- freely available
Crystals 2012, 2(1), 144-158; doi:10.3390/cryst2010144
Abstract: Anion substitution is at present one of the pathways to destabilize metal borohydrides for solid state hydrogen storage. In this work, a solid solution of LiBH4 and LiCl is studied by density functional theory (DFT) calculations, thermodynamic modeling, X-ray diffraction, and infrared spectroscopy. It is shown that Cl substitution has minor effects on thermodynamic stability of either the orthorhombic or the hexagonal phase of LiBH4. The transformation into the orthorhombic phase in LiBH4 shortly after annealing with LiCl is for the first time followed by infrared measurements. Our findings are in a good agreement with an experimental study of the LiBH4-LiCl solid solution structure and dynamics. This demonstrates the validity of the adopted combined theoretical (DFT calculations) and experimental (vibrational spectroscopy) approach, to investigate the solid solution formation of complex hydrides.
Mixtures of metal borohydrides with halides have recently evoked careful attention as candidates for hydrogen storage materials [1,2,3,4,5,6,7] and novel solid-state lithium electrolytes [8,9,10,11]. Whereas the improvement in the hydrogen absorption and release kinetics and thermodynamics of these materials is still under investigation, their recently-discovered high ionic conductivity opens new horizons for applications. Metal borohydride mixtures with halides are proved to form solid solutions [7,10,11,12,13]. Anion substitution changes the site symmetry of the BH4- ions, which is immediately reflected in the vibrational spectra. For example, in the LiBH4-LiI and LiBH4-LiBr solid solutions [14,15], Br− and I− stabilize the high temperature hexagonal phase of LiBH4 at room temperature. The phase transformation from o- to h-LiBH4 caused by anion exchange is shown to modify substantially the profile of the BH4− infrared vibrations.
Periodic ab initio CRYSTAL code  has already been successfully applied in a number of studies dealing with the computational prediction of solid solution formation, both for simple and complex hydrides [2,17]. The starting structures are taken from the experimental data collected in the Inorganic Crystal Structure Database  and are fully optimized to get the minimum energy geometry. Accurate calculations of the vibrational frequencies on the optimized system geometry allowed us to simulate infrared/Raman spectra and to draw a punctual comparison with the experimental measurements . The comparison can be very useful in assigning complex spectral patterns of novel compounds and also in stating whether the solid solution has formed or not. Moreover, by computing vibrations and applying the equations of statistical mechanics, thermodynamic properties can be evaluated, such as solid solution formation enthalpy, entropy, free energy and heat capacity at the desired temperatures. In particular, in the case of lithium borohydride, some of us have performed DFT calculations on the orthorhombic phase, mixed with LiBF4 . In that case, the major issue has regarded the calculation of a large number of possible configurations, because fluorine is substituting hydrogen atom(s) inside the borohydride tetrahedral units. Conversely, in the case of other halide ions, such as Cl−, the entire BH4- group is substituted because of the correspondent ionic radii (r = 1.81 Å for Cl− and 2.05 Å for BH4− [12,20]).
In this work, we present the study on the LiBH4-LiCl system, utilizing attenuated total reflection infrared spectroscopy (IR-ATR), powder X-ray diffraction (PXRD), DFT calculations with CRYSTAL code and thermodynamic modeling.
2. Results and Discussion
2.1. Optimized Structures of o-LiBH4-Cl and h-LiBH4-Cl Solid Solutions
Pure orthorhombic (o-LiBH4, Pnma space group) and hexagonal (h-LiBH4, P63mc space group) structures of LiBH4 were optimized at the DFT-Perdew-Burke-Ernzerhof (DFT-PBE) level of theory, starting from the experimental coordinates .The optimized unit cell structures are shown in Figure 1, whereas the most important structural parameters are summarized in Table 1 in comparison with experimental data.
|DFT -LiBH4 + LiCl|
|DFT h-LiBH4 + LiCl|
a Ref. .
For the orthorhombic crystal, a systematic overestimation of the B-H bond length is observed, as already pointed out in literature [2,19], which however does not significantly affect the unit cell volume.
The hexagonal phase is stable at high temperature (T ≥ 381 K) . Therefore, without inclusion of temperature effects, full geometry optimization starting from the experimental structure dramatically distorts the internal geometry and the cell volume, as reported in Table 1. Indeed, for the unit cell of h-LiBH4, frequency calculation at Gamma point on the optimized structure reveals six imaginary frequencies, showing the instability of this phase when temperature is not taken into account. Maintaining the cell parameters fixed at the experimental values does not remove the structural instability, as the internal atomic displacements are still very large, as shown also by Miwa et al. ,due to the dynamic disorder of BH4− units . In order to overcome these difficulties and, moreover, to simulate solid solutions, a supercell approach was adopted in the case of h-LiBH4, considering a larger and more representative scenario (for the original cell Z = 2 → 12 atoms, while in the supercell Z = 16 → 96 atoms). In this operation of doubling each cell vector, symmetry is completely lost and borohydride tetrahedra are free to rotate, so removing the phonon instability found in the single unit cell. Indeed, when computing frequency values for the hexagonal supercell, only one imaginary mode is found at −20 cm−1. In the following, to avoid numerical problems due to the variable number of imaginary frequencies for the structures, we have used the whole set of frequencies by considering also the imaginary values (by using their absolute value in the statistical thermodynamic formulae) for the calculation of the zero point energy (ZPE) and enthalpy corrections, as described below.
The relative energy stabilities calculated for the two phases favor the orthorhombic structure with respect to the hexagonal, as expected, but their enthalpy difference (ORTHO − HEXΔH = 10 kJ∙mol−1 per formula unit) overestimates experimental measurements [24,25], due to the instability of the hexagonal model.
Even if the stable LiCl polymorph at room temperature is cubic, corresponding structures were obtained for both the orthorhombic and hexagonal phases as the full substitution of BH4- with chlorine. The difference in enthalpy for the three phases of LiCl was calculated for the phase diagram calculation, giving CUBIC − ORTHOΔH = 21.8 kJ∙mol−1 and CUBIC − HEXΔH = 15.1 kJ∙mol−1.
The simulation of orthorhombic solid solution o-Li(BH4)1−xClx, where four borohydride units are present in the o-LiBH4 unary cell, was performed, considering three compositions with molar fraction of chlorine, x, equal to 0.25, 0.50 and 0.75. The corresponding unary cells are reported in Figure 1. For x = 0.5, three non-equivalent configurations were computed, namely C1, C2 and C3, as shown in Figure 1. Among them, C3 structure turned out to be the most stable, because of the largest Cl-Cl distance. Conversely, for the hexagonal solid solution h-Li(BH4)1−xClx, due to the large size of the supercell, only three compositions have been considered, that are Li(BH4)0.94Cl0.06, Li(BH4)0.5Cl0.5, and Li(BH4)0.06Cl0.94.
For the orthorhombic solid solutions, the unit cell volume decreases with the increase of Cl substitution, as expected, with a maximum variation of about 10% for the highest chlorine content (x = 0.75). For the hexagonal structures, the volume decreases as a function of Cl content, with a maximum variation of about 13% for x = 0.94. It can be mentioned here that the calculated cell volume reduction for the Cl-substituted o-LiBH4 and h-LiBH4 correlates well with the experimentally observed values .
Thermal entropy was calculated for each composition using classical statistical thermodynamic formulae. As it was computed using the harmonic set of frequencies, the hindered BH4− rotation is included, as well as the frustrated translation of the substituting Cl. It turned out that the hindered BH4− soft rotational motion is compensated by the frustrated translation of the substituting Cl ion, so that the thermal entropy contribution is very small, well below the contribution due to the ideal configurational entropy.
2.2. Thermodynamics of the Solid Solution Formation
The enthalpy of mixing was computed at room temperature for the models shown in Figure 1. The obtained results are shown in Figure 2 as a function of the increasing LiCl mole fraction. According to simulations, o-LiBH4 is slightly destabilized by the substitution of chloride inside the lattice, since computed enthalpy of mixing (ΔHmix) values are positive and small (less than 2 kJ mol−1 per formula unit). On the contrary, in the hexagonal phase, the enthalpy of mixing shows slightly negative values, less than −1 kJ mol−1 per formula unit, so that the h-LiBH4 is, to some extent, stabilized by LiCl. As stated above, the thermal entropy contribution is very small, so ideal entropy of mixing (ΔSmix) has been considered for free energy calculations. When ΔHmix and −TΔSmix terms are summed up at room temperature, the free energy of mixing (ΔGmix) becomes close to zero for the orthorhombic phase and slightly negative for the hexagonal phase for all compositions.
In order to describe thermodynamic behavior of the LiBH4-LiCl system, the CALPHAD approach  was used. Due to the lack of thermodynamic data for the LiBH4-LiCl liquid mixture, the phase diagram was evaluated, neglecting the liquid phase, and it is considered only below the melting temperature of LiBH4.The presence of an attractive interaction in the liquid state could induce a stabilization of the liquid phase below the melting temperatures of pure components, as found experimentally by in situ X-ray diffraction .
On the basis of the evaluated thermodynamic parameters, the pseudo binary phase diagram for the LiBH4-LiCl system has been calculated and the results shown in Figure 3. The calculated solubility of Cl into o-LiBH4 is rather low and it reaches a value x = 0.1 at about 500 K for the h-LiBH4 phase. A eutectoid phase transition is calculated at 372 K and x = 0.04. The phase diagram behavior is very sensitive to both lattice stabilities (i.e., free energy difference between different phases of the pure components) as well as to the free energy of mixing. The very strong instability, predicted for the metastable o-LiCl (CUBIC − ORTHOΔH = 21.8 kJ∙mol−1), and the calculated nearly zero ΔGmix , prevent any relevant solubility of Cl inside the orthorhombic phase. The negative ΔGmix for the hexagonal solid solution and a more stable h-LiCl, if compared to the orthorhombic one (HEX − ORTHOΔH = 6.7 kJ∙mol−1), allow for the stabilization of the hexagonal phase with respect to the orthorhombic one when Cl is added. Of course, a lower value of HEX − ORTHOΔH and a more negative enthalpy of mixing for the hexagonal phase would promote a higher solubility of Cl in h-LiBH4 phase.
2.3. Structural Properties of o-Li(BH4)1−xClx and h-Li(BH4)1−yCly
2.3.1. Computational Study of the o-Li(BH4)1−xClx and h-Li(BH4)1−yCly Vibrational Properties
In the mid-infrared region the vibrational spectra of LiBH4, orthorhombic and hexagonal phases exhibit stretching (ν1, ν3), bending (ν2, ν4) and combinational (not accounted for in the computed spectra) modes of the BH4− anions (Figure 4) [19,27,28,29,30]. The modes ν3 and ν4 are triply degenerate in free tetrahedral BH4− ions, and the ν2 is doubly degenerate. Due to the different BH4− site symmetry in the Pnma and P63mc space groups, Cs and C3v respectively, vibrational spectra of h-LiBH4 are expected to be simpler, since the ν2 mode remains degenerate and both ν3, ν4 split into only two components each. The computed IR spectrum of the h-LiBH4 supercell, however, is much more complex, due to the absence of any symmetry at all and 32 BH4− ions in the cell: see Figure 4b. Nevertheless, several observations can be made.
Substitution of BH4− with Cl− in the unit cell of o-LiBH4 does not modify significantly its IR vibrations. Stretching ν3 and bending ν4 modes of BH4− appear to be the most sensitive to the Cl− substitution, moving to higher frequencies by Δν = +10...+35 cm−1 (Figure 4a). The ν1 and ν2 modes are the least affected by the presence of Cl−, being shifted only with the highest amount of Cl− in the unit cell (x = 0.75). These negligible modifications in the BH4− vibrational profile can be explained by the BH4− low site symmetry in pure and all the Cl-substituted unary cells of o-Li(BH4)1−xClx, and that the substitution does not cause a significant change in the number of IR-active peaks. Since the symmetry in the supercell of the h-LiBH4 and h-Li(BH4)1−yCly is completely removed, the spectra of all compounds on the Figure 4b appear to be much more complex than are expected for the h-LiBH4 unary cell. Stretching modes in the 2500–2300 cm−1 region evidently shift to higher wavenumbers with increasing Cl− concentration. Apparently, it is difficult to distinguish between the spectra of pure and Cl-substituted o-LiBH4 or h-LiBH4 when the molar concentration of Cl− is small (compare black and blue curves in Figure 4).
Orimo et al.  suggested a correlation between the position of the ν1 and ν2 modes and the stability in the Li, Na, K, Rb, Cs borohydrides: in the most stable, CsBH4 ν2 has the lowest energy of vibrations. In this way, the almost unaffected position of the ν1 and ν2 modes in the Cl-substituted LiBH4 can be interpreted as evidence of a minor effect of the chlorine substitution on the stability of LiBH4.
2.3.2. Experimental Study of LiBH4-LiCl Mixture and Solid Solution
The structure and vibrations of LiBH4-LiCl mixture (1:1) were studied by powder X-ray diffraction and infrared spectroscopy. No chlorine substitution is found after hand mixing of the sample, as expected , (Figure 5a), whereas after annealing, a small amount of chlorine is found both in the hexagonal and orthorhombic phases of LiBH4 (Figure 5b, Table 2).
|Molar fraction, mol%|
|LiBH4-LiCl (1:1) S1 hm|
|LiBH4-LiCl (1:1) S1 hm, annealed|
The ATR spectrum of the hand-mixed mixture is shown in Figure 6 (violet curve). It is very similar to that of pure LiBH4 (grey curve). This is in agreement with the presence of pure o-LiBH4 and LiCl in the sample.
After annealing, however, the spectrum is strongly modified (Figure 6, black curve 1), but these modifications are not preserved with time. In particular, the spectrum 1 in Figure 6 has one broad peak in the B-H, stretching at ca. 2400–2100 cm−1, which within a short time (ca. 20 min), splits into two (spectra 2–5), narrows, and gains intensity. HBH bending modes in the 1300–1000 cm−1 region are also modified: the peak at 1298 cm−1 splits into two components at 1310–1286 cm−1, and the peaks at 1229 and 1081 cm−1 grow in intensity and shift upwards. The combinational modes at 2181 cm−1 and in the 2300–2550 cm−1 regions also gain intensity. These changes in the infrared spectra are similar to those observed  in the in situ Raman measurements of the LiBH4 upon heating in the 22–139 °C temperature range, and should be associated with C3ν → Cs site symmetry lowering of the BH4− tetrahedra upon P63mc → Pnma phase transformation in LiBH4. It is important to note that for the in situ Raman experiment, the phase transformation was observed during heating and cooling. For this study, all spectra were obtained at room temperature after the annealing of LiBH4 with LiCl. This fact evidences the role of Cl in the short-term stabilization of the high temperature hexagonal phase of LiBH4. In fact, Arnbjerg et al.  have demonstrated that the phase transition temperature in LiBH4 (during cooling) can approach 20 °C, depending on the degree of Cl-substitution. They note that this change in the phase transition temperature indicates a stabilization of the hexagonal phase caused by the incorporation of Cl− in the LiBH4 structure.
According to the X-ray diffraction data, which were obtained shortly after the infrared experiment (and therefore better correspond to the curve 5, Figure 6), o-Li(BH4)0.90Cl0.10 , phase prevails in this sample, which explains its similarity to the spectrum of pure o-LiBH4. Note that the computed spectra of o-LiBH4 and the o-Li(BH4)0.75Cl0.25 are very similar (Figure 4a). Present results are in good agreement with those reported by Arnbjerg et al. . In fact, after annealing during cooling, the hexagonal phase found at high temperature is quenched in the mixture. The ortho-to-hexa phase transition is promoted at RT, as evidenced by ATR measurements (Figure 6). During the phase transformation, the Cl− content in LiBH4 is strongly reduced and LiCl is formed The Cl− content in the orthorhombic phase (x = 0.10), observed in PXRD measurements, is in agreement with previous experiments , but it turns out higher than that predicted by combined ab initio and CALPHAD calculations (Figure 3). As described before, the estimated solubility range is very sensitive to the results of ab initio calculation, which would need a more accurate determination of lattice stability in order to fully describe the experimental findings.
3.1. Ab Initio
Ab initio calculations based on DFT GGA Hamiltonian (PBE) were carried out with the periodic CRYSTAL09 code and localized basis set functions of polarized double-ζ quality. In detail: Li cation was described with a 5–11G(d) basis set (αsp = 0.479 bohr−2 for the most diffuse shell exponent and αpol = 0.600 bohr−2 for polarization), while for boron a 6–21G(d) was adopted (αsp = 0.124 bohr−2 for the most diffuse shell exponent and αpol = 0.800 bohr−2 for polarization). For hydrogen, a 31G(p) (αsp = 0.1613 bohr−2 for the most diffuse shell exponent and αpol = 1.1 bohr−2 for polarization) was considered; for chlorine, a 86–311G basis set was used (αsp = 0.125 bohr−2 for the most diffuse shell exponent).
Phonons at Γ point in the harmonic approximation were computed to derive the thermodynamic functions by diagonalizing the associated mass-weighted Hessian matrix (for details on the computational procedure see references [31,32]). Grimme’s correction to the electronic energy was computed to take dispersion forces into account for all calculations, following the D* approach described in the literature [33,34]. The enthalpy data were obtained as the electronic energy, including the zero-point energy correction (ZPE), and the thermal factor at the desired temperature.
Unary phases (i.e., pure elements) have been described according to the SGTE database . The cubic phase was considered as stoichiometric LiCl, neglecting the possible solubility of LiBH4 in this structure. The thermodynamic parameters for this compound (CUBICG(LiCl)) were taken from the Substance SGTE database .
LiBH4-LiCl solid solutions with orthorhombic and hexagonal structures were modeled using two sublattices, the first occupied by Li+ and the second occupied by Cl− or by a BH4− unit.
As usual, the Gibbs free energy of these solutions can be expressed as :
ORTHOG(LiBH4) was taken from the Substance database. On the basis of ab initio calculations, the free energy of orthorhombic LiCl was evaluated as ORTHOG(LiCl) = CUBICG(LiCl) + A − BT, where CUBICG(LiCl) was taken from the Substance database and A = 21.8 kJ·mol−1 and B = 7.2 J·K−1·mol−1. As shown in Figure 2, since the ab initio calculated enthalpy of mixing is slightly positive and nearly symmetric, the excess Gibbs energy was modeled as a regular solution, giving with Ω = 5.940 kJ·mol−1.
Because the thermodynamic function for LiBH4 reported in the Substance database does not take into account the phase transition  from orthorhombic to hexagonal phases occurring at 383 °K, new thermodynamic parameters for the hexagonal LiBH4 have been evaluated. According to the enthalpy and temperature of transition measured by Price et al. , the Gibbs free energy of h-LiBH4 has been described as HEXG(LiBH4) = ORTHOG(LiBH4) + A − BT, where A = 4.4 kJ·mol−1 and B = 11.4 J·K−1·mol−1. Since no experimental data are available for the hexagonal LiCl, HEXG(LiCl) was evaluated on the basis of ab initio calculations as HEXG(LiCl) = CUBICG(LiCl) + A − BT, where A = 15.1 kJ·mol−1 and B = 2.3 J·K−1·mol−1. According to the results of ab initio calculations the excess Gibbs energy of the hexagonal solid solution was modeled as a regular solution, giving with Ω = −4.827 kJ·mol−1kJ·mol−1.
4. Experimental Section
The samples used for the infrared experiments were handled in a nitrogen-filled glove box. As received anhydrous LiCl (Aldrich, purity 98.0%) was additionally dried in a dynamic vacuum at 120 °C and then transferred to the glove box. LiBH4 (Aldrich, purity 95.0%) was stored in the glove box. The absence of water impurities was controlled by infrared analysis. The sample was thoroughly mixed in the agate mortar in 1:1 molar ratio (this sample is denoted as “S1 hm” in the text). The mixture was then closed in a quartz sample holder and annealed at 250 °C for 24 h in static vacuum. ATR spectra were recorded at room temperature within 40–60 min after annealing (denoted “S1 hm, annealed” in the text).
Infrared spectra were recorded on the single-reflection ALPHA-Platinum ATR (attenuated total reflection) instrument (BRUKER) with diamond crystal accessory. All infrared measurements were held in the glove box, using samples as such, at room temperature. The spectra were obtained in a 4000–400 cm−1 range at 2 cm−1 resolution. 64 scans were averaged for each spectrum and for the background.
To verify the phase composition of the mixtures after mixing and after annealing, the samples were sealed in 0.5 mm glass capillary and powder X-ray diffraction (PXRD) patterns were obtained in the 10–90° 2θ-region (within 1 h after treatment). PXRD patterns were collected with a X’Pert PRO MPD diffractometer (PANalytical), with a Cu Kα wavelength. Patterns were collected in Debye-Scherrer geometry at room temperature, placing the capillary with the sample on the rotating goniometer. PXRD data were analyzed by Rietveld refinement using FullProf Suite . The background was described by linear interpolation between selected points, while Gauss profile functions were used to fit the diffraction peaks. In the refinements, scale factors, unit cell parameters, profile parameters (U, V, W), the overall temperature factor and the background were refined.
Dissolution of LiCl in the hexagonal and orthorhombic LiBH4 were studied with ab initio calculations, thermodynamic modeling and infrared spectroscopy. According to our calculations, the enthalpy of mixing for the hexagonal phase is slightly negative, while that of the orthorhombic phase is positive. Overall, the thermodynamic effect of Cl substitution into the LiBH4 is negligible. Although computed infrared spectra do not give the possibility of punctual comparison and assignment of LiBH4-Cl solid solution modes, they clearly show that Cl does not affect the positions of BH4− fundamentals strongly. A minor effect is therefore expected for the stability of LiBH4 if the correlation between these properties is believed to exist. To our knowledge, this is the first infrared study of the phase transition from h- to o-LiBH4. The phase transition is observed at room temperature, due to the fact that the presence of Cl either decreases phase transition temperature or slows downs phase transition kinetics. Infrared spectra of the solid solution, obtained at ambient temperature shortly after annealing, have a profile characteristic for the high temperature hexagonal phase of LiBH4, where BH4− anions possess higher site symmetry. These spectra are also remarkably similar to those of LiBH4-LiBr and LiBH4-LiI solid solutions, where halides dissolve at high temperature in the hexagonal phase of LiBH4 and preserve this structure for a long time (months) at ambient temperature.
The authors thank Giuseppe Spoto (University of Turin) for useful discussion and critical reading of the manuscript. European Commission (contract NMP-2008-261/FLYHY, grant Agreement number 226943) financial support is highly appreciated.
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