SCIENTIFIC ABSTRACT KRESNIN, A. A. - KRESTINSKAYA, V. N.
Document Type:
Collection:
Document Number (FOIA) /ESDN (CREST):
CIA-RDP86-00513R000826420002-7
Release Decision:
RIF
Original Classification:
S
Document Page Count:
100
Document Creation Date:
January 3, 2017
Document Release Date:
July 31, 2000
Sequence Number:
2
Case Number:
Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
File:
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Body:
S1185
/60/005/002/001/022
Polarizat-Lon of garrpa-quanta... D274/D304
which agrees (to within a factor) with the exoression for the cross-~
section of the process obtained by S.D. Drell (Ref. L: Phys.. Rev.
1
87, 753, 1952). For the parameters t~l and 1~2 one finally obtains
2
[!t j4c2o - qI I+ L, 0)
-I+ 2cu OV + M4 -x
q,Q q, 2 -W2)
X (I - 2 '-'0) 'n3 I' (~pj ~kqj I + 2-0 (pn)' (kp.1 jkq,
q' X0
17
14," 2
0 + H~- r) P"
2- (Pn) Jl )(PI) +
0
+ 1 -21~ (P"1) + I - 2 (2p - p, I)j -
43f (15)
(171'
2
-lc +-5-(2p+p~, 1))].
~ (p.1) X0
M
Card 4/5
S/e185/60/005/002/001/022
Polarization of gamma-quanta... D274/D304
(n is the polarization vector, p and k are the energy vectors of
the electron and photon respectively, m, is the electron mass).
There are 5 references: 3 Soviet-bloc and 2 non-Soviet-bloc. The
reference to the English-language publication reads as follows:
S.D. Drell, Phys. Rev., 87, 753, 1952.
ASSOCIATION: Fizyko-tekhnichnyy instytut AN USSR (Physicotechni-
cal Institute of the AS UkrSSR)
SUBMITTED: July 20, 1959
Card 5/5
sj/185/60/005/004/001/021
D274/D306
,',,UT1iORS Kresnin, A.A. and Tishchenko, B.Y.
-------------
TITLE: Polarization effects in the scattering of electrons
by nuclei
PERIODICAL: Uhrayinslkyy fizychnyy zhurnal, v. 5, no. 4, 1960,
437-443
T F,'4,,.r: The scattering cross-section, the azimuthal asymmetry and
the polarization of the scattered electrons are calculated. Elec-
tron scattering by nuclei with Yuhawa charge-density distribution
is considered in the second Born- approximation. The Yultawa charge-
density distribution is
P(r) - X2-e--"r (4)
43C r
For describing the polarization of the scattered electrons, the
method of density matrices is used. For the cros-9-section one-ob-
Card 1/6
S/185/60/005/004/001/021
Polarization effects ... D274/D306
tains
do- ZC2 2 U V2)(l - v2sin2x)
rQ ( ]jj~V-2sin2X) + C42sin2x)2 X
X f, + Ze2v I + N2sin2x t --) -1
sinx[b, _ (I _ v2)-itgx (~Qn)6 (18)
V-'-Sin~4x 2
2]]
where 61 and 82 are given by expressions involving v , o~ and trig-
onometric functions of x, (x being half the scattering angle i~
and 04 = 2p/DC If oC >> 1, the cross section is
dd Ze2 2 (1 - V2) (I - V, S1n3 X)
X
d2 2mv2sin'x) (1+aL2s1n'x)2 (22)
X I +Ze,V 1 +&2 sins sinx rI-Sinx- 200 s1nx(1-v'*s1n2x) +
I -V2 sin, X V3
+ 2 (1 -0)%sin2X(I a si n x + a'(1 - s I n x)) n)
COS X
Card 2/6
Polarization effects...
S/18 60/005/004/001/021
D274YD306
For U_ a 0, formula (22) coincides with the well-known formula for
scattering crons-section of electrons in a Coulomb field. For
Oc