Transfer of F− in the reaction of SF 6 − with SOF4: Implications for SOF4 production in corona discharges

The temperature (T) and electric field-to-gas pressure (E/P) dependences of the rate coefficientk for the reaction SF ₆ ^– +SOF₄SOF ₅ ^– +SF₅ have been measured. ForT<270 K,k approaches a constant of 2.1×10^–9 cm³/s, and for 433>T>270 K,k decreases withT according tok (cm³/s)=0.124 exp [–3.3 lnT(K)]. ForE/Pk has a constant value of about 2.5×10^–10 cm³/s, and for 130 V/cm·torr>E/P>60 V/cm·torr, the rate is approximately given byk (cm³/s)7.0×10^–10 exp (–0.022E/P). The measured rate coefficient is used to estimate the influence of this reaction on SOF₄ production from negative, point-plane, glow-type corona discharges in gas mixtures containing SF₆ and at least trace amounts of O₂ and H₂O. A chemical kinetics model of the ion-drift region in the discharge gap is used to fit experimental data on SOF₄ yields assuming that the SF ₆ ^– +SOF₄ reaction is the predominant SOF₄ loss mechanism. It is found that the contribution of this reaction to SOF₄ destruction falls considerably below the estimated maximum effect assuming that SF ₆ ^– is the predominant charge carrier which reacts only with SOF₄. The results of this analysis suggest that SF ₆ ^– is efficiently deactivated by other reactions, and the influence of SF ₆ ^– +SOF₄ on SOF₄ production is not necessarily more significant than that of other slower secondary processes such as gas-phase hydrolysis.     

Gas-phase reactions in plasmas of SF6 with O2: Reactions of F with SOF2 and SO2 and reactions of O with SOF2

The plasma chemistry of SF₆/O₂ mixtures is particularly complicated because of the large number of possible reactions. Over a wide range of conditions, products including SF₄, SOF₄, SOF₂, and SO₂F₂ can be formed but thre is considerable uncertainty about the major reactions which contribute to the formation of these species. In this work reactions of oxygen atoms with SOF₂ and fluorine atoms with SOF₂ and SO₂ have been studied in order to determine the principal sources of SO₂F₂ in these plasmas. Reactions were studied at 295 K in a gas flow reactor sampled by a mass spectrometer. No reaction could be detected between oxygen atoms and SOF₂, which for the conditions employed, means that the upper limit for the reaction rate coefficient is 1×10^–14 cm³ sec^–1. The reaction of fluorine atoms with SOF₂ was studied with the helium bath gas number density ranging from 3.1×10¹⁶ to 2.0×10¹⁷ cm^–3. Within this range the rate coefficient increased with increasing [He] from (4.1 to 10.8)×10^–14 cm³ sec^–1. SO₂ was found to react with fluorine atoms with a rate coefficient which appeared to be independent of the helium bath gas number density over the range given above. The possibility that this reaction occurred entirely on the walls of the reactor is discussed.     

Molybdenum complexes of biochemical iinterest. New coordination complexes of oxomolybdenum(V) with the tridentate ONO donor schiff bases derived from salicylaldehydes and ethanolamine

Summary New oxomolybdenum(V) complexes MoOCIL (where LH₂ = Schiff base) derived from ethanolamine and salicylaldehyde, 5-chlorosalicylaldehyde, 5-bromosalicylaldehyde, 5-nitrosalicylaldehyde, 3-ethoxysalicylaldehyde and 2-hydroxy-1-naphthaldehyde have been synthesized and characterised by elemental analyses, conductance, molecular weight, i.r. and electronic spectra and magnetic measurements. The Schiff bases behave as dibasic tridentate ONO donor ligands. The complexes are non-electrolytes and dimers. The complexes exhibit subnormal magnetic moments and are involved in antiferromagnetic exchange withS=0 ground state. The complexes exhibit electronic spectral bands atca. 13000 andca. 17000 cm^–1 due to the transitionsd _xy d _xz,yz (²B₂ ²E) andd _xy d _x ²–y² (²B₂ ²B₁), respectively. The (Mo=O) frequency of the complexes is observed in the 900–970 cm^–1 region. On the basis of the magnetic susceptibility, i.r. and molecular weight data a dimetallic structure with alcoholic oxygen atoms as the bridging atoms is suggested.Abbreviations sal salicylaldehyde - 5-chlorosal 5-chlorosalicylaldehyde - 5-bromosal 5-bromosalicylaldehyde - 5-nitrosal 5-nitrosalicylaldehyde - 3-ethoxysal 3-ethoxysalicylaldehyde - hydroxy 2-hydroxyl-1-naphthaldehyde     

The influence of solvation on the calculated activation energy for the reaction CH3F+F−

The influence of the solvent on the activation energy of the synchronous, concerted, narcissistic reaction: CH₃F + F^–¦CH₃F₂&#x00A6;^–FCH₃+F^–, has been investigated by means of CNDO/2 method. The reaction path has been fully followed in vacuo, and at a suitable point only, of reaction coordinate, in solution. The geometries of H₂O, F^–, CH₃F, and ¦CH₃F₂¦^–, in vacuo and in different hydrated cages, have been optimized.

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Zusammenfassung Der Einfluß des Lösungsmittels auf die Aktivierungsenergie der synchronverlaufenden Reaktionen CH₃F+F^–¦CH₃F₂¦FCH₃+ F^–, wurde mit der CNDO/2 Methode geprüft. Der Reaktions-Ablauf wurde in Vakuum vollkommen und in der Lösung an einem geeigneten Punkt der Reaktionskoordinate durchgeführt. Die Geometrien von H₂O, F^–, CH₃F, und ¦CH₃F₂¦^– im Vakuum und in verschiedenen hydrierten Käfigen wurden optimalisiert.

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Résumé L'influence du solvent sur l'énergie d'activation de la réaction synchronique, concertée, narcissistique: CH₃F+ F^–¦CH₃F₂¦^–FCH₃+F^– a été examinée par la méthode CNDO/2. On a suivie l'entier chemin de réaction in vacuo, alors qu'on a observé un seul point convenable de la coordonée de réaction en solution. On a optimize les geometries de H₂O, F^–, CH₃F, et ¦CH₃F₂¦^– in vacuo et en differentes cages hydratés.

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Financial aid from Italian Centro Nazionale delle Ricerche is gratefully acknowledged.     

Gas-phase reactions in plasmas of SF6 with O2 in He

Processes which occur in microwave discharges of dilute mixtures of SF₆ and O₂ in He have been examined using a flow reactor sampled by a mass spectrometer. Two classes of experiments were performed. In the first set of experiments, mixtures containing 6×10¹¹ cm^–3 SF₆, 6×10¹⁶ cm^–3 He, and O₂ in the range (0–3.6)×10¹³ cm^–3 were passed through a 20-W 2450-MHz microwave discharge. The gas mixtures arriving at a sample point downstream from the discharge were examined for SF₆, SF₄, SOF₂, SOF₄, SO₂F₂, SO₂, F, and O. In the second class of experiments, rate coefficients were measured for the reactions of SF₄ with O and O₂ and for the reaction of SF with O. The rate coefficient for the reaction of SF with O was found to be (4.2±1.5)×10^–11 cm^–3 s^–1. SF₄ was found to react so slowly with both oxygen atoms and oxygen molecules that only upper limits could be placed on the rate coefficients for these reactions. These values were 2×10^–14 cm³ s^–1 and 5×10^–15 cm³ s^–1 for reactions with O and O₂ respectively. The observed distribution of products from the discharged mixtures is discussed in terms of the measured rate coefficients.     

Negative ion formation in compounds relevant to SF6 decomposition in electrical discharges

Dissociative and nondissociative electron attachment in the electron impact energy range 0–14 eV are reported for SOF₂ SOF₄, SO₂F₂, SF₄, SO₂, and SiF₄ compounds which can be formed by electrical discharges in SF₆. The electron energy dependences of the mass-identified negative ions were determined in a time-of-flight mass spectrometer. The ions studied include F^– and SOF ₂ ^–* from SOF₂; SOF ₃ ^– and F^– from SOF₄; SO₂F ₂ ^–* , SO₂F^–, F ₂ ^– , and F^– from SO₂F₂; SF ₄ ^–* and F^– from SF₄; O^–, SO^–, and S^– from SO₂; and SiF ₃ ^– and F^– from SiF₄. Thermochemical data have been determined from the threshold energies of some of the fragment negative ions. Lifetimes of the anions SOF ₂ ^–* , SO₂F ₂ ^–* , and SF ₄ ^–* are also reported.     

Low temperature absorption spectra of CrO 4 = in K2SO4 and VO 4 ≡ in Na3PO4 · 12H2O

The polarized absorption spectrum of the chromate ion has been measured at liquid hydrogen and helium temperatures. With chromate dissolved in K₂SO₄ evidence is found for two orbitally allowed ¹ A ₁¹ T ₂ electronic absorption bands. The first band is split into three sublevels with the 0-0 lines located at 26,316 cm^–1, 26,441 cm^–1 and 26,610 cm^–1. Built upon the 0-0 lines is seen a simple progression in quanta of 783 cm^–1. The second transition is nearly featureless, and is found at 34,000 cm^–1 to 44,000 cm^–1. The two bands are assigned as primarily t ₁2e and as 3t ₂2e respectively.VO ₄ dissolved in Na₃PO₄ · 12H₂O showed at liquid nitrogen temperature a broad featureless band found between 30,000 and 40,000 cm^–1.

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Zusammenfassung Das polarisierte Absorptionsspektrum des Chromations wurde bei den Temperaturen des flüssigen Wasserstoffs und Heliums gemessen. Für Chromat in K₂SO₄ werden zwei erlaubte Absorptionsbanden ¹ A ¹¹ T ₂ gefunden. Die erste Bande ist dreifach aufgespalten, ihre 0-0 Linien liegen bei 26316 cm^–1, 26441 cm^–1 und 26610 cm^–1. Von den 0-0 Linien ausgehend zeigt sich eine einfache Zunahme der Werte um 783 cm^–1. Der zweite Übergang ist nahezu strukturlos, er liegt zwischen 34000 cm^–1 und 44000 cm^–1. Die beiden Banden werden überwiegend t ₁2e bzw. 3t ₂2e zugeordnet. VO ₄ in Na₃PO₄ · 12H₂O zeigt bei der Temperatur des flüssigen Stickstoffs eine breite strukturlose Bande zwischen 30 000 und 40 000 cm^–1.

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Résumé Le spectre d'absorption en lumière polarisée de l'ion chromate a été mesuré aux températures de l'hydrogène et de l'hélium liquide. Pour le chromate dissous dans K₂SO₄ on met en évidence deux bandes d'absorption électronique de transition orbitale permise ¹ A ₁¹ T ₂. La première bande est séparée en trois sous niveaux dont les raies 0-0 se trouvent à 26,316 cm^–1, 26,441 cm^–1 et 26,610 cm^–1. A partir des raies 0-0 on distingue une période de 783 cm^–1. La seconde bande est presque non structurée et s'étend de 34,000 cm^–1 à 44,000 cm^–1. Les deux bandes sont décrites comme t ₁2e et 3t ₂2e respectivement.VO ₄ dissous dans Na₃PO₄ · 12H₂O révèle à la température de l'azote liquide une large bande sans structure entre 30,000 et 40,000 cm^–1.

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On leave of absence from Anorganisch Chemisch Laboratorium der Universiteit, Amsterdam.     

Pure rotational spectrum of PH3 in the 10–100 cm−1 range: Collisional broadening coefficients by H2 and He

The H₂- and He-broadened widths have been measured at room temperature for seven pure rotational lines of phosphine in the spectral range 10–80 cm^–1. The retrieval of linewidths values was carried out, on the assumption of identical linewidths for theJ+1K-components within a given multipletJ+1J. The results obtained are in good agreement with the previous determination reported for the 10 line, in the microwave range.     

Error of Atomic Charges Derived from Electrostatic Potential

The purpose of this article is to show that CHELP, CHELPG, and Merz and Kollman undergo error for the charge on atoms of HCOO^– (H₂O) _n for n = 1 6. We also demonstrate that the CHELP, CHELPG, and Merz and Kollman show error for the tendency toward change in the charges on carbons for CH₃NH⁺ ₃ (CH₃)₂NH⁺ ₂ (CH₃)₃NH⁺ (CH₃)₄N⁺.     

Anomalies of the partition coefficient and properties of crystals in the region of low concentrations of an isomorphous admixture. 1. Unusual decomposition of solid solutions of the NaCl—CdCl2 system

Solid solutions NaCl—CdCl₂ were studied in an interval of CdCl₂ concentrations of 0.05—3 mol.% by Raman spectroscopy. The molecular form Na₂CdCl₄ decomposes: Na₂CdCl₄ 2Na⁺ + Cd²⁺ + 2Cl₂ ^– + 2e^–; 2Na + 2e^– 2Na⁰. Free sodium atoms form color centers of crystal (F centers) in the region of jumpwise changing the partition coefficient of CdCl₂ in NaCl (K jump).     

Electron scattering and dissociative attachment by SF6 and its electrical-discharge by-products

Discrete electron-molecule processes relevant to SF₆ etching plasmas are examined. Absolute, total scattering cross sections for 0.2–12-eV electrons on SF₆, SO₂, SOF₂, SO₂F₂, SOF₄, and SF₄, as well as cross sections for negative-ion formation by attachment of electrons, have been measured. These are used to calculate dissociative-attachment rate coefficients as a function ofE/N for SF₆ by-products in SF₆.     

Kinetics of formation of sulfur dimers in pure SF6 and SF6-O2 discharges

The emission band spectra of S, molecule (B³ _u ^– X³ _g ^– transition) and of SO molecule (A³ X^3–) were detected in SF₆ and SF₆-O₂ rf discharges. It has been observed that the presence of a material which can be etched by SF₆ products considerably enhances the density of S₂ in the reactor. By means of mass spectrometry it has been shown that the m/e =83 mu signal assigned to S₂F⁴ ions evolves exactly in the same manner as the S₂ band intensity during the etching of Si or W in SF₆-O₂ discharge. A reaction scheme involving S₂F radicals is proposed to explain these experimental results.     

By-product formation in spark breakdown of SF6/O2 mixtures

The yields of SOF₄, SO₂F₂, SOF₂, and SO₂ have been measured as a function of O₂ content in SF₆/O₂ mixtures, following spark discharges. All experiments were made at a spark energy of 8.7 J/spark, a total pressure of 133 kPa, and for O₂ additions of 0, 1, 2, 5, 10, and 20% to SF₆. Even for the case of no added O₂, trace amounts of O₂ and H₂O result in the formation of the above by-products. However, addition of O₂ significantly increases the yields of SOF₄ and SO₂F₂, while SOF₂ is only slightly affected. The net yields for SOF₄ and SO₂F₂ formation range from 0.18×10^–9 and 0.64×10^–10 mol·J^–1, respectively, at 1% O₂ content to 10.45×10^–9 and 7.15×10^–10 mol·J^–1, respectively, at 20% O₂ content. The mechanism for SOF₄ production appears to involve SF₄, an important initial product of SF₆, as a precursor. Comparison of the SOF₄ and SO₂F₂ yield from spark discharges (arc and corona) shows that the yields from other discharges (arc and corona) shows that the yields can vary by at least three orders of magnitude, depending on the type of discharge and on other discharge parameters.     

CEPA calculations on open-shell molecules. V. The vibration frequencies of SF and SCl

Ab initio calculations for the ² ground states of SF and SCl have been performed on Hartree-Fock level and with inclusion of valence shell correlation effects by means of the CI and CEPA approaches. The calculated properties are: Equilibrium distances, vibration frequencies, and dipole moment curves in the vicinity of the respective equilibrium geometries. Our best estimates for the 0 1 infrared absorption frequencies _o for SF and SCl are 786 cm^–1 and 520 cm^–1, respectively, both with an uncertainty of about 10 cm^–1. This confirms a recent experimental value obtained by Willner for SF (791 cm^–1), but indicates that for SCl both experimental values reported previously in the literature (617 cm^–1 and 574 cm^–1) are wrong. The S—F and S—Cl bonds in SF and SCl are very similar to the ones in SF₂ and SCl₂, being essentially single p-bonds in either case. In the analogous oxygen-halogen molecules the situation is different, the O—F and O—Cl bonds in the diatomic radicals OF and OCl have partial double bond character and are much stronger than those in OF₂ and OCl₂ or in HOF and HOCl.     

Effect of the Nature of a Sodium-Conducting Solid Electrolyte on the Impedance of Its Interface with the SmCo0.8Ti0.2O3 Oxide Electrode in an Oxygen Atmosphere

Impedance spectroscopy is employed for studying the behavior of the interface of the SmCo_0.8Ti_0.2O₃ semiconducting oxide electrode with a sodium-conducting solid electrolyte (Na⁺–SE) in atmospheres of argon and oxygen. Compounds with the susceptibility to hydration decreasing in the row Na₅TbSi₄O₁₂ Na₃Zr₂Si₂PO₁₂ Na₃Sc₂(PO₄)₃ are used as the Na⁺–SE. Only the systems containing the Na₅TbSi₄O₁₂ solid electrolyte, the grain surfaces of which acquire boundary layers formed by hydration products, are sensitive to oxygen. The exchange current of the electrode reaction O₂ (g) + e O₂ ^– increases from 1.8 to 19 mA/cm² in the temperature interval 250–300°C. The systems with Na⁺–SE that are not prone to hydration remain inactive in the oxygen atmosphere probably due to quick blocking of the active centers by nonconducting products of the secondary chemical reaction Na⁺ + O₂ ^– NaO₂.     

Rate Coefficient for Self-Association Reaction of CF2 Radicals Determined in the Afterglowof Low-Pressure C4F8 Plasmas

We have analyzed decay kinetics of CF₂ radicals in the afterglow of low-pressure, high-density C₄F₈ plasmas. The decay curve of CF₂ density has been approximated by the combination of first- and second-order kinetics. The surface loss probability evaluated from the frequency of the first-order decay process has been on the order of 10^–4. This small surface loss probability has enabled us to observe the second-order decay process. The mechanism of the second-order decay is self-association reaction between CF₂ radicals (CF₂+CF₂C₂F₄). The rate coefficient for this reaction has been evaluated as (2.6–5.3)×10^–14 cm³/s under gas pressures of 2 to 100 mTorr. The rate coefficient was found to be almost independent of the gas pressure and has been in close agreement with known values, which are determined in high gas pressures above 1 Torr.     

Low temperature absorption spectra of KMnO4 in KClo4

The permanganate spectrum has been remeasured at liquid hydrogen and helium temperatures using spectrographs with reasonably high dispersion. Evidence is found for four absorption band systems. The first one is assigned as ¹ A ₁ ¹ T ₂ and displays a great deal of vibrational structure starting with the 0–0 line located at 18,072 cm^–1. The second transition found at 25,000 to 30,000 cm^–1 is rather featureless. The third transition with maximum at 33,000 cm^–1 shows a simple progression in quanta of 750 cm^–1. The fourth band is completely featureless with maximum intensity at 43,500 cm^–1. These findings are compared with a simplified SCF LCAO MO calculation.

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Zusammenfassung Das Permanganat-Spektrum wurde bei Temperaturen von flüssigem Wasserstoff und Helium unter Verwendung eines ausreichend auflösenden Spektrographen neu vermessen, wobei vier Absorptionssysteme gefunden wurden. Dem ersten von ihnen wurde ein ¹ A ₁ ¹ T ₂-Übergang zugeordnet; es besitzt eine ausgeprägte Vibrationsstruktur (0–0-Bande bei 18,072 cm^–1, während das folgende zwischen 25,000 und 30,000 cm^–1 kaum eine Struktur zeigt. Der dritte Übergang mit Maximum bei 33,000 cm^–1 zeigt einfache Progressionen entsprechend Quanten von 750 cm^–1. Die vierte Bande schließlich ist vollkommen strukturlos und hat ihr Maximum bei 43,500 cm^–1. Diesen Daten wurden die Ergebnisse einer einfachen SCF-LCAO-MO-Rechnung gegenübergestellt.

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Résumé Le spectre du permanganate de potassium a été réétudié aux températures de l'hydrogène et de l'hélium liquide en utilisant des spectrographes à dispersion raissonnablement élevée. On trouve la preuve de la présence de quatre systèmes de bandes d'absorption. Le premier, attribué à ¹ A ₁ ¹ T ₂, possède une forte structure vibrationnelle commencant à la bande 0–0 située à 18.072 cm^–1. La seconde transition située entre 25.000 et 30.000 cm^–1 est plutot sans structure. La troisième transition avec un maximum à 33.000 cm^–1 présente une progression simple de 750 cm^–1. La quatrième bande est complètement sans structure et a son maximum vers 43.500 cm^–1. Ces observations sont comparées avec un calcul simplifié SCF LCAO MO.

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NATO Postdoctoral Fellow 1965–66.     

Calculs non empiriques sur une réaction SN2 typique

Résumé On a calculé la structure électronique de l'état initial et de l'état de transition de la réaction de substitution F^–+CH₃FFCH₃+F^– par la méthode des orbitales moléculaires SCF dans l'approximation gaussienne. On trouve que l'énergie de l'état de transition est inférieure à la somme des énergies des produits séparés CH₃F et F^–. Cependant, cette contribution négative à l'énergie d'activation est contrebalancée par la variation des énergies de solvatation.

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Ab initio calculations on a typical SN₂ ReactionElectronic structure of methyl fluoride and of the transition state (FCH₃F)^–

The electronic structure of the initial and transition states of the substitution reaction F^–+CH₃F FCH₃+F^– have been calculated by the SCF molecular orbital method in the Gaussian approximation. It is found that the energy of the transition state is lower than the sum of the energies of the separated systems CH₃F and C^–. However, this negative contribution to the activation energy is balanced by the variation of solvatation energies.

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Zusammenfassung Die Elektronenstruktur des Ausgangs- und des Übergangszustandes der Substitutionsreaktion F^–+CH₃FFCH₃+F^– wurden mit einer SCF-MO-Methode mit Gaußfunktionen berechnet. Die Energie des Übergangszustandes ist niedriger als die Summe der Energien der separierten Systeme CH₃F und F^–. Dieser negative Beitrag zu der Aktivierungsenergie wird allerdings ausgeglichen durch eine Änderung der Solvatationsenergie.

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Remerciements. Nous remercions bien sincèrement M. A. Rassat (CEN, Grenoble) de nous avoir suggéré ce problème et M. Ph. Millie (ENS, Paris) de nous avoir apporté des éléments de discussion constructifs.     

Structure,vibrational spectra,and energetic stability of LnX<Stack><Subscript>4</Subscript><Superscript>−</Superscript></Stack> ions (Ln=La,Lu; X=F,Cl, Br,I)

Molecular structure and properties of La and Lu tetrahalide ions LnX ₄ ^– ) are studied by the configuration interaction singles-and-doubles method augmented with quadruple excitation correction (CISD+Q) and by the fourth-order Möller-Plesset perturbation theory with account for single, double, triple, and quadruple excitations (SDTQ-MP4). The atomic inner shells are described by Stevens relativistic effective core potentials. Valence basis sets are augmented with diffuse s-, p-, and polarization d-, f-, and g-functions. The equilibrium configuration of nuclei in LnX ₄ ^– ions was found to be tetrahedral. The equilibrium internuclear distances, quadratic force constants, vibrational frequencies, and IR intensities of LnX ₄ ^– ions are compared with the corresponding parameters of La and Lu trihalide molecules (LnX₃), calculated within the same approximations. Regularities in the behavior of molecular parameters on going along the LnF ₄ ^– LnCl ₄ ^– LnBr ₄ ^– LnI ₄ ^– series and from La compounds to Lu compounds are revealed. Heights of the energy barriers to the LnX ₄ ^– inversion through the square planar structures (T _d D _4h T _d ) are evaluated: 100–110 and 130–150 kJ/mol for LaX ₄ ^– and LuX ₄ ^– , respectively. Enthalpies of dissociation reactions LnX ₄ ^– LnX₃+X^– are calculated and the results obtained are compared with the available experimental data.Translated from Koordinatsionnaya Khimiya, Vol. 31, No. 3, 2005, pp. 218–228.Original Russian Text Copyright © 2005 by Solomonik, Smirnov, Mileyev.This revised version was published online in April 2005 with a corrected cover date.This revised version was published online in April 2005 with a corrected cover date.     

Raman spectra in the libration region of concentrated aqueous solutions of lithium-6 and lithium-7 halides. Evidence for tetrahedral Li(OH2) 4 +

The Raman spectra of saturated solutions of⁶LiCl and⁷LiCl have been decomposed into Gaussian components, one of which is a polarized band that occurs at 360 cm^–1 when the ion is⁶Li⁺ and shifts to 335 cm^–1 when the ion is⁷Li⁺. Equivalent bands occur in the spectra of saturated solutions of⁶LiBr and⁷LiBr at 343 and 320 cm^–1, respectively. These bands are assigned to solvent-separated ion aggregates. The Raman spectra of 8.0 and 3.5 m solutions of the isotopic lithium chlorides have been decomposed into five Gaussian components, three of which are assigned to water librations. In addition, there is a polarized band at 440 cm^–1 independent of the lithium isotope used, and a depolarized band which occurs at 385 cm^–1 in the⁶LiCl solutions and 360 cm^–1 in the⁷LiCl solutions. We interpret these two additional bands as theA ₁ andF ₂ stretching modes of Li⁺ tetrahedrally solvated by water molecules.