Special Matrices Of Mathematical Physics: Stochastic, Circulant And Bell MatricesWorld Scientific, 2001 M08 17 - 340 páginas This book expounds three special kinds of matrices that are of physical interest, centering on physical examples. Stochastic matrices describe dynamical systems of many different types, involving (or not) phenomena like transience, dissipation, ergodicity, nonequilibrium, and hypersensitivity to initial conditions. The main characteristic is growth by agglomeration, as in glass formation. Circulants are the building blocks of elementary Fourier analysis and provide a natural gateway to quantum mechanics and noncommutative geometry. Bell polynomials offer closed expressions for many formulas concerning Lie algebra invariants, differential geometry and real gases, and their matrices are instrumental in the study of chaotic mappings. |
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Página viii
... example chosen has been glass transition , a fascinating phenomenon for which there is no complete theory and for whose description they have made important contributions . More is said on glasses than on other sub- jects , because not ...
... example chosen has been glass transition , a fascinating phenomenon for which there is no complete theory and for whose description they have made important contributions . More is said on glasses than on other sub- jects , because not ...
Página xi
... - negative matrices 3.2 General properties 3.2.1 Flow diagrams · Chapter 4 Glass transition Chapter 5 The Kerner model vii 3 3 6 8 10 14 17 35 31 & a ☹N ~~~ 21 25 25 27 30 5.1 A simple example : Se - As glass 5.1.1 xi Contents.
... - negative matrices 3.2 General properties 3.2.1 Flow diagrams · Chapter 4 Glass transition Chapter 5 The Kerner model vii 3 3 6 8 10 14 17 35 31 & a ☹N ~~~ 21 25 25 27 30 5.1 A simple example : Se - As glass 5.1.1 xi Contents.
Página xii
Ruben Aldrovandi. 5.1 A simple example : Se - As glass 5.1.1 5.1.2 A simplified version The Selenium - Germanium glass Chapter 6 Formal developments 6.1 Spectral aspects 6.2 Reducibility and regularity 6.3 Projectors and asymptotics 6.4 ...
Ruben Aldrovandi. 5.1 A simple example : Se - As glass 5.1.1 5.1.2 A simplified version The Selenium - Germanium glass Chapter 6 Formal developments 6.1 Spectral aspects 6.2 Reducibility and regularity 6.3 Projectors and asymptotics 6.4 ...
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... example p = ( P1 , P2 , ... , PN ) T . ( 11 ) M is normal when it commutes with M : [ M , M ' ] = 0. In that case , - ( i ) M and Mt share all the eigenvectors ; ( ii ) the eigenvectors constitute a complete orthonormal ( v · Vk ' Skk ...
... example p = ( P1 , P2 , ... , PN ) T . ( 11 ) M is normal when it commutes with M : [ M , M ' ] = 0. In that case , - ( i ) M and Mt share all the eigenvectors ; ( ii ) the eigenvectors constitute a complete orthonormal ( v · Vk ' Skk ...
Página 6
... example . Consider the characteristic equation of a 3 x 3 matrix M : AM ( A ) = ( 1 − λ1 ) ( A — A2 ) ( A — A3 ) = 0 . - The Cayley - Hamilton theorem takes , in the present case , the form AM ( M ) = ( M- \ 1I ) ( M — \ 1⁄2I ) ( M ...
... example . Consider the characteristic equation of a 3 x 3 matrix M : AM ( A ) = ( 1 − λ1 ) ( A — A2 ) ( A — A3 ) = 0 . - The Cayley - Hamilton theorem takes , in the present case , the form AM ( M ) = ( M- \ 1I ) ( M — \ 1⁄2I ) ( M ...
Contenido
19 | |
CIRCULANT MATRICES | 79 |
BELL MATRICES | 147 |
Appendix A Formulary | 283 |
Bibliography | 309 |
Index | 315 |
Otras ediciones - Ver todas
Special Matrices of Mathematical Physics: Stochastic, Circulant, and Bell ... Ruben Aldrovandi Vista previa limitada - 2001 |
Special Matrices of Mathematical Physics: Stochastic, Circulant, and Bell ... Ruben Aldrovandi Vista previa limitada - 2001 |
Términos y frases comunes
alphabet basis Bell matrices Bell polynomials braid group canonical partition function characteristic polynomial circulant matrices circulant matrix classical cluster integrals column commutative components condition consequently continuum convolution corresponding cyclic defined derivative detailed balancing diagonal differential discrete distribution dynamical eigenvalues eigenvectors entries ep+1 equation equilibrium evolution example factor fermions finite formalism formula Fourier transformations Fredholm geometry given glass grand canonical partition Hamiltonian Hopf algebras identity imprimitive invariant inverse irreducible iterate leads Lie algebra Markov chain noncommutative notation obtained operator particles permutation phase space Phys physical Poisson bracket powers projectors properties QN(B Quantum Mechanics recursion representation Statistical Mechanics stochastic matrix summation symmetric functions symmetric group symplectic Taylor coefficients theorem theory totally regular unitary values variables vector virial Weyl-Wigner Wigner functions Σ Σ