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6篇 您的检索式：作者名="Pashinin"

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		题名	作者	年代	出处	被引量
	1	Passive Q switching of a neodymium laser by a Cr^4+:YAG crystal switch 显示文摘	II'ichev N N Gulyamova E S Pashinin P P	1997	Quantum Electronics1997，27，11：	1
	2	laser ablation of dental materials using a microsecond Nd:YAG laser 显示文摘	Siniaeva M L Siniavsky M W Pashinin V P	2009	Laser Physics2009，19，5：	1
	3	Formation and electrochemical properties of the superhydrophobic nanocomposite coating on PEO pretreated Mg–Mn–Ce magnesium alloy显示文摘	S.V. Gnedenkov V.S. Egorkin S.L. Sinebryukhov I.E. Vyaliy A.S. Pashinin A.M. Emelyanenko L.B. Boinovich	2013	Surface & Coatings Technology2013，，：	1
	4	HF激光脉冲与水柱表面相互作用产生电信号(英文)显示文摘研究了脉冲HF激光与水柱表面相互作用下电信号的产生过程。电信号显示了与激光能量线性相关的峰值间有时间间隔的两峰结构,且第二个尖峰在水柱底部的蒸汽腔塌缩后出现。实验还显示电信号的幅值和激光脉冲照射过程中是否存在膨胀和挤压的薄水层密切相关。如果在电池上边缘和石英平板(石英板紧邻电池,并与水柱上表面相接)之间存在一薄水层,电信号强度会增加10倍。	ANDREEV S N FIRSOV K N KAZANTSEV S Yu KONONOV I G PASHININ P P 张来明阮鹏	2011	中国光学2011，4，1：	1
	5	Generation of an electrical signal upon the interaction of laser radiation with water surface显示文摘	S. N. Andreev N. N. Il’ichev K. N. Firsov S. Yu. Kazantsev I. G. Kononov L. A. Kulevskii P. P. Pashinin	2007	Laser Physics2007，，8：	1
	6	An Investigation of Near-Equatorial Geomagnetic Pi2 Pulsations显示文摘There is understanding to date that Pi2 pulsations have two sources. One source is a high-latitude one and is due to fluctuations of electro jet parameters. The other source is a mid-latitude one and is driven by a global mode excited in the Earths plasmasphere. There is experimental evidence that in the nearequatorial regions the character of Pi2 excitation is different from high and mid-latitudes. In this connection,we investigated the amplitude-spectral-polarization characteristics of Pi2 pulsations using the date from nearequatorial Chinese stations. The detected regularities in the excitation of near-equatorial Pi2 pulsations are used in the discussion of the possible physical mechanism that is responsible for the generation of these pulsations.	A. Y. Pashinin R. A. Rakhmatulin H. Zhao	2005	空间科学学报2005，25，5：	0

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