Literature DB >> 21578033

Synchrotron study of the garnet-type oxide Li(6)CaSm(2)Ta(2)O(12).

Chung-Yul Yoo, Sung-Chul Kim, Seung-Soo Lee, Seung-Joo Kim.   

Abstract

Hexalithium calcium disamarium(III) ditantalum(V) dodeca-oxide, Li(6)CaSm(2)Ta(2)O(12), crystallizes in a cubic garnet-type structure. In the crystal structure, disordered Li atoms occupy two crystallographic sites. One Li has a tetra-hedral coordination environment in the oxide lattice, whereas the other Li atom occupies a significantly distorted octa-hedral site, with site occupancies for the two Li atoms of 0.26 (7) and 0.44 (2), respectively. Ca and Sm atoms are statistically distributed over the same crystallographic position with a occupancy of 2/3 for Sm and of 1/3 for Ca, and are eightfold coordinated by O atoms. The TaO(6) octa-hedron is joined to six others via corner-sharing LiO(4) tetra-hedra. One Li and the O atoms lie on general positions, while the other atoms are situated on special positions. The Sm/Ca position has 222, Ta has , and the tetra-hedrally coordinated Li atom has site symmetry.

Entities:  

Year:  2009        PMID: 21578033      PMCID: PMC2971154          DOI: 10.1107/S1600536809040008

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For a general description of structures and physical properties of garnets, see: Geller (1967 ▶). Recently, high Li-ion conductivity was discovered in garnet-related compounds such as Li5La3 M 2O12 (M = Nb, Ta), see: Thangadurai et al. (2003 ▶); Cussen (2006 ▶). For studies focused on the substitution of La3+ by divalent alkaline earth ions (Ca, Sr, Ba), see: Murugan et al. (2007 ▶); Thangadurai & Weppner (2005a ▶,b ▶); O’Callaghan & Cussen (2007 ▶); Percival & Slater (2007 ▶). For indexing the powder diffraction pattern, see: Boultif & Louër (2004 ▶).

Experimental

Crystal data

Li6CaSm2Ta2O12 M = 936.45 Cubic, a = 12.55128 (7) Å V = 1977.26 (2) Å3 Z = 8 Synchrotron radiation λ = 1.54900 Å T = 298 K Specimen shape: flat sheet 20 × 20 × 0.5 mm Specimen prepared at 103 kPa Specimen prepared at 1223 K Particle morphology: particle, yellowish-white

Data collection

Pohang Light Source 8C2 HRPD Beamline diffractometer Specimen mounting: ’packed powder pellet’ Specimen mounted in reflection mode Scan method: step 2θmin = 10.0, 2θmax = 131.0° Increment in 2θ = 0.01°

Refinement

R p = 15.0 R wp = 22.0 R exp = 13.1 R B = 6.62 S = 1.67 Excluded region(s): None Profile function: pseudo Voigt 151 reflections 20 parameters Preferred orientation correction: none Data collection: local software at 8C2 HRPD beamline; cell refinement: FULLPROF (Rodriguez-Carvajal, 2001 ▶); data reduction: FULLPROF; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: FULLPROF; molecular graphics: DIAMOND (Brandenburg, 1999 ▶); software used to prepare material for publication: FULLPROF. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809040008/wm2261sup1.cif Rietveld powder data: contains datablocks I. DOI: 10.1107/S1600536809040008/wm2261Isup2.rtv Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Li6CaSm2Ta2O12Dx = 6.292 Mg m3
Mr = 936.45Synchrotron radiation, λ = 1.5490 Å
Cubic, Ia3dT = 298 K
Hall symbol: -I 4bd 2c 3Particle morphology: particle
a = 12.55128 (7) Åyellowish-white
V = 1977.26 (2) Å3flat sheet, 20 × 20 mm
Z = 8Specimen preparation: Prepared at 1223 K and 103 kPa, cooled at 5 K/min K min1
F(000) = 3200
Pohang Light Source 8C2 HRPD Beamline diffractometerData collection mode: reflection
Radiation source: SynchrotronScan method: step
Si 111min = 10.00°, 2θmax = 131.00°, 2θstep = 0.01°
Specimen mounting: 'packed powder pellet'
Rp = 15.0Profile function: pseudo Voigt
Rwp = 22.020 parameters
Rexp = 13.10 restraints
RBragg = 6.62(Δ/σ)max < 0.001
χ2 = 2.789Background function: manual background
12100 data pointsPreferred orientation correction: 'None'
Excluded region(s): None
xyzUiso*/UeqOcc. (<1)
Sm10.000000.250000.625000.0089 (2)*0.6666
Ca10.000000.250000.625000.0089 (2)*0.3333
Ta10.000000.000000.500000.0071 (2)*
Li10.125000.000000.750000.0278 (11)*0.26 (7)
Li20.101 (5)0.192 (5)0.412 (5)0.0278 (11)*0.44 (2)
O10.0323 (5)0.0521 (5)0.6488 (6)0.0079 (13)*
(Sm,Ca)—O1i2.441 (18)Li1—O1xiv1.843 (7)
(Sm,Ca)—O1ii2.441 (18)Li2—O1xv1.63 (6)
(Sm,Ca)—O1iii2.441 (18)Li2—O1xi2.14 (6)
(Sm,Ca)—O1iv2.441 (18)Li2—O1i2.12 (6)
(Sm,Ca)—O1v2.561 (17)Li2—O1iii2.20 (6)
(Sm,Ca)—O12.561 (17)Li2—O1xvi2.55 (6)
(Sm,Ca)—O1vi2.561 (17)Li2—O1vii2.69 (6)
(Sm,Ca)—O1vii2.561 (17)Li1—Li2viii1.53 (6)
Ta1—O1viii2.014 (6)Li1—Li2xvii1.53 (6)
Ta1—O12.014 (6)Li1—Li2xviii1.53 (6)
Ta1—O1ix2.014 (6)Li1—Li2xix1.53 (6)
Ta1—O1x2.014 (6)Li1—Li2xx2.33 (6)
Ta1—O1xi2.014 (6)Li1—Li2ix2.33 (6)
Ta1—O1i2.014 (6)Li1—Li2vii2.33 (6)
Li1—O1xii1.843 (7)Li1—Li2xxi2.33 (6)
Li1—O11.843 (7)Li2—Li2xxii2.27 (9)
Li1—O1xiii1.843 (7)Li2—Li2xxiii2.27 (9)
O1i—(Sm,Ca)—O1ii158.8 (8)O1—Ta1—O1x180.000 (1)
O1i—(Sm,Ca)—O1iii72.8 (2)O1ix—Ta1—O1x87.2 (3)
O1ii—(Sm,Ca)—O1iii111.2 (2)O1viii—Ta1—O1xi180.0 (4)
O1i—(Sm,Ca)—O1iv111.2 (2)O1—Ta1—O1xi92.8 (3)
O1ii—(Sm,Ca)—O1iv72.8 (2)O1ix—Ta1—O1xi87.2 (3)
O1iii—(Sm,Ca)—O1iv158.8 (8)O1x—Ta1—O1xi87.2 (3)
O1i—(Sm,Ca)—O1v74.0 (2)O1viii—Ta1—O1i87.2 (3)
O1ii—(Sm,Ca)—O1v124.5 (4)O1—Ta1—O1i87.2 (3)
O1iii—(Sm,Ca)—O1v95.4 (2)O1ix—Ta1—O1i180.000 (2)
O1iv—(Sm,Ca)—O1v67.2 (2)O1x—Ta1—O1i92.8 (3)
O1i—(Sm,Ca)—O167.9 (8)O1xi—Ta1—O1i92.8 (3)
O1ii—(Sm,Ca)—O195.4 (2)O1xii—Li1—O1113.7 (6)
O1iii—(Sm,Ca)—O1124.5 (4)O1xii—Li1—O1xiii101.7 (3)
O1iv—(Sm,Ca)—O174.0 (2)O1—Li1—O1xiii113.7 (6)
O1v—(Sm,Ca)—O1108.13 (16)O1xii—Li1—O1xiv113.7 (6)
O1i—(Sm,Ca)—O1vi124.5 (4)O1—Li1—O1xiv101.7 (3)
O1ii—(Sm,Ca)—O1vi74.0 (2)O1xiii—Li1—O1xiv113.7 (6)
O1iii—(Sm,Ca)—O1vi67.2 (2)O1xv—Li2—O1i110 (3)
O1iv—(Sm,Ca)—O1vi95.4 (2)O1xi—Li2—O1i87 (2)
O1v—(Sm,Ca)—O1vi73.41 (16)O1xv—Li2—O1iii106 (3)
O1—(Sm,Ca)—O1vi167.0 (2)O1xi—Li2—O1iii150 (10)
O1i—(Sm,Ca)—O1vii95.4 (2)O1i—Li2—O1iii83 (2)
O1ii—(Sm,Ca)—O1vii67.2 (2)O1xv—Li2—O1xvi87 (10)
O1iii—(Sm,Ca)—O1vii74.0 (2)O1xi—Li2—O1xvi82 (2)
O1iv—(Sm,Ca)—O1vii124.5 (4)O1i—Li2—O1xvi165 (10)
O1v—(Sm,Ca)—O1vii167.0 (2)O1iii—Li2—O1xvi101 (2)
O1—(Sm,Ca)—O1vii73.41 (16)O1xv—Li2—O1vii148 (10)
O1vi—(Sm,Ca)—O1vii108.13 (16)O1xi—Li2—O1vii78.4 (19)
O1viii—Ta1—O187.2 (3)O1i—Li2—O1vii98 (10)
O1viii—Ta1—O1ix92.8 (3)O1iii—Li2—O1vii74.8 (18)
O1—Ta1—O1ix92.8 (3)O1xvi—Li2—O1vii67 (6)
O1viii—Ta1—O1x92.8 (3)
Table 1

Selected bond lengths (Å)

(Sm,Ca)—O12.561 (17)
Ta1—O12.014 (6)
Li1—O11.843 (7)
Li2—O1i1.63 (6)
Li2—O1ii2.14 (6)
Li2—O1iii2.12 (6)
Li2—O1iv2.20 (6)
Li2—O1v2.55 (6)
Li2—O1vi2.69 (6)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) .

  3 in total

1.  The structure of lithium garnets: cation disorder and clustering in a new family of fast Li+ conductors.

Authors:  Edmund J Cussen
Journal:  Chem Commun (Camb)       Date:  2006-01-28       Impact factor: 6.222

2.  Lithium dimer formation in the Li-conducting garnets Li(5+x)Ba(x)La(3-x)Ta2O12 (0 < x < or =1.6).

Authors:  Michael P O'Callaghan; Edmund J Cussen
Journal:  Chem Commun (Camb)       Date:  2007-05-28       Impact factor: 6.222

3.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

  3 in total

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