Scientific paper Hydrogen Fluoride Adducts with the Strontium Cation: Sr(HF)3(TaF6)2 and Sr(HF)(BF4)2 Tina Buni~, Melita Tram{ek, Evgeny Goreshnik* and Boris @emva* Department of Inorganic Chemistry and Technology, Jožef Stefan Institute, Jamova 39, SI-I000 Ljubljana, Slovenia * Corresponding author: E-mail: evgeny.goreshnik@ijs.si, boris.zemva@ijs.si Received: 29-02-2008 Dedicated to the memory of Professor Ljubo Golic Abstract By slow crystallization from anhydrous HF solution crystals of two new HF adducts with the composition Sr(HF)3(Ta-F6)2 and Sr(HF)(BF4)2 were obtained and investigated by X-ray single crystal technique and Raman spectroscopy. Sr(HF)3(TaF6)2 (I) crystallizes in a monoclinic P2j/c space group, a = 8.663(17) À, b = 12.714(5) À, c = 10.759(10) À, ß= 94.24(2)°, y=1181.77(300) À3, Z = 4. The metal coordination sphere consists of nine fluorine atoms and adopts the shape of tri-capped trigonal prism. Six F atoms belong to six TaF6- anions and 3 fluorine atoms are from three terminal HF molecules. Owing to the bridging function of TaF6- anions infinite double layers lying in bc plane appear. These layers are interconnected into 3-D structure by F-H^F(Ta) hydrogen bonds. Sr(HF)(BF4)2 (II) crystallizes in an orthor-hombic Pmn2^ space group with a = 5.1566(17) À, b = 9.637(3) À, c = 6.900(2) À, y=^42.89(18) À3, Z = 2. Seven F atoms from BF4- anions and two F atoms from two bridging HF molecules form tri-capped trigonal prismatic surrounding of Sr cation. One of BF4- anions is connected to 4 metal centres, another one to 3 Sr cations and H atom of HF molecule. Owing to bridging function of both HF and BF4- moieties the complex 3-D structure appears. Keywords: Strontium, weakly bonded anion, HF adduct, TaF6-, BF4- 1. Introduction Salts containing hexafluorometalate anions have rather low lattice energies as a consequence of the anion volume (>100 À3).1 Most of these anions, AF6-, where A is As, Sb, Bi, Ta, Nb, are poor Lewis bases, so that even anhydrous HF which has extremely low basicity can provide sufficient solvation energy to bring about dissolution of M(AF6)x salts. The cations in these solutions are solvated forming Mn+(HF)x species.2 After the solvent was removed only non-solvated M(AF6)x salts were isolated. HF functioning as a ligand was not observed until 1998 when the first compound [La(HF)2](AsF6)3,3 in which HF was introduced in the metal coordination sphere, was isolated. Later many new coordination compounds with HF molecules interacting directly with the metal centre were isolated and structurally characterized: [Pb(HF)](AsF6)2,4 [Ca(HF)2](AsF6)2,5 [Cd(HF)] (AsF6)2,6 [M(HF)2](SbF6)2 (M = Mg, Ca),7 [Ca(HF)6] (AsF6)2,8 [Au(HF)2](SbF6)2 ■ 2HF,9 [OsO3F(HF)2](AsF6)2 and [OsO3F(HF)] (SbF6)2,10 K2(HF)2CrF6, K3(HF)2 Cr2F11, Na2(HF)2CrF611 Even in the presence of cova-lently bonded fluoride-anion in the metal environment, the HF molecule can form direct bond to the metal centre as it was observed, for example, in BaF(HF2)12 and Ba(H3F4)213 compounds. High absolute electronegativity of Sr2+ (27.3 eV)14 is an important factor in the process of the formation of the coordination compounds with HF. The solubility of strontium difluoride in anhydrous HF is much higher (14.83(9) g/100 g HF) than in the case of other MF2 compounds, what makes the syntheses with SrF2 easier.15 The strontium hex-afluorophosphate forms in the presence of HF an unique compound Sr2[HF2][H2F3][PF6]216 where all F atoms are involved in bonding with the metal cation. One may expect that the strontium salts with other weakly bonded large anions could form adducts with HF. In this paper the synthesis and the characterization of two new compounds Sr(HF)3(TaF6)2 and Sr(HF) (BF4)2 are described. 2. Results and Discussion 2. 1. Description of the Crystal Structures In the structure of Sr(HF)(BF4)2 nine fluorine atoms form coordination surrounding of strontium atom in the shape of tri-capped trigonal prism (Fig. 1). Seven Sr -F(B) bonds tri-capped trigonal prism. But contrary to Sr(HF)(BF4)2 the metal Fig. 3. The surrounding of Sr atom in Sr(HF)3(TaFr)2 Fig. 1. The Sr atom surrounding and the bridging function of BF4 anions in Sr(HF)(BF4)2 4 appear to be equal to 2.453(4)-2.483(8) À, whereas two Sr - F(H) bonds are strongly elongated to 2 x 2.871(3) À. Each HF molecule acts as a bridge, being bound via F atom to two metal centres. Additionally H atom is involved in a formation of strong F-H_F(B) hydrogen bond (H_F 1.6(2) À, F_F 2.47(1) À). The surrounding of each of two crystallographically independent BF4- units differs: B(1)F4- is connected to 4 Sr atoms, B(2)F4- to 3 Sr atoms and one H atom of HF molecule. Owing to bridging function of both HF and BF4- moieties the complex 3-D structure appears (Fig. 2). Fig. 2. Packing diagram of Sr(HF)(BF4)2 In the structure of Sr(HF)3(TaF6)2 compound the coordination sphere of Sr atom also adopts the shape of a environment includes only six F atoms from six TaF6- anions and 3 fluorine atoms from three HF molecules (Fig. 3). All three F(H) centres are located on the same triangular face, and the Sr-F(H) distances lie in a rather narrow range of 2.51(2)-2.55(2) À, while the Sr-F(Ta) bond lengths vary from 2.48(2) to 2.61(2) À. The shortest metal - capping fluorine atom bond length of 2.51(2) À is slightly longer than the shortest distance from strontium atom to the fluorine atom at the corner of trigonal prism 2.48(2) À. Both crystallographically independent TaF6-units play the same ^j-cis-bridging function, i.e. all three F bridges belong to one triangular face of TaF6 octahedron. The distances from Ta atom to terminal (1.83(2)-1.89(3) À) and bridging (1.89(2)-1.93(2) À) fluorine atoms differ slightly. Owing to above mentioned bridging function of TaF6- anions infinite double layers lying in bc plane appear. These layers are interconnected into 3-D Fig. 4. Packing diagram of Sr(HF)3(TaFr)2 structure by F-H_F(Ta) hydrogen bonds with F_H distances of 1.69 - 1.88 À (Fig. 4). 2. 2. Raman Spectra The Raman spectra of Sr(HF)3(TaF6)2 and Sr(HF)(BF4)2 show only bands which could be attributed to the anions. Vibrational bands at frequencies higher than 1000 cm-1 which could be most probably associated with the HF bridges,10 were not observed. The octahedral TaF6- anion (Oh symmetry) has three Raman active fundamental vibrations v1, v2 and v5 which are expected at 692, 581 and 272 cm-1, respectively.17,18 The Raman spectrum of the compound Sr(HF)3(TaF6)2 is shown on Fig. 5. In this compound TaF6- octahedra are deformed due to interactions with strontium cations and therefore the vibrational bands appear at higher frequencies at 716, 664 and 289 cm-1. Fig. 5. Raman spectrum of Sr(HF)3(TaF6)2 in a capillary. In the case of the compound Sr(HF)(BF4)2 again only the bands of the BF4- anion are seen. T^ symmetry of the BF4- anion has vibrational bands v1 at 777, v2 at 360, v3 at 1070 cm-1 and v4 at 533 cm-1.18 In the Raman spectrum of Sr(HF)(BF4)2 these bands appear at 792, 354, and at 532 cm-1. The Raman band at around 1000 cm-1 was not seen due to a high fluorescence of the sample in this region. 3. Conclusions Because HF is extremely weak base no coordination compounds with HF acting as a ligand to metal ion were discovered before 1998. Already in the late seventies it was proven by spectroscopic methods that salts Mn+(AFg)n or Mn+(BF4)n dissolve in anhydrous HF yielding solvated cations of 4he type [M(HF)g]n+.19 When the solvent HF is slowly removed the coordination compounds of the type [Mn+(HF)m](AF6)n or [Mn+(HF)m](BF4)n are formed. These compounds are usually not stable at room temperature. They are loosing HF and yielding non-solvated salts. Therefore, if the preparation of coordination compounds with HF ligands to the metal centre is desired the isolation should be performed at low temperature. Using this synthetic approach two new coordination compounds Sr(HF)3(TaF6)2 and Sr(HF)(BF4)2 with HF as a ligand to metal cation were isolated and structurally characterized. 4. Experimental Section 4. 1. General Experimental Procedures A nickel vacuum line and Teflon vacuum system were used as previously described.20 Volatile material (aHF, BF3) was manipulated in an all-Teflon vacuum line equipped with Teflon valves. Non-volatile materials (SrF2, Ta) that were sensitive to traces of moisture were handled in the dry argon atmosphere in a glove box with maximum content of 0.1 ppm of water vapour (Mbraun, Garching, Germany). A FEP reaction vessel equipped with a Teflon valve and a Teflon-covered stirring bar was used for syntheses. A T-shaped FEP reaction vessel constructed from one large FEP tube (16 mm i.d.) and a smaller FEP tube (4 mm i.d.) joint at right angle and equipped with Teflon valve was used for crystallization. 4. 2. Reagents SrF2 (Alfa Aesar, 99.99%), tantalum (BDH, 99.5%) and fluorine (Solvay, 99.98%) were used as purchased. Boron trifluoride (Union Carbide, 99.5%) was used as supplied. Anhydrous HF (Fluka, purum) was treated with K2NiFg (Ozark-Mahoning, 99%) for several days prior to use. Caution: Anhydrous hydrogen fluorine must be handled in a well-ventilated hood and protective clothing must be worn all the times! The experimentalist must become familiar with these reagents and the hazards associated with them. Fresh tubes of calcium gluconate gel should always be on hand for the fast treatment of skin exposed to these reagents. For treatment of HF injuries see reference.21 4. 2. 1. Synthesis of Sr(HF)3(TaF6)2 SrF2 (0.159 g, 1.26 mmol) and Ta (0.458 g, 2.53 mmol) were weighed into reaction vessel inside the dry box. Anhydrous HF was added by sublimation at -196 °C. Then the reaction vessel was warmed up to room temperature and after two days hydrogen was pumped out at -196 °C. The procedure was repeated until there was no hydrogen in the reaction vessel. At the next stage the fluorine (approximately 2-4 mmol) was added to the reaction mixture. Reaction was left to proceed for one additional day. The excess of F2 was pumped off from the reaction vessel at -196 °C and "fresh" F2 was added again. At the end of the reaction F2 was pumped off at -196 °C and HF at -23 °C. The reaction vessel was warmed to room temperature and weighed: the mass of the product Sr(HF)3 (TaF6)2 was 0.944 g (1.28 mmol). 4. 2. 2. Synthesis of Sr(HF)(BF4)2 SrF2 (0.106 g, 0.842 mmol) was weighed into reaction vessel inside the dry box. The reaction vessel was cooled with liquid nitrogen and anhydrous HF was added by sublimation at -196 °C. Then the reaction vessel was warmed up to room temperature and weighed. The reaction vessel was cooled again at -196 °C and BF3 (0.308g, 4.55 mmol) was added to the reaction vessel. Reaction proceeded at room temperature for 24 hours. From the solution the product was isolated by pumping off the solvent and excessive BF3 at -23 °C. The reaction vessel was warmed to room temperature and weighed: the mass of the product was 0.241 g i.e. 0.857 mmol as calculated for Sr(HF)(BF4)2. 4. 2. 3. Preparation of Single Crystals Small amounts of compounds obtained (189 mg of Sr(HF)3(TaF6)2 and 166 mg of Sr(HF)(BF4)2) were transferred in the dry box into the crystallization PFA vessel. Anhydrous HF was added on the vacuum line and a saturated solution was prepared. This solution was decanted into narrower part of the reaction vessel, which was left at room temperature while the wider part was slightly cooled to generate a small temperature gradient. The crystallization proceeded for several days. Colourless crystals were isolated by pumping off the aHF at -15 °C for Sr(HF)3(TaFg)2 and at -21 °C for Sr(HF)(BF4)2. Inside the dry box they were put in perfluoronated oil (ABCR, F05960), selected under the microscope and transferred into cold nitrogen stream at the X-ray diffractometer. 4. 2. 4. Crystallography Single-crystal data were collected on a Mercury CCD area detector coupled to a Rigaku AFC7S diffractometer using monochromatized MoKa radiation. Data were corrected for Lorentz, polarization, and absorption effects and processed using Rigaku CrystalClear software suite program package.22 Both structures were solved by direct methods using SlR-92 program,23 and refined with SHELXL-97 software,24 implemented in program package WinGX.25 Because of poor quality of diffraction array in the case of [Sr(HF)3](TaFg)2 compound fluorine atoms were refined in isotropic mode. The figures were prepared using DIAMOND 3.1 software.26 The crystal data and the details of structure refinement for both compounds are given in Table 1. Table 1 Details of experimental and crystallographic data for I and II compounds Compound I II Empirical formula H3F15SrTa2 B2HF9Sr Formula weight 737.54 281.25 Crystal size, mm 0.12 X 0.1 X 0.08 0.12 X 0.1 X 0.04 Temperature, K 200 200 Radiation MoKa MoKa Color, shape Colorless, chunk Colorless, chunk Space group P21/c Pmn21 Unit cell dimensions a, À 8.6642(12) 5.1566(17) b, À 12.7256(14) 9.637(3) c, À 10.7687(14) 6.900(2) ß, o 94.201(8) y, À3 1184.1(3) 342.89(18) Z 4 2 Dc, g/cm3 4.137 2.724 mm-1 23.10 7.98 F(000) 1288 260 Scan range 6, ° 1.9-29.1 2.1-28.7 Measured reflections 4710 1518 Used (I > 2a(I)) 1200 757 Parameters refined 164 72 R (F) 0.088 0.039 R (F)2 0.198 0.093 Goodness-of-fit 0.95 1.11 4. 2. 5. Raman Spectroscopy Raman spectra of the powdered samples in sealed quartz capillaries were collected on a Renishaw Raman Imaging Microscope System 1000 with the exciting line at 632.8 nm of a He-Ne laser. The geometry for all the Raman experiments was 180° back scattering with laser power 25 mW. 5. Acknowledgements The authors gratefully acknowledge to the Slovenian Research Agency (ARRS) for the financial support of the Research Program P1-0045 (Inorganic Chemistry and Technology). 6. References 1. H. D. B. Jenkins, H. K. Roobottom, J. Passmore, L. Glasser, Inorg. Chem. 1999, 38, 3609-3620. 2. T. A. O'Donnell. Super-acids and acidic melts as inorganic chemical reaction media, VCH Publishers, Inc, New York, 1993. 3. Z. Mazej, H. Borrmann, K. Lutar, B. Zemva, Inorg. Chem. 1998, 37, 5912-5914. 4. M. Tramšek, E. Lork, R. Mews, B. Zemva, J. Fluorine Chem. 2001,110, 123-131. 5. M. Tramšek, P. Benkič, A. Turičnik, G. Tavčar, B. Žemva, J. Fluorine Chem. 2002, 114, 143-148. 6. G. Tavčar, P. Benkič, B. Žemva, Inorg. Chem. 2004, 43, 1452-1457. 7. A. Turičnik, P. Benkič, B. Žemva, J. Fluor. Chem. 2003, I2I, 245-251. 8. M. Tramšek, P. Benkič, Acta Chim. Slov. 2004, 51, 769-778. 9. I. C. Hwang, K. Seppelt, Z. Anorg. Allg. Chem. 2002, 628, 765-769. 10. M. Gerken, D. A. Dixon, G. J. Schrobilgen, Inorg. Chem. 2002, 4I, 259-277. 11. Z. Mazej, E. Goreshnik, Europ. J. Inorg. Chem. 2008, 17951812 12. H. Prevost, J. Moret, L. Anderson and O. Lindqvist, J. Fluor. Chem. 1982, 21, 31. 13. T. Bunič, M. Tramšek, E. Goreshnik, B. Žemva, Solid State Sciences 2006, 8, 927-931. 14. R. G. Pearson, Inorg. Chem. 1988, 27, 734-740. 15. A. W. Jache, G. H. Cady, J. Chem. Phys. 1953, 56, 11061109. 16. M. Tramšek, G. Tavčar, T. Bunič, P. Benkič, B. Žemva, J. Fluor. Chem. 2005, 126, 1088-1094. 17. K. Nakamoto, Infrared and Raman spectra of inorganic and coordination compounds, Part A: Theory and applications in inorganic chemistry, John Wiley&Sons, New York, 1997. 18. A. S. Quist, J. B. Bates, G. E. Boyd, J. Chem. Phys. 1971, 54, 4896-4901. 19. G. Barraclough, R. W. Cockman, T. A. O'Donnell, Inorg. Chem. 1977, I6, 673-677. 20. H. Borrmann, K. Lutar, B. Žemva, Inorg. Chem. 1997, 36, 880-882. 21. D. Peters, R. Miethchen, J. Fluorine Chem. 1996, 79, 161-165. 22. CrystalClear: Rigaku Corporation, The Woodlands, Texas, USA, 1999. 23. A. Altomare, M. Cascarano, M., C. Giacovazzo, A. Guagliar-di, J. Appl. Cryst. 1993, 26, 343-350. 24. G. M. Scheldrick, SHELXL-97, University of Göttingen, Germany, 1997. 25. L. J. Farrugia, J. Appl. Cryst. 1999, 32, 837-838. 26. DIAMOND v3.1. Crystal Impact GbR, Bonn, Germany. 2004-2005. Povzetek S počasno kristalizacijo iz brezvodnega HF smo izolirali dva nova HF adukta s sestavo Sr(HF)3(TaF6)2 in Sr(HF)(BF4)2, ki smo ju raziskovali z rentgensko tehniko za mono kristale in z ramansko spektroskopijo. Sr(HF)3(TaF6)2 (I) kristalizira v monoklinski prostorski skupini P21/c, a = 8.663(17) À, b = 12.714(5) À, c = 10.759(10) À, ß = 94.24(2)°, y=1181.77(300) À3, Z=4. V koordinacijski sferi kovine se nahaja devet fluorovih atomov v obliki trigonalne prizme s tremi kapami na pravokotnih ploskvah. Šest F atomov pripada šestim TaF6- anionom, tri F atome pa prispevajo tri terminalne HF molekule. Glede na to, da so TaF6- anioni mostovni dobimo neskončne dvojne plasti, ki ležijo v bc ravnini. Te plasti so med seboj povezane v 3-D strukturo z F-H^F(Ta) vodikovimi vezmi. Sr(HF)(BF4)2 (II) kristalizira v orto-rombski Pmn2I prostorski skupini z a = 5.1566(17) À, b = 9.637(3) À, c = 6.900(2) À, y=342.89(18) À3, Z=2. Sedem F atomov od BF4- anionov in dva F atoma od dveh mostovnih HF molekul tvori okrog Sr kationa trigonalno prizmo s tremi kapami na pravokotnih ploskvah. Eden od BF4- anionov je povezan s štirimi kovinskimi centri, medtem ko je drugi BF4- povezan le s tremi Sr kationi in H atomom od HF molekule. Glede na to, da je tako HF kot BF4- skupina mostov-na, dobimo 3-D strukturo.