回火温度对晶界添加烧结钕铁硼磁体结构演变及磁性提升机理的影响EI北大核心CSCD

采用晶界添加的方法制备了添加Tb65Cu35的烧结Nd-Fe-B磁体,研究了回火温度对晶界添加磁体微结构演变规律及磁性能的影响,并对其性能提升机制进行了分析。结果表明：经910℃一级回火2 h,460℃二级回火2 h的磁体性能最佳,获得了Br=14.14 k Gs,Hcj=12.31 k Oe,(BH)max=47.89 MGOe的磁性能,回火后的磁体的矫顽力从10.21 k Oe提升到12.31 k Oe,增加了约20%,剩磁基本保持不变。矫顽力的提升主要归因于硬磁的(Nd,Tb)-Fe-B壳层以及连续晶界层的形成。通过一阶反转曲线(FORC)对不同回火条件下样品的磁化反转过程进行了分析,可以发现最差回火态晶界添加磁体中有两个峰,然而,最佳回火态的晶界添加磁体只有一个明显的峰,表现出明显的相互作用的单畴晶粒特性,表明最佳回火态磁体内核壳之间具有强的耦合相互作用。     

反对称分子动力学模型中的冻结概念（英文）

给出了反对称分子动力学模型(AMD)计算的50 Me V/nucleon112Sn+112Sn反应的分析结果。该研究是反对称分子动力学模型中统计冻结概念的部分研究结果。利用自洽法结合修正的Fisher模型,提取了发射源的温度和密度分别为T=(6.1±0.2)Me V,ρ/ρ0=0.69±0.03。通过与AMD模型计算的系统在时间演化过程中的最大密度比较,得出碎片发射源的密度远小于系统的最大密度。利用自洽法提取的温度和密度与35 Me V/nucleon的40Ca+40Ca反应系统及40 Me V/nucleon的64Zn+112Sn反应系统所提取的温度和密度非常接近。该结果表明反对称分子动力学模型中,系统在中等质量碎片形成时刻处于统计冻结体积。     

磁场辅助静电纺有序聚丙烯腈纳米纤维的研究

磁场辅助静电纺丝方法能够制备有序纳米纤维,但是其参数之间的匹配关系很少被研究。本文通过正交实验,对影响磁场辅助静电纺丝制备聚丙烯腈纳米纤维的四个工艺参数(溶液浓度、磁铁间距、纺丝电压和注射速度)在3个水平上进行优化筛选。以纤维直径大小、均匀度和纤维有序度为考察目标,同时考虑溶液浓度、磁铁间距与纺丝电压这三个因素之间的两两交互作用,结合极差分析、方差分析,发现溶液浓度是影响纤维直径和均匀度的高度显著因素,溶液浓度和纺丝电压的交互作用对直径均匀度有显著影响,纺丝电压是影响纤维有序度的显著因素。     

Microwave reflection properties of planar anisotropy FesoNi50 powder/paraffin composites

The reflection properties of planar anisotropy Fe50Ni50 powder/paraffin composites have been studied in the microwave frequency range.The permeability of Fe50Ni50 powder/paraffin composites is greatly enhanced by introducing the planar anisotropy,and can be further enhanced by using a rotational orientation method.The complex permeability can be considered as the superposition of two types of magnetic resonance.The resonance peak at high frequency is attributed to the natural resonance,while the peak at low frequency is attributed to the domain-wall resonance.The simulated results of the microwave reflectivity show that the matching thickness,peak frequency,permeability,and permittivity are closely related to the quarter wavelength matching condition.The Fe50Ni50 powder/paraffin composites can be attractive candidates for thinner microwave absorbers in the L-band(1-2 GHz).     

利用FLUKA研究加速器生产医用放射性同位素的产额

针对目前核医学广泛关注的医用放射性同位素99Mo/99mTc、64,67Cu、68Ge/68Ga、82Sr/82Rb、211At、225Ac等，本文利用FLUKA程序对加速器生产上述同位素的产额及产物分布进行了研究。研究表明，医用放射性同位素的产额随束流能量增加而增加，增加趋势逐渐降低；产额随辐照时间的增长而增加，随辐照后冷却时间的增长而降低，变化情况主要取决于目标医用同位素的半衰期；入射束流在同位素靶的有效射程内产生医用放射性同位素，选取合适的靶厚可以优化目标医用同位素的比活度值等；此外，束流能量越高产生的杂质核素种类及产额也相应增加，合适的辐照能区和辐照时间等，可以降低后续目标医用同位素分离纯化等工作的复杂程度。本文通过FLUKA的计算初步为加速器生产医用同位素提供了重要的依据。     

一种机械谐振下的控制带宽扩展方法

针对系统固有机械谐振影响光电稳定跟踪系统频带宽度的问题,提出了一种机械谐振下的控制带宽扩展方案。该方案借助系统频率特性测量方法,利用最小二乘参数辨识算法实现。试验结果表明,利用本文方案,速度闭环下的谐振峰值减小至原来的1/3,控制带宽提高了接近2倍,证明本文提出的方案能够有效实现机械谐振抑制,提高系统控制带宽,保证系统稳定性能。     

A relativistic continuum Hartree-Bogoliubov theory description of N=3 isotones

The ground-state properties of N=3 isotones and mirror nuclei have been investigated in the Rrelativistic Continuum Hartree-Bogoliubov theory with the NLSH effective interaction. Pairing correlations are taken into account by a density-dependent δ-force. The calculations show that the proton density distributions of ⁸B and ⁹C have a long tail, the core has an increasing tendency of ⁹C and the paired off valence protons make the halo distribution shrink. The cross sections for the ⁸B(⁹C)+¹²C reaction which are consistent with the experimental data are calculated using the Glauber model. On the whole, we think that ⁸B is a one-proton halo nucleus and ⁹C is a two-proton halo nucleus.     

Effects of spacer layers on magnetic properties and exchange couplings of Nd-Fe-B/Nd-Ce-Fe-B multilayer films

The influences of the spacer-layer Ta on the structures and magnetic properties of Nd Fe B/Nd Ce Fe B multilayer films are investigated via DC sputtering under an Ar pressure of 1.2 Pa. An obvious(00l) texture of the hard phase is observed in each of the films, which indicates that the main phase of the film does not significantly change with Ta spacer-layer thickness. As a result, both the remanence and the saturation magnetization of the magnet first increase and then decrease,and the maximum values of 4πM_r and H_(cj) are 10.4 k Gs(1 Gs = 10_(-4)T) and 15.0 kOe(1 Oe = 79.5775 A·m_(-1)) for the film with a 2-nm-thick Ta spacer-layer, respectively, where the crystalline structures are columnar shape particles. The measured relationship between irreversible portion D(H) =-?M_(irr)/2 M_r and H indicates that the nucleation field of the film decreases with spacer layer thickness increasing, owing to slightly disordered grains near the interface between different magnetic layers.     

400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究

在ADS散裂靶系统的优化设计中,蒙特卡罗方法结合可靠的散裂反应理论模型进行中子学计算具有重要的作用。本工作利用Geant4程序中的INCLXX模型、BIC模型以及BERT模型和FLUKA程序分别模拟了597 MeV和1 500 MeV质子轰击薄铅靶不同出射角度的中子双微分截面,500,1 500 MeV质子轰击厚铅靶不同出射角度的中子双微分产额,以及400,600,800,1 000和1 200 MeV质子轰击厚钨靶在反角方向（175 °）的中子双微分产额,并与实验数据进行比较。研究表明,对于薄铅靶,Geant4程序的INCLXX模型和FLUKA程序模拟结果与实验符合得更好。能量在10～40 MeV范围内,BIC模型模拟结果明显高于实验数据,而BERT模型模拟结果略微低于实验数据。对于厚铅靶,在40 MeV左右所有的模拟结果都低于实验数据。对于厚钨靶,Geant4程序的BIC模型和FLUKA程序与实验数据符合得较好,INCLXX模型在能量高于60 MeV时模拟结果低于实验数据,BERT模型与实验数据差异较大。总体来看,Geant4程序的INCLXX模型和FLUKA程序进行ADS散裂靶相关的中子学的计算是合理和可靠的。The reliable Monte Carlo simulation codes coupled with nuclear reaction models play an important role in the neutronic calculation for the design and optimization of the ADS spallation target. In this work, the double differential cross sections at different angles produced from a thin lead target bombarded with 597 and 1 500 MeV protons, the neutron energy spectra at different angles produced from a thick lead target bombarded with 500 and 1 500 MeV protons, and the neutron energy spectra in the backward direction(175°) produced from a thick tungsten target bombarded with 400, 600, 800, 1 000 and 1 200 MeV protons are calculated with the Geant4 code coupled INCLXX, BIC and BERT models and the FLUKA code. The calculations are compared with the available experimental data. The results show that, for the thin lead target, the calculations with the Geant4 coupled INCLXX model and FLUKA code well reproduce the experimental results. In a energy range from 10 to 40 MeV, BIC model obviously overestimates the experimental results, and BERT model slightly underestimates the experimental results. For the thick lead target, all of the calculations underestimate the experimental results around 40MeV. For the thick tungsten target, the Geant4 coupled BIC model and FLUKA code well reproduce the experimental results. INCLXX model underestimates the experimental results above 60 MeV. BERT model bad reproduces the experimental results. Overall, the neutronic calculations with the Geant4 code coupled INCLXX model and FLUKA code for the ADS spallation target is reasonable and reliable.     

Clustering Structure of 10Be Studied with the Deformed RMF＋BCS Method

We investigate the nucleus 10Be using the deformed relativistic mean field （RMF） model and BCS theory. The calculated density distribution suggests two α clusters in the nucleus 10Be. According to BCS theory, the two valence neutrons transit to the first excited state 02＋ in a pair and form a 2-n cluster. By comparing the two neutron separation energy （S2n） with the single neutron separation energy （Sn）, and analyzing the difference between the neutron and proton rms radii （Rn-Rp） calculated by the deformed RMF, we suggest that 10Be is the best candidate for a two-neutron skin. The two-neutron skin clings to the 2α clusters closely and makes the two α clusters have cross and chain distribution.