Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536810045198/bt5401sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536810045198/bt5401Isup2.hkl |
Key indicators
- Single-crystal X-ray study
- T = 293 K
- Mean (La-Cl) = 0.003 Å
- R factor = 0.059
- wR factor = 0.142
- Data-to-parameter ratio = 37.5
checkCIF/PLATON results
No syntax errors found
Alert level A PLAT029_ALERT_3_A _diffrn_measured_fraction_theta_full Low ....... 0.92
Alert level B PLAT774_ALERT_1_B Suspect X-Y Bond in CIF: K -- K .. 4.34 Ang. PLAT774_ALERT_1_B Suspect X-Y Bond in CIF: K -- LA .. 4.39 Ang. PLAT774_ALERT_1_B Suspect X-Y Bond in CIF: K -- K .. 4.43 Ang. PLAT774_ALERT_1_B Suspect X-Y Bond in CIF: K -- K .. 4.48 Ang. PLAT774_ALERT_1_B Suspect X-Y Bond in CIF: LA -- K .. 4.39 Ang. PLAT774_ALERT_1_B Suspect X-Y Bond in CIF: LA -- K .. 4.39 Ang.
Alert level C REFLT03_ALERT_3_C Reflection count < 95% complete From the CIF: _diffrn_reflns_theta_max 32.98 From the CIF: _diffrn_reflns_theta_full 32.93 From the CIF: _reflns_number_total 1650 TEST2: Reflns within _diffrn_reflns_theta_max Count of symmetry unique reflns 1796 Completeness (_total/calc) 91.87% RINTA01_ALERT_3_C The value of Rint is greater than 0.12 Rint given 0.139 PLAT910_ALERT_3_C Missing # of FCF Reflections Below Th(Min) ..... 2 PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 35 PLAT913_ALERT_3_C Missing # of Very Strong Reflections in FCF .... 1 PLAT048_ALERT_1_C MoietyFormula Not Given ........................ ? PLAT194_ALERT_1_C Missing _cell_measurement_reflns_used datum .... ? PLAT912_ALERT_4_C Missing # of FCF Reflections Above STh/L= 0.600 49 PLAT922_ALERT_1_C wR2 * 100.0 in the CIF and FCF Differ by ....... -0.42 PLAT923_ALERT_1_C S values in the CIF and FCF Differ by ....... 0.02 PLAT927_ALERT_1_C Reported and Calculated wR2 * 100.0 Differ by . -0.43 PLAT951_ALERT_1_C Reported and Calculated Kmax Values Differ by .. 2
Alert level G REFLT03_ALERT_1_G ALERT: Expected hkl max differ from CIF values From the CIF: _diffrn_reflns_theta_max 32.98 From the CIF: _reflns_number_total 1650 From the CIF: _diffrn_reflns_limit_ max hkl 19. 11. 12. From the CIF: _diffrn_reflns_limit_ min hkl -19. -11. -12. TEST1: Expected hkl limits for theta max Calculated maximum hkl 19. 13. 12. Calculated minimum hkl -19. -13. -12. PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature 293 K PLAT764_ALERT_4_G Overcomplete CIF Bond List Detected (Rep/Expd) . 5.14 Ratio PLAT794_ALERT_5_G Note: Tentative Bond Valency for La ....... 3.02
1 ALERT level A = In general: serious problem 6 ALERT level B = Potentially serious problem 12 ALERT level C = Check and explain 5 ALERT level G = General alerts; check 15 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 6 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
# start Validation Reply Form _vrf_PLAT029_I ; PROBLEM: _diffrn_measured_fraction_theta_full Low ....... 0.92 RESPONSE: ... ;
1 ALERT level A = Data missing that is essential or data in wrong format 0 ALERT level G = General alerts. Data that may be required is missing
Colourless, transparent, brick-shaped single crystals of K2LaCl5 were obtained as by-product from the reaction of potassium azide (KN3), lanthanum (La), the corresponding sesquioxide (La2O3) and trichloride (LaCl3) in the presence of KCl as flux with the purpose to synthesize K2La4ONCl9. The mixture was transferred into a torch-sealed, evacuated, fused silica vessel, heated at 1123 K for seven days, followed by cooling to room temperature within 24 h.
The ternary rare-earth metal(III) halide K2LaCl5 (Fig. 1) belongs to the A2MX5 series (A = NH4, In, Na – Cs; M = La – Dy; X = Cl – I) (Meyer & Hüttl, 1983; Meyer et al., 1985; Wickleder & Meyer 1995). It can be described as ordered structural variety of U3Ch5 (Ch = S and Se) or the low-temperature phase of Yb5Sb3, respectively, as anti-isotypical arrangement. While the K+ cations have eight contacts to Cl- anions (Fig. 2), the La3+ cations are surrounded by only seven of them. In both cases distorted mono- or bicapped trigonal prisms [LaCl7]4– or [KCl8]7– originate. For the lanthanum bearing ones they are linked via common edges and form chains, which run along [010] (Fig. 3). Together with the chloride anions (Cl1)-, (Cl2)– and (Cl3)-, La3+ occupies the 4c position and shows the site symmetry m, while the (Cl4)- anion and the K+ cation are located at the 8d position with the site symmetry 1.
For the U3Ch5-type structure (Ch = S and Se) and its relationship to Y2HfS5, see: Moseley et al. (1972); Potel et al. (1972); Jeitschko & Donohue (1975). For the low-temperature phase of Yb5Sb3, see: Brunton & Steinfink (1971). For the series of the ternary rare-earth metal(III) halides with A = NH4, In, Na – Cs; M = La – Dy; X = Cl – I, see: Meyer & Hüttl (1983); Meyer et al. (1985); Wickleder & Meyer (1995).
Data collection: DIF4 (Stoe & Cie, 1992); cell refinement: DIF4 (Stoe & Cie, 1992); data reduction: REDU4 (Stoe & Cie, 1992); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).
K2LaCl5 | F(000) = 720 |
Mr = 394.36 | Dx = 2.893 Mg m−3 |
Orthorhombic, Pnma | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2n | θ = 3.4–33.0° |
a = 12.7402 (8) Å | µ = 7.02 mm−1 |
b = 8.8635 (6) Å | T = 293 K |
c = 8.0174 (5) Å | Bricks, colourless |
V = 905.35 (10) Å3 | 0.33 × 0.28 × 0.24 mm |
Z = 4 |
Stoe IPDS-I diffractometer | 1650 independent reflections |
Radiation source: fine-focus sealed tube | 872 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.139 |
imaging plate detector system scans | θmax = 33.0°, θmin = 3.4° |
Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1999) | h = −19→19 |
Tmin = 0.106, Tmax = 0.185 | k = −11→11 |
12421 measured reflections | l = −12→12 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.059 | w = 1/[σ2(Fo2) + (0.0799P)2] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.142 | (Δ/σ)max = 0.004 |
S = 0.90 | Δρmax = 1.58 e Å−3 |
1650 reflections | Δρmin = −2.64 e Å−3 |
44 parameters | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.0094 (12) |
K2LaCl5 | V = 905.35 (10) Å3 |
Mr = 394.36 | Z = 4 |
Orthorhombic, Pnma | Mo Kα radiation |
a = 12.7402 (8) Å | µ = 7.02 mm−1 |
b = 8.8635 (6) Å | T = 293 K |
c = 8.0174 (5) Å | 0.33 × 0.28 × 0.24 mm |
Stoe IPDS-I diffractometer | 1650 independent reflections |
Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1999) | 872 reflections with I > 2σ(I) |
Tmin = 0.106, Tmax = 0.185 | Rint = 0.139 |
12421 measured reflections |
R[F2 > 2σ(F2)] = 0.059 | 44 parameters |
wR(F2) = 0.142 | 0 restraints |
S = 0.90 | Δρmax = 1.58 e Å−3 |
1650 reflections | Δρmin = −2.64 e Å−3 |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s 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 > σ(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. |
x | y | z | Uiso*/Ueq | ||
K | 0.67125 (15) | 0.4946 (3) | 0.5481 (3) | 0.0379 (5) | |
La | 0.50680 (5) | 0.2500 | 0.07776 (8) | 0.0248 (2) | |
Cl1 | −0.0065 (2) | 0.7500 | 0.9311 (4) | 0.0310 (6) | |
Cl2 | 0.7911 (2) | 0.2500 | 0.3299 (4) | 0.0333 (7) | |
Cl3 | 0.6828 (2) | 0.2500 | 0.8662 (4) | 0.0374 (8) | |
Cl4 | 0.57990 (17) | 0.5441 (3) | 0.1663 (3) | 0.0342 (5) |
U11 | U22 | U33 | U12 | U13 | U23 | |
K | 0.0381 (10) | 0.0363 (14) | 0.0393 (11) | 0.0014 (8) | −0.0014 (7) | −0.0070 (9) |
La | 0.0286 (3) | 0.0234 (4) | 0.0222 (3) | 0.000 | 0.0022 (3) | 0.000 |
Cl1 | 0.0347 (13) | 0.0354 (17) | 0.0228 (11) | 0.000 | 0.0016 (12) | 0.000 |
Cl2 | 0.0282 (13) | 0.039 (2) | 0.0322 (15) | 0.000 | 0.0006 (11) | 0.000 |
Cl3 | 0.0368 (15) | 0.045 (2) | 0.0308 (15) | 0.000 | 0.0088 (12) | 0.000 |
Cl4 | 0.0460 (12) | 0.0267 (13) | 0.0301 (10) | −0.0030 (9) | −0.0102 (8) | 0.0025 (8) |
K—Cl1i | 3.160 (3) | La—Cl4x | 2.895 (2) |
K—Cl2 | 3.177 (3) | La—Kvi | 4.389 (2) |
K—Cl1ii | 3.206 (3) | La—Kxi | 4.389 (2) |
K—Cl2iii | 3.234 (3) | Cl1—Laxii | 2.833 (3) |
K—Cl3iv | 3.272 (4) | Cl1—Kxii | 3.160 (3) |
K—Cl4 | 3.304 (3) | Cl1—Kxiii | 3.160 (3) |
K—Cl4iii | 3.327 (3) | Cl1—Kxiv | 3.206 (3) |
K—Cl3 | 3.351 (4) | Cl1—Kxv | 3.206 (3) |
K—Kv | 4.336 (5) | Cl2—Laxvi | 2.845 (3) |
K—Lavi | 4.389 (2) | Cl2—Kv | 3.177 (3) |
K—Kvi | 4.432 (4) | Cl2—Kxvii | 3.234 (3) |
K—Kiii | 4.4838 (18) | Cl2—Kiv | 3.234 (3) |
La—Cl3vii | 2.812 (3) | Cl3—Laxviii | 2.812 (3) |
La—Cl1i | 2.833 (3) | Cl3—Kiii | 3.272 (4) |
La—Cl2viii | 2.845 (3) | Cl3—Kxix | 3.272 (3) |
La—Cl4 | 2.858 (2) | Cl3—Kv | 3.351 (4) |
La—Cl4v | 2.858 (2) | Cl4—Lax | 2.895 (2) |
La—Cl4ix | 2.895 (2) | Cl4—Kiv | 3.327 (3) |
Cl1i—K—Cl2 | 71.80 (8) | Cl3vii—La—Cl4 | 83.68 (6) |
Cl1i—K—Cl1ii | 91.76 (5) | Cl1i—La—Cl4 | 75.64 (5) |
Cl2—K—Cl1ii | 148.21 (10) | Cl2viii—La—Cl4 | 104.48 (5) |
Cl1i—K—Cl2iii | 141.81 (10) | Cl3vii—La—Cl4v | 83.68 (6) |
Cl2—K—Cl2iii | 142.29 (7) | Cl1i—La—Cl4v | 75.64 (5) |
Cl1ii—K—Cl2iii | 64.80 (8) | Cl2viii—La—Cl4v | 104.48 (5) |
Cl1i—K—Cl3iv | 136.03 (10) | Cl4—La—Cl4v | 131.62 (9) |
Cl2—K—Cl3iv | 87.34 (7) | Cl3vii—La—Cl4ix | 84.06 (7) |
Cl1ii—K—Cl3iv | 86.34 (8) | Cl1i—La—Cl4ix | 132.50 (6) |
Cl2iii—K—Cl3iv | 75.11 (8) | Cl2viii—La—Cl4ix | 78.89 (7) |
Cl1i—K—Cl4 | 65.30 (7) | Cl4—La—Cl4ix | 150.15 (6) |
Cl2—K—Cl4 | 75.52 (8) | Cl4v—La—Cl4ix | 73.58 (7) |
Cl1ii—K—Cl4 | 72.88 (8) | Cl3vii—La—Cl4x | 84.06 (7) |
Cl2iii—K—Cl4 | 127.34 (10) | Cl1i—La—Cl4x | 132.50 (6) |
Cl3iv—K—Cl4 | 72.27 (8) | Cl2viii—La—Cl4x | 78.89 (7) |
Cl1i—K—Cl4iii | 130.30 (10) | Cl4—La—Cl4x | 73.58 (7) |
Cl2—K—Cl4iii | 68.18 (8) | Cl4v—La—Cl4x | 150.15 (6) |
Cl1ii—K—Cl4iii | 136.98 (9) | Cl4ix—La—Cl4x | 78.15 (9) |
Cl2iii—K—Cl4iii | 74.46 (8) | Cl3vii—La—Kvi | 145.53 (4) |
Cl3iv—K—Cl4iii | 69.93 (8) | Cl1i—La—Kvi | 46.84 (5) |
Cl4—K—Cl4iii | 127.83 (9) | Cl2viii—La—Kvi | 47.41 (5) |
Cl1i—K—Cl3 | 79.12 (8) | Cl4—La—Kvi | 61.85 (6) |
Cl2—K—Cl3 | 87.50 (8) | Cl4v—La—Kvi | 117.97 (6) |
Cl1ii—K—Cl3 | 116.64 (9) | Cl4ix—La—Kvi | 126.15 (5) |
Cl2iii—K—Cl3 | 85.10 (7) | Cl4x—La—Kvi | 86.55 (6) |
Cl3iv—K—Cl3 | 139.63 (8) | Cl3vii—La—Kxi | 145.53 (4) |
Cl4—K—Cl3 | 143.76 (10) | Cl1i—La—Kxi | 46.84 (5) |
Cl4iii—K—Cl3 | 71.00 (8) | Cl2viii—La—Kxi | 47.41 (5) |
Cl1i—K—Kv | 46.68 (5) | Cl4—La—Kxi | 117.97 (6) |
Cl2—K—Kv | 46.96 (6) | Cl4v—La—Kxi | 61.85 (6) |
Cl1ii—K—Kv | 134.91 (5) | Cl4ix—La—Kxi | 86.55 (6) |
Cl2iii—K—Kv | 134.42 (6) | Cl4x—La—Kxi | 126.15 (6) |
Cl3iv—K—Kv | 133.77 (6) | Kvi—La—Kxi | 62.09 (7) |
Cl4—K—Kv | 97.63 (6) | Laxii—Cl1—Kxii | 107.21 (8) |
Cl4iii—K—Kv | 84.07 (6) | Laxii—Cl1—Kxiii | 107.21 (8) |
Cl3—K—Kv | 49.68 (5) | Kxii—Cl1—Kxiii | 86.64 (11) |
Cl1i—K—Lavi | 102.32 (7) | Laxii—Cl1—Kxiv | 93.04 (7) |
Cl2—K—Lavi | 167.59 (9) | Kxii—Cl1—Kxiv | 159.73 (10) |
Cl1ii—K—Lavi | 40.13 (5) | Kxiii—Cl1—Kxiv | 88.24 (5) |
Cl2iii—K—Lavi | 40.37 (6) | Laxii—Cl1—Kxv | 93.04 (7) |
Cl3iv—K—Lavi | 103.97 (7) | Kxii—Cl1—Kxv | 88.24 (5) |
Cl4—K—Lavi | 112.49 (7) | Kxiii—Cl1—Kxv | 159.73 (10) |
Cl4iii—K—Lavi | 110.55 (6) | Kxiv—Cl1—Kxv | 89.82 (11) |
Cl3—K—Lavi | 80.57 (6) | Laxvi—Cl2—Kv | 108.72 (9) |
Kv—K—Lavi | 121.04 (3) | Laxvi—Cl2—K | 108.72 (9) |
Cl1i—K—Kvi | 46.30 (6) | Kv—Cl2—K | 86.07 (11) |
Cl2—K—Kvi | 113.09 (10) | Laxvi—Cl2—Kxvii | 92.22 (8) |
Cl1ii—K—Kvi | 45.45 (6) | Kv—Cl2—Kxvii | 88.75 (3) |
Cl2iii—K—Kvi | 104.62 (9) | K—Cl2—Kxvii | 159.00 (11) |
Cl3iv—K—Kvi | 117.84 (10) | Laxvi—Cl2—Kiv | 92.22 (8) |
Cl4—K—Kvi | 59.28 (6) | Kv—Cl2—Kiv | 159.00 (11) |
Cl4iii—K—Kvi | 171.90 (11) | K—Cl2—Kiv | 88.75 (3) |
Cl3—K—Kvi | 100.93 (9) | Kxvii—Cl2—Kiv | 88.84 (11) |
Kv—K—Kvi | 91.23 (7) | Laxviii—Cl3—Kiii | 100.62 (8) |
Lavi—K—Kvi | 66.36 (5) | Laxviii—Cl3—Kxix | 100.62 (8) |
Cl1i—K—Kiii | 125.25 (10) | Kiii—Cl3—Kxix | 87.54 (11) |
Cl2—K—Kiii | 106.95 (10) | Laxviii—Cl3—K | 115.09 (9) |
Cl1ii—K—Kiii | 104.75 (8) | Kiii—Cl3—K | 85.21 (4) |
Cl2iii—K—Kiii | 45.10 (6) | Kxix—Cl3—K | 144.27 (10) |
Cl3iv—K—Kiii | 97.44 (9) | Laxviii—Cl3—Kv | 115.10 (9) |
Cl4—K—Kiii | 169.44 (11) | Kiii—Cl3—Kv | 144.27 (10) |
Cl4iii—K—Kiii | 47.24 (6) | Kxix—Cl3—Kv | 85.21 (4) |
Cl3—K—Kiii | 46.65 (6) | K—Cl3—Kv | 80.64 (10) |
Kv—K—Kiii | 91.22 (6) | La—Cl4—Lax | 106.42 (7) |
Lavi—K—Kiii | 67.00 (4) | La—Cl4—K | 102.93 (8) |
Kvi—K—Kiii | 126.56 (8) | Lax—Cl4—K | 147.62 (10) |
Cl3vii—La—Cl1i | 127.18 (9) | La—Cl4—Kiv | 98.37 (8) |
Cl3vii—La—Cl2viii | 157.97 (10) | Lax—Cl4—Kiv | 103.65 (8) |
Cl1i—La—Cl2viii | 74.85 (9) | K—Cl4—Kiv | 85.10 (6) |
Symmetry codes: (i) −x+1/2, −y+1, z−1/2; (ii) x+1/2, y, −z+3/2; (iii) −x+3/2, −y+1, z+1/2; (iv) −x+3/2, −y+1, z−1/2; (v) x, −y+1/2, z; (vi) −x+1, −y+1, −z+1; (vii) x, y, z−1; (viii) x−1/2, y, −z+1/2; (ix) −x+1, y−1/2, −z; (x) −x+1, −y+1, −z; (xi) −x+1, y−1/2, −z+1; (xii) −x+1/2, −y+1, z+1/2; (xiii) −x+1/2, y+1/2, z+1/2; (xiv) x−1/2, −y+3/2, −z+3/2; (xv) x−1/2, y, −z+3/2; (xvi) x+1/2, y, −z+1/2; (xvii) −x+3/2, y−1/2, z−1/2; (xviii) x, y, z+1; (xix) −x+3/2, y−1/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | K2LaCl5 |
Mr | 394.36 |
Crystal system, space group | Orthorhombic, Pnma |
Temperature (K) | 293 |
a, b, c (Å) | 12.7402 (8), 8.8635 (6), 8.0174 (5) |
V (Å3) | 905.35 (10) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 7.02 |
Crystal size (mm) | 0.33 × 0.28 × 0.24 |
Data collection | |
Diffractometer | Stoe IPDS-I |
Absorption correction | Numerical (X-SHAPE; Stoe & Cie, 1999) |
Tmin, Tmax | 0.106, 0.185 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12421, 1650, 872 |
Rint | 0.139 |
(sin θ/λ)max (Å−1) | 0.766 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.059, 0.142, 0.90 |
No. of reflections | 1650 |
No. of parameters | 44 |
Δρmax, Δρmin (e Å−3) | 1.58, −2.64 |
Computer programs: DIF4 (Stoe & Cie, 1992), REDU4 (Stoe & Cie, 1992), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 2006).
K—Cl1i | 3.160 (3) | La—Cl3v | 2.812 (3) |
K—Cl2 | 3.177 (3) | La—Cl1i | 2.833 (3) |
K—Cl1ii | 3.206 (3) | La—Cl2vi | 2.845 (3) |
K—Cl2iii | 3.234 (3) | La—Cl4 | 2.858 (2) |
K—Cl3iv | 3.272 (4) | La—Cl4vii | 2.858 (2) |
K—Cl4 | 3.304 (3) | La—Cl4viii | 2.895 (2) |
K—Cl4iii | 3.327 (3) | La—Cl4ix | 2.895 (2) |
K—Cl3 | 3.351 (4) |
Symmetry codes: (i) −x+1/2, −y+1, z−1/2; (ii) x+1/2, y, −z+3/2; (iii) −x+3/2, −y+1, z+1/2; (iv) −x+3/2, −y+1, z−1/2; (v) x, y, z−1; (vi) x−1/2, y, −z+1/2; (vii) x, −y+1/2, z; (viii) −x+1, y−1/2, −z; (ix) −x+1, −y+1, −z. |
The ternary rare-earth metal(III) halide K2LaCl5 (Fig. 1) belongs to the A2MX5 series (A = NH4, In, Na – Cs; M = La – Dy; X = Cl – I) (Meyer & Hüttl, 1983; Meyer et al., 1985; Wickleder & Meyer 1995). It can be described as ordered structural variety of U3Ch5 (Ch = S and Se) or the low-temperature phase of Yb5Sb3, respectively, as anti-isotypical arrangement. While the K+ cations have eight contacts to Cl- anions (Fig. 2), the La3+ cations are surrounded by only seven of them. In both cases distorted mono- or bicapped trigonal prisms [LaCl7]4– or [KCl8]7– originate. For the lanthanum bearing ones they are linked via common edges and form chains, which run along [010] (Fig. 3). Together with the chloride anions (Cl1)-, (Cl2)– and (Cl3)-, La3+ occupies the 4c position and shows the site symmetry m, while the (Cl4)- anion and the K+ cation are located at the 8d position with the site symmetry 1.