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Ammonium di­(zinc, gallium) bis­(phosphate), (NH4)(Zn,Ga)2(PO4)2, has a zeolite-like open-framework structure. It contains channels of four- and eight-membered rings of alternating tetrahedra of (Zn,Ga)O4 (Zn:Ga ≃ 1:1) and PO4, in which the tetrahedra are connected via corners. The NH4+ cations are located in the channels and provide weak hydrogen bonds to the framework O atoms. The average (Zn,Ga)—O bond lengths of the two non-equivalent (Zn,Ga)O4 tetrahedra are 1.863 and 1.870 Å. All atoms are in general positions. The compound is isostructural with K(CoII,Al)2(PO4)2 and [(NH4)x(NH3)0.5−x]CoxAl1−xPO4 (x = 0.38). Single-crystal Raman and IR spectra are discussed.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680200870X/br6049sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680200870X/br6049Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](P-O) = 0.002 Å
  • R factor = 0.023
  • wR factor = 0.059
  • Data-to-parameter ratio = 17.5

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_420 Alert C D-H Without Acceptor N - H(1) ? General Notes
FORMU_01 There is a discrepancy between the atom counts in the _chemical_formula_sum and _chemical_formula_moiety. This is usually due to the moiety formula being in the wrong format. Atom count from _chemical_formula_sum: H4 Ga1 N1 O8 P2 Zn1 Atom count from _chemical_formula_moiety: ABSTM_02 When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.904 Tmax scaled 0.465 Tmin scaled 0.328
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Computing details top

Data collection: COLLECT (Nonius, 2001); cell refinement: HKL SCALEPACK (Otwinowski & Minor, 1997); data reduction: HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ATOMS (Shape Software, 1999); software used to prepare material for publication: SHELXL97.

Ammonium di(zinc,gallium) diphosphate top
Crystal data top
(NH4)(Zn·Ga)2(PO4)2F(000) = 1328
Mr = 343.07Dx = 2.921 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 2331 reflections
a = 13.370 (3) Åθ = 2.3–30.0°
b = 13.190 (3) ŵ = 6.95 mm1
c = 8.998 (2) ÅT = 150 K
β = 100.46 (3)°Fragment, colourless
V = 1560.4 (6) Å30.18 × 0.11 × 0.11 mm
Z = 8
Data collection top
Nonius KappaCCD
diffractometer
2287 independent reflections
Radiation source: fine-focus sealed tube2207 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.011
ω scansθmax = 30.0°, θmin = 2.2°
Absorption correction: multi-scan
(HKL SCALEPACK; Otwinowski & Minor, 1997)
h = 1818
Tmin = 0.363, Tmax = 0.515k = 1818
4483 measured reflectionsl = 1212
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.023Only H-atom coordinates refined
wR(F2) = 0.059 w = 1/[σ2(Fo2) + (0.011P)2 + 9.80P]
where P = (Fo2 + 2Fc2)/3
S = 1.18(Δ/σ)max = 0.001
2287 reflectionsΔρmax = 1.00 e Å3
131 parametersΔρmin = 0.59 e Å3
4 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00097 (13)
Special details top

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. H atoms were constrained to have a Uiso of 0.05 Å2. N—H distances were restrained to a length of 0.9 (5) Å.

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Zn10.37042 (2)0.05625 (2)0.11547 (3)0.01214 (9)0.50
Ga10.37042 (2)0.05625 (2)0.11547 (3)0.01214 (9)0.50
Zn20.58004 (2)0.37567 (2)0.06484 (3)0.01230 (9)0.50
Ga20.58004 (2)0.37567 (2)0.06484 (3)0.01230 (9)0.50
P10.35211 (5)0.43822 (5)0.08472 (7)0.01297 (13)
P20.57660 (5)0.13577 (5)0.04242 (7)0.01139 (13)
O10.6526 (2)0.4051 (3)0.2552 (3)0.0491 (8)
O20.63921 (17)0.44698 (16)0.0795 (3)0.0257 (5)
O30.24507 (15)0.10156 (17)0.0141 (3)0.0251 (5)
O40.43892 (16)0.38788 (17)0.0219 (3)0.0293 (5)
O50.36881 (19)0.0803 (2)0.3189 (3)0.0358 (6)
O60.61803 (19)0.24192 (17)0.0297 (4)0.0370 (6)
O70.46198 (15)0.14235 (15)0.0414 (2)0.0203 (4)
O80.40204 (17)0.07976 (17)0.0977 (2)0.0228 (4)
N0.3244 (2)0.2490 (3)0.2222 (3)0.0294 (6)
H10.294 (4)0.302 (3)0.250 (6)0.050*
H20.265 (3)0.217 (4)0.221 (6)0.050*
H30.357 (4)0.222 (4)0.287 (5)0.050*
H40.371 (3)0.270 (4)0.157 (5)0.050*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.00842 (13)0.01667 (15)0.01109 (14)0.00092 (9)0.00113 (9)0.00309 (10)
Ga10.00842 (13)0.01667 (15)0.01109 (14)0.00092 (9)0.00113 (9)0.00309 (10)
Zn20.00988 (14)0.01168 (14)0.01535 (15)0.00052 (9)0.00234 (10)0.00154 (10)
Ga20.00988 (14)0.01168 (14)0.01535 (15)0.00052 (9)0.00234 (10)0.00154 (10)
P10.0091 (3)0.0163 (3)0.0129 (3)0.0022 (2)0.0002 (2)0.0046 (2)
P20.0103 (3)0.0106 (3)0.0135 (3)0.0002 (2)0.0029 (2)0.0010 (2)
O10.0523 (18)0.073 (2)0.0190 (11)0.0085 (16)0.0003 (11)0.0202 (13)
O20.0287 (11)0.0188 (10)0.0332 (12)0.0043 (8)0.0155 (9)0.0028 (9)
O30.0132 (9)0.0209 (10)0.0374 (12)0.0020 (7)0.0059 (8)0.0065 (9)
O40.0111 (9)0.0226 (10)0.0549 (15)0.0019 (8)0.0083 (9)0.0048 (10)
O50.0272 (12)0.0629 (18)0.0187 (10)0.0208 (12)0.0079 (9)0.0154 (11)
O60.0267 (12)0.0148 (10)0.075 (2)0.0065 (9)0.0246 (12)0.0068 (11)
O70.0134 (9)0.0175 (9)0.0311 (11)0.0003 (7)0.0066 (8)0.0027 (8)
O80.0274 (11)0.0249 (10)0.0176 (9)0.0034 (8)0.0083 (8)0.0005 (8)
N0.0212 (13)0.0418 (17)0.0259 (14)0.0028 (12)0.0059 (10)0.0108 (12)
Geometric parameters (Å, º) top
Zn1—O31.855 (2)O2—P1v1.520 (2)
Zn1—O81.857 (2)O2—Niv3.250 (4)
Zn1—O51.862 (2)O2—Niii4.501 (4)
Zn1—O71.878 (2)O3—P1i1.528 (2)
Zn1—Ni3.900 (3)O3—Ni2.980 (4)
Zn1—N3.923 (3)O3—N3.200 (4)
Zn1—Nii4.364 (3)O4—N3.050 (4)
Zn2—O11.850 (3)O4—Ni4.604 (4)
Zn2—O41.863 (2)O5—P2vi1.514 (2)
Zn2—O61.878 (2)O5—Ni3.418 (5)
Zn2—O21.889 (2)O5—Nii4.391 (5)
Zn2—Niii3.843 (3)O6—Niv3.005 (4)
Zn2—Niv3.920 (3)O6—Niii3.221 (4)
Zn2—N4.236 (3)O6—N4.163 (4)
Zn2—Nv5.243 (3)O7—N3.067 (4)
P1—O1vi1.517 (3)O7—Niv4.623 (4)
P1—O2v1.520 (2)O7—Ni4.649 (4)
P1—O3i1.528 (2)O8—P2viii1.532 (2)
P1—O41.532 (2)O8—Nii3.049 (4)
P1—N3.691 (3)O8—Nviii4.258 (4)
P1—Ni3.775 (3)N—O3i2.980 (4)
P1—Nvii4.518 (4)N—O6iv3.005 (4)
P2—O5vi1.514 (2)N—O1ix3.045 (4)
P2—O61.518 (2)N—O8x3.049 (4)
P2—O8viii1.532 (2)N—O6ix3.221 (4)
P2—O71.533 (2)N—O2iv3.250 (4)
P2—Niv3.698 (3)N—O5i3.418 (5)
P2—Niii3.902 (3)N—P2iv3.698 (3)
P2—N4.044 (3)N—H10.82 (4)
O1—P1vi1.517 (3)N—H20.90 (4)
O1—Niii3.045 (4)N—H30.86 (4)
O1—Nv4.587 (5)N—H40.83 (4)
O1—Nvi4.639 (4)
O3—Zn1—O8117.93 (10)O6iv—N—O7118.67 (12)
O3—Zn1—O5104.93 (12)O1ix—N—O794.87 (12)
O8—Zn1—O5107.04 (12)O8x—N—O782.01 (10)
O3—Zn1—O7102.69 (10)O4—N—O764.30 (9)
O8—Zn1—O7112.36 (9)O3i—N—O378.82 (10)
O5—Zn1—O7111.72 (10)O6iv—N—O3139.82 (13)
O1—Zn2—O4121.02 (13)O1ix—N—O345.76 (8)
O1—Zn2—O6103.92 (14)O8x—N—O395.41 (11)
O4—Zn2—O6109.93 (10)O4—N—O394.03 (11)
O1—Zn2—O2108.50 (13)O7—N—O355.40 (8)
O4—Zn2—O2110.42 (11)O3i—N—O6ix94.91 (10)
O6—Zn2—O2101.07 (11)O6iv—N—O6ix72.14 (10)
O1vi—P1—O2v109.44 (17)O1ix—N—O6ix55.82 (8)
O1vi—P1—O3i106.02 (16)O8x—N—O6ix89.44 (10)
O2v—P1—O3i112.69 (13)O4—N—O6ix137.02 (13)
O1vi—P1—O4113.00 (17)O7—N—O6ix150.63 (13)
O2v—P1—O4110.67 (13)O3—N—O6ix97.93 (10)
O3i—P1—O4104.92 (13)O3i—N—O2iv84.73 (11)
O5vi—P2—O6112.32 (17)O6iv—N—O2iv55.26 (8)
O5vi—P2—O8viii108.13 (14)O1ix—N—O2iv133.32 (12)
O6—P2—O8viii104.93 (14)O8x—N—O2iv101.35 (10)
O5vi—P2—O7111.32 (13)O4—N—O2iv78.86 (10)
O6—P2—O7108.99 (12)O7—N—O2iv131.65 (11)
O8viii—P2—O7110.97 (13)O3—N—O2iv162.54 (12)
O3i—N—O6iv139.45 (14)O6ix—N—O2iv77.53 (10)
O3i—N—O1ix99.58 (12)O3i—N—O5i54.35 (8)
O6iv—N—O1ix103.53 (12)O6iv—N—O5i95.39 (11)
O3i—N—O8x173.19 (14)O1ix—N—O5i84.08 (11)
O6iv—N—O8x47.08 (7)O8x—N—O5i131.40 (11)
O1ix—N—O8x78.55 (11)O4—N—O5i92.59 (10)
O3i—N—O447.43 (7)O7—N—O5i144.95 (11)
O6iv—N—O4120.14 (12)O3—N—O5i104.08 (10)
O1ix—N—O4136.30 (13)O6ix—N—O5i44.46 (7)
O8x—N—O4130.34 (12)O2iv—N—O5i60.81 (8)
O3i—N—O791.67 (10)
O4—Zn2—O1—P1vi1.3 (5)O8—Zn1—O3—P1i2.7 (3)
O6—Zn2—O1—P1vi122.6 (4)O5—Zn1—O3—P1i116.3 (3)
O2—Zn2—O1—P1vi130.4 (4)O7—Zn1—O3—P1i126.8 (2)
Symmetry codes: (i) x+1/2, y+1/2, z; (ii) x, y, z+1/2; (iii) x+1/2, y+1/2, z+1/2; (iv) x+1, y, z1/2; (v) x+1, y+1, z; (vi) x+1, y, z+1/2; (vii) x, y+1, z+1/2; (viii) x+1, y, z; (ix) x1/2, y+1/2, z1/2; (x) x, y, z1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N—H2···O1ix0.90 (4)2.19 (4)3.045 (4)160 (5)
N—H3···O6iv0.86 (4)2.28 (4)3.005 (4)141 (4)
N—H3···O8x0.86 (4)2.28 (4)3.049 (4)148 (4)
N—H4···O40.83 (4)2.30 (4)3.050 (4)151 (5)
Symmetry codes: (iv) x+1, y, z1/2; (ix) x1/2, y+1/2, z1/2; (x) x, y, z1/2.
 

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