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1.
According to first-principles density functional calculations,we have investigated the magnetic properties of Mn-doped GaN with defects,Ga 1-x-y V Gx Mn y N 1-z-t V Nz O t with Mn substituted at Ga sites,nitrogen vacancies V N,gallium vacancies V G and oxygen substituted at nitrogen sites.The magnetic interaction in Mn-doped GaN favours the ferromagnetic coupling via the double exchange mechanism.The ground state is found to be well described by a model based on a Mn 3+-d 5 in a high spin state coupled via a double exchange to a partially delocalized hole accommodated in the 2p states of neighbouring nitrogen ions.The effect of defects on ferromagnetic coupling is investigated.It is found that in the presence of donor defects,such as oxygen substituted at nitrogen sites,nitrogen vacancy antiferromagnetic interactions appear,while in the case of Ga vacancies,the interactions remain ferromagnetic;in the case of acceptor defects like Mg and Zn codoping,ferromagnetism is stabilized.The formation energies of these defects are computed.Furthermore,the half-metallic behaviours appear in some studied compounds.  相似文献   

2.
Ti-substituted LiMn2O4 (LiMn2−x Ti x O4, x=0, 0.15, 0.30, 0.45, 0.60, and 0.75) has been synthesized using solid-state reactions. Their crystal and electronic structures were investigated using X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), and ultraviolet photoelectron spectroscopy (UPS). XRD data suggested that the lattice parameters of LiMn2−x Ti x O4 increase due to the replacement of Mn by Ti ions. XPS results indicated that the substituted Ti ions were in +4 oxidation state; consequently, the normal oxidation state of Mn ions has been detected by measuring the binding energy splitting of Mn 3s states, which decreases with the content of substituted Ti. The valence band spectra suggested that the intensity of e g level of Mn 3d orbitals increased due to the increase of the Mn3+/Mn4+ ratio.  相似文献   

3.
A first-order transition at 290 K in LiMn2O4 with a cubic spinel-type structure is known to degrade the electrochemical performance of the positive electrode of rechargeable lithium-ion batteries. Using first-principles density functional theory (DFT), we confirm that the phase transition is induced by charge-ordering of Mn3+/Mn4+ accompanied by orbital-ordering due to Jahn–Teller distortion, which is in agreement with the previous experimental results of Rodríguez-Carvajal et al. [J. Rodríguez-Carvajal, G. Rousse, C. Masquelier, M. Hervieu, Phys. Rev. Lett. 81 (1998) 4660]. The optimized structure of the low-temperature (LT) phase has orthorhombic symmetry with five distinct crystallographic sites for Mn. The spin integration at each Mn site shows that Mn3+ resides at three Mn sites and the remaining two sites are occupied by Mn4+ ions. Total energy calculations indicate that the LT phase is about 0.23 eV/ LiMn2O4 more stable than cubic LiMn2O4 (high-temperature phase). The electrochemical Li extraction reaction from the LT phase is also investigated using DFT calculations. The results indicate that the reaction is initially divided into two voltage regions. Electrostatic interactions in the LT phase are calculated using a point charge model, accounting for the features of the electronic configurations and electrochemical reactions.  相似文献   

4.
A systematic study of the doping of the Mn-sites by cobalt in three series of manganites — La0.76Ba0.24(Mn1−xCox)O3 single crystals, La2/3Ba1/3(Mn1−xCox)O3 and La(Mn1−xCox)O3 ceramics has been performed. It was found that La(Mn1−xCox)O3 annealed at 800°C in the range 0.4x0.9 is a mixture of ferromagnetic domains with ordered Mn and Co ions and ionically disordered spin-glass domains. In the quenched samples the fraction of spin-glass-type component increases strongly. The La2/3Ba1/3(Mn1−xCox)O3 solid solutions exhibit also an evidence for phase separation in the range 0.5x0.8. All the La(Mn1−xCox)O3 samples show an insulating behavior, however, magnetoresistance reduces strongly when the cobalt content rises to x=0.5. The La0.76Ba0.24(Mn1−xCox)O3 single crystals show first-order phase transition below their Curie points associated with a change of ground state of the Co2+ ions. The magnetic phase diagrams are depicted. The results are discussed in terms of positive Mn3+–O–Mn4+, Mn3+–O–Mn3+, Mn4+–O–Co2+ and negative Mn4+–O–Mn4+, Co2+–O–Co2+, Co2+–O–Mn3+ superexchange interactions as well as Co2+ and Mn4+ ionic ordering.  相似文献   

5.
LiFe1 − xMnxPO4 olivines are promising material for improved performance of Li‐ion batteries. Spin–phonon coupling of LiFe1 − xMnxPO4 (x = 0, 0.3, 0.5) olivines is studied through temperature‐dependent Raman spectroscopy. Among the observed phonon modes, the external mode at ~263 cm−1 is directly correlated with the motions of magnetic Fe2+/Mn2+ ions. This mode displays anomalous temperature‐dependent behavior near the Néel temperature, indicating a coupling of this mode with spin ordering. As Mn doping increases, the anomalous behavior becomes clearly weaker, indicating the spin–phonon coupling quickly decreases. Our analyses show that the quick decrease of spin–phonon coupling is due to decrease of the strength of spin–phonon coupling, but not change of spin‐ordering feature with Mn doping. Importantly, we suggest that the low electrochemical activity of LiMnPO4 is correlated with the weak spin–phonon coupling strength, but not with the weak ferromagnetic ground state. Our work would play an important role as a guide in improving the performances of future Li‐ion batteries. Copyright © 2015 John Wiley & Sons, Ltd.  相似文献   

6.
高潭华  刘慧英  张鹏  吴顺情  杨勇  朱梓忠 《物理学报》2012,61(18):187306-187306
采用基于密度泛函理论的第一性原理方法, 在广义梯度近似(GGA)和GGA+U方法下对尖晶石型LiMn2O4及其Al掺杂 的尖晶石型LiAl0.125Mn1.875O4晶体的结构和电子性质进行了计算. 结果表明: 采用GGA方法得到尖晶石型LiMn2O4是立方晶系结构, 其中的Mn离子为+3.5价, 无法解释它的Jahn-Teller 畸变. 给出的LiMn2O4能带结构特征也与实验结果不符. 而采用GGA+U方法得到在低温下的LiMn2O4和其掺杂 体系LiAl0.125Mn1.875O4的晶体都是正交结构, 与实验一致. 也能明确地确定Mn的两种价态Mn3+/Mn4+的分布并且能够说明Mn3+O6z方向有明显的Jahn-Teller 畸变, 而Mn4+O6则没有畸变. LiMn2O4的能带结构与实验比较也能够符合. 采用GGA+U方法对Al掺杂体系的LiAl0.125Mn1.875O4的研究表明, 用Al替换一个Mn不会明显地改变晶体的电子性质, 但可以有效地消除Al3+O6 八面体的Jahn-Teller畸变, 从而改善正极材料LiMn2O4的性能, 这与电化学实验的观察结果相一致.  相似文献   

7.
采用KKR-CPA-LDA方法研究了CuMnAl,CoMnAl和CuCoMnAl四元合金中磁性原子磁矩和Co-Mn间的交换作用.通过与实验结果对比,揭示了Mn的磁矩和Co的磁矩以及它们的相互作用随成分变化的规律.研究发现,在Cu50Mn25+xAl25-x合金中超过化学配比并占据Al位的Mn原子是反铁磁的,而且由于近邻环境的不同,其磁矩大于原有Mn原子的磁矩.在Co50Mn25+< 关键词: KKR-CPA-LDA计算 Co-Mn间交换作用  相似文献   

8.
利用实验和能带计算相结合的方法,对介于两种预期的半金属Heusler合金Co2FeSi和Co2MnSi间的四元合金Co50Fe25-xMnxSi25的晶体结构、磁性、能带结构和半金属性进行了研究.采用考虑库仑相互作用的的广义梯度近似方法计算了系列合金的能带结构,通过与实验结果进行对比,揭示了成分变化过程中合金分子磁矩及原子磁矩的变化规律.研究发现, 关键词: 磁性 半金属 Heusler合金  相似文献   

9.
The spinel phases Mn3-x Co x O4 are prepared directly and at low temperature (600-700°C) by means of thermal decomposition of mixed oxalate salt precursors in air or controlled atmosphere. The powders so obtained when sintered at 1200°C behave as semiconducting or insulating ceramics, depending on their cobalt content. The electrical properties of these ceramics have been found to be related to the distribution and valencies of the cations in the spinel structure. The study of their crystalline structure and stability, complemented by electrical measurements have permitted us to distinguish two types of compounds. The first type includes those given by Mn3-x Co x O4 with 0 < x < 1. These are stable at high temperature, have a tetragonal structure and are insulators. The cation distributions for them can be deduced from that of hausmannite as given by Mn2+ [Mn3+ 2]O4, by substituting Mn2+ ions with Co2+ ions. The second type of compounds correspond to the cubic phases and occur for 1 < x < 3. These are unstable at high temperature and show a lower resistivity (e.g. 360 ° cm) which is of particular interest for their application in the design of negative temperature coefficient (N.T.C.) thermistor components.  相似文献   

10.
王桂英  郭焕银  毛强  杨刚  彭振生 《物理学报》2010,59(12):8883-8889
用固相反应法制备了La0.45Ca0.55Mn1-xVxO3(x=0.00,0.10)多晶样品.通过X射线衍射谱、质量磁化强度-温度曲线、电子自旋共振谱,研究了V5+替代Mn3+/Mn4+对La0.45Ca0.55MnO3电荷有序相和自旋玻璃态的影响.实验结果表明,当x=0.10时,不仅母体的电荷有序相基本破坏,而且母体在40K左右出现的自旋玻璃态也被融化.电荷有序相被破坏的主要原因是用V5+替代Mn3+/Mn4+后,增加了Mn3+与Mn4+的比例,使铁磁双交换作用优于反铁磁超交换作用;自旋玻璃态的融化是由于V替代Mn后破坏了反铁磁背景下有少量铁磁成分的自旋玻璃态的形成条件.  相似文献   

11.
Carbon nanotubes (CNT) coated with LiMn1-x Fe x PO4 (0.2?≤?x?≤?0.8), as possible cathode materials, was synthesized by using a sol–gel process (Polyol method), after annealing under flowing nitrogen. X-ray diffraction (XRD) patterns of the composites confirmed the formation of the olivine structured LiMn1-x Fe x PO4 phase and no secondary phases were detected. The morphological investigation revealed the formation of agglomerates with particles size ranging between 300 and 700 nm. XRD investigation of composites shows difference of the morphology by doping CNT and carbon black in the composites. Transmission electron microscopy shows the growth of nano-sized particles on CNT (20–70 nm) and the agglomeration of primary particles to form secondary particles. The X-ray photoelectron spectroscopy showed that the Fe and Mn ions are in divalent states in the LiMn1-x Fe x PO4 composites. The cyclic voltamograms showed the oxidation peaks of iron and manganese ions at 3.53–3.63 and 4.05–4.33 V, respectively, while the reduction peaks were found at 3.21–3.42 V (iron reduction) and 3.85–3.93 V (manganese reduction) depending on the iron content in the composition. The LiMn0.6Fe0.4PO4/CNT composite (x?=?0.4) (with 20 %?wt CNT) delivered a specific capacity of 120 mAhg?1 (at a discharge rate of C/20 and RT).  相似文献   

12.
Mei Li 《Ionics》2012,18(5):507-512
LiCo1−x Mn x PO4/C cathode materials are selectively synthesized by a solvothermal method in ethylene glycol solvent using glucose, LiCl, H3PO4, MnCl2·4H2O, and Co(NO3)2·6H2O as precursors. The obtained samples are characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), and transmission electron microscopy (TEM) and the electrochemical performances are also evaluated using a LAND CT2001A battery test system at room temperature. XRD result demonstrates the formation of LiCo1−x Mn x PO4 solid solution and the enlarged channels are benefit for Li+ migration. SEM graph indicates that the particle size of LiCo0.5Mn0.5PO4/C is about several hundred nanometers and aggregates to large particles located in the range of 2–3 μm. TEM image illustrates that the core/shell-structured LiCo0.5Mn0.5PO4/C solid solution is indeed obtained by this method. The high specific surface area (35 m2/g) of LiCo0.5Mn0.5PO4/C could make this solid solution contact with the electrolyte more sufficiently and benefit for Li+ transportation. The capacity, flat voltage, and cyclical stability of LiCo1−x Mn x PO4/C are improved compared to LiMnPO4 and LiCoPO4 due to the improved electronic conductivity and lithium-ion conductivity which resulted from carbon coating and foreign element incorporation.  相似文献   

13.
Effects of Mn substitution for Co and Fe on the structural and magnetic properties of inverse-spinel CoFe2O4 have been investigated. MnxCo1−xFe2O4 and MnyCoFe2−yO4 thin films were prepared by a sol–gel method. The observed increase of the lattice constant of MnxCo1−xFe2O4 indicates that Mn2+ ions substitute the octahedral Co2+ sites. Conversion electron Mössbauer spectroscopy data indicate that a fraction of octahedral Co2+ ions exchange sites with tetrahedral Fe3+ ions through Mn doping. Vibrating-sample magnetometry data exhibit a large increase of saturation magnetization for both MnxCo1−xFe2O4 and MnyCoFe2−yO4 films compared to that of the CoFe2O4 film. Such enhancement of magnetization can be explained in terms of a breaking of ferrimagnetic order induced by the Co2+ migration.  相似文献   

14.
A series of carbon-coated LiFe1???x Mn x PO4 compounds are prepared by a hydrothermal method at 170 °C for 12 h. The structure and morphology of the prepared composites are characterized to examine the effects of Mn2+ substitution. All LiFe1???x Mn x PO4 compositions are found to have an ordered olivine-type structure with homogeneous Fe2+ and Mn2+ distributions. The substitution leads to grain refinement from ~500 to ~150 nm, as well as to increased initial capacity and improved electronic conductivity. The amount of carbon coating varies with increased doping amount. The discharge curves of the LiFe1???x Mn x PO4/C materials reveal a high discharge plateau corresponding to Fe2+/3+ and no obvious plateau assigned to Mn2+/3+, although a slight contribution of manganese is detected. However, the electrochemical performance, including the discharge capacity and cyclic performance, deteriorates with increased Mn content in the composite.  相似文献   

15.
Perovskite-type La(Cr1−xMnx)O3+δ (0.0x1.0) was synthesized using a sol–gel process. The crystal structure of La(Cr1−xMnx)O3+δ changes from orthorhombic to rhombohedral at x=0.6. The Mn4+ ion content increases monotonically in the range 0.2x1.0. The magnetic measurement of La(Cr1−xMnx)O3+δ indicates that a Mn3+ ion is a high-spin state with (d)3(dγ)1. The variation of the average (Cr, Mn)-O distance is explained by ionic radii of the Cr3+, the Mn3+, the Mn4+ ions. Since the log σT–1/T curve is linear and the Seebeck coefficient (α) is independent of temperature, it is considered that La(Cr1−xMnx)O3+δ is a p-type semiconductor and exhibits the hopping conductivity.  相似文献   

16.
We have investigated the magnetic transition and magnetocaloric effects of Mn 1+x Co 1 x Ge alloys by tuning the ratio of Mn/Co.With increasing Mn content,a series of first-order magnetostructural transitions from ferromagnetic to paramagnetic states with large changes of magnetization are observed at room temperature.Further increasing the content of Mn (x=0.11) gives rise to a single second-order magnetic transition.Interestingly,large low-field magnetic entropy changes with almost zero magnetic hysteresis are observed in these alloys.The effects of Mn/Co ratio on magnetic transition and magnetocaloric effects are discussed in this paper.  相似文献   

17.
Zhang Li  Han Guo-Cai 《中国物理 B》2013,22(2):27803-027803
Novel Dy3+-doped Gd(PO3)3 white light phosphors each with an orthorhombic system are successfully synthesized by solid-state reaction. The luminescence properties of white-light Gd1-x(PO3)3:xDy3+ (0<x≤ 0.25) under vacuum ultraviolet (VUV) excitation are investigated. The strong absorption at around 147 nm in excitation spectrum energy can be transferred to the energy levels of Dy3+ ion from the host absorption. Additionally, the white light phosphor is activated by a single Dy3+ ion. Therefore, the luminescence of Gd1-x(PO3)3:xDy (0<x≤ 0.25) under VUV excitation is effective, and it has the promise of being applied to mercury-free lamp.  相似文献   

18.
本文用DFT计算方法研究了LiFexMn1-xPO4的热力学稳定性和嵌/脱锂电位. 结果表明,LiFexMn1-xPO4固溶体的自由能比相分离的LiFePO4/LiMnPO4混合物略高,这两种形式可能在实际LiFexMn1-xPO4材料中共存. 计算表明,LiFexMn1-xPO4固溶体的嵌/脱锂电位随锰/铁比以及过渡金属离子的空间排列而变化,并用计算结果解释了放电曲线的形状. 采用固相反应法合成了LiFexMn1-xPO4材料并研究了其电化学性质,实验中观察到附加的放电平台,其出现可能与LiFexMn1-xPO4固溶体的存在有关.  相似文献   

19.
利用X射线衍射(XRD)和X射线吸收近边结构(XANES)方法研究了在Si(100)衬底上及600℃温度条件下用分子束外延(MBE)共蒸发方法生长的MnxSi1-x磁性薄膜的结构.由XRD结果表明,只有在高Mn含量(8%和17%)样品中存在着Mn4Si7化合物物相.而XANES结果则显示,对于Mn浓度在0.7%到17%之间的MnxSi1-x样品,其Mn原子的XANES谱表现出了一致的谱线特征.基于多重散射的XANES理论计算进一步表明,只有根据Mn4Si7模型计算出的理论XANES谱才能够很好的重构出MnxSi1-x样品的实验XANES谱.这些研究结果说明在MnxSi1-x样品中,Mn原子主要是以镶嵌式的Mn4Si7化合物纳米晶颗粒存在于Si薄膜介质中,几乎不存在间隙位和替代位的Mn原子. 关键词xSi1-x磁性薄膜')" href="#">MnxSi1-x磁性薄膜 分子束外延 XRD XANES  相似文献   

20.
Ling Wu  Shengkui Zhong  Jiajia Lu  Jiequn Liu  Fan Lv 《Ionics》2013,19(7):1061-1065
LiMn1-x Cr x PO4/C (x?=?0, 0.01, 0.03, and 0.05) compounds are synthesized by a sol–gel combined ball milling method. The effects of Cr doping on the structure, morphology, and electrochemical performance of LiMnPO4 are investigated. XRD analysis results indicate that all the samples exhibit the single LiMnPO4 phase and Cr ions substitute on Mn site (x?≤?0.03), with charge compensating vacancies on Li site. The vacancies are of benefit to improving the electronic conductivity of LiMnPO4. SEM studies reveal that Cr doping can effectively inhibit the aggregation of LiMnPO4 particles. Electrochemical tests show that the Cr-doped samples exhibit higher initial capacities and better cycling performance than the undoped one. LiMn0.97Cr0.03PO4/C exhibit the best electrochemical performance that the first specific discharge capacity is 132.4 mAh g?1 at 0.1 C rate, and the capacity retention is 94.8 % after 30 cycles.  相似文献   

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