SCIENTIFIC ABSTRACT IVANENKO, D. - IVANENKO, G.D.

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
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• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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Ivaneako, D. D.. and KurdgaWdra, b. P. The b-01i
dqia-Gons'df mesodTnainics. DtAJ-. Ak;ad Nauk &'-;-9R F/W
C')' P, '~ -~ 96 11) 42 , 19~4 Ru&si'hn ~
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USSR/ ?hysics - Lovement. equations
Card 1/1 Pub. 22 - 9AO
Authors 11vahenko, D., and Tsytov ch,, V.
Title tRelativisiLlc eauation of three-bound bodies
Periodical t Dok. 'AN SSSR 99/3, 373-376, Nov 21, 1954
Abstraot t Properties of the interreacting operatori are d6d 01ribed. ~';Ifhe operMl oris
were obtained in the process'of th.e-derivaLion of' a irovemept equoton
for three bodies in an electromaenatic field reactIng i~pon each ~ihsr
(only e3ectrom-agnetically for simplicity). The oiquaLion ii-as derivod by
a method bAsed on Oe calculus of variations which led to the convariance
of equation tensors which had, been discussed by Wit'zol. In the-pizosent
"n-
ftii 4-6 _erences~. $SkAnC4
or
Institution: Moscow StALe University 'K;%V~ 1omonodov:
Presented by: Academician A.A. Lebeddv, August 7s-1954

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1VAIR,OKO, D. D.
"In Memory of Albert Einstein" from Works of the Historical Inst. on Natural
Sciences and Engineering, Vol. 5, P- 3, 1955.

'Y 4-
USSR/Physicii - - lecr-roayaamICS
Card 1/1 Pub. 146-4/25
Author ; Tvanenko) D., and Tsytovich, V. N.
Title : Theory of the loss of energy of charged particles through a forromagnetib
Periodical : Zhur. eksp. i teor. fiz. 280 291-296, March 1955
Abstract : T11.0 authors investigate the effect of saturation of energy losses when
charged particles pass through ferromagnetics, an studied by D. Ivanenko
and V. S. Gurgenidze (DAN SSSR, 67, 997, 1949; Vestnik IOU, 2, 69, 1950)
and Ch. Weizaaecker (Arm. d. Phys., 17, 1933). They analyze the division
of the losses into ionizational and Cherenkov losses. Nineteen references;
e.g. V. 11. Tsytovich) Vestnik MGjU, 11) 27, 1951-
Institution: Moscow State University
Submitted ; March 5, 1954

UwR/Physies - %wieer structures
Cardl/1' Pub.-22 9/50
Authors l Ivansnko, D., and Koleenikov, N.
Titla Re-_ -regarding anuclear model
Periodical l DOK. AN SSSR 100/1, 37-40, Ian. 1, 1955
e
Abstract I Nuclear models (shall, liquid-dropi are disium C A w4dift d model of1the
nuclear structure is suggested in order to overocite accie difficulties in the
interpretation of observed nuclear phea=ena. heme ac~ihaetions 4mcaily
concerning weekly excited states of an atom) are as fol lawsi 1. nurleow
are moving indepeadently (the filling of energy levels sad shells 1.9
determined through a self adjusted potential of tht field and of the
nucleons); 2. the considerations of the liquid-4rop-collactive movome0e.
mainly. connected distortions of the wave functIon i eald 3* existence of
of's certain number of nuclear groups of theo( . ead bt-partlele types.
Seventeen referencess 7 USM . 8 USA. I Fremoh wW 1 Gemin (1932-14,153),
Graph.
Institution i The 14. V. Lomonosov Moacow State UnIversity
Prevented bys Academician A. A.LeUdav, Septembor 27, 19$4
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Category t USSR/Nuclear Physics - Elementary Particles C_~
Abs Jour i Ref Zhur - Fizikap No 3, 1957, No 5897
Author Dfllwww", Folesnikov, N.
Inst :-Ro-scow State University
Title i Binding Energy of Hypernuelei.
Orig Pub t Zhe oksperim. I teorfizikij 1956# 30, No 49 800-8.C.:l
Abstract The binding energy and the stability of hypern4olel in,in-
vestigated, An anslysis of the eiperiLaontel. dqtr available at
present time leeds to the conoluelon thats (a)~~he binding
energy BA_of n./I0O perticle in hypernuelei dotba no,%,,* depend
noticeabIfon the spin and on the isotopic spin of ~Uie, core,
comprising the nucleus minus theAJO particle, and increase
approximately linearly with incroasing mass number X;. (b) the
interaction betwoon the-A-0 particle and tho,nmoleoti N is some-
what weaker than the LYN interaction.
Based on tho assumption that adding thojvo jinrtic~le chvmgos
littla the core potontinl in thnt tho rrdii of thejN?-N forcov
are not greater them that of the NN forces, tho authors oxplain
Card z 1/2
------------ --

SUBJECT USSR / PHYSICS C~LIID I / 2 PA - 1456
AUTITOR lVMNETTKO, D. D. , KER11TOV, B. K.
TITLE A Two-Nucleon Potential of the Intermolecular Type and Nuclear
Saturation.
PERIODICAL ~urn.eksp.i teor.fis, 31, faso.1 105-112 (1956)
Issued: '9 / 1956 reviewed: 1; / 1956
The present work points out a possibility for explaining repulsion on the basis
of a seiniplienomenological interaction potential of the -type of the intermolecular
p
,otential of L MErj:TARD- JONES, which, apart from a YUKOA force of attraction, con-
tains the usual not exchangelike repulsive force. For reasons of simplioity the
spin terms are not investigated. Many experimental data concerning scattering
make it necessary that, apart from attractive forces at distances of r rcalso
repulsive forces at smaller distances of r < r c exist. A special rule is shown
the form of which is easily generalized (as for example by the addition of a
"repulsion term" to the "best" known potential of pseudoscalar meBodynamioa) and
which may explain the lack of a constriated (?) state in the nuolei. The pre-
liminary character of these deliberations must, however, never be forgotten.
In the case of r < r 0 only a strong repulsion ("hard core") is assumed to act.
If the interaction potential has a repulsive core, the wave function T of the
basic state of the nucleus is assumed with A particles in form of a point of
SLATER'S determinant and a symmetrical function of the spatial coordinates of
the A nucleons. Next, expressions for the average potential energy V of the

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SUBJECT USSR / PHYSICS *RD 1 / 2 PA - 1979
AUTHOR SOKOLOV,A.A., IVANENKO,D.D.9 TERNOV,I.M.
TITLE On the Excitatlon oT croscopie Oscillations by Quantumlike
Fluctuations.
PERIODICAL Dokl.Akad.Nauk 111, faso.2t 334-337 (1956)
Issued: I / 1~557-
The energy of a relativistic electron moving in a homogeneous magnetic field H
can be represented as the sum of the energy of the rotation movement E, of the
electron and the ene
_R~ ~r of the oscillation motion E a along the radius:
2 4' -h W d - E(0 2 2/2c 2. H
E 2eHcT1 + m a , Es - a ere n a 1 + s denotes the
principal quantum number, 1 - the azimuthal- and a - theradial quantum number,
a - the amplitude of the radial oscillations. Next, formulae for the modifioa-
tion of the rotation- and o9eillation energy on the oooaeion of the transition
of an electron from the state n.into the state nf.- n - V is given. The sum
of these two modifications results in the entire energy lose by radiation while
taking account, of quantumlike corrections with an accuracy of up to 1i .
The quantumlike corrections to the rotation movement can take effect only in
the case of high energies. With t 4 0 there is no modification of the energy
of the radial oscillations at all, i.e. in the classical case the value of a
remains constant even if radiation is taken into account. Only in the quantum-
like case ( t - 0) does one peculiar energy jump occur If rotation energy is
used not only for radiation but also for the excitation of radial oscillations

L I

GRIGORITAN. k.T.; IVANERK0. I.D.
"Histor7 of ph7sical by*P.S. Kudriavtsev. Reviewed by A.T.
Grigorlian, D.D. Ivanenko. Vop.ist.est. i tekh. no-5:200-203
'57. (MIRA 11:2)
(Phynice) (Kudriavtaev, P.S.)

IVAIMNKO, D.D., professor.
1 1. -WwAftft,
Impressions on the status of the physical sciences in It&1jv.
Vest.Mosk.un. 12 no.1:196-198 157. (KM 10-.8)
(Italy--,Physics)

History of development of the generAl theory of relativity.
Trudy Inst.ist.eat.i tekh. 17:389-424 '57. (MLRA 10:7)
(Relativity(Physics))

AUTHORS: Brodskiy, AAA., Ivanenko, D.D., 56-4-12/54
TITLE: A New Possibility in the Neutrino Theory. (0 novoy vozmozhnosti
v teorii neytrino)
PERIODICAL: Zhurnal Eksperim.i Teoret.Fiziki, 1957, Vol. 33, Nr 4, pp. 91o-912
(USSR)
ABSTRACT: Analogous to thehitherto existing description of the electrons and
other fermions by second order spinors it is proposed to put first
order Cartanian 8pinorn for the neutrino, in which connection,
however, new rules governing the transformation oil the occasion of
reflection occur. quite apart froza the obtention of parity a num-
ber of conclusions of the new theory are analogous to that gi 'ven
by Yang-Lee, as for :instance the disintegration of r and E) mesons.
It shall not be omitted to point out an interesting. possibility of
using mixed spinors of first order in the case of spatial reflect-
ion (space inversion) and those of second order in the case of
time reflection. There is 1 Slavic reference.
ASSOCIATION: Eoscow State University (Moskovskiy gosudarstvennyy universitet)
SUBMITTED: April 1, 1957
AVAILABLE: Library of Congress.
Card 1/1

`AUTHOR: IvAN -1gXDm_b_,_PUS TOVALOV, G. F - FA - 2170
TITLE: Melloatoms. (Russian)
PERIODICAL: Uspekhl Fiz.Nauk, 1957, vol 61, Nr 1, pp 27-43 (U.S.S.R.
Received: 3 / 1957 Reviewed: 4 / 1957
ABSTRACT: Compared with ordinary hydrogen-like atoms with electrons, meso-
atoms have some peculiar features: small distance between meson
and nucleus, the possibility of capture of a meson by the nucleus,
nuclear interaction between the meson and the nucleons of the nu-
oleus, simultaneous existence of particles of various sorts (olec-
trons and mesons) in the orbits of the atom, various spine of me-
sons etc. The study of mesoatoms furnishes many new data concern-
ing the structure of nuclei and the interaction of particles. The
energy values, orbital radii, and the transition probabilities of
mesoatoms are described in first approximation by the formulae
for ordinary hydrogen-like atoms with electrons. Shape and dimen-
sions, however, influence to a great extent the entire system of
energy levels of the meson in the mesoatom. Therefore, the meson
in the mesoatomg as a much more effective medium (compared to
the electron in an ordinary atom) is suited for the investigation
of nuclear properties (dimensions, shape, distribution of posi-
tive charge over the nuolqar volume, electric quadrupole momen-
tum of the nucleus, forces of non-electromagnetical origin be-
Card 113 tween meson and nucleons). On the other hand, the study of meso-

Mesoatome. . PA - 2170
atoms facilitates the precise mentioning of some data concerning
the meson itself, e.g. concerning its magnetic momentum and its
mass. Pirst the experimental investigation of mesoatoma is dis-
oussed. A device typical for this purpose is demonstrated by
means of a drawing. The energy of the transitions of some meso-
atoms could be investigated also by means of the method of criti-
cal absorption. Also the quantum yield can be determined by the
same method. By means of the quantum yield the ratio between the
capture probability of the meson by a nucleus with a given orbit
and the probability of radiation transition oat be determined.
Consideration of nuclear volume: Because of the smeared out oba-
racter of the charge over a finite volume the levels of mes oatome
are shifted in an upward direction with respect to the level ex-
peoted for punctiform nuclei. This effect is strongest in the case
of an S-level, and less expressed in the case of P- and D-levels.
The influence of the dimensions and the shape of the nucleus is
expressed to a great extent especially by the position of the
energy levels of mesoutome with great Z.
oatom upplies an izter-
The polarizatiOU of the vacuum in meswoja+
eating and essential correction for tht energy of IMIS Of Meso-
Card 2/3

t
AUTHOR: IVANENKO,D. ,KHRISTOVo KHR. PA - 2290
TITLEt Dis 1sision of the book by WALTHER THIRRING "Introduction into
Quantum Electrodynamios" , Vienna, Franz Deuticke, 1955.(VAL'TER
TIRRING, vveaeniye v kvantovuyu elektrodinam:Lki, Russian).
MIODICAL: Uspekhi Fiz.Nauk, 1957, Vol 61, Nr 2, PP 308-3,10 (U.S.S.R.)
Receivedi 4 / 1957 Reviewed: 5 / 1957
ABSTRACT: The following are the most important points of this discussion: Un-
like all other existing monographies on quantum olectroidynamion this
book is very short (VIII + 122 rather small pages). Formulae oon-
tained in the text are camparatively simple. In spite of this, the
material dealt with is very voluminous.
In the introduction same formulac on classical relativistic eleotro-
dynamics are given and same phenomena in nuclear physics are sketched
out. The first part of the book, "The Quantization of Free Fields",
(39 Pages), successfully formulates the general principles of the
quantum theory of the field, discusses the most important relations
of the second quantization, as well as the oannection between spin
with statistics. Further, acme concrete fields (scalar, vectorialt
spinorial) and vacuum fluctuations are investigated.
The second part "Fields with Intemotiod, deals with general eqgaa-
tions of quantum electrodynamics and their solution by means of the
perturbation method. The scattering matrix is given and several
Card 1/2 types ofFEEMANadiagrams are explained.
Fa - 2290
Discussion of the book by WALTHER THIRRING "Introduction into
Quantum Eleotrodynamican, Vienna, Franz Deutickta, 1955.
The third part, "The Limits of the Theory", discusses the divergences,
self energy of the electron, LAMB'S shift, the vacuum-dependent
magnetic moment of the electron, the theory of the renormalization
of mass and discharge, the convergence of the extension of the
S-matrix, etc.
Two annexes (supplements) deal with DIRAC matrices, FOURIER repre-
sentations, as well as with 25 exercises with solutions.
Fran the outset this book concentrates on general physical prin-
oiples, the most important mathematical methods and the most im-
portant results of quantum eleatrodynamics, but it does not deal
with different applications on ooncrete problems.
The excellent representation of the vast and ocmplio&ted material
within so narrow a space is amazing. The entire book does not con-
tain a single superfluous word. Also the initial: assumptions of the
theory were well-chosen. The book also contains much that is new.
According to the opinion of the Russian reviewer the book ought to
contain more explanations of basic conceptions and supplementary
remarks. According to the reviewer's opinion it ought furthermore
to be translated into the Russian language (together with the book
by DYSON). (No illustrations).
ASSOCIATION: Not given
FBESENTED BY:
SURKITTED:
AVAILABLE: Library of Congress
Cara 2/2

L i
.01
AUTHOR: Ivanenko. D. D. 53-4-lo/10
'TITLE: Physical Sciences in Italy (Fizicheskaya nauka Italii)
PF:RIODICAL: Uspekhi Fiz. Nauk, 1957, vol. 62, Nr 4, pp. 523-537 (USSR)
ABSTRACT: The author was able, when attending the Congress on Fundamental
Constants, to form a fairly complete opinion on the present sta-
ge of physical sciences in Italy and on the organization of uni-
versities and institutes. This congress took place at Turin in
the autumn of 1956 and was organized by the Italian Physical
Society in collaboration with the International Phy:;ical Union
of the UNWO (UN).
First, the author gives a report on the congress. Aft_~!r the con-
gress the author visited all important centers of phyEical scien-
ces in Italy, which are sections of the National Nuclear Institute
and are connected with the univeraities of Turin, Milan, Padova
and Rome. The sections of the Nueldar Institute are better equipp-
ed than the other laboratories and special budgets are at their
disposal. Italian Physics has reason to be proud of the tradi-
tions of Galilei and the old Italian academies. During the midd-
le and end of the 19.century, Italian physicist played no lead-
ing part within the most important domains of physics. In the
twenties and thirties, however, B.Fermi and SegrA and later others
Card 1/4 (Razetti, Amaldip'. Pontecorvo and others) distinguished themselves.

Physical 5ciancerj iri Italy.
53-4-10/10
Most members of this group,however, emigrated. Italy suffered
great hardships during World War II and a noticeable advance in
the sciences did not occur before 1952 when the National Nuclear
Institute was established.
The main task of all four sections of the Nuclear Institute con-
sists in the investigation of elementary particles and serving
this purpose the research of cosmic radiation Proper nuclear phy-
sics, however, does not exist in Italy because of the lack up to
quite recently of reactors and accelerators. Thus,special photo-
plates for irradiation in accelerator laboratories are specially
sent over to the USA- and are then iitilized in Italy ( ! I). By
this fact the great interest displayed by Italian physicists for
the Soviet accelerator laboratories is explained.
The first small but very good accelerator (betatron, bought from
the Swiss firm of Brown-Boveri) was installed in the summer of
1956 at Turin university. A synchrotron for 1o9 eV is at present
under construction at the university of Rome. The parameters of
this accelerator are given here. E, Amaldi takes active part in
CERN in Geneva. (A proton accelerator for 5.1010 eV, by the way,
is planned in the USSR. Besides a Cockcroft-Walton device at the
Cise laboratory at Milano, no important proton accelerator exists
Card 2/4 in Italy (laboratoriya "Chizell,i.e. Centro informazioni,studie

Physical Sciences in Italy.
53-4-10/10
esperienze). Above all, not one single cyclotron exists in Italy.
Professor Bolls, is an active propagationist of technical nuclear
physics. Next, a short report is given on the lectures delivered
at the technical college of Milano. A qualified but very modest
training of staffs within the domain of technical nuclear physics
is concerned. Till recently no nuclear reactors existed in Italy.
In spite of this fact, according to the opinion of the author,
the physics of elementary particles and cosmic rays is highly de-
veloped in Italy. Thus, the Italians were successful in discov-
ering Lhe Y -particles. This fact is connected with the existence
of some stations for cosmic rays in alpine districts. Most of
all the author was impressed by the photoemulsion chambers. Ital-
ian theoreticians at present partly keep up the traditions of the
Fermi school. Young talented physicists, conversant with the la-
test developments already obtained new results in the theory of
the nucleus, in the quantum theory of the field, and in the theo-
ry of the elementary particles. The non-atomic branches of pby-
sics are represented in Italy much less frequently or not at all.
The insignificant development of work dealing with spectroscopy
and X-rays is remarkable. Also the physics of low temperatures is
still in its elementary stages. The physics of magnetic phenomena,
Card 3/4 ferromagnetic, and semi-conductors is hardly represented in Italy

Phygical Scienc!s in Italy.
53-4-10/lo
at all. However, liquids are subjected to ultrasonic investiga-
tion. In conclusion the author though stressing the excellent
quality of Italian physics, says that it is confined to a very
limited category of problems. Demands of modern science and
especially of their technical applications (particularly within
the domain of nuclear physics and atomic physics) at the present
level of Italian science cannot be satisfied. Within the next
lo years various institutes will be founded which are enumerated
here. The Academies of Science, with their center at Rome and
branches at Turin, Naples, etc,, are representative institutes
and do not play a noticeable part within the organization of
Italian sciences, The type of the discussions taking place at
summer schools remind on of the antique Platonian Academy. The
author then gives a report on Italian universities. There are
2 fi,,,ures.
0
AVAILABLE: Library of Congress
Card 4/4

KAYAR, Kariaa (( a " rt)~ KOLESMOT, N.S. (translator]; IVAR311KO, D.D.,
P136 1
red.
E319mutary theory of nuclear shell structure] Alementarnaia
teoriia iadernykh obolochek. Moskva, Isd-vo inostr.lit-ry.
1958. 318 P. (KmA 13:8)
(Nuclear shall theory)

IVANENKO, D.
ffEvolution of the physics of elementary particles." Tr. from the Russian.
P.
FIZIKA,' S2MUE. (Eotvos Lorand Fizikai Tarsulat). Budapestp Hungaryt
Vol. 8, No. 9, Nov. 1958..
Monthly list of East European Accessions (EEAI), LCO Vol. 8, No. 8,
August 1959.
Uncla.

A UTITOR: None P.,iven
SOV/3-59-12-30/43
TITLE: Intervuz Scientific and Methodical Conferences (,','ezhvuzovs-
kiye nauchnyye i metodichaskiy konferentaii). A Conference
on the History of Physics (Konferentsiira no istorii fiziki)
PERIODICAL: Vestnik vysshey shkoly, 1958, Nr 12, p 77 (USSR)
ABSTRACT: The recent Intervuz Conference on the History of Physics,
held at the Tambovskiy pedagogicheskiy institut (Tambov Peda-
gogical Institute) was attended by 50 scientific workers of
pedarofrical institutes of the RSFSR, Ukraine, Ceormia, Baltic
Republics, Moldavia, the MOU and the Institut istorii yestest-
voznaniya i tek~iniki AN SSSR (Institute for the History of
Natural Science and Engineering of the AS U--SR). The Direc-
tor of the latter- r---fessor N.A. Fipmirovskiy, spoke on the
role of the conference as the first successful attempt to
.unite the efforts of Soviet Historians of Physics on an All-
Union scale. The scientific worker of the institute for the
,ineering of the AS-7,9SR, O.A.
History of Natural Science and Eng
Card 1/2 Lezhneva ', told the conference of the first theories of elec-
SOV/3-513-12-30/43
Intervuz Scientific and Methodical Conferences. A Confer'ence on the History
of Physics
tromagnetitim. Prof essor._k. D,_LY"_e_nkQ_CjAoscow) gave a detailed
analysis of the peculiarities of development of physical
science in some forei countries. The report of Dotsent
B.T. Spasskiy (moscowrwas on the periodization of the histo-
ry of physics. Other orators were Professor P.S. Rudryavt-
sev (Tambov) and G.G. Lekhemas (Villnyus).
Card 2/2

AUTHOR: Ivanenko, D. D. SOV/53-65-2-" 4/14
TITLE: Iinterna Lion ~06 -egress Held in Italy on- Elementary Particles
(Y,ezhdunarodnyy kongress po elementarrAym ohastitsam v Italii)
PERIODICAL: Uspekhi fizicheskikh nauk, 1958, Vol. 65, Nr 2, PP. 331-349 (USSR)
ABSTRACT: 1.) The laboratories of Bologna and Pisa.
The Congress of the Italian Physics Society %v= held at Padova
and Venice from September 23-28, 1957 and vras attended by about
600 scientists. The following list contains the names of
prominent scientists from America, England, France, Western
Germa.ny, &ritzerlanrl, Holland, Hungary, and Poland, Mio took part
in th'i congress. The Russian delegation, headea by
A. A. Vorobyev of the Tomsk Polytechnioal Institute (Tmskiy
politekhnicheskiy institut) was composed of 10 scientists, of
which A. I. Alikhanov, A. It. Baldin, S. Ya. Nikitin and
1. L Gurevich are mentioned by name. The Unitea Institute of
Nuclear Research (Dubno) was represented by: Darii.sh (Wars&w) ,
Ulehla- (Prague), Khu Ning (Peking) The congress -~ms further
attended by several scientists of 6FAI (Centre Europe'en des
Card 1/3 Recherches Nucl6ires). The author of this article further gives

The Internatioual Congres3 Held in Italy on SOV/53-65-2-11v/14
Elementary Particles
a report about the first days at Padova during which the congres-3
,.,as held in the university buildings, as well as about -the follow-
ing period during %,thich sessions took place at Venice, Bologna. an]
Pisa. In this connecUon a large number of Italiain iiistitutes suid
Italian plVsicists are mentioned as viell aq geographical and
hlstorlc;~A details.
2.) The Pari;3 Labora-torieLs.
In the following the author tells about a visit to the Centre
Nucle'aire; visits to Paris, Avillon, Chatillon, and above all to
the reactor centers of Saclb and Marcoule are described and
several reactors (Zoe, Gl, G2, G3 etc.) are also described in
short. The author further deals with "rea--tor
of organization, universities, etc. in France.
3.) The 14on-Conservation of Parity.
The principal problem dealt Ath on this congress zias the
non- cons ervati ou of parity in the case of weak interaction. The
introductory lecture was delivered by T. D. Li. The author dis.-
cusses the problem and says in connection .,rith the experiments
Card 2/3 carriea out by Frauenfeld et al. (Phys.Rev. 106, 386 and 10Z,

The International Congres,,3 Held in Italy oil SOV/53-65-2-14/14
Elementary Particles
643) that aimilar but much more accuratt:~- experiments ,/',,re carried
out by the Russian research scientists Alikhanov and NAltin,
4.) The Nonlinear Field Theory and other theoretical lectures,
In this chapter the author deals in detqil vid.th the lectures de-
livered by various famous non-Soviet scientists such as Heisenberg,
Goldhaber, Kamefuchi, Pauli et al.
5.) Experimental data.
This charter contains numerous data concerning the results ob-
tained by research work carried out above all by Ameriow-A scien-
tists and institutes (Michigan University, Brookhaven (Brukkheven) ,
Columbia University, Berkel'eyg'MIT,, University of California etc.),
No Soviet lectures, instituGes, or research results are inentione-1.
1. Scientific reports 2. Nuclear physics
Card 313

24(0) SO11/53-66-3-6/ 7
AUTHOR: '~~,Kanenko, D. D.
TITLE: The Flanck-Celebrations at Berlin and Leipzig, (Plankovskiye
torzhestva v Borline i Leyptsige)
PERIODICAL: Uspekhi fizicheskikh nauk, 1958, Vol 66, Nr 3, pp 523-534(IISSR)
ABSTRACT: The German Academy of Sciences of Berlin (German Democratic
Republic) together with the Physics .5ociety of the German
Democratic Republic and the Union of Physics Societies of the
German Pederal Republic celebrated the hundredth anniversary
of Max Planck (Make Plank), the creator of the quantum theory.
The celebration was held on April 23 and 24, 1958. They were
followed by the annual congress of phyqicists of the German
Democratic Republic held at Leipzig (April 27 - 30)- At the
Planck-Jubilee congress and at the congress held at Leipzig
the USSR was represented by a delegation consisting of:
N. N. Bogolyubov (head of the delegation), D. D. Ivanenko,
S. A. Azimov, A. P. Ioffe, A. V. Ioffe, G. P. Keres,
V. I. Mamasaklilisov, A. B. Migdal, G. 1. Rakhmaninov (secretary
of the delegation), A. A. Smirnov, B. I. Stepanov and Zh. S.
Card 1/6 Takibayev. The delegates visited Physics Institutes and de-

The Planck-Celebrations at Berlin and Leipzig S07153-66-3-617
livered a number of scientific and popular lectures. - The
conferences were further attended by all active physicists
of the German Democratic Republic under the leadership of
Gustav Hertz (Gerts), holder of the Nobel Prize and Director
U
of the Physics Institute of the University of Leipzig, and
further also by R. Rompe, Secretary of the Department of
Mathematics, Physics, and Teahnology of the German *,cademy
of Sciences (German Democratic Republic), Professor Barvick
(Barvikh), Director of the Dresden Nuclear Center, Professor
Gerlich (Gerlikh) scientific manager of the firm of Zeiss
(Taeyss), and others. The German Federal Republic was represent-
ed by the holders of the Nobel Prize Heisenberg (Geyzenberg),
Laue, Born, and Halin (Gan), the theoreticians Hund (Gund),
Dopp, 118n1 (aenl'), Sauter (Zauter), and Bagge. The Chinese
representative was the physicist HU I'ling, Poland was
represented by Infeld, Rublnovicz., and others, Fungary b,-yr
Bud~q Bulgaria by Datuov, and Romania by Mcu.
Further, a list of the representatives of "Western se once"
is given such as Dirac, M61ler, 1,1eitner, Weisskopf, and others,
who were also present. A total of 12 countries was represented.
The Planck celebrations were held partly in the eastern and
Card 2/_6 partly in the western part of Berlin (on April 23 in East-Berlin

The Planck-Celebrationa at Berlin and Leipzig sovil:: 3-66-'x - ' '7
on Apri1241 in 7,e3t-Berlin), The PlanCk- celb-rations are then
described in detail, Lind an account i,* given of his life and
his scientific work. Heisenberg's lecture "Planck's Discover,-.-
and the Basic Phil oi-.ooh ic.al Problems of Atomic Theorw" is
discussed as well as other details Lis music-1
The annual meeting of the Physics Society of the Gevnun Demo-
cratic Republic held at Leipzig form April 27 to -~Inril- 30,
1957. The meeting was connected with, a thu-ork~:tic~-l conference.
It was oDened in the auditoriu.-,i of the Phjsics lnstit!.z~e of the
university, which is able to accomodate 450 peraonz5. The
important lecture delivered by Heisenberg(Geyzeriber,,-) dealt
with the standardized nonlinear theory of inatter, The lecture
is dealt with with respect to it.--, main outlines. The oumo-, is
the case with Dirac's lecture on the theory of grav--~Liticn.
The third of the Drincipal lectures aaj delivered by
J. N. bol-olyubov, Member,_Academy of Scien--e5' USSH. lie sucke
about a new method in the thoory of ~~upez-conductivity a-d
superfluidity. This method is bu~;ed upon tiie canonicLtl
transformation, wh1ch the speaker had recommenued alreadv
Card 3/6 in 194.7 for the development of the micros--opical theory of

'The Planck Celebrations at Berlin and Leinzig S,DIr/53-b6-.,-6/7
superfluidity and for calculation of the interaction between
bosons, -nd which now applies also to fermions. lie thus
continued along the same lines -,;s Fri'lilich (Frelikh) (in his
paper on the interaction between elc.-vtrons and phonons) and
Bardin COO-Oer (KUpel') et al. D'. il. BOgOlyUbov and his
kov, j. V. Tyablikov,
collab~ ators ~V. V. Tolmachev, D. V. Shirr
.D. 11. Zubarev, Yu. A. Tserkovnikov') further spoke about a
mathematically correct superconductivity theory, -.-ihich t'ak'es
not only 3ingle-fermion excittion but also collective
excitation and the part played by Coulomb (Kulon)-forces into
account. Further lectures were deli-.-ered by: J. P. Vigier
(Zh. P. Vizh'ye), L. Ji6aossi ;,,-i experiments carried out by
him in a depth of 30 m belniv the surf&ce of the eatrtb 1[oll-'ether
-with Ntrai, Varga, ~d~m et al. in thin optical laboratorZ( of
the Central Physics Instivate of the HungL~.rian A-S at Budupest
(interference tests); Curthcr, c, ----amber of ax,-perimental leoture
were held only some of -,,.-hich are mentioned (Krebs, Bern', 'ard,
Ardenne, Unmgst, IMUller, Eder, BiL---aLck, Meyer, Tsellr----~r
(~.A prosent in Dubna) on the dispersion for
Card 4/6 n + N42n + N proui~o:3e- F. Kaplun (Dubn:~) spok'o ;-boUt the

The Planck "'elebration3 at B.-,rlin and Leipzig jOV/53-66-3-6/'17
dispersion relations for elastic p-d scattering, K. S. Tseyten,
A. B. lAigdEL1 (quantum field theory), Kagan, Hbnl- (Genl'),
T. Kakushadze (Tbilisi) on X-ray spectra, V. Kofink, and
others). - The members of the Soviet delegation delivered a
number of lectures dealing with the development of physics
in the USSR. The important lectures delivered by Bogolyubov
and Ivanenko o.,ere attended by more than 1000 persons.
Ivanenko spoke about the Novosibirskiy nauchnyy tsentr
(Novosibirsk Scientific Center) and about the succ~-cs
attained by Soviet scientists in the fields of nuclear physics
and accelerators. Several members of the deleg~~ticn delivered
lectures on the situation of science in the variouq republics
of the Union: Gruziya (Profesjor V. I. Mainasaklilisov, Corres-
ponding Member AS Gruziru3kaya SO); Estoniya (Profe~~sor i;.P.
Kpres); Ukraina Urofesior A. A. Smirnov, Correziponding INlember,
AS UkrSSR); Kazakhstan (Doctor Zh. S. Takibuyev); Beloru3slya,
Minsk (Professor B. I. Stepanov, Member AS Belo_-russkayE
SSR ); finally, reports were deliverea concerning sev-~~ral
institutes of the Academy of Sciences of the German Democratic
Card 5/6 Republic, and visits as well as tours of i,'i3pecllion were

D -
AUTHORS: Ivanenko, D., Brodskiy, A. SOV/2o-12o-5-18/67
TITLE: On Non-Linear Theory of Elementary Particles (K nelineynoy
teorii elementarnykh chastits)
PERIODICAL: Doklady Akademii nauk SSSR, 1958p Vol. 12o, Hr 5v
PP. 995 - 998 (USSR)
ABSTRACT: This is a study of a non-linear generalization of the Dirac
(Dirak) equation for a quantized spinor field. The invariants
can be obtained by a method described already earlier by the
authors (Ref 2). This method is characterized by setting equal
all spinor fields in the expression for the interaction of two
Fermion pairs (as, for example in the theory of 0-decay). The
method is based upon the hypothesis of universal interaction
and the description of matter by a uniform "world spinor". The
Lagrangian corresponding to these conceptions is written down.
In the not quantized theory a number of relations exists between
the terms of this Lagrangian. A few of the non-linear terms
apparently are identically equal to zero. The spinorV is then
transformed to a form, in which every particle is described
by a two-component hall-spinor. This inveiitigation is limited
Card 1/3 to a certain non-linear part of the Lagrangian, The field

On Non-Linear Theory of Elementary Particles SOV/2o-120-5-18/67
equations resulting from a variation of the Lagrangian are
given. The problem of an ansatz for the equait:Lons of the causal
propagation functions for this non-linear LA2,Ttingian is
discussed by the authors. In order to solve this problem
additional terms with fictitious sources are introduced into
the Lagrangian. An operator for the mass &I is also introduced,
taking into account the translation Invartance of the kernels.,
The equation for the causal kernel :In thqi non-linear case in the
absence of external fields is equivalent to the equation for
the linear case, if an interaction with the boson vacuum of
an "electromagnetic" and of a "boson" type with the field mass
and with the "bare mass" is assumed. From the considerations
presented the addition of non-linear terms in the case of a
free particle is effectively reduced to a modification (or
the introduction) of a mass. When a two-particle kernel Is
considered the equations of non-linear theory cannot be
distinguished by their appearance from the equations of linear
theory with a boson field. According to 'the results obtained
the boson fields can in the non-linear theory be considered as
Card 2/3 a result of the unification of the "primary" spinors as In a

On Non-Linear Theory of Elementary Particles SOY/2o-12o-5-16/67
fusion. The authors express their gratitude to Professor B.
Heisenberg (Geyzenberg) for his friendly note on new interesting
results of non-linear theory. There are 8 references, 4 of
which are Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet im. M.V.Lomonosova
(Moscow State University imeni M.Y.Lomonosov)
PRESENTED: April 9, 19560 by N.N.Bogolyubov, Member, Acade Imy of Sciences,
USSR
SUBMITTED: April 7, 1958
1. Beta decay--Theory 2,, Part ic le stheza t -Lc,:,,l a_j&jys_ig
Card 3/3

KUKARKIN, Boris Vasillyevich, prof.; RYBNIKOV, Konstantin Aleksayevich
prof.; BASHMOVA, Izabella Grioorlyevan; TUSMVICII, Adollf
Pavlovich; TANOVSKAYA, Sofiya Aleksandrovna; SPASSIXY, Boris
Ivanovich, dotsent; MIXHAILOV, Glab lonstantinovich. starshiy
nalichn.y7 sotrudnik: MATYNOT, D.Ya., prof., otv.red.; GOROM,
D.I., prof.. red.; IVANMMO,._.D.U,,-prof., red.; KUIRYAVTsxvg
P,S,, prof., red.; KnIKOVSKIY, P.G., dotsent, red.; KWIM9
A*Khot profog red.; SHMSOV, N.S., prof., red.; YMUMMV.
V.R., assistent, red.; KONONKOV, A.F., red.; YLTMAKOV, H.S.,
teldm.red.
(Programs of courses on the history of the physicomathematical
sciences] Programmy po istorii f12iko-matematicheskikh nauk.
Moskva, 1939. 40 p. (MM 12:12)
1. Moscow. Universitet. 2. Orgkomitat Vaesoyusnoy mezhvuzovskoy
konferentaii po istorii fisiko-matematichaskikh nauk (for Kukarkin,
Rybnikov, Spasekiy, Gordeyevq.lvanenko, Kudryavtoev, Kulikovskiy,
Kikhaylov, Khrgian, Shevtsov, Verkhunov, Kononkov).
(Physics--Study and teaching)
(Hathematica--Study and teaching)

21(1,8); 24(_)) MA,3R, I BOOK EXPLOITATIO11 SOV/3369
Vsesoyuznaya mezhvuzovskaya (clonferentolya po Jcvantovoy teoril poley
i teorii elementarnykh chastits. Uzhgorod, 1958
Problemy sovremenno teorLI elementarnykh chastits. No. 2: Trudy
konferents-ii ... TProbleins In the Modern Theory of Elementary
Particles. Nr. 2: Transaotions of %'he All-Union Inter-Vuz
Conference on the Quantum Pield Theory and the Theory of,
Elementary Particles) Uzhgorod, &-ikarpatskoye oblastnoye' izd-vo,
1959. 214 P. 5,000 coples printed.
Ed.: Yu. Lomsadze, Docent; Tech. Ed.: M. Belous.
PURPOSE: This book is Intended,for physicists, particularly those
concerned with problems in tlie field of elementary particles and
the quantum theory.
COVERAGE: This book contains articles on elementary purticles
originally read at the kll-Union Inter-Vuz Conference held at
Uzhgorod State University on October 26, 1958. Among the topics
Card 1/,6

Problems in the Modern Theorly (Cont.) SOV/3369
discussed are: the spinor field theory, the fusion theory,
Lorentz contractlons, parity studies, nucleon-nucleon scattering,
etc. English abstracta ac(,onipany each article. References
follow each article.
TABLE OF CONTENTS:
Foreword
3
Ivanenko, D., and A. Brodskiy. Renthrks on the Unified
-Non-idmar-Sp-lnor Field Theory 5
Barashenkov, V.S. Multiple Formation of Particles in
Experiments With 9-Bev Protons on the UNIR Phasotron 10
Borgardt, A. Continuation of Wave-Field Functions Into
the Region of Nori-Linear 3elf-Action 20
Sokolik, G.A. New Formulation of Fuslon Theory 26
Card 2/6

Problems In the Modern Th;-or:t ((,ont. ) SOV/3369
Lomsadze Yu.M., and B.I. Maksimov. Application of
Schwinger's Variation Method to the PaIr liqieory 30
Sokolik, G.A. Generalization of the lx)rentz Group 37
Ivanitskaya, O.S. Generalized Equivalent Potential and
the Sequence of Infinitesimal Lorentz Contractil,:jn7, Under
Rotary Motion 44
Sokolik, G.A. Representation of the Complete Lorentz Group 52
Sokolik, G.A. Connection Between the "Anomal" Representation
of the Space-Time Inversion Gro~ip and the Paull Tranoformations 56
Geshkenbeyn, B.V., S.A. Remirovskaya, and A.r. Rudik
Non-Conservation of Parity In RaE 58
Bilen'kiy, S.M., and R.M. Ryndin. Determination of Parity
of'Strange Particles 63
Card 3/6

Problems in the Modenn TheorY (Cont. ) 3OV/3369
Lomsadze, Yu.M. The Possible Versiono of' the J, --
Decay Theory 69
Vanyaghin, V.S. Equations of the Onler for Spinor
Wave Functions N 80
Soiovlyev, V.G. Conservation of the CombAned Parlty, as a
Fundamental Law of the 3ymmetry 1n Nature 83
Geshlcenbeyn, B.V. PolArization of Electrons of the Inner
Co,nversion Sub.4equent to j6 -- Decay, Taking Tnto Account
the Electric Field of the Nucleus 89
1
Sitenko, A.G. Polarization of the Nucleons Under the
Stripping Reactlon in the High Energy Region 99
Yyglane, Kh. Wave Equations for Elementai-j Fai-ticles log
Barashenkov; V.S., and B.M. Barbashov. Some Remarks on the
Inner Structure of the Nucleon 117
Card 4/6

Problems in the Modern Theo-ty (Cont.) SOV13369
Solovlyev,' V.G. On the Superfluld State of an Atoxa Nucleus 126
Dolginov, A.Z. Polarization of Quanta.Emitted by A Mezoatoms 138
Barashenkov, V.3,, Optical Analysis of the Interaction Between
Fast Nucleons and Pions Partiales With 1.,Tueleons and Nucleus 142
Zharkov, G.F. The gemi-Phenomenological Theory of Nuclear
Forces 14q
Fisher., Ya., and S. Chulli. Partial Wave Analysis of the
Generation of Particles 157
Zlatev, I.S., and P.S. Isayev. The Effect of the Form-Factor
on the Processes of Bremostrahlung and Generation of Pairs
on Protons 165
Fillmonov, V,A. On the Interaction Between.,6 -Particles and
17C
Nucleons in the Hypernuclei
Card 5/6

IvANEmKO, D.D., red.; LARIN, S.I., red.; BELEVA, N.A., tekhn.red.
[Nonlinear quantum field theory; collection of articles]
Nelineinaia kvantovaia teoriia polia; abornik statei. Koskvat
Izd-vo inostr.lit-rys 1959. 464 pe (KIRA 13:2)
((bmntum theory)

IVANEUO, D. D.
"Transmitation of Gravitational Energy into Ord1nary Matter."
papbm presented at the Intl. Colloquium an Relative Tbeories of Graviatione,
Pariap 21-29 Jun 59.
pre-print in Russian available.
A-3135940
Moscow State Univ.

A C.
TITLZ I Th. Physics fjjxjLMj&rXjj
PIRIODICALS U.P.khi flatehookikh Back. 1960, yet 70. or 2, 11 361-3?4
LISTRACTi The authors give a report on The laternallEnal Conf4~rsn.SV~
0 held at 11yov 1. July 1959.
fl.kht.tes. " 1. To. Tama.' Too or the ..,9. holders
Is-
:f the Nobel PIL.- as :,
.4 P. A. Cherenkov, Ap f,,h 7lg I turea
soula"a vote htli,ln which the following Russian lecturire
spokel To. Tmjq~om *!Iagraw Technique and Flel4 Theory",
he No linter P1916- an# Gravitation
Collisions", ant
is Th. '14"&r7 ~.act*"
he first sessloa Sarsaritnt (Call)
spoke. Its selontiflo socre4azlea oars A. 2~14im. set A. Waravot
Tax report an tke looluxe %tattoos ille data Otain.
.4 at the platcheakly Lastitat I%. P. a. L0.40ow U assR
(Physics U00ste Isomi P. X. LoU4*v Ll V3111 an the -Pala
ISSWIMY of "One Is 3.
(Daluma) WiTIT94 a lavilfs, salon is discus
16111 " *?too scallorT Wy lustsafts &M rVeivollon of Ital
HONG In heloos-holso Rod hah-haless, tutors
Next. 2"_1AkiULjhW") spoke 410'al owl
lakeraotiona ia_tk* 1.5 10 14 hadeI

Ivarenko, D.D.
BIND11;G ENERGI:~S) OF 1TYPEW'i-NT'CT,?1 kM T1,1T*~MAGT_,O"S k^,F MM')4AIi-,T) ML
D.D. Ivanenko, N.N. Kolesnilov, V.A. Lyullha, V.A. Pllilironov
Hynarnuclei systorr.-s cort-iining)L nr ~/-hynerons in addlt.lon to orotons and
neutrons, are of q-ictt Jrterof~t both f,-r tl,r- 1nd-!rst,-tncHnF1 of' cosmic ray orocossen
and for rnsviarch Into ordinary nucloar �~rces. By mstking use of t1ho birrl-i-f-
f
constRnt.s known from sc-ittering tYeory, and having csxried out t~ai "out of"
as In the C1,ou-Harte.-+av,, metl-od in the theory of ordinary nualqi, im ob-
tained v--.luis for hyT)e-r-nuclel. bl!~dlng energi,~s In satisfactory aprrii~Trent w'it'h
e-,mer r-antal resvIts
An ovaluati.oVade on the 1,anis of felrl tl;)(,ry r-~V~aj.ed the exiFt;-)nce of
weak forced: of jA- Lattract'on in addlt,inn to tbi rtrongerA~intereactior, wl.icb)
in turn, is notl-'ably w--!ker than the *om:,,s. In tbJs connecti.on, th-i birding
energies of t~e normal and the ~axcited 1-tates of a ver-l-en of I.I.Pft nuclei contairl?!-
one or two,]%.- Dartic-jes -were ca3culated usi.-a t1-3 anorr-ri -!-.,Aon of a short ro.nae
of act-;on and a -Y-eno~eno].-,7ical notent4a! &-n-.ndi P,, or., Q,- snin, who.-,e T-klrareter;-
wer s r sqr~ binding erergy elf tYe 4- narticle in
,Plect,id so as to Inst, ~ the nices Y
J\ and. k A
The data on forces -roce-~dirg fror h-n.--:?r-nucle1, were e-n,,o-e,4 to efticulate
tl-~! crosq qqct'on -f R,0 c-inturn or slow nartic.19,; by ni;cl;~i.
-3d at tYe- International ~Cosmjc ~Rny,- nforenco, For-cow, 1-13-Nly 11159
Report prasent

IVANYENKO, D.D. (Ivanenko, D.D.);
Developmen. in the p oics
no,4:3.11-316 Ap 159.
ABONYI, Ivan [translator]
of elementary particles. Fiz szemle 9

24(5)
AUTHORS: Brodskiy, A. M., Ivanenko, D. D. SOV/56-36-4-46/70
TITLE: Anomalous Spinors and Bosons (Anomallnyye spinory i bozony)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki. 1959,
Vol 369 Nr 4, pp 1279-1285 (USSR)
ABSTRACT: The discovery of the isotopic and strw)ge properties of parti-
cl.es and of the nonconservation of parity in the case of weak
interaction stimulated a more intense investigation of the
properties of spinors and bosons in reversals~ As, however, the
usual representations of the Lorentz group do not suffice for
the purpose of describing the variety of the new particle
properties, the
~3- or 4-dimensional) iso-space theory was
l
developed (Ref . This also showed that additional consider-
ation of previously neglected possibilities of projective
representations in the spinor-, and "integron" theory (particles
with integral spin) offers the possibility of being able to
describe iso-spin and strangeness already within the frame-
work of the ordinary spaced These problems are of interest
for the application of the fusion method, the model of the
complex particles., and also in connection with the nonlinear
Card 1/2 theory of matter. The authors here give an analysis of the

Anomalous Spinore and Bosona
SOV/56-36-4-46/70
new spinor types, they discuss the problems of the unusual bi-
linear combinations, and problems of spin and statistics. The
anomalous commutation relations, to which these spinors which
show an unusual behavior with respect to inversions obey, are
investigated (cf,Gellfund and Tsetlin, Ref 7),. Finallyq the
possibility in investigated, by means of spinorn of the class
WA . e to describe the electron-positron, by means of the
self-adjoint spinors ~ 1C1C , ~, (zero mass) the neutrino, and
WA
by means of the spinors ~ . 9 - the p-menon. The authors
finally thank G. A. Sokolik for discuosinc 'the results. There
are 12 references, 9 of which are Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet (Moscow State University)
SUBMITTED,!' November 5, 1958
Card 2/2

AUTHORS: vanenko, D. D Xitskevich, N.V. sov/56-37-3-49/62
TITLE: Fe~ idto 4ea=t Gravitational Energy
PERIODICAM Zhurnal eksperimentallnoy i teoreticheskoy fisiki, 1959,
Vol 371 Nr 3(9)9 pp 666-669 (USSR)
ABSTRLCT: The determination of the energy and momentum of the gravitational
field (which is especially necessary for the conversion of these
quantities into the energy and momentuz of other fields) has met
with serious difficulties already since the foundation of the
general theory of relativity. The difficulties are due to the
fact that the equation of continuity gets the physical meaning
of a divergence brought about by the disappearance of the usuall
but not covariant divergence. The authors denote the law of
conservation in the disappearance of the usual divergence an
exact law of conservation. The "pseudotensor" of the exactly
conserved energy-momentum density of the gravitational field
introduced by Einstein is# on the one hand, no generally
covariant quantity, on the other, the energy defined by this
quantity considerably depends on the ueleotion of the reference
systems which are in connection with the purely spatial
Card 1/4 coordinate transformations at invariable time. For this reason,

Taking i1to 'Account Gravitational Energy SOV/56-37-3-49/62
Lorentz and Levi-Civita suggested other definitions of the
energy-momentum density. The tensor of all fields which they
suggested and which is accurately oonsexved has no great
physical importance. C. 119'ller (Refs 2j 3) supplied a new
expression (and the corresponding exclusion proof) for the -total
energy of the systems of gravitational fields and other fields
with the elimination of the above difficulty. On tb,, other hand,
quantities are obtained by the new formulation of Noether's
theorem (which was derived earlier by the authors (N. V.
Mitskevich, Ref 4)) which are conserved when applied to the
field of gravity. These quantities differ from those derived by
Einstein and - as will be shown in the present paper - are
closely connected with the pseudotensor derived later by
M~ller. In this connection gravitation and the other fields are
dealt with in the same way. The gravitational field is defined
by a metric tensor so that particles with spin are bound to
correspond to it. On the basis of the expressions derived by
M~ller and N. V. Mitakevich (Ref 4) the relation
= _R ce, (grav) is easily obtained. denotes the
Card 2/4

Taking into Account Gravitational Energy SOY/56-37-3-49/62
"pseudotensor" of the energy momentum of the total system of
fields introduced by MVIler and
(grav) the value of the spin part of the energy of the
gravitational field derived by the authors. This quantity has
the necessary gravitational propertieB also for ot'- - tields
(invariance of the integral energy in purely spatial transforma-
tions which do not refer to time). The te."or dete"rined by the
authors agrees with the expression by Levi-Civita also for the
total system of the fields. For this reason the following
p, 0~
relation holds: (Sym)(tot) A (tot) + (tot) = 0
Therefrom it may be concluded that
06 C6
(f (grav) (f ) + W (grav) where A~ (f
and (grav) belong to ordinary fields in the presence of
~6
Card 3/4 gravitation and to a pure field of gravity, respectively,

Taking filto Abcount'Gravitational Energy SOV/56-37-3-49/62
The authors think it more natural to regard the sum of canonic
(unsymmetrical) quasi-tensors of all fields as the energy-
momentum density of the total system of the fields and not the
sum of the symmetrical tensor of the fields of ordinary matter
and of the canonic quasi-tensor of the field of gravity. The
opinion of the author corresponds also to the generally covariant
bases of the second quantization. There are 6 references, 4 of
which are Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet (Moscow State University)
SUBMITTED; may 30, 1959
Card 4/4

AUTHORS: Brodskiy, A. M.,_Ivanenkoy Do D. SOV/56-37-3-53/62
TITLE: On the Connection of the Isospin,and the Strangeness With
the Behavior of Spinors in Inversion
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 37, Nr 3(g), PP 876-877 (USSR)
ABSTRACT: The usual-treatment of the isotopic properties and strangeness
properties is connected with an isospace of 2, 3, and 4 dimens-
ions,-with.transitions into the paeud.peuclidian space being
possible. These pToperties may alao be described within the
usual space, however, by, using the hitherto not used possibil-
ity of a different behavior of the spinars in inversions and
under consideration of the non-conservation of parity P. The
treatment of isotopic properties within the usual space sug-
gested here extends the more special considerations made al-
ready earlier. As is known, spinors may behave differently
towards one another in space and time reflections. In this
case, the matrices of transformations diffe-r by the factors
-1r i, y5 or by their products. Thus, spinor representations
of the Lorentz group are given which differ from one another
Card 1/4 and part of which is unitarily equivalent (which is different

On the Connection of the Isospin and the Strangeness SOVI'56-37-3-53/62
With the Behavior of Spinors in Inversion
in the case of charge conjugation). A considerable difference
between the spinors (which has not the character of a unitary
equivalence) occurs in the presence of the afore-montionod
additional factors only in the cace of purely space- or pavly
time reflectionse The spinors are characterized hero by the
two index pairs a,b and a,P . Index a assumeo the value I or
2, depending on whether the additional factor 75 is added or
not in space reflection. In similar way, index b - 1, 2 char-
acterizes the geometric time reflection TO, which may be re-
a
placed by Schwinger's transformation T , To TC, where
A
denotes tLe transposition in Hilbert I a space and T Wigner's
inversion. Indices a,P assume the 4 values (O11t2,3) corres-
pondingly to the occurrence of the additional factors
ia in space-, and J in time inversions. The essential differ-
ence of the apinors is characterized by the differences (a - b)
and (a - P), more exactly by the moduli of these differences.
In the invariance only with respect to Ps and TS the problem
Card 2/4 of the mutually different spinors arises. In order to solve it,

On the Connection of the laospin and the Strangeness SOV/56-37-3-53/62
With the Behavior of Spinors in Inversion
the self-conjugate ("large") spinors are introduced.
112 1(' + '15) + + (1 - '75) ~ c ,
1/2 rL(1 - iy5) ~ + (I + iy5) +cJ ,
- C V(i,2) - fli 2) . Y2
5
In strong inversions of small ~ the cp_-aritbities IF(1,2)trans-
form linearly and separately. In the phase transformation
~' - e ia ~ it holds that Y(1,2) = exp (;LY5a)11Y(1 2). In the
case of self-conjugate emall ~ (neutrino) -41(1) and If(2)
agree with each other. To characterize the behavior of spinors
in strong inversions P 8, T81 the index pairs J = a + at
K = b + are sufficient and correspondingly also the differ-
ence N J - K = (a - b) + (a - P) (mod 2). In this connection
at bi at P refer to the initial small spinors The Lagrangian
of the interaction is constructed by means of lf(1,2) because
Card 3/4 in this case the invariance with respect to Pa and Ts becomes

On the Connection of the Isospin and the Strangeness SOV/56-37-3-53/62
With the Behavior of Spinors in Inversion
manifest. The beat way is to charaoterize -the leptons by
"normal spinors" (by attributing the various factors +1 1
I Is 7
to the particles e,v and tho baryons by spinors which 5
are mixed in strong inversions. There are 11 references,
6 of which are Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet (Moscow state
University)
SUBMITTED: June 10, 1959
Card 4/4

21(1.)p21(7) soV/53_66-*_ 1/-;
AUTHORS: Ivanen1ko, D. D., Lyullka, V. A.9 -V. A.
TITLEi The Theory of Hyper-nuclei (Tooriya giperyader)
PERIODICAL: Uspekhi f izicheskikh nauk, 1959, Vol 68, Nr 4, -PP fr-
ABSTRACTs thors give a survey of the pre:5riat 6ta,~e of thE; thz
The atk
'
hyper-nuclei, nuclear systeras consisti.,,~Ce of nu,lecr.ts &-nA
investigation of thene 1r,,,,por-nuolf-A makeri t.1.
hyperons. An
'
possible to obtain data on Y
such as spin, parity, and the interaction betM;ea part' ~cl _e z,
The large amount of experimental -..!aterial availa-ble in thl~
respect makes it poosible to deal Ir. thpor.1, with hjper-rucl:z~,i
both from the phenomenological point of view, and by mearns
the quantum field theory. The authors onizqpral-e- th'? -,-nos'
essential experimental factorp a,,-,~ tlie iri-3t, im-~.iortent
theoretical investigations concerning hyperons. The experimental
part of the paper begins with the-discovery of hypernuolei in
1953 by the Polish physicists Danvsz and Pniewsky (Ref 1) in
nuclear emulsions (Fig 1)j in the following, the authors discuss
the identification of hyper-nualei; a ta.'ble shows a number of
Card 1/3 hypernucleus observations. It was found that whereas in the

The-Theory of Byper-nuclei
BOV/53-68-4-4/12
case of accelerator- and oosmic raaiation experiments, the
relative frequency with which hyper-nuclei are recorded is
about 1.10-3 (cosmic rays only 0.2.10-3)0 it was found to be
between 24 and 57-10- 3 for the case of K-captures. In the
following the question of the life time of hyper-nuclei is
briefly discussed; their value is near the order of magnitude
of 10-10sec. Further, the frequency of hyper-nuclei as a
function of the nuclear charge is discussed. Figures 3 and 4
show the Z-dependence of mesonic ana non-meeonic decay.
Pinallyp the binding energy of the Apparticles in the hyper-
nuclei is discussed according to the relation
B - M + M - 1: m Q (Figure 5 shows B (A) - a stTaight
A :& A L A
linal A denotes the number of nucleons in the hypernucleus,
mi the masses of the reaction products, and Q - the sum of their
kinetic energies), and also some anomalous cases observe&. In
the second part of the paper - the theoretical treatment of the
hypernucleus problem - the most important properties of the
hyperons and K-mesons are discussed (classification of inter-
Card 2/3 actioft into strongp electromagnetic and weak interaction, the

The Theory of Hyper-nuolei
SOV/53-68-4-4/12
theory of the former, special cases, some F- - and -:' -processe4v
after which the decay possibilities of hyper-nuclel-Onesonic
and nonmesonic decay), as well as the problem of the spin of the
A-Particles. In the following, the authors first mention some
general questions of a phenomenological treatment of the hyper-
nuclei with A 4 5, followed by the speeial cases of the hyper-
nuclei He5 H4 H94 and H3 . Finally, the treatment of
'& I A 9 A A
light hyper-nuclei on the basis of the field theory and severall
questions related to the spine of the h;yper-nuclei are
discussed. The material (particularly that of the theoretical
part) was mainly taken from Western papers. There are 5 fig-areav
5 tablesp and 136 referencesp 12 of which are Sovieto
Card 3/3

RT.BNIKOV, K.A., prof., red.; SPASSKIT, B.I., dotsent, red.; GORDETV, D.L.
prof.. red.; IVANENKO, D.D., prof,, red.; KUDRTAVTSEV, P.S., prof.,
red.; KUKARKIN, B.V,j: prof.. rod.; KULIKOVSKIT, P.G., doteent, red.;
KIKHAYGOT, G.K.. starshly nauchnyy sotrudnik. rod.; MGIAN. A.Kh..
prof., red.; SHICYTSOV. N.S., prof,, red.; VIFaaMOY, T.M.0 asaintent,
red.; KONONKOY, A.F,, red.; KALIKOYA, F.A,, red.,; SOROXINA, L.A,.,
red.; YERMAKOV, H.S.. tekhn.red.
(Summaries of papers and reports of the Interaniversity Conference
on the History of Physics and Mathematics] Tezisy dokladov i soob-
shchenii Mezhvuzovskoi konferentaii po istorii fiziko-niatematicheskikh
nauk. Moskva, Izd-vo Mosk.univ., 1960. 187 P. (MIRA 13:6)
1, Hezhvuzovakaya konferentsiya 'po istorii fiziko-matematichoskikh
nauk. ig6o. -
(Mathematics--Congresses) (Physics--Congressea)

2if V~"po
AUTHORS:
82431
S/056/60/038/03/32/033
BOO6/BO14
Braginskiy,. V. B.,Ivanenkog D. D.p Rukmanj G. I.
TITLE: The Possibility of Making Laboratory Tests for the Purpose
of Measuring the Propagation Rate of Gravitational Inter-
action
PERIODICALt Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 38, No- 3, PP- 1005-1007
TEXT: Hew experiments for investigating gravitational waves have been
suggested repeatedly (observation of gravitational radiationg verification
of effects of*the general relativity theory, Edtv8s experiments, eto.).
Measurement of the propagation rate of gravitational interaction has been
suggested only in Ref- 5. The difficulties involved are discussed in de-
tail. According to Ref. 6, the amplitude of a field at a distance R from
the emitter may be expressed by E R a 2p0ei(,)t R-3009 0 (I+k2R2/2_ ik3R3/2+.,..),
where k -co/c 9, and c9 is the propagation rate of the gravitational fieldq
Card 1/3

8201
The Possibility of Making Laboratory Tests for slo5616010381031321033
the Purpose of Measuring the Propagation Rate B006/ 'b014
of Gravitational Interaction
PO is the dipole moment (the uipole oscillates with the frequency w). This
holds for distances R, which are small as compared to the wavelength,
where kR