静电纺丝法制备La_(0.67)Ba_(0.33)MnO_3微纳米纤维及其红外发射率研究（英文）

采用静电纺丝法结合溶胶-凝胶技术制备了钙钛矿型La_(0.67)Ba_(0.33)MnO_3微纳米纤维,并利用差示扫描量热-热失重分析(DSC-TGA)、X射线衍射(XRD)、傅里叶变换红外光谱(FTIR)和扫描电子显微镜(SEM)等技术对产物进行了表征,利用IR-2红外发射率测试仪测试了La_(0.67)Ba_(0.33)MnO_3在280~370 K范围内的红外发射率.结果表明,La_(0.67)Ba_(0.33)MnO_3在600℃时已形成钙钛矿结构.随着煅烧温度的升高,La_(0.67)Ba_(0.33)MnO_3的形貌由纤维状向三维网络状转变,并最终失去纤维形态.在280~370 K范围内,La_(0.67)Ba_(0.33)MnO_3微纳米纤维的红外发射率随温度升高而升高,由0.564增加至0.689.利用钙钛矿材料双交换理论解释了这一现象,并进一步探讨了其在红外发射率可变材料中的应用前景.     

Sol-gel法制备La1-xSrxMnO3巨磁电阻薄膜材料

利用sol-gel法在单晶硅Si(100)衬底上,制备了钙钛矿La_1-xSr_xMnO₃(LSMO)低织构纳米晶薄膜.考察了制备条件对LSMO成相、晶粒的粒度和表面形貌的影响,研究了其磁特性和磁电阻性能.结果表明,La_0.7Sr_0.3MnO₃薄膜磁电阻效应在相当宽的温度范围内不随温度改变,在6T磁场中室温下磁电阻比MR值可达-30%.     

熔融碱法制备三重价态钙钛矿锰氧化物

以MnO₂, Ca(OH)₂和La(OH)₃为反应原料, 在惰性气氛、 低温(500 ℃)熔融KOH体系中合成了具有菱形钙钛矿结构Ca, K共掺杂的La_0.64Ca_0.25K_0.11MnO₃纳米材料, 并对Mn的价态及磁学性能等进行了讨论. X射线光电子能谱(XPS)分析结果表明, La_0.64Ca_0.25K_0.11MnO₃纳米材料中的Mn具有三重混合价态, 其零场冷却低温磁化率曲线表现出顺磁-铁磁转变, 居里温度(T_c)为280 K.     

负载型钙钛矿La0.8Sr0.2MnO3/SBA-15催化燃烧甲苯的研究

采用逐层负载-孔道内氨/水蒸气原位羟化法制备了一系列负载型钙钛矿La_0.8Sr_0.2MnO₃/SBA-15催化剂,用XRD、BET、TG-DTG、XPS、H₂-TPR等手段对催化剂的物性结构等进行了表征,并在常压连续流动固定床反应器上评价了该催化剂对甲苯催化燃烧的催化性能。结果表明,逐层负载-孔道内氨/水蒸气原位羟化法的使用有助于活性组分La_0.8Sr_0.2MnO₃进入SBA-15的孔道,并在SBA-15上形成钙钛矿结构。La_0.8Sr_0.2MnO₃/SBA-15上钙钛矿结构的形成和晶格氧的出现,可为催化剂提供较多的活性中心,有利于其催化燃烧甲苯的活性。     

双钙钛矿La2CoNiO6无机纳米纤维的制备及超级电容器性能

以聚乙烯吡咯烷酮/硝酸镧-乙酸钴-乙酸镍(PVP/LCN)为前驱体, 采用静电纺丝法, 经预氧化、碳化, 制得双钙钛矿La₂CoNiO₆无机纳米纤维超级电容器电极材料. 利用X射线衍射(XRD)、扫描电镜(SEM)和透射电镜(TEM)对其形貌和结构进行表征. 结果表明, 纤维由菱形结构的La₂CoNiO₆纳米颗粒相互连接而成, 呈链状空间网状结构. 循环伏安(CV)、恒流充放电(CP)和循环寿命测试表明, La₂CoNiO₆纳米纤维电极材料在三电极体系中, 电流密度为0.25 A·g^-1时, 比电容值达335.0 F·g^-1; 在对称型双电极体系中, 电流密度为0.25 A·g^-1时, 比电容值可达到129.1 F·g^-1,表现出良好的电容性能.     

La1-xLixMnO3体系的输运特性及EPR研究

利用固相反应法合成了掺杂锂的La_1-xLi_xMnO₃(x=0,0.10,0.15,0.20,0.25,0.30)钙钛矿氧化物.XRD测试表明,所有样品均为菱方结构.除x=0,0.3外,其它样品均随温度的降低在液氮温区可观察到从绝缘态到金属态的转变,其中x=0.15样品的转变温度最高为167K.在H=1T的磁场下,出现了负磁阻现象.EPR谱上的g=2.00信号与Mn³⁺和Mn⁴⁺组成的复合团簇有关.     

在温和条件下巨磁阻材料La0.5Ba0.5MnO3的水热合成与表征

报道了在温和条件下巨磁阻材料La_0.5Ba_0.5MnO₃的水热合成.系统地研究了原料配比、碱度、时间和温度对产物合成的影响,在最佳合成条件下得到了结晶度较高的纯相,并通过XRD、DTA-TG、化学分析及碘量法对产物进行了表征.该化合物属立方晶系,晶胞参数为α=0.3913nm,V=0.05990nm₃,Mn的平均价态为3.5,在1T的外磁场下,磁阻比(MR)的极大值为29%.     

La0.6Sr0.4Co1-yFeyO3钙钛矿复合氧化物的GNP法合成与导电性能

采用甘氨酸-硝酸盐(GNP)法合成出La_0.6Sr_0.4Co_1-yFe_yO₃(y=0～1.0)体系复合氧化物,对合成产物的结构、烧结性能和导电性进行了表征.研究结果表明,不同n(Co)/n(Fe)比的合成粉料中形成菱形六面体钙钛矿结构,合成粉料的颗粒细小均匀.在室温～900℃范围内,La_0.6Sr_0.4CoO₃(y=0)的电导率随温度的升高而单调降低,其它n(Co)/n(Fe)比的样品电导率随着温度升高到600℃附近时达到最大值.在低温段,La_0.6Sr_0.4Co_1-yFe_yO₃体系的导电行为符合小极化子导电机制,导电活化能随n(Co)/n(Fe)比的降低而增大.与常规固相合成法相比,甘氨酸-硝酸盐法制备的La_0.6Sr_0.4Co_1-yFe_yO₃具有更高的烧结活性和电导率.     

锂锌铁氧体微纳米纤维的电纺制备及吸波性能

采用静电纺丝技术结合后续热处理制备了尖晶石型Li_0.35Zn_0.3Fe_2.35O₄微纳米纤维. 利用差示扫描量热(DSC)-热重分析(TGA)、 傅里叶变换红外光谱(FTIR)、 X射线衍射(XRD)和场发射扫描电子显微镜(FESEM)等手段研究了煅烧温度(700, 800, 900, 1000 ℃)对产物物相和形貌的影响; 利用矢量网络分析仪分析了纤维状产物的吸波性能. 研究结果表明, Li_0.35Zn_0.3Fe_2.35O₄在700 ℃及以上温度煅烧后可生成单一尖晶石结构. 随着煅烧温度的升高, 产物依次呈现出微纳米纤维状、 三维网络状、 竹节状和颗粒状的微观形貌. 随着匹配厚度增加, 微纳米纤维状Li_0.35Zn_0.3Fe_2.35O₄的最低反射率向低频移动, 在8 GHz以下的最佳匹配厚度为6 mm, 在此厚度下吸波性能优良, 最低反射率为-26 dB, 对应的吸收频率为5.0 GHz, 低于-10 dB的吸收频带为4.0~8.0 GHz, 带宽为4 GHz.     

超疏水导电聚苯胺的界面聚合

采用界面聚合和无模板法相结合的方法, 以具有疏水链的全氟癸二酸(PFSEA)为掺杂剂, 通过调节苯胺单体和FeCl₃氧化剂的浓度实现了聚苯胺三维微/纳米结构形貌和尺寸的可控制备. 扫描电子显微镜测量结果显示, 聚苯胺是由一维纳米纤维自组装形成的三维微球结构; 红外吸收光谱和紫外-可见吸收光谱结果表明, 聚苯胺微球为掺杂态. 室温下, 该微/纳米结构聚苯胺微球的电导率为 9.6×10^-3 S/cm, 表面水接触角为161.4°, 表现出半导体特性和超疏水性.     

Gd掺杂对La0.67 Sr0.33 CoO3、La0.67 Sr0.33 MnO3体系磁行为的影响

M~T curves and M~H curves of the systems La0.67Sr0.33CoO3, La0.67Sr0.33MnO3 (x=0.00, 0.05, 0.10, 0.20, 0.30, 0.40, 0.50, 0.60, 0.67) were studied by experiments. Experimental results show that the magnetic structure of La0.67-xGdxSr0.33CoO3 system exhibits the cluster glass state with doping Gd increasing. The M~T curves of samples x>0.10 exhibit a peculiar phenomenon that M value rises sharply at low temperature range. The magnetic structure of La0.67-xGdxSr0.33MnO3 system changes from the long rang ferromagnetic order to the cluster glass state, and anti ferromagnetic state. The M~T curves of samples x≥0.50 decline sharply at low temperature range. The different phenomena shown by the two systems come from different coupling function between Gd and Co, Mn and from spin state transition of Co.     

Ultrafast photoinduced reflectivity transients in doped manganite

The temperature and magnetic field dependence of ultrafast photoinduced spin and quasiparticle relaxation dynamics is reported in La(0.67)Ca(0.33)MnO(3) and LaMnO(3) single crystals and thin films. Both manganites reveal an unusually slow ( approximately 10 micros) carrier relaxation process attributed to the spin-lattice relaxation in localized states. The quasiparticle dynamics is governed by the temperature- and magnetic field-dependent pseudogap in La(0.67)Ca(0.33)MnO(3), and by the temperature-independent Jahn-Teller gap in LaMnO(3). The loss of spectral weight near the Fermi level in La(0.67)Ca(0.33)MnO(3) strongy affects the quasiparticle relaxation dynamics as temperature increases from below T(C). Our results show that the coupled dynamics of charge, spin and lattice is strongly correlated with the distinct gap structures in these manganites.     

混合掺杂和非计量比对钕锶锰氧体系的影响

通过对Sr、Ba混合掺杂体系（x＝0．27、0．165、0．06）和非计量体系Nd0.67SrxBaxMnOz（x＝0．27．0．06）,导电性能的研究发现：混合二价离子掺杂体系Nd0.67SrxBa0.33-xMnO3与单一二价离子掺杂体系（Nd0.67Sr0.33MnO3和Nd0．67Ba0.33MnO3）具有不同的导电机制,非计量比使Nd0.67SrxBaxMnOz体系出现晶格收缩,电阻率随温度的降低出现半导体－金属转变,与此同时体系的电阻率减小,另外还发现,Mn离子的非计量与A位离子的相比对体系晶格收缩和导电性能的影响都更为显著。     

Formation of Ultrafine Apatite Fibers by Sol-gel/Electrospinning

Ultrafine apatite fibers were prepared by electrospinning of sol-gel precursor/poly（ vinyl pyrrolidone） （PVP） solutions followed by subsequent calcination. The as-electrospun and calcinated fibers were observed under a scanning electron microscope and an optical polarizing microscope. Results show that the morphology and the diameter of as-electrospun fibers strongly depend on the viscosity and the surface tension of sol-gel precursor/PVP solutions. After calcination, the smooth as-electrospun fibers shrink and the fiber diameter decreases because of the removal of the polymer. The chemical evolution upon the transformation of the precursor from a gel to the final apatite fibers was investigated by thermogravimetric-differenfial thermal analysis, X-ray diffraction, and Fourier transform infrared spectroscopy. It is thus suggested that the crystalline structure of the calcined fibers is largely influenced by the calcination temperature. After being calcined at 600 ℃, the apatite fibers with a diameter of about 280 nm containing β-tricalcium phosphate were obtained.     

相分离La0．33Pr0．34Ca0．33MnO3薄膜体系中的交换偏置效应

在相分离La0．33Pr0.34Ca0．33MnO3薄膜体系中发现了大的交换偏置效应．在4K时,交换偏置场的大小达到了约1kOe．交换偏置效应可能源自薄膜内禀的电子相分离特性或薄膜的表面效应．交换偏置效应表现出强的温度、冷却磁场以及厚度依赖的关系．     

酚醛基电纺纤维的制备和分散形态研究

用电纺技术制备了酚醛纤维及碳纤维.用合成的甲阶酚醛(A-stage resol)和聚乙烯醇(PVA)在不同配比下进行电纺,然后经150℃固化处理1h,制得酚醛(PF)纤维.将PF和PVA质量比为1∶2的酚醛纤维在不同的温度下进行热处理,得到的纤维直径均小于200nm.用场发射扫描电镜(FESEM)观察并比较了纤维的直径和分散形态.用红外光谱(IR)证实了,在600℃下热处理后的酚醛纤维为碳纤维,分散形态最为理想.     

Electronic structure of A- and B-site doped lanthanum manganites: a combined X-ray spectroscopic study

The electronic properties of a series of colossal magnetoresistance (CMR) compounds, namely LaMnO3, La(1-x)Ba(x)(MnO3 (0.2 < or = x < or = 0.55), La(0.76)Ba(0.24)Mn(0.84)Co(0.16)O3, and La(0.76)Ba(0.24)Mn(0.78)Ni(0.22)O3, have been investigated in a detailed spectroscopic study. A combination of X-ray photoelectron spectroscopy (XPS), X-ray emission spectroscopy (XES), X-ray absorption spectroscopy (XAS), and resonant inelastic X-ray scattering (RIXS) was used to reveal a detailed picture of the electronic structure in the presence of Ba, Co, and Ni doping in different concentrations. The results are compared with available theory. The valence band of La(1-x)()Ba(x)MnO3 (0 < or = x < or = 0.55) is dominated by La 5p, Mn 3d, and O 2p states, and strong hybridization between Mn 3d and O 2p states is present over the whole range of Ba concentrations. Co-doping at the Mn site leads to an increased occupancy of the e(g) states near the Fermi energy and an increase in the XPS valence band intensity between 0.5 and 5 eV, whereas the Ni-doped sample shows a lower density of occupied states near the Fermi energy. The Ni d states are located in a band spanning the energy range of 1.5-5 eV. XAS spectra indicate that the hole doping leads to mixed Mn 3d-O 2p states. Furthermore, RIXS at the Mn L edge has been used to probe d-d transitions and charge-transfer excitations in La(1-x)Ba(x)MnO3.     

Mn(I) in an extended oxide: the synthesis and characterization of La(1-x)Ca(x)MnO(2+δ) (0.6 ≤ x ≤ 1)

Reduction of La(1-x)Ca(x)MnO(3) (0.6 ≤ x ≤ 1) perovskite phases with sodium hydride yields materials of composition La(1-x)Ca(x)MnO(2+δ). The calcium-rich phases (x = 0.9, 1) adopt (La(0.9)Ca(0.1))(0.5)Mn(0.5)O disordered rocksalt structures. However local structure analysis using reverse Monte Carlo refinement of models against pair distribution functions obtained from neutron total scattering data reveals lanthanum-rich La(1-x)Ca(x)MnO(2+δ) (x = 0.6, 0.67, 0.7) phases adopt disordered structures consisting of an intergrowth of sheets of MnO(6) octahedra and sheets of MnO(4) tetrahedra. X-ray absorption data confirm the presence of Mn(I) centers in La(1-x)Ca(x)MnO(2+δ) phases with x < 1. Low-temperature neutron diffraction data reveal La(1-x)Ca(x)MnO(2+δ) (x = 0.6, 0.67, 0.7) phases become antiferromagnetically ordered at low temperature.     

La—Sm—Ca—Mn—O的晶格效应

在La0.67Ca0.33MnO3氧化物中进行了掺Sm研究,结果发现,随着Sm掺入量的增加,材料的金属-绝缘体相变温度逐渐降低,对应的峰值电阻急剧增大,居里温度逐渐下降,材料的磁电阻比迅速增加。对Sm掺杂的作用可以用晶格效应来解释。     

静电纺丝法制备LaFeO3微纳米纤维

采用静电纺丝技术并结合溶胶-凝胶方法制备了LaFeO3微纳米纤维. 用差热-热重分析(TG-DTA)、X射线衍射(XRD)、红外光谱(FTIR)、X射线光电子能谱和场发射扫描电镜(FE-SEM)对样品进行了表征. 实验结果表明, 390 ℃时钙钛矿结构的LaFeO3晶体开始形成, 同时伴有少量微弱的La2O2CO3和Fe2O3杂相存在, 600 ℃煅烧获得正交钙钛矿结构的LaFeO3微纳米纤维, 其纤维直径分布在300~600 nm之间, 其平均直径约为420 nm, 平均晶粒尺寸为28 nm.