Far-infrared spectra of alkaline-earth fluorenone triple ions in solution

Tetrahydrofuran solutions of 9-fluorenone show new absorption bands in the far-infrared region after contact with alkaline-earth amalgams. These bands can be ascribed to the interionic antisymmetric stretching vibration of triple ions, the internal vibration of the fluorenone anion coupled with the interionic vibration for the triple ions, and the vibrations of the higher-ion clusters.     

Esr studies of crown complexed semiquinone ion pairs in solution

ESR spectra of alkyl-substituted p-benzosemiquinone anion radicals produced by sodium reduction in the presence of 18-crown-6 in tetrahy drofuran show, remarkable temperature and concentration dependences, not observed in the absence of the crown. The observed spectral changes are interpreted in terms of equilibria between structurally different ion pairs.     

Raman spectra of biphenyl negative ion in tetrahydrofuran solution

Raman spectra of the mono-negative ion of biphenyl in tetrahydrofuran solution were obtained by Ar⁺, He–Ne and Kr⁺ laser exciting lines. The observed frequency shift from the neutral molecule and intensity enhancement by resonance Raman effect is discussed on the basis of MO considerations.     

Dynamic properties of metallocenium ion pairs in solution by atomistic simulations

We report a molecular dynamics study of the dynamics and energetic of the [H(2)Si(Cp)(2)ZrMe(+)][MeB(C(6)F(5))(3)(-)], IP1, and [Me(2)Si(Cp)(2)ZrMe(+)][B(C(6)F(5))(4)(-)], IP2, ion pairs in benzene. The metrical parameters obtained for the IP1 ion pair are in excellent agreement with the NMR data reported for the strictly related [Me(2)Si(Cp)(2)ZrMe(+)][MeB(C(6)F(5))(3)(-)] ion pair (J. Am. Chem. Soc. 2004, 126, 1448). This validates the molecular modeling protocol we developed. Simulation of the IP2 ion pair suggests that the counterion oscillates between two geometries characterized by a different coordination pattern of the F atoms to the Zr cation. In one case the B(C(6)F(5))(4)(-) coordinates to the metal with two F atoms of the same aryl ring, whereas in the other case two F atoms of different aryl rings are involved in the coordination. Strong solvent reorganization occurs around IP1 and IP2, as well as around the two isolated cations. In the case of the two ion pairs solvent is never coordinated directly to the metal, whereas in the absence of the counterion one benzene molecule is coordinated to the metal through a cation-pi interaction. Free energy calculations result in ion pair free energies of separation of 36.8 and 23.3 kcal/mol for IP1 and IP2, respectively. Simulations with the Zr-B distance fixed at values > 7 A have been also performed. This mimics the situation occurring after counterion displacement by an inserting monomer molecule during olefin polymerization by the title catalysts.     

The stereoregularity of polystyrenes obtained by different ion pairs of polystyryl alkali salts

The stereoregularity of polystyrenes obtained with sodium, potassium, rubidium, and cesium naphthalenes in various solvents was determined by ¹³C-NMR spectroscopy. Polystyrenes produced by contact ion pairs of polystyryl cesium in dioxane and tetrahydrofuran (THF) had the proportions of a 57–58% racemic dyad (P_r), whereas the P_r values increased to 65 and 69% by solvating Cs⁺ counterions in dimethoxyethane and by agent-separating them with crown ether, respectively. Polystyrene obtained by contact ion pairs of polystyryl sodium in dioxane showed a P_r of 66%; polymers produced by solvent-separated ion pairs of polystyryl sodium in THF at ?78°C had a P_r of 71%. A polymerization system which contained alkali counterions with large ionic radii and solvents with low dielectric constants in which only contact ion pairs existed produced polystyrenes with isotactic-rich configurations. The stereoregularity of polystyrene produced by contact ion pairs of polystyryl potassium and rubidium in tetrahydropyran (THP) occurred intermediately between that of polymers obtained in diethyl ether and THF. It was concluded that the stereoregulation of contact ion pairs may be closely related to the interionic distance of the ion pair.     

Far-infrared spectra of piezoelectric polyvinylidene fluoride

Poly(vinylidene fluoride) (PVF₂) is currently used to form piezoelectric films. The PVF₂ molecule can exist in more than one stable conformation and it has electrically polar groups making the polymer amenable to the electrification processes involved in the formation of the piezoelectric film. The two crystalline forms of PVF₂ are distinguishable by far-infrared spectroscopy. Polarized far-infrared spectra (1000-50 cm^?1) of uniaxially oriented PVF₂ show changes in the strong perpendicular dichroism in a number of absorptions before and after being made piezoelectric. The dichroism is attributed to a structural rearrangement from a staggered trans-gauche-trans-gauché conformation to a planar zig zag conformation. In the latter conformation the permanent dipoles are oriented approximately at right angles to the surfaces of the film and result in an electrically polarized film.     

Cation migration between two unequivalent sites in 4-cyano pyridine alkali metal ion pairs

The ESR spectra of 4-cyanopyridine alkali metal ion pairs were recorded at different temperatures. The different hyperfine components are selectively broadened by a dynamic process which affects the linewidths. The analysis of the linewidth parameters has been accomplished as due to a jumping process of the cation between two unequivalent positions. An ab initio calculation of the potential energy surface of the radical anion shows that the motion should take place between two positions near the two nitrogen atoms in the molecular plane. Modulation of the anisotropic interactions by the tumbling motion of the ion pair cannot explain the observed data.     

Amphiphilic organic ion pairs in solution: a theoretical study.

The macroscopic manifestation of hydrophobic interactions for amphiphilic organic ion pairs (tetraalkylammonium-anion) has been shown experimentally by measuring their association constants and their affinity with the organic phase. Beyond a certain size, there is a direct relation between association constants and chain lengths in tetraalkylammonium ions. We propose to cast a bridge between these results and geometrical properties considered at the level of a single ion pair by means of quantum chemistry calculations performed on model systems: trimethylalkylammonium-pentyl sulfate instead of tetraalkylammonium-dodecyl sulfate. Two limiting cases are considered: head-to-head configurations, which yield an optimal electrostatic interaction between polar heads, and parallel configurations with a balance between electrostatic and hydrophobic interactions. All properties (geometries, complexation energies, and atomic charges) were obtained at the MP2 level of calculation, with water described by a continuum model (CPCM). Dispersion forces link hydrocarbon chains of tetraalkylammonium ions and pentyl sulfate, thus yielding (for the largest ion pairs) parallel configurations favored with respect to head-to-head geometries by solute-solvent electrostatic interactions. Given the small experimental association energies, we probe the accuracy limit of the MP2 and CPCM methods. However, clear trends are obtained as a function of chain length, which agree with the experimental observations. The calculated monotonic stabilization of ion pairs when the hydrocarbon chain increases in length is discussed in terms of electrostatic interactions (between ions and between ion pairs and water), dispersion forces, and cavitation energies.     

Far-infrared studies of ion clustering in ionomers

The far-infrared spectra of polystyrene methacrylic acid/(PSMA) ionomers have been investigated as a function of cation and ion-site concentration to obtain spectroscopic evidence of domain formation. A far-infrared band, due to the vibration of a higher-order cluster, is found at 170 cm^?1in Na⁺-form PSMA. This band, which is observed in addition to the known cation-motion bands, is assigned to the vibrations of aggregates involving many cations and anionic sites close together, and the results are discussed in light of ion aggregation models.     

Origin of additional satellites in electron paramagnetic resonance spectra of rare earth ion pairs

Electron Paramagnetic Resonance (EPR) spectrum of pairs of two identical rare earth ions is considered in the case where the two ions feel slightly different crystal fields giving different g factors. When the differences Δg between the g factors give a Zeeman difference term ΔgβB₀ of the order of magnitude of the interaction between the two ions, the pair spectrum is composed of four lines instead of two: the usual doublet structure, and two additional satellites around the main central transitions. It is shown that for rare earth ions, the shape of the EPR pair spectrum is very sensitive to small g factor differences. This situation is illustrated by the case of neodymium pairs in the SrAl₁₂O₁₉ host.     

Far-infrared spectra of some β-hydroquinone clathrates

Far-infrared spectra (400-30 cm^?1) of Nujol mulls of the β-hydroquinone clathrates containing the following guest molecules were investigated: formic acid, formic acid-d₂, methanol, methanol-d₄, acetonitrile, acetonitrile-d₃, sulphur dioxide and also both of methanol and sulphur dioxide. The observed infrared bands of the mulls in the region of 4000-30 cm^?1 were classified into those due to the host lattice and those due to the guest molecules. On the basis of the comparison of the spectra, some bands were assigned to the translational or the rotational vibrations of guest molecules. Appearance of those bands suggested that some guest molecules are considerably bound in the cavities of the host lattice. Effect of temperature change on the bands was also measured.     

The structure of the ion pairs of the carbanion of indene with alkali metal cations

NMR spectra have been measured of the Li⁺, Na⁺ and K⁺ ion pairs of the indenyl carbanion in 1,2-dimethoxyethane and tetrahydrofuran as a function of temperature. The changes of the chemical shifts are explained in terms of the detailed structure of the ion pairs. The results in both solvents strongly suggest that in indenyl-Li⁺ the counterion is predominantly located over the six-membered ring. In THF the preferred position of the cations Na⁺ and K⁺ in the contact ion pairs seems to be the five-membered ring.     

Raman spectra of isotopic bisulfite and disulfite ions in alkali salts and aqueous solution

The Raman spectra of solid lithium, sodium, potassium, cesium, rubidium, and ammonium disulfite and of rubidium and cesium bisulfite were recorded and compared with the spectrum of an aqueous solution saturated with 1.2m K₂S₂O₅. Deuterium, ³⁴S₈, and ¹⁸O₂ were used to label cesium bisulfite, CsHSO₃, cesium disulfite, Cs₂S₂O₅, and potassium disulfite. All six fundamentals of the bisulfite ion were observed and assigned. Eleven of the fifteen expected fundamentals of the disulfite ion were observed and correlated to older experimental data, as well as recent calculations. Isotope shifts confirm assignments in the SO stretching region. In the low frequency region, assignment is less conclusive and two frequencies have been tentatively reassigned.     

Far-infrared spectra of lanthanide complexes with 8-hydroxyquinoline

Summary Vibrational spectra of lanthanide oxines have been measured in the far-infrared region. In addition, the similar yttrium complex was investigated for further experimental evidence for the proposed band assignments. The most important metal-oxygen and metal-nitrogen bond vibrations have been attributed to absorptions between 390–350 cm^–1 and 210–170 cm^–1, respectively.

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Ferne IR-Spektren von Lanthanidenkomplexen mit 8-Hydroxychinolin

Zusammenfassung Es wurden die Vibrationsspektren von Lanthanid-Oxinen im fernen IR-Bereich gemessen. Zusätzlich wurde der analoge Yttrium-Komplex untersucht, um die Bandenzuordnungen experimentell zu stützen. Die wichtigsten Metall-Sauerstoff- und Metall-Stickstoff-Bindungsschwingungen wurden den Absorptionen zwischen 390–350 cm^–1 und 210–170 cm^–1 zugeordnet.

     

Far-infrared and Raman spectra ofpseudo-tetrahedral complexes of ethylenedimorpholene

Summary The far-i.r. and Raman spectra of a closely related group ofpseudo-tetrahedral complexes of general formula [MX₂EDM] are reported (M = Co^II, Ni^II, Cu^II, Zn^II; X = Cl or Br). EDM, ethylenedimorpholene, acts in these compounds as a bidentate nitrogen donor. The main skeletal vibrations are assigned under the approximate symmetry of theC _2v (MX₂Y₂) point group.     

Theoretical IR spectra of ionized naphthalene

We report the results of a theoretical study of the effect of ionization on the IR spectrum of naphthalene, using ab initio molecular orbital theory. For that purpose we determined the structures, band frequencies, and intensities of neutral and positively ionized naphthalene. The calculated frequencies and intensities allowed an assignment of the most important bands appearing in the newly reported experimental spectrum of the positive ion. Agreement with the experimental spectrum is satisfactory enough to take into consideration the unexpected and important result that ionization significantly affects the intensities of most vibrations. A possible consequence on the interpretation of the IR interstellar emission, generally supposed to originate from polycyclic aromatic hydrocarbons (PAHs), is briefly presented.     

Tuning of the structure and emission spectra of upconversion nanocrystals by alkali ion doping

Recently, lanthanide based nanocrystals with upconversion fluorescence emission have attracted a lot of interest and the nanocrystals have been used for bioimaging, biodetection, and therapeutic applications. Use of the nanocrystals for multiplexed detection has also been explored; however, nanocrystals with multicolor emission are required. Some efforts have been made to tune the emission spectra of the nanocrystals based on manipulation of upconverting lanthanide ions doped in the crystals or creation of core/shell structures. In this work, alkali ions with an ionic radius slightly larger or smaller than Na such as Li and K were doped into NaYF(4):Yb,Er nanocrystals and their effect on the crystal structure and subsequently the upconversion emission spectra were studied. It was found that the phase transition occurs in the nanocrystals when a different amount of Li and K was doped. Furthermore, the intensity ratios between the blue, green, and red emission peaks changed accordingly, and make it possible to tune the upconversion fluorescence of the nanocrystals by Li and K doping.