Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 77
In the first case, the resulting ensemble would be correctly represented by the
statistical operator w'A= 2tt(wpjpJltt(wpj . i-1 ' i-1 In the second case, the resulting
ensemble would be correctly represented by the statistical operator W'D ...
In the first case, the resulting ensemble would be correctly represented by the
statistical operator w'A= 2tt(wpjpJltt(wpj . i-1 ' i-1 In the second case, the resulting
ensemble would be correctly represented by the statistical operator W'D ...
Page 100
cannot be represented as conditional probabilities on a classical probability
space. Yet, in some sense, a probability like pa (6;) = a*)|* is to be understood as
the conditional probability of 6, given a,. How do we make sense of this
probability ...
cannot be represented as conditional probabilities on a classical probability
space. Yet, in some sense, a probability like pa (6;) = a*)|* is to be understood as
the conditional probability of 6, given a,. How do we make sense of this
probability ...
Page 111
Like Jauch, they emphasize that the desired mixture represents the statistics of
the system only as far as the macroscopic quantities of M are concerned — i.e.
measurements of magnitudes incompatible with macroscopic magnitudes are not
...
Like Jauch, they emphasize that the desired mixture represents the statistics of
the system only as far as the macroscopic quantities of M are concerned — i.e.
measurements of magnitudes incompatible with macroscopic magnitudes are not
...
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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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3-geometry algebra applied assertion atoms axioms Boolean Borel field Borel sets calculus concept conditional probability conditionalization consider corresponding countable course defined definition denote derived deterministic dialog dialog-game disjoint dynamics edited Einstein elements equation equivalent exists experiment finite formal function geometry given Gleason's theorem Hence Hilbert space implies induction initial interaction interpretation irreversible Journ linear magnitude Math mathematical means Neumann non-Boolean notion observable orthogonal orthomodular lattice particle photon Phys physical quantity physical system physical theories physicists positive precision probabilistic probability measure probability space probability theory problem procedure quantum logic quantum mechanics quantum theory quantum-logical question radioactive random variable real numbers relation relative frequency relf represented respect result rule sequence space-time special relativity spin statistical operator subset subspace superspace theorem tion transformation truth universal constants vector velocity von Neumann algebra zero