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In order to clarify the polymorphism in the lithium sulfate family, LiREx(NH4)1 − xSO4 (0.5 ≤ x ≤ 4.0 mol%, nominal value; RE = Er3+, Yb3+ and Dy3+) crystals were grown from aqueous solution by slow evaporation between 298 and 313 K. The doping of the samples allowed us to obtain two polymorphic forms, α and β, of LiNH4SO4 (LAS). By means of X-ray diffraction (XRD) in single crystals, we determined the crystal structures of two new α-polytypes, which we have named α1- and α2-LAS. They present the same space group P21/c and the following relation among their lattice parameters: a2 = −c1, b2 = −b1, c2 = −2a1c1. In order to evaluate the stability of the new α-polytypes, we performed thermal analysis, X-ray diffraction and dielectric spectroscopy on single crystals and polycrystalline samples over the cyclic temperature range: 190 → 575  → 190 K. The results obtained by all the techniques used in this study demonstrate that α-polytypes are stable across a wide range of temperatures and they show an irreversible phase transition to the paraelectric β-phase above 500 K. In addition, a comparative study of α- and β-polytypes shows that both polymorphic structures have a common axis, with a possible intergrowth that facilitates their coexistence and promotes the reconstructive α → β transition. This intergrowth was related to small anomalies detected between 240 and 260 K, in crystals with an α-habit.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520616019028/yb5013sup1.cif
Contains datablocks alpha1_LAS, alpha2_LAS

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616019028/yb5013alpha1_LASsup2.fcf
Contains datablock alpha1_LAS

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616019028/yb5013alpha1_LASsup3.hkl
Contains datablock alpha1_LAS

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616019028/yb5013alpha2_LASsup4.fcf
Contains datablock alpha2_LAS

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616019028/yb5013alpha2_LASsup5.hkl
Contains datablock alpha2_LAS

CCDC references: 1519626; 1530426

Computing details top

For both compounds, program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2014). Molecular graphics: Diamond 4.0 for alpha1_LAS.

(alpha1_LAS) top
Crystal data top
O4SYb0.005·0.984(H4N)·LiF(000) = 497
Mr = 121.54Dx = 1.836 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 17.856 (8) ÅCell parameters from 25 reflections
b = 5.008 (3) Åθ = 9–21°
c = 10.264 (13) ŵ = 0.73 mm1
β = 106.46 (5)°T = 293 K
V = 880.2 (13) Å3Prism, colourless
Z = 80.18 × 0.14 × 0.09 mm
Data collection top
ENRAF-NONIUS CAD4
diffractometer
θmax = 30.0°, θmin = 2.4°
ω/2Θ–scanh = 250
4811 measured reflectionsk = 77
2549 independent reflectionsl = 1314
2020 reflections with I > 2σ(I)3 standard reflections every 120 min
Rint = 0.131 intensity decay: none
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.143Only H-atom coordinates refined
S = 1.17 w = 1/[σ2(Fo2) + (0.0484P)2 + 0.6832P]
where P = (Fo2 + 2Fc2)/3
2549 reflections(Δ/σ)max < 0.001
153 parametersΔρmax = 1.05 e Å3
74 restraintsΔρmin = 0.68 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2sigma(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
S10.40189 (3)0.78809 (13)0.35009 (6)0.01614 (17)
O110.40752 (12)0.7062 (5)0.4897 (2)0.0276 (5)
O120.41093 (12)1.0821 (4)0.3465 (2)0.0309 (5)
O130.32607 (11)0.7155 (5)0.2583 (2)0.0364 (6)
O140.46492 (11)0.6618 (4)0.3038 (2)0.0240 (4)
S20.09813 (3)0.28838 (12)0.44726 (6)0.01509 (16)
O210.09248 (11)0.2049 (5)0.58194 (19)0.0265 (4)
O220.08937 (11)0.5822 (4)0.4341 (2)0.0285 (5)
O230.03490 (10)0.1605 (4)0.33889 (18)0.0220 (4)
O240.17400 (11)0.2124 (5)0.4303 (2)0.0339 (5)
Yb10.33292 (13)0.2738 (5)0.0677 (3)0.0311 (11)0.0051 (12)
N10.33292 (13)0.2738 (5)0.0677 (3)0.0311 (11)0.985 (4)
H110.2772 (6)0.290 (6)0.031 (3)0.047*0.985 (4)
H120.3512 (16)0.137 (5)0.016 (3)0.047*0.985 (4)
H130.3573 (15)0.439 (4)0.055 (3)0.047*0.985 (4)
H140.3461 (17)0.224 (6)0.1612 (13)0.047*0.985 (4)
Yb20.16725 (13)0.7751 (5)0.2335 (3)0.0306 (10)0.0054 (12)
N20.16725 (13)0.7751 (5)0.2335 (3)0.0306 (10)0.984 (4)
H210.2230 (6)0.773 (6)0.255 (3)0.046*0.984 (4)
H220.1446 (16)0.660 (5)0.157 (2)0.046*0.984 (4)
H230.1509 (17)0.713 (6)0.310 (2)0.046*0.984 (4)
H240.1476 (16)0.953 (3)0.209 (3)0.046*0.984 (4)
Li10.0011 (2)0.2967 (10)0.1505 (5)0.0202 (8)
Li20.5016 (2)0.2965 (10)0.3519 (5)0.0226 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0186 (3)0.0195 (3)0.0119 (3)0.0004 (2)0.00700 (19)0.0006 (2)
O110.0352 (9)0.0369 (12)0.0142 (8)0.0014 (8)0.0125 (7)0.0070 (10)
O120.0404 (10)0.0197 (9)0.0394 (13)0.0025 (8)0.0223 (9)0.0033 (10)
O130.0224 (8)0.0535 (15)0.0296 (11)0.0027 (9)0.0015 (7)0.0163 (12)
O140.0313 (8)0.0232 (10)0.0235 (9)0.0072 (7)0.0178 (7)0.0024 (9)
S20.0180 (3)0.0167 (3)0.0109 (3)0.00004 (19)0.00455 (18)0.0003 (2)
O210.0346 (9)0.0341 (11)0.0116 (8)0.0002 (8)0.0076 (7)0.0051 (9)
O220.0368 (10)0.0144 (9)0.0292 (11)0.0016 (7)0.0009 (8)0.0019 (9)
O230.0282 (8)0.0196 (9)0.0152 (8)0.0050 (7)0.0012 (6)0.0003 (8)
O240.0214 (8)0.0491 (14)0.0339 (12)0.0053 (8)0.0122 (8)0.0118 (11)
Yb10.0309 (14)0.0371 (16)0.0259 (15)0.0004 (9)0.0087 (8)0.0005 (11)
N10.0309 (14)0.0371 (16)0.0259 (15)0.0004 (9)0.0087 (8)0.0005 (11)
Yb20.0344 (14)0.0325 (15)0.0266 (15)0.0006 (9)0.0113 (9)0.0024 (11)
N20.0344 (14)0.0325 (15)0.0266 (15)0.0006 (9)0.0113 (9)0.0024 (11)
Li10.0261 (18)0.021 (2)0.0142 (19)0.0014 (16)0.0060 (15)0.0006 (19)
Li20.0269 (19)0.023 (2)0.020 (2)0.0022 (17)0.0094 (16)0.004 (2)
Geometric parameters (Å, º) top
S1—O131.459 (2)Yb1—Li23.551 (6)
S1—O111.466 (3)Yb1—Li2xi3.707 (5)
S1—O141.482 (2)Yb1—Li2i3.858 (5)
S1—O121.483 (2)Yb1—H110.962 (9)
S1—Li23.035 (5)Yb1—H120.976 (9)
S1—Li2i3.049 (5)Yb1—H130.963 (9)
O11—Li2ii1.945 (5)Yb1—H140.954 (9)
O11—Yb1iii2.966 (4)Yb2—O24iv2.958 (4)
O12—Li2iv1.930 (5)Yb2—O21ix2.967 (4)
O12—Yb1iv2.965 (5)Yb2—O22x3.077 (5)
O12—Yb1v3.067 (4)Yb2—Li1vii3.534 (5)
O13—Yb22.791 (3)Yb2—Li13.720 (5)
O13—Yb12.978 (4)Yb2—Li1iv3.863 (5)
O14—Li21.958 (5)Yb2—H210.957 (9)
O14—Li2i1.976 (6)Yb2—H220.968 (9)
S2—O241.464 (2)Yb2—H230.963 (9)
S2—O211.475 (3)Yb2—H240.966 (9)
S2—O221.482 (2)Li1—O22vi1.929 (5)
S2—O231.487 (2)Li1—O23vii1.945 (5)
S2—Li1vi3.033 (5)Li1—O21ix1.952 (5)
S2—Li13.048 (6)Li1—S2vii3.033 (5)
O21—Li1iii1.952 (5)Li1—Li1vi3.238 (6)
O21—Yb2iii2.967 (4)Li1—Li1vii3.238 (6)
O22—Li1vii1.929 (5)Li1—Yb2vi3.534 (5)
O22—Yb22.955 (4)Li1—Yb2viii3.863 (5)
O22—Yb2v3.077 (5)Li2—O12viii1.930 (5)
O23—Li1vi1.945 (5)Li2—O11ii1.945 (5)
O23—Li11.976 (5)Li2—O14xi1.976 (6)
O24—Yb1iii2.789 (3)Li2—S1xi3.049 (5)
O24—Yb2viii2.958 (4)Li2—Li2i3.253 (7)
Yb1—O24ix2.789 (3)Li2—Li2xi3.253 (7)
Yb1—O12viii2.965 (5)Li2—Yb1i3.707 (5)
Yb1—O11ix2.966 (4)Li2—Yb1xi3.858 (5)
Yb1—O12x3.067 (4)
O13—S1—O11110.81 (15)O22x—Yb2—Li1iv61.38 (10)
O13—S1—O14109.66 (14)Li1vii—Yb2—Li1iv51.69 (10)
O11—S1—O14110.26 (13)Li1—Yb2—Li1iv82.64 (10)
O13—S1—O12108.61 (14)O13—Yb2—H219.4 (18)
O11—S1—O12108.90 (14)O22—Yb2—H21120.3 (18)
O14—S1—O12108.54 (13)O24iv—Yb2—H2190.8 (18)
O13—S1—Li2103.71 (14)O21ix—Yb2—H21113.3 (18)
O11—S1—Li283.67 (14)O22x—Yb2—H21112.0 (18)
O14—S1—Li232.67 (13)Li1vii—Yb2—H21148.6 (18)
O12—S1—Li2137.54 (13)Li1—Yb2—H21139.2 (18)
O13—S1—Li2i99.45 (15)Li1iv—Yb2—H21137.8 (18)
O11—S1—Li2i140.63 (13)O13—Yb2—H22100.9 (18)
O14—S1—Li2i32.93 (12)O22—Yb2—H22101.6 (19)
O12—S1—Li2i83.28 (13)O24iv—Yb2—H22157.5 (18)
Li2—S1—Li2i64.64 (12)O21ix—Yb2—H2221.2 (19)
S1—O11—Li2ii128.97 (19)O22x—Yb2—H2250.2 (19)
S1—O11—Yb1iii125.36 (13)Li1vii—Yb2—H2295.3 (18)
Li2ii—O11—Yb1iii95.78 (17)Li1—Yb2—H2246.2 (18)
S1—O12—Li2iv130.39 (19)Li1iv—Yb2—H2296.1 (18)
S1—O12—Yb1iv108.70 (13)H21—Yb2—H22110.3 (15)
Li2iv—O12—Yb1iv90.47 (17)O13—Yb2—H23115.2 (18)
S1—O12—Yb1v98.04 (12)O22—Yb2—H2310.0 (18)
Li2iv—O12—Yb1v113.64 (19)O24iv—Yb2—H2369.4 (19)
Yb1iv—O12—Yb1v116.77 (11)O21ix—Yb2—H2388.2 (19)
S1—O13—Yb2139.91 (15)O22x—Yb2—H23137.1 (18)
S1—O13—Yb1113.95 (13)Li1vii—Yb2—H2341.6 (18)
Yb2—O13—Yb1104.44 (10)Li1—Yb2—H2364.6 (18)
S1—O14—Li2123.22 (19)Li1iv—Yb2—H2390.4 (18)
S1—O14—Li2i123.01 (19)H21—Yb2—H23110.4 (15)
Li2—O14—Li2i111.50 (19)H22—Yb2—H23108.4 (15)
O24—S2—O21110.42 (14)O13—Yb2—H24114.0 (17)
O24—S2—O22108.95 (14)O22—Yb2—H24106.0 (18)
O21—S2—O22109.47 (14)O24iv—Yb2—H2455.6 (18)
O24—S2—O23109.34 (14)O21ix—Yb2—H24122.4 (18)
O21—S2—O23109.88 (14)O22x—Yb2—H2459.8 (18)
O22—S2—O23108.75 (12)Li1vii—Yb2—H2477.2 (18)
O24—S2—Li1vi102.87 (14)Li1—Yb2—H24109.1 (17)
O21—S2—Li1vi83.77 (14)Li1iv—Yb2—H2428.1 (17)
O22—S2—Li1vi137.68 (12)H21—Yb2—H24110.2 (15)
O23—S2—Li1vi32.26 (12)H22—Yb2—H24107.5 (14)
O24—S2—Li199.68 (14)H23—Yb2—H24109.9 (15)
O21—S2—Li1140.35 (13)O22vi—Li1—O23vii107.4 (2)
O22—S2—Li183.12 (12)O22vi—Li1—O21ix120.9 (3)
O23—S2—Li133.07 (12)O23vii—Li1—O21ix110.3 (2)
Li1vi—S2—Li164.34 (11)O22vi—Li1—O23103.5 (2)
S2—O21—Li1iii128.71 (17)O23vii—Li1—O23106.4 (2)
S2—O21—Yb2iii125.53 (13)O21ix—Li1—O23107.2 (2)
Li1iii—O21—Yb2iii96.06 (17)O22vi—Li1—S2vii88.12 (16)
S2—O22—Li1vii130.33 (18)O23vii—Li1—S2vii24.07 (8)
S2—O22—Yb2109.24 (13)O21ix—Li1—S2vii110.7 (2)
Li1vii—O22—Yb290.18 (17)O23—Li1—S2vii126.3 (2)
S2—O22—Yb2v97.69 (11)O22vi—Li1—S2127.5 (2)
Li1vii—O22—Yb2v113.85 (18)O23vii—Li1—S293.46 (17)
Yb2—O22—Yb2v116.82 (11)O21ix—Li1—S293.64 (17)
S2—O23—Li1vi123.67 (17)O23—Li1—S224.23 (9)
S2—O23—Li1122.70 (19)S2vii—Li1—S2117.07 (15)
Li1vi—O23—Li1111.31 (18)O22vi—Li1—Li1vi72.28 (16)
S2—O24—Yb1iii140.94 (15)O23vii—Li1—Li1vi128.8 (3)
S2—O24—Yb2viii114.43 (13)O21ix—Li1—Li1vi112.6 (2)
Yb1iii—O24—Yb2viii101.68 (10)O23—Li1—Li1vi34.03 (16)
O24ix—Yb1—O12viii128.95 (12)S2vii—Li1—Li1vi136.6 (2)
O24ix—Yb1—O11ix110.73 (11)S2—Li1—Li1vi57.61 (16)
O12viii—Yb1—O11ix82.76 (10)O22vi—Li1—Li1vii123.8 (3)
O24ix—Yb1—O1395.07 (11)O23vii—Li1—Li1vii34.65 (7)
O12viii—Yb1—O1372.67 (11)O21ix—Li1—Li1vii113.0 (2)
O11ix—Yb1—O13152.18 (10)O23—Li1—Li1vii72.8 (2)
O24ix—Yb1—O12x103.30 (12)S2vii—Li1—Li1vii58.05 (10)
O12viii—Yb1—O12x127.07 (12)S2—Li1—Li1vii59.03 (16)
O11ix—Yb1—O12x70.00 (9)Li1vi—Li1—Li1vii101.3 (3)
O13—Yb1—O12x115.03 (12)O22vi—Li1—Yb2vi56.74 (15)
O24ix—Yb1—Li2156.80 (13)O23vii—Li1—Yb2vi71.59 (15)
O12viii—Yb1—Li232.93 (10)O21ix—Li1—Yb2vi177.6 (2)
O11ix—Yb1—Li284.64 (11)O23—Li1—Yb2vi73.35 (16)
O13—Yb1—Li267.66 (11)S2vii—Li1—Yb2vi70.35 (10)
O12x—Yb1—Li298.22 (13)S2—Li1—Yb2vi87.72 (14)
O24ix—Yb1—Li2xi139.57 (13)Li1vi—Li1—Yb2vi66.48 (17)
O12viii—Yb1—Li2xi56.60 (10)Li1vii—Li1—Yb2vi69.41 (17)
O11ix—Yb1—Li2xi31.46 (9)O22vi—Li1—Yb2166.7 (2)
O13—Yb1—Li2xi120.74 (12)O23vii—Li1—Yb268.81 (14)
O12x—Yb1—Li2xi79.39 (11)O21ix—Li1—Yb252.48 (13)
Li2—Yb1—Li2xi53.19 (11)O23—Li1—Yb289.73 (16)
O24ix—Yb1—Li2i134.36 (13)S2vii—Li1—Yb284.61 (13)
O12viii—Yb1—Li2i83.77 (11)S2—Li1—Yb265.74 (10)
O11ix—Yb1—Li2i103.43 (11)Li1vi—Li1—Yb2120.3 (2)
O13—Yb1—Li2i61.78 (10)Li1vii—Li1—Yb260.57 (12)
O12x—Yb1—Li2i61.16 (11)Yb2vi—Li1—Yb2129.94 (15)
Li2—Yb1—Li2i51.88 (10)O22vi—Li1—Yb2viii102.44 (19)
Li2xi—Yb1—Li2i82.88 (10)O23vii—Li1—Yb2viii150.02 (19)
O24ix—Yb1—H117.4 (18)O21ix—Li1—Yb2viii53.72 (13)
O12viii—Yb1—H11124.0 (17)O23—Li1—Yb2viii63.13 (14)
O11ix—Yb1—H11117.0 (18)S2vii—Li1—Yb2viii164.14 (16)
O13—Yb1—H1188.1 (18)S2—Li1—Yb2viii65.58 (9)
O12x—Yb1—H11108.8 (17)Li1vi—Li1—Yb2viii58.90 (12)
Li2—Yb1—H11149.7 (18)Li1vii—Li1—Yb2viii122.0 (2)
Li2xi—Yb1—H11144.2 (18)Yb2vi—Li1—Yb2viii125.35 (15)
Li2i—Yb1—H11132.1 (18)Yb2—Li1—Yb2viii82.64 (10)
O24ix—Yb1—H12101.1 (17)O12viii—Li2—O11ii120.9 (3)
O12viii—Yb1—H1299.1 (18)O12viii—Li2—O14107.1 (2)
O11ix—Yb1—H1216.4 (18)O11ii—Li2—O14111.0 (3)
O13—Yb1—H12163.5 (17)O12viii—Li2—O14xi103.3 (2)
O12x—Yb1—H1258.1 (19)O11ii—Li2—O14xi107.5 (2)
Li2—Yb1—H1297.6 (17)O14—Li2—O14xi105.7 (2)
Li2xi—Yb1—H1245.7 (18)O12viii—Li2—S188.02 (17)
Li2i—Yb1—H12103.8 (18)O11ii—Li2—S1111.1 (2)
H11—Yb1—H12108.1 (14)O14—Li2—S124.11 (9)
O24ix—Yb1—H13110.1 (17)O14xi—Li2—S1125.7 (2)
O12viii—Yb1—H13107.7 (18)O12viii—Li2—S1xi127.2 (2)
O11ix—Yb1—H13114.0 (18)O11ii—Li2—S1xi94.00 (19)
O13—Yb1—H1363.5 (18)O14—Li2—S1xi93.13 (19)
O12x—Yb1—H1351.6 (18)O14xi—Li2—S1xi24.06 (9)
Li2—Yb1—H1376.9 (18)S1—Li2—S1xi116.79 (16)
Li2xi—Yb1—H13102.9 (17)O12viii—Li2—Li2i123.2 (3)
Li2i—Yb1—H1325.4 (17)O11ii—Li2—Li2i113.7 (2)
H11—Yb1—H13109.2 (15)O14—Li2—Li2i34.43 (7)
H12—Yb1—H13107.2 (14)O14xi—Li2—Li2i72.4 (2)
O24ix—Yb1—H14116.2 (18)S1—Li2—Li2i57.88 (9)
O12viii—Yb1—H1414.1 (18)S1xi—Li2—Li2i58.92 (17)
O11ix—Yb1—H1493.3 (19)O12viii—Li2—Li2xi72.04 (16)
O13—Yb1—H1465.1 (19)O11ii—Li2—Li2xi113.0 (2)
O12x—Yb1—H14140.5 (18)O14—Li2—Li2xi127.8 (3)
Li2—Yb1—H1443.3 (18)O14xi—Li2—Li2xi34.07 (17)
Li2xi—Yb1—H1469.7 (18)S1—Li2—Li2xi135.8 (2)
Li2i—Yb1—H1490.4 (18)S1xi—Li2—Li2xi57.48 (17)
H11—Yb1—H14110.7 (15)Li2i—Li2—Li2xi100.7 (3)
H12—Yb1—H14109.7 (15)O12viii—Li2—Yb156.60 (14)
H13—Yb1—H14111.8 (15)O11ii—Li2—Yb1177.4 (2)
O13—Yb2—O22124.64 (12)O14—Li2—Yb171.20 (14)
O13—Yb2—O24iv99.98 (10)O14xi—Li2—Yb172.88 (17)
O22—Yb2—O24iv72.69 (10)S1—Li2—Yb170.22 (10)
O13—Yb2—O21ix104.82 (11)S1xi—Li2—Yb187.27 (15)
O22—Yb2—O21ix82.52 (10)Li2i—Li2—Yb168.93 (17)
O24iv—Yb2—O21ix152.00 (11)Li2xi—Li2—Yb165.86 (17)
O13—Yb2—O22x106.02 (11)O12viii—Li2—Yb1i166.9 (2)
O22—Yb2—O22x127.10 (12)O11ii—Li2—Yb1i52.76 (14)
O24iv—Yb2—O22x115.42 (12)O14—Li2—Yb1i69.04 (15)
O21ix—Yb2—O22x69.85 (9)O14xi—Li2—Yb1i89.74 (17)
O13—Yb2—Li1vii155.77 (13)S1—Li2—Yb1i84.70 (13)
O22—Yb2—Li1vii33.09 (9)S1xi—Li2—Yb1i65.90 (11)
O24iv—Yb2—Li1vii67.76 (10)Li2i—Li2—Yb1i60.94 (13)
O21ix—Yb2—Li1vii84.38 (11)Li2xi—Li2—Yb1i120.5 (2)
O22x—Yb2—Li1vii98.18 (12)Yb1—Li2—Yb1i129.83 (15)
O13—Yb2—Li1132.54 (13)O12viii—Li2—Yb1xi102.3 (2)
O22—Yb2—Li156.40 (10)O11ii—Li2—Yb1xi53.79 (14)
O24iv—Yb2—Li1120.57 (11)O14—Li2—Yb1xi150.3 (2)
O21ix—Yb2—Li131.46 (9)O14xi—Li2—Yb1xi63.41 (15)
O22x—Yb2—Li179.36 (10)S1—Li2—Yb1xi164.60 (16)
Li1vii—Yb2—Li152.95 (10)S1xi—Li2—Yb1xi65.78 (10)
O13—Yb2—Li1iv142.16 (13)Li2i—Li2—Yb1xi122.2 (2)
O22—Yb2—Li1iv83.74 (10)Li2xi—Li2—Yb1xi59.19 (12)
O24iv—Yb2—Li1iv61.97 (10)Yb1—Li2—Yb1xi125.02 (16)
O21ix—Yb2—Li1iv103.22 (11)Yb1i—Li2—Yb1xi82.88 (10)
Symmetry codes: (i) x+1, y+1/2, z+1/2; (ii) x+1, y+1, z+1; (iii) x, y+1/2, z+1/2; (iv) x, y+1, z; (v) x, y+3/2, z+1/2; (vi) x, y1/2, z+1/2; (vii) x, y+1/2, z+1/2; (viii) x, y1, z; (ix) x, y+1/2, z1/2; (x) x, y+3/2, z1/2; (xi) x+1, y1/2, z+1/2.
(alpha2_LAS) top
Crystal data top
O4SYb0.013·0.961(H4N)·LiF(000) = 1000.0
Mr = 122.51Dx = 1.831 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 10.177 (15) ÅCell parameters from 25 reflections
b = 5.106 (4) Åθ = 9–19°
c = 34.234 (16) ŵ = 0.89 mm1
β = 90.2 (1)°T = 293 K
V = 1779 (3) Å3Prism, colourless
Z = 160.17 × 0.11 × 0.09 mm
Data collection top
ENRAF-Nonius CAD4
diffractometer
θmax = 30.0°, θmin = 2.0°
ω/2Θ–scanh = 1414
9573 measured reflectionsk = 77
5071 independent reflectionsl = 480
3231 reflections with I > 2σ(I)3 standard reflections every 120 min
Rint = 0.068
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.060Hydrogen site location: notdet
wR(F2) = 0.163H-atom parameters not defined
S = 1.20 w = 1/[σ2(Fo2) + (0.0263P)2 + 6.4506P]
where P = (Fo2 + 2Fc2)/3
5071 reflections(Δ/σ)max < 0.001
256 parametersΔρmax = 1.89 e Å3
0 restraintsΔρmin = 1.04 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
S10.64805 (7)0.73307 (14)0.20089 (2)0.00608 (14)
O110.6399 (4)0.4374 (5)0.20610 (11)0.0406 (9)
O120.7859 (3)0.8058 (10)0.20413 (11)0.0521 (12)
O130.5709 (3)0.8568 (6)0.23235 (9)0.0274 (7)
O140.5950 (4)0.7924 (10)0.16305 (10)0.0566 (13)
S20.89820 (8)0.28368 (18)0.04920 (3)0.01657 (19)
O210.8934 (3)0.5828 (6)0.04414 (10)0.0324 (8)
O221.0370 (3)0.2110 (6)0.04620 (9)0.0298 (7)
O230.8456 (3)0.2180 (7)0.08669 (9)0.0368 (8)
O240.8213 (3)0.1630 (6)0.01798 (9)0.0280 (7)
S30.39959 (8)0.21622 (18)0.04902 (3)0.01718 (19)
O310.5355 (3)0.2891 (6)0.04630 (10)0.0304 (7)
O320.3211 (3)0.3371 (6)0.01735 (9)0.0273 (7)
O330.3916 (3)0.0811 (6)0.04468 (10)0.0330 (8)
O340.3434 (3)0.2813 (7)0.08748 (9)0.0324 (7)
S40.14878 (11)0.8032 (3)0.20093 (4)0.0364 (3)
O410.1414 (3)1.1054 (7)0.20461 (9)0.0314 (7)
O420.2864 (2)0.7278 (5)0.20357 (8)0.0211 (5)
O430.0927 (3)0.7312 (6)0.16299 (9)0.0272 (6)
O440.0714 (3)0.6850 (7)0.23248 (9)0.0292 (7)
N10.4006 (3)0.2369 (6)0.16624 (10)0.0417 (11)0.907 (4)
N20.6508 (3)0.7697 (7)0.08377 (10)0.0364 (13)0.959 (4)
N30.1517 (3)0.7309 (7)0.08326 (11)0.0331 (14)0.978 (4)
N40.9005 (4)0.2744 (9)0.16666 (12)0.0381 (10)
Yb10.4006 (3)0.2369 (6)0.16624 (10)0.0417 (11)0.0311 (15)
Yb20.6508 (3)0.7697 (7)0.08377 (10)0.0364 (13)0.0137 (15)
Yb30.1517 (3)0.7309 (7)0.08326 (11)0.0331 (14)0.0074 (14)
Li10.3992 (7)0.7198 (14)0.2497 (2)0.0237 (14)
Li20.1017 (7)0.3041 (15)0.2508 (2)0.0278 (16)
Li30.1488 (7)0.2123 (13)0.0001 (2)0.0218 (14)
Li40.6491 (6)0.2976 (12)0.0013 (2)0.0190 (13)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0035 (3)0.0084 (3)0.0063 (3)0.0004 (3)0.0014 (2)0.0003 (3)
O110.065 (2)0.0118 (13)0.045 (2)0.0014 (14)0.0142 (18)0.0014 (13)
O120.0098 (13)0.114 (4)0.0322 (19)0.0037 (18)0.0014 (12)0.005 (2)
O130.0287 (15)0.0257 (14)0.0279 (17)0.0020 (12)0.0078 (13)0.0013 (12)
O140.0377 (19)0.122 (4)0.0099 (14)0.016 (2)0.0061 (13)0.001 (2)
S20.0104 (3)0.0249 (4)0.0144 (4)0.0028 (3)0.0027 (3)0.0003 (3)
O210.0384 (18)0.0255 (14)0.0332 (19)0.0041 (13)0.0138 (14)0.0020 (13)
O220.0117 (11)0.051 (2)0.0270 (16)0.0109 (12)0.0030 (11)0.0023 (14)
O230.0348 (17)0.060 (2)0.0155 (14)0.0126 (16)0.0031 (12)0.0080 (15)
O240.0218 (14)0.0364 (16)0.0257 (17)0.0053 (12)0.0079 (12)0.0079 (13)
S30.0114 (3)0.0266 (5)0.0135 (4)0.0016 (3)0.0026 (3)0.0019 (3)
O310.0112 (11)0.0487 (19)0.0313 (17)0.0048 (12)0.0051 (11)0.0013 (14)
O320.0209 (14)0.0369 (15)0.0238 (16)0.0019 (12)0.0116 (12)0.0060 (13)
O330.0323 (17)0.0259 (15)0.041 (2)0.0004 (12)0.0165 (15)0.0033 (14)
O340.0259 (14)0.0484 (19)0.0230 (15)0.0146 (14)0.0050 (12)0.0002 (14)
S40.0179 (4)0.0704 (9)0.0209 (5)0.0018 (5)0.0000 (4)0.0005 (6)
O410.0173 (13)0.057 (2)0.0205 (15)0.0063 (14)0.0055 (11)0.0008 (15)
O420.0074 (10)0.0309 (14)0.0249 (14)0.0036 (10)0.0002 (9)0.0053 (12)
O430.0234 (13)0.0381 (16)0.0200 (14)0.0162 (13)0.0093 (11)0.0002 (13)
O440.0111 (12)0.056 (2)0.0207 (15)0.0053 (12)0.0038 (11)0.0073 (13)
N10.0405 (18)0.0413 (17)0.0432 (19)0.0032 (13)0.0030 (12)0.0037 (14)
N20.034 (2)0.043 (2)0.032 (2)0.0015 (15)0.0024 (13)0.0043 (15)
N30.0247 (18)0.043 (2)0.032 (2)0.0003 (15)0.0039 (13)0.0048 (16)
N40.0216 (16)0.067 (3)0.0252 (19)0.0026 (19)0.0052 (14)0.002 (2)
Yb10.0405 (18)0.0413 (17)0.0432 (19)0.0032 (13)0.0030 (12)0.0037 (14)
Yb20.034 (2)0.043 (2)0.032 (2)0.0015 (15)0.0024 (13)0.0043 (15)
Yb30.0247 (18)0.043 (2)0.032 (2)0.0003 (15)0.0039 (13)0.0048 (16)
Li10.019 (3)0.034 (4)0.018 (3)0.001 (3)0.004 (2)0.002 (3)
Li20.018 (3)0.040 (4)0.025 (4)0.003 (3)0.006 (3)0.000 (3)
Li30.024 (3)0.021 (3)0.021 (3)0.002 (2)0.002 (3)0.006 (3)
Li40.011 (3)0.023 (3)0.023 (3)0.000 (2)0.002 (2)0.006 (2)
Geometric parameters (Å, º) top
S1—O141.434 (3)S4—O431.464 (3)
S1—O121.455 (4)S4—O441.469 (3)
S1—O131.477 (3)S4—O411.550 (4)
S1—O111.522 (3)S4—Li2ix3.043 (9)
S1—Li13.040 (8)O41—Li2iii1.922 (9)
S1—Li1i3.045 (7)O41—Yb1iii3.027 (6)
O11—Li1ii1.920 (8)O42—Li11.950 (8)
O12—Li2i1.918 (8)O44—Li2ix1.951 (8)
O13—Li1i1.976 (8)O44—Li22.066 (8)
O13—Li11.976 (8)Li1—O11i1.920 (8)
O14—Yb1iii3.013 (6)Li1—O13ii1.976 (8)
S2—O231.432 (3)Li1—S1ii3.045 (7)
S2—O241.459 (3)Li1—Li1ii3.275 (9)
S2—O221.464 (3)Li1—Li1i3.275 (9)
S2—O211.538 (3)Li1—Yb1i3.520 (8)
S2—Li43.016 (7)Li1—Yb1iii3.891 (8)
O21—Li3iv1.890 (8)Li2—O12ii1.918 (8)
O21—Yb3v3.042 (6)Li2—O41vii1.922 (9)
O22—Li3v1.948 (8)Li2—O44x1.951 (8)
O22—Yb3vi2.996 (5)Li2—S4x3.043 (9)
O23—Yb2vii3.030 (5)Li2—Li2ix3.287 (9)
O24—Li41.966 (7)Li2—Li2x3.287 (9)
O24—Li3viii2.037 (7)Li3—O21iv1.890 (8)
S3—O311.436 (3)Li3—O22xi1.948 (8)
S3—O341.475 (3)Li3—O24viii2.037 (7)
S3—O321.479 (3)Li3—Li4iv3.239 (9)
S3—O331.527 (3)Li3—Li4viii3.319 (9)
S3—Li33.047 (8)Li3—Yb2iv3.530 (9)
O31—Li41.930 (8)Li3—Yb3vii3.760 (8)
O32—Li31.954 (8)Li4—O33viii1.966 (7)
O32—Li4iv1.995 (7)Li4—O32iv1.995 (7)
O33—Li4viii1.966 (7)Li4—Li3iv3.239 (9)
O33—Yb3vii2.941 (6)Li4—Li3viii3.319 (9)
O33—Yb2vii3.050 (6)Li4—Yb3iv3.542 (9)
S4—O421.455 (3)Li4—Yb2vii3.904 (8)
O14—S1—O12112.0 (2)O13ii—Li1—Yb1i71.4 (2)
O14—S1—O13111.7 (2)O13—Li1—Yb1i74.2 (2)
O12—S1—O13110.5 (2)S1—Li1—Yb1i88.2 (2)
O14—S1—O11107.2 (3)S1ii—Li1—Yb1i70.03 (16)
O12—S1—O11107.3 (3)Li1ii—Li1—Yb1i69.8 (3)
O13—S1—O11108.0 (2)Li1i—Li1—Yb1i67.4 (3)
O14—S1—Li1101.0 (2)O11i—Li1—Yb1iii100.8 (3)
O12—S1—Li1140.2 (2)O42—Li1—Yb1iii52.7 (2)
O13—S1—Li133.14 (19)O13ii—Li1—Yb1iii149.8 (3)
O11—S1—Li182.4 (2)O13—Li1—Yb1iii62.2 (2)
O14—S1—Li1i105.6 (2)S1—Li1—Yb1iii64.90 (15)
O12—S1—Li1i84.5 (2)S1ii—Li1—Yb1iii164.3 (2)
O13—S1—Li1i32.91 (18)Li1ii—Li1—Yb1iii122.0 (3)
O11—S1—Li1i137.4 (2)Li1i—Li1—Yb1iii58.09 (19)
Li1—S1—Li1i65.12 (16)Yb1i—Li1—Yb1iii125.4 (2)
S1—O11—Li1ii132.7 (3)O12ii—Li2—O41vii122.5 (4)
S1—O12—Li2i129.2 (3)O12ii—Li2—O44x107.6 (4)
S1—O13—Li1i123.1 (3)O41vii—Li2—O44x105.6 (4)
S1—O13—Li1122.7 (3)O12ii—Li2—O44109.1 (4)
Li1i—O13—Li1112.0 (3)O41vii—Li2—O44106.2 (4)
S1—O14—Yb1iii111.8 (2)O44x—Li2—O44104.4 (3)
O23—S2—O24110.9 (2)O12ii—Li2—S4x93.5 (3)
O23—S2—O22111.5 (2)O41vii—Li2—S4x128.7 (3)
O24—S2—O22110.9 (2)O44x—Li2—S4x23.27 (15)
O23—S2—O21108.8 (2)O44—Li2—S4x92.4 (3)
O24—S2—O21108.67 (18)O12ii—Li2—Li2ix112.5 (4)
O22—S2—O21105.90 (19)O41vii—Li2—Li2ix122.1 (4)
O23—S2—Li4100.2 (2)O44x—Li2—Li2ix71.2 (4)
O24—S2—Li433.25 (17)O44—Li2—Li2ix33.96 (10)
O22—S2—Li4140.99 (19)S4x—Li2—Li2ix58.8 (3)
O21—S2—Li483.62 (17)O12ii—Li2—Li2x113.0 (4)
S2—O21—Li3iv130.3 (3)O41vii—Li2—Li2x73.2 (3)
S2—O21—Yb3v99.80 (16)O44x—Li2—Li2x36.3 (3)
Li3iv—O21—Yb3v114.2 (3)O44—Li2—Li2x129.3 (4)
S2—O22—Li3v128.5 (3)S4x—Li2—Li2x58.6 (3)
S2—O22—Yb3vi123.5 (2)Li2ix—Li2—Li2x101.9 (4)
Li3v—O22—Yb3vi96.8 (2)O21iv—Li3—O22xi121.3 (4)
S2—O23—Yb2vii113.19 (18)O21iv—Li3—O32105.2 (4)
S2—O24—Li4122.7 (3)O22xi—Li3—O32106.4 (4)
S2—O24—Li3viii122.7 (3)O21iv—Li3—O24viii108.1 (3)
Li4—O24—Li3viii112.0 (3)O22xi—Li3—O24viii109.4 (4)
O31—S3—O34112.1 (2)O32—Li3—O24viii105.3 (3)
O31—S3—O32111.2 (2)O21iv—Li3—S3128.6 (3)
O34—S3—O32110.49 (19)O22xi—Li3—S392.6 (3)
O31—S3—O33107.58 (19)O32—Li3—S323.58 (14)
O34—S3—O33106.9 (2)O24viii—Li3—S392.7 (2)
O32—S3—O33108.37 (18)O21iv—Li3—Li4iv72.7 (3)
O31—S3—Li3140.5 (2)O22xi—Li3—Li4iv112.8 (3)
O34—S3—Li399.5 (2)O32—Li3—Li4iv35.30 (19)
O32—S3—Li331.90 (19)O24viii—Li3—Li4iv128.8 (3)
O33—S3—Li384.04 (17)S3—Li3—Li4iv58.17 (16)
S3—O31—Li4129.6 (3)O21iv—Li3—Li4viii124.2 (3)
S3—O32—Li3124.5 (3)O22xi—Li3—Li4viii111.9 (3)
S3—O32—Li4iv122.8 (3)O32—Li3—Li4viii72.8 (2)
Li3—O32—Li4iv110.2 (3)O24viii—Li3—Li4viii33.33 (19)
S3—O33—Li4viii130.4 (3)S3—Li3—Li4viii59.68 (16)
S3—O33—Yb3vii108.95 (19)Li4iv—Li3—Li4viii102.3 (2)
Li4viii—O33—Yb3vii90.2 (2)O21iv—Li3—Yb2iv57.5 (2)
S3—O33—Yb2vii99.22 (15)O22xi—Li3—Yb2iv178.6 (3)
Li4viii—O33—Yb2vii113.0 (2)O32—Li3—Yb2iv73.5 (3)
Yb3vii—O33—Yb2vii116.06 (16)O24viii—Li3—Yb2iv71.9 (2)
O42—S4—O43111.2 (2)S3—Li3—Yb2iv87.8 (2)
O42—S4—O44111.4 (2)Li4iv—Li3—Yb2iv66.37 (18)
O43—S4—O44109.9 (2)Li4viii—Li3—Yb2iv69.43 (18)
O42—S4—O41107.78 (18)O21iv—Li3—Yb3vii165.9 (3)
O43—S4—O41107.7 (2)O22xi—Li3—Yb3vii52.3 (2)
O44—S4—O41108.9 (2)O32—Li3—Yb3vii88.9 (3)
O42—S4—Li2ix140.8 (2)O24viii—Li3—Yb3vii67.3 (2)
O43—S4—Li2ix99.1 (2)S3—Li3—Yb3vii65.44 (15)
O44—S4—Li2ix31.65 (19)Li4iv—Li3—Yb3vii120.9 (2)
O41—S4—Li2ix85.04 (19)Li4viii—Li3—Yb3vii59.66 (18)
S4—O41—Li2iii127.1 (3)Yb2iv—Li3—Yb3vii129.0 (2)
S4—O41—Yb1iii98.23 (15)O31—Li4—O33viii120.1 (3)
Li2iii—O41—Yb1iii115.2 (3)O31—Li4—O24107.2 (4)
S4—O42—Li1128.3 (3)O33viii—Li4—O24102.8 (3)
S4—O44—Li2ix125.1 (3)O31—Li4—O32iv111.6 (3)
S4—O44—Li2122.0 (3)O33viii—Li4—O32iv107.6 (4)
Li2ix—O44—Li2109.8 (3)O24—Li4—O32iv106.5 (3)
O11i—Li1—O42120.2 (4)O31—Li4—S294.0 (3)
O11i—Li1—O13ii109.3 (4)O33viii—Li4—S2126.6 (3)
O42—Li1—O13ii111.2 (4)O24—Li4—S224.01 (13)
O11i—Li1—O13102.6 (4)O32iv—Li4—S293.9 (2)
O42—Li1—O13105.5 (4)O31—Li4—Li3iv114.3 (3)
O13ii—Li1—O13106.9 (3)O33viii—Li4—Li3iv123.7 (3)
O11i—Li1—S1126.6 (3)O24—Li4—Li3iv73.1 (2)
O42—Li1—S192.5 (3)O32iv—Li4—Li3iv34.47 (19)
O13ii—Li1—S193.7 (3)S2—Li4—Li3iv59.59 (16)
O13—Li1—S124.12 (14)O31—Li4—Li3viii111.5 (3)
O11i—Li1—S1ii90.1 (3)O33viii—Li4—Li3viii71.1 (2)
O42—Li1—S1ii111.9 (3)O24—Li4—Li3viii34.71 (18)
O13ii—Li1—S1ii23.96 (13)O32iv—Li4—Li3viii129.3 (3)
O13—Li1—S1ii126.7 (3)S2—Li4—Li3viii57.96 (15)
S1—Li1—S1ii117.2 (2)Li3iv—Li4—Li3viii102.3 (2)
O11i—Li1—Li1ii125.3 (4)O31—Li4—Yb3iv175.9 (3)
O42—Li1—Li1ii112.8 (4)O33viii—Li4—Yb3iv56.1 (2)
O13ii—Li1—Li1ii34.03 (11)O24—Li4—Yb3iv73.2 (2)
O13—Li1—Li1ii73.9 (3)O32iv—Li4—Yb3iv71.9 (2)
S1—Li1—Li1ii59.8 (2)S2—Li4—Yb3iv87.77 (18)
S1ii—Li1—Li1ii57.36 (15)Li3iv—Li4—Yb3iv69.78 (18)
O11i—Li1—Li1i71.1 (2)Li3viii—Li4—Yb3iv66.38 (18)
O42—Li1—Li1i110.8 (3)O31—Li4—Yb2vii53.7 (2)
O13ii—Li1—Li1i129.3 (4)O33viii—Li4—Yb2vii101.0 (3)
O13—Li1—Li1i34.0 (2)O24—Li4—Yb2vii63.0 (2)
S1—Li1—Li1i57.5 (2)O32iv—Li4—Yb2vii151.2 (3)
S1ii—Li1—Li1i137.1 (4)S2—Li4—Yb2vii65.70 (15)
Li1ii—Li1—Li1i102.4 (4)Li3iv—Li4—Yb2vii122.9 (2)
O11i—Li1—Yb1i57.5 (2)Li3viii—Li4—Yb2vii57.83 (17)
O42—Li1—Yb1i177.3 (3)Yb3iv—Li4—Yb2vii124.17 (19)
Symmetry codes: (i) x+1, y+1/2, z+1/2; (ii) x+1, y1/2, z+1/2; (iii) x, y+1, z; (iv) x+1, y+1, z; (v) x+1, y, z; (vi) x+1, y1, z; (vii) x, y1, z; (viii) x+1, y, z; (ix) x, y+1/2, z+1/2; (x) x, y1/2, z+1/2; (xi) x1, y, z.
 

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