Лекции по основам кинематики элементарных процессов. Строковский Е.А. - 64 стр.

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E
±
=
(p
±
)
2
+ m
2
D =0 g
=1 β
= β
cm
p
+
= p
g
< 1 p
p
+
g
> 1 p
p
+
sin θ
max
=
γ
β
γ
cm
β
cm
=
γ
g γ
cm
.
tan θ =
sin θ
γ
cm
(cos θ
+ g
)
.
NN dN
p =
p
2
L
+ p
2
T
p
L
p
T
p + p p + p + π
0
d+p d+p+π
0
NN
       1       7 2 E ± = (p± )2 + m2 
    8  0   D = 0    5 g∗ = 10   β ∗ = βcmO 2 
p = p−  . g ∗ < 1
 +
                         p− F   1 TTG   
  0     0       9 
p+  . g ∗ > 1   9 0 p−  p+  5   C 1
 0   7      C 2  
1    9  
                                γ ∗β ∗      γ∗
                  sin θmax =
                               γcm βcm
                                       =
                                         g ∗ γcm
                                                 .        FAB-G
      0 C     2         
    8  
                                     sin θ∗
                    tan θ =
                               γcm (cos θ∗ + g ∗ )
                                                   .      FABEG

 *+/42%3& , 00&.239= 1+,44%=
H     C   2 1               
        12  
       AE 1 1  7 1 1  1
     2 C  N N  dN   / F   
  56/ 7 1 1     G . 
 1  1 p = p2L + p2T 0 2 pL  pT N 1   F
1  1   G  11   1   >  7 
 1 2 5 F /  7 21 G C
   1  10 C 2 /  /
I    1   0  9      
 p + p → p + p + π0           0
  1 7   0   9       
 d+p → d+p+π0 0 2        ”  ” 
     0      F   G    
  /    HC  1  1 0 1 
C6 7    0        6 &
   ; 0     7   8 0
 7    6     0
7 9     ' 3!0*
    %' ”0”   
     1 0 1                0
1     C   15 C     
     0 1 6     / N N    
                                   EB