Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 34
Finally, call states of the system the equivalence classes of 77; let £f be the set of
all states, and denote by ot, $i Y, ... single states. Not only E partitions 77 in
equivalence classes, but also 77 partitions E in equivalent classes : we say e, , et
e E ...
Finally, call states of the system the equivalence classes of 77; let £f be the set of
all states, and denote by ot, $i Y, ... single states. Not only E partitions 77 in
equivalence classes, but also 77 partitions E in equivalent classes : we say e, , et
e E ...
Page 165
In general, we will denote our physical variables (either deterministic or
probabilistic) by q,. By an elementary physical term we will understand any term
which has one of the following forms: tk, d, (tk), p, (tk). We will call the f„'s time-
variables ...
In general, we will denote our physical variables (either deterministic or
probabilistic) by q,. By an elementary physical term we will understand any term
which has one of the following forms: tk, d, (tk), p, (tk). We will call the f„'s time-
variables ...
Page 206
0=3x10 m Let T0 denote the period of the satellite M (Io) of Jupiter J whose
position in the solar system is, for simplicity, assumed to be stationary; and let tk
denote the time interval between k consecutive emersions of M from the shadow
...
0=3x10 m Let T0 denote the period of the satellite M (Io) of Jupiter J whose
position in the solar system is, for simplicity, assumed to be stationary; and let tk
denote the time interval between k consecutive emersions of M from the shadow
...
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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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