Long and short range spin-spin interactions in ErBaCuO

Dipolar spin-spin interactions play a crucial role as for the magnetic order in the compounds of the RBa₂Cu₃O_6+x family, (R = Dy, Er, Nd). However, inelastic neutron scattering data observed in ErBa₂Cu₃O₇ can be explained only if exchange interactions in addition to dipolar ones are taken into account. Received: 12 January 1998 / Received in final form: 26 March 1998 / Accepted: 10 April 1998     

Dispersion coefficients for interactions between two metastable helium-like ions

The dispersion coefficients C₆, C₈ and C₁₀ for the interactions between helium and helium-like ions in the metastable states of 2 ¹S and 2 ³S with Z up to 10 are calculated using variational wave functions in Hylleraas coordinates.     

Fluorescence enhancement of Eu3+ by Tb3+ in dimethylsulfoxide (DMSO)

Photoexcitation of EuCl₃.6H₂O and TbCl₃.6H₂O mixtures in DMSO at various wavelengths brings about a decrease in the fluorescence intensity of Tb³⁺ and a subsequent enhancement in the fluorescence intensity of Tb³⁺ provided that [Tb³⁺] < [Eu³⁺]. The average value of the electronic excitation energy transfer rate constant k₁₀ which was found to be independent of the excitation wavelength, was determined to be about 1.50 × 10³ M^-1 s^-1. Photoexcitation of Tb³⁺ and subsequent population of high energy excited states is accompanied by rapid nonradiative de-excitation processes to the lowest excited state ⁵D₄, which is the origin of the energy transfer process. A lower limit for the value of the reaction rate constant, associated with the transition ⁵D₃ ? ⁵D₄, namely k₅, is of the order of 10⁵ ?10⁶ s^-1. Excitation at conditions leading to the exclusive population of the ⁵D₄ state of Tb³⁺ gave rise to a value of k₁₀ equal to (2.2 ± 0.4) × 10³ M^-1 s^-1 and a critical separation (R₀)_exp between Tb³⁺ and Eu³⁺ of about 13 Å. A theoretical value of R₀ equal to 14.2 Å was calculated. The energy transfer process does not appear to take place via clear cut dipole-dipole interactions but rather via complex multipole and/or exchange interactions.     

Synthesis and characterization of hybrid nanocomposites of polypyrrole filled with iron oxide nanoparticles

Hybrid polypyrrole (PPy)/α-Fe₂O₃ nanocomposite films were fabricated by spin coating on a glass substrate. X-Ray diffraction analysis revealed the crystalline structure of α-Fe₂O₃ nanostructures and the nanocomposites. The broad PPy peak weakened in intensity as the α-Fe₂O₃ content increased in PPy/α-Fe₂O₃ nanocomposites. Characteristic Fourier-transform IR peaks for pure PPy shifted to higher wavenumbers on addition of α-Fe₂O₃ to PPy/α-Fe₂O₃ nanocomposites. This can be attributed to better conjugation and interactions between PPy and α-Fe₂O₃ nanoparticles. Field-emission scanning electron microscopy, transmission electron microscopy, and atomic force microscopy images of the nanocomposites reveal a uniform distribution of α-Fe₂O₃ nanoparticles in the PPy matrix. UV-vis absorption spectroscopy revealed a blue shift from λ_max= 441 nm for PPy to λ_max= 392 nm for PPy/α-Fe₂O₃, reflecting strong interactions between PPy and α-Fe₂O₃ nanoparticles. The room-temperature dc electrical conductivity increased from 4.33×10⁻⁹ to 1.81×10⁻⁸ S/cm as the α-Fe₂O₃ nanoparticle content increased from 10 to 50 wt.% in PPy/α-Fe₂O₃ nanocomposites.     

Longitudinal nuclear spin relaxation in solids in a triply rotating coordinate system: Selective observation of the multispin dipole contribution

The longitudinal nuclear spin relaxation in an effective magnetic field H _e3 acting in a triply rotating coordinate system is recorded. Rotating and doubly rotating coordinate systems are employed for strong suppression of the secular nuclear dipole interactions in the first two orders and for separation of higher-order interactions (four-and five-spin). Experiments on protons in polycrystalline benzene showed that the contribution of such multispin dipole interactions to this relaxation can be observed selectively as a pronounced local minimum in the temperature dependence of the relaxation time. This contribution correponds to ultraslow molecular motions with rates ≃ γH _e3≃2π(10¹−10³) s⁻¹ and can be employed to study such motions in detail, including for purposes of identification of the form of the motion. Pis’ma Zh. éksp. Teor. Fiz. 64, No. 5, 335–340 (10 September 1996)     

129Xe contact shift in oxygen gas

We have determined the temperature dependence of σ₁ of ¹²⁹Xe in oxygen gas. These results were obtained by measurement of the resonance frequency of ¹²⁹Xe in gas samples of known densities in Xe and O₂. The shift of the resonance frequency due to Xe-Xe interactions has been measured in pure Xe gas samples with improved precision. This allows the determination of σ₁(Xe-O₂) by subtracting out the known effect of Xe-Xe interactions in mixed Xe-O₂ samples. σ₁(Xe-O₂) values are reported here for the temperature range 220 to 440 K. The values of σ₁(Xe-O₂) are adequately described by the polynomial function in p.p.m. amagat^-1 σ₁(Xe-O₂) = - 1·061 + 3·64 × 10^-3τ - 2·19 × 10^-5τ² + 9·58 × 10^-8τ³ - 2·08 × 10^-10τ⁴, where τ = (T - 300 K). It is found that the temperature dependence of σ₁(Xe-O₂) can be interpreted in terms of a contact interaction between Xe and the paramagnetic O₂ molecule.     

Crystal field and exchange interactions in rare earth transition metal salen compounds containing bipyridine, pyrazole complexes

Crystal field parameters for Pr³⁺ in {[Ni(salen)Pr-(hfac)₃](H₂O)} (noted as NiPr) and {[Ni(salen)Pr(hfac)₃(pyr)]-(CHCl₃)} (noted as NiPrpyr) have been found from a fit to the thermal variation in the magnetic susceptibility of NiPr and NiPrpyr. The nature of exchange interaction in [Cu(salen)Pr(hfac)3(pyr)] (noted as CuPrpyr), {[{Cu(salen)Pr(hfac)₃}₂(pyz)](H₂O)₃} (noted as Cu₂Pr₂pyz) and {[{Cu(salen)Pr(hfac)₃}₂(bpy)]-(CHCl₃)₂} (noted as Cu₂Pr₂bpy, bpy=4,4_-bipyridine) have been found using the derived results for NiPr and NiPrpyr. All the exchange interactions give significant contribution to the thermal variation in magnetic susceptibility below 50 K. The contribution due to Pr-Cu interaction is positive while that of the Cu-Cu and Pr-Pr interactions are negative. The behaviors below 10 K for Pr-Cu and Pr-Pr are difficult to explain, and point to a possible change in structure of CuPrpyr, Cu₂Pr₂pyz and Cu₂Pr₂bpy below 10 K. The theoretical thermal variations in the magnetic specific heat of NiPr and NiPrpyr are computed and discussed.     

Noncommutative Heat Kernel

Schrödinger operators on Sobolev spaces are considered as new solvable models with point interactions. A simple formula for the deficiency indices of a minimal Schrödinger operator with point interactions is given. Examples of point interactions on the space W₂¹( ³) are constructed.Mathematical Subject Classification (2000). 37J10, 47A10     

Hadron weak interactions at high energy and the parton model

It is shown that, within the parton picture, weak (P-odd) effects increase with energy and momentum transfer. The presence of an effctive current with ΔS = 0 and 1 due to constituent interchange or annihilation is expected in the parton picture of hadron-hadron weak interactions. A typical value of P-odd effects, nucleon or hyperon polarization or asymmetry in quasi two-body reactions is about 10^?4 at E_lab ～ 10³ GeV and 10^?3 in large angle (t ～ s) scattering in the conventional current × current scheme of weak interactions. A principal possibility to clear up quark statistics is pointed out.     

Final results from the ντ appearance search in the NOMAD experiment

An updated analysis of the full NOMAD data corresponding to 1.35 × 10⁶ charged current interactions has been performed to search for neutrino oscillations through ν_τ appearance. This document updates the recently published results on the ν_μ → ν_τ and ν_μ → ν_e oscillations search in NOMAD [1] with a unified analysis of the hadronic channels.     

Three-body interaction between an atom and a monolayer film

An atom (B) situated near a plane of atoms (A) experiences an interaction potential energy V = (V₂ + V₃ + … The leading term is the sum over the monlayer of 2-body interactions. We compute here the 3-body correction V₃. Numerical results are presented for the case of noble gases, H and CH₄. For H or He near a Xe layer, V₃ reduces the well depth by ~ 10%.     

Structural Investigation of (5-Amino-1,3,4-thiadiazolyl-2-thionato)trimethyltin(IV): 1D Chains Generated by Hydrogen Bonding

ABSTRACT

The geometry of the four-coordinated Sn atom in the title compound, (CH₃)₃Sn(C₂H₂N₃S₂), is distorted tetrahedral with three Sn–C bonds and one Sn–S bond. Two crystallographically distinct molecules a and b within the asymmetric unit are hydrogen bonded. Intermolecular “N–H?N” hydrogen bond interactions generate infinite 1D chains consisting of alternating, centrosymmetric R2,2(8) and R4,2(10) rings.     

Room-temperature fluorescence quenching of indoles by trivalent lanthanide ions in dimethyl sulfoxide

Quenching of the room-temperature fluorescence excitation and emission spectra of indole, 3-carbinolindole, 5-methoxyindole, and 3-methylindole in dimethyl sulfoxide by trivalent lanthanide ions Ln³⁺ was interpreted in terms of dynamic interactions between (¹L_a, ¹L_b) states of indoles and Ln³⁺. The fluorescence lifetimes of these indoles vary from 5.3 to 8.4 ns, according to their structure. Quenching rate constants (k_Q) range between 2.6×10⁸ and 1.7×10¹⁰ M⁻¹s⁻¹. Values of k_Q are significantly larger for Eu³⁺ and Yb³⁺ than for other lanthanide ions.     

Relaxation studies using selective excitation double Mössbauer techniques

We have developed a technique for studying time dependent hyperfine interactions using selective excitation double Mössbauer (SEDM) procedures. The measured relaxation time between the two spin orientations of the iron atoms in α-Fe₂O₃ at the Morin transition is 1.1 ± 0.2 × 10^-7 sec.     

Associated charm production in neutrino–nucleus interactions

In this paper a search for associated charm production both in neutral and charged current ν-nucleus interactions is presented. The improvement of automatic scanning systems in the CHORUS experiment allows an efficient search to be performed in emulsion for short-lived particles. Hence a search for rare processes, like the associated charm production, becomes possible through the observation of the double charm-decay topology with a very low background. About 130000 ν interactions located in the emulsion target have been analysed. Three events with two charm decays have been observed in the neutral-current sample with an estimated background of 0.18±0.05. The relative rate of the associated charm cross-section in deep inelastic ν interactions, σ(cc̄ν)/σ_NC ^DIS=(3.62^+2.95 _-2.42(stat)±0.54(syst))×10^-3 has been measured. One event with two charm decays has been observed in charged-current ν_μ interactions with an estimated background of 0.18±0.06 and the upper limit on associated charm production in charged-current interactions at 90% C.L. has been found to be σ(cc̄μ^-)/σ_CC<9.69×10^-4.     

Anomalous magnetocaloric effect in van vleck paramagnet HoVO<Subscript>4</Subscript> near energy level crossing

The anomalous magnetocaloric effect in singlet rare-earth paramagnets near energy level crossing has been experimentally observed for the first time. The magnetization and differential magnetic susceptibility of Ho_{1 ? x} Y _x VO₄ crystals (x = 0, 0.5) measured along the tetragonal axis in a pulsed magnetic field with various change rates near the crossover field, dH/dt, from 3 × 10³ to 2.5 × 10² T/s are compared to the data in static magnetic fields down to 0.1 K. These data indicate the large negative magnetocaloric effect in the pulsed magnetic field, so that the crystal with the initial temperature T ₀ = 4.2 K is cooled much lower than 1 K. The experimental data are qualitatively described in the crystal field model with various interactions including hyperfine interactions and with the known interaction parameters.     

Synthesis and magnetic properties of Cu3B2O6 single crystals

The temperature dependence of the magnetic susceptibility of Cu₃B₂O₆ single crystals grown by spontaneous crystallization from a melt consisting of a mixture of CuO and B₂O₃ and the behavior of their magnetization are investigated in magnetic fields up to 55 kOe. A broad susceptibility maximum is observed near 39 K, and a sharp drop in susceptibility is observed at T<10 K. The paramagnetic Néel temperatures for all orientations of the magnetic field in the crystal investigated are negative, attesting to the predominantly antiferromagnetic character of the exchange interactions. The effective magnetic moment of the Cu²⁺ ion is anisotropic and lies in the range from 1.054μ _B to 1.545μ _B. The magnetization depends linearly on magnetic field at T>10 K, whereas at temperatures below 10 K a discontinuity is observed at fields of the order of 40 kOe. At room temperature, electron magnetic resonance characterized by an almost isotropic g factor (g=2.165) is detected at 36.22 GHz. The exchange interactions in Cu₃B₂O₆ are analyzed on the basis of the Goodenough-Kanamori rules. The possibility of the establishment of a singlet magnetic state in the crystal is analyzed. Fiz. Tverd. Tela (St. Petersburg) 41, 677–679 (April 1999)     

Analysis of the ν9/ν10 band system of allene

The infrared spectrum of allene has been recorded with high resolution (0.002-0.004 cm⁻¹) on a Fourier transform instrument in the region 730 to 1170 cm⁻¹ containing the perpendicular bands, ν₉ and ν₁₀. A total of 21 subbands with KΔK ranging from −6 to +14 have been assigned in the ν₉ band, and 26 subbands with KΔK = −10 to +15 have been assigned in the ν₁₀ band. The bands are affected by a combination of a J_z-Coriolis and a quartic anharmonic interaction between their upper states ν₉ and ν₁₀. In addition, several other more localized perturbations are found in the spectrum. The nature of the interactions responsible for these perturbations is discussed, and five of the strongest perturbations are quantitatively accounted for by constructing a Hamiltonian matrix which includes five different perturbing states and their Coriolis and anharmonic resonances with the ν₉ and ν₁₀ upper states. A set of spectroscopic constants for the ν₉ and ν₁₀ states and for some of the perturbing states is reported.     

Nuclear spin-lattice relaxation in the triply rotating frame and ultraslow molecular motions in solids

A method for measuring nuclear magnetic spin-lattice relaxation in solids in the effective field H_e3 acting in the triply rotating frame (TRF) is described. The method advances the previously described techniques whereby nuclear magnetic resonance and relaxation in the rotating (RF) and doubly rotating frames (DRF) are measured directly. In the present work, the RF and DRF are employed for suppressing the secular part of nuclear dipole-dipole (DD) interactions in the first two orders. As a result, the higher-order DD interactions (four- and five-particle ones) were separated, and their contribution to the nuclear spin-lattice relaxation in the TRF was studied experimentally. The experiments were carried out on protons in polycrystalline benzene. With the introduced technique, an overall spin-lattice relaxation decay in the TRF was recorded continuously during a single radio-frequency pulse with a length not exceeding 1 s. The contribution of multiproton nonsecular DD interactions to the proton spin-lattice relaxation in the TRF was observed selectively as a pronounced local minimum in the temperature dependence of the relaxation timeT _1ϱϱϱ. This contribution corresponds to ultraslow motion of benzene molecules with a rate about γH_e3 ≈ 2π · (10¹-10³) s^-1 and is determined quantitatively by specific correlation functions corresponding to the multiparticle nonsecular DD interactions of protons. The prospects of using this method for studying ultraslow atomic and molecular dynamics in solids are discussed.     

Nuclear resonance fluorescence from the 58keV level in159Tb

The half-life of the 58keV level of¹⁵⁹Tb was determined by classical resonance absorption using the centrifuge technique and by Mössbauer spectroscopy measuring the natural line width and found to beτ _1/2=(58±10)ps. Mössbauer spectra for Tb and Tb₂O₃ absorbers and for Dy₂O₃ and GdFe₂ sources were investigated for temperatures between 9 and 385 K. Results for hyperfine interactions and Debye Waller factors are given. The Debye Waller factors are compared with predictions obtained from other experimental results.