## Interactions of High Energy Particles with Nuclei |

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Page 18

From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of finding out whether the inelastic shadowing ( or inelastic screening )

From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of finding out whether the inelastic shadowing ( or inelastic screening )

**corrections**are important at very ... Page 19

Let us consider first the Coulomb

Let us consider first the Coulomb

**corrections**for heavy nuclei . One can , in principle , use the individual amplitudes which have Coulomb interactions built into them ( this very tedious cal- culation has been done , e.g. , in refs . Page 22

These two factors make Coulomb

These two factors make Coulomb

**corrections**insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ... Page 23

SA ' ) ( 3.8 ) Then we can compute the

SA ' ) ( 3.8 ) Then we can compute the

**correction**factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . Page 24

Hence if we can factor out the c.m. wave function from the product = II ; ; ( r ; ) we can stick to calculating M with Yo but we have to multiply it by a

Hence if we can factor out the c.m. wave function from the product = II ; ; ( r ; ) we can stick to calculating M with Yo but we have to multiply it by a

**correction**factor : ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 .### What people are saying - Write a review

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