## Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |

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Page 220

or in detail (4.28) x' = rc(x— a), t which are the Lorentz-type

equations, where (4.29) r. = (1 - pt/m-j)-* . We shall now show that causality

implies that w* is positive. To this end assume that w2 = — ut, where « is a

positive (real) ...

or in detail (4.28) x' = rc(x— a), t which are the Lorentz-type

**transformation**equations, where (4.29) r. = (1 - pt/m-j)-* . We shall now show that causality

implies that w* is positive. To this end assume that w2 = — ut, where « is a

positive (real) ...

Page 226

Furthermore, elaborating on results obtained by LiOUviLLE and Darboux, Lie

and Felix Klein [47] demonstrated already in 1871 that in a space of n

dimensions conformal

d*l into a ...

Furthermore, elaborating on results obtained by LiOUviLLE and Darboux, Lie

and Felix Klein [47] demonstrated already in 1871 that in a space of n

dimensions conformal

**transformations**which map the expression &x\ + dx] + ... +d*l into a ...

Page 227

nificant

as a physically significant

the specific numerical value of the « limiting velocity » «,), some concrete ...

nificant

**transformations**, that is to interpret the formal Lorentz-type**transformation**as a physically significant

**transformation**(which can be done only by determiningthe specific numerical value of the « limiting velocity » «,), some concrete ...

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### Contents

E Amaldi Radioactivity a pragmatic pillar of probabilistic | 1 |

Statistical fluctuations | 10 |

Final remarks | 21 |

Copyright | |

24 other sections not shown

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