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51.
52.
Different variation behaviors of resistivity for high-temperature-grown and low-temperature-grown p-GaN films 下载免费PDF全文
Two series of p-GaN films grown at different temperatures are obtained by metal organic chemical vapor deposition(MOCVD). And the different variation behaviors of resistivity with growth condition for high- temperature(HT)-grown and low-temperature(LT)-grown p-GaN films are investigated. It is found that the resistivity of HT-grown p-GaN film is nearly unchanged when the NH_3 flow rate or reactor pressure increases. However, it decreases largely for LT-grown p-GaN film.These different variations may be attributed to the fact that carbon impurities are easy to incorporate into p-GaN film when the growth temperature is low. It results in a relatively high carbon concentration in LT-grown p-GaN film compared with HT-grown one. Therefore, carbon concentration is more sensitive to the growth condition in these samples, ultimately,leading to the different variation behaviors of resistivity for HT- and LT-grown ones. 相似文献
53.
Output light power of InGaN-based violet laser diodes improved by using a u-InGaN/GaN/AlGaN multiple upper waveguide 下载免费PDF全文
The upper waveguide(UWG) has direct influences on the optical and electrical characteristics of the violet laser diode(LD) by changing the optical field distribution or barrier of the electron blocking layer(EBL). In this study, a series of In GaN-based violet LDs with different UWGs are investigated systematically with LASTIP software. It is found that the output light power(OLP) under an injecting current of 120 mA or the threshold current(Ith) is deteriorated when the UWG is u-In_(0.02)Ga_(0.98)N/GaN or u-In_(0.02)Ga_(0.98)N/Al_xGa_(1-x)N(0 ≤ x ≤ 0.1), which should be attributed to small optical confinement factor(OCF) or severe electron leakage. Therefore, a new violet LD structure with u-In_(0.02)Ga_(0.98)N/GaN/Al_(0.05)Ga_(0.95)N multiple layer UWG is proposed to reduce the optical loss and increase the barrier of EBL. Finally,the output light power under an injecting current of 120 mA is improved to 176.4 mW. 相似文献
54.
丁二烯/苯乙烯/4-乙烯基吡啶共聚物蒙脱土嵌入混杂材料的研究 总被引:4,自引:0,他引:4
用聚合物乳液与蒙脱土的水分散体共混共凝的方法制备混杂材料.在混合过程中乳胶粒与蒙脱土晶层相互穿插,用盐酸絮凝,带正电的共聚物能够嵌入带负电的蒙脱土层间.萃取实验发现在混杂材料中蒙脱土吸附了大量的共聚物,说明蒙脱土晶层与共聚物之间存在静电吸附作用.XRD实验发现在混杂材料中蒙脱土的晶层结构发生了膨胀,并且变得混乱,而在共混物中蒙脱土晶层结构几乎不变.用TEM观察在混杂材料中蒙脱土晶层均匀分散于共聚物基体中,蒙脱土的层间距大于6nm.共聚物嵌入蒙脱土的层间,受到蒙脱土晶层的限制作用,共聚物的Tg发生了变化.交联以后的混杂材料的性能比共聚物有了较大的提高,蒙脱土晶层在共聚物基体中起到很好的补强作用. 相似文献
55.
56.
正橡胶在三大高分子材料中由于具有不能被其它材料替代的独一无二的高弹性,被称为具有战略地位的材料,在国民经济和国防军工中有着十分广泛的应用。中国已连续多年在世界橡胶耗量和轮胎产量排行榜上位居第一。2012年,橡胶工业总产值已占我国GDP的1.67%,全球三分之一的轮胎制造于中国。在这样的一种形式下,应《高分子通报》的邀请,想出一期关于橡胶材料研究进展的专刊,反映一下近 相似文献
57.
We obtained the Cα continuity for weak solutions of a class of ultraparabolic equations with measurable coeffcients of the form
δt u = δx(a(x, y, t)δx u) + b0(x, y, t)δxu + b(x, y, t)δyu, which generalized our recent results on KFP equations. 相似文献
δt u = δx(a(x, y, t)δx u) + b0(x, y, t)δxu + b(x, y, t)δyu, which generalized our recent results on KFP equations. 相似文献
58.
The sensitive adsorptive-complex wave of the complexes formed by light rare earth elements and DSPCF is studied in this paper. The electroactivities of the complexes of light (La-Eu) and heavy rare earth elements (Gd-Lu), are quite different, so we can determine a certain light rare earth element or the total amounts of light rare earths without separating them from heavy rare earths. The mechanism of the adsorptive-complex wave and the reason why heavy rare earths could not form the electroactive complexes have been studied as well. 相似文献
59.
张立群 《数学物理学报(A辑)》1991,11(2):130-142
本文讨论方程正解的唯一性 作者证明了若f(u)=-u+u~p,则存在ε~*>0,使当1
0,使当|ε|<ε~*时,方程(Ⅰ)的正解是唯一的。 相似文献
60.
A violet laser diode (LD) structure is grown on a
free-standing c-plane GaN substrate and 4~μ m× 800~μ
m ridge waveguide LDs are fabricated. The electrical and the
optical characteristics of LDs under different facet-coating and
chip-mounting conditions are investigated under pulse mode
operation. The active region temperatures of p-side up and p-side
down mounted LDs are calculated with different injection currents.
The calculated thermal resistances of p-side up and p-side down
mounted LDs are 4.6~K/W and 3~K/W, respectively. The threshold
current of the p-side down mounted LD is much lower than that of the p-side
up mounted LD. The blue shift of the emission wavelength with increasing
injection current is observed only for the LD with p-side down mounting
configuration, due to the more efficient heat dissipation. 相似文献