## Interactions of High Energy Particles with Nuclei |

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Page 7

We can also see that the physical reason for this phenomenon is the

We can also see that the physical reason for this phenomenon is the

**coupling**between different spin states produced by the term K ( 01.B. - id..E10 ) . So , we have to deal with a coupled channels problem . We can make the following ... Page 8

Because CXI - CX ) 1b we have [ Q ( x , y , z ) , Q ( x , y , z ' ) ] + 0 . A , One could argue that the

Because CXI - CX ) 1b we have [ Q ( x , y , z ) , Q ( x , y , z ' ) ] + 0 . A , One could argue that the

**coupling**to the anomalous moment is weak and hence not very relevant . This is true , but one can give some other 8 silicet )3-6*** ... Page 10

... and hence there is no

... and hence there is no

**coupling**between various spin channels . To conclude this section we may say that Examples 1 and 2 warn us that if the strong interactions are mediated through vector fields ( analogous to the electromagnetic ... Page 36

Let this

Let this

**coupling**be weak so that it is sufficient to take only the lowest order corrections : ( kpkr | H ' | kp ) | Vi ( kp ) ) = 2 || kp , 0 , 0 ) + E | 0 , kr , kn ) + ... Exp - Ern Eks kake + .. ] + . Page 53

do dt a PN - PN 72 40 AIR 4 do dt YN- > PN one determines the

do dt a PN - PN 72 40 AIR 4 do dt YN- > PN one determines the

**coupling**Yp . ( Here a is the fine structure constant . ) ( iii ) The results of this analysis check beautifully with the results obtained from po photoproduction on larger ...### What people are saying - Write a review

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