in red, five-coordinated Al in blue, SiO4 tetrahedra in yellow. (Right) Measured (solid squares) and calculated
(solid line) phonon dispersion curves along the Σ direction in andalusite. The (zone centre) phonon frequencies knownfrom Raman (open triangle) and infrared (open diamond) measurements are also shown.
. M2O (M=Cu, Ag): Negative Thermal Expansion materialsM2O (M=Cu, Ag)
exhibits negative thermalexpansion (NTE).
Experiments helped todevelop lattice dynamical
model which identifiedlibrational mode related
to NTE, explainedbond length variation
in agreement withpublished EXAFS data, and stabilized lattice with a single M-M potential. (left) Experimental and calculated phonon spectra
for Cu2O. (centre) Structure of M2O. The solid circles denote M and O atoms in decreasing order of size. (right) Polarizationvector of T2u mode shows rotation of M4O (M=Cu,Ag) tetrahedra about the aaaaa axis.
Some references
1. R. Mittal, S.L. Chaplot, S.K. Mishra, Preyoshi P. Bose, Phys. Rev. B75 (2007) 174303.2. A. Sen, Mala N. Rao, R. Mittal, and S.L. Chaplot, J. Phys.: Condens. Matter, 17 (2005) 6179.3. R. Mukhopadhyay, A. Sayeed, Mala N. Rao, A.V. Anilkumar, S. Mitra, S. Yashonath, S.L. Chaplot, Chem.Phys.
292 (2003) 217.4. R. Mittal, S.L. Chaplot, A. Sen, S.N. Achary, A.K. Tyagi, Phys. Rev. B 67 (2003) 134303.5. P. Goel, Mala N. Rao, N. Choudhury, S.L. Chaplot, Subrata Ghose, M. Yethiraj, Appl. Phys. A 74 [Suppl.]
S1149 (2002).
28 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole no. TT1004
Monochromator (2 nos. in tandem)crystals (2nd one vertically focused): PG(0002) (100 × 80 mm2)
λincident 1.3 – 4.7Å
Scattering angle 2θ< 80O
Flux at sample 5 ×105 n/cm2/sec
Analyser PG(0002)(MARX Mode)
ΔE range 2.3 meV(for Ei=4 meV)
ΔE/E 4 %
QuasiElastic Neutron
Scatteringinstrument
This instrument is used to studyStochastic Motion (like Diffusion) inCondensed Matter. ‘Quasi’ means nearelastic (≤ 2 meV). Provides informationabout the time scale and geometry ofdiffusive motion as also the potentialexperienced by the species.
Some distinct features of thisinstrument are mentioned below:
• Virtue of Double Monochromator,neutrons of different incident
energy can be obtained at a fixedsample position
• The instrument works in Multi
angle Reflecting X-tal mode (MARX)thereby facilitating complete energy
spectrum for one instrumentalconfiguration.
• Provision to change in the distance
between different axes to obtaindifferent energy resolutions.
• The out-of-pile portion of the
instrument is on a ‘tanzboden’facilitating easy maneuvering
R. Mukhopadhyay et al. , Nucl. Instr. Meth. A 474 474 474 474 474, 55 (2001).S. Mitra and R. Mukhopadhyay, Current Science 8484848484, 653 (2003)
29Bhabha Atomic Research Centre, Mumbai, India
Selected examples. Alkyl Chain Dynamics in Monolayer Protected Metal nano-Clusters (MPCs)
Schematic of MPCs system
A) Isolated MPCs (Au-clusters): Chains are dynamic only above Tc (340 K: chain melting) and all the chains are dynamic.B) Superlattice MPC (Ag-clusters): Only chains (50 %) are dynamic < Tc (393 K: Superlattice melting) Others held due to
interdigitation . T> Tc all the chains dynamics.
. Diffusion of Molecular absorbed in Zeolite
MD Simulation results show translational motion exists in three differenttime scales. Only one contributes to QENS-data (Red circle). Rotational motion
is much faster and measurable in Triple axis spectrometer with a wider energywindow.
Rotational Diffusion coefficient
of propane in Na-Y zeolite
Some references
1. T. Pradeep, S. Mitra, A. Sreekumaran Nair, R. Mukhopadhyay, J. Phys. Chem. B 108108108108108, 7012 (2004).2. A. Sayeed, S. Mitra, A. V. Anil Kumar, R. Mukhopadhyay, S. Yashonath, S. L. Chaplot, J. Phys. Chem. B 107107107107107,
527 (2003).3. R. Mukhopadhyay, A. Sayeed, S. Mitra, A. V. Anil Kumar, Mala N. Rao, S. L. Chaplot, S. Yashonath Phys.
Rev. E 6666666666, 061201 (2002).4. Siddharth Gautam, S. Mitra, R..Mukhopadhyay, S. L. Chaplot, Phys. Rev. E 7474747474, 041202 (2006).5. S. Mitra, R. Mukhopadhyay, A. K. Tripathi, N. M. Gupta, Applied Physics A 7474747474, S1308 (2002).
30 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole no. HS1017
Monochromator Doubly focusingCu(111)
ΔE range 15 – 250 meV
Q range 1 – 10 Å-1
Incidentwavelength range 0.6 – 2.3 Å
Flux at sample 106 n/cm2/sec
Analyzer Be filter
Scattering angle 10O – 100O
Detector BF3 Counter
FilterDetector
Spectrometer
This instrument is usedto study inelastic neutron scatteringfrom condensed matter.
Principal components of thisinstrument are:
(i) Monochromator that producesthe mono-energetic neutronbeam
(ii) positional spectrometer that setsthe scattering angle.
(iii) Analyzer that measures theoutgoing energy.
Continuous variation of the incidentneutron energy is allowed for by liftingof the shielding wedges of themonochromator shield.
The scattered neutron beam from thesample is filtered by polycrystalline Bemade of beryllium blocks interleavedwith cadmium, intended to capture anyBragg diffracted neutrons. Theneutron scattering cross section of Beexhibits a sharp drop at a neutronenergy of 5 meV. Thus, neutronswhose energy is less than 5 meV areallowed to pass through the filter andall others are scattered out of thebeam.
C.L. Thaper, B.A. Dasannacharya,, and P.K. Iyengar, Nucl. Instr. Meth. 113(1973) 15.
31Bhabha Atomic Research Centre, Mumbai, India
Selected examples. Libration of NH4+ ion in NH4Cl at RT (CsCl Phase)Ammonium chloride NH4Cl is a simple ionic crystal containing distinctNH4
+ tetrahedra. At atmospheric pressure, three phases of ammonium chloridehave been found to exist. Above 243 K (i.e. in the CsCl (disordered) phase), theNH4
+ ions are randomly distributed between two possible orientations,with N-H bonds lying along threefold axes (body diagonals). Ammonium ions inthis room temperature phase may be considered torsional oscillators withfrequency ~ 359 cm-1 (~45 meV). This libration mode exhibits a ratherflat dispersion in the Brillouin zone, with the next branch occurring at least15 meV away.
. Vibration of Hydrogen in Zirconium Hydride (ZrH2)The thermal vibration spectrum ofzirconium hydride includes (in additionto the band of acoustical frequencies)a sharp “optical” frequency νcorresponding approximately tovibrations of the individual hydrogenatoms in an isotropic harmonic well.This implies a set of optical energylevels for the lattice En=nhν. Peakscorresponding to transitions betweenthese optical energy levels will be seenin the spectrum of neutrons scatteredfrom zirconium hydride. The firsttransition is observed as a peak at anenergy transfer of about 140 meV.
The data shown on this page have been taken on an instrument with a PG (0002) monochromator.
32 Bhabha Atomic Research Centre, Mumbai, India
Instrument parameters
Beam hole No. 6 of Apsara,a swimming pool type Reactor
Useful beam size: 15 cm dia.
Thermal NeutronFlux: (n/cm2/sec) 1 x 106
Gamma level: 4R/h
Cadmium ratio: 6.3
Neutron/gammaratio: (n/cm2/mR) 9 x 105
NR Techniques used:converter screens : Gd (25 μm), Dy(100 μm), CCD- based imagingsetup, Neutron Imaging plate
NeutronRadiography
Applications
Non-Destructive Testing andEvaluation of :Nuclear fuel pins,fuel plates,ControlRods, INSAT-pyrovalves & cable cutters,electric detonator, marker shells, boralcomposites
Hydride blisters in zircaloy-2 and Zr-2.5%Nb PT coupons (lab generatedand from power reactor).
Hydrogen Sensitive EpithermalNeutron Radiography
Real time imaging, Two-phase flowstudy, Neutron tomography.
NR Facility At Beam Hole No. 6, Apsara reactor.
Schematic (above) Photograph of the Facility (below).
NR Album : Neutron radiographs of various objectsrecorded using film techniques
(1) INSAT Cable cutters
(2) INSAT Pyro valve(3) Fuel pins
(4) Flower plant through lead brick(1) (2) (3) (4)
←←←←←
33Bhabha Atomic Research Centre, Mumbai, India
Selected examples. Study of zirconium Hydride blister formation in zirconium based PHWR pressuretube materials.
A zirconium hydride blister of nearly 0.35% of job thickness could be detected using neutron radiography.
(1) (2)Hydride blisters in zircaloy-2
(1) and Zr-2.5%Nb(2) PT coupons
(Lab.generated)
Zr-Nb(R) PT coupon from a powerreactor. Enlarged view of the
blister shown at RHS
Neutron radiograph of burst tested Zr-2.5%Nb pressure tube piece containing
laboratory generated hydride blisters(B).The axial crack is seen passing through two
blisters at position 4 on the tube.
. Hydrogen SensitiveEpithermal Neutron(HYSEN) radiographytechnique
. CCD based Electronic imaging
HYSEN radiograph of 1-, 2-, 3-, 4- layers of cellophane adhesive tape as object.Calculated hydrogen sensitivity: 0.1 mg/cm2.
Neutron images of (1) carburetor, (2) spark plug, (3) INSAT cable cutter &
U-tube filled with wax recorded using electronic imaging system.
Some references
1. A.M. Shaikh, P.R. Vaidya, B.K. Shah, S. Gangotra and K.C. Sahoo, J. Non Destr Test. & Eval. 22222(3), 9-12, 2003.2. A.M. Shaikh, Suparna Bannerji and D.N. Sah The e-Journal & Exhibition of nondestructive
Testing-ISSN1435-4934, URL:www.ndt.net/article/nde-india2006/files/tp- 58-pap.pdf3. Amar Sinha, A.M. Shaikh, A. Shyam , Nucl. Instr and Meth. in Phys. Res. B 142142142142142, 425- 431, 1998.
(1) (2) (3)
1 2 3 4 ←←←←←
34 Bhabha Atomic Research Centre, Mumbai, India
A large variety of neutron detectors both BF3 and 3He gas–filled and X-ray detectors with excellent characteristics and long
shelf life are routinely fabricated. They range from
. Small beam monitors (0.2c/nv) to. Large size signal detectors (200c/nv),. Single wire & multiwire 1-D position sensitive detectors (1-D PSDs). A curvilinear multiwire 1-D PSD and. A large area multiwire 2-D PSD.Typical energy resolution of these detectors is 8 % 25 % (FWHM) for BF3 and 5%-15% for
3He-filled detectors.
The detectors developed are of various dimensions, sensitivity and efficiency as per requirements,
Applications: Neutron scattering, flux monitoring, area monitoring and nuclear waste monitoring.
Developmentof NeutronDetectors
Fig.1. Various types of neutron andFig.1. Various types of neutron andFig.1. Various types of neutron andFig.1. Various types of neutron andFig.1. Various types of neutron andXXXXX-ray detectors developed by Solid-ray detectors developed by Solid-ray detectors developed by Solid-ray detectors developed by Solid-ray detectors developed by SolidState Physics DivisionState Physics DivisionState Physics DivisionState Physics DivisionState Physics Division
AAAAA : 2-D Position Sensitive NeutronDetector,
BBBBB : 1-D Position Sensitive NeutronDetectors,
C C C C C : Neutron Proportional Counters,
DDDDD : 1-D Curvilinear Position SensitiveNeutron Detector
EEEEE : 2-D Position Sensitive X-raydetector,
F:F:F:F:F: Microstrip Detector for X-rays andNeutrons,
G G G G G : X-ray Proportional counters,
HHHHH : 1-D Position Sensitive X-rayDetector.
35Bhabha Atomic Research Centre, Mumbai, India
. 3He-filled 1-D position sensitive neutron detector
Fig. 2. Picture of some of the high resolution 1-D PSDs developed.36DHP1 : 3He + Kr (8 + 4 bar), sensitive length 89 cm.
36CHP1 : 3He + iso-C4H10 (8 + 2 bar), sensitive length 89 cm.36CHP2 : 3He + Kr (10 + 4 bar), sensitive length 89 cm.
8E : 3He + Kr (3 + 1.5 bar), Anode: CCQF, sensitive length 17 cmPosition resolution: 4 mm – 7 mm, Efficiency: 60 % to 90 %
Fig.3. Neutron diffraction patterns of Nickel with
36DN2 and 36DHP1 obtained at high-Qdiffractometer at Dhruva (λ=0.783 Å.).
Sensitive area of 345 mm x 345 mm,pixel size: 5mm x 5mm and efficiency
of 70% for 4 Å neutrons has beendeveloped.
Fig. 4. Schematic of 2-D PSD for neutrons. The PSD is shown in photograph
(Fig.1.) as Å
Fig. 5. Position spectrum of 1″ φ directneutron beam (λ ≥ 4Å) (LHS) and thatof scattered beam with alumina sampleplaced in direct beam (RHS). Sample
to detector distance ∼1.5m.
. 3He-filled 2-D multiwire position sensitive neutron detector:
36 Bhabha Atomic Research Centre, Mumbai, India
. 3He-filled 1-D PSD based on microstrip geometry:with anode : 12 μm, cathode:300 μm, pitch : 612 μm and active area of 20 mm x 15 mm is developedand tested for Neutron and X-rays.
Fig. 6. Schematic of designed microstrip pattern on insulating substrate(LHS)
A, anode; C, cathode; B, bonding pad; R,meandering resistive strip Photograph(RHS) of rectangular chamber containing the Microstrip plate (top plate not
shown),
Fig.7. Response of microstrip detector
to 1.5mm wide, , , , , 4Å neutron beam.Position resolution ~ 1.8 mm
. Neutron Detector Development and Testing Facilities:
Fig.8. Facility for Testing 1-D Position Sensitive Neutron Detector at Beam Hole
No. 9, Apsara. Schematic of Neutron Beam Collimator and Detector Shielding,Experimental Setup (left). The BF3-gas generation, purification and fillingBF3-gas generation, purification and fillingBF3-gas generation, purification and fillingBF3-gas generation, purification and fillingBF3-gas generation, purification and filling
stationstationstationstationstation is shown above.
Design of neutron detectors,Assembly of detector components,anode assemblyEvacuation and gas filling systems,Facility for performance Testing ofdetectors with laboratory andreactor sources
Some references
1. S. S. Desai and A.M. Shaikh, Rev. Sci. Instr. 7878787878, 023304 (2007).2. S.S. Desai and A.M. Shaikh, Nucl. Instr. and Meth. in Phy. Res. A 557557557557557,
607 (2006).3. S.S. Desai and A.M. Shaikh, J. of Neutron Research 1414141414, 121 (2006).4. A.M. Shaikh, S.S. Desai and A.K. Patra, Pramana: J. of Phys. 6363636363, 465
(2004).5. V.Radhakrishna, S.S. Desai, A.M. Shaikh and K. Rajanna, Curr. Sci. 8484848484,
1327 (2003).
37Bhabha Atomic Research Centre, Mumbai, India
Sample Environment Facilities
Low Temperature: CCR- 1.5 - 300 K
High Temperature: Furnace: 300-1800 K
High Pressure Apparatus: A piston-cylinder type high-pressure cell with pressure range up to 25 kbar.
Magnetic Field: 12 kOe at Room Temperature
1.5 kOe and 2 kOe in vertical and horizontal direction with CCR
Up to 7 Tesla and T=1.5 to 300 K
38 Bhabha Atomic Research Centre, Mumbai, India
Contact Scientists
39Bhabha Atomic Research Centre, Mumbai, India
For further information about facilities and proposals for experiments contact:
Dr. S.L. Chaplot
Head, Solid State Physics Division
Bhabha Atomic Research Centre, Trombay
Mumbai 400085, India
Telephone: +91 22 25595376, 25593754
Fax: +91 22 25505151, 25519613
E-mail: [email protected]
Published by:
DrDrDrDrDr. Vijai K. Vijai K. Vijai K. Vijai K. Vijai Kumarumarumarumarumar,,,,,
Associate Director, Knowledge Management Group &
Head, Scientific Information Resource Division,
Bhabha Atomic Research Centre,
Trombay, Mumbai 400 085, India
Front PageC o n t e n t sNational Facility for Neutron Beam ResearchNeutrons for Condensed Matter ResearchSingle Crystal Neutron DiffractometerPowder Diffractometer-1Powder Diffractometer-2Powder Diffractometer-3Polarized Neutron SpectrometerHigh - Q DiffractrometerSmall-angle Neutron Scattering DiffractometerDouble Crystal based SANS InstrumentPolarized Neutron ReflectometerSpin Echoand Polarized SANSInstrumentTriple Axis SpectrometerQuasi Elastic NeutronScattering instrumentFilter Detector SpectrometerNeutron RadiographyDevelopmentof Neutron DetectorsSample Environment FacilitiesContact ScientistsFor further information about facilities and proposals for experiments contactBack Page