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1.
Purely kinetic k-essence models in which the Lagrangian contains only a kinetic factor and does not depend explicitly on the field itself are considered, and a theoretical constraint is obtained: Fx -= F0a^-3. Under this theoretical constraint, we discuss a kind of purely κ-essence with form F(X) = -(1 + 2X^n)^1/2n, which can be considered as the generalized tachyon field, and find that this kind of κ-essence is not likely a candidate of dark energy to describe the present accelerated expansion of the Universe. This is contrary to a previous suggestion that κ-essence with such a form may be used to describe phantom cosmologies.  相似文献   

2.
Ca3Y2 (BO3)4:Eu^3+ phosphor is synthesized by high temperature solid-state reaction method, and the Iuminescence characteristics are investigated. The emission spectrum exhibits two strong red emissions at 613 and 621 nm corresponding to the electric dipole ^5 Do- ^7F2 transition of Eu^3+ under 365 nm excitation, the reason is that Eu^3+ substituting for Y^3+ occupies the non-centrosymmetric position in the crystal structure of Ca3 Y2 (BO3)4. The excitation spectrum for 613 nm indicates that the phosphor can be effectively excited by ultraviolet (UV) (254 nm, 365nm and 400nm) and blue (470nm) light. The effect of Eu^3+ concentration on the emission intensity of Ca3 Y2 (BO3)4 :Eu^3+ phosphor is measured, the result shows that the emission intensities increase with increasing Eu^3+ concentration, then decrease. The CIE colour coordinates of Ca3Y2 (BO3)4:Eu^3+ phosphor is (0.639, 0.357) at 15mol% Eu^3+.  相似文献   

3.
By using an Ar^+ ion laser, a tunable Rh 6G dye laser (linewidth 0.5cm^-1) pumped by the second harmonic of a YAG:Nd laser and a Coherent 899-21 dye laser as light sources and using a monochromator, a phase-locking amplifier and a computer as the data detecting system, we detect the optical properties of Eu^3+-doped Y2SiO5 crystal. Persistent ,spectral hole burning (PSHB) are observed in the Eu^3+ ions spectral lines (^5 Do-T Fo transition) in the crystal at the temperature of 16K. For 15mW dye laser burning the crystal for 0.1 s spectral holes with hole width about 80 MHz both at 579.62nm and at 579.82nm are detected and the holes can remain for a long time, more than 10h.  相似文献   

4.
A single band t-U-J1-J2 model is proposed as the minimum model to describe the superconductivity of the newly discovered iron-based superconductorsR(O1-xFx)FeAs and RO1-xFeAs (R=La, Ce, Sm, Pr, Nd, Gd). With the mean-field approach, it is found that the pairing occurs in the d-wave channel. In the likely parameter region of the real materials, by lowering temperature, the system enters firstly the dxy superconducting phase with D4h-symmetryand then enters the time-reversal-symmetry-broken dxy+idx2-y2 superconducting phase with C4h-symmetry.  相似文献   

5.
We report a novel charge-trap memory device with a composition-modulated Zr-silicate high-k dielectric mul- tilayer structure prepared by using the pulsed laser deposition technique. The device employs amorphous (ZrO2)0.5(SiO2)0.5 as the tunneling and blocking oxide layers, and ZrO2 nanocrystals as the trapping storage layer. Zr02 nanocrystals are precipitated from the phase separation of (ZrO2)0.5(SiO2)0.2 films annealed at 800℃, and isolated from each other within the amorphous (ZrO2)0.5(SiO2)0.5 matrix. Our charge trapping device shows a memory window of 2.6 V and a stored electron density of 1×10^13/cm2.  相似文献   

6.
文中,针对X形谐振腔的特点及结合纵向泵浦理论,分析了X形谐振腔几何参数的确定条件和模式匹配条件;根据有关NaCl(OH-):(F2+)H和KCl(Na+,OH-):(F2+)AH色心激光的主要研究结果,分析了提高色心激光输出效率的可能途径.  相似文献   

7.

The scale-breaking parameter F2ep(x, Q2) of non-singlet component F2ep-F2en and some other quantities in the electro-production process are discussed by usinb the analytic expression for the distribution function of valence quarks in ha.drons up to leading log approximation given by a, previous paper[1]. Comparisons with data are also given.

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8.
The angular distributions of CO^+ from the dissociation of CO2^2+ and CO2^+ in intense femtosecond laser fields (45 fs, about 5 × 10^15 W/cm^2) are studied at a laser wavelength of 800nm based on the time-of-flight mass spectra of CO^+ fragment ions. The experimental results show that structural deformation occurs in the charge state of CO2^2+ and the CO^+ maintains linear geometrical structure.  相似文献   

9.
Gd2O2S:Eu荧光谱及能级的高压研究   总被引:1,自引:0,他引:1       下载免费PDF全文
 在21 500~11 500 cm-1光谱区间内测量了Gd2O2S:Eu的荧光光谱,测量是在室温和液氮条件下进行的,对122条低温谱线和96条常温谱线进行了指认。识别了Eu3+离子5D0~27F0~6的39个斯塔克能级中的35个能级。在0~15 GPa压力范围内,研究了Gd2O2S:Eu高压下的发射光谱。在压力作用下,发现所有观测到的谱线都红移,强度降低。6个5D0~2能级下降速度大于7FJ5D27F2~5多重态的斯塔克劈裂变大,而5D17F1的劈裂变小。  相似文献   

10.
The novel vacuum ultraviolet (VUV) excited Na3 Y9O3 (BO3)8:Tb^3+ (NYOB:Tb^3+) green phosphor is prepared. Strong VUV photoluminescence and high quenching concentration of Tb^3+ (20 wt%) are observed in NYOB: Tb^3+ and the strong emission are correlated with the unique layer-type structure of NYOB. All the characteristic 4 f - 5d transitions of Tb^3+ and the host absorption band in VUV region are identified in the excitation spectrum. Based on the results, the energy levels scheme of Tb^3+ in NYOB:Tb^3+ is first established. This newly developed NYOB:Tb^3+ phosphor shows excellent optical properties when compared with the commercial Zn2SiO4:Mn^2+ and would be a potential VUV-excited green phosphor.  相似文献   

11.
 在室温下测量了GdoBr:Eu的常压和高压荧光谱,光谱范围在13 000~21 500 cm-1之间,压力至12 GPa。由光谱数据得到了Eu3+晶场能级随压力的变化曲线。7F0~5能级随压力的变化规律比较复杂,而5D0~2各能均随压力的升高几乎线性地降低。在基态谱项7F的49个状态上进行了晶场拟合计算,所得常压下的5个非零晶场参数分别为:B02=-1 124.0 cm-1,B04=-969.6 cm-1,B44=827.9 cm-1,B06=889.6 cm-1,B46=377.0 cm-1。高压下的计算结果表明,B04、B06这两个晶场参数随压力的增加而增大,B46随压力的增加而减小,而B02、B44随压力的变化有些起伏。晶场强度在8 GPa以下随压力增加而减小,其后开始变强。  相似文献   

12.
The GRACE Earth's gravitational field complete up to degree and order 120 is recovered based on the same and different three-axis resolution indexes from satellite-borne accelerometer using the improved energy conservation principle. The results show that designing XA1(2) as low-sensitivity axis (3 × 10^-9 m/s^2) of accelerometer and designing YA1(2) and ZA1(2) as high-sensitivity axes (3 × 10^-10 m/s^2) are reasonable. The physical reason why the resolution of XA1(2) is one order of magnitude lower than YA1(2) and ZA1(2) is that non-conservative forces acting on GRACE satellites are mainly decomposed into YA1(2) and ZA1(2) in the orbital plane. Since XA1(2) is not orthogonal accurately to orbital plane during the development of accelerometer, the measurement of XA1(2) can not be thrown off entirely, but be reduced properly.  相似文献   

13.
We report that a deep ultraviolet (DUV) laser from the sixth harmonic of a 1064nm laser has been firstly used as light source in an ultrahigh energy-resolution angle-resolved photoemission spectroscopy (ARPES). The wavelength is 177.3nm obtained by using the second harmonic KBe2BO3F2 crystal with a frequency tripled 1064nm Nd:YVO4 laser. The large flux (10^14 - 10^15 photons/s) and narrow line width (0.26 meV) are suitable for the ultrahigh-energy resolution ARPES. The laser-ARPES can be a powerful tool to study the electronic structure at and near the Fermi level of the superconductor and correlated materials. The laser-ARPES has worked more than 500 h already.  相似文献   

14.
Anisotropic flows (v1, v2, v3 and v4) of light fragments up to the mass number 4 as a function of rapidity are studied for 25 MeV/nucleon ^40Ca + ^40Ca at large impact parameters by a quantum molecular dynamics model. A phenomenological scaling behaviour of rapidity dependent flow parameters vn (n = 1, 2, 3 and 4) is found as a function of mass number plus a constant term, which may arise from the interplay of collective and random motions. In addition, v4/v2^2 keeps to be almost independent of rapidity and remains a rough constant of 1/2 for all light fragments.  相似文献   

15.
Charged particle multiplicity distributions for e+e annihilation are shown to be very well described by a negative binomial distribution in high energy collisions.The factorial moments F2,F3 and F4 are given in terms of 3k.  相似文献   

16.
The properties of fermion causal Green's function is discussed according to the theory of spectral representation. The definition of effective mass is established from the view point of field theory, and the approximate expression of SF' (p) as |p2|«M2 and the asymptotic formula of SF' (p) as p2→+∞ is given. In terms of these result the problem of quark confinement is discussed. We find that: (ⅰ) Based on the theory of spectral re presentation the concept of relative confinement is allowed, and if renormalization effect is strong, the quarks can demonstrate definitely lighter effective mass when they are far away from the mass shell; (ⅱ) Based on the theory of spectral representation the concept of absolute confinement is unallowable, even the absolute confinement is taken as the limit of relative confinement. That is if the concept of absolute confinement is introduced, we must discard a part of elementary hypothesis of spectral representation theory.  相似文献   

17.
The ^8Li(p, d)^7 Li reaction plays an important role in the inhomogeneous Big Bang nucleosynthesis and in the seed-nuclide production phase for the r-process. For the first time, its angular distribution at backward angles was measured in inverse kinematics at Ec.m.=4.0 MeV by using an ^8Li secondary beam. The result of measurement includes the contributions of ^8Li(p, d0)^7Li and ^8Li(p, d1)^7Li^*. The ^8Li(p, d0)^7Li component is estimated to be 40%-58% in the mixture angular distribution by analysing the measured result.  相似文献   

18.
Masses of the Ds(0^±) mesons are investigated from a view-point of ordinary light-heavy system in the framework of the Gaussian sum rules, which are worked out by means of the Laplacian transformation to the usual Borel sum rules. Using the standard input of QCD non-perturbative parameters, the corresponding mass spectra and couplings of the currents to the Ds(0^±) mesons are obtained. Our results are mDs(0-) = 1.968±0.016±0.003 GeV and mDs(0+) = 2.320 ±0.014 ± 0.003 GeV, which are in good accordance with the experimental data, 1.969 GeV and 2.317 GeV.  相似文献   

19.
Using the multi-configuration Dirac-Fock self-consistent field method and the relativistic configuration interaction method with quantum-electrodynamics corrections performed by the GRASP code, we calculate the fine-structure energy levels of the ground-state configuration (1s^22s^22p^3) of the nitrogen isoelectronic sequence, according to the L-S coupling scheme with atomic number Z up to 22. Based on the calculated results, we elucidate the mechanism of the orderings of fine-structure energy levels of 2^ D3/2,5/2 and 2^P1/2,3/2 respectively, i.e. for 2^D3/2,5/2 orderings, the competition between the spin-orbit interactions and the Breit interactions; for 2^P1/2,3/2 orderings, the electron correlations, especially the electron correlations owing to the 2p^5 configuration interactions.  相似文献   

20.
The effects of annealing on the chemical states of N dopant, electrical, and optical properties of N-doped ZnO film grown by molecular beam epitaxy (MBE) are investigated. Both the as-grown ZnO:N film and the film annealed in N2 are of n-type conductivity, whereas the conductivity converts into p-type conductivity for the film annealed in O2. We suggest that the transformation of conductivity is ascribed to the change in ratio of the N molecular number on O site (N2)O to the N atom number on O site (NO) in ZnO:N films under the various annealed atmosphere. For the ZnO:N film annealed in N2, the percentage content of (N2)O is larger than that of NO, i.e.the ratio >1, resulting in the n-type conductivity. However, in the case of the ZnO:N film annealed in O2, the percentage content of (N2)O is fewer than that of NO, i.e., the ratio <1, giving rise to the p-type conductivity. There is an obvious difference between low-temperature (80K) PL spectra of ZnO:N film annealed in N2 and that of ZnO:N film annealed in O2. An emission band located at 3.358eV is observed in the spectra of the ZnO:N film after annealed in N2, this emission band is due to donor-bound exciton (D0X). After annealed in O2, the PL of the donor-bound exciton disappeared, an emission band located at 3.348eV is observed, this emission band is assigned to acceptor-bound exciton (A0X).  相似文献   

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