Literature DB >> 32431920

Dehydration synthesis and crystal structure of terbium oxychloride, TbOCl.

Saehwa Chong1, Brian J Riley1, Zayne J Nelson1.   

Abstract

Terbium oxychloride, TbOCl, was synthesized via the simple heat-treatment of TbCl3·6H2O and its structure was determined by refinement against X-ray powder diffraction data. TbOCl crystallizes with the matlockite (PbFCl) structure in the tetra-gonal space group P4/nmm and is composed of alternating (001) layers of (TbO) n and n Cl-. The unit-cell parameters, unit-cell volume, and density were compared to the literature data of other isostructural rare-earth oxychlorides in the same space group and showed good agreement when compared to the calculated trendlines. © Chong et al. 2020.

Entities:  

Keywords:  oxychloride; powder diffraction; rare-earth oxyhalide

Year:  2020        PMID: 32431920      PMCID: PMC7199267          DOI: 10.1107/S2056989020004387

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Chemical context

Rare-earth oxychlorides, REOCl, are promising materials for various applications including use as catalysts, sensors, and phosphors (Podkolzin et al., 2007 ▸; Au et al., 1997 ▸; Peringer et al., 2009 ▸; Marsal et al., 2005 ▸,; Kim et al., 2019 ▸; Berdowski et al., 1984 ▸; Imanaka et al., 2001a ▸,b ▸; Okamoto et al., 2002 ▸; Kim et al., 2014 ▸). LaOCl is a stable catalyst for converting methane to methyl chloride (Podkolzin et al., 2007 ▸) and can be used as a sensor material to detect CO2 and Cl2 gases (Marsal et al., 2005 ▸; Imanaka et al., 2001b ▸). The EuOCl catalyst showed high efficiency in converting ethyl­ene to vinyl chloride (Scharfe et al., 2016 ▸). The luminescent properties of REOX (RE = La, Eu; X = F, Cl, Br, I) can be controlled to emit a wide range of visible light from blue to red by changing the crystal symmetries and compositions (Kim et al., 2014 ▸, 2019 ▸). As part of our studies in this area, we now describe the dehydration synthesis and structure of the title compound.

Structural commentary

The structural parameters of REOCl (RE = La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho) in the literature and current study are summarized in Table 1 ▸. All these REOCl compounds crystallize in the matlockite (PbFCl; Bannister, 1934 ▸) structure within the tetra­gonal P4/nmm space group. The crystal structure of TbOCl contains alternating (001) layers of (TbO) and n Cl− (Fig. 1 ▸ a). The Tb cation is coordinated by five chloride ions and four oxygen atoms, forming a mono-capped TbO4Cl5 square anti­prism (Fig. 1 ▸ b and 1c). The RE—Cl and RE—O bond lengths in the REOCl compounds are provided in Table 1 ▸. With larger RE cations in the structures, the RE—Cl and RE—O bond lengths increase (Fig. 2 ▸).
Table 1

Structural parameters of REOCl compounds

All compounds crystallize in the P4/nmm space group. For the RE—Cl bond lengths, the first value refers to one neighboring Cl atom, and the second number refers to four neighboring Cl atoms. Densities are calculated from crystallographic data.

RE a(Å) c(Å) V3)Density(g cm−3) RE—O(Å) RE—Cl(Å)Cl⋯Cl(Å)Cl⋯O(Å)O⋯O (Å)ICSD/PDF
Ho3.8936.602100.17.1822.2473.04, 3.053.243.122.75376171 (Templeton & Dauben, 1953)
Dy3.916.62101.27.023     00–047-1725 (Kirik et al., 1996)
Tb3.92696.648102.56.815     00–048-1648 (Kirik et al., 1996)
Tb3.92796.6556102.76.8042.26493.064, 3.0823.2713.1512.7774Current study
Gd3.94956.6708104.16.6612.28393.036, 3.0983.2673.1762.792759232 (Meyer & Schleid, 1986)
Gd3.96986.7008105.66.5642.283.212, 3.0713.4283.0892.807177820 (Hölsä et al., 1996)
Eu3.96466.695105.26.422.2863.08, 3.113.33.172.803428529 (Bärnighausen et al., 1965)
Eu3.96686.6955105.46.4122.29013.062, 3.11033.2893.1832.8049254682 (Schnick, 2004)
Sm3.9826.721106.66.2892.2963.09, 3.123.313.192.815726581 (Templeton & Dauben, 1953)
Nd4.046.77110.55.8822.3593.114, 3.113.4283.1652.8631665 (Zachariasen, 1949)
Nd4.02496.7837109.95.9142.33623.082, 3.1413.3433.2212.8460359231 (Meyer & Schleid, 1986)
Pr4.0536.799111.75.7232.36743.128, 3.1163.4413.1782.86631664 (Zachariasen, 1949)
Ce4.08666.8538114.55.5582.36873.1190, 3.18463.39423.25722.8897412069 (Schnick, 2004)
Ce4.07856.8346113.75.5962.364133.103, 3.1803.383.2542.8839372154 (Wołcyrz & Kepinski, 1992)
La4.1096.865115.95.4542.393.14, 3.183.453.242.905524611 (Sillen & Nylander, 1941)
La4.1176.881116.65.422.38663.126, 3.20463.4163.27512.911240297 (Brixner & Moore, 1983)
La4.13516.904118.15.3552.3953.165, 3.2093.4573.2682.9239777815 (Hölsä et al., 1996)
La4.11626.8746116.55.4282.38323.138, 3.2013.4253.2652.910684330 (Hölsä et al., 1997)
La4.126.882116.85.412     00–008-0477 (Swanson et al., 1957)
Figure 1

(a) Crystal structure of TbOCl, (b) the coordination environment of Tb, and (c) polyhedron representation of the Tb environment.

Figure 2

The RE—Cl and RE—O bond lengths in the REOCl compounds listed in Table 1 ▸ as a function of RE crystal radius (coordination = 9) according to Shannon (1976 ▸). Where multiple values were available, averages and standard deviations are included for the datapoints. For (a), 1-nd and 4-nd denote 1 and 4 neighbor distances, respectively

The shortest Cl⋯Cl separation in TbOCl is 3.271 (4) Å, which compares with the van der Waals diameter of a Cl− ion of about 3.62 Å. The Cl⋯Cl distances of other REOCl compounds are also short, ranging from 3.24 to 3.46 Å on going from Ho3+ to La3+. With non-bonded vectors shorter than the van der Waals separation, strong inter­actions between atoms are expected in the structure (Maslen et al., 1996 ▸). Templeton & Dauben (1953 ▸) mention the presence of weaker anion–anion repulsion between Cl atoms in REOCl structures. The structural parameters of TbOCl were compared with the trendlines calculated using the values from Table 1 ▸ (Fig. 3 ▸). The unit-cell parameters and volumes increase linearly with the larger RE cations (Shannon, 1976 ▸) whereas the densities decrease non-linearly, fitting well to a 2nd order polynomial trend.
Figure 3

(a, b) Unit-cell parameters (a and c, respectively), (c) unit-cell volumes, and calculated unit-cell densities as a function of the crystal radius of the RE (coordination = 9) according to Shannon (1976 ▸) compared to literature values provided in Table 1 ▸.

Synthesis and crystallization

The title compound was synthesized by a simple heat treatment of TbCl3·6H2O (Alfa Aesar, 99.99%). About 0.5 g of TbCl3·6H2O was placed in an alumina crucible, heated to 400°C at 5°C min−1, held for 8 h, and then cooled to room temperature at 5°C min−1. This synthesis method was used in our previous study (Riley et al., 2018 ▸). The resulting product was a light-brown powder, which was ground in a mortar and pestle for X-ray powder diffraction analysis.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2 ▸. The unit-cell parameters were obtained using TOPAS (version 4.2; Bruker, 2009 ▸) by refining the GdOCl pattern (ICSD 77820) with geometrical and chemical resemblance as a starting model. The Rietveld refinement was performed using JANA2006 (Petříček et al., 2014 ▸) with the obtained unit-cell parameters as initial values. A pseudo-Voigt function with other peak-shape parameters were used to fit peaks, and the background was modeled with a Chebychev polynomial. The plot of the Rietveld refinement result is shown in Fig. 4 ▸. The final refinement converged at R wp = 3.22%.
Table 2

Experimental details

Crystal data
Chemical formulaTbOCl
M r 210.4
Crystal system, space groupTetragonal, P4/n m m
Temperature (K)293
a, c (Å)3.9279 (2), 6.6556 (5)
V3)102.68 (1)
Z 2
Radiation typeCu Kα, λ = 1.54188 Å
Specimen shape, size (mm)Cylinder, 25 × 25
 
Data collection
DiffractometerBruker D8 Advance
Specimen mountingPacked powder pellet
Data collection modeReflection
Scan methodStep
2θ values (°)min = 5, 2θmax = 68.977, 2θstep = 0.019
 
Refinement
R factors and goodness of fit R p = 0.020, R wp = 0.032, R exp = 0.009, R(F) = 0.033, χ2 = 13.690
No. of parameters17

Computer programs: XRD Commander (Kienle & Jacob, 2003 ▸), TOPAS (Bruker, 2009 ▸), SUPERFLIP (Palatinus & Chapuis, 2007 ▸), JANA2006 (Petříček et al., 2014 ▸), VESTA (Momma & Izumi, 2011 ▸) and publCIF (Westrip, 2010 ▸).

Figure 4

Measured, calculated, and difference XRD patterns of TbOCl.

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S2056989020004387/hb7896sup1.cif Rietveld powder data: contains datablock(s) I. DOI: 10.1107/S2056989020004387/hb7896Isup2.rtv Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989020004387/hb7896Isup3.hkl CCDC reference: 1993793 Additional supporting information: crystallographic information; 3D view; checkCIF report
TbOClZ = 2
Mr = 210.4Dx = 6.804 Mg m3
Tetragonal, P4/nmmCu Kα radiation, λ = 1.54188 Å
a = 3.9279 (2) ÅT = 293 K
c = 6.6556 (5) Ålight brown
V = 102.68 (1) Å3cylinder, 25 × 25 mm
Bruker D8 Advance diffractometerData collection mode: reflection
Radiation source: sealed X-ray tubeScan method: step
Specimen mounting: packed powder pelletmin = 5°, 2θmax = 68.977°, 2θstep = 0.019°
Rp = 0.02017 parameters
Rwp = 0.032Weighting scheme based on measured s.u.'s
Rexp = 0.009(Δ/σ)max = 0.030
R(F) = 0.033Background function: 8 Chebyshev polynoms
3292 data pointsPreferred orientation correction: March & Dollase
Profile function: Pseudo-Voigt
xyzUiso*/Ueq
Tb10.500.3305 (2)0.002
Cl100.50.1298 (9)0.002
O1100.50.002
U11U22U33U12U13U23
Tb10.0020.0020.002000
Cl10.0020.0020.002000
O10.0020.0020.002000
Tb1—Tb1i3.5784 (13)Tb1—O1v2.2649 (7)
Tb1—Tb1ii3.5784 (13)Tb1—O12.2649 (7)
Tb1—Tb1iii3.5784 (13)Tb1—O1vi2.2649 (7)
Tb1—Tb1iv3.5784 (13)Tb1—O1vii2.2649 (7)
Tb1i—Tb1—Tb1ii66.57 (2)Tb1iii—Tb1—O1vii99.31 (4)
Tb1i—Tb1—Tb1iii66.57 (2)Tb1iv—Tb1—O1v99.31 (4)
Tb1i—Tb1—Tb1iv101.82 (4)Tb1iv—Tb1—O137.817 (14)
Tb1i—Tb1—O1v37.817 (14)Tb1iv—Tb1—O1vi99.31 (4)
Tb1i—Tb1—O199.31 (4)Tb1iv—Tb1—O1vii37.817 (14)
Tb1i—Tb1—O1vi37.817 (14)O1v—Tb1—O1120.25 (6)
Tb1i—Tb1—O1vii99.31 (4)O1v—Tb1—O1vi75.63 (3)
Tb1ii—Tb1—Tb1iii101.82 (4)O1v—Tb1—O1vii75.63 (3)
Tb1ii—Tb1—Tb1iv66.57 (2)O1—Tb1—O1vi75.63 (3)
Tb1ii—Tb1—O1v37.817 (14)O1—Tb1—O1vii75.63 (3)
Tb1ii—Tb1—O199.31 (4)O1vi—Tb1—O1vii120.25 (6)
Tb1ii—Tb1—O1vi99.31 (4)Tb1—O1—Tb1viii120.25 (4)
Tb1ii—Tb1—O1vii37.817 (14)Tb1—O1—Tb1iii104.37 (2)
Tb1iii—Tb1—Tb1iv66.57 (2)Tb1—O1—Tb1iv104.37 (2)
Tb1iii—Tb1—O1v99.31 (4)Tb1viii—O1—Tb1iii104.37 (2)
Tb1iii—Tb1—O137.817 (14)Tb1viii—O1—Tb1iv104.37 (2)
Tb1iii—Tb1—O1vi37.817 (14)Tb1iii—O1—Tb1iv120.25 (4)
  3 in total

1.  Self-emitting blue and red EuOX (X = F, Cl, Br, I) materials: band structure, charge transfer energy, and emission energy.

Authors:  Donghyeon Kim; Jae Ryeol Jeong; Yujin Jang; Jong-Seong Bae; In Chung; Runli Liang; Dong-Kyun Seo; Seung-Joo Kim; Jung-Chul Park
Journal:  Phys Chem Chem Phys       Date:  2019-01-23       Impact factor: 3.676

2.  Blue-emitting Eu2+-activated LaOX (X = Cl, Br, and I) materials: crystal field effect.

Authors:  Donghyeon Kim; Sangha Park; Sungyun Kim; Seong-Gu Kang; Jung-Chul Park
Journal:  Inorg Chem       Date:  2014-10-30       Impact factor: 5.165

3.  Methyl chloride production from methane over lanthanum-based catalysts.

Authors:  Simon G Podkolzin; Eric E Stangland; Mark E Jones; Elvira Peringer; Johannes A Lercher
Journal:  J Am Chem Soc       Date:  2007-02-13       Impact factor: 15.419

  3 in total

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