Summary
Some of the statistical properties corresponding to Gaussian ensembles of random matrices whose matrix elements are not all functionally independent are investigated. Three types of ensembles are studied. First, an ensemble whose matrix elements are all real is examined. Next, an ensemble whose matrix elements are not all real, but whose off-diagonal elements have real and imaginary parts which are of the same size on the average is studied. Finally, ensembles with of order-N and-N 2 nonzero imaginary parts of arbitrary size are investigated. Each of the above ensembles is compared with the corresponding Gaussian ensemble in which all of the nonzero matrix elements are functionally independent.
Riassunto
Si esaminano alcune proprietà statistiche corrispondenti a insiemi gaussiani di matrici casuali i cui elementi di matrice non sono tutti funzionalmente indipendenti. Si studiano tre tipi di insieme: prima un insieme i cui elementi di matrice sono tutti reali, poi un insieme i cui elementi di matrice non sono tutti reali, ma i cui elementi al di fuori della diagonale hanno parti reali e immaginarie che sono in media della stessa grandezza, infine insiemi con parti immaginarie diverse da zero di ordineN oN 2 di grandezza arbitraria. Ciascuno dei suddetti insiemi è confrontato con il corrispondente insieme gaussiano nel quale tutti gli elementi di matrice diversi da zero sono funzionalmente indipendenti.
Резюме
Исследуются некоторые статистические свойства, соответствующие гауссовым ансамблям случайных матриц, не все матричные элементы которых являются функционально независимыми. Рассматриваются три типа ансамблей. Сначала исследуется ансамбль, все мчтричные элементы которого являются вещественными. Затем рассматривается ансамбль, у которого не все матричные элементы являются вещественными, но недиагоналяные матричные элементы имеют вещественные н мнимые чссти, которые в среднем являются одинаковыми. В заключение исследуются ансамбли с ненулевыми мнимыми частями порядкаN иN 2. Каждый ие сассмотренных ахсамблей шравнивается с соответствующим гауссовым ансамблем, в котором все ненулевые матричные элемменты являются функционально независимыми.
Similar content being viewed by others
References
M. L. Mehta:The International Conference on Statistical Properties of Nuclei, Albany, N. Y., August 1971, seeStatistical Properties of Nuclei, edited byJ. B. Garg (New York, N. Y., 1972).
See, for example,C. E. Porter:Statistical Theories of Spectra: Fluctuations (New York, N. Y., 1965);M. L. Mehta:Random Matrices and the Statistical Theory of Energy Levels (New York, N. Y., 1967).
N. Rosenzeweig, J. E. Monahan andM. L. Mehta:Nucl. Phys. A,109, 437 (1968).
M. L. Mehta:Nuovo Cimento B,65, 107 (1970).
L. D. Favro andJ. F. McDonald:Phys. Rev. Lett.,19, 1254 (1967).
J. F. McDonald:J. Math. Phys. (N. Y.),10, 1191 (1969).
J. F. McDonald:J. Math. Phys. (N. Y.),15, 596 (1974).
J. F. McDonald:J. Math. Phys. (N. Y.),17, 1042 (1976).
See, for example, the introductory review of C. E. Porter’s book listed in ref. (2).C. E. Porter:Statistical Theories of Spectra: Fluctuations (New York, N. Y., 1965).
It might also be noted that this theory is generally felt to be valid only in that region of the energy spectrum where the energy levels of the system are equally spaced. See. ref. (2)C. E. Porter:Statistical Theories of Spectra: Fluctuations (New York, N. Y., 1965).
A parametrization for arbitrary orthogonal and unitary matrices is given inJ. F. McDonald:J. Math. Phys. (N. Y.),13, 1399 (1972).
N. Ullah:Nucl. Phys. 58, 65 (1964).
It is perhaps worth noting that this spacing distribution corresponds to the entire ensemble (i.e. each matrix in the ensemble has equally spaced eigenvalues). According to the basic postulates of the theory, it is this distribution which should correspond to the spacing distribution of energy levels for a particular physical system. See ref. (2).C. E. Porter:Statistical Theories of Spectra: Fluctuations (New York, N. Y., 1965).
E. P. Wigner:Gatlinburg Conference on Neutron Physics by Time-of-Flight, Oak Ridge National Laboratory Report ORNL-2309 (1957, unpublished), p. 59; see alsoProceedings of the International Conference on Neutron Interactions with the Nucleus, Columbia University Report CU-175 (TID-7547) (1957, unpublished), p. 49.
M. L. Mehta:Nucl. Phys.,18, 395 (1960).
M. Gaudin:Nucl. Phys.,25, 447 (1961).
C. E. Porter andR. G. Thomas:Phys. Rev.,104, 483 (1956).
P. B. Kahn:Nucl. Phys.,41, 159 (1963).
N. Ullah:J. Math. Phys. (N. Y.),4, 1279 (1963).
See, for example,Applied Mathematics Series, No. 55,Handbook of Mathematical Functions (Washington, D. C., 1964), p. 589.
Author information
Authors and Affiliations
Additional information
To speed up publication, the author of this paper has agreed to not receive the proofs for correction.
This work was supported in part by the National Research Council of Canada.
Traduzione a cura della Redazione.
Переведено редакцией.
Rights and permissions
About this article
Cite this article
McDonald, J.F. Some mathematically simple ensembles of random matrices which represent Hamiltonians with a small time-reversal-noninvariant part. Nuov Cim B 57, 95–124 (1980). https://doi.org/10.1007/BF02722404
Received:
Revised:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02722404