Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 127
... integral + ∞ S1⁄2μ ( x ( 12 ) ) is called ( when it exists ) the expectation of ƒ ( in the state μ ) . Paraphrasing the classical definition , we can define a ( real ) random variable . on the generalized probability space ( L , z ) as ...
... integral + ∞ S1⁄2μ ( x ( 12 ) ) is called ( when it exists ) the expectation of ƒ ( in the state μ ) . Paraphrasing the classical definition , we can define a ( real ) random variable . on the generalized probability space ( L , z ) as ...
Page 350
... integral over A exists when the integral over K does . As defined , the integral is a linear function on the r.v. and also additive for integration over disjoint sets , and order preserving . We note specifically for future reference ...
... integral over A exists when the integral over K does . As defined , the integral is a linear function on the r.v. and also additive for integration over disjoint sets , and order preserving . We note specifically for future reference ...
Page 443
... integral below , ( 46 ) dy = [ ( § ¥ / dA2 ) dAxd3x = − [ 2 [ ( ĉ / ĉx * ) ( § ¥ / 844 ) ] d3x , Sy k the expression in square brackets must vanish everywhere . This is the condition that the divergence of the electric field should ...
... integral below , ( 46 ) dy = [ ( § ¥ / dA2 ) dAxd3x = − [ 2 [ ( ĉ / ĉx * ) ( § ¥ / 844 ) ] d3x , Sy k the expression in square brackets must vanish everywhere . This is the condition that the divergence of the electric field should ...
Contents
The discovery of the law of radioactive decay | 6 |
Early models of the nucleus | 15 |
Final remarks | 21 |
Copyright | |
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