Sternheimer free determination of the47Ti nuclear quadrupole moment from hyperfine structure measurements

The hyperfine structure (hfs) of 12 metastable states of⁴⁷Ti has been measured by laser induced fluorescence. 11 of these states have been measured additionally very precisely by a laser-rf double resonance method. Taking into account results of earlier hfs measurements, the hfs of altogether 17 fine structure states has been analyzed by the simultaneous parametrization of the one- and two-body interactions in the atomic hfs for the model space (3d+4s) ^N+2 (N=2). This gives 16 parameters for the magnetic dipole interaction and 12 parameters for the electric quadrupole interaction. From the model space parameters, obtained from the hfs fit, the nuclear quadrupole momentQ(⁴⁷Ti)=0.303(24b), has been evaluated at the first time; it is free of Sternheimer corrections up to second order.     

Hyperfine structure measurements of the metastable (3d 6 4s 2)3 H 4, 5, 6 states of57Fe: Configuration interaction in the hyperfine structure of the iron atom

We report the hyperfine structure (hfs) measurement of the metastable (3d ⁶ 4s ²)a ³ H _{4, 5, 6} states of⁵⁷Fe. The kHz-precision of these experimental results together with the hyperfine structure values of (3d ⁶ 4s ²)a ⁵ D _{1, 2, 3, 4}, (3d ⁷ 4s)a ⁵ F _{2, 3, 4, 5}, and (3d ⁷ 4s)a ³ F _{2, 3, 4}, which were measured earlier, allowed to determine a very detailed set of effective radial parameters describing the hfs of these states, using a new parametrization method. This method treats one- and two-body contributions to the hfs separately. In this way configuration interaction effects in the hfs of the⁵⁷Fe atom can be studied in detail and compared with configuration interaction effects in the fine structure of the same atom.     

Reanalysis of the Am I level spectrum and the nuclear quadrupole moments of Am-isotopes

The fine structure (fs) and hyperfine structure (hfs) level scheme of Am I is reanalysed using a semi empirical fitting procedure which incorporates experimental data. Especially new laserspectroscopic measurements of the hfs of some electronic transitions in the Am atom enables us to make a more detailed analysis of 5f ⁷ 7s 7p fine structure in Am I. In particular a relation is given between theB-factor values and the value of the nuclear electric quadrupole moment of²⁴¹Am independent of a calibration by results of nuclear spectroscopy.     

Laser-Rf double-resonance measurements of the metastable 3d 34s 5P1,2,3, 3d 24s 2 1 G 4 states of 47Ti

The hyperfine structure (hfs) of 4 metastable states of ⁴⁷Ti has been measured very precisely by a laser-rf double resonance method. The corresponding hyperfine structure constants A _exp and B _exp have supplied a set of experimental data necessary for hyperfine structure analysis and determination of Sternheimer free nuclear quadrupole moment Q.     

Single crystal ERP and powder endor spectra of a five coordinated low-spin Co(II) schiff base complex: N,N'-ethylene-bis (salicylideniminato)-cobalt(II

The magnetic parameters g and A^Co of Cosalenpy doped in a Znsalenpy single crystal have been measured and the orientations of their principal axes with respect to the molecular structure have been determined. Furthermore, the hfs and quadrupole tensor of the axial nitrogen were obtained from powder ENDOR. Data are discussed using well-established theories.     

Precise determination of the ground state hyperfine structure splitting of43Ca II

Within the framework of systematic hyperfine structure (hfs) investigation of titanium atom the hfs-splittings of 3d ³(² G)4s b ¹ G ₄ levels for two stable isotopes⁴⁷Ti and⁴⁹Ti have been studied. 5 hfs intervals for each isotope have been measured using ABMR-LIRF method (atomic beam magnetic resonance detected by laser induced resonance fluorescence) with an accuracy of about 300 Hz. TheJ-off-diagonal second order perturbation effects have been taken into account in the interpretation. Upper limit of the contributions from octupole and hexadecapole hyperfine structure interaction to hfs intervals of this level have been estimated to be about 400 Hz. However, for most of hfs intervals these contributions are almost within experimental error and in order to study such effects a more precise experimental method should be used.     

Isotope shift and hyperfine structure of stable platinum isotopes

Isotope shift (IS) and hyperfine structure (hfs) measurements have been performed on seven lines of the platinum I spectrum with interference as well as laser fluorescence spectroscopy. In the latter case a frequency-doubled single-mode cw dye laser was applied. The IS of¹⁹⁰Pt with a natural abundance of only 0.01% was determined to beδν ^{190, 192}=?38.65(8) mK in theλ306.47 nm transition. The IS parameters and the effective hfs integrals in the configuration (5d+6s)¹⁰ were determined in intermediate coupling by a least squares fit of the IS and hfs data with eigenvectors obtained from the platinum fine structure (fs). The results are compared with theoretical values and yield improvedδ〈r ²〉 data.     

Hyperfine structure investigations in excitedD-states of171Yb and173Yb

The hyperfine structure splittings in the excited 4f ¹⁴6s6d states of¹⁷¹Yb and¹⁷³Yb have been measured. Isotope selection was achieved by stepwise laser excitation of the¹ D ₂ and³ D _{2, 1} states. The³ D ₃ state of¹⁷¹Yb was excited via collisional excitation of an intermediate level. The magnetic and electric hfs coupling constants are given and compared to ab initio values calculated from relativistic self-consistent-field wavefunctions.     

HFS and isotope shift in the atomic spectrum of205Pb

The hfs of²⁰⁵Pb in the 283.3-nm resonance line and its isotope shift (IS) have been measured in absorption with the use of dispersive spectroscopy. A new method for calibration and analysis, when internal standards are not available is described. The results are: hfs interaction constantsA=70.3(5)×10^?3 cm^?1,B=?0.6(1.1)×10^?3 cm^?1,²⁰⁵Pb-²⁰⁸Pb IS=?123.9(2.0)×10^?3 cm^?1. The derived nuclear magnetic dipole moment,μ=0.704(5)μ _N is in good agreement with values calculated with a nuclear configuration mixing model.     

Doppler-free laserspectroscopic investigations of hyperfine structure in the atomic cobalt spectrum

Performing Doppler-free laserspectroscopic investigations in the red wavelength region (640–670 nm) we were able to determine 10A-factors and 9B-factors of atomic cobalt levels. Now precise values of 18A-factors and 16B-factors of levels belonging to the configurations (3d+4s)⁹ are known. Fitting of the one-electron radial parameters to introduce agreement between experimental and theoretical hfs constants allows the prediction of hfs constants of not yet investigated fine structure levels. Values of the electric quadrupole moment of the Co⁵⁹ nucleus are determined in two electron configurations. The resulting mean value of the spectroscopic quadrupole moment isQ=0.35(3) barn.     

Study of the hyperfine structure of Titanium atom by laser induced fluorescence on an atomic beam

Within the framework of systematic hyperfine structure (hfs) investigation of titanium atom the hfs splitting of 3d ³4s ³H_4,5,6 levels for two stable isotopes ⁴⁷Ti and ⁴⁹Ti have been measured by laser induced fluorescence. Experimental hfs constants A _exp and B _exp have been determined. The hfs measurements confirm an existence of a significant spin-dependent interaction effect on hfs structure of the level 3d ³ 4s ³H₄.     

Laser and radiofrequency spectroscopy of the 5d 4 6s 6 D multiplet in Ta I

The hyperfine structure (hfs) of¹⁸¹Ta has been investigated using laser radio-frequency double resonance and high resolution laser spectroscopy on collimated atomic beams. The magnetic dipole and electric quadrupole hyperfine structure coupling constants of the 5d ^{4 6} s 6D _{3/2, 5/2, 7/2, 9/2} metastable states have been determined using radio-frequency spectroscopy. In the 5d ⁴ 6s ⁶ D _1/2 metastable state and the excited 5d ³ 6s 6p ⁴ D _3/2,⁶ D _{5/2, 9/2} as well as the unidentified 28 182.6 cm^–1 and 30 021.2 cm^–1 states, hfs constants have been obtained from high resolution laser spectroscopy. A radio-frequency converter has been developed in order to reach the frequency region 2.7–10 GHz.     

Hyperfine structure of the 4f 7 (8 S 0) 6s 7 S 3 0 level in151,153Eu II by fast ion beam — laser spectroscopy

The hyperfine structure (hfs) of the level 4f ⁷(⁸ S ⁰) 6s ⁷ S ₃ ⁰ in^151,153Eu II has been measured with collinear fast ion beam — laser spectroscopy. The hfs of the⁷ S ₃ ⁰ level has been measured with interferometric methods previously but, to our knowledge, this is the first measurement with the laser ion beam technique. In the present experiment the hfs of the 4f ⁷(⁸ S ₇ ^2/0 ) 6p _1/2 levels were also obtained. Corresponding magnetic dipole and electric quadrupole coupling constantsA andB are evaluated.     

Accurate time-resolved laser spectroscopy on silver atoms

The lifetimes of the silver 5p ² P states have been measured with high accuracy by time-resolved laser spectroscopy using the delayed coincidence technique. Also, the hyperfine structure of¹⁰⁷Ag and¹⁰⁹Ag in these two states has been studied by observing quantum beats.     

Polarization spectroscopy of Sr79Br and Sr81Br: Analysis of theX 2 Σ + andB 2 Σ + hyperfine structure

Microwave optical polarization spectroscopy has been used to measure the hyperfine structure in theX ² Σ ⁺ (v=0) electronic ground state of Sr⁷⁹Br and Sr⁸¹Br. Optical hyperfine structure in theB ² Σ ⁺?X ² Σ ⁺ (0,0) system was resolved by Doppler-free laser polarization spectroscopy. The magnetic hyperfine parametersb andc and the electricquadrupole hfs parametereqQ were determined for theX ² Σ ⁺ andB ² Σ ⁺ states of both molecules. The magnetic hfs has been interpreted as an effect of halide electron spin polarization. The electric quadrupole coupling constants are compared with the alkali halides and discussed in terms of Sternheimer antishielding in polar molecules.     

The hyperfine structure of the predissociated stateB′0+ of IBr

TheB′0⁺ state of IBr is strongly predissociated which leads to fragmentary rovibrational structure and level broadening. Using Doppler free laser polarization spectroscopy, the hyperfine structure of the sharpest rotational lines of several band fragments in theB′?X system was investigated for the first time. The hyperfine analysis yields a strong vibrational dependence of the nuclear quadrupole interaction for Br and the nuclear spin-rotation interaction for I and Br. The magnitude of the hyperfine parameters and their variation with vibrational state are discussed in a configuration model for the bound and repulsive states according to the observed predissociation.     

Hyperfine structure constants and isotope shift of the levels of the configuration 4f 6 5d 6s 2 in Eu I

The hyperfine structure (hfs) and the isotope shift (IS) of transitions between metastable levels of the configuration 4f ⁷ 5d 6s and levels of the configuration 4f ⁶ 5d 6s ² of¹⁵¹Eu and¹⁵³Eu were studied by means of the high resolution laser-atomic-beam technique. New data for the hfs in¹⁵¹Eu and¹⁵³Eu were obtained as well as new and more accurate for the IS between¹⁵¹Eu and¹⁵³Eu. The measured hfs constantsA andB of the 4f ⁶ 5d 6s ² configuration allow to perform a parametric analysis using the Sandars and Beck theory. The value of the Sternheimer correction is also disscused.     

Nuclear spin-spin coupling in the spectrum of I2 at 6328 Å

The effects of nuclear spin-spin coupling are included in the analysis of the nuclear hyperfine structure of the R(127) line of the 11-5 band in the B-X electronic band system of I₂. The fit to the experimental data is improved over earlier fits in which only the effects of nuclear spin-rotation interaction and nuclear electric quadrupole coupling were considered. The electron-coupled contribution to the spin-spin constant of the upper state is determined to be d_E = ?36.3 ± 8.5 kHz. However, the fit (standard deviation = 59.8 kHz) is still not at the level of the experimental precision (40 kHz) and further measurements are in progress to test the model used for the hfs hamiltonian.     

Expanding the Averievite Family, (MX)Cu5O2(T5+O4)2 (T5+ = P,V; M = K,Rb, Cs,Cu; X = Cl,Br): Synthesis and Single-Crystal X-ray Diffraction Study

Averievite-type compounds with the general formula (MX)[Cu₅O₂(TO₄)], where M = alkali metal, X = halogen and T = P, V, have been synthesized by crystallization from gases and structurally characterized for six different compositions: 1 (M = Cs; X = Cl; T = P), 2 (M = Cs; X = Cl; T = V), 3 (M = Rb; X = Cl; T = P), 4 (M = K; X = Br; T = P), 5 (M = K; X = Cl; T = P) and 6 (M = Cu; X = Cl; T = V). The crystal structures of the compounds are based upon the same structural unit, the layer consisting of a kagome lattice of Cu²⁺ ions and are composed from corner-sharing (OCu₄) anion-centered tetrahedra. Each tetrahedron shares common corners with three neighboring tetrahedra, forming hexagonal rings, linked into the two-dimensional [O₂Cu₅]⁶⁺ sheets parallel to (001). The layers are interlinked by (T⁵⁺O₄) tetrahedra (T⁵⁺ = V, P) attached to the bases of the oxocentered tetrahedra in a “face-to-face” manner. The resulting electroneutral 3D framework {[O₂Cu₅](T⁵⁺O₄)₂}⁰ possesses channels occupied by monovalent metal cations M⁺ and halide ions X⁻. The halide ions are located at the centers of the hexagonal rings of the kagome nets, whereas the metal cations are in the interlayer space. There are at least four different structure types of the averievite-type compounds: the P-3m1 archetype, the 2 × 2 × 1 superstructure with the P-3 space group, the monoclinically distorted 1 × 1 × 2 superstructure with the C2/c symmetry and the low-temperature P2₁/c superstructure with a doubled unit cell relative to the high-temperature archetype. The formation of a particular structure type is controlled by the interplay of the chemical composition and temperature. Changing the chemical composition may lead to modification of the structure type, which opens up the possibility to tune the geometrical parameters of the kagome net of Cu²⁺ ions.