{
"id": "fnd:cand2cuti2o9.pbnm.300k.iturbe2012.geometry",
"changelog": [
{
"timestamp": "2026-09-30T05:59:03+00:00",
"user": "perovskite-atlas/fer_export.py",
"description": "Geometry. Generated from atlas records at git 98609f0."
}
],
"description": "Reported geometry of CaNd2CuTi2O9 at 300 K",
"correct": true,
"state": [
{
"name": "temperature",
"description": "conditions of the refined structure",
"quantity_value": {
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#T",
"name": "Temperature",
"description": "Temperature of the measurement as reported (uncertainty not reported)",
"quantities": [
"Temperature"
],
"symbols": [
"$T$"
],
"units": [
"K"
],
"values": [
[
300.0
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"standard_uncertainties": [
[
0.0
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],
"atlas": {
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false
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"reported_as": [
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}
}
}
],
"results": [
{
"id": "fnd:cand2cuti2o9.pbnm.300k.iturbe2012.geometry#angles",
"name": "Bond angles",
"description": "",
"quantities": [
"a/Ln-O1(×1)(Å)",
"a/Ln_-O2(×2)(Å)",
"a/Ln-O2(×2)(Å)",
"a/Ln-O>8short^a(Å)",
"u/Ti-O1_ax(×2)(Å)",
"u/Ti-O2_eq(×2)(Å)",
"u/Ti-O2^′_eq(×2)(Å)",
"u/Ti-O>(Å)",
"O1_ax-Cu/Ti-O2_eq(^°)",
"O1_ax-Cu/Ti-O2^′_eq(^°)",
"O2_eq-Cu/Ti-O2^′_eq(^°)",
"Cu/Ti-O1_ax-Cu/Ti(^°)",
"Cu/Ti-O2_eq-Cu/Ti(^°)"
],
"symbols": [
"$\\angle(a/Ln-O1(×1)(Å))$",
"$\\angle(a/Ln_-O2(×2)(Å))$",
"$\\angle(a/Ln-O2(×2)(Å))$",
"$\\angle(a/Ln-O>8short^a(Å))$",
"$\\angle(u/Ti-O1_ax(×2)(Å))$",
"$\\angle(u/Ti-O2_eq(×2)(Å))$",
"$\\angle(u/Ti-O2^′_eq(×2)(Å))$",
"$\\angle(u/Ti-O>(Å))$",
"$\\angle(O1_ax-Cu/Ti-O2_eq(^°))$",
"$\\angle(O1_ax-Cu/Ti-O2^′_eq(^°))$",
"$\\angle(O2_eq-Cu/Ti-O2^′_eq(^°))$",
"$\\angle(Cu/Ti-O1_ax-Cu/Ti(^°))$",
"$\\angle(Cu/Ti-O2_eq-Cu/Ti(^°))$"
],
"units": [
"°",
"°",
"°",
"°",
"°",
"°",
"°",
"°",
"°",
"°",
"°",
"°",
"°"
],
"values": [
[
3.2
],
[
2.67
],
[
3.37
],
[
2.52
],
[
1.97
],
[
1.99
],
[
2.03
],
[
1.99
],
[
89.2
],
[
90.4
],
[
90.0
],
[
154.1
],
[
152.4
]
],
"standard_uncertainties": [
[
0.02
],
[
0.01
],
[
0.01
],
[
0.02
],
[
0.01
],
[
0.01
],
[
0.01
],
[
0.01
],
[
0.30000000000000004
],
[
0.2
],
[
0.2
],
[
0.5
],
[
0.30000000000000004
]
],
"atlas": {
"uncertainty_reported": [
true,
true,
true,
true,
true,
true,
true,
true,
true,
true,
true,
true,
true
],
"reported_as": [
"3.20(2)",
"2.67(1)",
"3.37(1)",
"2.52(2)",
"1.97(1)",
"1.99(1)",
"2.03(1)",
"1.99(1)",
"89.2(3)",
"90.4(2)",
"90.0(2)",
"154.1(5)",
"152.4(3)"
]
}
}
],
"measurands": [
"bond lengths",
"bond angles",
"bond-valence sums"
],
"source": {
"id": "fnd:cand2cuti2o9.pbnm.300k.iturbe2012.geometry#derivation",
"name": "Geometry derived from the refined structure",
"description": "",
"model": "Interatomic distances, angles and bond-valence sums computed from the refined coordinates and cell (as reported in the source document)",
"influence_quantities": [],
"input_quantities": [
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012",
"changelog": [
{
"timestamp": "2026-09-30T05:59:03+00:00",
"user": "perovskite-atlas/fer_export.py",
"description": "Refined structure. Generated from atlas records at git 98609f0."
}
],
"description": "Refined crystal structure of CaNd2CuTi2O9 at 300 K, Pbnm",
"correct": true,
"state": [
{
"name": "temperature",
"description": "conditions of the refined structure",
"quantity_value": {
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#T",
"name": "Temperature",
"description": "Temperature of the measurement as reported (uncertainty not reported)",
"quantities": [
"Temperature"
],
"symbols": [
"$T$"
],
"units": [
"K"
],
"values": [
[
300.0
]
],
"standard_uncertainties": [
[
0.0
]
],
"atlas": {
"uncertainty_reported": [
false
],
"reported_as": [
"300"
]
}
}
}
],
"results": [
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#cell",
"name": "Unit cell",
"description": "Cell parameters, space group Pbnm (No. 62)",
"quantities": [
"a",
"b",
"c",
"alpha",
"beta",
"gamma"
],
"symbols": [
"$a$",
"$b$",
"$c$",
"$\\alpha$",
"$\\beta$",
"$\\gamma$"
],
"units": [
"Å",
"Å",
"Å",
"°",
"°",
"°"
],
"values": [
[
5.4557
],
[
5.5769
],
[
7.6594
],
[
90.0
],
[
90.0
],
[
90.0
]
],
"standard_uncertainties": [
[
0.0001
],
[
0.0001
],
[
0.0002
],
[
0.0
],
[
0.0
],
[
0.0
]
],
"atlas": {
"uncertainty_reported": [
true,
true,
true,
false,
false,
false
],
"reported_as": [
"5.4557(1)",
"5.5769(1)",
"7.6594(2)",
"90",
"90",
"90"
]
}
},
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#atom:Ca/Nd",
"name": "Atom Ca/Nd (Ca, Wyckoff 4c)",
"description": "Fractional coordinates and isotropic displacement; occupancy 0.35/0.65",
"quantities": [
"x",
"y",
"z",
"B_iso"
],
"symbols": [
"$x$",
"$y$",
"$z$",
"$B_{\\mathrm{iso}}$"
],
"units": [
"1",
"1",
"1",
"Å^2"
],
"values": [
[
-0.0079
],
[
-0.0467
],
[
0.75
],
[
0.7
]
],
"standard_uncertainties": [
[
0.0006000000000000001
],
[
0.0004
],
[
0.0
],
[
0.06
]
],
"atlas": {
"uncertainty_reported": [
true,
true,
false,
true
],
"reported_as": [
"-0.0079(6)",
"-0.0467(4)",
"0.75",
"0.70(6)"
]
}
},
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#atom:Cu/Ti",
"name": "Atom Cu/Ti (Cu, Wyckoff 4b)",
"description": "Fractional coordinates and isotropic displacement; occupancy 0.35/0.65; B_iso fixed",
"quantities": [
"x",
"y",
"z",
"B_iso"
],
"symbols": [
"$x$",
"$y$",
"$z$",
"$B_{\\mathrm{iso}}$"
],
"units": [
"1",
"1",
"1",
"Å^2"
],
"values": [
[
0.5
],
[
0.0
],
[
0.0
],
[
0.5
]
],
"standard_uncertainties": [
[
0.0
],
[
0.0
],
[
0.0
],
[
0.0
]
],
"atlas": {
"uncertainty_reported": [
false,
false,
false,
false
],
"reported_as": [
"0.5",
"0",
"0",
"0.5"
]
}
},
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#atom:O1",
"name": "Atom O1 (O, Wyckoff 4c)",
"description": "Fractional coordinates and isotropic displacement; occupancy 1",
"quantities": [
"x",
"y",
"z",
"B_iso"
],
"symbols": [
"$x$",
"$y$",
"$z$",
"$B_{\\mathrm{iso}}$"
],
"units": [
"1",
"1",
"1",
"Å^2"
],
"values": [
[
0.423
],
[
0.02
],
[
0.75
],
[
1.5
]
],
"standard_uncertainties": [
[
0.003
],
[
0.003
],
[
0.0
],
[
0.30000000000000004
]
],
"atlas": {
"uncertainty_reported": [
true,
true,
false,
true
],
"reported_as": [
"0.423(3)",
"0.020(3)",
"0.75",
"1.5(3)"
]
}
},
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#atom:O2",
"name": "Atom O2 (O, Wyckoff 8d)",
"description": "Fractional coordinates and isotropic displacement; occupancy 1",
"quantities": [
"x",
"y",
"z",
"B_iso"
],
"symbols": [
"$x$",
"$y$",
"$z$",
"$B_{\\mathrm{iso}}$"
],
"units": [
"1",
"1",
"1",
"Å^2"
],
"values": [
[
0.202
],
[
0.79
],
[
0.458
],
[
1.5
]
],
"standard_uncertainties": [
[
0.002
],
[
0.002
],
[
0.002
],
[
0.30000000000000004
]
],
"atlas": {
"uncertainty_reported": [
true,
true,
true,
true
],
"reported_as": [
"0.202(2)",
"0.790(2)",
"0.458(2)",
"1.5(3)"
]
}
},
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#reliability",
"name": "Rietveld reliability factors",
"description": "As reported; no uncertainties",
"quantities": [
"chi2"
],
"symbols": [
"$\\chi^2$"
],
"units": [
"1"
],
"values": [
[
2.12
]
],
"standard_uncertainties": [
[
0.0
]
],
"atlas": {
"uncertainty_reported": [
false
],
"reported_as": [
"2.12"
]
}
}
],
"measurands": [
"unit cell",
"atomic coordinates",
"displacement parameters"
],
"source": {
"id": "ref:cand2cuti2o9.pbnm.300k.iturbe2012.all-modes",
"name": "Rietveld refinement (FullProf, symmetry-mode)",
"description": "",
"model": "Least-squares Rietveld refinement of the powder pattern; symmetry-mode parametrisation where method = symmetry-mode; variant all-modes",
"influence_quantities": [
{
"id": "str:cand2cuti2o9.pbnm.300k.iturbe2012#T",
"name": "Temperature",
"description": "Temperature of the measurement as reported (uncertainty not reported)",
"quantities": [
"Temperature"
],
"symbols": [
"$T$"
],
"units": [
"K"
],
"values": [
[
300.0
]
],
"standard_uncertainties": [
[
0.0
]
],
"atlas": {
"uncertainty_reported": [
false
],
"reported_as": [
"300"
]
}
}
],
"input_quantities": [
{
"id": "dat:cand2cuti2o9.iturbe2012.npd.rt",
"changelog": [
{
"timestamp": "2026-09-30T05:59:03+00:00",
"user": "perovskite-atlas/fer_export.py",
"description": "Dataset stub. Generated from atlas records at git 98609f0."
}
],
"description": "NPD pattern of mat:cand2cuti2o9 at 300 K on D2B high-resolution neutron powder diffractometer (Institut Laue-Langevin, Grenoble)",
"correct": true,
"state": [],
"results": [],
"measurands": [
"diffraction pattern"
],
"source": {
"id": "ins:ill-d2b",
"name": "D2B high-resolution neutron powder diffractometer",
"description": "",
"model": "powder diffraction",
"influence_quantities": [],
"input_quantities": []
},
"atlas": {
"record_id": "dat:cand2cuti2o9.iturbe2012.npd.rt",
"status": "published",
"evidence": [
{
"doc": "doc:thesis-03",
"md_line": 2120,
"table": "10.2",
"status": "thesis-only"
}
],
"atlas_schema_version": "0.1",
"note": "raw pattern not yet attached; results are empty by design until data rescue"
}
}
]
},
"atlas": {
"record_id": "str:cand2cuti2o9.pbnm.300k.iturbe2012",
"status": "published",
"evidence": [
{
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"md_line": 2120,
"table": "10.2",
"status": "thesis-only"
}
],
"atlas_schema_version": "0.1",
"refinement": {
"record_id": "ref:cand2cuti2o9.pbnm.300k.iturbe2012.all-modes",
"status": "published",
"evidence": [
{
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"md_line": 2120,
"table": "10.2",
"status": "thesis-only"
}
],
"atlas_schema_version": "0.1"
}
}
}
]
},
"atlas": {
"record_id": "fnd:cand2cuti2o9.pbnm.300k.iturbe2012.geometry",
"status": "published",
"evidence": [
{
"doc": "doc:thesis-03",
"md_line": 2167,
"table": "10.3",
"status": "thesis-only",
"cell": {
"col": "CaNd2CuTi2O9"
}
}
],
"atlas_schema_version": "0.1"
}
}Temperature · Temperature of the measurement as reported (uncertainty not reported)
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| Temperature | T | 300 | 0 | K | not reported |
Bond angles
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| a/Ln-O1(×1)(Å) | \angle(a/Ln-O1(×1)(Å)) | 3.20 | 0.02 | ° | |
| a/Ln_-O2(×2)(Å) | \angle(a/Ln_-O2(×2)(Å)) | 2.67 | 0.01 | ° | |
| a/Ln-O2(×2)(Å) | \angle(a/Ln-O2(×2)(Å)) | 3.37 | 0.01 | ° | |
| a/Ln-O>8short^a(Å) | \angle(a/Ln-O>8short^a(Å)) | 2.52 | 0.02 | ° | |
| u/Ti-O1_ax(×2)(Å) | \angle(u/Ti-O1_ax(×2)(Å)) | 1.97 | 0.01 | ° | |
| u/Ti-O2_eq(×2)(Å) | \angle(u/Ti-O2_eq(×2)(Å)) | 1.99 | 0.01 | ° | |
| u/Ti-O2^′_eq(×2)(Å) | \angle(u/Ti-O2^′_eq(×2)(Å)) | 2.03 | 0.01 | ° | |
| u/Ti-O>(Å) | \angle(u/Ti-O>(Å)) | 1.99 | 0.01 | ° | |
| O1_ax-Cu/Ti-O2_eq(^°) | \angle(O1_ax-Cu/Ti-O2_eq(^°)) | 89.2 | 0.3 | ° | |
| O1_ax-Cu/Ti-O2′_eq(°) | \angle(O1_ax-Cu/Ti-O2^′_eq(^°)) | 90.4 | 0.2 | ° | |
| O2_eq-Cu/Ti-O2′_eq(°) | \angle(O2_eq-Cu/Ti-O2^′_eq(^°)) | 90.0 | 0.2 | ° | |
| Cu/Ti-O1_ax-Cu/Ti(^°) | \angle(Cu/Ti-O1_ax-Cu/Ti(^°)) | 154.1 | 0.5 | ° | |
| Cu/Ti-O2_eq-Cu/Ti(^°) | \angle(Cu/Ti-O2_eq-Cu/Ti(^°)) | 152.4 | 0.3 | ° |
Geometry derived from the refined structure · model: Interatomic distances, angles and bond-valence sums computed from the refined coordinates and cell (as reported in the source document)
Input quantities
str:cand2cuti2o9.pbnm.300k.iturbe2012 · Refined crystal structure of CaNd2CuTi2O9 at 300 K, Pbnm · own page
Temperature · Temperature of the measurement as reported (uncertainty not reported)
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| Temperature | T | 300 | 0 | K | not reported |
Unit cell · Cell parameters, space group Pbnm (No. 62)
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| a | a | 5.4557 | 0.0001 | Å | |
| b | b | 5.5769 | 0.0001 | Å | |
| c | c | 7.6594 | 0.0002 | Å | |
| alpha | \alpha | 90 | 0 | ° | not reported |
| beta | \beta | 90 | 0 | ° | not reported |
| gamma | \gamma | 90 | 0 | ° | not reported |
Atom Ca/Nd (Ca, Wyckoff 4c) · Fractional coordinates and isotropic displacement; occupancy 0.35/0.65
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| x | x | -0.0079 | 0.0006 | ||
| y | y | -0.0467 | 0.0004 | ||
| z | z | 0.75 | 0 | not reported | |
| B_iso | B_{\mathrm{iso}} | 0.70 | 0.06 | Ų |
Atom Cu/Ti (Cu, Wyckoff 4b) · Fractional coordinates and isotropic displacement; occupancy 0.35/0.65; B_iso fixed
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| x | x | 0.5 | 0 | not reported | |
| y | y | 0 | 0 | not reported | |
| z | z | 0 | 0 | not reported | |
| B_iso | B_{\mathrm{iso}} | 0.5 | 0 | Ų | not reported |
Atom O1 (O, Wyckoff 4c) · Fractional coordinates and isotropic displacement; occupancy 1
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| x | x | 0.423 | 0.003 | ||
| y | y | 0.020 | 0.003 | ||
| z | z | 0.75 | 0 | not reported | |
| B_iso | B_{\mathrm{iso}} | 1.5 | 0.3 | Ų |
Atom O2 (O, Wyckoff 8d) · Fractional coordinates and isotropic displacement; occupancy 1
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| x | x | 0.202 | 0.002 | ||
| y | y | 0.790 | 0.002 | ||
| z | z | 0.458 | 0.002 | ||
| B_iso | B_{\mathrm{iso}} | 1.5 | 0.3 | Ų |
Rietveld reliability factors · As reported; no uncertainties
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| chi2 | \chi^2 | 2.12 | 0 | not reported |
Rietveld refinement (FullProf, symmetry-mode) · model: Least-squares Rietveld refinement of the powder pattern; symmetry-mode parametrisation where method = symmetry-mode; variant all-modes
Influence quantities
Temperature · Temperature of the measurement as reported (uncertainty not reported)
| quantity | symbol | value | u (standard) | unit | |
|---|---|---|---|---|---|
| Temperature | T | 300 | 0 | K | not reported |
Input quantities
dat:cand2cuti2o9.iturbe2012.npd.rt · NPD pattern of mat:cand2cuti2o9 at 300 K on D2B high-resolution neutron powder diffractometer (Institut Laue-Langevin, Grenoble)
Empty (no results attached yet).
D2B high-resolution neutron powder diffractometer · model: powder diffraction
| timestamp | user | description |
|---|---|---|
| 2026-09-30T05:59:03+00:00 | perovskite-atlas/fer_export.py | Dataset stub. Generated from atlas records at git 98609f0. |
| timestamp | user | description |
|---|---|---|
| 2026-09-30T05:59:03+00:00 | perovskite-atlas/fer_export.py | Refined structure. Generated from atlas records at git 98609f0. |
| timestamp | user | description |
|---|---|---|
| 2026-09-30T05:59:03+00:00 | perovskite-atlas/fer_export.py | Geometry. Generated from atlas records at git 98609f0. |
record fnd:cand2cuti2o9.pbnm.300k.iturbe2012.geometry · status published