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Three new potassium rare-earth/titanium phosphate structures, K2ErTi(PO4)3 (KErTP), K2YbTi(PO4)3 (KYbTP) and K2YTi(PO4)3 (KYTP), are presented, all of which are characterized by single-crystal X-ray diffraction studies. In addition, a fourth structure, K2CrTi(PO4)3 (KCrTP), has been reinvestigated. All structures are isostructural to the langbeinite-type structure and result from changes made to the growth constituents in high-temperature flux-growth experiments intended to give structurally modified potassium titanyl phosphate (KTP). The two crystallographically independent octahedra sites (site symmetry 3) have a mixed Ti/M (M = Er, Yb, Y or Cr) population, although the rare-earth metals favour one site while chromium favours the other. An alternative approach for the description of the channels and cation cages in langbeinite and related structures is given using [M5X6O39] units. The framework of langbeinite is compared with that of nasicon using these alternative building units. All of the investigated structures crystallize in space group P213 with Z = 4; a = 10.1053 (2) Å, R = 0.023 (KErTP); a = 10.0939 (8) Å, R = 0.022 (KYbTP); a = 10.1318 (6) Å, R = 0.047 (KYTP); a = 9.8001 (2) Å, R = 0.016 (KCrTP).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768102013782/os0095sup1.cif
Contains datablocks global, KErTP, KYbTP, KYTP, KCrTP

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102013782/os0095KErTPsup2.hkl
Contains datablock KErTP

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102013782/os0095KYbTPsup3.hkl
Contains datablock KYbTP

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102013782/os0095KYTPsup4.hkl
Contains datablock KYTP

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102013782/os0095KCrTPsup5.hkl
Contains datablock KCrTP

Computing details top

For all compounds, data collection: CAD-4 Software (Enraf-Nonius, 1989). Cell refinement: CAD-4 Software (Enraf-Nonius, 1989) for KErTP, KYbTP, KCrTP; Xtal3.71 (Hall et al., 2000) program: LATCON for KYTP. For all compounds, data reduction: Xtal3.71 (Hall et al., 2000) programs: DIFDAT; SORTRF; ADDREF; ABSORB; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: Xtal3.71 (Hall et al., 2000) program: CRYLSQ; software used to prepare material for publication: Xtal3.71 (Hall et al., 2000) programs: BONDLA; ATABLE; CIFIO.

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
(KErTP) top
Crystal data top
K2ErTiP3O12Dx = 3.722 Mg m3
Mr = 578.25Mo Kα radiation, λ = 0.71073 Å
Cubic, P213Cell parameters from 20 reflections
Hall symbol: P 2ac 2ab 3θ = 26.6–29.8°
a = 10.1053 (2) ŵ = 10.19 mm1
V = 1031.92 (4) Å3T = 293 K
Z = 4Tetrahedron, colourless
F(000) = 10760.06 × 0.06 × 0.05 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
967 reflections with F2 > 2σ(F2)
Radiation source: Fine-focus sealed tubeRint = 0.048
Graphite monochromatorθmax = 29.9°, θmin = 3.5°
ω–2θ scansh = 140
Absorption correction: analytical
(Alcock, 1974)
k = 140
Tmin = 0.567, Tmax = 0.650l = 1414
3285 measured reflections3 standard reflections every 120 min
1008 independent reflections intensity decay: none
Refinement top
Refinement on F2 w = 1/[σ2(Fsqd) + 0.008(Fsqd)2]
Least-squares matrix: full(Δ/σ)max = 0.00018
R[F2 > 2σ(F2)] = 0.023Δρmax = 0.60 e Å3
wR(F2) = 0.077Δρmin = 0.76 e Å3
S = 1.06Extinction correction: Isotropic Gaussian, Zachariasen, 1967; Larson (1970), Eq22 p292 "Cryst. Comp." Munksgaard 1970
1008 reflectionsExtinction coefficient: 90 (22) × 102
61 parametersAbsolute structure: Flack (1983) parameter refined
0 restraintsAbsolute structure parameter: 0.04 (3)
9 constraints
Crystal data top
K2ErTiP3O12Z = 4
Mr = 578.25Mo Kα radiation
Cubic, P213µ = 10.19 mm1
a = 10.1053 (2) ÅT = 293 K
V = 1031.92 (4) Å30.06 × 0.06 × 0.05 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
967 reflections with F2 > 2σ(F2)
Absorption correction: analytical
(Alcock, 1974)
Rint = 0.048
Tmin = 0.567, Tmax = 0.6503 standard reflections every 120 min
3285 measured reflections intensity decay: none
1008 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0230 restraints
wR(F2) = 0.077Δρmax = 0.60 e Å3
S = 1.06Δρmin = 0.76 e Å3
1008 reflectionsAbsolute structure: Flack (1983) parameter refined
61 parametersAbsolute structure parameter: 0.04 (3)
Special details top

Refinement. The following constraints were used during the refinement:

H-atom parameters constrained x(Ti1)=0.0 + 1.0*x(Er1) H-atom parameters constrained u11(Ti1)=0.0 + 1.0*u11(Er1) H-atom parameters constrained u12(Ti1)=0.0 + 1.0*u12(Er1) H-atom parameters constrained x(Ti2)=0.0 + 1.0*x(Er2) H-atom parameters constrained u11(Ti2)=0.0 + 1.0*u11(Er2) H-atom parameters constrained u12(Ti2)=0.0 + 1.0*u12(Er2) H-atom parameters constrained pop(Ti1)=1.0–1.0*pop(Er1) H-atom parameters constrained pop(Ti2)=0.0 + 1.0*pop(Er1) H-atom parameters constrained pop(Er2)=1.0–1.0*pop(Er1)

No restraints used.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
K10.04526 (18)0.54526 (18)0.04526 (18)0.0307 (6)
K20.18088 (16)0.31912 (16)0.18088 (16)0.0261 (5)
Er10.16698 (4)0.66698 (4)0.33302 (4)0.0131 (2)0.583 (3)
Ti10.16698 (4)0.66698 (4)0.33302 (4)0.0131 (2)0.417 (3)
Er20.39957 (4)0.60043 (4)0.10043 (4)0.0129 (3)0.417 (3)
Ti20.39957 (4)0.60043 (4)0.10043 (4)0.0129 (3)0.583 (3)
P0.12640 (17)0.48419 (18)0.28844 (17)0.0195 (7)
O10.0993 (8)0.3452 (8)0.2408 (7)0.049 (4)
O20.0052 (8)0.5669 (11)0.2705 (9)0.065 (5)
O30.1693 (7)0.4850 (7)0.4327 (7)0.044 (4)
O40.2331 (8)0.5476 (9)0.2023 (10)0.058 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
K10.0307 (6)0.0307 (6)0.0307 (6)0.0007 (6)0.0007 (6)0.0007 (6)
K20.0261 (5)0.0261 (5)0.0261 (5)0.0031 (5)0.0031 (5)0.0031 (5)
Er10.0131 (2)0.0131 (2)0.0131 (2)0.0046 (4)0.0046 (4)0.0046 (4)
Ti10.0131 (2)0.0131 (2)0.0131 (2)0.0046 (4)0.0046 (4)0.0046 (4)
Er20.0129 (3)0.0129 (3)0.0129 (3)0.0004 (5)0.0004 (5)0.0004 (5)
Ti20.0129 (3)0.0129 (3)0.0129 (3)0.0004 (5)0.0004 (5)0.0004 (5)
P0.0158 (7)0.0232 (8)0.0196 (7)0.0015 (6)0.0019 (6)0.0004 (6)
O10.053 (4)0.048 (4)0.046 (4)0.022 (4)0.002 (4)0.015 (3)
O20.044 (4)0.086 (6)0.064 (5)0.038 (4)0.009 (4)0.028 (5)
O30.045 (4)0.055 (4)0.033 (3)0.001 (4)0.019 (3)0.011 (3)
O40.049 (4)0.049 (4)0.076 (6)0.017 (4)0.034 (4)0.006 (4)
Geometric parameters (Å, º) top
K1—K23.958 (2)Er1—O22.109 (9)
K1—O23.224 (9)Ti1—O22.109 (9)
K1—O43.141 (9)Ti1—O1ii2.065 (8)
K1—O32.909 (8)Ti1—O22.109 (9)
K1—O32.909 (8)Ti1—O1iii2.065 (8)
K1—O23.224 (9)Ti1—O1i2.065 (8)
K1—O43.141 (9)Ti1—O22.109 (9)
K1—O2i3.224 (9)Er2—O42.043 (9)
K1—O4i3.141 (9)Er2—O32.026 (7)
K1—O32.909 (8)Er2—O3iv2.026 (7)
K2—O12.907 (8)Er2—O42.043 (9)
K2—O23.145 (11)Er2—O32.026 (7)
K2—O43.033 (9)Er2—O42.043 (9)
K2—O23.145 (11)Ti2—O42.043 (9)
K2—O43.033 (9)Ti2—O32.026 (7)
K2—O12.907 (8)Ti2—O3iv2.026 (7)
K2—O1i2.907 (8)Ti2—O42.043 (9)
K2—O23.145 (11)Ti2—O32.026 (7)
K2—O43.033 (9)Ti2—O42.043 (9)
Er1—O22.109 (9)P—O11.510 (8)
Er1—O1ii2.065 (8)P—O21.494 (10)
Er1—O22.109 (9)P—O31.521 (7)
Er1—O1iii2.065 (8)P—O41.527 (9)
Er1—O1i2.065 (8)
O2—K1—O444.5 (2)O1i—K2—O259.4 (2)
O2—K1—O3102.0 (2)O1i—K2—O499.8 (2)
O2—K1—O3164.4 (2)O2—K2—O445.9 (2)
O2—K1—O287.2 (3)O2—Er1—O1ii92.1 (4)
O2—K1—O4130.8 (3)O2—Er1—O289.7 (4)
O2—K1—O2i87.2 (3)O2—Er1—O1iii172.5 (4)
O2—K1—O4i82.3 (2)O2—Er1—O1i83.0 (3)
O2—K1—O380.7 (3)O2—Er1—O289.7 (4)
O4—K1—O357.5 (2)O1ii—Er1—O283.0 (3)
O4—K1—O3148.5 (2)O1ii—Er1—O1iii95.4 (3)
O4—K1—O282.3 (2)O1ii—Er1—O1i95.4 (3)
O4—K1—O4118.9 (2)O1ii—Er1—O2172.5 (4)
O4—K1—O2i130.8 (3)O2—Er1—O1iii92.1 (4)
O4—K1—O4i118.9 (2)O2—Er1—O1i172.5 (4)
O4—K1—O382.1 (2)O2—Er1—O289.7 (4)
O3—K1—O392.1 (2)O1iii—Er1—O1i95.4 (3)
O3—K1—O280.7 (3)O1iii—Er1—O283.0 (3)
O3—K1—O482.1 (2)O1i—Er1—O292.1 (4)
O3—K1—O2i164.4 (2)O2—Ti1—O1ii92.1 (4)
O3—K1—O4i148.5 (2)O2—Ti1—O289.7 (4)
O3—K1—O392.1 (2)O2—Ti1—O1iii172.5 (4)
O3—K1—O2102.0 (2)O2—Ti1—O1i83.0 (3)
O3—K1—O457.5 (2)O2—Ti1—O289.7 (4)
O3—K1—O2i80.7 (3)O1ii—Ti1—O283.0 (3)
O3—K1—O4i82.1 (2)O1ii—Ti1—O1iii95.4 (3)
O3—K1—O392.1 (2)O1ii—Ti1—O1i95.4 (3)
O2—K1—O444.5 (2)O1ii—Ti1—O2172.5 (4)
O2—K1—O2i87.2 (3)O2—Ti1—O1iii92.1 (4)
O2—K1—O4i130.8 (3)O2—Ti1—O1i172.5 (4)
O2—K1—O3164.4 (2)O2—Ti1—O289.7 (4)
O4—K1—O2i82.3 (2)O1iii—Ti1—O1i95.4 (3)
O4—K1—O4i118.9 (2)O1iii—Ti1—O283.0 (3)
O4—K1—O3148.5 (2)O1i—Ti1—O292.1 (4)
O2i—K1—O4i44.5 (2)O4—Er2—O391.6 (3)
O2i—K1—O3102.0 (2)O4—Er2—O3iv87.7 (3)
O4i—K1—O357.5 (2)O4—Er2—O486.1 (4)
O1—K2—O259.4 (2)O4—Er2—O3173.5 (3)
O1—K2—O499.8 (2)O4—Er2—O486.1 (4)
O1—K2—O2157.1 (2)O3—Er2—O3iv94.4 (3)
O1—K2—O4151.6 (2)O3—Er2—O4173.5 (3)
O1—K2—O197.7 (2)O3—Er2—O394.4 (3)
O1—K2—O1i97.7 (2)O3—Er2—O487.7 (3)
O1—K2—O286.1 (2)O3iv—Er2—O491.6 (3)
O1—K2—O4101.9 (2)O3iv—Er2—O394.4 (3)
O2—K2—O445.9 (2)O3iv—Er2—O4173.5 (3)
O2—K2—O2114.8 (2)O4—Er2—O387.7 (3)
O2—K2—O499.7 (3)O4—Er2—O486.1 (4)
O2—K2—O186.1 (2)O3—Er2—O491.6 (3)
O2—K2—O1i157.1 (2)O4—Ti2—O391.6 (3)
O2—K2—O2114.8 (2)O4—Ti2—O3iv87.7 (3)
O2—K2—O486.4 (2)O4—Ti2—O486.1 (4)
O4—K2—O286.4 (2)O4—Ti2—O3173.5 (3)
O4—K2—O454.7 (2)O4—Ti2—O486.1 (4)
O4—K2—O1101.9 (2)O3—Ti2—O3iv94.4 (3)
O4—K2—O1i151.6 (2)O3—Ti2—O4173.5 (3)
O4—K2—O299.7 (3)O3—Ti2—O394.4 (3)
O4—K2—O454.7 (2)O3—Ti2—O487.7 (3)
O2—K2—O445.9 (2)O3iv—Ti2—O491.6 (3)
O2—K2—O159.4 (2)O3iv—Ti2—O394.4 (3)
O2—K2—O1i86.1 (2)O3iv—Ti2—O4173.5 (3)
O2—K2—O2114.8 (2)O4—Ti2—O387.7 (3)
O2—K2—O499.7 (3)O4—Ti2—O486.1 (4)
O4—K2—O199.8 (2)O3—Ti2—O491.6 (3)
O4—K2—O1i101.9 (2)O1—P—O2109.5 (5)
O4—K2—O286.4 (2)O1—P—O3111.3 (4)
O4—K2—O454.7 (2)O1—P—O4109.7 (5)
O1—K2—O1i97.7 (2)O2—P—O3110.3 (5)
O1—K2—O2157.1 (2)O2—P—O4106.0 (5)
O1—K2—O4151.6 (2)O3—P—O4110.0 (5)
Symmetry codes: (i) z, x+1/2, y+1/2; (ii) x, y+1/2, z+1/2; (iii) y, z+1/2, x+1/2; (iv) y, z, x.
(KYbTP) top
Crystal data top
K2YbTiP3O12Dx = 3.772 Mg m3
Mr = 584.03Mo Kα radiation, λ = 0.71073 Å
Cubic, P213Cell parameters from 24 reflections
Hall symbol: P 2ac 2ab 3θ = 24.0–29.8°
a = 10.0939 (8) ŵ = 11.16 mm1
V = 1028.4 (2) Å3T = 293 K
Z = 4Tetrahedron, colourless
F(000) = 10840.04 × 0.03 × 0.03 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
904 reflections with F2 > 2σ(F2)
Radiation source: Fine-focus sealed tubeRint = 0.063
Graphite monochromatorθmax = 29.9°, θmin = 3.5°
ω–2θ scansh = 140
Absorption correction: analytical
(Alcock, 1974)
k = 1414
Tmin = 0.687, Tmax = 0.753l = 1414
6213 measured reflections3 standard reflections every 120 min
1008 independent reflections intensity decay: none
Refinement top
Refinement on F29 constraints
Least-squares matrix: full w = 1/[σ2(Fsqd) + 0.045(Fsqd)2]
R[F2 > 2σ(F2)] = 0.022(Δ/σ)max = 0.000041
wR(F2) = 0.066Δρmax = 1.28 e Å3
S = 1.08Δρmin = 0.93 e Å3
1008 reflectionsAbsolute structure: Flack (1983) parameter refined
60 parametersAbsolute structure parameter: 0.00 (3)
0 restraints
Crystal data top
K2YbTiP3O12Z = 4
Mr = 584.03Mo Kα radiation
Cubic, P213µ = 11.16 mm1
a = 10.0939 (8) ÅT = 293 K
V = 1028.4 (2) Å30.04 × 0.03 × 0.03 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
904 reflections with F2 > 2σ(F2)
Absorption correction: analytical
(Alcock, 1974)
Rint = 0.063
Tmin = 0.687, Tmax = 0.7533 standard reflections every 120 min
6213 measured reflections intensity decay: none
1008 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0220 restraints
wR(F2) = 0.066Δρmax = 1.28 e Å3
S = 1.08Δρmin = 0.93 e Å3
1008 reflectionsAbsolute structure: Flack (1983) parameter refined
60 parametersAbsolute structure parameter: 0.00 (3)
Special details top

Refinement. The following constraints were used during the refinement:

H-atom parameters constrained x(Ti1)=0.0 + 1.0*x(Yb1) H-atom parameters constrained u11(Ti1)=0.0 + 1.0*u11(Yb1) H-atom parameters constrained u12(Ti1)=0.0 + 1.0*u12(Yb1) H-atom parameters constrained x(Ti2)=0.0 + 1.0*x(Yb2) H-atom parameters constrained u11(Ti2)=0.0 + 1.0*u11(Yb2) H-atom parameters constrained u12(Ti2)=0.0 + 1.0*u12(Yb2) H-atom parameters constrained pop(Ti1)=1.0–1.0*pop(Yb1) H-atom parameters constrained pop(Ti2)=0.0 + 1.0*pop(Yb1) H-atom parameters constrained pop(Yb2)=1.0–1.0*pop(Yb1)

No restraints used.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
K10.0454 (2)0.5454 (2)0.0454 (2)0.0315 (7)
K20.18045 (16)0.31955 (16)0.18045 (16)0.0250 (5)
Yb10.16699 (3)0.66699 (3)0.33301 (3)0.0116 (2)0.643 (3)
Ti10.16699 (3)0.66699 (3)0.33301 (3)0.0116 (2)0.357 (3)
Yb20.39847 (5)0.60153 (5)0.10153 (5)0.0106 (3)0.357 (3)
Ti20.39847 (5)0.60153 (5)0.10153 (5)0.0106 (3)0.643 (3)
P0.12740 (17)0.48538 (19)0.28995 (18)0.0178 (8)
O10.0972 (7)0.3469 (7)0.2412 (7)0.041 (4)
O20.0051 (8)0.5704 (10)0.2720 (8)0.056 (5)
O30.1694 (7)0.4856 (7)0.4354 (7)0.038 (3)
O40.2364 (8)0.5474 (9)0.2076 (9)0.057 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
K10.0315 (7)0.0315 (7)0.0315 (7)0.0010 (7)0.0010 (7)0.0010 (7)
K20.0250 (5)0.0250 (5)0.0250 (5)0.0021 (6)0.0021 (6)0.0021 (6)
Yb10.0116 (2)0.0116 (2)0.0116 (2)0.0052 (4)0.0052 (4)0.0052 (4)
Ti10.0116 (2)0.0116 (2)0.0116 (2)0.0052 (4)0.0052 (4)0.0052 (4)
Yb20.0106 (3)0.0106 (3)0.0106 (3)0.0006 (5)0.0006 (5)0.0006 (5)
Ti20.0106 (3)0.0106 (3)0.0106 (3)0.0006 (5)0.0006 (5)0.0006 (5)
P0.0144 (7)0.0201 (8)0.0188 (8)0.0016 (6)0.0030 (6)0.0005 (6)
O10.042 (4)0.042 (4)0.040 (3)0.012 (3)0.004 (3)0.018 (3)
O20.041 (4)0.075 (6)0.051 (4)0.036 (4)0.005 (4)0.017 (5)
O30.037 (3)0.050 (4)0.028 (3)0.005 (4)0.013 (3)0.007 (3)
O40.048 (5)0.054 (5)0.069 (6)0.011 (4)0.037 (4)0.004 (4)
Geometric parameters (Å, º) top
K1—K23.949 (3)Yb1—O22.085 (8)
K1—O23.240 (9)Ti1—O22.085 (8)
K1—O43.199 (9)Ti1—O1ii2.087 (7)
K1—O32.902 (7)Ti1—O22.085 (8)
K1—O32.902 (7)Ti1—O1iii2.087 (7)
K1—O23.240 (9)Ti1—O1i2.087 (7)
K1—O43.199 (9)Ti1—O22.085 (8)
K1—O2i3.240 (9)Yb2—O42.030 (8)
K1—O4i3.199 (9)Yb2—O32.014 (7)
K1—O32.902 (7)Yb2—O3iv2.014 (7)
K2—O12.882 (8)Yb2—O42.030 (8)
K2—O23.112 (9)Yb2—O32.014 (7)
K2—O43.023 (9)Yb2—O42.030 (8)
K2—O23.112 (9)Ti2—O42.030 (8)
K2—O43.023 (9)Ti2—O32.014 (7)
K2—O12.882 (8)Ti2—O3iv2.014 (7)
K2—O1i2.882 (8)Ti2—O42.030 (8)
K2—O23.112 (9)Ti2—O32.014 (7)
K2—O43.023 (9)Ti2—O42.030 (8)
Yb1—O22.085 (8)P—O11.513 (8)
Yb1—O1ii2.087 (7)P—O21.515 (9)
Yb1—O22.085 (8)P—O31.528 (7)
Yb1—O1iii2.087 (7)P—O41.514 (9)
Yb1—O1i2.087 (7)
O2—K1—O444.4 (2)O1i—K2—O259.4 (2)
O2—K1—O3101.5 (2)O1i—K2—O4100.9 (2)
O2—K1—O3164.2 (2)O2—K2—O446.7 (2)
O2—K1—O287.9 (2)O2—Yb1—O1ii91.1 (3)
O2—K1—O4131.2 (2)O2—Yb1—O289.7 (3)
O2—K1—O2i87.9 (2)O2—Yb1—O1iii173.0 (3)
O2—K1—O4i81.9 (2)O2—Yb1—O1i83.4 (3)
O2—K1—O379.9 (2)O2—Yb1—O289.7 (3)
O4—K1—O357.1 (2)O1ii—Yb1—O283.4 (3)
O4—K1—O3148.9 (2)O1ii—Yb1—O1iii95.9 (3)
O4—K1—O281.9 (2)O1ii—Yb1—O1i95.9 (3)
O4—K1—O4118.8 (2)O1ii—Yb1—O2173.0 (3)
O4—K1—O2i131.2 (2)O2—Yb1—O1iii91.1 (3)
O4—K1—O4i118.8 (2)O2—Yb1—O1i173.0 (3)
O4—K1—O382.4 (2)O2—Yb1—O289.7 (3)
O3—K1—O392.8 (2)O1iii—Yb1—O1i95.9 (3)
O3—K1—O279.9 (2)O1iii—Yb1—O283.4 (3)
O3—K1—O482.4 (2)O1i—Yb1—O291.1 (3)
O3—K1—O2i164.2 (2)O2—Ti1—O1ii91.1 (3)
O3—K1—O4i148.9 (2)O2—Ti1—O289.7 (3)
O3—K1—O392.8 (2)O2—Ti1—O1iii173.0 (3)
O3—K1—O2101.5 (2)O2—Ti1—O1i83.4 (3)
O3—K1—O457.1 (2)O2—Ti1—O289.7 (3)
O3—K1—O2i79.9 (2)O1ii—Ti1—O283.4 (3)
O3—K1—O4i82.4 (2)O1ii—Ti1—O1iii95.9 (3)
O3—K1—O392.8 (2)O1ii—Ti1—O1i95.9 (3)
O2—K1—O444.4 (2)O1ii—Ti1—O2173.0 (3)
O2—K1—O2i87.9 (2)O2—Ti1—O1iii91.1 (3)
O2—K1—O4i131.2 (2)O2—Ti1—O1i173.0 (3)
O2—K1—O3164.2 (2)O2—Ti1—O289.7 (3)
O4—K1—O2i81.9 (2)O1iii—Ti1—O1i95.9 (3)
O4—K1—O4i118.8 (2)O1iii—Ti1—O283.4 (3)
O4—K1—O3148.9 (2)O1i—Ti1—O291.1 (3)
O2i—K1—O4i44.4 (2)O4—Yb2—O392.7 (3)
O2i—K1—O3101.5 (2)O4—Yb2—O3iv87.1 (3)
O4i—K1—O357.1 (2)O4—Yb2—O486.2 (4)
O1—K2—O259.4 (2)O4—Yb2—O3173.2 (3)
O1—K2—O4100.9 (2)O4—Yb2—O486.2 (4)
O1—K2—O2157.1 (2)O3—Yb2—O3iv93.9 (3)
O1—K2—O4151.6 (2)O3—Yb2—O4173.2 (3)
O1—K2—O197.7 (2)O3—Yb2—O393.9 (3)
O1—K2—O1i97.7 (2)O3—Yb2—O487.1 (3)
O1—K2—O285.6 (2)O3iv—Yb2—O492.7 (3)
O1—K2—O4100.8 (2)O3iv—Yb2—O393.9 (3)
O2—K2—O446.7 (2)O3iv—Yb2—O4173.2 (3)
O2—K2—O2115.0 (2)O4—Yb2—O387.1 (3)
O2—K2—O4100.7 (2)O4—Yb2—O486.2 (4)
O2—K2—O185.6 (2)O3—Yb2—O492.7 (3)
O2—K2—O1i157.1 (2)O4—Ti2—O392.7 (3)
O2—K2—O2115.0 (2)O4—Ti2—O3iv87.1 (3)
O2—K2—O485.5 (2)O4—Ti2—O486.2 (4)
O4—K2—O285.5 (2)O4—Ti2—O3173.2 (3)
O4—K2—O454.6 (2)O4—Ti2—O486.2 (4)
O4—K2—O1100.8 (2)O3—Ti2—O3iv93.9 (3)
O4—K2—O1i151.6 (2)O3—Ti2—O4173.2 (3)
O4—K2—O2100.7 (2)O3—Ti2—O393.9 (3)
O4—K2—O454.6 (2)O3—Ti2—O487.1 (3)
O2—K2—O446.7 (2)O3iv—Ti2—O492.7 (3)
O2—K2—O159.4 (2)O3iv—Ti2—O393.9 (3)
O2—K2—O1i85.6 (2)O3iv—Ti2—O4173.2 (3)
O2—K2—O2115.0 (2)O4—Ti2—O387.1 (3)
O2—K2—O4100.7 (2)O4—Ti2—O486.2 (4)
O4—K2—O1100.9 (2)O3—Ti2—O492.7 (3)
O4—K2—O1i100.8 (2)O1—P—O2108.7 (5)
O4—K2—O285.5 (2)O1—P—O3111.7 (4)
O4—K2—O454.6 (2)O1—P—O4110.5 (5)
O1—K2—O1i97.7 (2)O2—P—O3109.9 (4)
O1—K2—O2157.1 (2)O2—P—O4107.0 (5)
O1—K2—O4151.6 (2)O3—P—O4109.0 (4)
Symmetry codes: (i) z, x+1/2, y+1/2; (ii) x, y+1/2, z+1/2; (iii) y, z+1/2, x+1/2; (iv) y, z, x.
(KYTP) top
Crystal data top
K2YTiP3O12Dx = 3.192 Mg m3
Mr = 499.89Mo Kα radiation, λ = 0.71073 Å
Cubic, P213Cell parameters from 18 reflections
Hall symbol: P 2ac 2ab 3θ = 7.5–17.3°
a = 10.1318 (6) ŵ = 7.65 mm1
V = 1040.06 (11) Å3T = 293 K
Z = 4Tetrahedron, colourless
F(000) = 9600.02 × 0.01 × 0.01 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
701 reflections with F2 > 2σ(F2)
Radiation source: Fine-focus sealed tubeRint = 0.107
Graphite monochromatorθmax = 29.9°, θmin = 3.5°
ω–2θ scansh = 140
Absorption correction: analytical
(Alcock, 1974)
k = 140
Tmin = 0.917, Tmax = 0.933l = 1414
3303 measured reflections3 standard reflections every 120 min
1014 independent reflections intensity decay: none
Refinement top
Refinement on F29 constraints
Least-squares matrix: full w = 1/[σ2(Fsqd) + 0.025(Fsqd)2]
R[F2 > 2σ(F2)] = 0.047(Δ/σ)max = 0.000038
wR(F2) = 0.180Δρmax = 1.65 e Å3
S = 1.19Δρmin = 2.22 e Å3
1014 reflectionsAbsolute structure: Flack (1983) parameter refined
60 parametersAbsolute structure parameter: 0.10 (5)
0 restraints
Crystal data top
K2YTiP3O12Z = 4
Mr = 499.89Mo Kα radiation
Cubic, P213µ = 7.65 mm1
a = 10.1318 (6) ÅT = 293 K
V = 1040.06 (11) Å30.02 × 0.01 × 0.01 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
701 reflections with F2 > 2σ(F2)
Absorption correction: analytical
(Alcock, 1974)
Rint = 0.107
Tmin = 0.917, Tmax = 0.9333 standard reflections every 120 min
3303 measured reflections intensity decay: none
1014 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0470 restraints
wR(F2) = 0.180Δρmax = 1.65 e Å3
S = 1.19Δρmin = 2.22 e Å3
1014 reflectionsAbsolute structure: Flack (1983) parameter refined
60 parametersAbsolute structure parameter: 0.10 (5)
Special details top

Refinement. The following constraints were used during the refinement:

H-atom parameters constrained x(Ti1)=0.0 + 1.0*x(Y1) H-atom parameters constrained u11(Ti1)=0.0 + 1.0*u11(Y1) H-atom parameters constrained u12(Ti1)=0.0 + 1.0*u12(Y1) H-atom parameters constrained x(Ti2)=0.0 + 1.0*x(Y2) H-atom parameters constrained u11(Ti2)=0.0 + 1.0*u11(Y2) H-atom parameters constrained u12(Ti2)=0.0 + 1.0*u12(Y2) H-atom parameters constrained pop(Ti1)=1.0–1.0*pop(Y1) H-atom parameters constrained pop(Ti2)=0.0 + 1.0*pop(Y1) H-atom parameters constrained pop(Y2)=1.0–1.0*pop(Y1)

No restraints used.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
K10.2048 (4)0.7048 (4)0.7952 (4)0.0317 (13)
K20.4309 (3)0.9309 (3)0.5691 (3)0.0266 (11)
Y10.08346 (14)0.91654 (14)0.41654 (14)0.0141 (8)0.614 (18)
Ti10.08346 (14)0.91654 (14)0.41654 (14)0.0141 (8)0.386 (18)
Y20.14820 (15)0.35180 (15)0.64820 (15)0.0127 (9)0.386 (18)
Ti20.14820 (15)0.35180 (15)0.64820 (15)0.0127 (9)0.614 (18)
P0.2659 (4)0.6239 (3)0.4618 (4)0.0209 (17)
O10.4027 (15)0.6537 (16)0.5101 (15)0.052 (8)
O20.182 (2)0.7454 (15)0.4782 (16)0.062 (10)
O30.2653 (14)0.5810 (13)0.3180 (13)0.042 (7)
O40.2050 (18)0.5188 (18)0.546 (2)0.067 (11)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
K10.0317 (13)0.0317 (13)0.0317 (13)0.0008 (14)0.0008 (14)0.0008 (14)
K20.0266 (11)0.0266 (11)0.0266 (11)0.0034 (12)0.0034 (12)0.0034 (12)
Y10.0141 (8)0.0141 (8)0.0141 (8)0.0044 (17)0.0044 (17)0.0044 (17)
Ti10.0141 (8)0.0141 (8)0.0141 (8)0.0044 (17)0.0044 (17)0.0044 (17)
Y20.0127 (9)0.0127 (9)0.0127 (9)0.0006 (18)0.0006 (18)0.0006 (18)
Ti20.0127 (9)0.0127 (9)0.0127 (9)0.0006 (18)0.0006 (18)0.0006 (18)
P0.0248 (18)0.0168 (16)0.0211 (17)0.0011 (13)0.0007 (13)0.0013 (13)
O10.045 (8)0.061 (9)0.049 (8)0.022 (7)0.018 (6)0.005 (7)
O20.090 (13)0.031 (7)0.063 (10)0.031 (8)0.020 (9)0.000 (7)
O30.050 (8)0.040 (7)0.037 (7)0.006 (6)0.011 (5)0.014 (6)
O40.064 (11)0.057 (10)0.080 (12)0.015 (9)0.012 (9)0.044 (9)
Geometric parameters (Å, º) top
K1—K23.969 (5)Y1—O12.100 (15)
K1—O23.246 (17)Ti1—O22.097 (16)
K1—O43.15 (2)Ti1—O12.100 (15)
K1—O32.921 (14)Ti1—O12.100 (15)
K1—O32.921 (14)Ti1—O22.097 (16)
K1—O23.246 (17)Ti1—O22.097 (16)
K1—O43.15 (2)Ti1—O12.100 (15)
K1—O23.246 (17)Y2—O42.066 (18)
K1—O43.15 (2)Y2—O32.047 (14)
K1—O32.921 (14)Y2—O42.066 (18)
K2—O12.886 (17)Y2—O32.047 (14)
K2—O23.146 (19)Y2—O3i2.047 (14)
K2—O43.054 (19)Y2—O42.066 (18)
K2—O12.886 (17)Ti2—O42.066 (18)
K2—O23.146 (19)Ti2—O32.047 (14)
K2—O43.054 (19)Ti2—O42.066 (18)
K2—O23.146 (19)Ti2—O32.047 (14)
K2—O43.054 (19)Ti2—O3i2.047 (14)
K2—O12.886 (17)Ti2—O42.066 (18)
Y1—O22.097 (16)P—O11.501 (16)
Y1—O12.100 (15)P—O21.504 (17)
Y1—O12.100 (15)P—O31.520 (14)
Y1—O22.097 (16)P—O41.497 (19)
Y1—O22.097 (16)
O2—K1—O444.2 (4)O2—K2—O445.7 (5)
O2—K1—O3102.2 (4)O2—K2—O159.7 (4)
O2—K1—O380.6 (5)O4—K2—O1100.0 (5)
O2—K1—O287.3 (4)O2—Y1—O191.7 (7)
O2—K1—O481.7 (5)O2—Y1—O182.6 (6)
O2—K1—O287.3 (5)O2—Y1—O289.7 (7)
O2—K1—O4130.4 (5)O2—Y1—O289.7 (7)
O2—K1—O3164.2 (4)O2—Y1—O1172.2 (7)
O4—K1—O358.0 (4)O1—Y1—O196.1 (6)
O4—K1—O382.5 (4)O1—Y1—O2172.2 (7)
O4—K1—O2130.4 (5)O1—Y1—O282.6 (6)
O4—K1—O4118.6 (5)O1—Y1—O196.1 (6)
O4—K1—O281.7 (5)O1—Y1—O291.7 (7)
O4—K1—O4118.6 (5)O1—Y1—O2172.2 (7)
O4—K1—O3149.0 (5)O1—Y1—O196.1 (6)
O3—K1—O391.9 (4)O2—Y1—O289.7 (7)
O3—K1—O2164.2 (4)O2—Y1—O182.6 (6)
O3—K1—O4149.0 (5)O2—Y1—O191.7 (7)
O3—K1—O280.6 (5)O2—Ti1—O191.7 (7)
O3—K1—O482.5 (4)O2—Ti1—O182.6 (6)
O3—K1—O391.9 (4)O2—Ti1—O289.7 (7)
O3—K1—O2102.2 (4)O2—Ti1—O289.7 (7)
O3—K1—O458.0 (4)O2—Ti1—O1172.2 (7)
O3—K1—O2164.2 (4)O1—Ti1—O196.1 (6)
O3—K1—O4149.0 (5)O1—Ti1—O2172.2 (7)
O3—K1—O391.9 (4)O1—Ti1—O282.6 (6)
O2—K1—O444.2 (4)O1—Ti1—O196.1 (6)
O2—K1—O287.3 (4)O1—Ti1—O291.7 (7)
O2—K1—O481.7 (5)O1—Ti1—O2172.2 (7)
O2—K1—O380.6 (5)O1—Ti1—O196.1 (6)
O4—K1—O2130.4 (5)O2—Ti1—O289.7 (7)
O4—K1—O4118.6 (5)O2—Ti1—O182.6 (6)
O4—K1—O382.5 (4)O2—Ti1—O191.7 (7)
O2—K1—O444.2 (4)O4—Y2—O391.7 (7)
O2—K1—O3102.2 (4)O4—Y2—O487.5 (7)
O4—K1—O358.0 (4)O4—Y2—O3174.6 (7)
O1—K2—O259.7 (4)O4—Y2—O3i87.1 (6)
O1—K2—O4100.0 (5)O4—Y2—O487.5 (7)
O1—K2—O197.2 (4)O3—Y2—O487.1 (6)
O1—K2—O285.7 (4)O3—Y2—O393.6 (5)
O1—K2—O4101.5 (5)O3—Y2—O3i93.6 (5)
O1—K2—O2156.9 (4)O3—Y2—O4174.6 (7)
O1—K2—O4152.7 (5)O4—Y2—O391.7 (7)
O1—K2—O197.2 (4)O4—Y2—O3i174.6 (7)
O2—K2—O445.7 (5)O4—Y2—O487.5 (7)
O2—K2—O1156.9 (4)O3—Y2—O3i93.6 (5)
O2—K2—O2115.0 (4)O3—Y2—O487.1 (6)
O2—K2—O486.7 (5)O3i—Y2—O491.7 (7)
O2—K2—O2115.0 (4)O4—Ti2—O391.7 (7)
O2—K2—O4100.5 (5)O4—Ti2—O487.5 (7)
O2—K2—O185.7 (4)O4—Ti2—O3174.6 (7)
O4—K2—O1152.7 (5)O4—Ti2—O3i87.1 (6)
O4—K2—O2100.5 (5)O4—Ti2—O487.5 (7)
O4—K2—O455.8 (5)O3—Ti2—O487.1 (6)
O4—K2—O286.7 (5)O3—Ti2—O393.6 (5)
O4—K2—O455.8 (5)O3—Ti2—O3i93.6 (5)
O4—K2—O1101.5 (5)O3—Ti2—O4174.6 (7)
O1—K2—O259.7 (4)O4—Ti2—O391.7 (7)
O1—K2—O4100.0 (5)O4—Ti2—O3i174.6 (7)
O1—K2—O285.7 (4)O4—Ti2—O487.5 (7)
O1—K2—O4101.5 (5)O3—Ti2—O3i93.6 (5)
O1—K2—O197.2 (4)O3—Ti2—O487.1 (6)
O2—K2—O445.7 (5)O3i—Ti2—O491.7 (7)
O2—K2—O2115.0 (4)O1—P—O2108.7 (10)
O2—K2—O486.7 (5)O1—P—O3112.0 (8)
O2—K2—O1156.9 (4)O1—P—O4109.7 (10)
O4—K2—O2100.5 (5)O2—P—O3109.7 (9)
O4—K2—O455.8 (5)O2—P—O4106.6 (10)
O4—K2—O1152.7 (5)O3—P—O4109.9 (9)
Symmetry code: (i) z, x, y.
(KCrTP) top
Crystal data top
K2CrTiP3O12Dx = 3.267 Mg m3
Mr = 462.98Mo Kα radiation, λ = 0.71073 Å
Cubic, P213Cell parameters from 23 reflections
Hall symbol: P 2ac 2ab 3θ = 31.3–34.9°
a = 9.8001 (2) ŵ = 3.47 mm1
V = 941.22 (4) Å3T = 293 K
Z = 4Tetrahedron, green
F(000) = 9000.09 × 0.09 × 0.07 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
1346 reflections with F2 > 2σ(F2)
Radiation source: Fine-focus sealed tubeRint = 0.027
Graphite monochromatorθmax = 35.0°, θmin = 3.6°
ω–2θ scansh = 150
Absorption correction: analytical
(Alcock, 1974)
k = 150
Tmin = 0.759, Tmax = 0.813l = 1515
4496 measured reflections3 standard reflections every 120 min
1394 independent reflections intensity decay: none
Refinement top
Refinement on F2 w = 1/[σ2(Fsqd) + 0.0035(Fsqd)2]
Least-squares matrix: full(Δ/σ)max = 0.00016
R[F2 > 2σ(F2)] = 0.016Δρmax = 0.42 e Å3
wR(F2) = 0.052Δρmin = 0.47 e Å3
S = 1.05Extinction correction: Isotropic Gaussian, Zachariasen, 1967; Larson (1970), Eq22 p292 "Cryst. Comp." Munksgaard 1970
1394 reflectionsExtinction coefficient: 114 (19) × 102
61 parametersAbsolute structure: Flack (1983) parameter refined
0 restraintsAbsolute structure parameter: 0.02 (2)
9 constraints
Crystal data top
K2CrTiP3O12Z = 4
Mr = 462.98Mo Kα radiation
Cubic, P213µ = 3.47 mm1
a = 9.8001 (2) ÅT = 293 K
V = 941.22 (4) Å30.09 × 0.09 × 0.07 mm
Data collection top
Enraf-Nonius CAD-4
diffractometer
1346 reflections with F2 > 2σ(F2)
Absorption correction: analytical
(Alcock, 1974)
Rint = 0.027
Tmin = 0.759, Tmax = 0.8133 standard reflections every 120 min
4496 measured reflections intensity decay: none
1394 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0160 restraints
wR(F2) = 0.052Δρmax = 0.42 e Å3
S = 1.05Δρmin = 0.47 e Å3
1394 reflectionsAbsolute structure: Flack (1983) parameter refined
61 parametersAbsolute structure parameter: 0.02 (2)
Special details top

Refinement. The following constraints were used during the refinement:

H-atom parameters constrained x(Ti1)=0.0 + 1.0*x(Cr1) H-atom parameters constrained u11(Ti1)=0.0 + 1.0*u11(Cr1) H-atom parameters constrained u12(Ti1)=0.0 + 1.0*u12(Cr1) H-atom parameters constrained x(Ti2)=0.0 + 1.0*x(Cr2) H-atom parameters constrained u11(Ti2)=0.0 + 1.0*u11(Cr2) H-atom parameters constrained u12(Ti2)=0.0 + 1.0*u12(Cr2) H-atom parameters constrained pop(Ti1)=1.0–1.0*pop(Cr1) H-atom parameters constrained pop(Ti2)=0.0 + 1.0*pop(Cr1) H-atom parameters constrained pop(Cr2)=1.0–1.0*pop(Cr1)

No restraints used.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
K10.04267 (6)0.54267 (6)0.04267 (6)0.02127 (17)
K20.18241 (5)0.31759 (5)0.18241 (5)0.01717 (15)
Cr10.16346 (3)0.66346 (3)0.33654 (3)0.00506 (11)0.388 (17)
Ti10.16346 (3)0.66346 (3)0.33654 (3)0.00506 (11)0.612 (17)
Cr20.39336 (3)0.60664 (3)0.10664 (3)0.00519 (11)0.612 (17)
Ti20.39336 (3)0.60664 (3)0.10664 (3)0.00519 (11)0.388 (17)
P0.12393 (4)0.47720 (4)0.29292 (4)0.00488 (17)
O10.10088 (16)0.32849 (14)0.25110 (16)0.0121 (5)
O20.01088 (15)0.55333 (16)0.27003 (17)0.0136 (6)
O30.17127 (15)0.48624 (14)0.44146 (14)0.0106 (5)
O40.22865 (15)0.54768 (15)0.20204 (15)0.0131 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
K10.02127 (17)0.02127 (17)0.02127 (17)0.00006 (17)0.00006 (17)0.00006 (17)
K20.01717 (15)0.01717 (15)0.01717 (15)0.00182 (13)0.00182 (13)0.00182 (13)
Cr10.00506 (11)0.00506 (11)0.00506 (11)0.0002 (2)0.0002 (2)0.0002 (2)
Ti10.00506 (11)0.00506 (11)0.00506 (11)0.0002 (2)0.0002 (2)0.0002 (2)
Cr20.00519 (11)0.00519 (11)0.00519 (11)0.0006 (2)0.0006 (2)0.0006 (2)
Ti20.00519 (11)0.00519 (11)0.00519 (11)0.0006 (2)0.0006 (2)0.0006 (2)
P0.00481 (16)0.00516 (16)0.00468 (17)0.00033 (12)0.00082 (12)0.00012 (12)
O10.0163 (6)0.0066 (5)0.0134 (5)0.0002 (5)0.0022 (5)0.0042 (4)
O20.0102 (5)0.0151 (6)0.0157 (6)0.0079 (5)0.0002 (5)0.0002 (5)
O30.0134 (5)0.0131 (6)0.0051 (5)0.0037 (5)0.0010 (4)0.0005 (4)
O40.0130 (6)0.0154 (6)0.0109 (5)0.0055 (5)0.0060 (4)0.0008 (5)
Geometric parameters (Å, º) top
K1—K23.8205 (7)Cr1—O21.9559 (15)
K1—O23.1108 (17)Ti1—O21.9559 (15)
K1—O43.0126 (16)Ti1—O1ii1.9312 (14)
K1—O32.8220 (15)Ti1—O21.9559 (15)
K1—O32.8220 (15)Ti1—O1iii1.9312 (14)
K1—O23.1108 (17)Ti1—O1i1.9312 (14)
K1—O43.0126 (16)Ti1—O21.9559 (15)
K1—O2i3.1108 (17)Cr2—O41.9528 (15)
K1—O4i3.0126 (16)Cr2—O31.9622 (14)
K1—O32.8220 (15)Cr2—O3iv1.9622 (14)
K2—O12.8588 (16)Cr2—O41.9528 (15)
K2—O22.9834 (16)Cr2—O31.9622 (14)
K2—O42.9128 (16)Cr2—O41.9528 (15)
K2—O42.9128 (16)Ti2—O41.9528 (15)
K2—O12.8588 (16)Ti2—O31.9622 (14)
K2—O22.9834 (16)Ti2—O3iv1.9622 (14)
K2—O1i2.8588 (16)Ti2—O41.9528 (15)
K2—O2i2.9834 (16)Ti2—O31.9622 (14)
K2—O42.9128 (16)Ti2—O41.9528 (15)
Cr1—O21.9559 (15)P—O11.5307 (14)
Cr1—O1ii1.9312 (14)P—O21.5338 (15)
Cr1—O21.9559 (15)P—O31.5304 (14)
Cr1—O1iii1.9312 (14)P—O41.5244 (16)
Cr1—O1i1.9312 (14)
O2—K1—O446.95 (4)O1i—K2—O2i49.92 (4)
O2—K1—O3103.02 (4)O1i—K2—O495.36 (4)
O2—K1—O3163.71 (5)O2i—K2—O4132.77 (5)
O2—K1—O282.68 (4)O2—Cr1—O1ii94.08 (6)
O2—K1—O4128.72 (4)O2—Cr1—O290.96 (7)
O2—K1—O2i82.68 (4)O2—Cr1—O1iii172.52 (7)
O2—K1—O4i82.04 (4)O2—Cr1—O1i83.44 (7)
O2—K1—O382.94 (4)O2—Cr1—O290.96 (7)
O4—K1—O356.25 (4)O1ii—Cr1—O283.44 (7)
O4—K1—O3148.28 (5)O1ii—Cr1—O1iii91.99 (6)
O4—K1—O282.04 (4)O1ii—Cr1—O1i91.99 (6)
O4—K1—O4118.99 (4)O1ii—Cr1—O2172.52 (7)
O4—K1—O2i128.72 (4)O2—Cr1—O1iii94.08 (7)
O4—K1—O4i118.99 (4)O2—Cr1—O1i172.52 (6)
O4—K1—O382.56 (4)O2—Cr1—O290.96 (7)
O3—K1—O392.89 (4)O1iii—Cr1—O1i91.99 (6)
O3—K1—O282.94 (4)O1iii—Cr1—O283.44 (7)
O3—K1—O482.56 (4)O1i—Cr1—O294.08 (7)
O3—K1—O2i163.71 (4)O2—Ti1—O1ii94.08 (6)
O3—K1—O4i148.28 (5)O2—Ti1—O290.96 (7)
O3—K1—O392.89 (4)O2—Ti1—O1iii172.52 (7)
O3—K1—O2103.02 (4)O2—Ti1—O1i83.44 (7)
O3—K1—O456.25 (4)O2—Ti1—O290.96 (7)
O3—K1—O2i82.94 (4)O1ii—Ti1—O283.44 (7)
O3—K1—O4i82.56 (4)O1ii—Ti1—O1iii91.99 (6)
O3—K1—O392.89 (4)O1ii—Ti1—O1i91.99 (6)
O2—K1—O446.95 (4)O1ii—Ti1—O2172.52 (7)
O2—K1—O2i82.68 (4)O2—Ti1—O1iii94.08 (7)
O2—K1—O4i128.72 (4)O2—Ti1—O1i172.52 (6)
O2—K1—O3163.71 (4)O2—Ti1—O290.96 (7)
O4—K1—O2i82.04 (4)O1iii—Ti1—O1i91.99 (6)
O4—K1—O4i118.99 (4)O1iii—Ti1—O283.44 (7)
O4—K1—O3148.28 (5)O1i—Ti1—O294.08 (7)
O2i—K1—O4i46.95 (4)O4—Cr2—O389.48 (6)
O2i—K1—O3103.02 (4)O4—Cr2—O3iv89.13 (6)
O4i—K1—O356.25 (4)O4—Cr2—O489.46 (6)
O1—K2—O249.92 (4)O4—Cr2—O3178.24 (7)
O1—K2—O495.36 (4)O4—Cr2—O489.46 (6)
O1—K2—O4149.29 (5)O3—Cr2—O3iv91.91 (6)
O1—K2—O1101.61 (4)O3—Cr2—O4178.24 (6)
O1—K2—O252.51 (4)O3—Cr2—O391.91 (6)
O1—K2—O1i101.61 (4)O3—Cr2—O489.13 (6)
O1—K2—O2i116.16 (5)O3iv—Cr2—O489.48 (6)
O1—K2—O499.76 (4)O3iv—Cr2—O391.91 (6)
O2—K2—O4132.77 (5)O3iv—Cr2—O4178.24 (7)
O2—K2—O4140.17 (4)O4—Cr2—O389.13 (6)
O2—K2—O1116.16 (5)O4—Cr2—O489.46 (6)
O2—K2—O287.06 (4)O3—Cr2—O489.48 (6)
O2—K2—O1i52.51 (4)O4—Ti2—O389.48 (6)
O2—K2—O2i87.06 (4)O4—Ti2—O3iv89.13 (6)
O2—K2—O494.48 (4)O4—Ti2—O489.46 (6)
O4—K2—O456.30 (4)O4—Ti2—O3178.24 (7)
O4—K2—O199.76 (4)O4—Ti2—O489.46 (6)
O4—K2—O294.48 (4)O3—Ti2—O3iv91.91 (6)
O4—K2—O1i149.29 (5)O3—Ti2—O4178.24 (6)
O4—K2—O2i140.17 (4)O3—Ti2—O391.91 (6)
O4—K2—O456.30 (4)O3—Ti2—O489.13 (6)
O4—K2—O195.36 (4)O3iv—Ti2—O489.48 (6)
O4—K2—O2132.77 (5)O3iv—Ti2—O391.91 (6)
O4—K2—O1i99.76 (4)O3iv—Ti2—O4178.24 (7)
O4—K2—O2i94.48 (4)O4—Ti2—O389.13 (6)
O4—K2—O456.30 (4)O4—Ti2—O489.46 (6)
O1—K2—O249.92 (4)O3—Ti2—O489.48 (6)
O1—K2—O1i101.61 (4)O1—P—O2107.27 (9)
O1—K2—O2i52.51 (4)O1—P—O3110.76 (8)
O1—K2—O4149.29 (4)O1—P—O4111.98 (8)
O2—K2—O1i116.16 (5)O2—P—O3111.85 (8)
O2—K2—O2i87.06 (4)O2—P—O4105.90 (9)
O2—K2—O4140.17 (4)O3—P—O4108.99 (8)
Symmetry codes: (i) z, x+1/2, y+1/2; (ii) x, y+1/2, z+1/2; (iii) y, z+1/2, x+1/2; (iv) y, z, x.

Experimental details

(KErTP)(KYbTP)(KYTP)(KCrTP)
Crystal data
Chemical formulaK2ErTiP3O12K2YbTiP3O12K2YTiP3O12K2CrTiP3O12
Mr578.25584.03499.89462.98
Crystal system, space groupCubic, P213Cubic, P213Cubic, P213Cubic, P213
Temperature (K)293293293293
a (Å)10.1053 (2) 10.0939 (8) 10.1318 (6) 9.8001 (2)
V3)1031.92 (4)1028.4 (2)1040.06 (11)941.22 (4)
Z4444
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)10.1911.167.653.47
Crystal size (mm)0.06 × 0.06 × 0.050.04 × 0.03 × 0.030.02 × 0.01 × 0.010.09 × 0.09 × 0.07
Data collection
DiffractometerEnraf-Nonius CAD-4
diffractometer
Enraf-Nonius CAD-4
diffractometer
Enraf-Nonius CAD-4
diffractometer
Enraf-Nonius CAD-4
diffractometer
Absorption correctionAnalytical
(Alcock, 1974)
Analytical
(Alcock, 1974)
Analytical
(Alcock, 1974)
Analytical
(Alcock, 1974)
Tmin, Tmax0.567, 0.6500.687, 0.7530.917, 0.9330.759, 0.813
No. of measured, independent and
observed [F2 > 2σ(F2)] reflections
3285, 1008, 967 6213, 1008, 904 3303, 1014, 701 4496, 1394, 1346
Rint0.0480.0630.1070.027
(sin θ/λ)max1)0.7020.7020.7010.807
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.023, 0.077, 1.06 0.022, 0.066, 1.08 0.047, 0.180, 1.19 0.016, 0.052, 1.05
No. of reflections1008100810141394
No. of parameters61606061
Δρmax, Δρmin (e Å3)0.60, 0.761.28, 0.931.65, 2.220.42, 0.47
Absolute structureFlack (1983) parameter refinedFlack (1983) parameter refinedFlack (1983) parameter refinedFlack (1983) parameter refined
Absolute structure parameter0.04 (3)0.00 (3)0.10 (5)0.02 (2)

Computer programs: CAD-4 Software (Enraf-Nonius, 1989), Xtal3.71 (Hall et al., 2000) program: LATCON, Xtal3.71 (Hall et al., 2000) programs: DIFDAT; SORTRF; ADDREF; ABSORB, SHELXS97 (Sheldrick, 1997), Xtal3.71 (Hall et al., 2000) program: CRYLSQ, Xtal3.71 (Hall et al., 2000) programs: BONDLA; ATABLE; CIFIO.

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