共查询到20条相似文献,搜索用时 15 毫秒
1.
Minamisono T. Matsuta K. Minamisono K. Kudo S. Ogura M. Fukuda S. Sato K. Mihara M. Fukuda M. 《Hyperfine Interactions》2001,136(3-8):225-231
In order to precisely determine the |eqQ(41Sc)/h| of 41Sc(I
π=7/2−, T
1/2=0.596 s) implanted in a TiO2 single crystal the electric field gradient tensor and anisotropic chemical shift were determined by detecting the Fourier
Transformed Pulse-NMR of 45Sc(I
π=7/2−, stable) in the crystal at a high field of 7.0 T and 9.4 T. Combining the new |eqQ(41Sc)/h| value with the Q(45Sc)=−(23.6±0.2) fm2, also renewed by using the known atomic hyperfine interaction constants and Sternheimer polarization effect, the |Q(41Sc;I
π=7/2−,T
1/2=0.596 s)|=(15.6±0.3) fm2 has been precisely determined. The value is compared with the theoretical Q(41Sc) given by a shell model code.
This revised version was published online in September 2006 with corrections to the Cover Date. 相似文献
2.
T. Minamisono Y. Yasui T. Ohtsubo A. Kitagawa Y. Matsuo Y. Nojiri K. Matsuta S. Takeda 《Hyperfine Interactions》1990,59(1-4):153-156
The nuclear electric quadrupole moment of41Sc(Iπ=7/2−) was experimentally determined by use of the NMR detection in which the asymmetric β-ray distribution from spin polarized
nuclei was monitored. The magnetic interaction of the state with high external magnetic field and the nuclear quadrupole interaction
with the electric field gradient obtained in TiO2 crystal were studied. The field gradient seen to the implanted41Sc was measured independently by the high field NMR detection on the stable isotope45Sc located in the equivalent41Sc site with. |Q(41Sc;Iπ=7/2−)|=(0.120±0.006) b was determined. 相似文献
3.
Precise measurement of magnetic moment of short-lived β-emitting nuclei12B ( I π=1+, T 1/2=20.18 ms)
Zhou Dongmei Zheng Yongnan Du Enpeng Xu Yongjun Zhu Jiazheng Yuan Daqing Wang Zhiqiang Luo Hailong Zuo Yi Ma Ruigang Duan Xiao M. Mihara M. Fukuda K. Matsuta T. Minamisono Zhu Shengyun 《中国科学G辑(英文版)》2004,47(5):531-539
The spin polarized β-emitting nuclei12B (I
π=1+,T
1/2=20.18 ms) were produced by the nuclear reaction11B(d, p)12B and by the selection technique of the incident deuteron energy and the12B recoil angle following the nuclear reaction. The nuclear magnetic moment of the short-lived nuclei12B was measured by β-NMR with the β-NMR and β-NQR setup established for the first time in China. The nuclear magnetic moment
of12B was determined to be μ=0.99993±0.00048 nm org=0.99993±0.00048 after the precise correction of the Knight shift. 相似文献
4.
T. Minamisono T. Ohtsubo Y. Nakayama T. Araki K. Mashitani K. Matsuda E. Takahashi M. Tanigaki Y. Someda M. Tanaka A. Kitagawa M. Fukuda K. Matsuta Y. Nojiri 《Hyperfine Interactions》1992,73(3-4):347-356
Hyperfine interactions of β-emitting17F implanted in single crystals of NaF and CaF2 were studied. The nuclear magnetic moment of theT
π=5/2+ state was determined with an improved precision to be |μ(17F;π=5/2+,T
1/2=64.5s|=4.72130±0.00025. nm. Isoscalar magnetic moments of the doubly closed shell ±1 nucleon nuclei around mass number 16
were derived and the effective nucleon mass in the nucleus was discussed. 相似文献
5.
T. Minamisono Y. Nojiri K. Matsuta K. Takeyama A. Kitagawa T. Ohtsubo A. Ozawa M. Izumi 《Hyperfine Interactions》1990,59(1-4):149-152
The nuclear magnetic moment of41Sc(Iπ=7/2−, Tl/2=0.59sec) was remeasured, and the precision of the value was improved about 10 times compared with the previously known one.
The value was determined to be |μ(41Sc;Iπ=7/2)|=(5.4305±0.0018) nm. Comparing the value with the previously known NMR of the nuclei in Pt, the knight shift, K=−(0.4±5.3)·10−4 was determined. 相似文献
6.
T. Nagatomo T. Sumikama M. Ogura K. Matsuta Y. Nakashima K. Akutsu T. Iwakoshi H. Fujiwara T. Minamisono M. Fukuda M. Mihara K. Minamisono T. Miyake S. Momota Y. Nojiri A. Kitagawa M. Sasaki M. Torikoshi M. Kanazawa M. Suda M. Hirai S. Sato S. Y. Zhu J. Z. Zhu Y. J. Xu Y. N. Zheng J. R. Alonso G. F. Krebs T. M. Symons 《Hyperfine Interactions》2004,159(1-4):269-272
The electric quadrupole coupling constants eqQ/h of 8B (, T
1/2 = 769 ms) and 13B (, T
1/2 = 17.4 ms) in single crystal TiO2 have been precisely measured by the β-NQR technique. The ratios of these Q moments to Q(12B) were determined as ∣Q(8B)/Q(12B)∣ = 4.882(32) and ∣Q(13B)/Q(12B)∣ = 2.768(24). 相似文献
7.
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. 相似文献
8.
P. Thakur R. Dogra A. K. Bhati S. C. Bedi R. P. Singh S. Muralithar R. K. Bhowmik 《Hyperfine Interactions》2000,131(1-4):103-109
The electric quadrupole moments of the 9/2− and 21/2− isomeric states of 173Ta at 165.8 keV and 1713.2 keV, respectively, were measured as Q(9/2−)=2.92(15) b and Q(21/2−)=6.23(18) b for the first time using the TDPAD technique. A 66 MeV pulsed 12C ion beam from the 15UD pelletron accelerator facility of the Nuclear Science Centre at New Delhi was used in the reaction
165Ho(12C, 4nγ)173Ta. The experimental values of equilibrium deformations β2(9/2−)=0.251(7) and β2(21/2−)=0.391(7) were extracted.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
9.
We analyze the proton and deutron data on the spin-dependent asymmetry A
1(x, Q
2), supposing that the DIS structure functions g
1(x, Q
2) and F
3(x, Q
2) have a similar Q
2 dependence. As a result, we have found that Λ
1
p
−Λ
1
n
=0.190±0.038 at Q
2=10 GeV2 and Λ
1
p
−Λ
1
n
=0.165±0.026 at Q
2=3 GeV2; these values are in the best agreement with the Bjorken sum rule predictions.
Pis’ma Zh. éksp. Teor. Fiz. 65, No. 1, 9–14 (10 January 1997)
Published in English in the original Russian journal. Edited by Steve Torstveit. 相似文献
10.
Ogura M. Minamisono K. Sumikama T. Nagatomo T. Iwakoshi T. Miyake T. Hashimoto K. Kudo S. Arimura K. Ota M. Akutsu K. Sato K. Mihara M. Fukuda M. Matsuta K. Akai H. Minamisono T. 《Hyperfine Interactions》2001,136(3-8):195-199
It was confirmed by detecting the β-NMR of 12B (I
π=1+, T
1/2=20.2 ms) in a TiO2 (rutile) crystal that the nuclear spin polarization of 12B was totally maintained in the crystal as produced through a nuclear reaction before implantation. Two locations, site 1
and site 2, were found with the relative populations 9 and 1, respectively, and the electric field gradients (EFGs) at those
sites were obtained to be q(site 1)=+(37.1±0.5)1015 V/cm2, η(site 1)<0.03, q(site 2)=+(185±5)1015 V/cm2 and η(site 2)=0.62±0.02. We also found that about 30% of the initial polarization of 8Li (I
π=2+, T
1/2=838 ms) was maintained in the crystal. Since the polarizations of other β emitting nuclei, 12,16N, 13,19O, and 41Sc were also totally maintained in the crystal, the crystal can be a “Spin Dewar” in which many short-lived nuclides can be
implanted with their polarizations totally maintained during their lifetimes for the studies not only on the electronic structure
of impurities in it but also on the nuclear properties.
This revised version was published online in September 2006 with corrections to the Cover Date. 相似文献
11.
The absorption spectra, fluorescence spectrum and fluorescence decay curve of Nd3+ ions in CaNb2O6 crystal were measured at room temperature. The peak absorption cross section was calculated to be 6.202×10−20 cm2 with a broad FWHM of 7 nm at 808 nm for E//a light polarization. The spectroscopic parameters of Nd3+ ions in CaNb2O6 crystal have been investigated based on Judd-Ofelt theory. The parameters of the line strengths Ω
t
are Ω
2=5.321×10−20 cm2,Ω
4=1.734×10−20 cm2,Ω
6=2.889×10−20 cm2. The radiative lifetime, the fluorescence lifetime and the quantum efficiency are 167 μs, 152 μs and 91%, respectively. The fluorescence branch ratios are calculated to be β
1=36.03%,β
2=52.29%,β
3=11.15%,β
4=0.533%. The emission cross section at 1062 nm is 9.87×10−20 cm2. 相似文献
12.
Tanigaki M. Ohkubo Y. Taniguchi A. Kawase Y. Goto J. Sasanuma T. 《Hyperfine Interactions》2001,136(3-8):391-396
A 140La(I
π=3−, T
1/2=40.3 h)-doped layer has been produced in CaB6 by means of radioactive isotope (RI) beam technique: 140Cs(I
π=1−, T
1/2=63.7 s) was implanted into CaB6 and the radioactive equilibrium of 140Ba–140La was achieved. The concentration of La in CaB6 was La/Ca ∼0.001. Obtained TDPAC spectra of the 2083 keV level of 140Ce (I
π=4+, T
1/2=3.4 ns, μ=+4.35±0.10 μ
N
) followed by the β decay of 140La showed the existence of hyperfine magnetic fields: B
hyp=−15.0±0.5 T and −1.00±0.15 T.
This revised version was published online in September 2006 with corrections to the Cover Date. 相似文献
13.
The third-order elastic constants of single crystal GaSb are determined using ultrasonic pulse interferometer at 10 MHz. The
constants at 300°K, in units of 1011 N.m.−2, are Cl11 = ™ 4 ·75 ± 0·06 C144 = + 0·50 ± 0·25 C113 = ™ 3 ·08 ± 0·02 C166 = ™ 2·16 ± 0·13 C123 = ™ 0 ·44 ± 0·29 C456 = ™ 0·25 ± 0·15 These constants are used to evaluate the three anharmonic first and second neighbour force constants based
on modified Keating’s model. The constants are (in units of 1011 N.m−2)γ=− 2·406;δ=0·407;ε=−0·222. 相似文献
14.
T. Bądicą V. Cojocaru D. Pantelicą I. Popescu R. Ion-Mihai 《Hyperfine Interactions》1986,30(4):291-295
The magnetic moment μ=−(1.69±0.47) μN of the 15/2+, 3578 KeV level in67Ga was determined from measurements of the integral perturbed angular distributions in implanted sources. The excited levels
were populated by the reaction56Fe(16O, αp)67Ga. 相似文献
15.
β-γ-γ directional correlation studies for the cascades (i)β-rays ofE
max=0.12 MeV,γ-rays of 557 keV andγ-rays of 53 keV and (ii)β-rays ofE
max=0.21 MeV,γ-rays of 444 keV andγ-rays of 53 keV have been made. The triple correlation functionsW(θ) were obtained to beW(θ)=1+(−0.153±0.031)P
2(cosθ)+(0.004±0.035)P
4(cosθ) forβ-rays ofE
max 0.12 MeV→557→53 keV cascade andW(θ)=1+(0.163±0.042)P
2(cosθ)+(−0.035±0.058)P
4(cosθ) forβ rays ofE
max=0.21 MeV→444 keV→53 keV cascade.
Spins and parities of the 650, 537 and 93 keV levels of103Rh are deduced by triple angular correlation and the internal conversion coefficient studies. Multipolarities of the transitions
are also determined. 相似文献
16.
Electrical resistance measurements are reported on the binary liquid mixtures CS2 + CH3CN and CS2 + CH3NO2 with special reference to the critical region. Impurity conduction seems to be the dominant mechanism for charge transport.
For the liquid mixture filled at the critical composition, the resistance of the system aboveT
c follows the relationR=R
c−A(T−T
c)
b
withb=0·6±0·1. BelowT
c the conductivities of the two phases obey a relation σ2−σ1=B(T
c−T)β with β=0·34±0·02, the exponent of the transport coefficient being the same as the exponent of the order parameter, an equilibrium
property. 相似文献
17.
Mihara M. Hashimoto K. Arimura K. Kudo S. Akutsu K. Minamisono K. Miyake T. Fukuda M. Matsuta K. Minamisono T. 《Hyperfine Interactions》2001,136(3-8):339-343
The hyperfine interactions of short-lived β-emitter 12B implanted into a CaB6 crystal have been studied by means of the β-NMR technique. An electric quadrupole splitting has been observed at room temperature
from which an electric field gradient of q=−(1.34±0.05)×1021 V/m2 was determined. From the present result, it was found that the 12B nuclei are mainly implanted in the substitutional boron site.
This revised version was published online in September 2006 with corrections to the Cover Date. 相似文献
18.
《The European Physical Journal C - Particles and Fields》2006,48(3):715-748
A detailed analysis is presented of the diffractive deep-inelastic scattering process ep→eXY, where Y is a proton or a low
mass proton excitation carrying a fraction 1-xIP>0.95 of the incident proton longitudinal momentum and the squared four-momentum transfer at the proton vertex satisfies |t|<1 GeV2. Using data taken by the H1 experiment, the cross section is measured for photon virtualities in the range 3.5≤Q2≤1600 GeV2, triple differentially in xIP, Q2 and β=x/xIP, where x is the Bjorken scaling variable. At low xIP, the data are consistent with a factorisable xIP dependence, which can be described by the exchange of an effective pomeron trajectory with intercept αIP(0)=1.118±0.008(exp.)+0.029
-0.010(model). Diffractive parton distribution functions and their uncertainties are determined from a next-to-leading order DGLAP
QCD analysis of the Q2 and β dependences of the cross section. The resulting gluon distribution carries an integrated fraction of around 70% of
the exchanged momentum in the Q2 range studied. Total and differential cross sections are also measured for the diffractive charged current process e+p→ν̄eXY and are found to be well described by predictions based on the diffractive parton distributions. The ratio of the diffractive
to the inclusive neutral current ep cross sections is studied. Over most of the kinematic range, this ratio shows no significant
dependence on Q2 at fixed xIP and x or on x at fixed Q2 and β. 相似文献
19.
L. Šamaj 《Journal of statistical physics》2006,124(5):1179-1206
This paper is a continuation of a previous one [L. Šamaj, J. Stat. Phys.
120:125 (2005)] dealing with the renormalization of a guest charge immersed in a two-dimensional logarithmic Coulomb gas of pointlike ± unit charges, the latter system being in the stability-against-collapse regime of reduced inverse temperatures 0 ≤ β < 2. In the previous work, using a sine-Gordon representation of the Coulomb gas, an exact renormalized-charge formula was derived for the special case of the pointlike guest charge Q, in its stability regime β |Q| < 2. In the present paper, we extend the renormalized-charge treatment to the guest charge with a hard core of radius σ, which allows us to go beyond the stability border β|Q| = 2. In the limit of the hard-core radius much smaller than the correlation length of the Coulomb-gas species and at a strictly finite temperature, due to the counterion condensation in the extended region β|Q| > 2, the renormalized charge Q
ren turns out to be a periodic function of the bare charge Q with period 1. The renormalized charge therefore does not saturate at a specific finite value as |Q| →∞, but oscillates between two extreme values. In the high-temperature Poisson-Boltzmann scaling regime of limits β→ 0 and Q→∞ with the product β Q being finite, one reproduces the Manning-Oosawa type of counterion condensation with the uniform saturation of β Q
ren at the value 4/π in the region β|Q| ≥ 2. The obtained results disprove the “regularization hypothesis” of the previous work about the possibility of an analytic continuation of the formula for Q
ren from the stability region β |Q| < 2 to β |Q| ≥ 2. 相似文献
20.
Matsuta K. Onishi T. Fukuda M. Minamisono T. Akai H. Sasaki M. Yamaguchi T. Miyake T. Sato K. Minamisono K. Ohsumi F. Muramoto Y. Oui S. Ha C. Tanaka K. Kidera K. Morishita A. Kitagawa A. Torikoshi M. Kanazawa M. Nishio T. Koda S. Ohtsubo T. Fukuda S. Nojiri Y. Momota S. Ozawa A. Yoshida K. Suzuki T. Kobayashi T. Tanihata I. Hanna S.S. Alonso J.R. Krebs G.F. Symons T.J.M. 《Hyperfine Interactions》1999,120(1-8):673-677
The β-NMR spectra of 21F, 23Mg, 27Si and 39Ca which were produced in heavy ion collisions and implanted in various crystals have been observed. The magnetic moments
of 21F and 27Si were determined to be |μ(21F)| = 3.9194 ± 0.0012 μN and |μ(27Si)| = 0.8653 ± 0.0003 μN, respectively. The electric quadrupole coupling constants were determined for the first time to be |eqQ(21F in MgF2)/h|= 9.94 ± 0.09 MHz, |eqQ(23Mg in MgF2)/h|= 1.96 ± 0.06 MHz, |eqQ(27Si in Al2O3)/h|= 1.90 ± 0.12 MHz, |eqQ(39Ca in CaCO3)/h|= 0.60 ± 0.04 MHz. From the present eqQ/h, the Q moments were deduced as |Q(21F)|= 110 ± 22 mb, |Q(23Mg)|= 114 ± 3 mb, |Q(27Si)|= 60 ± 13 mb and |Q(39Ca)|= 36± 7 mb. The present data were compared with the theoretical values obtained by the OXBASH shell model code.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献