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 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) ...
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 transformations which map the expression &x\ + dx] + ... +
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 transformations, that is to interpret the formal Lorentz-type transformation
as a physically significant transformation (which can be done only by determining
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 determining
the 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 | |
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