Interactions of High Energy Particles with Nuclei |
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Page 2
Hence we shall start with the very successful model of such processes : the Glauber model . 2. Description of Multiple Scattering 2.1 . General Remarks To construct the relevant formulae for the theory of multiple scattering one can ...
Hence we shall start with the very successful model of such processes : the Glauber model . 2. Description of Multiple Scattering 2.1 . General Remarks To construct the relevant formulae for the theory of multiple scattering one can ...
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2m 3 Ay + ky = Vy , ha v = eikap ( x , y , z ) , 32 a2 26 Ay = eika + მი P ( x , y , z ) — kļeikzp + 2ikeikz az ar ? ду ? teika aze ' hence , neglecting second derivatives of y , we obtain the following equation for : до 2ikeikz az 2m ...
2m 3 Ay + ky = Vy , ha v = eikap ( x , y , z ) , 32 a2 26 Ay = eika + მი P ( x , y , z ) — kļeikzp + 2ikeikz az ar ? ду ? teika aze ' hence , neglecting second derivatives of y , we obtain the following equation for : до 2ikeikz az 2m ...
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( 2.3 ) Hence , in the limit Ewe have to have ( 1 - a3 ) 6-0 , ( 1 + 03 ) 4-2 . This is because the right - hand side of ( 2.3 ) does not contain the energy , E. We multiply eq ( 2.3 ) from the left by ...
( 2.3 ) Hence , in the limit Ewe have to have ( 1 - a3 ) 6-0 , ( 1 + 03 ) 4-2 . This is because the right - hand side of ( 2.3 ) does not contain the energy , E. We multiply eq ( 2.3 ) from the left by ...
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... this case we also have additivity of phase shifts — hence the Glauber model : But when K + 0 the principle of additivity of phase shifts breaks down . Let us consider this case in more detail . a From the equation -2 + eV – KB ( 2.
... this case we also have additivity of phase shifts — hence the Glauber model : But when K + 0 the principle of additivity of phase shifts breaks down . Let us consider this case in more detail . a From the equation -2 + eV – KB ( 2.
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Hence we have to use a z - ordered product to express x in a compact form : x = { explis . = dz'a ( x , y , z ' » , - ) ) } . ) Xi . Each infinitesimal step x ( z + Az ) – x ( z ) = iAzK ( 01.31 - idi.E10 , ) x ( 2 ) , x ( 2+ Az ) = eiA ...
Hence we have to use a z - ordered product to express x in a compact form : x = { explis . = dz'a ( x , y , z ' » , - ) ) } . ) Xi . Each infinitesimal step x ( z + Az ) – x ( z ) = iAzK ( 01.31 - idi.E10 , ) x ( 2 ) , x ( 2+ Az ) = eiA ...
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Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
| Export Citation | BiBTeX EndNote RefMan |