Лекции по основам кинематики элементарных процессов. Строковский Е.А. - 158 стр.

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R
3
=
1
8
sP
a
!
2π
0
!
dt
1
ds
2
λ
1/2
s
2
,m
2
2
,m
2
3
8s
2
!
d
c.m.
3
.
t
1
=(m
a
m
1
)
2
m
b
= m
2
= m
1
=1
m
b
m
5
=5 m
3
=2 s =60
m
a
+ m
b
m
1
+
s
2
s
2
t
1
m
2
+ m
3
s
2
s m
1
; | cos θ
1
|≤ 1 .
2 3
s
±
2
= s + m
2
1
1
2m
2
a

s + m
2
a
m
2
b

m
2
a
+ m
2
1
t
1

1
2m
2
a
λ
1/2
s, m
2
a
,m
2
b
λ
1/2
t
1
,m
2
a
,m
2
1
.
C   0   F"! G 2 1  
                  !   2π        !                                !
         1                                    λ1/2 s2 , m22 , m23
   R3 = √ ∗
       8 sPa
                           dϕ       dt1 ds2
                                                    8s2
                                                                    dΩc.m.
                                                                      3    .   F"! AG
                  0




H "!"" %
               O!U !+     !0   t1 = (ma −
      0  .+ mb = m2 = m1 = 1 1   0
m 1 )2
     mb 4+ m5 = 5 m3 = 2 s = 60 1
  JVL4
   = 5       ma + mb → m1 + √s2 C
  ?
   • 19  C   s2  t1 O
   • 1    1     
                    √     √
           m2 + m3 ≤ s2 ≤ s − m1 ; | cos θ1∗ |≤ 1 .  F"! BG
   >     1 5  2     2 
 F"! AG 81  1   F/ C   QARG0 1
9         2      1
  2 → 3?
         s±
          2   =       s + m21 −
                        1                                        
              −          2
                              s + m2a − m2b m2a + m21 − t1 ∓
                      2ma
                        1  1/2                                      
              ∓
                      2m2a
                            λ     s, m 2
                                       a , m 2
                                             b   λ1/2
                                                       t 1 , m 2
                                                               a , m 2
                                                                     1   .     F"! -G
                                              "-,