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  • About
  • The Global ETD Search service is a free service for researchers to find electronic theses and dissertations. This service is provided by the Networked Digital Library of Theses and Dissertations.
    Our metadata is collected from universities around the world. If you manage a university/consortium/country archive and want to be added, details can be found on the NDLTD website.
31

Duality and multiparticle production.

Gordon, Earl Mark. January 1972 (has links)
No description available.
32

Recreation of the Bullet Cluster (1E 0657-56) merging event via N-body computer simulation

Balint, Zsolt T. 21 July 2012 (has links)
In this study I present two N-body computer simulations of the Bullet Cluster (1E 0657-56) merging system. The models are fully self-consistent, meaning that all gravitational forces are determined by the distribution of the particles. Initial positions and velocities of the two clusters are determined by solving a two-body problem. Post-collision time period shows an increase in the line-of-sight velocity dispersion in both clusters, and is consistent with previous Bullet Cluster studies. I also investigate the temporal evolution of the average cluster radial velocities of the galaxies located in the inner, middle, and outer regions of the clusters. I show that the orbital trajectories differ in pre- and post-collision periods. Inner region galaxies receive an impulse that moves them outward from the cluster center immediately after collision, while at the same time the outer region galaxies are pulled back towards the cluster center. / Department of Physics and Astronomy
33

The n-body problem with repulsive-attractive quasihomogeneous potential functions.

Jones, Robert T. 12 November 2008 (has links)
This thesis involves the study of a repulsive-attractive N-body problem, which is a subclass of a quasihomogeneous N-body problem [5]. The quasihomogeneous N-body problem is the study of N point masses moving in R3N, where the negative of the potential energy is of the form, X 1≤i<j≤N bmimjr−β ij + X 1≤i<j≤N amimjr−α ij . In the above equation, rij is the distance between the point mass mi and the point mass mj , and a, b, α > β > 0 are constants. The repulsive-attractive N-body problem is the case where a < 0 and b > 0. We start the ground work for the study of the repulsive-attractive N-body problem by defining the first integrals, collisions and pseudo-collisions and the collision set. By examining the potentials where a < 0 and b > 0, we see that the dominant force is repulsive. This means that the closer two point masses get the greater the force acting to separate them becomes. This property leads to the main result of the first chapter: there can be no collisions or pseudo-collisions for any repulsive-attractive system. In the next chapter we study central configurations of the system. Quasihomogeneous potentials will have different central configurations than homogeneous potentials [6], thus requiring the classification of two new subsets of central configurations. Loosely speaking, the set of central configurations that are not central configurations for any homogeneous potential are called extraneous. The set of configurations that are central configurations for both homogeneous potentials that make up the quasihomogeneous potential, are called simultaneous configurations. We also notice that every simultaneous central configuration will be non-extraneous, therefore the two subsets are disjoint. Next we show the existence of oscillating homothetic periodic orbits associated with non-extraneous configurations. Finally in this chapter, we investigate the polygon solutions for repulsive-attractive N-body problems [11]. In particular we show that the masses need no longer to be equal, for repulsive-attractive potentials. It will be shown that there exists a square configuration with m1 = m2 6= m3 = m4, that leads to a relative equilibrium. Therefore, for N = 4 the set of extraneous configurations is non-empty. The last chapter deals with the complete analysis of the generalized Lennard- Jones 2-body problem. The generalized Lennard-Jones problem is the subcase of the repulsive-attractive N-body problem, where a = −1, b = 2, and α = 2β. We proceed as in [13] by using diffeomorphic transforms to get an associated system thereby generating a picture of the global flow of the system. This gives us the complete flow for the generalized Lennard-Jones 2-body problem.
34

Collectivity in A ~ 60 nuclei : superdeformed and smoothly terminating rotational bands /

Svensson, Carl Edward. January 1998 (has links)
Thesis (Ph.D.) -- McMaster University, 1998. / Includes bibliographical references (leaves 241-264). Also available via World Wide Web.
35

Quantum theory of many Bose atom systems /

Khan, Imran. January 2007 (has links)
Dissertation (Ph.D.)--University of Toledo, 2007. / Typescript. "Submitted as partial fulfillment of the requirements for The Doctor of Philosophy Degree in Physics." Bibliography: leaves 87-90.
36

On the N-body problem /

Xie, Zhifu, January 2006 (has links) (PDF)
Thesis (Ph. D.)--Brigham Young Dept. of Mathematics, 2006. / Includes bibliographical references (p. 87-90).
37

Two problems in many-body physics

Wang, Cheng-Ching, January 1900 (has links)
Thesis (Ph. D.)--University of Texas at Austin, 2008. / Vita. Includes bibliographical references.
38

Some problems in the theory of many-body systems

Leggett, Anthony J. January 1964 (has links)
No description available.
39

Some problems in the theory of many-body systems

Moore, M. A. January 1967 (has links)
No description available.
40

Some problems in the theory of many body systems

Coblans, Y. January 1965 (has links)
No description available.

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