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绝热极限下HMMC链中的量子晶格涨落效应
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作者 王沁 刘吉超 《新疆师范大学学报(自然科学版)》 1998年第4期15-21,41,共8页
准一维HMMC链的物理结构和相互作用特点决定着系统各种对称破缺基态存在的可能性。为分析电声子相互作用和二聚化位移,从Hamiltonian模型出发,采用正则变换和位移变换,引进电子一声子散射函数,对绝热极限条件下HMMC链系统进行了研究。... 准一维HMMC链的物理结构和相互作用特点决定着系统各种对称破缺基态存在的可能性。为分析电声子相互作用和二聚化位移,从Hamiltonian模型出发,采用正则变换和位移变换,引进电子一声子散射函数,对绝热极限条件下HMMC链系统进行了研究。讨论了系统的二聚化相变、能隙、准粒子激发能谱等,并根据基态能量应满足的变分极值条件,得到确定格点位移二聚化序参量的自洽方程。结果表明,在绝热极限情况下,当电声子耦合强度很小时,系统的二聚化非常弱。随着电声子耦合强度的不断增强,系统的二聚化程度不断增大。 展开更多
关键词 量子晶格涨落 绝热极限 序参量 电声子耦合
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无自旋态反绝热极限下MX链晶体中的量子晶格涨落效应
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作者 王沁 《新疆师范大学学报(自然科学版)》 1999年第3期27-34,共8页
MX链的准一维、电子跃迁、电子——声子耦合和电子——电子相互作用等物理特性决定着系统的相转变和对称破缺电荷密度波态的稳定性。从紧束缚Hamiltonian模型出发,在反绝热极限条件下,对费米子无自旋态MX链系统进行了研究。讨论了系统... MX链的准一维、电子跃迁、电子——声子耦合和电子——电子相互作用等物理特性决定着系统的相转变和对称破缺电荷密度波态的稳定性。从紧束缚Hamiltonian模型出发,在反绝热极限条件下,对费米子无自旋态MX链系统进行了研究。讨论了系统的电荷密度波态,二聚化相变、绝缘相能隙等。并根据基态能量的解析性质,得到确定导体相的Luttingcr指数。计算结果表明,在反绝热极限情况下,系统存在一非平凡相变点。电声子耦合强度大于临界值时,系统处于二聚化电荷密度波态,小于临界值时,系统处于Luttinger液体相。 展开更多
关键词 MX链 二聚化相变 量子晶格涨落 绝热极限
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反绝热极限下MX链晶体中的量子晶格涨落效应:费米子自旋1/2态
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作者 王沁 《新疆师范大学学报(自然科学版)》 2000年第4期26-31,42,共7页
相转变和对称破缺电荷密度波态的稳定性等物理特性决定于MX链系统的准一维、电子跃迁、电子-声子耦合和电子-电子相互作用。为讨论费米子自旋态MX 链系统的量子晶格涨落效应,从紧束缚Hamiltonisn模型出发,在反绝热... 相转变和对称破缺电荷密度波态的稳定性等物理特性决定于MX链系统的准一维、电子跃迁、电子-声子耦合和电子-电子相互作用。为讨论费米子自旋态MX 链系统的量子晶格涨落效应,从紧束缚Hamiltonisn模型出发,在反绝热极限条件下,采用Hartree-Fock近似,对MX链系统的电荷密度波序参量,绝缘相能隙,基态能量等进行了研究,并得到确定绝缘相能隙的自洽解方程。计算结果表明,在反绝热极限条件下,绝缘相能隙随电声子耦合强度的增大而增大,当电声子耦合强度达到临界值时,系统发生二聚化相变。 展开更多
关键词 对称破缺电荷密度波态 绝缘相能隙 绝热极限
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准经典极限与绝热极限之间的对易性
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《中国基础科学》 2006年第2期60-60,共1页
依赖于某些外界参量的量子系统存在两种极限:一是准经典极限n→0,在这个极限下量子系统表现得越来越像经典系统;二是绝热极限,也就是外界参量随时间的变化率α→0。J.T.Hwang(1977)等曾论证这两种极限等价。但M.V.Berry(198... 依赖于某些外界参量的量子系统存在两种极限:一是准经典极限n→0,在这个极限下量子系统表现得越来越像经典系统;二是绝热极限,也就是外界参量随时间的变化率α→0。J.T.Hwang(1977)等曾论证这两种极限等价。但M.V.Berry(1984)发现这两种极限不但不等价而且不对易。 展开更多
关键词 绝热极限 经典极限 对易 量子系统 经典系统 系统表 变化率 外界 等价 时间
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Numerical Analysis of Explosion Characteristics of Vent Gas From 18650 LiFePO_(4) Batteries With Different States of Charge
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作者 Shi-Lin Wang Xu Gong +5 位作者 Li-Na Liu Yi-Tong Li Chen-Yu Zhang Le-Jun Xu Xu-Ning Feng Huai-Bin Wang 《电化学(中英文)》 CAS 北大核心 2024年第8期28-35,共8页
The combustion and explosion characteristics of lithium-ion battery vent gas is a key factor in determining the fire hazard of lithium-ion batteries.Investigating the combustion and explosion hazards of lithium-ion ba... The combustion and explosion characteristics of lithium-ion battery vent gas is a key factor in determining the fire hazard of lithium-ion batteries.Investigating the combustion and explosion hazards of lithium-ion batteries vent gas can provide guidance for rescue and protection in explosion accidents in energy storage stations and new energy vehicles,thereby promoting the application and development of lithium-ion batteries.Based on this understanding and combined with previous research on gas production from lithium-ion batteries,this article conducted a study on the combustion and explosion risks of vent gas from thermal runaway of 18650 LFP batteries with different states of charge(SOCs).The explosion limit of mixed gases affected by carbon dioxide inert gas is calculated through the“elimination”method,and the Chemkin-Pro software is used to numerically simulate the laminar flame speed and adiabatic flame temperature of the battery vent gas.And the concentration of free radicals and sensitivity coefficients of major elementary reactions in the system are analyzed to comprehensively evaluate the combustion explosion hazard of battery vent gas.The study found that the 100%SOC battery has the lowest explosion limit of the vent gas.The inhibitory elementary reaction sensitivity coefficient in the reaction system is lower and the concentration of free radicals is higher.Therefore,it has the maximum laminar flame speed and adiabatic flame temperature.The combustion and explosion hazard of battery vent gas increases with the increase of SOC,and the risk of explosion is the greatest and most harmful when SOC reaches 100%.However,the related hazards decrease to varying degrees with overcharging of the battery.This article provides a feasible method for analyzing the combustion mechanism of vent gas from lithium-ion batteries,revealing the impact of SOC on the hazardousness of battery vent gas.It provides references for the safety of storage and transportation of lithium-ion batteries,safety protection of energy storage stations,and the selection of related fire extinguishing agents. 展开更多
关键词 Combustion and explosion characteristics Explosion limit Laminar flame speed Adiabatic flame temperature Sensitivity analysis
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旋转中子及螺旋光纤的几何相 被引量:2
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作者 高玉梅 胡连 张晓燕 《华南师范大学学报(自然科学版)》 CAS 2005年第1期60-65,81,共7页
计算得到自旋1/2粒子在旋转磁场下的Bloch方程的严格解及精确波函数,Berry几何相可对演化波函数取绝热极限得到,并将结果与Bitter等的慢中子实验做了比较.对旋转磁场的一般非绝热循环解,给出了Aharonov Anandan(AA)几何相和动力学相的... 计算得到自旋1/2粒子在旋转磁场下的Bloch方程的严格解及精确波函数,Berry几何相可对演化波函数取绝热极限得到,并将结果与Bitter等的慢中子实验做了比较.对旋转磁场的一般非绝热循环解,给出了Aharonov Anandan(AA)几何相和动力学相的解析结果,并用AA几何相理论圆满的解释了有争议的螺旋光纤实验,这项研究证明的关于AA的另一定理表明:对非绝热动力学相取绝热根限时,可得到绝热的动力学相和绝热的几何相.建议用正交态方法排除绝热近似而获得平行传输条件,从而实现所谓几何量子计算. 展开更多
关键词 螺旋光纤 Berry几何相 BLOCH方程 动力学相 旋转磁场 演化波函数 绝热极限 解析结果 传输条件 绝热近似 量子计算 绝热 严格解 慢中子 循环解 正交态 实验 AA 粒子 自旋 定理
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从A-A相到Berry几何相 被引量:2
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作者 孙世军 赵鹏飞 《湛江师范学院学报》 2001年第6期6-9,共4页
研究核磁共振系统产生A -A相的条件 ,计算出核磁共振系统的A -A相 ,并在绝热极限下从A
关键词 A-A相 Berry几何相 核磁共振系统 绝热极限 状态演变 波函数
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关于核磁共振系统两类A-A相的计算
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作者 孙世军 彭承琳 +1 位作者 张爱萍 罗光 《重庆大学学报(自然科学版)》 EI CAS CSCD 北大核心 2003年第2期63-67,共5页
从求解核磁共振系统Schr dinger方程的一般解出发 ,得到核磁共振系统产生A -A相的cyclic条件和循环初态条件。cyclic条件要求系统的频率只能取离散的序列而初态可以是任意的 ;循环初态条件要求对系统的初态作一定的限定而系统的频率可... 从求解核磁共振系统Schr dinger方程的一般解出发 ,得到核磁共振系统产生A -A相的cyclic条件和循环初态条件。cyclic条件要求系统的频率只能取离散的序列而初态可以是任意的 ;循环初态条件要求对系统的初态作一定的限定而系统的频率可以是任意的。在此基础上计算出系统在满足cyclic条件和循环初态条件时产生的A -A相 ,在cyclic条件下 ,系统产生的A -A相是依赖于初态和大于 1的自然数的离散序列 ;在循环初态的条件下 ,系统产生的A -A相仅依赖于频率。证明了在绝热极限下 ,从这两类A 展开更多
关键词 计算 A-A相 核磁共振系统 绝热极限 Berry几何相
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Evaluation of dynamic performance and ballistic behavior of Ti-5Al-5Mo-5V-3Cr-1Zr alloy 被引量:2
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作者 王艳玲 惠松骁 +1 位作者 刘睿 叶文君 《Transactions of Nonferrous Metals Society of China》 SCIE EI CAS CSCD 2015年第2期429-436,共8页
Terminal ballistic tests using 7.62 mm armor-piercing incendiary (API) projectiles were performed to evaluate the resistance to penetration of Ti-5Al-5Mo-5V-3Cr-IZr (Ti-55531) alloy. The dynamic properties were de... Terminal ballistic tests using 7.62 mm armor-piercing incendiary (API) projectiles were performed to evaluate the resistance to penetration of Ti-5Al-5Mo-5V-3Cr-IZr (Ti-55531) alloy. The dynamic properties were determined by a split Hopkinson pressure bar (SHPB) test system. Ti-55531 plates were subjected to two kinds of heat treatments, leading to the formation of high-strength and high-toughness plates. The results of SHPB test exhibit that the maximum impact absorbed energy of the high-strength plate at a strain rate of 2200 s^-1 is 270 MJ/m^3; however, the maximum value for the high-toughness plate at a strain rate of 4900 s^-1 is 710 MJ/m^3. The ballistic limit velocities for the high-strength and high-toughness plates with dimensions of 300 mm×300 mm×8 mm are 330 and 390 m/s, respectively. Excellent dynamic properties of Ti-55531 alloy correspond to good resistance to penetration. The microstructure evolution related to various impact velocities are observed to investigate the failure mechanism. 展开更多
关键词 Ti-5Al-5Mo-5V-3Cr-1Zr alloy dynamic property split Hopkinson pressure bar adiabatic shear band ballisticbehavior ballistic limit
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Necessity of Integral Formalism
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作者 陶勇 《Communications in Theoretical Physics》 SCIE CAS CSCD 2011年第10期648-654,共7页
To describe the physical reality, there are two ways of constructing the dynamical equation of field, differential formalism and integral formalism. The importance of this fact is firstly emphasized by Yang in case of... To describe the physical reality, there are two ways of constructing the dynamical equation of field, differential formalism and integral formalism. The importance of this fact is firstly emphasized by Yang in case of gauge field [Phys. Rev. Lett. 33 (1974) 44fi], where the fact has given rise to a deeper understanding for Aharonov-Bohm phase and magnetic monopole [Phys. Rev. D 12 (1975) 3846]. In this paper we shall point out that such a fact also holds in general wave function of matter, it may give rise to a deeper understanding for Berry phase. Most importantly, we shall prove a point that, for general wave function of matter, in the adiabatic limit, there is an intrinsic difference between its integral formalism and differential formalism. It is neglect of this difference that leads to an inconsistency of quantum adiabatic theorem pointed out by Marzlin and Sanders [Phys. Rev. Lett. 93 (2004) 160408]. It has been widely accepted that there is no physical difference of using differential operator or integral operator to construct the dynamical equation of field. Nevertheless, our study shows that the Schroedinger differential equation (i.e., differential formalism for wave function) shall lead to vanishing Berry phase and that the Schroedinger integral equation (i.e., integral formalism for wave function), in the adiabatic limit, can satisfactorily give the Berry phase. Therefore, we reach a conclusion: There are two ways of describing physical reality, differential formalism and integral formalism; but the integral formalism is a unique way of complete description. 展开更多
关键词 quantum adiabatic theorem integral formalism differential formalism Berry phase gauge field
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Berry几何相与量子跃迁 被引量:3
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作者 张忠灿 方祯云 +1 位作者 胡陈果 孙世军 《高能物理与核物理》 EI CSCD 北大核心 2000年第12期1106-1114,共9页
针对Berry几何相的出现所关联的量子能级,微弱变化跃迁的物理背景条件进行分析研究;对严格产生(获得)Berry几何相与这种微弱变化跃迁之间的内在关系作进一步探讨.结果表明: Berry几何相的严格产生都是由系统在演... 针对Berry几何相的出现所关联的量子能级,微弱变化跃迁的物理背景条件进行分析研究;对严格产生(获得)Berry几何相与这种微弱变化跃迁之间的内在关系作进一步探讨.结果表明: Berry几何相的严格产生都是由系统在演变过程中所出现的量子能级微弱变化跃迁的绝热极限效应所必然导致的结果. 展开更多
关键词 BERRY 几何相 量子跃迁 绝热近似 绝热极限
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