{"id":{"repo_id":"soton","oai_identifier":"oai:eprints.soton.ac.uk:173977"},"canonical_url":"https://search.dev.ndltd.org/etd/soton/oai:eprints.soton.ac.uk:173977","repository":{"repo_id":"soton","name":"University of Southampton","base_url":"https://eprints.soton.ac.uk/cgi/oai2"},"display":{"title":"Structural studies of layered transition metal oxides","abstract":"A number of transition metal oxide materials, both new and previously reported, have been
synthesised, their structures based on the n = 2 Ruddlesden-Popper layered perovskites. Their
structures were determined through Rietveld refinement against X-ray and neutron powder
diffraction, supported by vibrating sample magnetometry and thermal analysis.
The structure of the double layered phase Gd2SrCo2O7 was determined in the temperature
range 300 – 973 K by refinement of powder neutron diffraction data. The room temperature
structure is tetragonal, and displays small tilts of the oxygen sublattice that are described by a
2a0 2a0 x c supercell model in the space group P42/mnm rather than the idealised
Sr3Ti2O7 I4/mmm structure as previously reported. A structural transition at ~ 580 K is
characterised by reduction in the unit cell symmetry and distortion of CoO6 octahedra; the
behaviour is concurrent with a spin crossover in the Co (III) ions from intermediate to high
spin.
The structure of the new phase Nd2BaCo2O7 was determined in the temperature range 298 –
873 K by refinement of powder neutron diffraction data. At all temperatures, the structure is
metrically tetragonal, however the octahedral rotations are best described in the orthorhombic
space group Bbcb, with a = b = 2a0.
The structures of the phases Ln2SrFe2O7 (Ln = La, Nd, Gd) have been determined by
refinement of variable temperature powder neutron diffraction data. At room temperature all
the materials crystallise in the tetragonal space group P42/mnm, isostructural with the phase
Tb2BaFe2O7. On heating, the gadolinium and neodymium phases undergo transitions to lower
symmetry; the octahedral tilts of the high temperature phases are best described in the space
group Bbmm.
The new phases Nd2-xSr1+xFe2-xO7 have been prepared and their structures determined by
Rietveld refinement of room temperature powder neutron diffraction. All the materials
crystallise in the tetragonal space group P42/mnm. The degree of octahedral tilting decreases
as x increases, indicating a reduction of compression of the perovskite lattice as the average
A-site cationic radius increases.
The phase Sr3CoNbO7 has been prepared and its structure determined by refinement of
powder neutron diffraction data. At room temperature and 3.4 K there is no evidence of
magnetic ordering, B-site cationic ordering or octahedral tilting. The material is isostructural
with the undistorted Sr3Ti2O7, which implies that the spin state of Co (III) in the material is
low spin.
The material Sr3Ti2O7 was prepared and its structure determined in the temperature range
298 – 1073 K. At all temperatures, the structure is tetragonal, with no rotations of octahedra.
Unit cell parameters and bond lengths expand smoothly over the temperature range.","abstract_html":"A number of transition metal oxide materials, both new and previously reported, have been<br/>synthesised, their structures based on the n = 2 Ruddlesden-Popper layered perovskites. Their<br/>structures were determined through Rietveld refinement against X-ray and neutron powder<br/>diffraction, supported by vibrating sample magnetometry and thermal analysis.<br/><br/>The structure of the double layered phase Gd2SrCo2O7 was determined in the temperature<br/>range 300 – 973 K by refinement of powder neutron diffraction data. The room temperature<br/>structure is tetragonal, and displays small tilts of the oxygen sublattice that are described by a<br/>2a0 2a0 x c supercell model in the space group P42/mnm rather than the idealised<br/>Sr3Ti2O7 I4/mmm structure as previously reported. A structural transition at ~ 580 K is<br/>characterised by reduction in the unit cell symmetry and distortion of CoO6 octahedra; the<br/>behaviour is concurrent with a spin crossover in the Co (III) ions from intermediate to high<br/>spin.<br/><br/>The structure of the new phase Nd2BaCo2O7 was determined in the temperature range 298 –<br/>873 K by refinement of powder neutron diffraction data. At all temperatures, the structure is<br/>metrically tetragonal, however the octahedral rotations are best described in the orthorhombic<br/>space group Bbcb, with a = b = 2a0.<br/><br/>The structures of the phases Ln2SrFe2O7 (Ln = La, Nd, Gd) have been determined by<br/>refinement of variable temperature powder neutron diffraction data. At room temperature all<br/>the materials crystallise in the tetragonal space group P42/mnm, isostructural with the phase<br/>Tb2BaFe2O7. On heating, the gadolinium and neodymium phases undergo transitions to lower<br/>symmetry; the octahedral tilts of the high temperature phases are best described in the space<br/>group Bbmm.<br/><br/>The new phases Nd2-xSr1+xFe2-xO7 have been prepared and their structures determined by<br/>Rietveld refinement of room temperature powder neutron diffraction. All the materials<br/>crystallise in the tetragonal space group P42/mnm. The degree of octahedral tilting decreases<br/>as x increases, indicating a reduction of compression of the perovskite lattice as the average<br/>A-site cationic radius increases.<br/><br/>The phase Sr3CoNbO7 has been prepared and its structure determined by refinement of<br/>powder neutron diffraction data. At room temperature and 3.4 K there is no evidence of<br/>magnetic ordering, B-site cationic ordering or octahedral tilting. The material is isostructural<br/>with the undistorted Sr3Ti2O7, which implies that the spin state of Co (III) in the material is<br/>low spin.<br/><br/>The material Sr3Ti2O7 was prepared and its structure determined in the temperature range<br/>298 – 1073 K. At all temperatures, the structure is tetragonal, with no rotations of octahedra.<br/>Unit cell parameters and bond lengths expand smoothly over the temperature range.","abstract_has_math":false,"creators":["Hickey, Peter James"],"institution":"University of Southampton","degree_name":"Ph.D.","degree_level":"doctoral","degree_discipline":null,"degree_department":null,"school":null,"contributors":[],"advisors":["Weller, Mark T."],"committee_chairs":[],"committee_members":[],"year":2009,"date_issued":"2009-10","date_published":"2009-10","updated_at":"2026-07-24T04:36:21Z","subjects":[],"languages":[],"rights":[],"rights_urls":[],"identifier_entries":[]},"links":{"outbound_url":null,"outbound_label":null,"outbound_source":null},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor.advisor","label":"Advisor","values":["Weller, Mark T."]},{"key":"dc:creator","label":"Author","values":["Hickey, Peter James"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2009-10"]},{"key":"dc:date.issued","label":"Date","values":["2009-10"]},{"key":"dc:publisher.department","label":"Dc Publisher Department","values":["Chemistry (pre 2011 reorg)","School of Chemistry"]},{"key":"dc:publisher.institution","label":"Dc Publisher Institution","values":["University of Southampton"]},{"key":"dc:relation.isreferencedby","label":"Dc Relation Isreferencedby","values":["https://eprints.soton.ac.uk/173977/"]},{"key":"dc:type","label":"Dc Type","values":["Thesis"]},{"key":"dc:type.qualificationlevel","label":"Dc Type Qualificationlevel","values":["doctoral"]},{"key":"dc:type.qualificationname","label":"Dc Type Qualificationname","values":["Ph.D."]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier.uri","label":"Identifier URI","values":["https://eprints.soton.ac.uk/173977/1/HICKEY_2C_Peter.pdf"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description.abstract","label":"Abstract","values":["A number of transition metal oxide materials, both new and previously reported, have been
synthesised, their structures based on the n = 2 Ruddlesden-Popper layered perovskites. Their
structures were determined through Rietveld refinement against X-ray and neutron powder
diffraction, supported by vibrating sample magnetometry and thermal analysis.
The structure of the double layered phase Gd2SrCo2O7 was determined in the temperature
range 300 – 973 K by refinement of powder neutron diffraction data. The room temperature
structure is tetragonal, and displays small tilts of the oxygen sublattice that are described by a
2a0 2a0 x c supercell model in the space group P42/mnm rather than the idealised
Sr3Ti2O7 I4/mmm structure as previously reported. A structural transition at ~ 580 K is
characterised by reduction in the unit cell symmetry and distortion of CoO6 octahedra; the
behaviour is concurrent with a spin crossover in the Co (III) ions from intermediate to high
spin.
The structure of the new phase Nd2BaCo2O7 was determined in the temperature range 298 –
873 K by refinement of powder neutron diffraction data. At all temperatures, the structure is
metrically tetragonal, however the octahedral rotations are best described in the orthorhombic
space group Bbcb, with a = b = 2a0.
The structures of the phases Ln2SrFe2O7 (Ln = La, Nd, Gd) have been determined by
refinement of variable temperature powder neutron diffraction data. At room temperature all
the materials crystallise in the tetragonal space group P42/mnm, isostructural with the phase
Tb2BaFe2O7. On heating, the gadolinium and neodymium phases undergo transitions to lower
symmetry; the octahedral tilts of the high temperature phases are best described in the space
group Bbmm.
The new phases Nd2-xSr1+xFe2-xO7 have been prepared and their structures determined by
Rietveld refinement of room temperature powder neutron diffraction. All the materials
crystallise in the tetragonal space group P42/mnm. The degree of octahedral tilting decreases
as x increases, indicating a reduction of compression of the perovskite lattice as the average
A-site cationic radius increases.
The phase Sr3CoNbO7 has been prepared and its structure determined by refinement of
powder neutron diffraction data. At room temperature and 3.4 K there is no evidence of
magnetic ordering, B-site cationic ordering or octahedral tilting. The material is isostructural
with the undistorted Sr3Ti2O7, which implies that the spin state of Co (III) in the material is
low spin.
The material Sr3Ti2O7 was prepared and its structure determined in the temperature range
298 – 1073 K. At all temperatures, the structure is tetragonal, with no rotations of octahedra.
Unit cell parameters and bond lengths expand smoothly over the temperature range."]},{"key":"dc:format","label":"Dc Format","values":["text"]},{"key":"dc:title","label":"Title","values":["Structural studies of layered transition metal oxides"]}]}],"canonical_facts":{"dc:contributor.advisor":["Weller, Mark T."],"dc:creator":["Hickey, Peter James"],"dc:date":["2009-10"],"dc:date.issued":["2009-10"],"dc:description.abstract":["A number of transition metal oxide materials, both new and previously reported, have been
synthesised, their structures based on the n = 2 Ruddlesden-Popper layered perovskites. Their
structures were determined through Rietveld refinement against X-ray and neutron powder
diffraction, supported by vibrating sample magnetometry and thermal analysis.
The structure of the double layered phase Gd2SrCo2O7 was determined in the temperature
range 300 – 973 K by refinement of powder neutron diffraction data. The room temperature
structure is tetragonal, and displays small tilts of the oxygen sublattice that are described by a
2a0 2a0 x c supercell model in the space group P42/mnm rather than the idealised
Sr3Ti2O7 I4/mmm structure as previously reported. A structural transition at ~ 580 K is
characterised by reduction in the unit cell symmetry and distortion of CoO6 octahedra; the
behaviour is concurrent with a spin crossover in the Co (III) ions from intermediate to high
spin.
The structure of the new phase Nd2BaCo2O7 was determined in the temperature range 298 –
873 K by refinement of powder neutron diffraction data. At all temperatures, the structure is
metrically tetragonal, however the octahedral rotations are best described in the orthorhombic
space group Bbcb, with a = b = 2a0.
The structures of the phases Ln2SrFe2O7 (Ln = La, Nd, Gd) have been determined by
refinement of variable temperature powder neutron diffraction data. At room temperature all
the materials crystallise in the tetragonal space group P42/mnm, isostructural with the phase
Tb2BaFe2O7. On heating, the gadolinium and neodymium phases undergo transitions to lower
symmetry; the octahedral tilts of the high temperature phases are best described in the space
group Bbmm.
The new phases Nd2-xSr1+xFe2-xO7 have been prepared and their structures determined by
Rietveld refinement of room temperature powder neutron diffraction. All the materials
crystallise in the tetragonal space group P42/mnm. The degree of octahedral tilting decreases
as x increases, indicating a reduction of compression of the perovskite lattice as the average
A-site cationic radius increases.
The phase Sr3CoNbO7 has been prepared and its structure determined by refinement of
powder neutron diffraction data. At room temperature and 3.4 K there is no evidence of
magnetic ordering, B-site cationic ordering or octahedral tilting. The material is isostructural
with the undistorted Sr3Ti2O7, which implies that the spin state of Co (III) in the material is
low spin.
The material Sr3Ti2O7 was prepared and its structure determined in the temperature range
298 – 1073 K. At all temperatures, the structure is tetragonal, with no rotations of octahedra.
Unit cell parameters and bond lengths expand smoothly over the temperature range."],"dc:format":["text"],"dc:identifier.uri":["https://eprints.soton.ac.uk/173977/1/HICKEY_2C_Peter.pdf"],"dc:publisher.department":["Chemistry (pre 2011 reorg)","School of Chemistry"],"dc:publisher.institution":["University of Southampton"],"dc:relation.isreferencedby":["https://eprints.soton.ac.uk/173977/"],"dc:title":["Structural studies of layered transition metal oxides"],"dc:type":["Thesis"],"dc:type.qualificationlevel":["doctoral"],"dc:type.qualificationname":["Ph.D."]},"updated_at":"2026-07-24T04:36:21Z"}