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Level statistics

At its foundation level, statistical mechanics mvolves some profound and difficult questions which are not fiilly understood, even for systems in equilibrium. At the level of its applications, however, the rules of calculation tliat have been developed over more than a century have been very successfLil. [Pg.378]

The instrument has been evaluated by Luster, Whitman, and Fauth (Ref 20). They selected atomized Al, AP and NGu as materials for study that would be representative of proplnt ingredients. They found that only 2000 particles could be counted in 2 hours, a time arbitrarily chosen as feasible for control work. This number is not considered sufficient, as 18,000 particles are required for a 95% confidence level. Statistical analysis of results obtained for AP was impossible because of discrepancies In the data resulting from crystal growth and particle agglomeration. The sample of NGu could not be handled by the instrument because it consisted of a mixt of needles and chunky particles. They concluded that for dimensionally stable materials such as Al or carborundum, excellent agreement was found with other methods such as the Micromerograph or visual microscopic count. But because of the properties peculiar to AP and NGu, the Flying Spot Particle Resolver was not believed suitable for process control of these materials... [Pg.531]

Another development in the quantum chaos where finite-temperature effects are important is the Quantum field theory. As it is shown by recent studies on the Quantum Chromodynamics (QCD) Dirac operator level statistics (Bittner et.al., 1999), nearest level spacing distribution of this operator is governed by random matrix theory both in confinement and deconfinement phases. In the presence of in-medium effects... [Pg.172]

We note that the integral over the energetically allowed phase space— that is, the classical level density (97)—was found in Fig. 20 to be in excellent agreement with the quantum-mechanical level density. This finding indicates that there is a valid correspondence between the quantum-mechanical two-state system and its classical mapping representation. A similar conclusion was drawn in a recent smdy of a mapped two-state problem, which focused on the Lyapunov exponents and the energy level statistics of the system [124, 235]. [Pg.328]

Structural and molecular biologists often study the temperature dependence of the equilibrium position of a reaction or process. The Gibbs free energy undoubtedly provides the correct thermodynamic criterion of equilibrium. An understanding of this parameter can be achieved from either a macroscopic level (classical thermodynamics) or a molecular level (statistical thermodynamics). Ultimately, one seeks to understand the factors influencing AG° for a specific reaction. [Pg.365]

The traditional approach to quality control is to generate charts of various kinds to monitor the performance of a production unit. At a superficial level, statistical process control (SPC) and statistical quality control (SQC) [9] are terms used interchangeably to describe traditional... [Pg.273]

The preceding considerations are essentially based on the model of random-matrix ensembles proposed by Dyson and others in the 1960s. Recent works, in particular by Casati and co-workers [89], have focused on band random matrices. Such matrices naturally arise in quantum systems with subspaces coupled only to next-neighboring subspaces such as for electronic states in a chain of atoms or in the kicked rotator. In such systems, localized states are observed that present a level statistics interme-... [Pg.518]

The fundamental question in transport theory is Can one describe processes in nonequilibrium systems with the help of (local) thermodynamic functions of state (thermodynamic variables) This question can only be checked experimentally. On an atomic level, statistical mechanics is the appropriate theory. Since the entropy, 5, is the characteristic function for the formulation of equilibria (in a closed system), the deviation, SS, from the equilibrium value, S0, is the function which we need to use for the description of non-equilibria. Since we are interested in processes (i.e., changes in a system over time), the entropy production rate a = SS is the relevant function in irreversible thermodynamics. Irreversible processes involve linear reactions (rates 55) as well as nonlinear ones. We will be mainly concerned with processes that occur near equilibrium and so we can linearize the kinetic equations. The early development of this theory was mainly due to the Norwegian Lars Onsager. Let us regard the entropy S(a,/3,. ..) as a function of the (extensive) state variables a,/ ,. .. .which are either constant (fi,.. .) or can be controlled and measured (a). In terms of the entropy production rate, we have (9a/0f=a)... [Pg.63]

The only study of the interannual variability of the T,S characteristics of the Black Sea waters at depths from 500 to 2000 m published to date [32] suggests the vertical and horizontal homogeneity of the deep temperature variations with standard deviations of 0.01-0.03 °C. The standard deviations of the interannual salinity variations decrease with depth from 0.2-0.3 psu at a depth of 500 m to 0.02-0.03 psu at depths of 1500-2000 m. At all the levels, statistically significant quadratic trends dominate with temperature and salinity maximums confined approximately to 1980. The mean rates of the salinity increase (decrease) before (after) 1980 comprised 0.0025 psu year-1. Against the background of the quadratic trends, 6.5-year and 20-year periodicities were recognized. [Pg.248]

Since the phenomenon of spectra is so ubiquitous in physics it is important to have a tool to characterize energy or frequency spectra. Such a tool is provided by the theory of (energy) level statistics. Following closely the standard literature (Haake (1991), Mehta (1991)) we will now introduce some elements of this field. [Pg.87]

The subscript C/ in (4.1.45) stands for unitary since the system Hamiltonian is invariant under general unitary transformations in case all antiunitary symmetries are broken. The effects of time reversal symmetry breaking on the level statistics were recently investigated experimentally by So et al. (1995) and Stoffregen et al. (1995) by measuring the resonance spectrum of quasi-two-dimensional microwave cavities in the presence of time reversal breaking elements such as ferrites and directional couplers. These experiments are of considerable relevance for quantum mechanics since quasi-two-dimensional microwave cavities are generally considered to be excellent models for two-dimensional quantum billiards. [Pg.97]

This book introduces you to the statistical methodology employed in drug development at both a conceptual and a computational level. Statistical methodology provides numerical representations of information that facilitate rational, information-based decision-making during regulatory considerations and clinical practice. [Pg.8]

Most theoretical procedures for deriving expressions for AG iix start with the construction of a model of the mixture. The model is then analyzed by the techniques of statistical thermodynamics. The nature and sophistication of different models vary depending on the level of the statistical mechanical approach and the seriousness of the mathematical approximations that are invariably introduced into the calculation. The immensely popular Flory-Huggins theory, which was developed in the early 1940s, is based on the pseudolattice model and a rather low-level statistical treatment with many approximations. The theory is remarkably simple, explains correctly (at least qualitatively) a large number of experimental observations, and serves as a starting point for many more sophisticated theories. [Pg.145]

Defect types Defect action levels Statistical reference... [Pg.79]

A related but somewhat more fundamental question concerns the underlying thermodynamic basis of the transition. Specifically, we need to know whether it is sufficient to understand the behavior of simplest atomic models to explain the thermodynamic aspects of the phenomenon (as is the case, e.g., for the equilibrium melting and freezing transitions. If so, it would be possible for computer simulation experiments of sufficient accuracy to provide the basis for a molecular level statistical mechanical account of all aspects of the glass transition. [Pg.400]

Odd-even electron numbers and energy level statistics in cluster assemblies... [Pg.1445]

Energy-level statistics in assemblies of small metal particles summary of theoretical background... [Pg.1449]


See other pages where Level statistics is mentioned: [Pg.381]    [Pg.244]    [Pg.80]    [Pg.2]    [Pg.93]    [Pg.344]    [Pg.381]    [Pg.440]    [Pg.772]    [Pg.446]    [Pg.98]    [Pg.104]    [Pg.440]    [Pg.229]    [Pg.91]    [Pg.98]    [Pg.25]    [Pg.222]    [Pg.456]    [Pg.203]    [Pg.388]    [Pg.317]    [Pg.522]    [Pg.525]    [Pg.526]    [Pg.1447]    [Pg.1450]   
See also in sourсe #XX -- [ Pg.87 , Pg.91 , Pg.95 , Pg.97 , Pg.98 ]




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