SCIENTIFIC ABSTRACT VOLKOV, D.I. - VOLKOV, F.G.
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SCIENTIFIC ABSTRACT
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21355
S/126/61/011/004/002/023
24.9q0(11.37, 117, //SX) E032/E314
AUTHORS: Volkov,, and Pshenlchkin, P.A.
TITLE: Paramagnetism of Manganese-AntImony at High
Temperatures
PERIODICAL: FIzika metallov I metallovedenlye, 1961, Vol. 11,
No. 4, PP. 513 - 518
TEXT: The present authors report experimental data on the
susceptibility of MnSb alloys in the paramagnetic region.
In distinction to earlier work, the susceptibility is
measured not only near the melting point but well above this
point as well. The suvqceptibility was measured with the aid
of the Faraday-Sucksmith method, using argon as the inert
medium. The specimens were obtained In a high-frequency K
vacuum furnace. Fig. 1 shows the reciprocal of the suscept-
ibillty as a function of temperature for MnSb (Curve 1),
alloys with 25% Yin (Curve 2), 209/o Mn (Curve 3), 15% Mn
(Curve 4) and 35% Mn (Curve 5)- It follows that below the
melting point the paramagnetism of MnSb obeys the Curie-Weiss
Card 1/7
-1- . -S - ~~ NGM ~,,u!
M_AK*r~_
21355
S/126/61/0.1-1/004/002/023
Paramagnetism of .... E032/E3i4
law (meltIng point approximately 700 - 750 0C). The MnSb
alloys represented by Curves 2-4 also obey thIs law. This is
due to the fact that the ferromagnetic compound MnSb Is
always present In those alloys in whIch there Is less than
310% Mn (by weight). A dIffevent dependence Is found in the
case of Mn2 Sb (Fig. 2: Curve I - Mn 2Sb; Curve 2 - 40.7% Mn).
Analysis of the data showed -that the paramagnetic suscepti-
bility of Mn2 Sb can be described by the Neel laws ifith Neel
constants 1/%, = 270, a-= 6 200 and 0 = 553 0K. The MnSb
alloys can be divided into two groups; namely - those
containing,MnSb and obeying the Curie-Weiss law and those
near the 1N1n2Sb composItIon, which are described by the
hyperbolIc Neel law
T
&o C T
Card 2/7
S/126/61/011/0~4/002/023
Paramagnetism of .... E032/E314
Fig. shows 1/% as a function of temperature above the
nielting point (Curve 1. 150,'D' Mn; *Curve 2 - 25%. D1n) -
Fig. 5 shows the same relationship for alloys witsi 200pl, Mn
(Curve 1) and 291% Mn (Curve 2). Fig. 6 shows the Curie-
Weiss constant, C , as a function of concentration of ~.'n.
The upper curve refers to solids axid the lower to-liquids.-
The numerical data are summarised in Table 1.
There are e~ figures, 1 table and 8 references: 6 Soviet
and 2 no*n-boviet.
ASSOCIATION: Moskovskly gosudarstvennyy univex-si-tet
im. N.V. Lomonosova (Moscow State University
im. M.V. Loinonosov)
SUBMITTED: july 8, 196o
Card 3/7
S/126/61/011/004/0.02/023
Paramagnetism of E032/E314
Fl~. 2:.
4F
' ~2
.:i 100
7,7,-70'-0- ~-7~ 'goo Oq 200.. ....... 600 800 /000 OK
550 600 "a
.500
Card 11/7
s/126/61/011/004/002/023
Paramagnetlsm of .... E032/E-314
Fig. 3: Fig. 4:
JO -
122
20-, /JO*
170*.
219*
0
00600 Oro MOO 1? 0'
0 2000 1/000 &~Ofl- -3J0-99 /0000
Cavd 5/7
MMMT~2~1111___
-355
S/126/61/oll/oo4/002/023
E032/E314
Paramagnetism Of
Fig. 6:
5
250
200-
/J0
10
100
50
4b 10 25 L"y
0 /000 1700 1400.0K
~o 600 4600
Card 6/7
t. J,
Paramagnetism of ....
Table-.
Manganes
Content,
weight ./0
21-355
s/.jn-6/61/o.ii/oo4/ooz/o2l?
E03-"/E3]4
L ~-i qu i dC 1.0 c I i qui d L 0
15 288 -224 57 70
20 c14 139
303 -600 1
25 298 -9920 108 j-62
29 299 3 9 0 1-16 230
Card 7/7
1
VOLKOV, D.I.: PSHIENIGHKIN, P.A.; BUBLIY, II.I.
Anomalous temperature dependence of the parEmaagnzetf,:! --usc--P-
tibilility of certain manganese alloys. Fiz. met. i metalloved.
17 no.5:698-702 My 164. (MIRA 17:9)
1. 14oskovskiy gosudarstvennyy universitet imeni '"n-onosova.
16(l) PHASE I BOOK EXPLOITATION sovI2660
V4600yuznYY matemAticheakiy s*yezd. 3rd, Koacow, 1956
Dokl
d
d
l
a
ov.
a
Y
Trudy. t. 4t xratkoya sodarzhanlys sektalonnykh dok
inoetrannykh uchenykh (Transactions of the 3rd All-Union Mathems-
tical Conference in Moscow. vol. 41 Summary or Sectional Rop6rts.
Reports of Foreign Scientists) Noscowi Izd-vo 1W 533.11,
247 p. 2,200 copies printed.
Sponsoring Agencyc Akademiya nauk SSSR. Matematichaskly Inatitut.
Tedh. Ed. a. G.M. Shevchanko, Editorial Board: A.A. Abramov, V.0.
Boltyansicly, A.M. VaBillyev, B.V. Medvedev, 4.D. Kyahki3, S.M.
Kikol-skly (Romp. Ed.), A.G. Postnikov, YU. V. Prokhorov, K.A.
RybnJkov, P. L. Ullyanov, V.A. Uspenskiyj K.O. Chetayev, 0. Ye.
ShIlov, and A.I. Shirshov.
PURFOSZt This bo6k Is intended for mathematicians and physicists.
COVERAGE; The book to Volume rv or the Transactions of the Third All-
Union Mathematical Conference, held In June and July 1956. The
parts. The first part contains sym-
marlea of the papers presented by Soviet scientists at the Con-
ference that were not Included In the first two volumes. The
second part contains the text of reports submitted to the editor
by nOn-SOVIet scientists. In those cases when the non-Soviet act-
entiat did not submit a copy of his paper to the editor, the title
or the paper in cited and, If the paper was printed in a previous
viums, reference to made to the appropriate volune. The Papers,
both Soviet and non-Soviet, cover varroua topics in number theory,
algebrat dirrarentima and Integral equations, function theory,
functional analysis$ probability theoryj topology, mathematical
problems or mechanics and physics, computational mathematics,
mathematical logic and the foundations or mathematics, and the
history of mathematica.
Leningrad). Certain generalizations of the concept
problems of stability for Partial differential
equations
16
u
Gavel & S-P C~'vov). On the behavior of solutions of linear
s"1 ";r*.
UW41-t-.76111i In the neighborhood, or certain singular
manifolds 16
G*l'"1L_A_Y*_-4I4nIngrad). On the reducibility or systems
~07_afffsrentlal equations with quaelperiodic cofficients 17
Description of noncoaras singular
Points of a dynastic system on the plane by means or the cosrse
Points of proximate systems .18
Deetc~_A_A_ (Moscow). On the solvable extensions of linear
differential operators of the first order 18
fl=", A 0-- (Llvov). On one method of determining the
asymptotic properties Of the eieenvalues and 4igonfunctione
Card 5/34 .fiir'.111ptic mystems. 1y
SAKHAIUMCV, N.A.; 7OLKOV, D.M.
Mean of caIculating the field of a point source when there is a
vertical layer. Uch.zap.IGU no-303:193-202 162. (IMIFA 15:11)
(Electrio prospecting)
OS
AUTHORt Volkovq D.M.
TITLE-. the solution of
and of other polyh%rmonic
infinite algebraic
S/044 602/00/010/006/021
C1 1 1YC333
static problems of elasticity theory
problems with the method of
systems
PERIODICALs Referativ-nyy zhurnal, Matematika, no. 10, 1960, 76,
abstract 11563. (Tr.Leningr.tekhnol.in-ta im. Lensoveta,
19599 vYP- 501 6-10)
TEXTs By the example of the static problem of elasticity
theory it is shown that, if the coordinates of the contour (considered
as functions of the polar angle 0 under a mapping of the domain onto
a circle) possess continuous derivatives of the four first orders,
the problem can be red-aced to the solution of a quaai-regular infinite
system of linear algebraic equations; the unknowns are the coefficients
of the Taylor expansion of where F occurs in the boundary
conditions
where X - conat,
f1+ 'f2'
f1 and f2 are given continuous functions, and z(5) maps the circle
Card 1/2
;M
~~ ~--, - -; ~~ 0 1 rs --E WMINOINEW
22583
on the solution of static problems ... S/044/60/000/010/006/021
C111/C333
1~1 < 1 onto that domain for which the problem is being solved.
[Abstracter's notes Complete translation .1
Card 2/2
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A, Itctrous in a 6~14 of pUne nonpoLanxed clactromad-
waves from the point of view of the Dirac equation. -00
Volk,,v, J. Thre,el. PAY, (11. S. S, It.) 7. ..46
rnj; volu"). The Ilnutins If analtion of quantum Into -9*
claasicst mechanics. N';&. 1'. '1 VI it IAJ. Jbij. 1,.~)U S.
I It, vh.knuv Ilf 0001 -11 A WAVV I'dCUt WIM tint" isful flit' -00
06 1, -ml t,m .4 1 h.- ,I,% III- I If ., J,ks I i, 1" 'A it It
1-10"I'dat Ittwm... I.. III, ~1--[ ;",
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'
U33P / Fr.~na Animals - Poultry
Abs Jour : Rof Zhur - Biologiya, No 5, 1959, No. 21309
Author : V04~ge-D,-T--
Inst :-5-clontific Rosaarch Instituto of Poultry Farming
Title : Preeding Work in DermArkis Poultry Parming
Orig Pub : 13yul.. nauchno-tekhn. inforlh.'N."i. in-ta ptitsovodstva,
1957, No 2, 47-49
Abstract : No abstract givon
Card 1/1
240)
AUTHORS: Volkov,D.I.,and Chechernikov, V.I. SOV/155-58-2-44/47
TITLE: The Temperature Dependence of the Paramsgnetic Receptivit7 of
Soma Ferrites (Temperaturnaye, zavisimost' paramagnitnoy
vo,qprilmehivasti nekotorykh ferritov)
PERIODICAL: Nai;ichnyye doklady vysshey shkoly. Fiziko-matematicheakiye nauki,
1958, Nr 2, pp 208-213 (USSR)
ABSTRACT: The present paper is a report on the experimental investigation
of the temperature dependence of the paramagnetic receptivity of
several ferrites (nickel-, cobalt-9 manganese-, magnesium-,
lithium ferrites). It was stated: in the immediate neighborhood
of the ferromagnetic Curie-point the receptivity is a function of
the temperature and the field. For higher temperatures the depedence
on the field suspends, but not always it follows the law of Neel
,rRef 1]; e.g.'the behavior of the manganese ferrite in the interval
from 6730K to 900 0K deviates essentially from Neel without depend-
ing on the field. For 13600K the receptivity of the lithium ferrite
changes desultorily.
There are 5 figures, and 4 references, 2 of which are Soviet, and
2 American.
Card 1/2
-~--2ZW n N k
;Egzwm_~l-~Wxg in YNRP~~.--iFlle-zl;'-A --1 -.1.1 .1 lllf~t-~. - 1-
The Temperature Dependence of the Paramagnetic SOV/155-58-2-44/47
,Receptivity of Some Ferrites
ASSOCIATION:Moskovskiy gosudarstvennyy universitet imeni M.V.Lomonosova
(Moscow State University imeni M.V.Lomonosov)
SUBMITTED: January 17, 1958
Card 2/2
Vp1
Un!iqueness of the classical energ7 integral. Vest. IGU 8 no.5:3-Ij
MY '53. (MIRA 12'-7)
(Integrals)
VOLKOV, D. M.
VS13R/Physics - Electromagnetism 11 May 50
Waves, Blectromaigaetic
"Second Integral of the Conservation-Law Type for
Electromagnetic Fields," D. M. Volkov, 2 pp
"'Dok Ak Rauk SSSR" Vol LXXII, Ifo 2
Considers case where electroma.Xnetic waves are
completely reflected, and are -propagated in empty
finite region D of arbitrary form from metallic
surface S bounding a given reF;ion. The fields E,
'H in D are assumed to satisfy classical Mmmell's
equations. Submitted 14 Mar 90 by Acad S. L.
Sobolev.
PA 160T88
T.
Z'
Stb&6'i6I`- i linear
t Of
wpeouol~?'. U' d-f-on
I ar
ution - of" tion,
.i i" 11tv+S' "dt e inte
or xi, *:,: ,!."
-i- ~ ~, - .41,
MIA iiisd
. d k6tia..
o4no
"ich are
th PIP 9"-
Tj
d' -
econ itions
A: of ite
~Oib~lexn con-
r, er, bdup
Ik~~,q [C
I ere
3, ~'jrj 8 545, (1945),
A,irv4s* tidhs iNhich, perm it::;
CV, or e wn
*e
6ons, emoyh'
js
77
USSR/Mathematics - Integrals May/.Tun 51
"Higher-Order Integrals of the Cons ervation-Laws
Typo For Linear Hyperbolic Problems," D. M. Volkov
"Iz Ak Nauk SSSR, Ser Matemat" Vol XV, %0 3,
PP 255-278
Seeks integrals similar to classical integral of
energy not contg higher de.rivs of unknown func-
tions of the hyperbolic linear boundary-value
problem. Writes out integrals of the 2d order in
3 classical boundary-value problems for vave eq
vhich contains frequently encountered boundary
conditions. Gives nethod for constructing pos
186T5
USSR/Mathematics - Integrals (Contd) May/Jun 51
definite integral of the Nth order. Write* !rA%-A i -
vidual higher-order integrals for certain hyper-
bolic systems, particularly Maxwell's eqs in the
case of complete reflexion of electromagnetic
vaves from metal surface limiting region of propa-
gation. Describes integral E2 vhich is independent
const of the electromagnetic fld relative to
classical integral of energy El. Cf. Courant and
Hilbert, "Methods of Mathematical Physics," 1945;
Frank and Mises, "Differential and Integral Equa-
tions of Mathematical Physics," 1937. Submitted
by Acad S. L. Sobolev 16 Nov 49.
186T52-
D
j"i
otkov D. M. A second inte iKrVing a new conservation
11
"
Methl3matioal Reviews
; 1~
aw 0
reffe.
aw ore ec owaggetic Ycstniklte-ninzrad. Univ.
r
1
Val. 14 No. 11
'
1952, nd -2 -42-43 (IYYZT.- (Russian)
1952 'no
_'A;
Doc. 1955 For a field active inside an empty finite region D, bounded
or afi d c1
~
7~
Physics
Mathematical
. _ __
by a metallic surface S, the author gives the time-con-
stancy of
P-.-f f f
D J4 1-t
-ff(IEI'EP"+F_-H"_Pkj*jP dS~
Here, in the space-,integral, Ilik, Ej* are the space-deriva-
tives of tLe field components; in the surface-integral the x,
are I~cal coordinates with xs* the normal, xs* =P (xl*, xj*)
the Ibcal equation of S, and *111 the corresponding field
e-
components. A proof is sketched. E, is stated to be ind
pendent of the energy, and to measure the excitation of the
field. Theie are said to be other such results involjving
higher deriVatives. F. V. Alkinson (lbadan). ,t
I.' VOT'KOv: 1).'
-IL, GITITZIFURG, I. P.
2. ussR (600)
4. Hydraulics
7- Calculatin~, the hydraulic impact in pipes of varying cross sections,
Vest. Leri. un. 7 No. 6, 1952-.
9 Monthly List of Russian Accessions, Library of Congress, May -19G3. Unclassified.
VOLROV.0 D. M. f Y /11 AAA
Mathematical Roviews
Vol. 15 NO- 1
Jan. 1954
Analysis
/VolkovD,.JML On exact solutions of a class of hyperbolic
--~-~tzo~ns having application in the theory of hydrialici-
shock. Doklady Akad. Nauk SSSR (N.S.) 90, 49-501i
(1953). (Russian)
Certain problems of hydraulic shock in tubes of variable
cross-section lead to the equation
At au au
_=Bq+'?) +
at
By a separation of variables of the type E.g. (t+,7)d'.pW1deV
certain exact solutions of the above equation can be
obtained. Al. 11. Proller (Berkeley, Calif.).
VOLKOV, Daniil Mikarlyevich; TSA:"l'KOVA, Z.1.1 red.
fDil'ferential- equations ant' t-hc---r app--Ifcation in n~-,-,iral
science] Differen-~siall-yf, .-I -Lkh p-211oznanlia
v astestvomanii. Loningrad, lzd-vo Lening-r. Univ.
Pt.2., 1964. 155 P. (MIRA 1-8:2)
VOLKOV, Dani-il Mak 'ye3dah- TSARtKOVA, Z.I., red.; ZHUIKOVA, Ye.G.,
red.
[Differential equations and their application in natural Sci-
onco] DifferentsiallrWo uravneniia i ikh prilozheniia v
estest'vomanii. Leningrad# Izd-vo Leningr. univ;j 1961. 132 p.
(Differential ecuations) MIRA 15:3)
VOLKOV9. D.M.-
Solving static problems in the theory of elasticity and other poly-
harmonic problems by the- method of infinite algeb:~aic systems. Tz-ady
LTI no 5096-10 159. (MM 14:3)
Waiticity)
(Harmonic analysis)
A
VOLKavpMj-triy-FaYloxjch. dok'Llor tekbn. nauk, pr~:f.7 RYAKHIN,
V.A., kand. tekhn. nauk, retsenzen',-
[Dynamics and strength of bucket ex~-avators] Dinami-ka i
prochnost' odnokovsho-rjkh ek.9ka-vatoro-7. Moskva, Mashiy.o-
stroenie, 1965. 462 p. (MIRA l8tll)
-__TOIXQV.__~,_P,"oktor tekhn.nauk
Outlood for -the development of earthmoving machinery. Stroi. I
dor. maohine-br. 5 no.8:5-8 Ag 160. (MIRA 13:8)
(Barthmoving machinery)
-VOLYLOV, D.P.; CHANGLI, I.I., inzh., kand.ekonom.nauk, red.; IVANOV, V.S..
.-I.--- - .inzh., retsenzent; DANILOV, L.N., red.izd-va; SMIRNOVA, G.V.,
takhn.red.
[Earthmoving machinery] Mashiny dlia zemlianykh rabot. Red.I.I.
Changli. Moskva, Gos.nauchno-tekhn.izd-vo mashinostroit.lit-ry.
1960. ill p. (9IRA 13:7)
(Barthmoving machinery)
PHASE I BOOK EMPLOITATION SOV/4167
Volkovz D.
Mashiny dlya zemlyanykh rabot (Earthwork Machinery) Moscow,
Mashgiz, 1960. 111 p. (Serles: Sovetskoye ma8hinostroyeniye
v 1959-1965 g.g.) 2,000 copiets printed.
Ed. of Series: I. I. Changli, Candidate of Economics, Engineer;
Reviewer: V. S. ivanov; Ed. of Publishing House: L. N.
Danilov; Tech. Ed..- G. V. SmIrnova; Managing Ed. for
Literature on General Technioal and Transport Mach."Me
Building: A. P. Kozlov, Engineer.
PURPOSE: This booklet Is Intended for technical personnel
engaged In desIgnIng,building and operating machinery for
mechanized earthwork.
COVERAGE: The author discusses the present state of basic
types of machinery for mechanized earthwork and the
prospects for the development of this machinery during
the current seven-year plan. He describes the single-
bucket general purpose excavator-cranes, multibucket
Card 112
Earthwork Machinery
SOV/4167
treneb-excavators, special shovels for stripping and
quarrying and walking dragline excavators. The author
also considers rotary-type excavators, continuous-action
automated equipment for open pit mining, scrapers, bull-
dozers and ground-compacting machinery. There are no
personalities mentioned. No bibliography or references
are attached.
TABLE OF CONTENTS-.
Introduction
Excavators
Earth-Excavating and-Moving Machines
Ground-CompactIng Machines
Earth-Transporting Equipment
Conclusion
AVAILABLE: Library of Congress
Card 2/2
7
93
10_3
log
ill
Vx/wro/ec
10-17-60
VASILIYEV, V.G., kand.tekhn.nauk; VOLKOV.,D.P.,-doktor tekhn.nauk
.-I - ---- -
Using electronic models in investigating excavators. Stroi. i dDr.
miashinootr. 4 no-3:6-9 Mr '59. (MIRA 12:4)
(Excavating machinery-Testing)
(Engineering modela)
VOLYLOV, D.P., doktor takhn. nauk.
Some results and prospects for the development of the excavator
industr7. Stroi. i dor. manhinootr. 4 no.1;20-15 Ja 159.
(MIR.k 12: 1)
(Excavating mzkchinery)
TOLKOV. Dmit MLOV-ic-h.; POLKOVNIKOV. V.S.. kand. tekhm. nauk, reteenzent,;
-Mxi
BYET, A.S., inzh., rod.; SOKOLOVA, T.F., takhn. red.
[Dynamic looda in universal excavating cranes; testing and
principles of designing] Pinsmicheskie nagruzki v univereal'afth
eko1mvetorakh-kranakh; issledovaniia I oBnovy rasebsta. Moskva,
Gos. nauchno-tekhn. izd-vo mashinostroit. lit-ry, 1958. 267 p.
(MIRA 11:11)
(Rxcavating machinery)
Iqw1a '701-KOV, D. F.
Dissertation Dynamic loads of basic units o."' single-
iactor e;~cavatorsj investigations and
princiules of design
Degree Doe Tech Sci
C,
Defended At Min Higher 12.ducation USSR., Moscow Order
of Labor Red Banner Consti-action
73ngineering Inst imeni V. V. Kuybyshev
Publication Date, Place 1956, Moscow
Source Knizhnaya Letopis' 'No 5, 1957
VOLKOV, D.P., Imnd. tekhn. nauk.
Basic results of studYing dynamic loads in universal ez-,wrating r,-raneu.
[Izd.] LOITITOMASH 43:5~-11 157. (MIRA 11:6)
(Excavatiiig machinery)
volicov 9. D.P.. kandidat tekhnicheskikh nauk; VASIL'C 0. V.A.. inzhener.
.Inve-stigating disk friction_flywheel clutches. [Trudy] VNIIStroi-
dormash no.15:42-62 '57. (KISA io.-6)
(Clutches (Machinery))
opo,.,kandidat tekhnicheskikh Pauk; BULANOV, A.A., inzhener.
04"VOL"Ov. DOU42
I mml-IrIm
7riction and wear' teats of friction linings in excavator clutches.
[Trudy] VNIIStroldormash no.15,-63-72 #57. (KLRA io:6)
(Clutches (Machinery)--Testing)
VOLKOV, D. P. (DOGENT)
VOLKOV, D. P. ( DWENT) -- "Outline of t,he 111!Ao17 ot' tho Devolopmont In tho 19th
Century of the Course of Complex Projecti~-,ns in Russia." Sul 11 Mar `2, Moscow
Order of Labor Red Banner En;rineering Construc+ion Inst imeni V. V. Kuybyshev
(Dissertation for the Degree of Candidate in Technical Sciences.)
'~'O: VEMMIAYA MCSF. A, January-December 1952
VOLKOV, D.P., doktor tekhn. nauk; NIKOLAYEV, S.N., inzh.
Dynimic-oads and the longevity of rotary trench excavatorE. Stroi.
i dor. ma'sh. 9 no-4:33-36 Ap 164. 0 18: 1)
VOLKOV, D. P.
"Study of Dynammic Phenomena Daring the T~imning of -Excavating Cranmea.3 Sub 6
Mar 5 1, YIOBCOW Order of the Labor Red Banner Coastruction Rngineering Inst imeni
V. V. Kuyb,,shev
Dissertations presented for science and engineering degrees In Moscow during 1951.
6u: t5um. ft. 4b0, 9 MaY 55
RUROV, A.S., inzhener, laureat Stalinskay premii; VOLKOV. D.P., kandidat
tekhnicbaskikh nauk.
New type friction cl7atch for excavators. Mekh.stroi. 11 no.5:16-20 My '54.
(MLRA 7:5)
(Bxcavators) (Clutches (Kachinery))
VOL J r-o
VSSR/Kiscellan6otis Excavatora, Design.
Card 1/1 t Pub. 70 - 3/9
Authors I Volkov, D. P., Gand. of Techn. So.
Title: S Problems of reducing the weight and improving the quality of
eXCavators
Periodical IMekh. stroi. 3, 11-16, March-1954
AbstrOAt IThe problems involved in reducing 'the frame and chassis weights of
F,505 and F,255 single-bucket crane-excavator c-cmbinations are discussed.
In order to obtain conclusive data regarding the proper weight re-
(~htction of excavatcro and improvement of their quality, special d3mamic
Wid static load.tests were conducted by the Enitineering-Con8truction
:11istitute in Moscow, and the results are desar-lbed. Tables; graph;
cb!awings; illustrations.
Institution
Submitted
-VOIKOV, D.P... RANNEV, AN.
Strains and StraBses
Experimental testing of actual stresses and strains in structural components of
excavators. Melch. stroi. 9 no. 4, 1952.
2
9. Monthl List of Russian Accessions, Library of Congress, July 195~, Uncl.
I - --youoy, -D.-P., RANNEV, A. V.
ExcavatIng MachInery
Experimental te:3ting of actual stresses and strains in structural components of
excavators. Melch. stroi. 9 no. 4 152.
2
9. Monthly fist ~)f Russian Accessions, Library of Congress, July -1951, Uncl.
t- -.- , . - " - K~,. ... ~ lll-~.'~..--
- ' - - ----
Vo~-Kov.,,---D prof. doktor tekhn.nauk; CHERKASOV, V.A., inzh.
Study of the dynamics of waste stackers. Gor.zhur. no.4:511-54
Ap 64. W RA 17:4)
t
1. Moskovskiy inzhenerno-stroitellnyy institut imeni Kuybyaheva.
VOLKOV., D.P., doktor tekhnonauk
Construction of excavators in the capital-istist countries. Stroib
i dor. mash. 7 no*7:36-39 JI 162. (MA 15:7)
(Excavating machinery)
1. VOLKOV, D. P.': RANNEV, A. V-p Dig.
2. UWR (600)
4. Excavating Machinery
7. Study of the work of an excavator equipped witli a reversible shovel.
Mckh. strol. 9 No. 9j, 1952-
9. Monthly List of Russian Accessions, Library of Congress, January -1953. Unclassified
VOLKOV, D.P., kandidat tekhnicheskikh nauk; BORISOV, S.M., inzhener.
Directives of the 20th congress of the Commmist Part7 of the
Soviet Union concerning the sixth five-Tear plan of economic
devolopment of the U.S.S.R. and the tanks it assigns to us.
Stroi. i dor.mashinost. 1 no.3 Mr 156o (MLPIA 10:1)
(Clutches (Machinery))
V(-)Li'-OV, b.e. kandidat tekbnichei3kIkb nauk.
-------
Effect of de3ign on dynamic loads in univer&al excavators.
Strol. 4. dor. mehl-nostif. 2 no.5.4--8 MY 157. (W.RA IG:(,)
(ExcavatizLe machinery)
. . II .--1. - . I
. ~ ---
VOLKOV, D.P., kandidat tekhnichaskikh nailk.
~Ici
Potentials for reducing the weight and. improving the quality
of excavators. Makh.stroi.11 no-3:11-15 )Ir '54. WaA 7:2)
(Excavating machinery)
VOLKOV, D. P., doktor tekhn. nauk
Study of the operatirm of an EVG--15 stripping excavator wl-th,--t
a reducing gear on the drive of the hoisting mechanism,, Sloor,
trud. MISI no.39.-364-365 161. (MIRA :16-.4)
L. Moskovskiy inzhenerno-stroitellnyy institut imeni V. V.
Kuybysheva.
(Excavating machinery-Falectric driving)
RANNEV, A.V., kand. Lijklin. rinuk; PANKHASHUN, I%V., kand. t-tikiin.
nt.-~uk; VASITLICIENKO, V.A., inzh.; V(-ILKOV, D.T., 'Joktor
t~lkhn. naW,, prof., retsenzent
[Drive mechanism_- or all-purpose excavatoi-3 wid Lhei:,
tE.Istingj Fr-.ivoc,-j universallrrjkh ekskaiatorwv V-h i-p-,
taniia. Vlo-.izva, MashinosLcoanle, 1964. 29.1
Air
240V D..S.,, kand.t.ekhn.nauk
Imeetigating Morganto floor-type charging machine. Stall
21 no.8:700-701 Ag 161, (MIRA 14:9)
1. Zaporozhskiy mashinostroitelinyy institut.
(Open-hearth furnaces-Equipment and supplies)
KOLKOV, D.S., kand.tekha.nauk
Improving the perfornance of belt conveyers in sintering plants.
Stall 21 no. 1:20 Ja 161. (m MA 14: 1)
1. Zaporozhakiy mashinastroitelinyy institut.
(Conveying machinery) (Sintering)
aricu:,
~zs
-AUTHORSt A Aleksin, V;Fi, Volkov, D.Y., 56-4-33/54
TITLE: Radiation Correction to the Scattering of Particles in the
External Magnetic Pield and to the Compton Effect in the
Scalar Quantum Electrodynamics (Radiatsionn)yepopravki k ras-
seyaniyu chastitsy vo vneshnem pole i k Kompton - effektu v
?kalyarnoy kvantovoy elektrodinamike)
Letter to the Editor)
PERIODICALt Zhurnal Eksperim. i Teoret. Fiziki, 1957, Vol- 33, ITr 4,
PP- 1044 - 1045 (USSR)
ABSTRACTt The expression for the one-photon mass operator of a scalar
particle is used to calculate as well the radiation correction
to the scattering of scalar particles in the ecternal magnetic
field as to calculate the Compton effect. 1.) The differential
scattering cross section in Born's approximation has the form:
do-/dO - (do-/dg) a + (d 6'/d!2 )6 M + (d C-/d Q ) A,
where d6 /d-P ) is the differential scattering cross section
without the tak?ng into account of the radiation correction.
A M, A' are the radiation corrections which belong to the
,ard 1/2
56-4-33/54
Radiation Correction to the Scattering of Particles in the External Magnetic
Field and tot the Compton Effect in the Scalar Quantum Electro-
dynamics
mass operator and the polarization of the vacuum reapectively.
The corresponding expressions for these two corrections are
derived. 2.) For the Compton effect d&'/d Q has the formi
cl~-/dQ - (M,/m) 2 (C~20/q-10)2 U, where
d/,Q - in the solid angle element in the direction of photon
scattering and q1O/ q 20 - the energy of the inciding and
the scattered photons. For U the corresponding equations are
derived. There is 1 Slavic reference.
ASSOCIATION: Physico-Technical Institute AN Ukrainian SSR
(Fiziko-tekhnicheskiy institut 1~kademii nauk Ukrainskoy SSR)
SUBUITTED: may 19, 1957
AVAILABLEt Library of Congress
Card 2/2
C, h:r;,-, rith c 1 If
.-.,,LjjntIjm
tol
bf 3, nnor
(I.-in of "Iduc,'.tion
st - le U im Gorlidy) 100 Go-nies- cnu a,
(10 tit-IC.E) Ina)
- ---- - -- -- ... , .'w
- , -
VOLKOV, D.V.; ORAYEVSKIY, V.M. [Oraievslkyit V.M.1
Role of the form factor in 51-0 -.* g -~- et -j- e- decay. U-L=.fiz.
zhur. 4 no.6:804,-806 1-~-D 159. OMA 14: 10)
1. F:Lziko--'%-,ekhnicheskiy institut AN USSR.
(Mesons--Decay)
24(5)
AUTHOR: Volkov, D. V. BOV56-36-5-42/76
TITLE: On the Quantization of Fields With Half-integral Spin Fields
CO kvantovanii poley s polutselym spinom),
PERIODICAL: Zhurnal ekspt:rimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, Nr 5, pp 1560-1566 (USSR)
ABSTRACT: In the present paper the author, on the basis of the simple
example of the Dirac equation, investigates the possibility of
constructing an algebra of.operator wave functions which leads to
an unusual statistics with maximum occupation number (two for each
individual state), and, connected herewith, to a statistics with
relativistic causality principle, positivenese of energy (for the
free non-intefacting field), and with Lagrangian formalism. For the
purpo3e of formulating the latter, the author operated with
Schwinger's principle (Ref 1). It is shown that the quantization
scheme concerned is a consequence of Schwinger's variation principle
First, the conditions of relativistic causality are discif"ed and
formulated mathematically. In the following, a foxnulation of the
field operator algebra is given in momentum representation and the
properties and mutual relations of the introduced operators are
Card 1/,# discussed. As a concrete example, the expressions for the energy-,
W'M~=' _tir'-zm- _;~a
On the Quantization of Fields With Half-integral Spin Fields 307/56-36-5-42/76
momentum-, and charge operators of a free Dirac field, which are
antisymmetric with respect to the operators of the wave function,
are written down; the latter are also explicitly written down in
momentum representation; for the commutators of these operators
(E,?,Q) the relations are also given. In the following it is
further shown that the half-integral spin wave field quantization
scheme investigated by the author is not only consistent with the
principle of relativistic causality, the positiveness of energy,
and with the Lagrangian formalism in Schwinger"s formulation, but
that it is also invariant with respect to CPT -transformations.
This invariance in the caee of fields with half-integral spin is
a consequence of the antisymmeirization of the equations of motion
with respect to the operator wave function. The author finally
thanks A. 1. Akhiyezer, Ye. V. Inopin, I. M. ldfohits, S. V.
Peletminakiy and P. 1. Fomin for discussing the results obtained
by this investigation. There are 5 referencon, 4 of which are Soviet
ASSOCIATION: Piziko-tekhnicheskiy institut Akademii nauk Ukrainskoy SSR
(Physico-technical Institute of the Academy of Sciences,
Ukrainskaya, SSR)
Card 2/3
24(5) SOV/56-37-1-27/64
Peletminskiyp
AUTRORS Volkov _.D,,,,X S. V.
TITLE: On the Lagrangian Formalism for Spin Variables (0 lagranzhavom
formalizme dlya spinovykh peremennykh)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 37, Nr 10), PP 170-178 (USSR)
ABSTRACT: In the present paper, it is shown that the olasa limitations
of admissible variations postulated by 1. Schwinger (Ref 1)
are not necessary. A change of the class of admissible varia-
tions permits the introduction of spin variables (for any
spin value) into the general scheme of Schwinger's variation
principle, both in the non-relativistic and in the relativis-
tic case. The Lagrangian formalism for the spin variables
leads in the relativistic case to a natural introduction of
the-proper time into theory. In the non-relativ.~stic case2
the spin variables are described by thb vector s
The equ&tions of motion and the operator properties of the
vector a are determined on the basis of the application of
Qor form to the Lagrangian
the action principle written in opera,
function -H(e) denotes any-function
L H(s
Card 1/3 2 I-S
On'the Lagrangian Formalism for Spin Variables SOV56-37-1-27/64
-OP
of a which agrees with the Hamiltonian func4ion of the
system, 7k the derivation of the operator a with respect to
time in Heisenberg's representation. The square brackets
denote the commutator. The first summand in the above for
mula corresponds to the kinematic part of the Lagrangian
function* The cou4se of the calculation is followed step by
step. The vector s really describes, according -to these
calculations, the spin degrees of freedom of the particle.
The authors then show that the principle of steady action
t2 -0 241 1 -
f filb 89 s 6Hj dt = 0 is really satisfied in the class
t
of admissible variations discussed here. The results of the
first part show the following: The data on the equat.~ons of
motion and on the operator properties of the vector a, which
were determined on the basis of application of the operator-
like action principle to the above-mentioned-Ligrangian func-
tion are in internal agreement and describe cor-rerally the
properties of the spin variables. The second part describes
Card 2/3 the introduction of spin variables into the scheme of the
-On the Lagrangian Formalism for Spin Variables SOV/56-37-1-27/64
Lagrangian formalism in the relativistic case, The four-
dimensional vector T, is investigated as a natural re-
lativistic generalization of the spin vector a. The four-
dimensional vectors of the coordinate and of the momentum
are denoted x A and p The Lagrangian function is written
down in the form t T T2;gl - i (fX4'Q-K'PVP-0Y
4
Ix denoting a certain function of 'r 91 X11 9 Pg . Finally, the
equotions of motion and the exchange relations are written
down. The authors thank A. I. Akhiyezer and P. I. Fomin for
useful discussions. There are 11 references, 9 of which are
Soviet.
ASSOCIATION: Fiziko-tekhnicheskiy institut Akademii nauk Ukrainskoy SSR
(Physical-technical Institute of the Academy of Sciences
of the Ukrainskaya SSR)
SUBMITTED: January 29, 1959
Card 3/3
V
1-5-0 0
AUTHOR: Volkov, D. V.
3/056 601S*021301061
Boc6 Boli
TITLE: S-Matrix in the Generalized Quantization Method
PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fiziki, 1960,
Vol. 38, No. 2, PP- 518 - 523
TEXT: Green (Ref. 1) and later the author of the present paper (Ref. 2)
had already carried out a generalization of the wave field quantization
methods, at the same time taking into account symmetric and antisymmetric
wave functions within the framework of the relativistic quantum theory.
Those investigations, however, did not consider problems related with
interaction. This very interaction between the fields might help to
solve the problem as to which of the existing quantization methods is to
be preferred. In the paper under review the author investigates the for-
malism*of scattering matrix for intarantiQng agn am electromaxMeticl\
field and tae field of charged spin-1/2 particleWthe 3-matrix is set up
in the form S - T(exp(-i IH(x)d4x)), where H(x) Gnotes the density
Hamiltonian in interaction representation H(X) . ie[f(x), I,,+ (x)] A,(x),
Card 1/3
820?4
S-Matrix in'the Generalized Quantization S/056/60/038/02/30/061
Method B006/BO11
~(x), and T(x) - f".(x)V4 are the operators of the particle field obey-
ing the Dirac equation (without interaction)* Particle field quantiza-
tion occurs on the basis of modified commitation relations given by for-
mula (3). A (z) are the operators of the electromagnetic field, sub-
jected to the common commutation laws. It is shown that in spite of the
change in quantization rules, there exists a clear procedure of series
expansion of the S-matrix with respect to normal derivatives (similar
to the ordinary technique by Wicki,"Ref. 8), which permits the separa-
tion of vacuum effects in the 3-matrix. The basic concepts of the con-
ventional S-matrix theory (N7Product, Wickto theorem, Feynman graphs)
permit a simple generalization within the framework of the quantization
scheme considered. The results obtained can be applied without major
changes to other local variants of field interaction as well. They are
applIed, foz example, to the process of the scattering of two particles
characterized by apin and momentum. The author finally thanks
A. I* Akhiyezer, S. V. Feletminakiy, and P. I. Fomin for their discus-
sions. There are 8 references: 4 Soviet, 3 American, and I German.
Card 2/3
S-Matrix in the Generalized Quantization S/056/00J04'62/30/061
Method B006/B011
ASSOCIATION: Fiziko-tekhnicheakiy institut kkademii nauk Ukrainakoy Ssh
(Institute of Physics and Technoloffx of the Academy of
Sciences of the Ukraa-aya-ya SSR)
SUBMITTED: August 10, 1959
Card 313
85684
4-,570 0 6/3070
AUTHORS: Vclkov, D, V.j Inopin.. Ye. V.
TITLE. Motion of Nucleonjkn an Anisot-ropic Oscillator Fctentlial
Taking Into- Account Spin-Orbit Interaction
PERIODICAL. Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 38, No.. 6, pp~ 1765-1770
TEXT: A method is proposed for the calculation of the wave functions eand
level energies of nucleons moving in an oscillator potential. This problem
appears in treating the bound state of individual nucleons according to
the generalized model (where it wag solved by Nilsson), and is of
particular interest for deformed nucloi, as was sh(,,wr. by A. S. Davydov
et al. and B. T. Geylikman. The method proposed in the present paper is
suitable for calculating the wa-e functions and eigen-alues of nucleon
energies in non-axial. nuclei. It is mentioned in the introduction that
this method differs from that of Nilsson in important respects, and this
difference is discussed. The present method is Is-,zed on the smallness of
Card 1/4
8_568h
- f601'038/006-1 026" 010'* Xx
Motion of Nucleons in an Anisc"ropic S 050'/
Oscillator Potential Taking Into Account B006/BO70
Spin-Orbit Interaction
the spin-orbit coupling constant (X~0-05)., In the representation cf the
anisotropic oscillator., the spin-or~,it coupling is diagonalized when terms
only up to the order of x_2 are considered. Taking into account the spin-
orbit coupling, the Hamiltonian describing the motion of the nuGleons in
the nuclear field has -.he form;
-4. - V2
H = H + As grad [V(r),.'j ; Ho /2 V(r4). (N , coupling constaaf
0 P
M = 1; M nucleon mass); V('r)
Taking x a a
k k k
and 2
t a !a4 -t ror
Pk k'k _' 'ik). where [a Ij .a 0 holds
2 k'al ~kl' Lk~ 1,
+' he form
the operators ak and ak the Hamiltonian take5
H (a a+ + a + a. f -a fa- /2; 0 are Paul i
2 ik-L kl k i
matrices) in the approximation made here; addends ~,ontair~ing terms of the
Card 2/4
~~ ~~. ~i
W
Motio~a -of- Nucleons in an Anisotropic S/05 60/03-S/0G6/02G/CL-1iXX
0sciliator Potential Taking Into Account B006Y5070
Spin-,Orbit Interaction
+ +
t.ype a a -a a can be neSlected. It is shown in the folloy.-in& that the
1 1 k 1 k
prob1lem. can be reduced to a simple analytical solution in the limiting care
of a otrong deformation of the nucleus. Since the spin-orbit coupling
makes'! a. contribution of the order of )r2, the case of a strongly non-
spherical nucleus wit'h large non-axiality cannot be considered. In-the
case,of a strongly non-spherical nucleus with arbitrary non-axiality, the
are non-diagonal with respect to n. are negligible, and after
a can!onical transfor~iatlon, the Hamiltonian takes the form:
1 2 ____ 2
H A;(N, n Y + *7 10 0 + (2 (a+'a' - 2~_V). Fig. 1 shows -the nuclear
z X x y Y
energ.'y as a function of non-axiality: a -.oscillator without spin-orbit
coupll,ing; b - real oscillator. The non-physical region,is shaded. Broken-.
.lines'
- show the case when a small perturbation of the nucleus displaces
the (~'nergy minimum..From the curves it can be concluded that the spin-
orbit?,*coupling stabilizes the axial nuclear form against the influence of
small; perturbations. G. Ya. L-yubarskiy is thanked for discussions. There
Card
3/4
Motiop of Nucleons in an Anisotropic
OscilAator Potential Taking Into Account
Spin-~,Orbit interaction
are figures and 3 references: 2 Soviet
ASSOd.IATION:
8568h
S/056/60/038/006/026/049/XX
B006/BO70
and 1 Danish.
Fiziko-tekhniplieskiy institut Akademii nauk Ukrainskoy SSR
(Institute o:e Physics and Technology of the- Academy of
Sciences Ukrainskaya SSR)
SUBMITTED - December 21, 10,59
if
a ex 0
Card -4/4
Pic
J:)
B 10 4/31 C, 2
ATI-WR: vol,kov, D. V.
T I T 7, E, Caulamb e-r-itat'or, of -carticles
7
PERIOIJICA~ Zhurn,11 ek3rierimentallnoY 4. teoret4lcheskoy 'I-74k;, V, 4.1
.62, 1112-111'
no. 30) . 1~
TEXT: I th a. sbeen sho-xn -.nat at *---,-"-, enerEies an _7 su f f i Ce
small scatterinC_ angles the contr-butior, of the Coulomb poles to "'-e
am:,Iitu,,Je of t2he reac-I.-ion A + X exceeds t--- contribu-clon ~D~L
stron-7 int~,rac';on ZI-7-TIF, 40, 18"4,' 1961;
-, r C, k~ I - - , C
. 1*11. Shm~i.7hkevich, Nuci. Phys. 273, 152, 1961). The -lifetime , -
L th-
hyperons can t-hezefore be from Coulci.-ib interact.4cn. A t 1 C, V.-
C, n Z. rE i e s, t, h e m, o s t c- ILi c an 1. c,- nt r i b u'_ -; c n t o t h e am 141 t 1i d e o f tn 1- S
redetion will be from 13'i~rorE_ inLeractions and from interference olC ti-.e
strong interactions with the eleotromagnetic interactions. 7hese two
mechanisms can be separatf-d because cf the c.-Iaracteristic de-,_en~:`encr__ Of
~I I ction on the variables of isotopic spin. 4'h~-re two nucle_',
stront-lintera
belong1to one isotopic doublet, the -,atrix -lements of strolls,- Jnt~2raGt`r,
,%.,a-L,d 1/3
or. of ...
C..-
-L
c
2nd e-,end ent of the I i s o tko7cic
s c t t
10""er cc~U'Omo ~Xcj' r 0 0 r" L
the Taze-
t 'ua n- (1, a
:itiOrl al'ld Ol Ul. ec o. 3 .. - -
to be
ero-r, E: 4 S
above the up.,er of p
02 4. 0
dOKY.1 --- Z-2
(ol fj2)2
4
E:17~ n-.
0 r, wh a "'3
S, ror,:-
:rcm th~- ~r;tr-i x a 7 e n 41-- - : - -x
c,.~rntr`butions of nt ~' C Jvl. r. c e,
i '12 i-~; i'ollo-as that stronz- ~--ract:- c---
each cther out if the respective Paftic!Os --a:e i'l equal- st~ites-
/7
Card -, I
.0 U 10 r.-"rj a t I o
SUB;,! TT T---D:
31 102
t ek'-lr. i ch e s k - y j r,_,z tt.- A!, ad ez: 1 -1 n auk Sc- F, R s 1, cc -
4 e
'I--Stitutt~ Of the Act-~dom~y 041 Sciences -USS~R)
june io62
Card 5/3
L 17622-63 BW(J)/E7dr(m)/BDS AFFTC/ASD/IJP(C) JF4
S/056/63/044/003/040/053
AUTHOR: Volkov, V. and gribov, V. N.
..-TITLEv Rejrg2 polearin nucleon-nu%leon and nucleon-antinucleon
scattering amplitudes /7
PERIODICAL: Zhurnal elwparimentalinoy i tekhnicheskoy fiziki, V. 44, no- 3,
1963, 1 o68-1077
_UXTs The letter by V. 11. Gribov and I. Ya. Pomeranchuk (Rof'o 8: Phys. Rev.
Let~.,,8 412, 1962) discussed in detail the spin structure of th nucleon-nucloon
a
aIcattering amplitude due to the main (romoranc~uk) vacuum Dole. The present paper
investiptes the spin.struoture and the charactor of the kinematic features o~ ihe
Icontributions.to the nucleon-nucleon and nucleon-antinucleon scattering amplitude
from Regge poles with various quantum numbers. The,authors study the
classification of poles, the partial waves amplitudo decomposition,and tho
contributions to the amplitude by the scatt,ering from polos of different quantum
'numbei. It is shown that the presence of kinemstic singularities at t 0 in the
-Card--l /2- -
.-L,17622-63. 5/0%/63/044/003/040/Q53
Rogge poles...
-rom certain Regge poles together with the requirement of analyticity
contributions
the whole amplitude leads to the SDnearance at t - 0 Of Simple relations between
:-.'tha positions of the Rogge poles belonging to different trajectories. The
dependence ofthe forward acsttaring amplitude on the character of the relations
thus obtained is discussed. There is 1 table.-
r-iziko-tekh-nicheskiy institut im. A. F. loffe Akademii nauk SSSR
(Physico-Tachnical Institute im. A. F. Ioffe of the AS USSR)
SUBI-MTTED: October 24,, -1962
~Card 2/2
VOLKOV., D.V.
Factorization of scattering amplitudes of particles with spins
in a Regge pole. Zhur. eksp. i teor. fiz. 45 no.3:742-745 S 163.
(MM 16:10)
(Scattering (Physics)) (Nuclear spin)
L 58520-6,2 EWT k'm)/T/E7h A (m) -2
ACCESSION KR: A?50162TT UP/0336/65/001/C05/0009/0012
AUTHOR: ;ZQ14at~D. V.
TITLN- SWO) x S190) aynnetry and the bar7on-meson couplindlonstants
SOURCE: Zhurnal eksperimente-l'noy I teareticheakay Miki. Pis'= Y redaXtaiyu.
Prilo-zheniye, v. 1, no. 1, 1965, 9-12
14.
TOPIC TAGSt symmetr7 property, baryon meson coupling, coupling constanti3, broken
symmetry, iwmrimace
AWq_1WTr The author considers the relation between the coupling comitants of a
unitary oetet of tm-iryone witb octets of paeu4oscalar and singlet vector mevonB. The
analysis is bs.aed on the ~~srrm-ptlon thAr the breaking of the EU(6) srime-rry for a
vertex functlar, vtth threA ~-)merna-' i-,nes hai a r'~'neivaatic natuxe and .a lue. t~) the
preaence of two iade-i)endent enezrg~- ---Omen' un veators :-n Licu :)0' one,
as Is the care fo!- the self-energy of tne par-i~iclee when s-L~61 dquareti--y is satis-
fied. The rsq%iirment that thc con," guTat"Aon of the system 4-momerita be Irrva.;-iant
leada to the redu--tion )~ thr- 311f6 w?--~-, to ~ne grou-P SU(3) x SSTJCI~ X U, Whi!re
the two SU(3) groups correspond to unitary t ransformat ions cf quarkE tita dif ferent
polarization dire..-tions along a preferred axis, u131le the group U corresponds to
the usual spatial rotatians about this mxis. The 35- and 56-plet repreeentations
of the g-roup SU(6), correcponding to meson and baryon cupermultiplets, containg the
following irredueLble rel)resentations of the grouP SUO) X SU(3):
1/ 3
L 58520-65
ACCEBSION NRt Aj)5ol6zn
(35) - (3, 3*); (3*, 3); (8, 1); (1, 8); (1, 1)
(56) - (1, 10); (10, 1); (6, 3); (3, 6).
tit folicive from (L) that the vertex (56) (35), which is invaria,at against
'W(3) x SUO-4) traagformat ions, contains in the general ease eight independent
For vertices which do not contain th
par-' -y- conser-ring interaction constants e
1) (1, 10), (10, 1~, and (I.C. I wu-'I~iDl ets, which are clasnified az bazyon reson'-
amees because the spin h-se st---es in equa.1 to ~"2. the
th, tetw-en an~'- the mesons is chaxacteri:ed by four
conatam-ra in tho A- SU.,
invaxi&nce. Thr- fo]-Iow,~n~g q Valid for axbitra-r7 Na-1,,ed --)f
iZ
meson MaZG CIZId off the mcLss &7-~ Db-~aiaed for the coupling coneitajfts,
D 2 D F~
G G G (2'
ti 5
G-Y) (3;
Card e~j
L 565201-65
ACCESSION NR: AP50.i6277
GD -, GF 3 : 2 ! 1 (4)
M M M
The upper Index ref�rs here to the type of coupling (F or D) of the menon octet,
4ndqx determinf-s the character of the Interaction of the -rector
5; r 1~ M--m- n,~tl.- moment). 11h, e Lj e r e ' t~ o n 8
L ~
11, 299, !~b4) ',-r -~he coup-~~ -onstan's =4 when the coiiu
r _oin-_Ides with the anslogous cona~,-ant In the Dirac Y&.-4,&rt, i.e., vl~er the meson.
mass or a-1-1 -he conatents of the M~interaction &re equai to zero. When ~i there
is no C-interar--tior of the vector meson octed vith baryons at iLl-1- As a result,
some variants of the dynamic theory of strong irrteractions, e-re not SU(3) X SU(3)-
invaz-llant. An an&] agotis paradox concerning the inacmpatibbility of the minimal elec-
tromagnetic int-ra