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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Nov 21;65(Pt 12):i91–i92. doi: 10.1107/S1600536809048788

The type IV polymorph of KEu(PO3)4

Abdelghani Oudahmane a, Mohamed Daoud a, Boumediene Tanouti a, Daniel Avignant b, Daniel Zambon b,*
PMCID: PMC2972142  PMID: 21578546

Abstract

Single crystals of KEu(PO3)4, potassium europium(III) polyphosphate, were obtained by solid-state reactions. This monoclinic form is the second polymorph described for this composition and belongs to type IV of long-chain polyphosphates with general formula A I B III(PO3)4. It is isotypic with its KEr(PO3)4 and KDy(PO3)4 homologues. The crystal structure is built of infinite helical chains of corner-sharing PO4 tetra­hedra with a repeating unit of eight tetra­hedra. These chains are further linked by isolated EuO8 square anti­prisms, forming a three-dimensional framework. The K+ ions are located in pseudo-hexa­gonal channels running along [Inline graphic01] and are surrounded by nine O atoms in a distorted environment.

Related literature

Besides crystals of the title compound, crystals of the type III polymorph (Hu et al., 1984)) have also been obtained. For isotypic AB(PO3)4 structures, where A is an alkali metal, Tl or NH4 +, and B is a rare earth element, see: Palkina et al. (1977) for TlNd; Maksimova et al. (1978) for RbNd; Dago et al. (1980) for KEr; Maksimova et al. (1981) for CsNd; Maksimova et al. (1982) for RbHo; Horchani et al. (2004) for RbEr; Rekik et al. (2004) for KGd; Naïli & Mhiri (2005) for CsGd; Ben Zarkouna et al. (2006) for (NH4)Gd; Khlissa & Férid (2006) for RbTb; Ettis et al. (2006) for RbGd; Chehimi-Moumen & Férid (2007) for KDy; Horchani-Naifer & Férid (2007) for CsPr; Zhu et al. (2009) for CsEu. For a review on the crystal chemisty of polyphosphates, see: Durif (1995). Jaouadi et al. (2003) have discussed the main crystal chemical characteristics of the seven AB(PO3)4 structure types. For applications of rare earth polyphosphates, see: Rashchi & Finch (2000); Barsukov et al. (2004). For general background, see: Porai-Koshits & Aslanov (1972). For ionic radii, see: Shannon (1976).

Experimental

Crystal data

  • KEu(PO3)4

  • M r = 506.94

  • Monoclinic, Inline graphic

  • a = 10.3723 (1) Å

  • b = 8.9721 (1) Å

  • c = 10.8320 (1) Å

  • β = 106.053 (1)°

  • V = 968.73 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 7.63 mm−1

  • T = 296 K

  • 0.12 × 0.11 × 0.10 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2008) T min = 0.466, T max = 0.513

  • 24299 measured reflections

  • 6201 independent reflections

  • 5023 reflections with I > 2σ(I)

  • R int = 0.045

Refinement

  • R[F 2 > 2σ(F 2)] = 0.030

  • wR(F 2) = 0.072

  • S = 1.04

  • 6201 reflections

  • 163 parameters

  • Δρmax = 1.72 e Å−3

  • Δρmin = −2.04 e Å−3

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809048788/wm2282sup1.cif

e-65-00i91-sup1.cif (17.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809048788/wm2282Isup2.hkl

e-65-00i91-Isup2.hkl (297.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

P1—O7 1.480 (2)
P1—O4i 1.483 (2)
P1—O12 1.588 (2)
P1—O3ii 1.5968 (19)
P2—O10iii 1.4795 (19)
P2—O5 1.483 (2)
P2—O11iii 1.6015 (18)
P2—O3iv 1.602 (2)
P3—O6 1.482 (2)
P3—O2 1.4873 (19)
P3—O11 1.6005 (19)
P3—O1 1.6033 (19)
P4—O9 1.4784 (19)
P4—O8v 1.484 (2)
P4—O1 1.601 (2)
P4—O12iii 1.601 (2)

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

supplementary crystallographic information

Comment

Rare earth polyphosphates are interesting materials and bear potential applications (Rashchi & Finch, 2000; Barsukov et al., 2004). The title compound is a member of a large family of polyphosphates with general formula AIBIII(PO3)4 (where AI is a monovalent cation: Li, Na, K, Rb, Cs, Tl, NH4, Ag and BIII is a trivalent cation: Ln,Y, Bi). It is now well known that these compounds are classified into seven structural types usually labelled by roman numerals from I to VII. A short recapitulation of the main crystal chemical characteristics of these seven structural types has recently been given by Jaouadi et al. (2003). The KEu(PO3)4 polymorph described in this article belongs to the IV structural type.

In the crystal structure the Eu3+ ion is eight-coordinated by the oxygen atoms and its 8-coordination polyhedron is better described as a square antiprism than a dodecahedron according to the criteria of Porai-Koshits & Aslanov (1972) (δ1 = 10.37°, δ2 = 10.85°, δ3 = 47.97°, δ4 = 53.54°). The Eu—O distances range from 2.3199 (19) Å to 2.4827 (19) Å with an average <Eu—O> distance of 2.399 Å that is slightly shorter than the sum of the ionic radii i.e. 2.466 Å (Shannon, 1976). The structure of this type IV polymorph is built of infinite helical chains of corner-sharing PO4 tetrahedra further linked by isolated EuO8 square antiprisms. The (PO3) chains exhibit a repeating unit of eight PO4 tetrahedra (Fig. 1) and are running along the [101] direction. The three-dimensional framework resulting from the edge-sharing between the PO4 tetrahedra and the EuO8 square antiprisms exhibits pseudo hexagonal channels where the K+ ions reside. The K+ ion is 9-coordinated by oxygen atoms with distances ranging from 2.789 (2) Å to 3.370 (3) Å. By sharing corners, the KO9 coordination polyhedra form corrugated chains running along the [010] direction (Fig. 2). Whereas the K atoms are separated by 6.599 (2) Å within the chain, the shortest K—K distance in the structure, 4.770 (2) Å, occurs between two adjacent (KO9) chains. This shortest distance corresponds to the separation between two K+ ions within the channels of the structure running along the [201] direction. This separation distance AIAI is strongly dependent on the nature of the AI element and decreases as the size of the AI element increases. For instance, in the AIGd(PO3)4 homologue series, where AI = K, Rb, Cs, this AIAI shortest distance varies from 4.801 Å for K to 4.211 Å for Cs (4.524 Å for Rb). For CsEu(PO3)4 the shortest Cs—Cs distance is equal to 4.237Å (Zhu et al. 2009).

For isotypic AB(PO3)4 structures, where A is an alkali metal, Tl or NH4+, and B is a rare earth element, see: Palkina et al. (1977) for TlNd, Maksimova et al. (1978) for RbNd, Dago et al. (1980) for KEr, Maksimova et al. (1981) for CsNd, Maksimova et al. (1982) for RbHo, Horchani et al. (2004) for RbEr, Rekik et al. (2004) for KGd, Naïli & Mhiri (2005) for CsGd, Ben Zarkouna et al. (2006) for (NH4)Gd, Khlissa & Férid (2006) for RbTb, Ettis et al. (2006) for RbGd, Chehimi-Moumen & Férid (2007) for KDy, Horchani-Naifer & Férid (2007) for CsPr, and Zhu et al. (2009) for CsEu. For a review on the crystal chemisty of polyphosphates, see: Durif (1995).

Experimental

Crystals of the title compound were synthesized by reacting Eu2O3 with (NH4)H2PO4 and K2CO3 in a platinum crucible. A mixture of these reagents in the molar ratio 34:57:9 was used for the synthesis. The mixture was heated at 473 K for 6 h, then at 573 K for 6 h and finally at 873 K for 24 h. The furnace was then cooled down first to 773 K at the rate of 2 K.h-1 and then to room temperature at the rate of K.h-1. Single crystals were extracted from the batch by washing with hot water. Besides crystals of the title compound, crystals of the type III polymorph (Hu et al., 1984)) have also been obtained.

Refinement

The highest residual peak in the final difference Fourier map was located 0.68 Å from atom Eu and the deepest hole was located 0.45 Å from atom K.

Figures

Fig. 1.

Fig. 1.

ORTEP-3 view of the repeating unit with eight PO4 tetrahedra, leading to helical (PO3)∞ chains. Displacement ellipsoids are drawn at the 50 % probability level. Symmetry codes: (a) -1/2+x, 3/2-y, 1/2+z; (b) -1+x, -1+y, z; (c) x, -1+y, 1+z; (d) -1+x, y, z; (e) -1/2+x, 1/2-y, 1/2+z; (f) 3-x, 1-y, 1-z; (g) 2-x, 1-y, 1-z; (h) 5/2-x, -1/2+y, 1/2-z; (i) -3/2+x, 1/2-y, -1/2+z; (j) 3/2-x, -1/2+y, 1/2-z; (k) 2-x, 1-y, -z.

Fig. 2.

Fig. 2.

Partial view of infinite chains of corner-sharing KO9 polyhedra.

Crystal data

KEu(PO3)4 F(000) = 952
Mr = 506.94 Dx = 3.476 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 6203 reflections
a = 10.3723 (1) Å θ = 2.6–40.6°
b = 8.9721 (1) Å µ = 7.63 mm1
c = 10.8320 (1) Å T = 296 K
β = 106.053 (1)° Hexagonal prism, colourless
V = 968.73 (2) Å3 0.12 × 0.11 × 0.10 mm
Z = 4

Data collection

Bruker APEXII CCD diffractometer 6201 independent reflections
Radiation source: fine-focus sealed tube 5023 reflections with I > 2σ(I)
graphite Rint = 0.045
Detector resolution: 8.3333 pixels mm-1 θmax = 40.6°, θmin = 3.1°
ω and φ scans h = −18→18
Absorption correction: multi-scan (SADABS; Bruker, 2008) k = −16→16
Tmin = 0.466, Tmax = 0.513 l = −19→5
24299 measured reflections

Refinement

Refinement on F2 0 constraints
Least-squares matrix: full Primary atom site location: structure-invariant direct methods
R[F2 > 2σ(F2)] = 0.030 Secondary atom site location: difference Fourier map
wR(F2) = 0.072 w = 1/[σ2(Fo2) + (0.0311P)2 + 1.1689P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.002
6201 reflections Δρmax = 1.72 e Å3
163 parameters Δρmin = −2.04 e Å3
0 restraints

Special details

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
K 0.79467 (11) 0.57090 (14) 0.04227 (10) 0.0395 (2)
Eu 0.500385 (11) 0.772652 (13) 0.184899 (12) 0.00645 (3)
P1 0.85428 (6) 0.90558 (7) 0.24010 (7) 0.00615 (10)
P2 0.54001 (6) 0.82848 (7) −0.14102 (7) 0.00607 (10)
P3 0.24938 (6) 1.02436 (7) 0.22927 (6) 0.00609 (10)
P4 0.17657 (6) 0.89469 (7) −0.01962 (6) 0.00626 (10)
O1 0.14215 (17) 0.9549 (2) 0.10673 (19) 0.0085 (3)
O2 0.35389 (19) 0.9131 (2) 0.29039 (19) 0.0093 (3)
O3 −0.02278 (19) 0.7943 (2) 0.2518 (2) 0.0103 (3)
O4 0.6017 (2) 0.5368 (2) 0.1754 (2) 0.0117 (3)
O5 0.5648 (2) 0.7615 (2) −0.0114 (2) 0.0117 (3)
O6 0.17180 (19) 1.0919 (2) 0.3112 (2) 0.0106 (3)
O7 0.73783 (19) 0.8192 (2) 0.2547 (2) 0.0134 (4)
O8 0.5691 (2) 0.7074 (2) 0.4090 (2) 0.0114 (3)
O9 0.31707 (19) 0.8419 (2) 0.0175 (2) 0.0121 (3)
O10 0.53947 (19) 1.0334 (2) 0.1765 (2) 0.0121 (3)
O11 0.31589 (17) 1.1548 (2) 0.1668 (2) 0.0092 (3)
O12 0.8309 (2) 0.9497 (2) 0.0936 (2) 0.0125 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
K 0.0363 (5) 0.0581 (6) 0.0243 (4) 0.0047 (4) 0.0085 (4) −0.0045 (4)
Eu 0.00596 (4) 0.00617 (4) 0.00701 (5) 0.00051 (3) 0.00144 (3) 0.00084 (4)
P1 0.0054 (2) 0.0053 (2) 0.0068 (2) −0.00011 (17) 0.0002 (2) 0.00105 (19)
P2 0.0060 (2) 0.0053 (2) 0.0071 (2) −0.00059 (17) 0.0021 (2) −0.00025 (19)
P3 0.0057 (2) 0.0065 (2) 0.0062 (3) 0.00066 (17) 0.0020 (2) −0.00024 (19)
P4 0.0052 (2) 0.0077 (2) 0.0050 (2) −0.00047 (17) 0.00004 (19) 0.00081 (19)
O1 0.0071 (6) 0.0106 (7) 0.0078 (7) −0.0029 (5) 0.0023 (6) −0.0027 (6)
O2 0.0094 (7) 0.0093 (7) 0.0087 (8) 0.0032 (5) 0.0015 (6) 0.0013 (6)
O3 0.0108 (7) 0.0104 (7) 0.0101 (8) 0.0053 (6) 0.0036 (6) 0.0047 (6)
O4 0.0163 (8) 0.0086 (7) 0.0117 (8) 0.0013 (6) 0.0063 (7) 0.0015 (6)
O5 0.0135 (8) 0.0155 (8) 0.0074 (8) 0.0021 (6) 0.0048 (7) 0.0014 (6)
O6 0.0114 (7) 0.0126 (7) 0.0095 (8) 0.0022 (6) 0.0059 (7) −0.0018 (6)
O7 0.0073 (7) 0.0148 (8) 0.0173 (10) −0.0029 (6) 0.0019 (7) 0.0051 (7)
O8 0.0114 (7) 0.0125 (8) 0.0093 (8) 0.0046 (6) 0.0011 (6) 0.0038 (6)
O9 0.0083 (7) 0.0193 (9) 0.0080 (8) 0.0053 (6) 0.0011 (6) 0.0024 (7)
O10 0.0099 (7) 0.0060 (6) 0.0212 (10) 0.0017 (5) 0.0059 (7) 0.0020 (7)
O11 0.0060 (6) 0.0077 (6) 0.0146 (9) −0.0005 (5) 0.0040 (6) 0.0009 (6)
O12 0.0191 (9) 0.0087 (7) 0.0069 (8) −0.0009 (6) −0.0009 (7) 0.0026 (6)

Geometric parameters (Å, °)

K—O4 2.789 (2) P1—O7 1.480 (2)
K—O5 2.860 (2) P1—O4vi 1.483 (2)
K—O6i 2.874 (2) P1—O12 1.588 (2)
K—O2i 2.961 (2) P1—O3iii 1.5968 (19)
K—O10ii 3.075 (3) P1—Kvi 3.4868 (13)
K—O3iii 3.221 (2) P2—O10iv 1.4795 (19)
K—O7ii 3.234 (3) P2—O5 1.483 (2)
K—O11iv 3.326 (2) P2—O11iv 1.6015 (18)
K—O7 3.370 (3) P2—O3i 1.602 (2)
K—P3i 3.4008 (12) P3—O6 1.482 (2)
K—P1ii 3.4868 (13) P3—O2 1.4873 (19)
Eu—O9 2.3199 (19) P3—O11 1.6005 (19)
Eu—O4 2.3775 (19) P3—O1 1.6033 (19)
Eu—O10 2.3799 (18) P3—Kvii 3.4008 (12)
Eu—O5 2.401 (2) P4—O9 1.4784 (19)
Eu—O7 2.4045 (19) P4—O8viii 1.484 (2)
Eu—O8 2.406 (2) P4—O1 1.601 (2)
Eu—O6v 2.4214 (18) P4—O12iv 1.601 (2)
Eu—O2 2.4827 (19)
O4—K—O5 59.57 (6) O5—Eu—O2 141.68 (7)
O4—K—O6i 100.70 (7) O7—Eu—O2 118.10 (7)
O5—K—O6i 89.02 (7) O8—Eu—O2 72.99 (6)
O4—K—O2i 147.48 (7) O6v—Eu—O2 77.51 (6)
O5—K—O2i 99.06 (6) O7—P1—O4vi 118.08 (13)
O6i—K—O2i 51.47 (5) O7—P1—O12 109.51 (12)
O4—K—O10ii 76.15 (6) O4vi—P1—O12 110.78 (11)
O5—K—O10ii 118.26 (7) O7—P1—O3iii 108.73 (11)
O6i—K—O10ii 143.04 (7) O4vi—P1—O3iii 110.13 (12)
O2i—K—O10ii 135.75 (6) O12—P1—O3iii 97.66 (11)
O4—K—O3iii 94.01 (6) O10iv—P2—O5 121.60 (13)
O5—K—O3iii 93.77 (6) O10iv—P2—O11iv 110.86 (11)
O6i—K—O3iii 164.29 (7) O5—P2—O11iv 106.08 (11)
O2i—K—O3iii 112.83 (6) O10iv—P2—O3i 107.58 (12)
O10ii—K—O3iii 46.46 (5) O5—P2—O3i 109.67 (12)
O4—K—O7ii 49.24 (5) O11iv—P2—O3i 98.65 (10)
O5—K—O7ii 108.54 (6) O6—P3—O2 117.21 (12)
O6i—K—O7ii 97.63 (6) O6—P3—O11 108.85 (11)
O2i—K—O7ii 138.36 (6) O2—P3—O11 109.42 (10)
O10ii—K—O7ii 52.04 (5) O6—P3—O1 106.70 (11)
O3iii—K—O7ii 96.13 (6) O2—P3—O1 111.17 (11)
O4—K—O11iv 105.76 (6) O11—P3—O1 102.44 (11)
O5—K—O11iv 46.23 (5) O9—P4—O8viii 119.05 (12)
O6i—K—O11iv 78.27 (6) O9—P4—O1 108.15 (11)
O2i—K—O11iv 57.13 (5) O8viii—P4—O1 109.93 (11)
O10ii—K—O11iv 138.47 (6) O9—P4—O12iv 108.86 (12)
O3iii—K—O11iv 92.53 (6) O8viii—P4—O12iv 110.62 (12)
O7ii—K—O11iv 153.96 (6) O1—P4—O12iv 98.17 (11)
O4—K—O7 55.48 (6) P4—O1—P3 124.84 (11)
O5—K—O7 56.64 (6) P3—O2—Eu 126.82 (12)
O6i—K—O7 144.25 (6) P3—O2—Kvii 93.80 (9)
O2i—K—O7 135.83 (6) Eu—O2—Kvii 139.28 (8)
O10ii—K—O7 63.35 (5) P1ix—O3—P2vii 130.06 (14)
O3iii—K—O7 44.54 (5) P1ix—O3—Kix 91.84 (9)
O7ii—K—O7 85.78 (3) P2vii—O3—Kix 97.17 (9)
O11iv—K—O7 83.30 (6) P1ii—O4—Eu 138.08 (12)
O9—Eu—O4 118.75 (7) P1ii—O4—K 105.27 (10)
O9—Eu—O10 79.54 (7) Eu—O4—K 108.28 (7)
O4—Eu—O10 142.30 (6) P2—O5—Eu 143.49 (12)
O9—Eu—O5 71.81 (7) P2—O5—K 110.57 (10)
O4—Eu—O5 71.94 (7) Eu—O5—K 105.40 (8)
O10—Eu—O5 85.13 (7) P3—O6—Eux 144.03 (13)
O9—Eu—O7 138.27 (7) P3—O6—Kvii 97.49 (9)
O4—Eu—O7 75.03 (7) Eux—O6—Kvii 118.48 (8)
O10—Eu—O7 70.79 (7) P1—O7—Eu 148.46 (13)
O5—Eu—O7 76.95 (8) P1—O7—Kvi 87.05 (10)
O9—Eu—O8 143.51 (7) Eu—O7—Kvi 92.57 (7)
O4—Eu—O8 79.39 (7) P1—O7—K 88.34 (10)
O10—Eu—O8 105.75 (7) Eu—O7—K 91.59 (7)
O5—Eu—O8 143.72 (7) Kvi—O7—K 175.37 (7)
O7—Eu—O8 74.50 (7) P4xi—O8—Eu 130.26 (12)
O9—Eu—O6v 75.16 (7) P4—O9—Eu 146.27 (13)
O4—Eu—O6v 75.02 (7) P2iv—O10—Eu 138.15 (12)
O10—Eu—O6v 142.48 (6) P2iv—O10—Kvi 106.53 (11)
O5—Eu—O6v 112.01 (7) Eu—O10—Kvi 97.15 (7)
O7—Eu—O6v 143.80 (7) P3—O11—P2iv 132.40 (12)
O8—Eu—O6v 80.43 (7) P3—O11—Kiv 136.15 (9)
O9—Eu—O2 75.52 (7) P2iv—O11—Kiv 88.55 (8)
O4—Eu—O2 143.69 (7) P1—O12—P4iv 133.66 (14)
O10—Eu—O2 69.57 (7)

Symmetry codes: (i) x+1/2, −y+3/2, z−1/2; (ii) −x+3/2, y−1/2, −z+1/2; (iii) x+1, y, z; (iv) −x+1, −y+2, −z; (v) −x+1/2, y−1/2, −z+1/2; (vi) −x+3/2, y+1/2, −z+1/2; (vii) x−1/2, −y+3/2, z+1/2; (viii) x−1/2, −y+3/2, z−1/2; (ix) x−1, y, z; (x) −x+1/2, y+1/2, −z+1/2; (xi) x+1/2, −y+3/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2282).

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809048788/wm2282sup1.cif

e-65-00i91-sup1.cif (17.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809048788/wm2282Isup2.hkl

e-65-00i91-Isup2.hkl (297.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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