Interactions of High Energy Particles with Nuclei |
From inside the book
Page 19
... not well known : we know pretty well the absorption , which is given by dominating process , but not έ ( b ) ) . If the Coulomb interaction is absent ( x . = 0 ) the elastic cross section is invariant against the change of sign of .
... not well known : we know pretty well the absorption , which is given by dominating process , but not έ ( b ) ) . If the Coulomb interaction is absent ( x . = 0 ) the elastic cross section is invariant against the change of sign of .
Page 28
Consider the absorption of polarized light by an anisotropic absorber . The incident wave is polarized in the direction n ( perpendicular to the z direction ) . n = ( nz , ny ) ¥ 2 = n2 ¥ z + ny where is the wave polarized in the x ...
Consider the absorption of polarized light by an anisotropic absorber . The incident wave is polarized in the direction n ( perpendicular to the z direction ) . n = ( nz , ny ) ¥ 2 = n2 ¥ z + ny where is the wave polarized in the x ...
Page 29
Hence due to the process of absorption , a new object is created : the wave which is polarized in the direction n Xe .. Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which ...
Hence due to the process of absorption , a new object is created : the wave which is polarized in the direction n Xe .. Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which ...
Page 30
We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal sets ( 4.1 ) of states .
We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal sets ( 4.1 ) of states .
Page 31
The trouble is with the outgoing objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In fact , one usually determines them experimentally ( see the end of this ...
The trouble is with the outgoing objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In fact , one usually determines them experimentally ( see the end of this ...
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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 |