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P AUL SCHERRER INSTITUT
Technology Transfer R&D Services
Neutron Powder Diffraction
Investigation of crystal structures
Introduction Figure 2: HRPT: Powder
diffractometer.
X-rays vs. Neutrons
For many decades X-ray powder diffraction
(XRD) has been an established and versatile
tool for manifold applications in material
science and engineering. It is well known
as a rapid analytical method, used for both
routine examination and scientific charac-
terization of crystalline materials.
Neutron powder diffraction in terms of
its principles of operation is similar to X-ray
diffraction. Contrary to X-rays, however,
which interact primarily with the electron
cloud surrounding each atom of a given The extracted information is in many Physical properties gained
material, most scattering of neutrons occurs cases unique compared to that obtained
at the atom nuclei, thus providing comple- from conventional X-ray diffraction tech- The most common information typically
mentary information not accessible with niques, because neutrons are sensitive to extracted from a neutron powder diffraction
X-rays. low atomic number materials, such as Hy- experiment includes the symmetry of crys-
The neutron furthermore carries a mag- drogen and Boron, and capable of distin- tal lattices, the dimensions of the unit cells
netic moment, which makes it an excellent guishing between elements with adjacent of the crystal structures and the elemental
probe for the determination of magnetic atomic numbers, such as Iron and Cobalt, composition thereof. Additionally, the frac-
properties of matter. Isotopes of the same element, or element tional coordinates and occupation factors
In the majority of cases, diffraction is groups whose atomic numbers are wide of the atoms within the unit cell are ex-
the main mechanism of the interaction of apart, such as Palladium and Hydrogen tracted with typically very high precision,
the neutron with matter. This is why powder (Deuterium). For these materials systems providing reliable information on the in-
diffraction experiments are perhaps the ,neutron powder diffraction is ideally suited teratomic bond distances, angles and ther-
most straightforward among all neutron to addressing the shortcomings of conven- mal displacements of atoms.
scattering techniques. tional XRD methods.
Finally, microstructure parameters charac-
terizing the grain size distributions and
microstresses in the crystal lattice may also
be determined.
Applications
Figure 1: Structual
determination of Neutron powder diffraction is most widely
orthorhombic RbFeO –
2 used in the fields of crystallography, min-
Rietveld refinement plot eralogy, geochemistry, solid-state physics,
of the HRPT data collected chemistry, material science & engineering
at T=1.5K: both crystal
and magnetic structure and biology. Some materials systems, spe-
refinement. cifically accessible and predestined to be
analyzed with this technique, are high-
lighted below:
• Metallic alloys
• Powdered minerals
• Ceramics
• Isotope-substituted materials
• Low atomic number materials
• Hydrogen storage materials
• Antiferromagnetic and ferromagnetic
materials
Neutron powder diffractometers
at SINQ
Neutron diffraction experiments are carried
out using sophisticated modern instru-
ments located at powerful neutron sources,
such as nuclear reactors or spallation (ac-
celerator-type) sources. Among other large-
scale facilities, PSI operates the Swiss spal- Figure 3: The DMC powder diffractometer is also appropriate for the investigation of magnetic
lation neutron source SINQ1, which phenomena.
encompasses an up-to-date park of neutron
scattering instruments.
Among these, two neutron powder dif- The table below details the key operational Please feel free to ask us for further details.
fractometers, DMC2 3
and HRPT , are high- characteristics of the DMC and HRPT instru-
lighted below: ments. Individual sample environment set-
ups are possible on demand. 1 http://sinq.web.psi.ch/
DMC 2 http://sinq.web.psi.ch/dmc
The high-intensity diffractometer DMC is Properties DMC HRPT 3 http://sinq.web.psi.ch/hrpt
mainly designed for studies of phase tran- Wavelength 2.3–6.0 Å 0.94–2.41 Å 4 https://duo.psi.ch/duo/,
sitions and the detection of weak or fast Scattering range 80° (400 160° (1600 http://sinq.web.psi.ch/sinq/sinq_call.html
processes. DMC provides: channels) channels)
• high intensity for weak scattering Best resolution ≥ 0.006 ≥ 0.0009
materials or small samples ∆d/d
• access to low scattering angles, needed Temperature 110mK–1400 K
for magnetic structure determination range, sample (–273°C…1127°C) Contact
Magnetic field, ≤ 4 T (vertical), ≤ 2 T Dr. Denis Sheptyakov,
HRPT sample (horizontal) Dr. Lukas Keller
3),
Complementary to DMC, the diffractometer Hydrostatic pres- 1.5 GPa (few cm Laboratory for Neutron Scattering,
3
HRPT is designed for high-resolution neu- sure, sample 10 GPa (few 10 mm ) ETHZ & PSI
tron powder diffraction studies with thermal Beam size Up to 5 cm (h) x 1 cm (w)
neutrons. Tel. +41 (0)56 310 30 70
Tel. +41 (0)56 310 40 07
HRPT provides: Example Email: Denis.Sheptyakov@psi.ch
• very high resolution over a large A typical HRPT diffraction pattern and the re- Email: Lukas.Keller@psi.ch
scattering angle range sulting crystal structure are shown in figure 1. Technology Transfer PSI
• high suitability for advanced structural Tel. +41 (0)56 310 27 22
determination Contact us techtransfer@psi.ch
The broad range of research topics investi- Both, the HRPT and DMC diffractometers Paul Scherrer Institute
gated at DMC and HRPT is complemented are open to users from the world-wide sci- 5232 Villigen PSI, Switzerland
by a large collection of sample environ- entific community through the user-access Tel. +41 (0)56 310 21 11
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ments, covering an extremely wide range program , as well as for scientific coopera- www.psi.ch
of pressures and temperatures. tion with industry. NUM-F08-D-10, 9.3.2010
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