CdxZn1-xO∶Eu3+荧光粉的制备及其发光性质

采用高温固相法在1 100 ℃下合成了Eu3+掺杂的CdxZn1-xO发光材料.采用X射线衍射对所合成样品的结构进行了表征.分析了不同浓度Cd2+的掺杂对于样品发光及激发峰位置的影响.通过对荧光光谱的测试,表明Cd2+的引入使得体系的禁带宽度变窄,并且通过Cd2+掺杂浓度的变化,可以对样品的激发光谱峰值在380～410 nm进行调制,样品的发光以520 nm处的宽带发射为主,并没有明显的Eu3+的特征发射,表明基质与Eu3+之间的能量传递并不有效.在加入Li+作为电荷补偿剂之后,出现了来自Eu3+的特征发射,相应的发射光谱的发射主峰位于609 nm.样品380～410 nm的激发峰范围覆盖了紫外LED芯片的输出波长.因此,这种荧光粉是一种可能应用在白光LED上的红色荧光粉材料.     

白光LED用Ca7（SiO4）2Cl6∶Eu2+荧光粉的光谱性能研究

通过高温固相法制备了用于紫外激发白光LED的蓝绿色Ca7(SiO4)2Cl6∶Eu2+荧光粉,并对样品进行了XRD分析和发光性能测试。结果表明,合成的样品为单相Ca7(SiO4)2Cl6;在紫外光激发下,样品的发射谱包括418和502nm两个发射峰。分别监测这两个发射峰,得到了峰值位于290和360nm处的两个宽带激发谱,说明Eu2+离子在基质晶格中可能占有两个不同的格位。研究了Eu2+离子浓度对发光强度的影响,最佳掺杂浓度为0.75mol%。结果表明该荧光粉是一种较好的蓝绿色发光材料。     

发光二极管用红色荧光粉SrMoO4:Eu3+的制备和发射性质

采用化学共沉淀法制备了适合于紫外、近紫外、蓝光发光二极管(LED)激发的红色荧光粉SrMoO4:Eu3+.研究了样品的晶体结构和发光性质.结果表明:化学共沉淀法合成的SrMoO4:Eu3+荧光粉为四方纯相,其激发光谱包括一个宽带峰和一系列尖峰,峰值位于280nm(宽带峰中心),395nm,465nm,可以被紫外LED和蓝光LED有效激发.在395nm的激发下,测得发射光谱的强发射峰位于613nm,对应Eu3+离子的5D0→7F2跃迁.Eu3+离子掺杂浓度的改变对基质的晶格常数、Eu3+离子在晶体中对称性及发光性能有较大影响.通过对比不同掺杂浓度Eu3+离子的发射谱,发现在SrMoO4基质中Eu3+离子掺杂存在浓度猝灭现象,其最佳掺杂浓度为15%.     

K_2ZnSiO_4∶Eu~(3+)红色荧光粉的制备及发光性能

采用高温固相法合成了适合近紫外光、蓝光激发的K2ZnSiO4∶Eu3+红色荧光粉,研究了该荧光粉的发光特性。XRD结果显示,所合成的荧光粉主晶相为K2ZnSiO4。样品的激发光谱由O2-→Eu3+电荷迁移带(200~350nm)和Eu3+离子的特征激发峰(350~500nm)组成,最强峰位于396nm,次强峰位于466nm。在396nm和466nm激发下,样品均呈多峰发射,分别由Eu3+离子的5D0→7FJ(J=0,1,2,3,4)能级跃迁产生,其中619nm处峰值最大。增加Eu3+离子的掺杂浓度,荧光粉的发光逐渐增强。在实验测定的浓度范围内,未出现浓度猝灭现象。不同Eu3+浓度样品的色坐标均位于色品图红光区,非常接近NTSC标准。     

用于白光LED的高亮度蓝白色荧光粉Ca2SiO3Cl2∶Eu2+的发光性质

采用固相法在较低温度下合成了Eu2 激活的Ca2S iO3C l2高亮度蓝白色发光材料,并对其发光性质进行了研究。其发射光谱由两个谱带组成,峰值分别位于420,498 nm处,归结为Ca2S iO3C l2晶体中占据两种不同Ca2 格位的Eu2 离子的5d→4 f跃迁发射。改变Eu2 浓度,可以使样品的发光在蓝白色和绿白色之间变化。当Eu2 浓度为0.005 mol-1时,样品呈现很亮的蓝白色发光。两个发射峰的激发光谱均分布在250~410nm的波长范围内,峰值分别位于333,369 nm处。Ca2S iO3C l2∶Eu2 可被InGaN管芯产生的近紫外辐射有效激发,是一种性能良好的白光LED用单一基质蓝白色荧光粉。     

Ba_2Ca(PO_4)_2:Eu~(2+)蓝色荧光粉的合成及其发光特性

采用高温固相法合成了Ba2Ca(PO4)2:Eu2+蓝色荧光粉,研究了合成温度、合成时间、Ba/Ca比值以及Eu2+掺杂量等对材料的物相及发光特性等的影响.研究结果显示,合成温度为900/1200?C,合成时间为4 h时,可以获得纯相的Ba2Ca(PO4)2;以343 nm紫外线作为激发源时,Ba2Ca(PO4)2:Eu2+呈非对称的宽谱特征,主峰位于454 nm,分析认为,Eu2+在Ba2Ca(PO4)2中占据不同的晶体学格位,形成了不同的发光中心,造成材料呈非对称发射;监测454 nm发射峰,对应的激发光谱覆盖200—450 nm区域,主峰位于343 nm,且在长波紫外段(350—410 nm)有很强的激发带;增大Eu2+掺杂量,Eu2+在Ba2Ca(PO4)2中的发射出现了浓度猝灭现象,且材料的发射峰出现了明显的红移;减小基质中Ba/Ca配比,材料在绿色区域的发射逐渐增强,材料的发光颜色由蓝逐渐变为蓝绿色,分析认为,Eu2+进入Ba2Ca(PO4)2基质体系后,不但取代Ba2+的格位,而且取代Ca2+的格位,形成不同的发光中心,从而影响材料的发光特性.     

白光LED用Ba3SiO4Cl2∶Eu2+材料的光谱特性

采用高温固相法合成了Ba₃SiO₄Cl₂∶Eu2+蓝绿色荧光粉,并测量了材料的光谱特性等。研究结果显示,在365 nm近紫外光激发下,Ba₃SiO₄Cl₂∶Eu2+材料呈双峰宽带发射,主发射峰分别为445和510 nm;分别监测这两个发射峰,所得激发光谱覆盖范围为250～450 nm,主激发峰分别为350和400 nm,但光谱分布不同,说明两发射峰来源于不同的Eu2+发光中心。研究了Eu2+掺杂浓度对材料光谱性能的影响,发现随Eu2+掺杂量的增大,445 nm发射峰的强度增加,而510 nm发射峰的强度减弱。采用去离子水清洗Ba₃SiO₄Cl₂∶Eu2+材料后,445 nm发射峰消失,只保留了510 nm发射峰,且发射峰的强度明显减弱。     

CaZn2(PO4)2:Eu3+的制备及其发光性能

采用高温固相法合成了CaZn2( PO4)2:Eu3+橙红色荧光粉,研究了其发光特性.该荧光粉在350 ～410nm处有一个宽带激发,其激发主峰位于394 nm.在紫外激发下,发射峰分别由Eu3的5D0→7F1(585,595nm)、5D0→7F2(615、622 nm)、5Do→7F3 (645 nm)及5Do→7F...     

白光LED用Sr_3(PO_4)_2∶Eu~(2+)蓝色荧光粉的制备及发光性能研究

采用高温固相法在N2-H2还原气氛下合成了一系列Sr3(PO4)2∶Eu2+蓝色荧光粉,通过X射线衍射仪(XRD)、荧光光谱仪(PL)对荧光粉的晶体结构、激发和发射光谱进行了表征。结果表明:微量的Eu2+掺杂不会改变其晶体结构;Sr3(PO4)2∶Eu2+荧光粉在310~390nm范围内可以有效的被激发,激发峰位于359nm;发射光谱为主峰位于438nm宽带发射(带宽约为150nm),对应于Eu2+的4f65d1→4f7跃迁.通过高斯拟合发现,Eu2+至少占据了Sr3(PO4)2两种不同的Sr2+格位,形成两个发光中心(430和459nm).当Eu2+的掺杂浓度为7%时,其具有最大的发光强度,继续增大Eu2+的掺杂浓度,Sr3(PO4)2∶Eu2+的发射光谱会出现浓度猝灭现象,且其发射峰会随着铕离子浓度增加而发生红移。Sr3(PO4)2∶Eu2+荧光粉在近紫外区有着强而宽的吸收带,与近紫外LED芯片发射相匹配,相对发光强度是蓝色荧光粉BaMgAl10O17∶Eu2+(BAM)的1.3倍,是一种很有前途的白光LED用蓝色荧光粉材料。     

绿色荧光粉NaCaPO_4∶Tb~(3 )的制备与发光特性

采用高温固相法合成了适用于UVLED芯片激发的NaCaPO4∶Tb3 绿色荧光粉并对其发光性质进行了研究。该荧光粉的发射峰位于418,440,492,545,586,622nm,分别对应Tb3 的5D3→7F5、5D3→7F4、5D4→7F6、5D4→7F5、5D4→7F4、5D4→7F3能级跃迁。其中位于492,545nm的发射峰最强,样品发射很好的绿光。主要激发峰位于380~400nm之间,属于4f→4f电子跃迁吸收,与UVLED芯片的发射相匹配。考察了Tb3 掺杂浓度和Li ,Na 和K 作为电荷补偿剂对样品发光性能的影响:Tb3 的最佳掺杂浓度为10%,以Li 的补偿效果最好。NaCaPO4∶Tb3 是一种适用于白光LED的绿色荧光材料。     

Current-confined-path (CCP) giant magnetoresistive (GMR) sensors

Current-perpendicular-to the plane (CPP) giant magnetoresistive (GMR) sensors with a current-confined-path (CCP) layer inserted within the Cu spacer have been manufactured using ultrahigh vacuum PVD sputtering, photolithography, and ion milling processes. Compared with a pure metallic CPP system, the CCP insertion layer enables a substantial increase in sensor resistance with an equivalent or better GMR ratio, and thus a significant improvement in the ΔRA amplitude. Heads with such a sensor have been tested under various bias currents, both quasistatically and on a spinstand. It was found that the resistance of the sensors increases with increasing bias current and voltage, following typical metallic behavior. Also, the CCP insertion layer enables operation at higher bias currents compared with the pure metallic sensors (without the insertion layer) and thus a higher output signal. This effect is attributed to less magnetic instability due to the reduced Ampere fields around the narrow (∼6 nm) current-confined paths. Finally, the CPP-GMR heads with CCP layer were tested under high-density recording conditions using the perpendicular recording media. Bit error rate (BER) as a function of linear density is reported. Microtrack profiles were also recorded to determine track density capability.     

Er0.1La0.9P5O14非晶的双光子上转换发光

本文研究了全浓度ＥｒＬａＰ５Ｏ１４非晶在波长λ为６４９．０ｎｍ脉冲染料激光激发下的上转换发光现象，并对其进行了简要的分析。     

Surface modification of poly(styrene-b-(ethylene-co-butylene)-b-styrene) elastomer via photo-initiated graft polymerization of poly(ethylene glycol)

Poly(styrene-b-(ethylene-co-butylene)-b-styrene) (SEBS) copolymer biomedical elastomer was covalently grafted with poly(ethylene glycol) methyl ether methacrylate (PEGMA) via a photo-initiated graft polymerization technique. The surface graft polymerization of SEBS with PEGMA was verified by ATR-FTIR and XPS. Effect of graft polymerization parameters, i.e., monomer concentration, UV irradiation time and initiator concentration on the grafting density was investigated. Comparing with the virgin SEBS film, the PEGMA-modified SEBS film presented an enhanced wettability and a larger surface energy. Besides, the surface grafting of PEGMA imparted excellent anti-platelet adhesion and anti-protein adsorption to the SEBS surface.     

三螺旋DNA分子poly(dT)·poly(dA)·poly(dT)的构型和振动谱

我们计算了ｐｏｌｙ（ｄＴ）·ｐｏｌｙ（ｄＡ）·ｐｏｌｙ（ｄＴ）的Ｈｏｗａｒｄ模型的原子笛卡尔坐标，并利用晶格动力学方法对模型进行了简正分析。结果发现其０ Ｐ ０对称振动模式位于８０４ｃｍ－１，这和８１０ｃｍ－１附近没有拉曼和红外谱线的实验结果不符。在８００～１０００ｃｍ－１的范围内只有四个振动模式，明显少于拉曼和红外光谱在该范围内的谱线数目。所以我们认为Ｈｏｗａｒｄ模型需要进一步地完善和修正，ｐｏｌｙ（ｄＴ）·ｐｏｌｙ（ｄＡ）·ｐｏｌｙ（ｄＴ）必须具有三条不完全一致的脊骨     

Compaction of poly(dimethylsiloxane) (PDMS) due to proton beam irradiation

This work is about the detailed investigation of the changes of the surface topography, the degree of compaction/shrinkage and its relation to the irradiation fluence and the structure spacing in poly(dimethylsiloxane) (PDMS) patterned with 2 MeV proton microbeam. The irradiated periodic structures consisted of parallel lines with different widths and spacing. To achieve different degrees of compaction, each structure was irradiated with more different fluences. At the irradiated areas the surface topography, the adhesion, the wettability and the rigidity of the surface also changes due to the chemical/structural change of the basic poly(dimethylsiloxane) polymer. The surface topography, the phase modification of the surface, and the connection between them was revealed with using an atomic force microscope (AFM).     

Spin-diffusion lengths in dilute Cu(Ge) and Ag(Sn) alloys

We used current-perpendicular-to-plane (CPP) exchange-biased spin valves to directly measure spin-diffusion lengths ?_sf^N for N=Cu(2.1 at% Ge) and Ag(3.6 at% Sn) alloys. We found ?_sf^{Cu(2% Ge)}=117₋₆⁺¹⁰ nm and ?_sf^{Ag(4% Sn)}=39±3 nm. The good agreement of this ?_sf^{Cu(2% Ge)} with the value ?_sf^{Cu(2% Ge)}=121±10 nm derived from an independent spin-orbit cross-sectional measurement for Ge in Cu quantitatively validates the use of Valet-Fert theory for CPP-MR data analysis to layer thicknesses several times larger than had been done before. From the value of ?_sf^{Ag(4% Sn)}, we predicted the ESR spin-orbit cross-section for Sn impurities in Ag.     

Energy Dispersive X-ray Diffraction (Edxd) Investigation Of Amorphous Poly(phenylacetylene) (Ppa)

The application of wide-angle x-ray diffraction in energy-dispersive modality (EDXD) to the investigation of the static structure of amorphous poly(phenylacetylene) (PPA) is discussed. The structural investigation was carried out through the systematic comparison of the measured functions (the reduced interference function and the radial distribution function) and the same functions calculated from three-dimensional theoretical models, suitably optimized. Possible configurations and conformations, coming from the combination of the polymeric repeating units, were analyzed separately. Consistent with the literature, a general agreement for a cis-transoidal head-to-tail configuration was achieved. Possible coexistence of trans-transoidal head-to-head with cis-transoidal head-to-tail configuration is also discussed. Several simple models were investigated to gain information about the chain packing. Moreover, a first quantitative investigation of the dependence of the interference function upon mechanical compression of PPA was performed.     

三丁基锡(TBT)化合物与牛血清白蛋白(BSA)的相互作用

通过紫外、荧光和圆二色(CD)光谱,研究了船体防污漆的防污成分三丁基锡(TBT)化合物与牛血清白蛋白(BSA)的相互作用,考察了浓度、酸度和有机溶剂等因素的影响。结果表明,TBT与BSA的相互作用是双重的,既有TBT中丁基基团的疏水作用,又有锡离子与BSA的配位作用,使BSA内部的色氨酸和酪氨酸等芳香氨基酸残基裸露,导致BSA二级结构破坏,α-螺旋含量减少和构象改变。     

Electrosyntheses and Characterization of Poly-N-(9-Fluorenylmethoxycarbonyl)-L-isoleucine (PFI) with Chirality

Poly-(N-(9-fluorenylmethoxycarbonyl)-L-isoleucine) (PFI) films with chirality were synthesized electrochemically by direct anodic oxidation of N-(9-fluorenylmethoxy- carbonyl)-L-isoleucine (FI) in a medium strong Lewis acid, boron trifluoride diethyl etherate (BFEE). The oxidation potential of FI in BFEE was only 0.6 V vs. Pt, which was much lower than that determined in acetonitrile + 0.1 mol L^?1 tetrabutylammonium tetrafluoroborate (TBATFB) (1.0 V vs. Pt). Results of FT-IR, UV–visible spectra and ¹H NMR spectra indicated that FI was polymerized successfully and the polymerization positions were C2 and C7. Results of electrochemical measurements showed PFI had good redox activity and stability. SEM provided the surface morphology of the PFI film. Result of thermogravimetric analyses (TG) indicated PFI films obtained from BFEE had good thermostability. As-formed PFI films can be dissolved in ethanol, N,N-Dimethylformamide(DMF), etc.     

Toughening of Poly (Butylene Terephthalate) with Epoxy-Filled Poly (Ethylene–Octene) Copolymer

Toughened poly (butylene terephthalate) (PBT) with triglycidyl isocyanurate (TGIC)-filled poly (ethylene–octene) (POE) was prepared by melt reaction extrusion. For retarding the reaction extent between PBT and the epoxy component, the TGIC was first blended with POE to enwrap its reactive epoxy groups. Then, the TGIC-filled POE was used to melt blend with PBT. The Fourier transform infrared (FTIR) spectra showed that no other peaks appeared in the POE/TGIC specimens except for those originally existing in pure POE and TGIC. The rheological results further confirmed that no reaction occurred between the epoxy and the POE matrix. When the POE/TGIC was blended with PBT, a distinct increase of the viscosity suggested that the migration of the TGIC from POE to PBT during the melt processing induced chain extension reactions of PBT. The results obtained from DSC and DMA revealed that the chain extension of PBT induced by the reaction with TGIC restricted the mobility of PBT chains leading to a limitation of the recrystallization-remelting process and an increase of the glass transition temperature of PBT. The mechanical tests showed that the presence of TGIC in the POE phase distinctly improved the toughness of PBT. Compared to the case of a PBT/POE (80/20, wt%/wt%) blend, the elongation at break and impact strength of the system filled with 5 phr TGIC were increased more than three and six times, respectively.