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Exponential representation of complex Lorentz matrices

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Il Nuovo Cimento (1955-1965)

Summary

It is shown that every proper, complex Lorentz matrixL can be expressed in the formL=Σ exp [AG], whereA is an antisymmetric matrix,G is the metric matrix, and Σ=±l. It is then shown that not every proper, complex Lorentz matrixL can be expressed in the formL=exp [AG], withA andG as above.

Riassunto

Si dimostra che ogni matrice di Lorentz propria e oomplessa,L, puÒ essere espressa nella formaL = Σ exp [AG], doveA è una matrice antisimmetrica,G è la matrice metrica, e Σ=±1. Si dimostra poi che non tutte le matrici di Lorentz proprie e complesse,L, si possono esprimere nella formaL = exp [AG], conA eG come sopra.

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References

  1. F. D. Mubnaghan:The Theory of Group Representations (Baltimore, 1938), p. 356.

  2. V. I. Smirnov:Linear Algebra and Group Theory (New York, 1961), p. 417, problems 13, 14.

  3. F. R. Gantmacher:Applications of the Theory of Matrices (New York, 1959), p. 14, 15, Theorem 7.

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Additional information

The contribution of H. E. M. was made prior to his employment with Lincoln Laboratories.

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Lomont, J.S., Moses, H.E. Exponential representation of complex Lorentz matrices. Nuovo Cim 29, 1059–1067 (1963). https://doi.org/10.1007/BF02750132

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  • DOI: https://doi.org/10.1007/BF02750132

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