Interactions of High Energy Particles with Nuclei |
From inside the book
Page 19
... well the absorption , which is given by $ ( 6 ) because this is the dominating process , but not E ( 6 ) ) . If the Coulomb interaction is absent ( Xe = 0 ) the elastic cross section is invariant against the change of sign of ē .
... well the absorption , which is given by $ ( 6 ) because this is the dominating process , but not E ( 6 ) ) . If the Coulomb interaction is absent ( Xe = 0 ) the elastic cross section is invariant against the change of sign of ē .
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 ) V = n , y , + ny , where V , 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 ) V = n , y , + ny , where V , 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 Xez . Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is y = n , V , the wave ...
Hence due to the process of absorption , a new object is created : the wave which is polarized in the direction n Xez . Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is y = n , V , the wave ...
Page 30
We expand Ni ) into a set of states | 1 ; ) whose scattering and absorption in the target we assume known : 14 : ) = dij | ; ) Ili ) , 1 n , ) form orthonormal sets ( 4.1 ) | Α . - 18. | 1 ; ) = Ecij | 1 ; ) j of states .
We expand Ni ) into a set of states | 1 ; ) whose scattering and absorption in the target we assume known : 14 : ) = dij | ; ) Ili ) , 1 n , ) form orthonormal sets ( 4.1 ) | Α . - 18. | 1 ; ) = Ecij | 1 ; ) j of states .
Page 31
In this approximation ( Til T | 1i ) = 1 - mi = 2 Hence the absorption parameters ni are determined by elastic scattering of real particles . The inelastic amplitude ( il T | ; ) = ( 1 - ni ) ...
In this approximation ( Til T | 1i ) = 1 - mi = 2 Hence the absorption parameters ni are determined by elastic scattering of real particles . The inelastic amplitude ( il T | ; ) = ( 1 - ni ) ...
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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 |