STRUCTURAL RELAXATION OF AMORPHOUS ALLOYS Fe_(77.8)Si_(7.5)B_(14.7) AND Fe_(78.5)Si_(8.9)B_(12.6)

<正> 本文用Mossbauer技术结合DTA和电阻分析,对两种非晶态合金(Ⅰ)Fe_(77.8)Si_(7.5)B_(14.7)和(Ⅱ)Fe_(78.5)Si_(8.9)B_(12.6)的结构弛豫进行了研究。 Ⅰ和Ⅱ两种非晶态合金的DTA曲线如图1,晶化开始温度分别为530和500℃,晶化前均出现较长的放热峰,预示其结构弛豫过程中可能发生某种结构变化。     

Crystallization Behavior of Metallic GlassCo_（65．1）Fe_（4．7）Ni_（4．6）Si_（10．2）B_（15．4）

ＣｒｙｓｔａｌｌｉｚａｔｉｏｎＢｅｈａｖｉｏｒｏｆＭｅｔａｌｌｉｃＧｌａｓｓＣｏ＿（６５．１）Ｆｅ＿（４．７）Ｎｉ＿（４．６）Ｓｉ＿（１０．２）Ｂ＿（１５．４）ＬｉＺｏｎｇｑｕａｎ；ＱｉｎＹｏｎｇａｎｄＨｅＹｉｚｈｅｎ（李宗全），（秦勇）（何怡贞）（...     

机械合金化法制备的Mn15Bi34Te51和La15Bi34Te51热电材料

用机械合金化法制备了Mn15Bi34Te51和La15Bi34Te51合金，XRD分析表明Mn15Bi34Te51和La15Bi34Te51分别在真空球磨150h和100h后实现合金化，La15Bi34Te51在真空球磨150h后形成了纳米结构的合金，镧原子的加入有助于Bi2Te3基合金的晶粒细化及非晶化。对La15Bi34Te51合金的XRD结构分析表明镧原子有可能进入了Bi2Te3层状结构的Te-Te原子层间。La15Bi34Te51合金Seebeck系数的测量表明当晶粒尺寸减小到纳米尺寸时，载流子散射机制有可能发生改变，导致了Seebeck系数的大幅上升。     

Mg61Cu28Gd11和(Mg0.61Cu0.28Gd0.11)99.5Sb0.5非晶合金的晶化动力学和腐蚀行为（英文）

研究0.5%(摩尔分数)Sb的引入对Mg61Cu28Gd11块体非晶合金性能的影响。利用差热扫描量热仪测试样品的晶化动力学。结果表明:在等时加热的过程中,非晶合金的玻璃转变温度、起始晶化和峰值晶化温度都表现出对加热速率强的依赖性。基于Oawza方法可以确定非晶合金的起始晶化和峰值晶化激活能。Vogel-Fulcher-Tamman公式分析表明:含Sb元素的非晶合金具有更高的强度系数和更长的延迟时间。采用电化学极化和失重测试方法研究2种玻璃合金的腐蚀行为。与基体非晶合金相比,添加微量Sb降低了非晶合金的在含Cl-的碱性溶液中的钝化电流密度和腐蚀速率,表现出相比基体合金更为优越的耐蚀性。最后基于"点缺陷模型"进一步分析微量Sb元素对基体合金耐蚀性能的影响机理。     

退火方式对La_(0.75)Mg_(0.25)Ni_(3.44)Co_(0.2)Al_(0.03)Ti_(0.03)合金的电化学性能影响

为了研究不同退火方式对La0.75Mg0.25Ni3.44Co0.2Al0.03Ti0.03铸态合金的电化学性能影响,设计最终退火温度为1223K,并采用不同保温程序对合金进行退火处理。X射线衍射(XRD)与扫描电镜(SEM)分析一段、两段保温法退火后合金的结构与性能结果表明,铸态及退火后合金由LaNi5,(La,Mg)2(Ni,Co,Al)7相以及少量LaNi2、TiNi3相组成,且退火后合金中(La,Mg)(Ni,Co,Al)3相出现。前者微观组织较后者均匀,并且前者的放电容量、放电效率好于后者。一段保温法更有利于改善合金的循环稳定性。     

Formation and Structural Evolution of Fe_(72.5)B_(15.6)Si_(7.8)Nb_(1.7)Zr_(1.7)Cu_(0.7) Nanocrystalline Alloy

A 2.5-mm Fe_(72.5)B_(15.6)Si_(7.8)Nb_(1.7)Zr_(1.7)Cu_(0.7) glassy rod was successfully fabricated using copper mold casting.The introduction of Cu resulted in the formation of large quantities of a-Fe nanoparticles embedded in the glassy matrix after isothermal annealing.The Fe_(72.5)B_(15.6)Si_(7.8)Nb_(1.7)Zr_(1.7)Cu_(0.7) nanocrystalline alloy exhibited high saturation magnetization(～1.26 T) and a low coercive force(～0.8 A/m) after annealing at 833 K for 15 min due to the precipitation of ～15-nm-sized a-Fe nanoparticles in the glassy matrix.The structural evolution of the FeBSiNbZrCu amorphous alloy during the annealing process was discussed using a dual-cluster model.     

RESISTIVITY ANOMALY IN METALLIC GLASSES(Fe_(1-x)Co_x)_(78)Si_(9.5)B_(12.5)

用四端引线法测量了4.2K到室温的非晶态(Fe_(1-x)Co_x)_(18)Si_(9.5)B_(12.5)(x=0—1.0)合金的电阻率。结果表明,x=0—1.0的所有样品都出现了电阻率与温度关系的极小值。电阻率极小值温度T_(min)随Co含量x的增加而增加,在x=0.9时出现极大值。在T_(min)温度以下,电阻率与温度关系符合-lnT规律。x=0.5—1.0的样品,电阻率与-lnT关系出现两个斜率。在T_(min)温度以上,约100K以下电阻率符合T~2规律,在约100K以上电阻率则按T~(3/2)规律变化。实验结果表明,约在9.5K和100K温区,电阻率与温度关系可近似表达为:ρ/ρ_(min)=ρ_0+AlnT+BT~2。显现类Kondo型电阻极小。电阻率的T~2关系来源于电子-声子散射。     

Fe_(4.5)Co_(67.5)Nb_(0.5)Mn_(0.5)Si_(12)B_(15)丝材中的巨磁阻抗效应

报道了淬火态Fe45Co675Nb05Mn05Si12B15丝中GMI效应,发现淬火态非晶丝GMI(Z)=|(Z(65Oe)-Z(0))/Z(0)|可高达73%。我们也对简单退火下对Fe45Co675Nb05Mn05Si12B15钴基材料中GMI效应的影响也进行了深入细致的研究,发现GMI峰值随退火温度从300℃增加到450℃而先上升,达到一个最大值,然后下降。350℃退火的效果较佳。同时发现低于1MHz时,淬火态对应的GMI效应优于退火态的值,而高于1MHz时,350℃退火材料的GMI(Z)值相应的要高。     

金属间化合物（Fe60Ni40）3（V98Ti2）的蠕变断裂

对有序金属间化合物(Fe_(60)Ni_(40))_3(V_(98)Ti_2)的蠕变断裂行为进行了初步研究。用透射电镜观察了稳态蠕变过程中位错亚结构的变化,发现存在大量的堆垛层错和成对位错以及较高密度的位错网络。对断口及近断口剖面的扫描电镜观察指出,晶界上空洞所形成的沿晶断裂是(Fe_(60)Ni_(40))_3(V_(98)Ti_2)蠕变断裂的主要机制。     

FeCoCrMoCBY块体非晶合金在强酸介质中的耐蚀性能

采用静态浸泡法研究了Fe43.7Co7.3Cr14.7Mo12.6C15.5B4.3Y1.9块体非晶合金(BMG)在浓HCl、浓H2SO4、浓HNO3以及王水中的腐蚀行为。研究表明该合金在强酸介质中具有优异的耐蚀性,在王水中浸泡236h的平均腐蚀速率仅为不锈钢的1/130。利用扫描电子显微镜(SEM)和X射线光电子能谱(XPS)分别对非晶合金在王水中腐蚀后的形貌和表面钝化膜的成分进行了分析。结果表明,合金的非晶态结构促使腐蚀过程中发生均匀腐蚀以及Cr元素在钝化膜中的富集是其具有强耐蚀能力的主要原因。     

MnFeP_(0.63)Ge(0.12)Si_(0.25)B_x(x=0,0.01,0.02,0.03)化合物的磁热效应

对MnFeP_(0.63)Ge_(0.12)Si_(0.25)B_x(x=0,0.01,0.02,0.03,原子分数)化合物的结构和磁热效应(MCE)进行了研究.XRD分析结果表明:MnFeP_(0.63)Ge_(0.12)Si_(0.25)B_x(x=0,0.01,0.02,0.03)的主相均为Fe_2P型六角结构,空间群为P62m.随着B含量的增加晶格常数a增大c减小,晶胞体积基本保持不变.磁性测量表明:随着B含量由0增加到0.03时,Curie温度(T_C)从300 K升到347 K,热滞分别为20,17,11和6 K.0-1.5 T外磁场下最大磁熵变△S_M分别为14.83,11.41,11.26和11.8 J/(kg·K).     

MAGNETIC PERMEABILITY RELAXATIONS IN AMORPHOUS ALLOYS(Fe_(0.1)Ni_(0.55)Co_(0.55))_(78)Si_8B_(14) AND Fe_(40)Ni_(38)Mo_4B_(18)

在0—300℃间研究非晶(Fe_(0.1)Ni_(0.35)Co_(0.55))_(78)si_(?)B_(14)和Fe_(40)Ni_(38)Mo_4B_(18)合金的可逆磁导率等温弛豫行为.给出等时弛豫谱,观察到三个弛豫峰.计算弛豫时间的分布和最可几激活能.初步考查Curie温度以上的退火和较慢冷却对弛豫动力学的影响.对这两种成分截然不同的合金观察到十分相似的动力学行为,表明磁寻率弛豫主要是由基本结构缺陷的局域运动引起的,成分的影响则十分次要.     

Mo对铁基块体非晶合金Fe_(71.2-x)C_(7.0)Si_(3.3)B_(5.5)P_(8.7)Cr_(2.3)Al_(2.0)Mo_x腐蚀性能的影响

系统研究了3.5%NaCl和1N HCl两种溶液中Mo对工业原材料制备的块体非晶合金Fe71.2-xC7.0Si3.3B5.5P8.7Cr2.3Al2.0Mox的抗腐蚀性能的影响,结果发现随着Mo含量的增加,两种溶液中均表现出抗腐蚀性能的增强。其中Fe64.7C7.0Si3.3B5.5P8.7Cr2.3Al2.0Mo6.5块体非晶合金因为其最低的钝化电流、最高的临界钝化电位、最低的腐蚀速率而表现出最高的抗腐蚀能力。抗腐蚀性能随着Mo含量增加而增强,其可能的原因包括:化学和结构均匀单相固溶体的形成;样品表面形成了富Cr的钝化膜,而Mo则在钝化过程中进一步阻止了Cr的溶解;MoO3及其他的复合钝化膜的形成以及Mo的添加在Cl-离子介质中所引起的抗点蚀能力的增强。     

Synthesis and photoluminescence properties of Eu(pzc)3(phen) and Eu(mpzc)3(phen)

Novel europium(III) complexes, (2-pyrazinecarboxylato)(phenanthroline) europium(III) [Eu(pzc)₃(phen)] and (5-methyl-2-pyrazinecarboxylato) (phenanthroline)europium(III) [Eu(mpzc)₃(phen)] have been designed and synthesized. These complexes were characterized by FT-IR, UV-Vis, and X-ray photoelectron spectroscopy. Photoluminescence (PL) studies showed that the two complexes emitted remarkably red luminescence. When powder samples of Eu(pzc)₃(phen) and Eu(mpzc)₃(phen) were examined using time-resolved spectroscopic analysis, the luminescence lifetimes were found to be 1.05 and 2.36 ms, respectively. Thermogravimetric analysis showed that the europium complexes possessed good thermal stability up to 345–350 °C.     

非晶合金Fe_(80-x)Cu_xSi_5B_(15)和(Fe_(1-y)Co_y)_(82)Cu_(0.4)Si_(4.4)B_(13.2)的晶化行为

用X射线衍射、吸收和内转换电子发射Mossbauer谱技术,研究了Fe_(80-x)Cu_xSi_5B_(15)和(Fe_(1-y)Co_y)_(82)Cu_(0.4)Si_(4.4)B_(13.2)两系列非晶合金的晶化行为.单辊急冷法制备的非晶带,晶化首先从贴辊面开始,晶化产物为α-Fe相.在Fe_(80)Si_5B_(15)非晶合金中以少量Cu替代Fe可以提高晶化温度.我们的结果表明,过渡金属的含量超过80at.-%,如增加到82at.-%,晶化温度就明显降低.所研究两系列含Si的铁基非晶合金在400—450℃范围内退火2h,都出现α-Fe,Fe_3B和Fe_2B三种晶态相共存状态.退火温度再升高,亚稳相Fe_3B逐渐转变为Fe_2B和α-Fe.     

MICROSTRUCTURAL CHARACTERIZATION OF Nd_(34)Fe_(60)O_(6) ALLOY

The microstructure of Nd_(34)Fe_(60)O_6 alloy was characterized by means of scanning electronmicroscope,Auger electron multiprobe,X-ray diffraction,differential thermal analysesand thermomagnetic analyses.It is found that the equilibrium microstructure of the alloy iscomposed of a Nd_2Fe_(17) matrix,an oxygen-containing Nd-rich phase anda Nd-Fe-O ternary ferromagnetic phase (referred to T_1).This phase forms via aperitectic reaction between Nd_2Fe_(17) and Nd-rich phase at 840 ℃.Its composition isaround Nd_(36)Fe_(54)O_(10),and Curie temperature 180℃.The X-ray diffraction peaks can beindexed on a tetragonal cell with lattice parameter of a=0.771nm and c=2.228nm.Thisstable phase is believed to be transformed from the metastable phase (A_1) in Nd-Febinary system as a result of oxygen introduced.     

Cu74Ni12—xSnxP14合金的非晶形成趋势

用X射线衍射(XRD)和差动扫描量热(DSC)法研究了Sn对液态淬火Cu_(74)Ni_(12-x)Sn_xP_(14)合金非晶形成能力的影响,并从动力学和结构化学方面进行了分析,结果表明,适量添加Sn可使合金非晶形成能力得到改善,在x=2—6at-％Sn的成分范围内得到完全非晶组织。     

Structures and electrochemical performances of La_(0.75-x)Zr_xMg_(0.25)Ni_(3.2)Co_(0.2)Al_(0.1) (x=0-0.2) electrode alloys prepared by melt spinning

The La-Mg-Ni system A2B7-type electrode alloys with nominal composition La0.75-xZrxMg0.25Ni3.2Co0.2Al0.1(x=0,0.05, 0.1,0.15,0.2)were prepared by casting and melt-spinning.The influences of melt spinning on the electrochemical performances as well as the structures of the alloys were investigated.The results obtained by XRD,SEM and TEM show that the as-cast and spun alloys have a multiphase structure,consisting of two main phases(La,Mg)Ni3 and LaNi5 as well as a residual phase LaNi2.The melt spinning leads to an obvious increase of the LaNi5 phase and a decrease of the(La,Mg)Ni3 phase in the alloys.The results of the electrochemical measurement indicate that the discharge capacity of the alloys(x≤0.1)first increases and then decreases with the increase of spinning rate,whereas for x0.1,the discharge capacity of the alloys monotonously falls.The melt spinning slightly impairs the activation capability of the alloys,but it significantly enhances the cycle stability of the alloys.     

EFFECT OF INITIAL CRYSTALLIZATION ON MAGNETIZATION OF METALLIC GLASSES(Fe_(1-x)Co_x)_(78)Si_(10)B_(12)

<正> 文献[1]曾对金属玻璃(Fe_(1-x)Co_x),_(78)Si_(10)B_(12)的晶化,作过X射线衍射和透射电镜研究,指出初期晶化相为相应晶态Fe_(1-x)Co_x的室温平衡相.本工作将在验证这一结论的基础上,研究初期晶化对一定磁场强度下磁化强度(定场磁化)的影响。 一、样品和实验方法 成分为(Fe_(1-x)Co_x)_(78)Si_(10)B_(12)(x=0.1,0.5,0.7,1)的合金用单辊快淬法制成截面为～1×0.3mm的金属玻璃窄带,用示差扫描热分析法测定其晶化温度T_(cr)(升温速率10℃/min)分别为505,490,440和420℃.磁性试样在石英管式炉中依次进行退火,退火温度T_a=350-500℃,除了x=0.7的样品在T_a≥450℃退火10min外,T_a≤450℃退火20min,     

MEASUREMENT OF THE THERMAL PARAMETER OF THEBULK AMORPHOUS Zr_(41)Ti_(14)Ni_(10)Cu_(125)Be_(225)ALLOY

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