標(biāo)題: Titlebook: Classical Planar Scattering by Coulombic Potentials; Markus Klein,Andreas Knauf Book 1992 Springer-Verlag Berlin Heidelberg 1992 Chaotic S [打印本頁] 作者: otitis-externa 時間: 2025-3-21 18:22
書目名稱Classical Planar Scattering by Coulombic Potentials影響因子(影響力)
書目名稱Classical Planar Scattering by Coulombic Potentials影響因子(影響力)學(xué)科排名
書目名稱Classical Planar Scattering by Coulombic Potentials網(wǎng)絡(luò)公開度
書目名稱Classical Planar Scattering by Coulombic Potentials網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Classical Planar Scattering by Coulombic Potentials被引頻次
書目名稱Classical Planar Scattering by Coulombic Potentials被引頻次學(xué)科排名
書目名稱Classical Planar Scattering by Coulombic Potentials年度引用
書目名稱Classical Planar Scattering by Coulombic Potentials年度引用學(xué)科排名
書目名稱Classical Planar Scattering by Coulombic Potentials讀者反饋
書目名稱Classical Planar Scattering by Coulombic Potentials讀者反饋學(xué)科排名
作者: 龍蝦 時間: 2025-3-21 21:26
Book 1992n-body problem ([38], p. 183). As it turned out, even by confining oneselfto questions ofqualitativenature, the general n-body problem could not be solved. Rather, simplified models were treated, like planar motion or the restricted 3-body problem, where the motion of a test particle did not influence the other two bodies.作者: 水槽 時間: 2025-3-22 03:40
0940-7677 omb‘s potential. But whereas the fundamental laws of motion thus have a simple form, the n-body problem withstood (for n > 2) all attempts of an explicit solution. Indeed, the studies of Poincare at the end of the last century lead to the conclusion that such an explicit solution should be impossibl作者: 四溢 時間: 2025-3-22 07:38
Introduction to Requirements Management,ry 2.8). On the other hand, the bounded orbits . important since they influence the structure of those scattering states which have a long time delay. Lemma 7.4 gives a first example of a global observable (the topological entropy) which is determined entirely by the bounded orbits.作者: Ccu106 時間: 2025-3-22 10:11
The Distribution of the Closed Orbits,ry 2.8). On the other hand, the bounded orbits . important since they influence the structure of those scattering states which have a long time delay. Lemma 7.4 gives a first example of a global observable (the topological entropy) which is determined entirely by the bounded orbits.作者: Condescending 時間: 2025-3-22 13:23
The Scattering Transformation, := ?. (. for . ≠ .). To control the asymptotic behaviour, we assume that . decomposes into the sum of a Coulombic potential and a short range potential. By this we mean the following: . A smooth, real-valued function . on the . . is called . if作者: Condescending 時間: 2025-3-22 19:01 作者: –scent 時間: 2025-3-22 23:33 作者: Irremediable 時間: 2025-3-23 04:53 作者: 郊外 時間: 2025-3-23 09:33
Introduction to Requirements Engineering,In this chapter we are to analyse the positive energy periodic orbits. The basic technique is to minimize the energy functional on the infinite-dimensional manifold of .-curves . : . → M, with . ?[0,1]. As we shall see, this approach gives us full qualitative information for . large.作者: 死貓他燒焦 時間: 2025-3-23 11:00
Introduction to Requirements Engineering,After this existence result for closed orbits, we consider the question of uniqueness. How many closed orbits do exist in a given conjugacy class?作者: condone 時間: 2025-3-23 16:20
Why Requirements Management and Engineering,Our next task is to describe the high-energy bounded and unbounded orbits using symbolic dynamics based on the fundamental group .(.).作者: 提升 時間: 2025-3-23 18:33
Why Requirements Management and Engineering,Our next task will be to determine the topological entropy of the flow . on .. First we study the related question for the flow . on ..作者: Mhc-Molecule 時間: 2025-3-23 23:24 作者: 粗鄙的人 時間: 2025-3-24 03:33
Configuration Management interface,In this chapter we discuss the question of the Liouville measure λ(.) of the set . of positive energy bound states and relate it to time delay.作者: 大暴雨 時間: 2025-3-24 07:16
Stefan Gruner,Manfred Nagl,Andy SchürrThe scattering transformation .=Ω.oΩ. contains complete information on the scattering process. As we have seen in the previous chapters, it exhibits many aspects of irregularity if . ≥ 3. Nevertheless, the scattering transformation is not directly accessible in a (classical) scattering experiment.作者: happiness 時間: 2025-3-24 13:40 作者: 細(xì)節(jié) 時間: 2025-3-24 16:12
Introduction,Astronomy as well as molecular physics describe non-relativistic motion by an interaction of the same form: By Newton’s respectively by Coulomb’s potential.作者: 松馳 時間: 2025-3-24 21:26 作者: faucet 時間: 2025-3-25 02:31 作者: arbiter 時間: 2025-3-25 06:54
Symbolic Dynamics,Our next task is to describe the high-energy bounded and unbounded orbits using symbolic dynamics based on the fundamental group .(.).作者: Juvenile 時間: 2025-3-25 10:14
Topological Entropy,Our next task will be to determine the topological entropy of the flow . on .. First we study the related question for the flow . on ..作者: 預(yù)感 時間: 2025-3-25 14:40
Time Delay,In this chapter we relate the time delay . of the scattering orbits to the structure of the motion near the bounded orbits.作者: 低能兒 時間: 2025-3-25 16:16
Measure of the Bound States,In this chapter we discuss the question of the Liouville measure λ(.) of the set . of positive energy bound states and relate it to time delay.作者: burnish 時間: 2025-3-25 20:31
The Differential Cross Section,The scattering transformation .=Ω.oΩ. contains complete information on the scattering process. As we have seen in the previous chapters, it exhibits many aspects of irregularity if . ≥ 3. Nevertheless, the scattering transformation is not directly accessible in a (classical) scattering experiment.作者: abolish 時間: 2025-3-26 01:59 作者: arousal 時間: 2025-3-26 05:57 作者: 懶惰人民 時間: 2025-3-26 12:24 作者: Amorous 時間: 2025-3-26 16:06 作者: 泰然自若 時間: 2025-3-26 18:08 作者: circuit 時間: 2025-3-26 23:33 作者: Excitotoxin 時間: 2025-3-27 02:42
978-3-662-13900-4Springer-Verlag Berlin Heidelberg 1992作者: cardiovascular 時間: 2025-3-27 06:29 作者: pulmonary 時間: 2025-3-27 11:14 作者: 敏捷 時間: 2025-3-27 17:39
Introduction to Requirements Management, := ?. (. for . ≠ .). To control the asymptotic behaviour, we assume that . decomposes into the sum of a Coulombic potential and a short range potential. By this we mean the following: . A smooth, real-valued function . on the . . is called . if作者: Aphorism 時間: 2025-3-27 20:28 作者: Endemic 時間: 2025-3-27 22:16 作者: 確定無疑 時間: 2025-3-28 05:54 作者: grotto 時間: 2025-3-28 08:33
Regularization,tion scheme employed in this chapter has several disadvantages: It leads to a reparametrization of time; it works only for a fixed value of the energy; and the configuration plane . is replaced by a surface . covering . with branch points.作者: mitten 時間: 2025-3-28 14:14 作者: Living-Will 時間: 2025-3-28 16:37
Fractional Dimension,n its own right, governs the measure of those scattering orbits which have a large time delay. In our semiclassical analysis of the quantum mechanical problem, the fractional dimension of the bounded orbits will determine a bound for the number of resonance poles near the real energy axis.作者: morale 時間: 2025-3-28 19:01
0940-7677 not be solved. Rather, simplified models were treated, like planar motion or the restricted 3-body problem, where the motion of a test particle did not influence the other two bodies.978-3-662-13900-4978-3-540-47336-7Series ISSN 0940-7677 作者: remission 時間: 2025-3-29 01:11
Classical Planar Scattering by Coulombic Potentials作者: 責(zé)怪 時間: 2025-3-29 06:41
9樓作者: 胖人手藝好 時間: 2025-3-29 07:41
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