Tony Bell | Sheffield Hallam University (original) (raw)
1987 by Tony Bell
J. Chem. Soc. Perkin Trans. I , 1987
""The adducts formed between various aryl-substituted nitrones and aryl isocyanates have been sho... more ""The adducts formed between various aryl-substituted nitrones and aryl isocyanates have been shown,
using 15N n.m.r. spectroscopy and X-ray crystallography, to be substituted 1,2,4-oxadiazolidinones and
not the previously reported 1,3,4-oxadiazolidinones.""
1990 by Tony Bell
Superconductor Science and Technology, Feb 1990
""X-ray powder diffraction patterns have been calculated, from published singlecrystal data, for... more ""X-ray powder diffraction patterns have been calculated, from published
singlecrystal data, for phases encountered in the preparation of yttrium barium
copper oxide ceramics. These patterns have been used to characterise samples
from a small programme of work at NRL-Springfields on novel production
techniques for superconductor materials.""
Acta Crystallographica Section C, 1990
""[YC12(H20)6]C1, Mr = 303"356, monoclinic, P2/n, a = 7.8346 (25), b = 6.4729 (26), c = 9.5817 ... more ""[YC12(H20)6]C1, Mr = 303"356, monoclinic,
P2/n, a = 7.8346 (25), b = 6.4729 (26), c =
9.5817 (50) A, /3 = 93.768 (35) °, V = 484.86 A 3, Z =
2, Dx = 2.0776 g cm -3, Mo Kc~ (A = 0.71069/~),/z =
68.66 cm- 1, F(000) = 300, room temperature, final R
= 0.0449 for 940 unique observed reflexions. The
yttrium is coordinated, as expected, by two chlorines
and six water molecules in a square antiprismatic
arrangement.""
1992 by Tony Bell
Review of Scientific Instruments, Jan 1992
"The two-circle powder diffractometer on Station 8.3 at the SRS has recently been relocated to s... more "The two-circle powder diffractometer on Station 8.3 at the SRS has recently been relocated to
station 2.3, some half the distance from a dipole radiation source with the same nominal
1.2T field. The purpose of this paper is to detail the changes and modifications to the
diffractometer operation."
1994 by Tony Bell
Acta Crystallographica Section C, Oct 1994
""Analyses of high-resolution synchrotron X-ray powder diffraction patterns of dry-synthesized M... more ""Analyses of high-resolution synchrotron X-ray powder
diffraction patterns of dry-synthesized MFemSi206
leucites (M = K, Rb, Cs) showed that the K- and Rbcontaining
leucites (iron potassium silicate, KFeSi206,
and iron rubidium silicate, RbFeSi206) each have a
tetragonal 141/a structure and the Cs-containing leucite
(caesium iron silicate, CsFeSi206) has a cubic la3d
structure. The structures of these materials have been refined
by the Rietveld method. In CsFeSi206 leucite, Fe tu
and Si are disordered on tetrahedral framework sites
as required by space-group constraints. In KFeSi206
leucite, Fe shows significant ordering and is concentrated
on the T3 tetrahedral site. RbFeSi206 leucite
shows less pronounced T-site ordering reflecting the fact
that it is closer to the tetragonal-cubic phase transition
at which the T sites become identical.""
Acta Crystallographica Section C, Jul 1994
""Analysis of a high-resolution synchrotron X-ray powder diffraction pattern of a dry-synthesize... more ""Analysis of a high-resolution synchrotron X-ray powder
diffraction pattern of a dry-synthesized rubidium zinc silicate,
leucite analogue Rb2ZnSi5Ol2, showed that this material
has a cubic la43d structure. The structure of this material
has been refined by the Rietveld method. Si and Zn atoms are disordered on tetrahedral framework sites and
Rb occupies large channel sites along the [ 111] direction.""
Acta Crystallographica Section B, Sep 1994
""A previously unknown leucite-related structure has been determined for synthetic Cs2CdSi5O12. ... more ""A previously unknown leucite-related structure has
been determined for synthetic Cs2CdSi5O12. NMR
spectroscopy shows that there are five distinct tetrahedral
sites (T-sites) occupied by Si and one T-site
occupied by Cd in the framework structure, while
analysis of the synchrotron X-ray powder diffraction
pattern establishes that this material is orthorhombic,
Pbca [RI = 13.1%, R wp = 16.1%, Rex p =
13.1%; eight formula units per unit cell; unit-cell
parameters a= 13.6714(1), b= 13.8240 (1), c=
13.8939 (1) ,~, V = 2625.83 (6) ,~3]. Tetrahedral
cation ordering rates for Si and Cd are sufficiently
high for both hydrothermally and dry-synthesized
samples to be fully ordered. The symmetry relations
between leucites with P2/c and Pbca structures are
discussed and it is shown that such materials are
related by a displacive phase transition, in which the
number of T-sites is reduced from 12 in P2/c to 6 in
Pbca. The 295i MAS NMR data are, at present, less
useful than the X-ray results for providing absolute
T---O distances and T--O--T bond angles.""
Acta Crystallographica Section B, Jan 1994
""The structures of disordered and ordered varieties of the title compound have been determined ... more ""The structures of disordered and ordered varieties of
the title compound have been determined using
integrated TEM, MAS NMR and Rietveld analysis
of synchrotron X-ray powder diffraction data. Both
samples have a 'leucite-like' framework topology.
The dry-synthesized sample is cubic, la3d [a=
13.4190 (1) ,~, V= 2416.33 (5) A 3] with disordered
Mg and Si in tetrahedral framework sites. The
hydrothermally synthesized analogue is monoclinic,
P21/c [a = 13.168 (5), b = 13.652 (1), c =
13.072 (5)/~,/3 = 91.69 °, V = 2348 (2) A3], and has a
fully ordered framework with four K, ten Si and two
Mg sites per 24 O atoms (one quarter of the unit
cell). Two of these Si sites are linked to Si tetrahedra
only [Q4(4Si)], while the other eight Si sites have one
Mg and three Si tetrahedra as next-nearest neighbours
[Q4(3Si, IMg)]. Q4(4Si) and Mg tetrahedra share opposite corners of four rings. Si and Mg
ordering is accompanied by a volume contraction of
2.8%. The X-ray structural data for the ordered
sample allow the 29Si MAS NMR peaks to be
assigned to particular Si tetrahedra, and thus to
particular values of the mean T--O---T angle. The
nature of the polymorphism between the disordered
and ordered samples is discussed and related to the
different synthesis conditions. Water in the hydrothermal
synthesis accelerates Si-Mg ordering, allowing
the thermodynamically more stable phase to be
formed.""
1995 by Tony Bell
J. Phys. Chem. Solids, Oct 1995
"The crystal structure of barium oxalate hydrate, BaC204.2H20, was reinvestigated using a synchr... more "The crystal structure of barium oxalate hydrate, BaC204.2H20, was reinvestigated using a
synchrotron X-ray powder pattern and a single crystal X-ray data set. The compound is monoclinic,
a = 7.538(l), b = 11.062(l), c = 7.105( 1) A, 0 = 105.42(l)“, space group P21/c, with Z = 4. The precision
of the structure arrived at with the synchrotron X-ray powder pattern is not as high as that obtained with the
single crystal X-ray data. The barium atoms are bonded to the. oxalate ions and to the water molecules
with nine barium oxygen- bonds in the range 2.71(l)-2.97(l)A. The structure has hydrogen bonds in
the range 2.72(2)-2,91(2)A, and the oxalate ion has only a minor deviation from planarity."
1996 by Tony Bell
Acta Crystallographica Section C, Sep 1996
Analysis of high-resolution synchrotron X-ray powder diffraction patterns of hydrothermally synth... more Analysis of high-resolution synchrotron X-ray powder diffraction patterns of hydrothermally synthesized Rb2CdSi5O12 and Cs2MnSi5O12 leucite analogues and dry-synthesized Cs2CoSi5O12 and Cs2NiSi5O12 leucite analogues showed that they have an orthorhombic Pbca structure. The structures have been refined by the Rietveld method showing that the tetrahedrally coordinated atoms (Si, Cd, Mn, Co and Ni) are ordered onto separate sites. The Cs2MnSi5O12, Cs2CoSi5O12 and Cs2NiSi5O12 leucite samples are unusual in having SiO4 tetrahedra more distorted, on average, than the larger MnO4, CoO4 and NiO4 tetrahedra. The JCPDS file numbers for Rb2CdSi5O12, Cs2MnSi5O12, Cs2CoSi5O12 and Cs2NiSi5O12 are 46-1491, 46-1492, 46-1493, respectively.
1998 by Tony Bell
Nature, Dec 17, 1998
"Charge-ordering is an important phenomenon in conducting metal oxides: it leads to metal-insula... more "Charge-ordering is an important phenomenon in conducting
metal oxides: it leads to metal-insulator transitions in manganite
perovskites (which show `colossal' magnetoresistances), and the
Verwey transition in magnetite (in which the material becomes
insulating at low temperatures when the conduction electrons
freeze into a regular array). Charge-ordered `stripes' are found in
some manganites and copper oxide superconductors; in the
latter case, dynamic fluctuations of the stripes have been
proposed as a mechanism of high-temperature superconductivity.
But an important unresolved issue is whether the chargeordering
in oxides is driven by electrostatic repulsions between
the charges (Wigner crystallization), or by the strains arising
from electron-lattice interactions (such as Jahn-Teller distortions)
involving different localized electronic states. Here we
report measurements on iron oxoborate, Fe2OBO3, that support
the electrostatic repulsion charge-ordering mechanism: the
system adopts a charge-ordered state below 317 K, in which Fe2+
and Fe3+ ions are equally distributed over structurally distinct
Fe sites. In contrast, the isostructural manganese oxoborate,
Mn2OBO3, has been previously shown to undergo charge-ordering
through Jahn-Teller distortions. We therefore conclude that
both mechanisms occur within the same structural arrangement."
1999 by Tony Bell
Journal of Materials Chemistry, 1999
"Transition metal oxoborates are of interest for magnetic and optical properties. Crystals of man... more "Transition metal oxoborates are of interest for magnetic and optical properties. Crystals of many MII2MIIIO2BO3
andMIIMIIIOBO3 materials can be grown from borate fluxes. In the FeII–FeIII–B–O system, flux growth results in
Fe3O2BO3 crystals, but solid state reaction at higher temperatures has yielded Fe2OBO3 as a polycrystalline powder.
This has been characterised by synchrotron and neutron diffraction, electron microscopy, Mo¨ssbauer spectroscopy,
and conductivity and magnetic measurements. Two notable transitions occur, a broad semiconductor–
semiconductor change accompanied by a structural transition at 317 K, and L-type ferrimagnetic order below a
Curie temperature of 155 K. An average (Fe2+)0.5(Fe3+)0.5 valence is observed at the two crystallographically
distinct sites in Fe2OBO3, indicating that charge ordering occurs."
New Journal of Chemistry, 1999
The crystal structure of the title compound, C6H2F3CNSSN,containing two independent molecules in ... more The crystal structure of the title compound, C6H2F3CNSSN,containing two independent molecules in the asymmetric unit,was determined from synchrotron powder X-ray diffraction data using a global optimisation model building method and confirmed using rigid-body Rietveld refinement; the asym-metric unit contains two independent molecules linked through intermolecular S-S contacts at 3.25 and 3.30 A.
2000 by Tony Bell
Solid State Sciences, 2000
"Neutron powder diffraction data have been collected from a sample of polycrystalline Fe3O4. High... more "Neutron powder diffraction data have been collected from a sample of polycrystalline Fe3O4. High resolution data
collected at 60 K are fitted using a simple rhombohedral distortion of the cubic unit cell. This model accounts for all of the
peak splittings that occur upon cooling through the Verwey transition temperature (TV). Lower resolution data collected
between 2 and 280 K are fitted using the same model, which gives TV11095 K. These data show a change in the thermal
expansion due to the softening of phonons above TV and a change in crystallite extinction arising from twinning at the
transition."
Physica B, 2000
"Lithium manganate spinels with the formula Li1`xMn2~xO4 undergo lithium%proton ion exchange to g... more "Lithium manganate spinels with the formula Li1`xMn2~xO4 undergo lithium%proton ion exchange to give a defect
k-MnO2 phase which can act as a lithium selective sorbent. The substitution of manganese by other metals, such as Co,
Cr, Ti and Ga allow the structural properties of the spinel lattice to be modi"ed and tailored. This work uses neutron
di!raction, inelastic neutron scattering, XAFS and atomistic calculations to show that in the non-substituted spinel,
inserted protons are present predominantly as hydroxyl groups directed into the vacant 8a site, with an orientation
in#uenced by the presence of manganese vacancies. The in#uence of cation substitution is explained within this
context."
2001 by Tony Bell
Journal of the American Chemical Society, Jul 13, 2001
"It is shown by magnetometry and íSR spectroscopy that short-range magnetic interactions between ... more "It is shown by magnetometry and íSR spectroscopy that short-range magnetic interactions between
the Mn cations in the nonmetallic K2NiF4-like phase La0.8Sr1.2Mn0.6Rh0.4O4 become significant below 200
K. Negative magnetoresistance (F/F(0) 0.5 in 14 T at 108 K) is apparent below this temperature. Neutron
diffraction has shown that an applied magnetic field of 5 T is sufficient to induce saturated (3.38(7)íB per
Mn) long-range ferromagnetic ordering of the atomic moments at 2 K, and that the induced ordering persists
up to a temperature of 50 K in 5 T. Spin glass behavior is observed below 20 K in the absence of an applied
field. The induced magnetic ordering is attributed to the subtle changes in band structure brought about by the
external field, and to the controlling influence of Rh3+ over the relative strength of competing magnetic exchange
interactions."
2002 by Tony Bell
J. Solid State Chemistry, 2002
"The room-temperature crystal structure of the brownmillerite SrCaMnGaO5+d (d ¼ 0:035) has been ... more "The room-temperature crystal structure of the brownmillerite
SrCaMnGaO5+d (d ¼ 0:035) has been refined from neutron
powder diffraction data; space group Ima2, a ¼ 15:7817ð6Þ;
b ¼ 5:4925ð2Þ, c ¼ 5:3196ð2ÞA( . Mn and Ga occupy 99.0(2)% of
the 6- and 4-coordinate sites, respectively. A combination of
magnetometry, neutron diffraction and lSR spectroscopy has
shown that the compound orders magnetically at 180 K, and that
the low-temperature phase has a G-type antiferromagnetic
structure, with an ordered magnetic moment of 3.30(2) lB per
Mn at 2K. Displaced hysteresis loops provide evidence that the
atomic moment has an additional, glassy component. Magnetometry
shows that significant short-range magnetic interactions
persist above 180 K, and lSR that the spin fluctuations are
thermally activated in this temperature region. The compound is
an electrical insulator which at 159K shows an unusually large
magnetoresistance of 85% in 6T, increasing to 90% in
13 T."
2005 by Tony Bell
Electrochemistry Communications, 2005
The focus of this study consists of examining how simultaneous SR-XRD and electrochemical measure... more The focus of this study consists of examining how simultaneous SR-XRD and electrochemical measurements can provide information
on the effectiveness of stabilization and storage treatments of copper artefacts in aqueous solution. The electrochemical cell used here was
designed for in situ, time resolved SR-XRD studies of corrosion and inhibition studies on cultural heritage materials. Key objectives of
the new cell were to monitor corrosion layers on alloys with realistic metallographic structures and to obtain co-incident, time resolved,
electrochemical data such as reduction measurements, oxidation measurements and corrosion potential (Ecorr) measurements. Here we
present some early results from the cell. Firstly, a correlated SR-XRD and corrosion potential (Ecorr) study of the reduction of nantokite
during storage in sodium sesquicarbonate, which shows that the surface chemistry continues to change after Ecorr has stabilized. Secondly,
the use of X-ray data to identify specific changes occurring as a function of potential in the forced reduction of a more complex
system.
2007 by Tony Bell
J. American Ceramic Soc., Dec 2007
"Mixed-oxide prepared Ca0.7Ti0.7La0.3Al0.3O3 (CTLA) ceramics (96% dense), grain size 6–7 lm, wi... more "Mixed-oxide prepared Ca0.7Ti0.7La0.3Al0.3O3 (CTLA) ceramics
(96% dense), grain size 6–7 lm, with dielectric properties (at
4 GHz) of er46, Qf 38 000 GHz, and sf113 ppm/1C,
were studied at 251–13001C using synchrotron X-ray powder
diffraction. At room temperature, CTLA exhibits a distorted
orthorhombic structure, with two tilt systems: a55.40383 (4)
A ˚
, b55.41106 (6) A ˚ , and c57.64114 (7) A ˚ with space group
Pbnm. At 105017251C, there is a transition from orthorhombic
(Pbnm) to tetragonal (I4/mcm), with a simpler tilt arrangement.
The lattice parameters at 11001C were: a55.44285 (4) A ˚ and
c57.68913 (8) A ˚ ."
Z. Krist., 2007
The bacterium Geobacter sulfurreducens can produce nanoparticulate magnetite (Fe3O4) by the redu... more The bacterium Geobacter sulfurreducens can produce nanoparticulate magnetite
(Fe3O4) by the reduction of amorphous Fe(III) oxyhydroxide coupled to the oxidation of
organic matter in the anoxic subsurface as an alternative to oxygen respiration. G. sulfurreducens
can transfer electrons to solid Fe(III)-bearing minerals through either direct contact
between the cell and the mineral surface or by using an electron shuttling compound. Highresolution
synchrotron X-ray powder diffraction has been used to study samples taken at
different stages of this reaction. This shows that an initial amorphous phase first transforms
to goethite (FeO(OH)), before undergoing a further transformation to magnetite. Magnetite is
formed faster in the presence of the electron shuttling compound disodium anthraquinone 2,6
disulphonate.
J. Chem. Soc. Perkin Trans. I , 1987
""The adducts formed between various aryl-substituted nitrones and aryl isocyanates have been sho... more ""The adducts formed between various aryl-substituted nitrones and aryl isocyanates have been shown,
using 15N n.m.r. spectroscopy and X-ray crystallography, to be substituted 1,2,4-oxadiazolidinones and
not the previously reported 1,3,4-oxadiazolidinones.""
Superconductor Science and Technology, Feb 1990
""X-ray powder diffraction patterns have been calculated, from published singlecrystal data, for... more ""X-ray powder diffraction patterns have been calculated, from published
singlecrystal data, for phases encountered in the preparation of yttrium barium
copper oxide ceramics. These patterns have been used to characterise samples
from a small programme of work at NRL-Springfields on novel production
techniques for superconductor materials.""
Acta Crystallographica Section C, 1990
""[YC12(H20)6]C1, Mr = 303"356, monoclinic, P2/n, a = 7.8346 (25), b = 6.4729 (26), c = 9.5817 ... more ""[YC12(H20)6]C1, Mr = 303"356, monoclinic,
P2/n, a = 7.8346 (25), b = 6.4729 (26), c =
9.5817 (50) A, /3 = 93.768 (35) °, V = 484.86 A 3, Z =
2, Dx = 2.0776 g cm -3, Mo Kc~ (A = 0.71069/~),/z =
68.66 cm- 1, F(000) = 300, room temperature, final R
= 0.0449 for 940 unique observed reflexions. The
yttrium is coordinated, as expected, by two chlorines
and six water molecules in a square antiprismatic
arrangement.""
Review of Scientific Instruments, Jan 1992
"The two-circle powder diffractometer on Station 8.3 at the SRS has recently been relocated to s... more "The two-circle powder diffractometer on Station 8.3 at the SRS has recently been relocated to
station 2.3, some half the distance from a dipole radiation source with the same nominal
1.2T field. The purpose of this paper is to detail the changes and modifications to the
diffractometer operation."
Acta Crystallographica Section C, Oct 1994
""Analyses of high-resolution synchrotron X-ray powder diffraction patterns of dry-synthesized M... more ""Analyses of high-resolution synchrotron X-ray powder
diffraction patterns of dry-synthesized MFemSi206
leucites (M = K, Rb, Cs) showed that the K- and Rbcontaining
leucites (iron potassium silicate, KFeSi206,
and iron rubidium silicate, RbFeSi206) each have a
tetragonal 141/a structure and the Cs-containing leucite
(caesium iron silicate, CsFeSi206) has a cubic la3d
structure. The structures of these materials have been refined
by the Rietveld method. In CsFeSi206 leucite, Fe tu
and Si are disordered on tetrahedral framework sites
as required by space-group constraints. In KFeSi206
leucite, Fe shows significant ordering and is concentrated
on the T3 tetrahedral site. RbFeSi206 leucite
shows less pronounced T-site ordering reflecting the fact
that it is closer to the tetragonal-cubic phase transition
at which the T sites become identical.""
Acta Crystallographica Section C, Jul 1994
""Analysis of a high-resolution synchrotron X-ray powder diffraction pattern of a dry-synthesize... more ""Analysis of a high-resolution synchrotron X-ray powder
diffraction pattern of a dry-synthesized rubidium zinc silicate,
leucite analogue Rb2ZnSi5Ol2, showed that this material
has a cubic la43d structure. The structure of this material
has been refined by the Rietveld method. Si and Zn atoms are disordered on tetrahedral framework sites and
Rb occupies large channel sites along the [ 111] direction.""
Acta Crystallographica Section B, Sep 1994
""A previously unknown leucite-related structure has been determined for synthetic Cs2CdSi5O12. ... more ""A previously unknown leucite-related structure has
been determined for synthetic Cs2CdSi5O12. NMR
spectroscopy shows that there are five distinct tetrahedral
sites (T-sites) occupied by Si and one T-site
occupied by Cd in the framework structure, while
analysis of the synchrotron X-ray powder diffraction
pattern establishes that this material is orthorhombic,
Pbca [RI = 13.1%, R wp = 16.1%, Rex p =
13.1%; eight formula units per unit cell; unit-cell
parameters a= 13.6714(1), b= 13.8240 (1), c=
13.8939 (1) ,~, V = 2625.83 (6) ,~3]. Tetrahedral
cation ordering rates for Si and Cd are sufficiently
high for both hydrothermally and dry-synthesized
samples to be fully ordered. The symmetry relations
between leucites with P2/c and Pbca structures are
discussed and it is shown that such materials are
related by a displacive phase transition, in which the
number of T-sites is reduced from 12 in P2/c to 6 in
Pbca. The 295i MAS NMR data are, at present, less
useful than the X-ray results for providing absolute
T---O distances and T--O--T bond angles.""
Acta Crystallographica Section B, Jan 1994
""The structures of disordered and ordered varieties of the title compound have been determined ... more ""The structures of disordered and ordered varieties of
the title compound have been determined using
integrated TEM, MAS NMR and Rietveld analysis
of synchrotron X-ray powder diffraction data. Both
samples have a 'leucite-like' framework topology.
The dry-synthesized sample is cubic, la3d [a=
13.4190 (1) ,~, V= 2416.33 (5) A 3] with disordered
Mg and Si in tetrahedral framework sites. The
hydrothermally synthesized analogue is monoclinic,
P21/c [a = 13.168 (5), b = 13.652 (1), c =
13.072 (5)/~,/3 = 91.69 °, V = 2348 (2) A3], and has a
fully ordered framework with four K, ten Si and two
Mg sites per 24 O atoms (one quarter of the unit
cell). Two of these Si sites are linked to Si tetrahedra
only [Q4(4Si)], while the other eight Si sites have one
Mg and three Si tetrahedra as next-nearest neighbours
[Q4(3Si, IMg)]. Q4(4Si) and Mg tetrahedra share opposite corners of four rings. Si and Mg
ordering is accompanied by a volume contraction of
2.8%. The X-ray structural data for the ordered
sample allow the 29Si MAS NMR peaks to be
assigned to particular Si tetrahedra, and thus to
particular values of the mean T--O---T angle. The
nature of the polymorphism between the disordered
and ordered samples is discussed and related to the
different synthesis conditions. Water in the hydrothermal
synthesis accelerates Si-Mg ordering, allowing
the thermodynamically more stable phase to be
formed.""
J. Phys. Chem. Solids, Oct 1995
"The crystal structure of barium oxalate hydrate, BaC204.2H20, was reinvestigated using a synchr... more "The crystal structure of barium oxalate hydrate, BaC204.2H20, was reinvestigated using a
synchrotron X-ray powder pattern and a single crystal X-ray data set. The compound is monoclinic,
a = 7.538(l), b = 11.062(l), c = 7.105( 1) A, 0 = 105.42(l)“, space group P21/c, with Z = 4. The precision
of the structure arrived at with the synchrotron X-ray powder pattern is not as high as that obtained with the
single crystal X-ray data. The barium atoms are bonded to the. oxalate ions and to the water molecules
with nine barium oxygen- bonds in the range 2.71(l)-2.97(l)A. The structure has hydrogen bonds in
the range 2.72(2)-2,91(2)A, and the oxalate ion has only a minor deviation from planarity."
Acta Crystallographica Section C, Sep 1996
Analysis of high-resolution synchrotron X-ray powder diffraction patterns of hydrothermally synth... more Analysis of high-resolution synchrotron X-ray powder diffraction patterns of hydrothermally synthesized Rb2CdSi5O12 and Cs2MnSi5O12 leucite analogues and dry-synthesized Cs2CoSi5O12 and Cs2NiSi5O12 leucite analogues showed that they have an orthorhombic Pbca structure. The structures have been refined by the Rietveld method showing that the tetrahedrally coordinated atoms (Si, Cd, Mn, Co and Ni) are ordered onto separate sites. The Cs2MnSi5O12, Cs2CoSi5O12 and Cs2NiSi5O12 leucite samples are unusual in having SiO4 tetrahedra more distorted, on average, than the larger MnO4, CoO4 and NiO4 tetrahedra. The JCPDS file numbers for Rb2CdSi5O12, Cs2MnSi5O12, Cs2CoSi5O12 and Cs2NiSi5O12 are 46-1491, 46-1492, 46-1493, respectively.
Nature, Dec 17, 1998
"Charge-ordering is an important phenomenon in conducting metal oxides: it leads to metal-insula... more "Charge-ordering is an important phenomenon in conducting
metal oxides: it leads to metal-insulator transitions in manganite
perovskites (which show `colossal' magnetoresistances), and the
Verwey transition in magnetite (in which the material becomes
insulating at low temperatures when the conduction electrons
freeze into a regular array). Charge-ordered `stripes' are found in
some manganites and copper oxide superconductors; in the
latter case, dynamic fluctuations of the stripes have been
proposed as a mechanism of high-temperature superconductivity.
But an important unresolved issue is whether the chargeordering
in oxides is driven by electrostatic repulsions between
the charges (Wigner crystallization), or by the strains arising
from electron-lattice interactions (such as Jahn-Teller distortions)
involving different localized electronic states. Here we
report measurements on iron oxoborate, Fe2OBO3, that support
the electrostatic repulsion charge-ordering mechanism: the
system adopts a charge-ordered state below 317 K, in which Fe2+
and Fe3+ ions are equally distributed over structurally distinct
Fe sites. In contrast, the isostructural manganese oxoborate,
Mn2OBO3, has been previously shown to undergo charge-ordering
through Jahn-Teller distortions. We therefore conclude that
both mechanisms occur within the same structural arrangement."
Journal of Materials Chemistry, 1999
"Transition metal oxoborates are of interest for magnetic and optical properties. Crystals of man... more "Transition metal oxoborates are of interest for magnetic and optical properties. Crystals of many MII2MIIIO2BO3
andMIIMIIIOBO3 materials can be grown from borate fluxes. In the FeII–FeIII–B–O system, flux growth results in
Fe3O2BO3 crystals, but solid state reaction at higher temperatures has yielded Fe2OBO3 as a polycrystalline powder.
This has been characterised by synchrotron and neutron diffraction, electron microscopy, Mo¨ssbauer spectroscopy,
and conductivity and magnetic measurements. Two notable transitions occur, a broad semiconductor–
semiconductor change accompanied by a structural transition at 317 K, and L-type ferrimagnetic order below a
Curie temperature of 155 K. An average (Fe2+)0.5(Fe3+)0.5 valence is observed at the two crystallographically
distinct sites in Fe2OBO3, indicating that charge ordering occurs."
New Journal of Chemistry, 1999
The crystal structure of the title compound, C6H2F3CNSSN,containing two independent molecules in ... more The crystal structure of the title compound, C6H2F3CNSSN,containing two independent molecules in the asymmetric unit,was determined from synchrotron powder X-ray diffraction data using a global optimisation model building method and confirmed using rigid-body Rietveld refinement; the asym-metric unit contains two independent molecules linked through intermolecular S-S contacts at 3.25 and 3.30 A.
Solid State Sciences, 2000
"Neutron powder diffraction data have been collected from a sample of polycrystalline Fe3O4. High... more "Neutron powder diffraction data have been collected from a sample of polycrystalline Fe3O4. High resolution data
collected at 60 K are fitted using a simple rhombohedral distortion of the cubic unit cell. This model accounts for all of the
peak splittings that occur upon cooling through the Verwey transition temperature (TV). Lower resolution data collected
between 2 and 280 K are fitted using the same model, which gives TV11095 K. These data show a change in the thermal
expansion due to the softening of phonons above TV and a change in crystallite extinction arising from twinning at the
transition."
Physica B, 2000
"Lithium manganate spinels with the formula Li1`xMn2~xO4 undergo lithium%proton ion exchange to g... more "Lithium manganate spinels with the formula Li1`xMn2~xO4 undergo lithium%proton ion exchange to give a defect
k-MnO2 phase which can act as a lithium selective sorbent. The substitution of manganese by other metals, such as Co,
Cr, Ti and Ga allow the structural properties of the spinel lattice to be modi"ed and tailored. This work uses neutron
di!raction, inelastic neutron scattering, XAFS and atomistic calculations to show that in the non-substituted spinel,
inserted protons are present predominantly as hydroxyl groups directed into the vacant 8a site, with an orientation
in#uenced by the presence of manganese vacancies. The in#uence of cation substitution is explained within this
context."
Journal of the American Chemical Society, Jul 13, 2001
"It is shown by magnetometry and íSR spectroscopy that short-range magnetic interactions between ... more "It is shown by magnetometry and íSR spectroscopy that short-range magnetic interactions between
the Mn cations in the nonmetallic K2NiF4-like phase La0.8Sr1.2Mn0.6Rh0.4O4 become significant below 200
K. Negative magnetoresistance (F/F(0) 0.5 in 14 T at 108 K) is apparent below this temperature. Neutron
diffraction has shown that an applied magnetic field of 5 T is sufficient to induce saturated (3.38(7)íB per
Mn) long-range ferromagnetic ordering of the atomic moments at 2 K, and that the induced ordering persists
up to a temperature of 50 K in 5 T. Spin glass behavior is observed below 20 K in the absence of an applied
field. The induced magnetic ordering is attributed to the subtle changes in band structure brought about by the
external field, and to the controlling influence of Rh3+ over the relative strength of competing magnetic exchange
interactions."
J. Solid State Chemistry, 2002
"The room-temperature crystal structure of the brownmillerite SrCaMnGaO5+d (d ¼ 0:035) has been ... more "The room-temperature crystal structure of the brownmillerite
SrCaMnGaO5+d (d ¼ 0:035) has been refined from neutron
powder diffraction data; space group Ima2, a ¼ 15:7817ð6Þ;
b ¼ 5:4925ð2Þ, c ¼ 5:3196ð2ÞA( . Mn and Ga occupy 99.0(2)% of
the 6- and 4-coordinate sites, respectively. A combination of
magnetometry, neutron diffraction and lSR spectroscopy has
shown that the compound orders magnetically at 180 K, and that
the low-temperature phase has a G-type antiferromagnetic
structure, with an ordered magnetic moment of 3.30(2) lB per
Mn at 2K. Displaced hysteresis loops provide evidence that the
atomic moment has an additional, glassy component. Magnetometry
shows that significant short-range magnetic interactions
persist above 180 K, and lSR that the spin fluctuations are
thermally activated in this temperature region. The compound is
an electrical insulator which at 159K shows an unusually large
magnetoresistance of 85% in 6T, increasing to 90% in
13 T."
Electrochemistry Communications, 2005
The focus of this study consists of examining how simultaneous SR-XRD and electrochemical measure... more The focus of this study consists of examining how simultaneous SR-XRD and electrochemical measurements can provide information
on the effectiveness of stabilization and storage treatments of copper artefacts in aqueous solution. The electrochemical cell used here was
designed for in situ, time resolved SR-XRD studies of corrosion and inhibition studies on cultural heritage materials. Key objectives of
the new cell were to monitor corrosion layers on alloys with realistic metallographic structures and to obtain co-incident, time resolved,
electrochemical data such as reduction measurements, oxidation measurements and corrosion potential (Ecorr) measurements. Here we
present some early results from the cell. Firstly, a correlated SR-XRD and corrosion potential (Ecorr) study of the reduction of nantokite
during storage in sodium sesquicarbonate, which shows that the surface chemistry continues to change after Ecorr has stabilized. Secondly,
the use of X-ray data to identify specific changes occurring as a function of potential in the forced reduction of a more complex
system.
J. American Ceramic Soc., Dec 2007
"Mixed-oxide prepared Ca0.7Ti0.7La0.3Al0.3O3 (CTLA) ceramics (96% dense), grain size 6–7 lm, wi... more "Mixed-oxide prepared Ca0.7Ti0.7La0.3Al0.3O3 (CTLA) ceramics
(96% dense), grain size 6–7 lm, with dielectric properties (at
4 GHz) of er46, Qf 38 000 GHz, and sf113 ppm/1C,
were studied at 251–13001C using synchrotron X-ray powder
diffraction. At room temperature, CTLA exhibits a distorted
orthorhombic structure, with two tilt systems: a55.40383 (4)
A ˚
, b55.41106 (6) A ˚ , and c57.64114 (7) A ˚ with space group
Pbnm. At 105017251C, there is a transition from orthorhombic
(Pbnm) to tetragonal (I4/mcm), with a simpler tilt arrangement.
The lattice parameters at 11001C were: a55.44285 (4) A ˚ and
c57.68913 (8) A ˚ ."
Z. Krist., 2007
The bacterium Geobacter sulfurreducens can produce nanoparticulate magnetite (Fe3O4) by the redu... more The bacterium Geobacter sulfurreducens can produce nanoparticulate magnetite
(Fe3O4) by the reduction of amorphous Fe(III) oxyhydroxide coupled to the oxidation of
organic matter in the anoxic subsurface as an alternative to oxygen respiration. G. sulfurreducens
can transfer electrons to solid Fe(III)-bearing minerals through either direct contact
between the cell and the mineral surface or by using an electron shuttling compound. Highresolution
synchrotron X-ray powder diffraction has been used to study samples taken at
different stages of this reaction. This shows that an initial amorphous phase first transforms
to goethite (FeO(OH)), before undergoing a further transformation to magnetite. Magnetite is
formed faster in the presence of the electron shuttling compound disodium anthraquinone 2,6
disulphonate.
Chemical Geology, 2007
We have examined alkaline sulfidic (0.5–0.003 M Na2S), aqueous solutions of Hg(II)-S complexes (4... more We have examined alkaline sulfidic (0.5–0.003 M Na2S), aqueous solutions of Hg(II)-S complexes (4–370 ppm Hg(II)) by Hg
LIII edge EXAFS spectroscopy at 296, 348 and 423 K. Data were collected using the ID26 High Brilliance X-ray Spectroscopy
beamline at the ESRF. Analysis of these EXAFS spectra shows Hg coordinated by two S atoms at 2.30 Å; multiple scattering
analyses reveal a linear [–S–Hg–S–] arrangement in the solution complex. These results are in agreement with earlier results on
more concentrated solutions of these complexes. There is also evidence in the data for polynuclear sulfide complexes at 296 K and
348 K for samples with the lowest sulfide concentrations although this is complicated by multiple scattering effects.
Appl. Phys. A, Jan 2008
The phase transformations as a function of the temperature of two natural illitic clays were inv... more The phase transformations as a function of the temperature
of two natural illitic clays were investigated through
XRD measurements, ex situ at room temperature with conventional
set up and in situ with synchrotron radiation, in order to
understand the origin of the corundum phase, which is one of
the main characteristics of the red glaze (slip) of Terra Sigillata
from south Gaul. These clays were chosen on the basis of their
chemical composition and for the quality of vitrification in the
firing temperature range of sigillata (1030–1080 ◦C). Results
show that corundum can be formed above 1000 ◦C if the amount
of Mg is not too high. The corundum formation does not result
directly from the total decomposition of illite (< 900 ◦C)
but from the formation and disruption of an intermediate potassium
aluminum silicate phase. On the other hand, if chlorite is
present in the raw clay so that the amount of Mg > 3–4 wt. %,
this intermediate phase is not observed and only a spinel phase
is formed.
Journal of Synchrotron Radiation, Jan 2008
"The design and performance characterization of a new light-weight and compact X-ray scintillati... more "The design and performance characterization of a new light-weight and compact
X-ray scintillation detector is presented. The detectors are intended for use on
the new I11 powder diffraction beamline at the third-generation Diamond
synchrotron facility where X-ray beams of high photon brightness are generated
by insertion devices. The performance characteristics of these detection units
were measured first using a radioactive source (efficiency of detection and
background count rate) and then synchrotron X-rays (peak stability, light yield
linearity and response consistency). Here, the results obtained from these tests
are reported, and the suitability of the design for the Diamond powder beamline
is demonstrated by presenting diffraction data obtained from a silicon powder
standard using a prototype multicrystal analyser stage."
American Mineralogist, 2008
The Fe(III)-reducing bacterium Geobacter sulfurreducens produces nanometer-sized magnetite by tra... more The Fe(III)-reducing bacterium Geobacter sulfurreducens produces nanometer-sized magnetite by transferring electrons from organic matter or hydrogen to ferrihydrite, resulting in the reductive transformation of the ferrihydrite to magnetite, and the generation of ATP for growth. Electron transfer can occur by direct contact between the cell surface and the mineral or via a soluble “electron shuttle,” for example a quinone-containing humic species. The minerals produced at different stages of ferrihydrite reduction during two experiments, one with and one without the humic analog anthraquinone-2, 6-disulphonate (AQDS), were measured using high-resolution synchrotron powder X-ray diffraction. Amorphous 2-line ferrihydrite converts to goethite, then to a mixture of goethite and magnetite, and finally to magnetite. Samples with and without AQDS showed the same general mineralogical trends, and the rate of reaction was faster in the presence of AQDS. In addition, two transient minerals structurally similar to goethite and magnetite were observed to form as intermediates between ferrihydrite and goethite and goethite and magnetite, but only in samples produced in the absence of the electron shuttle. These transient minerals were named proto-goethite and proto-magnetite. Proto-goethite has a shorter c-axis [4.467(20) Å] than crystalline goethite, a function of size (<2 nm) where quantum properties prevail.
Proto-magnetite is identified by long tetrahedral (2.113 Å) and short octahedral (1.943 Å) Fe-O bonds compared to stoichiometric magnetite, possibly indicative of a coordination crossover caused by charge density [Fe(II)] migration to tetrahedral sites. Fe(II) in solution or sorbed to the mineral surface is considered to be the catalyst causing the mineral transformations. The Fe(II) is thought to form predominantly from the reductive dissolution of 2-line ferrihydrite by G. sulfurreducens.
Acta Crystallographica Section E, Sep 2008
The apatite-type compound Ba5(AsO4)3Cl, pentabarium tris[arsenate(V)] chloride, has been synthesi... more The apatite-type compound Ba5(AsO4)3Cl, pentabarium tris[arsenate(V)] chloride, has been synthesized by ion exchange at high temperature from a synthetic sample of mimetite (Pb5(AsO4)3Cl) with BaCO3 as a by-product. The results of the Rietveld refinement, based on high resolution synchrotron X-ray powder diffraction data, show that the title compound crystallizes in the same structure as other halogenoapatites with general formula A5(YO4)3X (A = divalent cation, Y = pentavalent cation, X = Cl, Br) in space group P63/m. The structure consists of isolated tetrahedral AsO43- anions (m symmetry), separated by two crystallographically independent Ba2+ cations that are located on mirror planes and threefold rotation axes, respectively. The Cl- anions are at the 2b sites ( symmetry) and are located in the channels of the structure.
Acta Crystallographica Section B, Sep 2008
"""The crystal structures and phase behaviour of phase II and the metastable phases III0 and III... more """The crystal structures and phase behaviour of phase II and the
metastable phases III0 and III of cyclohexanol, C6H11OH,
have been determined using high-resolution neutron powder,
synchrotron X-ray powder and single-crystal X-ray diffraction
techniques. Cyclohexanol-II is formed by a transition from the
plastic phase I cubic structure at 265 K and crystallizes in a
tetragonal structure, space group P4421c (Z0 = 1), in which the
molecules are arranged in a hydrogen-bonded tetrameric ring
motif. The structures of phases III0 and III are monoclinic,
space groups P21/c (Z0 = 3) and Pc (Z0 = 2), respectively, and
are characterized by the formation of hydrogen-bonded
molecular chains with a threefold-helical and wave-like
nature, respectively. Phase III crystallizes at 195 K from a
sample of phase I that is supercooled to ca 100 K.
Alternatively, phase III may be grown via phase III0, the
latter transforming from supercooled phase I at ca 200 K.
Phase III0 is particularly unstable and is metastable with
respect to both I and II. Its growth is realised only under very
restricted conditions, thus making its characterization especially
challenging. The cyclohexanol molecules adopt a chair
conformation in all three phases with the hydroxyl groups in
an equatorial orientation. No evidence was found indicating
hydroxyl groups adopting an axial orientation, contrary to the
majority of spectroscopic literature on solid-state cyclohexanol;
however, the H atom of the equatorial OH groups is
found to adopt both in-plane and out-of-plane orientations."""
Acta Crystallographica Section B, Aug 2009
The crystal structures of the leucite analogues Cs2MgSi5O12, Cs2ZnSi5O12 and Rb2MgSi5O12 have bee... more The crystal structures of the leucite analogues Cs2MgSi5O12, Cs2ZnSi5O12 and Rb2MgSi5O12 have been determined by synchrotron X-ray powder diffraction using Rietveld refinement in conjunction with 29Si MAS NMR spectroscopy. These leucites are framework structures with distinct tetrahedral sites (T sites) occupied by Si and a divalent cation (either Mg or Zn in these samples); there is also a monovalent extra-framework cation (either Cs or Rb in these samples). The refined crystal structures were based on the Pbca leucite structure of Cs2CdSi5O12, thus a framework with five ordered Si T sites and one ordered Cd T site was used as the starting model for refinement. 29Si MAS NMR shows five distinct Si T sites for Cs2MgSi5O12 and Rb2MgSi5O12, but six Si T sites for Cs2ZnSi5O12. The refined structures for Cs2MgSi5O12 and Rb2MgSi5O12 were determined with complete T-site ordering, but the refined structure for Cs2ZnSi5O12 was determined with partial disorder of Mg and Si over two of the T sites.
Mineralogical Magazine, Jun 2009
The chemical composition of the natural arsenate-apatite mineral johnbaumite [nominally Ca10(AsO4... more The chemical composition of the natural arsenate-apatite mineral johnbaumite [nominally Ca10(AsO4)6(OH)2] and its alteration product hedyphane [Ca4Pb6(AsO4)6Cl2] have been determined by electron microprobe analysis and the structures of johnbaumite and synthetic Sr-, Ba- and Pb-arsenate apatites have been studied by As K-edge X-ray absorption spectroscopy and synchrotron X-ray powder diffraction. All samples belong to the holosymmetric apatite space group P63/m with As5+ substituted for P5+ in the tetrahedral structural site. Johnbaumite contains small amounts of F and Pb (∼0.9 and ∼4.4 wt.% respectively) and hedyphane has the ideal composition (formula given above); the compositions of these coexisting phases define the two limbs of a solvus occurring between Ca- and Pb-arsenate apatite end members. The unit-cell parameters and cation-oxygen bond lengths for the arsenate apatites studied are discussed alongside published data for end-member Ca-, Sr-, Ba- and Pb-phosphate apatite analogues with (OH), F, Cl or Br as the anions at the centres of the channels in the apatite structure. This discussion rationalizes the relationships between the two structural sites A(1) and A(2) occupied by divalent cations in terms of the size of the A-O polyhedra and the distortion of the A(1)-O polyhedron as measured by the metaprism twist angle [O(1)-A(1)-O(2) projected onto (001)].
Acta Crystallographica Section E, Mar 2009
The apatite-type compound, pentastrontium tris[arsenate(V)] chloride, Sr5(AsO4)3Cl, has been synt... more The apatite-type compound, pentastrontium tris[arsenate(V)] chloride, Sr5(AsO4)3Cl, has been synthesized by ion exchange at high temperature from a synthetic sample of mimetite [Pb5(AsO4)3Cl] with SrCO3 as a by-product. The results of the Rietveld refinement, based on high resolution synchrotron X-ray powder diffraction data, show that the title compound crystallizes in the same structure as other halogenoapatites with general formula A5(YO4)3X (A = divalent cation, Y = pentavalent cation, and X = F, Cl or Br) in the space group P63/m. The structure consists of isolated tetrahedral AsO43- anions (the As atom and two O atoms have m symmetry), separated by two crystallographically independent Sr2+ cations that are located on mirror planes and threefold rotation axes, respectively. One Sr atom is coordinated by nine O atoms and the other by six. The chloride anions (site symmetry ) are at the 2a sites and are located in the channels of the structure.
Acta Crystallographica Section B, Feb 2010
"The crystal structure of a hydrothermally synthesized leucite analogue Cs2CuSi5O12 has been det... more "The crystal structure of a hydrothermally synthesized leucite
analogue Cs2CuSi5O12 has been determined and refined using
the Rietveld method from high-resolution synchrotron X-ray
and neutron powder diffraction data. This structure is based
on the topology and cation-ordering scheme of the Pbca
leucite structure of Cs2CdSi5O12, and exhibits five ordered Si
sites and one ordered Cu tetrahedrally coordinated (T) site.
This structure for Cs2CuSi5O12 is topologically identical to
other known leucite structures and is different from that
originally proposed by Heinrich & Baerlocher [(1991), Acta
Cryst. C47, 237–241] in the tetragonal space group P41212. The
crystal structure of a dry-synthesized leucite analogue
Cs2CuSi5O12 has also been refined; this has the Ia33d cubic
pollucite structure with disordered T sites"
Z. Krist., 2010
"Multi heavy atom cluster compounds like K2PtBr6 offer a way forward to solve, de novo, unknown ... more "Multi heavy atom cluster compounds like
K2PtBr6 offer a way forward to solve, de novo, unknown
protein structures by powder diffraction involving dispersive
(measured at two X-ray wavelengths) and isomorphous
intensity differences as a complement to micro-crystallography
or by using both approaches in combination.
Towards this end, using the ESRF high resolution synchrotron
X-ray powder diffraction beamline ID31, we
have recorded high quality protein powder diffractograms
at the platinum LIII and bromine K absorption edges, as
well as reference wavelengths, for K2PtBr6 bound to lysozyme.
These experiments were conducted at 80K to protect
the sample against X-radiation damage as much as
possible and also to fix the K2PtBr6 bound state, which
seemed to show instability at room temperature. With multiple
powder pattern analysis we extracted intensities and
showed the PtBr6 bound in lysozyme using ‘omit electron
density maps’. In addition the wavelength dispersive Fourier
around the Br K edge shows up the bromine signal at
PtBr6 binding site 1 in one of the six samples tested. To
better understand the chemical properties of this heavy
atom compound we have elucidated the detailed binding
behaviour using single crystal analyses with time-resolved
freeze quenching after soak times of 10, 90 and 170 minutes.
Whilst the quick soaking of 10 to 30 minutes, used
at ESRF ID31 shows clear binding, there is increasing
binding strength with increasing soak time. Thus, these
time-resolved analytical chemistry results show that further
heavy atom signal optimizations are possible. Prospects
for extending our approach to the yet larger isomorphous
and wavelength dispersive signal case of Ta6Br12 bound to
lysozyme are also described."
Mineralogical Magazine, Feb 2010
In situ, high-temperature energy-dispersive X-ray powder diffraction (EDXRD) data have been colle... more In situ, high-temperature energy-dispersive X-ray powder diffraction (EDXRD) data have been collected on synthetic and a natural sample of mercury sulphide (HgS). These measurements were made between temperatures of 295 and 798 K. Synthetic samples of HgS were prepared by reaction between sulphide and mercury in aqueous solution. In a subsequently dried and aged synthetic HgS sample, heated in vacuo, there is a change from a poorly crystalline pseudocubic material into a well crystalline cubic material in the temperature region 583–623 K. At higher temperature (748 K), there is evidence for a partial phase transition to the high temperature hypercinnabar HgS structure. In a neoformed synthetic sample, heated in a sealed Ti container, the initial `pseudocubic' metacinnabar phase partially transforms to a previously unknown phase (XHgS) in the temperature range 467–522 K. This phase disappears at 527 K, and the metacinnabar phase changes to a well crystalline cubic phase; cinnabar develops at 542 K. The proportion of cinnabar continues to increase up to 647 K. Both metacinnabar and cinnabar phases are retained on cooling. No phase transitions were observed for the natural cinnabar sample.
Z. Krist, 2011
Two samples of the spinel ferrite system Cu1-xZnxFe2O4 with x = 0.0 and x = 0.1 were synthesised ... more Two samples of the spinel ferrite system Cu1-xZnxFe2O4 with x = 0.0 and x = 0.1 were synthesised by a combustion method. The effect of zinc ion substitution for copper on low temperature structural properties of CuFe2O4 ferrite is reported. Synchrotron X-ray measurements have been performed in the temperature range 300K – 15K. It was found that for Cu0.9Zn0.1Fe2O4, the sample begins to transform from cubic to tetragonal at about 250K, with the coexistence of both phases down to 15K. No phase transition was observed in the CuFe2O4 spinel below room temperature.
Scripta Materialia, Feb 26, 2011
"The thermodynamics of structural phase transformations in thin films depends on the mechanical s... more "The thermodynamics of structural phase transformations in thin films depends on the mechanical stress that can be released by
plastic deformation. For thin films below a critical film thickness, plastic deformation is energetically unfavourable: thus, the system
stays coherent and stress remains. For PdHc films less than 22 nm thick, a new situation emerges: while the interfaces between matrix
and hydride precipitates remain coherent throughout the complete phase transition, misfit dislocations form between the hydride
phase and the substrate."
Z. Kristallogr., 2011
We have recently revised the ambient temperature crystal structure of the hydro-thermally synthes... more We have recently revised the ambient temperature crystal structure of the hydro-thermally synthesized leucite analogue Cs2CuSi5O12 [1] using high-resolution synchrotron X-ray and neutron powder diffraction. This has the Pbca crystal structure with Si and Cu com-pletely ordered over the tetrahedral T-sites (T1 = Cu, T2-6 = Si). The Cs2CuSi5O12 lattice parameters are: - a = 13.58943(6)Å, b = 13.57355(5)Å and c = 13.62296(4)Å. As a, b and c are so close it was thought that if this sample were to be heated the crystal structure may undergo a phase transition to a higher symmetry space group and/or to a structure with some T-site disorder. High temperature synchrotron X-ray powder diffraction measurements show a significant lattice parameter shift in the temperature range 329-335K. Above this tempera-ture range the crystal structure becomes less distorted but the ordered Pbca structure is re-tained. This “phase transition” is reversible on cooling but takes place in the temperature range 319-317K.
Physical Review B, Oct 10, 2012
"We have studied the magnetic properties and crystal structure of Sr3CoIrO6 and Sr3NiIrO6 as a fu... more "We have studied the magnetic properties and crystal structure of Sr3CoIrO6 and Sr3NiIrO6 as a function of
temperature. Two characteristic temperatures, T1 = 90 K and T2 = 25 K for Sr3CoIrO6, and T1 = 85 K and
T2 = 15 K for Sr3NiIrO6, were observed. Below T1 a significant increase of magnetization and below T2 a weak
temperature dependence of magnetization in the field-cooled and practically zero magnetization values in the
zero-field-cooled mode were detected for both compounds. The existence of Ir4+ in Sr3CoIrO6 was confirmed
by an Ir-LIII x-ray absorption measurement. Magnetoelastic effects have been observed in the temperature
dependence of the lattice parameters of Sr3CoIrO6 and Sr3NiIrO6. The magnetic structure of Sr3CoIrO6 in zero
fields can be described as a commensurate modulated antiferromagnet with a propagation vector k = (0,0,1).
Neutron powder diffraction with polarized neutrons gave evidence of short-range magnetic order, above and
below the magnetic ordering temperature."
Journal of Alloys and Compounds, Jun 15, 2012
""The structural, magnetic and magnetocaloric properties of CoMnGe0.95Ga0.05 have been investigat... more ""The structural, magnetic and magnetocaloric properties of CoMnGe0.95Ga0.05 have been investigated by
using electron microscopy, calorimetric, synchrotron and magnetic measurements. The substitution of
Ga for Ge leads to decreasing on the martensitic transition temperature from 650 K to 315 K. CoMnGe0.95Ga0.05
has hexagonal structure (space group P63/mmc) above the martensitic transition temperature
and orthorhombic structure (space group Pnma) below this temperature. The magnetic field
dependence of magnetization measurements are performed in the heating and cooling processes around
the martensitic transition temperature to determine magnetocaloric effect. It is observed that the magnetic
entropy change associated with the martensitic transition temperature can be as high as
5.2 J kg1 K1 in field of 1 T.""
Mineralogical Magazine, Oct 2012
Synchrotron X-ray powder diffraction data have been collected on three synthetic leucite analogue... more Synchrotron X-ray powder diffraction data have been collected on three synthetic leucite analogues with the general formula Cs2XSi5O12 (X = Cd, Cu, Zn) between 295 and 1173 K. All three samples have the orthorhombic Pbca leucite structure at room temperature with ordered framework T-site cations. The sample with X = Cd retains the Pbca structure over the whole of the investigated temperature range. The sample with X = Cu also retains the Pbca structure, but there is a transition to a less distorted structure with a larger unit-cell volume at ~333 K. The sample with X = Zn shows evidence for a transition to a previously unknown Pa3İ cubic structure, with some T-site cation disorder, at 566 K, on heating. This transition is reversible on cooling to 633 K.
Chemical Physics Letters, Feb 12, 2013
Kinetics of the amorphous–anatase phase transition in single immobilized 5-nm TiO2 nanoparticles ... more Kinetics of the amorphous–anatase phase transition in single immobilized 5-nm TiO2 nanoparticles has
been studied at temperatures between 400 and 1000 C at the DORIS-III synchrotron source of Hasylab.
The measurements indicate the anatase phase appearance at temperatures above 500 C. No formation of
rutile phase was observed. The transformation kinetics for each fixed temperature is rapid and completes
within 5 min. The crystalline mass progressively increases with temperature and the full transformation
into anatase polymorph is achieved above 800 C. The results suggest higher surface energy of the anatase
phase compared to amorphous one, which delays the crystallization process.
Powder Diffraction, Sep 2013
The Sr analogue of the mineral fresnoite (Sr2TiSi2O8) is of interest as a potential storage mediu... more The Sr analogue of the mineral fresnoite (Sr2TiSi2O8) is of interest as a potential storage medium for radioactive Sr from nuclear waste. No high or low temperature crystal structure information is known on this phase. Therefore high-resolution synchrotron X-ray powder diffraction meas-urements have been done on a synthetic sample of Sr-fresnoite in the temperature range 87-1223K. This was done as a test experiment using the HRPD beamline P02.1 at PETRA-III, DESY. Synchrotron X-ray wavelengths of 0.2067(3)Å (293K and 573-1223K) and 0.2079(3)Å (87-499K) were used. Powder diffraction data were collected with a counting time of 30s using a PerkinElmer XRD 1621 flat panel image plate detector. CeO2 was included as an internal stand-ard to calibrate the sample to detector distance. The
P4bm tetragonal crystal structure of fresnoite (Ba2TiSi2O8) was used as a starting model for Sr-fresnoite. Small amounts of SrTiO3
and SrSiO3 were also found as impurities in this sample; therefore four-phase Rietveld refinements were done. The P4bm
fresnoite structure is retained over the temperature range 87-1223K.
Acta Crystallographica Section, Jan 2013
""The fresnoite-type compound Sr2TiO(Si2O7), distrontium oxidotitanium disilicate, has been prep... more ""The fresnoite-type compound Sr2TiO(Si2O7), distrontium
oxidotitanium disilicate, has been prepared by high-temperature
solid-state synthesis. The results of a Rietveld refinement
study, based on high-resolution synchrotron X-ray powder
diffraction data, show that the title compound crystallizes in
the space group P4bm and adopts the structure of other
fresnoite-type mineral samples with general formula
A2TiO(Si2O7) (A = alkaline earth metal cation). The structure
consists of titanosilicate layers composed of corner-sharing
SiO4 tetrahedra (forming Si2O7 disilicate units) and TiO5
square-based pyramids. These layers extend parallel to the ab
plane and are stacked along the c axis. Layers of distorted
SrO6 octahedra lie between the titanosilicate layers. The Sr2+
ion, the SiO4 tetrahedron and the bridging O atom of the
disilicate unit are located on mirror planes whereas the TiO5
square-based pyramid is located on a fourfold rotation axis.""
Solid State Communications
Lattice parameter of metastable high-pressure phase of zinc oxide, rock-salt ZnO, was measured in... more Lattice parameter of metastable high-pressure phase of zinc oxide, rock-salt ZnO, was measured in the
10–300K temperature range using synchrotron X-ray powder diffraction. No phase transition was
observed down to10K.The lattice parameter of rock-salt ZnO was found to increase from 4.266Å in the
10–80 K range up to 4.2752(3)Å at 298K, while the volume thermal expansion coefficient increases from
slight negative values below 40K up to 4.7710-5 K-1 at 298K.
PHYSICAL REVIEW LETTERS, Nov 21, 2014
SmFeO3 has attracted considerable attention very recently due to its reported multiferroic proper... more SmFeO3 has attracted considerable attention very recently due to its reported multiferroic properties
above room temperature. We have performed powder and single crystal neutron diffraction as well as
complementary polarization dependent soft X-ray absorption spectroscopy measurements on floating-zone
grown SmFeO3 single crystals in order to determine its magnetic structure. We found a k ¼ 0 G-type
collinear antiferromagnetic structure that is not compatible with inverse Dzyaloshinskii-Moriya interaction
driven ferroelectricity. While the structural data reveal a clear sign for magneto-elastic coupling at the
Néel-temperature of ∼675 K, the dielectric measurements remain silent as far as ferroelectricity is
concerned.
The Journal of Physical Chemistry C, Jan 9, 2014
A series of isostructural trigonal molybdates CsMZr0.5(MoO4)3 with M = Al, Ga, In, Sc, Cr, V, Fe... more A series of isostructural trigonal molybdates CsMZr0.5(MoO4)3
with M = Al, Ga, In, Sc, Cr, V, Fe, and CsCrTi0.5(MoO4)3 was synthesized by
solid state reactions and characterized by synchrotron powder diffraction,
differential scanning calorimetry, thermal conductivity measurements, and
magnetization measurements for compounds with a magnetic 3d transition
metal cation. The NASICON-type structure of these compounds represents a
three-dimensional framework of corner-sharing trigonal MoO4-pyramids and
MO6-octahedra, in which M and Zr (Ti) ions are randomly distributed. The Cs
ions occupy large channels along the c-axis. A combination of phenomena like
a drastic increase of thermal conductivity, endothermic signals in the DSC
curve and anomalies in the thermal expansion coefficients, observed for the
compounds with M = Cr, V, Fe, and CsCrTi0.5(MoO4)3 above 700 K, allows
one to propose a structural phase transition. The crystal structure of the hightemperature
phase is very close to the low-temperature one. A significant hysteresis in high-temperature electronic and thermal
conductivity was observed. A possible transition from the piezoelectric to the paraelectric state is discussed.
Zeitschrift für Kristallographie, 2010
Mineralogical Magazine, 1997
Sulphosalts in the system CuSbS2-CuBiS2 (chalcostibite-emplectite) form a complete solid solution... more Sulphosalts in the system CuSbS2-CuBiS2 (chalcostibite-emplectite) form a complete solid solution series. Seven compositions with the general formula Cu(Sb x Bi1–x )S2 have been synthesized using dry methods at 310°C. All members of the series are orthorhombic (space group Pnma) and show smoothly increasing a and b cell parameters with substitution of Bi for Sb; the c cell parameter increases up to 50% CuBiS2 substitution and then becomes constant. DSC experiments on CuBiS2 show an endothermic heat effect (2.45 kJ/mol.) at 472°C due to the breakdown reaction to Cu3BiS3 (wittichenite) plus Bi2S3 (bismuthinite). With the addition of 10% CuSbS2 to CuBiS2, the decomposition temperature increases and the endothermic peak is broadened but the energy remains essentially the same (2.53 kJ/mol.). No evidence of this decomposition was observed when the amount of the CuSbS2 component was >30%. The local structure and co-ordination of Cu in the samples were studied by EXAFS analysis of the C...
Journal of Applied Crystallography, 1990
... The powder diffraction pat-tern was analysed by the Rietveld method (Rietveld, 1969) using th... more ... The powder diffraction pat-tern was analysed by the Rietveld method (Rietveld, 1969) using the MPROF program of Murray &amp; Fitch (1990). ... There were 302 Bragg peaks included in the angular range covered by these data. ...
Electrochemistry Communications, 2005
Chemical Physics Letters, 2013
ABSTRACT Kinetics of the amorphous–anatase phase transition in single immobilized 5-nm TiO2 nanop... more ABSTRACT Kinetics of the amorphous–anatase phase transition in single immobilized 5-nm TiO2 nanoparticles has been studied at temperatures between 400 and 1000 °C at the DORIS-III synchrotron source of Hasylab. The measurements indicate the anatase phase appearance at temperatures above 500 °C. No formation of rutile phase was observed. The transformation kinetics for each fixed temperature is rapid and completes within 5 min. The crystalline mass progressively increases with temperature and the full transformation into anatase polymorph is achieved above 800 °C. The results suggest higher surface energy of the anatase phase compared to amorphous one, which delays the crystallization process.
Journal of Materials Chemistry, 1999
European Journal of Chemistry, 2021
The synthetic leucite silicate framework mineral analogues Cs2XSi5O12 (X = Cu, Cd, Zn) were prepa... more The synthetic leucite silicate framework mineral analogues Cs2XSi5O12 (X = Cu, Cd, Zn) were prepared by high-temperature solid-state synthesis. The results of Rietveld refinement, using 18 keV synchrotron X-ray powder diffraction data collected at low temperatures (8K X = Cu, Zn; 10K X = Cd) show that the title compounds crystallize in the space group Pbca and are isostructural with the ambient temperature structures of these analogues. The structures consist of tetrahedrally coordinated SiO4 and XO4 sharing corners to form a partially substituted silicate framework. Extraframework Cs cations sit in channels in the framework. All atoms occupy the 8c general position for this space group. In these refined structures, silicon and X atoms are ordered onto separate tetrahedrally coordinated sites (T-sites).
Journal of physics. Condensed matter : an Institute of Physics journal, Jan 30, 2018
Lanthanide orthoferrites have wide-ranging industrial uses including solar, catalytic and electro... more Lanthanide orthoferrites have wide-ranging industrial uses including solar, catalytic and electronic applications. Here a series of lanthanide orthoferrite perovskites, LnFeO<sub>3</sub> (Ln = La; Nd; Sm; Eu; Gd), prepared through a standard stoichiometric wet ball milling route using oxide precursors, has been studied. Characterisation through X-ray diffraction and X-ray fluorescence confirmed the synthesis of phase-pure or near-pure LnFeO<sub>3</sub> compounds. <sup>57</sub>Fe Mössbauer spectroscopy was performed over a temperature range of 10 K to 293 K to observe hyperfine structure and to enable calculation of the recoil-free fraction and Debye temperature (θD) of each orthoferrite. Debye temperatures (Ln = La 474 K; Nd 459 K; Sm 457 K; Eu 452 K; Gd 473 K) and recoil-free fractions (Ln = La 0.827; Nd 0.817; Sm 0.816; Eu 0.812; Gd 0.826) were approximated through minimising the difference in the temperature dependent experimental Centre Shift ...
Poster Number: CCG06 Synthetic analogues of the silicate framework mineral leucite (KAlSi2O6) wit... more Poster Number: CCG06 Synthetic analogues of the silicate framework mineral leucite (KAlSi2O6) with the stoichiometry Rb2XSi5O12 (X = Mn, Ni) have been prepared by high temperature solid-state synthesis. Ambient temperature X-ray powder diffraction data have been collected on these samples. Analysis of these powder diffraction data show that these samples both consist of single phases [1] isostructural with the Pbca cation-ordered framework leucite structure of Cs2CdSi5O12 [2]. Rietveld refinement [3] shows that for X = Mn this crystal structure has complete Mn and Si cation order over the tetrahredrally coordinated sites (T-sites) in the silicate framework. However, for X = Ni, Rietveld refinement suggests that there may be some Ni and Si cation T-site cation disorder
Acta Chemica Scandinavica, 1995
Acta Crystallographica Section C Crystal Structure Communications, 1996
Analysis of high-resolution synchrotron X-ray powder diffraction patterns of hydrothermally synt... more Analysis of high-resolution synchrotron X-ray powder diffraction patterns of hydrothermally synthesized Rb2CdSi5O12 and Cs2MnSi5O12 leucite analogues and dry-synthesized Cs2CoSi5O12 and Cs2NiSi5O12 leucite analogues showed that they have an orthorhombic Pbca structure. The structures have been refined by the Rietveld method showing that the tetrahedrally coordinated atoms (Si, Cd, Mn, Co and Ni) are ordered onto separate sites. The Cs2MnSi5O12, Cs2CoSi5O12 and Cs2NiSi5O12 leucite samples are unusual in having SiO4 tetrahedra more distorted, on average, than the larger MnO4, CoO4 and NiO4 tetrahedra. The JCPDS file numbers for Rb2CdSi5O12, Cs2MnSi5O12, Cs2CoSi5O12 and Cs2NiSi5O12 are 46–1491, 46–1492, 46–1493, respectively.
Acta crystallographica. Section E, Crystallographic communications, 2016
The synthetic leucite silicate framework mineral analogues Rb2 XSi5O12 {X = Ni [dirubidium nickel... more The synthetic leucite silicate framework mineral analogues Rb2 XSi5O12 {X = Ni [dirubidium nickel(II) penta-silicate] and Mn [dirubidium manganese(II) penta-silicate]} have been prepared by high-temperature solid-state synthesis. The results of Rietveld refinements, using X-ray powder diffraction data collected using Cu Kα X-rays, show that the title compounds crystallize in the space group Pbca and adopt the cation-ordered structure of Cs2CdSi5O12 and other leucites. The structures consist of tetra-hedral SiO4 and XO4 units sharing corners to form a partially substituted silicate framework. Extraframework Rb(+) cations sit in channels in the framework. All atoms occupy the 8c general position for this space group. In these refined structures, silicon and X atoms are ordered onto separate tetra-hedrally coordinated sites (T-sites). However, the Ni displacement parameter and the Ni-O bond lengths suggest that for the X = Ni sample, there may actually be some T-site cation disorder.
Materials Science Forum, 1993
High resoln. synchrotron x-ray powder diffraction, in conjunction with magic angle spinning 29Si ... more High resoln. synchrotron x-ray powder diffraction, in conjunction with magic angle spinning 29Si NMR and electron diffraction, were used to det. structures of synthetic analogs based on the 3 dimensional silicate framework of the natural mineral leucite (KAlSi2O6). These structures were refined by the Rietveld method. The structure detns. of dry and hydrothermal synthesized K2MgSi5O12 analogs illustrate the techniques used, and the structural differences between analogs are discussed in terms of cation sizes and synthetic conditions. [on SciFinder(R)]
Materials Science Forum, 1994
A review, with 26 refs. There are three exptl. stations dedicated to powder diffraction on the UK... more A review, with 26 refs. There are three exptl. stations dedicated to powder diffraction on the UK Synchrotron Radiation Source at the SERC Daresbury Lab. Station 2.3 houses a two-circle angle-dispersive (monochromatic) powder diffractometer, based on the Hart-Parrish design, and is sited on a 1.2 T dipole bending magnet source. This diffractometer can be used to collect data on specimens in the temp. range 10-300K. Station 9.1, which also houses a two-circle angle-dispersive powder diffractometer, is sited on a 5T wiggler magnet source and can be used in high and low resoln. modes. This diffractometer can be used to collect data on specimens in the temp. range 15-1200K and at high pressures. It is also possible to collect data for in situ chem. reaction studies. Station 9.7 houses an energy-dispersive (white beam) diffractometer, and is also sited on a 5T wiggler magnet source. The very high synchrotron radiation flux from the white beam means that it is possible to carry out diffraction expts. on very small samples (e.g. samples under pressure in diamond anvil cells), or to collect time-resolved powder diffraction data (e.g. kinetic studies). Two new stations are currently under construction and will be commissioned during 1994. [on SciFinder(R)]
Journal of the Chemical Society, Perkin Transactions 1, 1987
Page 1. J. CHEM. SOC. PERKIN TRANS. I 1987 2593 Cycloadducts of Nitrones with Isocyanates; 1,2,4-... more Page 1. J. CHEM. SOC. PERKIN TRANS. I 1987 2593 Cycloadducts of Nitrones with Isocyanates; 1,2,4-or 1,3,4-Oxadiazolidinones? Anthony M. T. Bell, Jonathan Bridges, Richard Cross, Christopher P. Falshaw," Brian F. Taylor ...
The Journal of Physical Chemistry C, 2014
ABSTRACT A series of isostructural trigonal molybdates CsMZr0.5(MoO4)3 with M = Al, Ga, In, Sc, C... more ABSTRACT A series of isostructural trigonal molybdates CsMZr0.5(MoO4)3 with M = Al, Ga, In, Sc, Cr, V, Fe, and CsCrTi0.5(MoO4)3 was synthesized by solid state reactions and characterized by synchrotron powder diffraction, differential scanning calorimetry, thermal conductivity measurements, and magnetization measurements for compounds with a magnetic 3d transition metal cation. The NASICON-type structure of these compounds represents a three-dimensional framework of corner-sharing trigonal MoO4-pyramids and MO6-octahedra, in which M and Zr (Ti) ions are randomly distributed. The Cs ions occupy large channels along the c-axis. A combination of phenomena like a drastic increase of thermal conductivity, endothermic signals in the DSC curve and anomalies in the thermal expansion coefficients, observed for the compounds with M = Cr, V, Fe, and CsCrTi0.5(MoO4)3 above 700 K, allows one to propose a structural phase transition. The crystal structure of the hightemperature phase is very close to the low-temperature one. A significant hysteresis in high-temperature electronic and thermal conductivity was observed. A possible transition from the piezoelectric to the paraelectric state is discussed.
The synthetic leucite silicate framework mineral analogues Rb2XSi5O12 {X = Ni [dirubidium nickel(... more The synthetic leucite silicate framework mineral analogues Rb2XSi5O12 {X = Ni
[dirubidium nickel(II) pentasilicate] and Mn [dirubidium manganese(II)
pentasilicate]} have been prepared by high-temperature solid-state synthesis.
The results of Rietveld refinements, using X-ray powder diffraction data
collected using Cu K X-rays, show that the title compounds crystallize in the
space group Pbca and adopt the cation-ordered structure of Cs2CdSi5O12 and
other leucites. The structures consist of tetrahedral SiO4 and XO4 units sharing
corners to form a partially substituted silicate framework. Extraframework Rb+
cations sit in channels in the framework. All atoms occupy the 8c general
position for this space group. In these refined structures, silicon and X atoms are
ordered onto separate tetrahedrally coordinated sites (T-sites). However, the Ni
displacement parameter and the Ni—O bond lengths suggest that for the X = Ni
sample, there may actually be some T-site cation disorder.
X-ray absorption study of 3d transition-metals and Mg in glasses and analogue crystalline materia... more X-ray absorption study of 3d transition-metals and Mg in glasses and analogue crystalline materials in AFe 3 + Si 2 O 6 and A 2 X 2 + Si 5 O 12 , where A = K, Rb, or Cs and X = Mg, Mn, Fe, Co, Ni, Cu, or Zn Crystalline and glassy phases in the 'leucite' systems (K,Rb,Cs)Fe 3+ Si 2 O 6 and (K,Rb,Cs) 2 –(Mg,Mn,Fe,Co,Ni,Cu,Zn) 2+ Si 5 O 12 have been studied using K-edge X-ray Absorption Spectroscopy (XAS) for 3d transition elements and Mg. Crystalline samples of known structure are used as model compounds for deducing the local structures of the equivalent glasses. 'Ideal' tetrahedral framework X 2+ –O distances are: Mn 2+ –O 2.02, Fe 2+ –O 1.98; Co 2+ –O 1.96, Ni 2+ –O 1.95, Cu 2+ –O 1.92, Zn 2+ –O 1.93 and Mg 2+ –O 1.93 Å. The quenched glasses have Extended X-ray Absorption Fine Structure (EXAFS) first-shell distances and coordination numbers consistent with Mg and 3d elements occurring in tetrahedral coordination in most cases. The X-ray Absorption Near Edge Structure (XANES) spectra of the glasses are basically the same as those for the crystalline samples showing that they have similar medium range order, consistent with most of the Mg and 3d elements acting as network formers along with the associated alkalis as X 2 Y 2+ O 2 complexes. Anhydrous glasses in the system CaO–MgO–Al 2 O 3 –SiO 2 together with a basalt glass from Hawaii show examples of Mg in octahedral-(2.07 Å, basalt), tetrahedral-(1.97 Å, siliceous glass) and 5-coordinated (2.01–2.04 Å) sites. Although most Earth scientists assume that Mg and Fe 2+ act as network modifiers in natural magmas, ultra-potassic, peralkaline compositions ((Na + K)/(Al + Fe 3+) N 1) could have had some Fe 2+ and Mg complexes with alkalis in the melt network as K 2 (Mg,Fe 2+)O 2 and the implications of this to melt density and viscosity are considered.
The synthetic leucite silicate framework mineral analogues Rb2XSi5O12 {X = Ni [dirubidium nickel(... more The synthetic leucite silicate framework mineral analogues Rb2XSi5O12 {X = Ni [dirubidium nickel(II) pentasilicate] and Mn [dirubidium manganese(II) pentasilicate]} have been prepared by high-temperature solid-state synthesis. The results of Rietveld refinements, using X-ray powder diffraction data collected using Cu K X-rays, show that the title compounds crystallize in the space group Pbca and adopt the cation-ordered structure of Cs2CdSi5O12 and other leucites. The structures consist of tetrahedral SiO4 and XO4 units sharing corners to form a partially substituted silicate framework. Extraframework Rb+ cations sit in channels in the framework. All atoms occupy the 8c general position for this space group. In these refined structures, silicon and X atoms are ordered onto separate tetrahedrally coordinated sites (T-sites). However, the Ni displacement parameter and the Ni—O bond lengths suggest that for the X = Ni sample, there may actually be some T-site cation disorder.