Лекции по основам кинематики элементарных процессов. Строковский Е.А. - 114 стр.

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P
2
N
m
2
N
= 2m
N
s
M
tar
M
tarm
N
+
s
· p
2
f
+
2
s
,
s
M
ejected
P
2
ejected
P
2
ejected
ω
2
F
=(P
N
+ P
transf
)
2
=(ν + E
N
, p + p
f
)
2
,
ω
2
F
= t +(m
N
s
)
2
+2ν (m
N
s
)
(M
tar
+ ν) ·
p
2
f
M
tar
m
N
+
s
2p
f
· p .
t
ω
F
R
ω
12
ω
0
Γ
R
(1+2)
σ
Γ
R
(R 1+2)
(ω
2
0
ω
2
12
)
2
+ ω
2
0
Γ
2
R
/4
.
        2  O 7    1              
 5
            2
           PN − m2N = −2mN s −
                                        Mtar
                                     Mtar−mN +s
                                                 · p2f + 2s ,    F+,G
  /               ”  /    
1 / ”  7 2     16  F  G 
       0  7     1   
1 1     7 20  /   20   
   2       ; 1 2     
  C 0      2  122   
” ”    2 C    2  
F2  C         2  0   
 1      1                1  sG
    16  F  G   Mejected 1   
  Pejected
            2
                   0         0 
     2
    Pejected
                                     2                     2
              ≡ ωF2 = (PN + Ptransf ) = (ν + EN , ∆p + pf ) , F+*G
  C 1  
                               2
        ωF2   =   t + (mN − s ) + 2ν (mN − s ) −
                                     p2f
              −   (Mtar + ν) ·
                               Mtar − mN + s
                                              − 2pf · ∆p .       F+"!G
@  t N     1    F   1  2 
  B1 G ; 1  2  9   0    
 6             2 
 ? 2  C  1   A1   A1   
  2 C   0    19   
       122        F 
G0  ωF     0   0   
  8    0 2  7    N   F1 
∆G0   6            
         1  / 2   
 2  2   RO 7     5  ” 26
” ω12  2 ”  ” ω0 0        
C C 0  56 1 5      
   9 ΓR 1       (1 + 2)?
                            ΓR (R → 1 + 2)
                    σ∼               2             .             F+""G
                         (ω02 − ω12
                                 2 ) + ω 2 Γ2 /4
                                        0 R

                                   ""B