A physical application of the function exp(−1/x2)

1975 ◽  
Vol 43 (3) ◽  
pp. 268-269
Author(s):  
Mary L. Boas
Keyword(s):  
Physical Application

CHAPTER 3 A PHYSICAL APPLICATION

1982 ◽  
Vol 60 (sup1) ◽  
pp. 44-63
Author(s):  
Leonard Goddard ◽  
Brenda Judge
Keyword(s):  
Physical Application

ON THE PHYSICAL APPLICATION OF SIMULATED ANNEALING ALGORITHM

1999 ◽  
Vol 10 (06) ◽  
pp. 1065-1070 ◽  
Author(s):  
SHU-YOU LI ◽  
ZHI-HUI DU ◽  
MENG-YUE WU ◽  
JING ZHU ◽  
SAN-LI LI
Keyword(s):  
Simulated Annealing ◽  
Parameter Optimization ◽  
High Performance ◽  
Simulated Annealing Algorithm ◽  
Optimization Problems ◽  
Source Code ◽  
Physical Application ◽  
General Program ◽  
Annealing Algorithm

A high-performance general program is presented to deal with the multi-parameter optimization problems in physics. Considering the requirements of physical application, some small but significant modifications were made on the conventional simulated annealing algorithm. A parallel realization was suggested to further improve the performance of the program. Mathematical and physical examples were taken to test the feasibility and the efficiency of the program. The source code is available from the authors free of charge.

Wave Mechanics

2019 ◽  
pp. 91-174
Author(s):  
P.J.E. Peebles
Keyword(s):  
Magnetic Field ◽  
Wave Function ◽  
Angular Momentum ◽  
Hydrogen Atom ◽  
Physical System ◽  
Adjoint Operator ◽  
Physical Application ◽  
Wave Mechanics ◽  
Definite Form ◽  
Quantum Wave

This chapter develops the wave mechanics formalism. The emphasis here is on symmetries and conservation laws: parity, linear and angular momentum, and the electromagnetic interaction. The only specific physical application is the completion of the study of an isolated hydrogen atom, with some discussion of the motion of a particle in a magnetic field. The chapter also outlines the general assumptions of quantum wave mechanics, which may be summarized as follows: the state of a physical system is represented by a wave function and each measurable attribute of the system is represented by a linear self-adjoint operator in the space of functions. To apply these general assumptions to a given physical system, one must give a specific prescription for the observables and their algebra, and one must adopt a definite form for the Hamiltonians as a function of the observables.

Joint physical-application layer security for wireless multimedia delivery

2014 ◽  
Vol 52 (3) ◽  
pp. 66-72 ◽  
Author(s):  
Liang Zhou ◽  
Dan Wu ◽  
Baoyu Zheng ◽  
Mohsen Guizani
Keyword(s):  
Physical Application ◽  
Wireless Multimedia ◽  
Application Layer ◽  
Multimedia Delivery
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