SCIENTIFIC ABSTRACT SHIROKOV, V.YA. - SHIROKOV, YU.M.
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CIA-RDP86-00513R001549530002-2
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RIF
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S
Document Page Count:
100
Document Creation Date:
November 2, 2016
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2
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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14UZYCHU,KO, Nina Mbaylovna; YURKEVIGH, Tattyana. Yakovlevna; BAKIROV,
A.A., prof., glav.red.; RYABUKHIN, G.Ye., prof., red.;
USPENSKAYA, N.Yu.,prof.,red.; ZHDANOV,M.A., prof., red.;
DOLITSKIYI V.A., dots., red.; SPIKHINA, A.Y., kanda geolo nauk,
red.; YUDIN, G.T., kand. geol.-min. naukq red.; TABASARANSKIY,
Z.A., dots., red.; BAKDOV, E.A., dots., red.; BYKOV, R.I.,
dots., red.; FaIKIN, K.V., kand. geol.-min. nauk, red.1 JOYAZEV,
V.S., dots., red.; SHLiOKOV, V.Ya., st. nauchn. sotr., red.j
YUVGAS, S.V.p ved. red.; NEVELISHTEYN, V.I., ved. red.
(Geological conditions and fundamerrLal characteristics of oil
and gas accumulations in the limits of the Bpi-Hercynian platform
in the south of the U.S.S.R.) Geologicheskie usloviia i osmvnye
zakonomernosti ra=eshcheniia skoplenil nefti i gaza v predelakh
epigertsinskoi platformy iuga SSSR. Pod red. A.A.Bakirova. Mo-
skva., Gostoptekhizdat. "1 1.1, (Central Asia] Sredniaia Wis.
1963. 442 p. Vol.3. [Volga Valley portion of Saratov and
Volgograd Provinces) Saratovsko-Volgogradskoe Povo2zhle. 1963.
153 P. (MIRA 17:4)
1. Moscow. Institut neftekhimicheskoy i gazovoy promyshlennosti.
BAKIROVI A.A.; SHIROKOV, V.Ta.
Proapects for finding- ImTs oil and ga3 accumilation3 in the
Tajik S.S.R. Sov. geol. 6-no.5.*51-62 My 163. (MIRA 16:6)
1. Moskovskiy inatitut naftakhimichookcry i gazovoy proa3h-
lannosti, imeni I.M. OubIcina.
(TaJiki3tan-Patroleum geology)
(Tajiki3tan-Gas, Natural-Geology)
T~-'IPOV, '1';.; SHIPOKOV, V.Ya.
Water.3 and brInnn or oie meijoz-)i
Tajik DepreBsion in connection wt,.
Nefte,gaz.geol. i geofiz. no.12:1%-
1. Moskovskiy ordena Trudovogo KraL
neftekhimicheskoy i gazovoy prorky:;h
-38
1;,".
3
al,jp
PIS unitary, finite 112, V2 . ..... I
+M
Ps unitary, finite 0; 1, 2,
-M
PIS unitary, finite 1/2, 3/2 . ..... -1
-M
For P - Unitarity; mieasurements Nain invariants Aaclitional
U
Represer.- of representation accord- n2 2 > 0 invariants
tation Ing to spin-variabJ13 -P ~1~ 2 2
CC F~ If T
Pa- unitary. infinite
n
pia. unitary, infinite
n
P+n unitary, infinite
>
> I/V
Bro
Card
56-5-20/46
A Group-Theoretical InVC3tigation of the First Principles of Relativistic
. Quantum Mechanics II. A Classification of Irreducible Representations of an
Inhowgencous Lorentz Grorip
which ar--. Slavic.
ASSOCIATION- Moscow State Univi~rsity (Moskovskiy gosudarstvannyy universitet)
SURMITTED: Deceaber I I , ! 956
AVAIIABLE, Libmry of Congress
Card LA
AUTHOR: Shirokov, 11u.M. 56-5-21/46
TITLE: A Group Theoretical Investigation of the First Princip2es Of
Relativistic Quantum Mechanics III. Irreducible Representations
of Classes P. and 00 and Not Fully Reducible Representations of
an Inhomogeneous Lorentz Group (Teoretiko-grappovoye ra3smotreniye
oanov relvativistskoy kvantovoy mekhaniki III. KeprivoU~e
predstavlaniya klaasov PO 1 00 1 ne vpolne privodimyye predstav-
leniya. neodnorodnoy gruppy Lorentsa)
PERIODICAL: Zhurnal EkBpe-rim. i Teoret. Fiziki, 1957, Vol- 33, Nr 5,
pp. 1208-1214 (USSR)
ABSTRACT: The classification of the states of a relativistic quantum system
is derived theoretically. The unitary and nonunitary characteristics
for the classes Po and 0. are shown in the following table:
Represen- Unitarity,mea3ure- Main in- Additional in-mriants
tation ments according to variantis
spin variables p2 01
rKl--4~
Card 1/2 P unitary, simple CC it 0 SH= �1 , S r =il =O' l v2.
t 0 0
56-5-21/46
A Group Theoretical Investigation of the Fir-at Principles of Relativistic
Quantum Mechanics III. Irreducible Representations of Classes PC and 00 and
Not Fully Reducible Representations of an Inhamogeneous Lorentz Group
P unitary, simple C( . 0 SH= ti , Sf0=tl'7-j
PC unitary, infinite 0(-C > 0 SH= *1
:r 0
PIC unitary, infinite G( SH= t1
0
C nonunitary,infinite C < 0 S - ti
P
i0 H-
e nonunitary,infinite cC= Cn mn n m>n mn
correction to the kinetic energy of the n-th nucleon)& Furthert
the correction term to the interaction -17aniltonian if' is
mn
investigated. This interaction correction formula is written
down for 2 particles in the states
Jos2 01 > 082 10---., 11p2/, O1N , 11P2 01>
1/2 1/2 3 112
with r 0 = 1.65-10-13cm(hw - 15 Mev), the potential is written
down in the form V-V o(O-317 + 0.500 P + 0.183 PQ) f(r/a)
and for the Gaussian potential course
On Relativistic Corroctions to the SOV/56-36-2-19/63
Phenomenological Theory of,the Levels of Light Nuclei
and for the square potential well (Ref 1)
Vo . -33.6 Mev, A " 2.1.10-13cm . V(in kev) is calculated and
compiled in a table. The correction was found to dependto a
high degree on the shape of the potential and i3 of the order
of magnitude 0.02 - 0.2 Mev for a pair of nucleons, 0.2-2 Mev
for liCht nuclei, and 2-20 Mev for heavy nuclei. For nuclear
levels it is of the same order as for nucleon pairs. There are
I table and 3 references, 2 of which are Soviet.
ASSOCIATION; Inztitut yadernoy fiziki MoskovskoGo gosudarstvennogo universiteta
(institute for 'Nuclear Physics of Yoscow State University)
SUBMITTED: June 16, 1958
Card 3/3
21(l) BOV/56-36-3-35/71
AUTHORS: Kaminskiy, A. K., �,hirokov, Yu. It.
TITLE: On the Electromagnetic Radii. of the Lightest Nuclei in the
Ground - and in the Lowes'EkaillMm States (Ob elektromagnitnyleh
radiusakh legebayshikh yader v ouiiovnykh i nizahikh vozbuzll-
dennykh sostoyaniyakh)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheakoy fiziki, 1959,
Vol 36, T1r 3, PP 874 - 878 (USSR)
ABSTRACT: In the present paper the authors calculate the radii of nuclei
with mass numbers 5 - 8 for the ground- and the first excited
states on the basis of experimental data on isotopic multiplets
and scatterine of high energy electrons on nuclei, and they
especially investigate the dependence of the radius on the
excited state. In a figure, 4 diagrams show the de endence
3
of r
on excitation energy: Figure a) for He5 - Li
'
0
b) for He 6 _ Li 6 _Be6 (in dependence on E
of Li6
exe
c) for Li a - Be a -B8 (in dependence on E
of Be8) and
exe
d) for Li7 _ Be7. It was found that the nuclear radius of He5
Card 1/2 and Li5, as an exception, shows no monotonous increase with
SOV/56-36-3-35/'71
On t:ie Electro,-_- -:,,-tic R!,. !ii a-*' the Lightest !Iuclei in the Gro-un':- and in
the --owect ExcltatiocL.S~tes
For the 2. excited level with E - 16.69 Yev the nuclear
radios is smaller than for the firit aA also smaller than
for the qround Btate. For Li7 - Be the nyclear radius in-
creases rapidly with energy, for L17 - Be there is a weak
clopondence, and the namo in the cace for the nuclear radius
with A.=B. In general it may be said that, with the exception
of the He5-Li5 doublet, the nuclear radii for all nuclei in-
crease monotonously with energy. It was found that agreement
between experimental data from the scattering of fast neutrons
on nuclei and those calculated from the Coulomb (Kulon) energy
difference can be improved by ssuming a different value for
r for s- and,y-shells. For Lil, fo example, one gbtains
o 13 Ir
r. . 2-42.10- cm and rp . 1.32.10- am and for Li . 9 -
- 2.65-10-13cm and rp - 1.07.10-13cm is obtained. There are
1 figure and 8 references, 3 of which are Soviet.
ASSOCIATIO'T: Moskovskiy gosudarstvennyy universitet (Moscow State University)
SUBMITTED: September 16, 195.9
Card 212
Shirokov, Yu. L'. SOV/56- 36- 3-, (", Y
The Groun-Thco.~ctic.-.l Trcrtment of the Bases of
Quantum ilcchanJes. V. (Teoretiko-gruppovoye rasr :;,:otreniy,~
osnov relyatjvi-;.skoy kvantovoy mel.,haniki. V.).Irroducible
ul t.ie Inhomogencouo Lorentz Group Inclu-lir,-
Sp;~tiacl tnd 'Leflections (Neprivodiryye prods tavloniya
neodnorotino.-y* [~,rup.--y Lorentsa, vklyuchayushchey otrazheni,-a
p:-ostrnr.:1tve i vo vromeni)
~!-DDICAL: Zhurntl e':3perirentallnoy i teoreticheskoy fiziki,
1959, Val )6, !~r 3, Pp 079-608 (USSR)
Int
A C-2: The praL~cnt 7. ended to carry out a systematic
inve-,itication u-' timc reflection 1a%7 within the rr-:
of the ordinary of the representation of th~.-
inhomoi7,encoun :,,~xlup oithout using a certain
form of enuatio-n -,ot-~cr. The Wigner-formulation of the ti.,.c
reflection law -'q Cto~i2.t vith by a separate paper, and the
is the care ',lc connected with the CPT theor.----".
In the present 7a-.cr a--thor, by utilizing the re-ultr
obtained by papers I - ;1, gives a complete classifi: .1.2-,,P-i
1/2 all irreducible rcp-rc::--!rt--tionc o1' the inhomocnnc--..,-
';r,)uP-*-'hro.-etica1 Treatnunt of tht, Danes of SO//56-3(--.1'5-,'6/7 1
.1, 'J,,rif;tjc ;uantum Mechanics. V. lr:-ed,~Cible lwpreccntations ol" the
Lorentz Group Includir.,,~; Sprttial and Time Reflections
Lorcii't.n. ,~,roup includin,-' jpace and time reflections. It in
~:hown 'that the concc.,jit of time parity cannot be intro,luc,2d for
i,~,-~rticlos --.-rith a rest mass. For such parLiclas
trio unequivalcni., cc~nc*ptz, -.-.,hich differ in respect zo
.ime paarit~;, prof),,?r-A-:~s, jxist for a Civen spin. '.',ith th" -'lit. of
t`1C conce -ot of % covering i_-roup it is --hown tnat fo--
j.~rxticlo-- half--Jlnt(--~-~er spins the number of possible
rc':~rc--~ntr~ticnr; -.ith various reflection laws is larger than
hitherto ns:~uned. Ther- r-re 4 tables and 9 references, 6 of
-Alich Soviet.
.'ookovskiy uaiver',:itet (Yoscow State Univer--it-,)
T
Sontonber 16, 1'.
SHIROKOV, Yu. M., Doe Phys-Math Sci -- (diss) "Theoretico-group
methods in relativistic quantum theory." Moscow, 1960. 12 pp;
(Academy of Sciences USSR, Physics Inst im P. N. Lebedev); 150
copies; price not given; bibliography on pp 11-12 (30 entries);
(KL, 25-60, 125)
SHIROKOV, Yu.M.
Spatial and time reflections In the relativistic theory. Zhur.
eksp. I teor. fiz. )8 no.1:140-1.50 Jan '(0. (MIRA 14:9)
1. Institut yadernuy fiziki Moskovskogo gosudarstvennogo universi-
teta.
(Relativity (Physics)) (Particles (Nuclear physics))
9u
S/056/61/041/006/040/054
B109/B102
AUTHORSt Zelenskaya, N. S., Shirokov,
TITLEs Relativistic corrections to the magnetic moments of H3 and
He3
PERIODICALt Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 41,
no. 6(12), 1961, 1934-1937
TEXT: Ageneral expression is derived for the relativistic corrections
to t e nuclear magnetic moments arisinG as a result of non-Galilean
relativistic corrections to the Hamiltonian of nucleon-nucleon interaction.
According to F. A. Zhivopistsev, A. I. Perelomov, an4 Yu. M. Shirokov
(ZhETF, 36, 476, 1959), the non-Galilean correction to nucleon-nucleon
interaction has the form
Card 1/4
t
S/056/61/041/006/040/054
Relativistic corrections to the ... B109/B102
H' iiM,P, 4- i (P OHM") (P
MR op.
+
d%
+ W.~ IPPI - (PL"--,,) (pp) + ip,p)
00-
P = p ,, +,P,, - P (PM - P"), x = XM - X,
denotes the interaction energy of the m-th and n-th nucleons.
r of the non-Galilean relativistic correction to the nuclear
.,.-?nt is- obtained from. (2) as
Alt 2HM,, (e,,, + e,,) (n (r - R)J P
31
(et + e~)(Cr. - 13.) [n ((r (r - R) n
Card 21,; dr . (I dr
31790
S/05 61/041/006/040/054
Relativistic corrections to the ... B109YB102
(3) has been calculated "or the 2 S1/2 'tate of mirror nuclei by using
the wave function of the harmonic oscillator and the expression
H - (W + u + BP + -~'P P V(r) (V(r) - Gauss or Yukawa potential).
mn x Lr x r
The results are shown in a table. Concluslonsi A) The relativistic
non-Galilean correction exceeds considerably the correction of the
spin-orbital interaction; B) the correction terms have the cirrect sign;
the maximum value of 0.086 explains only 30A of the discrepancy between I
theoretical and experimental values. The difference is attributed to
the ef5ect of exchanee mecons, which has been discussed by S. D. Drell
and J. D. Walecka ~Phys. Rev., 120, 1069, 1960). T),ere are I table and
13 referencest 4 Soviet and 9 non-Soviet. The four most recent
references to Enrlish-language publications read az; followat L. D.
Rearlstein, J. C. TurLf, K. Wildermuth. Nu--l. Phyz., 18, 23, ig6o; A. C.
Butcher, J. M. 11c Namee. Proc. Phys. Soc., 1_4, 529, ~7959; R. A. Ferrel#
W. M. Visscher, Phys. Rev., 102, 450, 1956; J. M. Berger. ?hys. Rev.,
115t 223, 1959.
Card 3/4
317 ~0
S/05 611041100610401054
Relativistic correction3 to the ... B109YB102
ASSOCIATIONs Moskovskiy gosudarstvennyy universitet (moscow state
University)
SUBAIITTEDt July 12, 1961
Legend to the 'fable: (1) shape and parameter of V(r) (V is given in
0
'YPv i in 10- 13 cm); (2) Gauss potential; (3) Yukawa potential.
;v, napamelpw Y(r) -0 B 0=. X-0,022111
A~L(Hl) 4 MHCS) AMR,) I AIL(Re)
ar=1,73 111 0 -0,048 O,Ot4 -O,Ot4
a~1'94 1-1 0 -0,032 0,009 -0,009
a~1,55 0 -0,018 D,OD5 -.0.005
11memma.-i lOxans
V, :- &9* a-1, 17
j.. 0 -O.DS6 0.026 -0,026
v,46.-w .-t &1
. 0 -0,056 0.017 --41,017
Curd 4/4
SIUR~!nV4 Yu. M. -- -- -
- -t~-! ~~ - , , - . I
"On the Conditions of the Mikrocovariance and Mikrocausality without
any References to the Postulates of the Quantum Field Theory"
report presented at the Intl. Conference on Ifigh Energy Physics, Geneva,
h -11 July 1962
Inst. for Nuclear Research of the Moscow State University
S/056/62/042/001/027;/048
B100102
AUTHORS: Cheshkcv~ A, A., Shirokov, Yu. M.
TITLE: Invariant parametrization of the relativisti: scattering
matrix
PE'RIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 42,
no 1, 1962, 144-151
TEM Tne parametrization is first performed in the center-of-mass system
A number of 7ersions, all of them relativistically noninvariant, are
tested In so doin the authors base on M. Yacob, G. C- Wick (Ann of"
- 7, 404 9 L. Wolfenstein, J. Ashk
Ph,s 595, in (Phys. Rev., ft~, 947,
-,9~52), 71, 1. Ritus (ZhETF, 1264, 1957); S. M. Bilenlkiy, L. I Lapidui,
L D Puzikov R. M. Ryndinj~ZhETF, a, 959, 1958); and Ya. Fisher,
S Ck.ulli (ZhETF, 36, 1740, 1960; .12, 1349, 1960). The scattering matrix
3 ~ms parametrized in the c.m.s. does not essentially differ from other
parametrized matrices. However, the invariantly parametrized elements of
the. S matrix are written in matrix form, in which no nonpkysicai parameter5
appear, and the particle chiralities are used to describe the initial an-a
Card /2