Fe84Zr3.5Nb3.5B8Cu1薄带的动态磁化过程

由于铁磁性样品的交流磁化率虚部χ″随磁场强度H的变化是非线性的，在低场(0～12 mT)有一个与铁磁共振信号强度相当的低场非共振信号. 利用ESR谱仪测量交流磁化率虚部χ″对磁场强度H的一次微分随磁场强度的变化dχ″/dH～H，研究Fe₈₄Zr_3.5Nb_3.5B₈Cu₁合金薄带的动态磁化特性. 合金薄带样品是各向异性的，易磁化轴（易轴）在薄带的横向方向，外加磁场H在易轴方向. 样品在可逆磁化区域(0～2.0 mT)和趋近饱和的磁化区域(9.0 mT以上)，dχ″/dH=0；在不可逆畴壁移动过程中，当H为4.2 mT 时, χ″(H)达到最大值χ_max；在磁畴转动过程中，χ″(H)正比于H²（瑞利区）；而实验中却发现，在某些区域交流磁化率虚部χ″(H) 与磁场强度H的n次方即Hⁿ(n≥3)有关；而且发现，在一定区域，有三段不可逆畴壁移动和磁畴转动交替出现的现象. 在这一过程中，dχ″/dH为常数的磁场范围分别为4.8～5.2mT, 5.8～6.4 mT, 8.0～8.5 mT, 其常数相对值分别为1：0.85：0.60. 样品的交流磁化率虚部χ″对磁场H的微分dχ″/dH随磁场H的这一变化规律反映了不可逆畴壁移动和磁畴转动交替发生的微观过程.     

磁共振法研究(Fe1-xCox)84Zr3.5Nb3.5B8Cu1纳米晶薄带的磁各向异性

铁磁共振(FMR)实验研究(Fe1-xCox)84Zr3.5 Nb3.5B8Cu1(x=0.0,0.2,0.4,0.6, 0.8)合金薄带的各向异性,易轴在薄带的横向方向,同等宽度样品的各向异性常数K′随Co掺杂量的增加而减小, K′值在4.67×10-5 J/m(x=0.0)到2.54×10-5 J/m4(x=0.8)之间.由于磁化率的虚部χ″(H)随磁场强度H非线性变化,在低场(0-12 mT)有一个与FMR信号强度相当的低场非共振信号.特别是对Fe84Zr3.5 Nb3.5B8Cu1合金薄带的磁化,在可逆磁化(0-2.0 mT)和趋近饱和磁化(9.0-12 mT)区域, dχ″/dH=0;不可逆畴壁移动过程中,交流磁化率虚部χ″(H)与磁场强度的n次方即Hn(n≥3)有关;在磁畴转动过程中χ″(H)正比于H2(瑞利区),(dχ″)/(dH)为常数;而且发现,有不可逆畴壁移动-磁畴转动三段交替变化的过程,此过程对应三种磁畴的消失过程.     

3.5 MeV无箔注入器束流调试

3.5 MeV 注入器是“神龙一号”直线感应加速器的束源,在注入器束流调试中,首先通过数值模拟方法,初步确定束流过聚焦和聚焦不足两种极端情况下引出线圈输运磁场峰值的变化范围;然后以注入器出口束流波形为参考,通过实验调试找到了这两种情况下引出线圈输运磁场峰值的实际配置;再通过测量束流的剖面或发射度,在这两种配置中选定一个折中的引出线圈磁场配置,并最终确定了注入器输运磁场的总体配置。经过调试完成后的注入器束流为3.6 MeV,流强为2.8 kA,归一化边发射度为1 040 mm·mrad,达到了预期的指标。     

3.5 MeV无箔注入器束流调试

 3.5 MeV 注入器是“神龙一号”直线感应加速器的束源,在注入器束流调试中,首先通过数值模拟方法,初步确定束流过聚焦和聚焦不足两种极端情况下引出线圈输运磁场峰值的变化范围;然后以注入器出口束流波形为参考,通过实验调试找到了这两种情况下引出线圈输运磁场峰值的实际配置;再通过测量束流的剖面或发射度,在这两种配置中选定一个折中的引出线圈磁场配置,并最终确定了注入器输运磁场的总体配置。经过调试完成后的注入器束流为3.6 MeV,流强为2.8 kA,归一化边发射度为1 040 mm·mrad,达到了预期的指标。     

磁共振法研究(Fe1-xCox)84Zr3.5Nb 3.5B8Cu1纳米晶薄带的磁各向异性

铁磁共振（FMR）实验研究(Fe_1-xCo_x)₈₄Zr_{3.5 Nb3.5B8Cu1（x=0.0,0.2,0.4,0.6, 0.8）合金薄 带的各向异性，易轴在薄带的横向方向,同等宽度样品 的各向异性常数K′随Co掺杂量的增加而减小, K′值在4.67×10^-5　J/m（x=0. 0）到 2.54×10^-5　J 关键词： 铁磁共振 各向异性常数 低场非共振信号 磁化过程}     

3.5MeV注入器脉冲功率系统

用于直线感应加速器的3.5 MeV注入器脉冲功率系统采用了感应叠加原理。整个系统包含了脉冲形成系统、触发系统以及感应腔负载。脉冲形成系统主要由Marx发生器和Blumlein脉冲形成线组成,产生12个脉宽约90 ns,幅度约200 kV的高压脉冲,通过12个感应腔和变阻抗阴阳极杆,在阴阳极间隙处产生3.5 MV的二极管电压,由天鹅绒阴极发射强流电子束。触发系统主要由两级触发开关构成,严格控制12个高压脉冲的输出时间,时间分散性统计值小于1 ns(动作时间抖动)。采用该脉冲功率系统注入器能产生能量约3.5 MeV,电流2～3 kA的强流电子束。     

3.5 MeV注入器脉冲功率系统

用于直线感应加速器的3.5 MeV注入器脉冲功率系统采用了感应叠加原理。整个系统包含了脉冲形成系统、触发系统以及感应腔负载。脉冲形成系统主要由Marx发生器和Blumlein脉冲形成线组成,产生12个脉宽约90 ns,幅度约200 kV的高压脉冲,通过12个感应腔和变阻抗阴阳极杆,在阴阳极间隙处产生3.5 MV的二极管电压,由天鹅绒阴极发射强流电子束。触发系统主要由两级触发开关构成,严格控制12个高压脉冲的输出时间,时间分散性统计值小于1 ns(动作时间抖动)。采用该脉冲功率系统注入器能产生能量约3.5 MeV,电流2～3 kA的强流电子束。     

High-resolution ellipsometric measurements of Ni from 1.8 to 3.5 eV

High-resolution scanning ellipsometric measurements of the energy dependent complex dielectric function of Ni were made in the range 1.8–3.5 eV at 300 and 4.2 K. A single structure appears at 2.36 eV in contrast to reports of multiple fine structure in this region.     

Solutal Convection of Liquid Al-3.5 wt%Li during Its Upward Solidification

The onset of solutal convection during the directional solidification of Bridgman type of liquid Al-3.5 wt%Li is studied.Based on the analysis of a liquid-inhomogeneous-porous-double-layer system,a bimodal feature of neutral stability curve is found.The pulling rate is ascertained as the governing parameter for the mode transition,i.e.,it determines whether the microstructure in the mushy layer is related to convection after the system destabilizes.     

THE INFLUENCE OF Co SUBSTITUTION ON THE MAGNETIC PROPERTIES AND THE GIANT MAGNETO-IMPEDANCE EFFECT OF (Fe1-xCox)84Zr3.5Nb3.5B8Cu1

The microstructure, magnetic properties and the giant magneto-impedance (GMI) effect of the nanocrystalline (Fe_1-xCo_x)₈₄Zr_3.5Nb_3.5B₈Cu₁ ribbons have been studied. With increasing Co concentration, the nanocrystallized grain size and volume fraction of the α-Fe(Co) phase decrease under the same annealing condition, while the coercivity H_c increases from 1.92 A/m at x=0.0 to 30.38 A/m at x=0.8. The effective permeability drops sharply with increasing Co concentration so that the GMI effect goes down. A value of more than 380% for the magneto-impedance(MI) ratio was measured at frequency f=2.5 MHz and the sensitivity can reach 0.9% (A/m)^-1 for Fe₈₄Zr_3.5Nb_3.5B₈Cu₁ ribbon. When x is equal to 0.8, the MI ratio drops to about 30% and the sensitivity only reaches a value of lower than 0.025% (A/m)^-1. The concise analysis in theory is also expounded.     

Quasi-degenerate dark matter for DAMPE excess and 3.5 keV line

We propose a quasi-degenerate dark matter scenario to simultaneously explain the 1.4 Te V peak in the high-energy cosmic-ray electron-positron spectrum reported by the DAMPE collaboration very recently and the 3.5 ke V X-ray line observed in galaxies clusters and from the Galactic centre and confirmed by the Chandra and Nu STAR satellites. We consider a dark S U(2)′× U(1)′gauge symmetry under which the dark matter is a Dirac fermion doublet composed of two S U(2)′doublets with non-trivial U(1)′charges. At the one-loop level the two dark fermion components can have a mass split as a result of the dark gauge symmetry breaking. Through the exchange of a mediator scalar doublet the two quasi-degenerate dark fermions can mostly annihilate into the electron-positron pairs at the tree level for explaining the 1.4 Te V positron anomaly, meanwhile, the heavy dark fermion can very slowly decay into the light dark fermion with a photon at the one-loop level for explaining the 3.5 ke V X-ray line. Our dark fermions can be also verified in the direct detection experiments.     

Synthesis and characterization of NaAlSi_2O_6 jadeite under 3.5 GPa

The high pressure and high temperature(HPHT) method is successfully used to synthesize jadeite in a temperature range of 1000℃–1400℃ under a pressure of 3.5 GPa. The initial raw materials are Na_2SiO_3·9H_2O and Al_2(SiO_3)_3.Through the HPHT method, the amorphous glass material is entirely converted into crystalline jadeite. We can obtain the good-quality jadeite by optimizing the reaction pressure and temperature. The measurements of x-ray diffraction(XRD),scanning electron microscopy(SEM), Fourier-transform infrared(FTIR) and Raman scattering indicate that the properties of synthesized jadeite at 1260℃ under 3.5 GPa are extremely similar to those of the natural jadeite. What is more, the results will be valuable for understanding the formation process of natural jadeite. This work also reveals the mechanism for metamorphism of magma in the earth.     

Fundamental reflectivity spectra of Hg1−xMnxTe mixed crystals in the 1.7 to 3.5 eV energy range

The room temperature reflectivity coefficient R(E) for the mixed crystals Hg_1?xMn_xTe (x up to 0.57) in the energy range 1.7 to 3.5 eV was investigated. Two distinct maxima E₁ and E₁ + Δ₁ connected with the transitions in the critical points on the [111] direction of the Brillouin zone for the samples with x up to 0.3 and the more diffused structure of R(E) for the samples with x > 0.3 was observed. A quadratic dependence of E₁ and E₁ + Δ₁ transition energy vs alloy composition with x up to 0.3 was found, with bowing coefficient c = 1.21 ± 0.02 and 1.06 ± 0.02 respectively. The energy variation of an additional shoulder probably connected with the e₁ transitions at L point of the Brillouin zone is also reported.     

High-spin states above 3.5 MeV in 91Nb

High-spin states in ⁹¹Nb populated by the ⁸⁹Y(α, 2nγ) reaction were studied at 24.0 MeV and 35.7 MeV incident α-particle energy. Gamma-gamma coincidence and γ-ray angular distribution measurements were made. Several high-spin states in ⁹¹Nb were observed at 35.7 MeV bombarding energy which were not observable at 24.0 MeV. The shell model structure of these states is discussed.