The low temperature quadrupole orientation of103Ru in ruthenium

The quadrupole frequencyv _Q =e ² qQ/h of¹⁰³Ru (Z=44,N=59) in a ruthenium single crystal has been measured using the technique of low temperature quadrupole orientation to bev _Q (¹⁰³RuRu)=−14.7(5) MHz. Temperatures below 2 mK were reached in this experiment using a PrNi₅ demagnetization stage attached to a³He−⁴He dilution refrigerator. Using the measured magnitude of the RuRu electric field gradient (EFG) at low temperatures |eq(RuRu)|=1.02(3)×10¹⁷ V.cm⁻² [1] and adopting the sign ofeq(RuRu) to be negative from systematics, this result yields a value for the ground-state electric quadrupole moment of¹⁰³Ru ofQ(¹⁰³Ru)=+0.59(2) b. This moment may be interpreted using the weak coupling model of de-Shalit [2]. A Korringa constant for¹⁰³RuRu ofC _K=39(6) Ks was measured in this experiment. Taking advantage of a small iridium contamination of the ruthenium single crystal, the quadrupole moment of the¹⁹²Ir ground state was determined to beQ(¹⁹²Ir)=+2.12(25) b. The sign of the IrRu electric field gradient was found to be negative as a result of this work.     

Quadrupole Interaction of 99Ru in Pr,Nd and 100Rh in Tb Hosts

The electric field gradient at transition element impurities ⁹⁹Ru and ¹⁰⁰Rh in metallic rare earth hosts Pr, Nd and Tb has been investigated by time differential perturbed angular correlation (TDPAC) technique at room temperature. The electric field gradients, calculated from the measured quadrupole interaction frequencies at room temperature, are; RuPr: 6.06×10¹⁷ V/cm², RuNd: 5.83×10¹⁷ V/cm² and RhTb: 5.40×10¹⁷ V/cm². The electronic enhancement factors (α) for RuPr and RuNd are about 2.5 times the value observed in RuGd and RhTb (it is found to be more than 40 as in RhGd). The results cannot be explained in terms of the existing models based on charge transfer or volume mismatch of the impurity and the host. This revised version was published online in September 2006 with corrections to the Cover Date.     

Sign of the electric field gradient at111Cd in Zr and Sb

The Β-γ TDPAC technique was applied to¹¹¹Ag implanted in Zr and Sb metal single crystals in order to determine sign and magnitude of the quadrupole interaction at the site of¹¹¹Cd in these metals. An analysis of the data taken at 293K yielded Ν_Q=+15.4(6) MHz for¹¹¹Cd in Zr and Ν_Q=?107.5(20) MHz for¹¹¹Cd in Sb. From these values electric field gradients of +7.3(8)×10¹⁶ V/cm² and ?5.56(62)×10¹⁷ V/cm² for Cd in Zr and Sb are derived respectively.     

Quadrupole interaction at Ta and lattice location of Hf in Be

The time-differential perturbed angular correlation technique (TDPAC) has been applied to the 482 keV excited state of¹⁸¹Ta, to determine the nuclear electric quadrupole interaction (QI) at Ta in Be. Sources were prepared by ion-implantation of¹⁸¹Hf in Be. Particle channeling measurements have revealed that. Hf impurities implanted in Be reside primarily at the tetrahedral interstitial site. The fundamental QI frequency obtained for Ta at this interstitial site in Be is |v _Q| =e ² qQ/h = 227.0 ± 2.2 MHz which corresponds to an electric field gradient |eq|=(3.71±0.15)×10¹⁷ V/cm². This result is discussed in terms of results for Cd impurities in the same system and the systematics of the impurity QI in metals.     

The quadrupole interaction at181Ta in Zn

The quadrupole interaction (QI) in hexagonal close packed zinc lattice was measured using the 482 keV, 10.6 ns probe state of¹⁸¹Ta employing the time-differential perturbed angular correlation technique. The electric field gradient (EFG) at¹⁸¹Ta in Zn was derived from the measured quadrupole interaction frequency at room temperature asV _zz =12.202×10¹⁷ V/cm². The quadrupole interaction measured at various temperatures displayed normal temperature dependence similar to that seen by this probe in many non-cubic hosts.     

Electric quadrupole orientation of iridium isotopes in rhenium

The quadrupole frequenciese ² qQ/h, for^{186, 188–190}Ir in a Re single crystal have been determined by nuclear orientation at temperatures down to 2 mK. Using a modeldependent value of +1.0 b for the quadrupole moment of the ground state of¹⁸⁹Ir, the electric field gradient of IrRe at 0 K is found to be–3.6×10¹⁷ V·cm^–2. The value is consistent with systematics proposed by Raghavan et al. Using this EFG, quadrupole moments are deduced for^{186, 188, 190}Ir.     

LMR quadrupole interaction measurement on69mGe and71mGe in Zn

A new experimental set-up to perform in-beam LMR (Level Mixing Resonance) measurements is briefly outlined. The first results are reported here. The quadrupole interaction of^69mGeZn is measured and in good agreement with earlier measurements:v _Q=80.6(4) MHz; for^71mGeZn, the valuev _Q=33.1(30)MHz is found. In addition, the relaxation behaviour and radiation damage of Ge recoil implanted in Zn is studied.     

Static electric quadrupole interaction of Ta- and Hf-ions in barium and lead titanate

The static electric quadrupole interaction of¹⁸¹Ta and¹⁷⁸Hf in polycrystalline barium and lead titanate at the site of titanium has been measured using time differential PAC and the Mössbauer effect. The electric field gradients (EFG) at room temperature at the¹⁸¹Ta nucleus are ¦V _zz¦=(3.6±0.2)·10¹⁷V/cm² in BaTiO₃ and ¦V _zz¦=(14.6±0.6)·10¹⁷ V/cm² in PbTiO₃. The temperature dependence of the quadrupole interaction has been studied giving the following EFG values: ¦V _zz¦=(2.4±0.2)·10¹⁷ V/cm² in the monoclinic and ¦V _zz¦=(1.1±0.3)·10¹⁷ V/cm² in the rhomboedral phase of BaTiO₃, and ¦V _zz¦=(15.7±0.6)·10¹⁷ V/cm² for¹⁸¹Ta/PbTiO ₃ at 77 °K. The EFG of¹⁷⁸Hf in PbTiO₃ has been derived from a Mössbauer effect experiment to beV _zz=+(10.7±0.5)·10¹⁷ V/cm². The results are compared with EFG's calculated in a point charge model and with experimental EFG's measured at⁴⁴Sc and⁵⁷Fe in the same titanates by other authors. Contributions of covalent bonds to the effective EFG's in perovskit crystals are discussed.     

Temperature dependence of the quadrupole interaction of69GeTl and113SnSn

The quadrupole interaction constants of⁶⁹GeT1 and¹¹³SnSn were measured by means of the perturbed angular distribution technique as a function of temperature in the range of 80KT508 K and 80KT480 K, respectively. Isomeric states in⁶⁹Ge and¹¹³Sn were populated by the heavy ion reactions⁵⁶Fe(¹⁶O, 2p n) and¹⁰⁰Mo(¹⁶O, 3n) and recoil implanted into polycrystalline Tl- and single crystalline Sn-backings. In the case of¹¹³SnSn, where the quadrupole coupling is weak, a special single crystal geometry was employed to enhance the sensitivity of the measurement. Within the limits of the errors the temperature dependence for both systems follows the empirical T^1.5-dependence. While a strong temperature dependence comparable to InIn is observed for⁶⁹GeT1, that for¹¹³SnSn is weaker than expected. The strength of the temperature dependence for¹¹³SnSn does not agree with the predictions of a lattice vibration model proposed recently for the temperature dependence of the quadrupole interaction.Supported in part by NSFAssociate of the Graduate Faculty of Rutgers University     

The electric field gradient at the nuclear site of177Lu in Zn and In

The electric quadrupole interaction frequencyν _Q =eQV _zz /h of¹⁷⁷Lu in single crystals of Zn and In has been measured by the method of low temperature nuclear orientation. The results are $$\begin{gathered} v_Q ({}^{177}Lu\underline {Zn} ) = - 180(5)MHz \hfill \\ v_Q ({}^{177}Lu\underline {In} ) = - 19(5)MHz. \hfill \\ \end{gathered} $$ With the known quadrupole moment of¹⁷⁷LuQ=3.39 (2) b we derive for the electric field gradientV _zz (Lu Zn)=?2.20 (5)×10¹⁷ V/cm² andV _zz (Lu In)=?0.23 (6)×10¹⁷ V/cm². The results are compared with magnetostriction measurements of silver single crystals doped with rare earth atoms.     

Quadrupole interaction of tantalum impurities in bismuth metal

The time differential perturbed angular correlation technique has been used in the measurement of the electric quadrupole interaction of Ta impuritiy in bismuth metal. The interaction frequencies at 293, 400 and 500 K have been observed to be 288±1.5, 266.9±3 and 244.5±4.3 MHz respectively. The electric field gradient at 293 K is 4.75±0.3 × 10¹⁷ V/cm² with the temperature coefficientB=2.2±0.2 × 10⁻⁵ (K)^−3/2.     

Electric quadrupole interactions in Ru-Sc alloys

In TDPAC studies of the electric quadrupole interaction in Ru_xSc_1–x alloys two different electric fieldgradients (EFG) have been observed at the site of⁹⁹Ru: V_zz(I)=12.6·10¹⁷ V/cm² and V_zz(II)=18.9·10₁₇ V/cm². The corresponding relative fractions f(I) and f(II), respectively, vary with the Ru concentration x. For low concentrations x<0.01 most nuclei (f(I)0.8) experience the smaller EFG V_zz(I). At x=0.01, however, the fraction f(I) goes abruptly to zero and V_zz(II) becomes dominant. In view of these results the previous interpretation of V_zz(II) as the EFG of dilute Ru on substitutional Sc sites can no longer be maintained. The Ru-Sc configurations producing these EFG's have not yet been identified. In the intermetallic compound Ru₂Sc the interaction is completely different, in RuSc₃, however, similar values have been observed.     

Double resonance NMR-on study on oriented188Ir in iron

The quadrupole splitting of oriented¹⁸⁸Ir in iron was studied at 8.6 mK using a double resonance NMR-ON method. With r.f. power applied at the strongest resonance frequency, a second frequency was used to simultaneously investigate the second resonance component, where the splitting is caused by an electric quadrupole interaction. The electric hyperfine splitting frequency ν_Q=e ² qQ/h was measured to be 3.37(11) MHz. With the known electric field gradient of −0.283(6)×10¹⁷ V/cm² at Ir in iron, the spectroscopic quadrupole moment of¹⁸⁸Ir was deduced to be 0.492(26)b. The present results show that the double resonance method is a powerful tool in establishing the quadrupole splitting, if it leads to well-resolved NMR-ON resonance components.     

Electric field gradient at100Rh in HCP zirconium and gadolinium

The measurement of QI frequencies at¹⁰⁰Rh in Zr and Gd reveal that the electronic contribution to the EFG is quite large. The value of ¦K¦ is 8 for¹⁰⁰RhZr whereas it is 45 for¹⁰⁰RhGd. The temperature variation of¹⁰⁰RhZr neither follows T^1.5 nor has a linear T dependence.     

Radiation damage in γ-Mo4O11

We investigated the radiation damage induced by thermal neutron capture of⁹⁸Mo in γ-Mo₄O₁₁ by measuring the⁹⁹Mo(β⁻)⁹⁹Tc nuclear quadrupole interaction by time differential perturbed angular correlations. At room temperature, a fraction of about 20% of all activated Mo-atoms exhibits a large quadrupole interaction of ω₁=550 Mrad/s and an asymmetry parameters of η≊0.75, practically independent of the dose in the range from 7.9·10¹⁶ to 7.8·10¹⁸ n/cm². We attribute this signal to Mo-atoms with a near-neighbour oxygen vacancy which was created in a knock-on process following prompt de-excitation by gamma emission after the thermal neutron capture.     

Quadrupole interaction studies of Hg in Sb

Time differential perturbed angular correlation and nuclear orientation studies of the electric quadrupole interaction for Hg in Sb have been performed. The effective field gradients |V _zz ^eff (HgSb)|=1.43(18)×10¹⁷V cm^–2 at room temperature andV _zz ^eff (HgSb)=+1.8(2) × 10¹⁷V cm^–2 below 0.05 K have been derived. These two values are no indication for an anomalous temperature dependence of the effective field gradient for Hg in Sb. The value of the electric field gradient fits well into the systematics for Hg in other hosts. It is shown that the electronic enhancements of the field gradients are correlated to the valence of the impurities and are rather insensitive to the host properties.On leave of absence from: University of Lisboa, Portugal     

Quadrupole interaction at57Fe in zirconium metal

The nuclear quadrupole interaction at⁵⁷Fe nuclei in hcp -zirconium metal is measured in the temperature range 4.2 to 560 K using Mössbauer spectroscopy of⁵⁷Fe. The quadrupole splitting at room temperature is measured to be 0.660(8) mm/sec which corresponds to an electric field gradient of |eq|=3.17×10¹⁷ V/cm² at the⁵⁷Fe nucleus in a -Zr host. As has been observed in many other systems, the results show significant electronic contributions. The temperature variation of the quadrupole interaction is much stronger than is expected from the lattice contributions and is found to follow theT ^3/2 dependence approximately.⁵⁷FeZr does not follow the universal correlation betweeneq _ion andeq _el observed in most of the normal metal hosts but follows the trends recently observed by Krusch and Forker for the transition metal hosts. Our results are compared with the predictions of the conduction electron charge shift model recently proposed by Bodenstedt and Perscheid.     

Photoluminescence as a tool for the study of the electronic surface properties of gallium arsenide

Electronic surface parameters of GaAs have been determined from a qualitative and quantitative analysis of the relative photoluminescence intensity at 300 K. Characteristics of etched (100) surfaces ofn- andp-type liquid phase epitaxial GaAs have been found to be governed by negative surface charges. A density of charged surface states of about 10¹² cm⁻² and a band bending of 0.59 eV have been found forn-type material with an electron concentration of 1.1×10¹⁷ cm⁻³. Forp-type samples with hole densities ranging from 6×10¹⁵ to 4.3×10¹⁸ cm⁻³ the estimated density of negatively charged surface states was below 2×10¹¹ cm⁻², and the band bending was not more than a few kT.     

TDPAD measurements with highly oriented pyrolytic graphite using the19F(p,p′)19F* and19F(α, n)22Na* reactions

The TDPAD technique has been used to investigate quadrupole interactions of¹⁹F*(E _x =197 keV,J ^π=5/2⁺,T _1/2=88.5 ns) and²²Na*(E _x =583 keV,J ^π=1⁺,T _1/2=243 ns) in highly oriented pyrolytic graphite (HOPG). For¹⁹F* a single static quadrupole interaction was found with field gradientV _ZZ =3.24(19) × 10¹⁸ V/cm². For the case of²²Na* no quadrupole interaction was detected, leading to the conclusion that |QV _ZZ |<5.2(5) × 10¹⁵ b V/cm². TakingQ=0.06 b for the 583 keV state on the basis ofB(E2) measurements and theoretical estimates, we find that |V _ZZ | <8.7(8) × 10¹⁶ V/cm². The data demonstrate the advantages of using HOPG as a host material for the study of quadrupole interactions. Former Central Bureau for Nuclear Measurements (CBNM).     

The electric field gradient at188Os nuclei in Re metal

The electric quadrupole interaction of the first excited 2⁺ state of¹⁸⁸Os in hexagonal rhenium metal was investigated by means of the time-differential perturbed angular correlation technique. From the observed quadrupole frequencyV _Q=170(7) MHz, we deduce an electric field gradient value of |V_zz|=4.77(23)·10²¹V/m² for the system OsRe. The half-life of the 2⁺ state was measured to be 641(4)ps.