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ensemble having the energy E k is (9.29). The ensemble with such an energy distribution is the canonical ensemble.

Introduction to JSP Anatomy of a JSP Tag Libraries JSP and the UML JSP in Enterprise Applications Summary

let .Yt' be the Hamiltonian operator of a system of N identical spinless particles. * Let .Yt' be the sum of two operators, the kinetic energy operator K, and the potential energy operator Q: .Yt'=K+Q (9.32)

"It is straightforward to generalize the following considerations to the case of particles with spin and to the case of a mixed system of two or more more different kinds of particles.

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O'l'(rl, ,rN) = O(rl, ,rN)'l'(rl, ,r N)

Process Check: In this chapter, we focus on design as we progress through the Rational Unified Process (RUP) analysis and design discipline We also discuss aspects of implementation in the context of the JSP technology

(9.33) (9.34)

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where m is the mass of a particle, V' is the Laplacian operator with respect to r i , and 0 (rl , ... , r N) is a sum of two-body potentials: O(rl, ,rN) where

[Vii i<)

Until a few years ago, the term thin client was unheard of That changed with the advent of the Web browser and the subsequent rush to create sophisticated Web-based applications in virtually every industry

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(9.35)

(9.36)

Whenever convenient, we use the abbreviation (1, ... , N) for (rl , ... , r N ). The partition function of the system is

Thin clients, as we all know, utilize a markup language for presentation Sophisticated server-side applications written in languages such as Java are thus used to generate the markup language for presentation to the client

QN(V, T)

Tre-,8 '= [(cI>n,e-,8 'cI>n)

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(9.37)

This intermingling of the programming side of the application with the presentation side has some drawbacks:

where cI>n(l, ... , N) is a member of any complete orthonormal set of wave functions of the system and cI>n*(l, ... , N) is its complex conjugate. For any operator (9,

(9.38)

Each cI>n satisfies the boundary conditions imposed on the system and is normalized in the box of volume V containing the system. It is a symmetric (antisymmetric) function of r l , ... , r N , if the system is a system of bosons (fermions). It will be shown that when the temperature is sufficiently high we can make the approximation

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