Лекции по основам кинематики элементарных процессов. Строковский Е.А. - 59 стр.

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p
=
λ
1/2
s, m
2
a
,m
2
b
2
s
,
λ
s, m
2
a
,m
2
b
λ (a, b, c)=a
2
+ b
2
+ c
2
2ab 2bc 2ac .
λ (a, b, c)=(a b c)
2
4bc .
p
s m
a
+ m
b
c d
m
a
m
b
m
c
m
d
a + b a
+ b
ϑ
p
,p
p
p
p
p
m
c
= m
a
m
b
= m
d
p
fin
p
  1   2 1    / 1 0 1    C 
5                        
                       λ1/2 s, m2a , m2b
                    ∗
                   p =        √
                             2 s
                                         ,          FA *G
     
2 λ s, m2a, m2b N       0   
  !"  " .  1/C  F   
! G 7 2  2 0   1 9 5  
3   1 6   2 ?
               λ (a, b, c) = a2 + b2 + c2 − 2ab − 2bc − 2ac .   FAA!G
    1 7  0 / 2 1   
  0  1  FAA!G N    L 
       56 1?
                                                2
                       λ (a, b, c) = (a − b − c) − 4bc .        FAA"G
             0   1  p∗   √F   C
       9    G0   s ≥ ma + mb
F   FA"AGTG0     1 7      2 
    
     L      9   FA *G   FA +G0   
    1   1  1 /  7 2/
   /    2   c  dD 4 2 2  0    
   N  20     ma 0 mb   mc  md
   0  C 0 C   ; ?  FA *G   0   1
12   a + b → a + b 1       
   0  C 1       2  
ϑ∗  .                     0  9  
 C     C 1   Fp∗⊥ , p∗ G0 2 p∗⊥ N 11  
F   1 1    1 5  2 1   
    G 1  0  p∗ N 1   1     
F1     1  1 5  2
1    G  7  1       p∗ 
   C   C    p∗ 
       C     12    Fmc = ma  
mb = md 0   1      G    7 2 9
  56 2 120   1     2 
    C  22   p∗f in ≤ p∗ F  
12    7  C  C   G
                                 -*