SCIENTIFIC ABSTRACT NOVOZHILOV, V.V. - NOVOZHILOV, Y.V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001237610007-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: July 13, 2001
• Sequence Number: 7
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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SUBICTTED. 29Jano'4' DATE ACQ,: l9jun64 ENCL. 00
SUB CODE: AS, lv"el No R12 E'I-QV: 007 onr~~R: co5
Card 2/2 ---- - 7
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CBUVIKOV KIY, Vladislav Sergeyevich;. V.','., nauchn.
red.; O3VEN-I-KJ.YA, A.A., red.
[Principles of dynamics in the structural mechanics of a
ship] Printsipy dinamiki v struitelinoi mekhanike korablia.
Leningrad, Izd-vo "~--udostroenie," 196/.. 191 p.
kj,jT,tA 17:7)

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ACC NR&. AP6015812 -SOURCE GODE~ -.UR/O()40/65/029/002/0261/0281
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-(Leningrad)
ili~i6k: ji-do Ad
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TITLE:..,: Saint,- Vignant principle in the: dynamics ~f :bars

ZOURCE. -,-!.-PiikladnM matematikal. kekhanika no.
pl wo 290- 19659,2 1-281'
1
PIC me e ress, fabriod ted stmotural met Ia
TAGS t a. at
ABST9APT.: Aptrbicimate s6luti.ons-to equitions'describing:th6~~beha~tio,t of bars under
,-~igtrisj.ar v and
P.-ZLI "I 'somespecific examples are given,
' This ,kokk i 'based an
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P~',,TIMOSHEM` ("Th4ory' ot-osailiati6ns'in,Engiieeiing",, dtekhizdatp 1932). 4id 6thers

a''hiss" -6 ures and
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NOV(r,,iliLov, v.v. (Len-ingrad)
Fla3tic dLsintegrattcr.. Prik]. inat. i mekh. 29 no.4:681-6R.G,
ii-Ag 165. NIRA IF-?)

ACC NR1 AP6030743
AUTWR.- Navozhilov. V. W (LonLvWad)
ORG: none
TITIL, : Plastia lootiening
'3 r
P
SOURGS; Prilp-ladnaya matematUa i mokhanika, v. 29, no*- 4, 1965, 681-689
TOPIC TAGSt cyclic load, plasticity, elastic stress, plastic defQrmation, alumimim
alloy
ABSTIUCT.- The term "loosening of solids" caused by pj4stla de formation (or plastic
7--
loosening) is understood to mean their monotorLto volume increase w1di-ch can be explain(d
physically by format-ion of microcavities in the solid. The solJd is treated as a
freo-floiTing medium with strong cohesion among its particles; principal attention is
paid to altarnated plastic deformations* Two yield criteria--one recommended by L.
Prandtl and J. Guest (accounting for the effect of normal stresses or, on the critical
tangential stresses in St.-Venant's criterion), and the other derived by Fe Sohleichj~l
(accounting for the effect of the mean normal stress ~a on the critical value of ULU
man tangential stress in the Hisea criterion)-are generalized with the purpose of
investigating the process of plastic loosening in strain-hardening materials*
Soul= CODE:

ACC NR%. AP6030743
The stress-strain relationships* under plastic deformation,4
,fe dia-
cussed from two different viewpoints: 1) the strain -hardening Oenomenon
is ascribed to internal microelastic forces (of intergranular 114wre),
:assuming a constant coefficient of internal. friction; and 2) the strain-
hardening is assumed. to be caused only by an increase in the internal
,,frictiolvfactor.
It
e analyses In both cases lead to the conclusions that any plastic
deformation is followed by a residual increase in volume.(I. e. , plastic
loosening) which is proportional either to the length of the "path" of plastic
deformation (in the case of the Prandtl-Guest criterion) or to the work
cauaing the plastic deformation (in the case of Schleicher's criterion);
the additional plastic deformations due to on (Prandtl-Guest) are reduced
to plane deformation (amnidirectional expansion in the plane of shear),
'and the additional plastic deformations due to a (Schleicher) result in an
,omnidirectional (three-dimensional) expansion. An experimental in-
:vesUgation should make clear which criterion produces results closer to
:the truth.
The effect of normal stresses (Y and an on the plastic deformation.
ds small in cases of steady loading. In the came of cycHc (alternated)
:loading, the additional plastic deformations in eadh cycle caused by a

Nil. AP60307h3
and Gn are accumulated and increase monotonically (proportionally to
the number of cycles), as does the plastic loosening. After a large number
of cycles, the additional plastic deformations caused by normal stresses
can reach a considerable value and lead to fracture. Therefore, cyclic
-loading is a special case from which one can get an idea of the corrections
which sliould be introduced in the theory of plasticity in order to account
,for the effect of normal stresses a and an considered in the yield
criteria. 'V
.' Three tubula aluminum-alloy specimens (120 mm long, 30 mm
outside diameter, 2 nun wall thickness) were tested in alternated torsion,
and their elongation (E) and variation in diameter (F-2) were exactly meas -
gs. I and 2,
.ured after each cycle; the results are shown in diagrams (Fi
respectively), where n is the number of cycles, and lines 1. 2, and 3
stand for specimens. Specimen I was subjected to 69 cycles, and speci-
mens 2 and 3 collapsed after 21 and 26 cycles, respectively. As the
.thickness of the specimens could not be measured exactly, no comparative
evaluation of the Prandtl-Guest and Schleicher criteria can be given, since
according to the first criterion, the thickness must be constant, and
according to the second, it must change in the same proportion as the
length and diameter. The theoretical considerations are qualitatively
confirmed by the testing. Appropriate experimental investigations are
being continued and their results will be published in. the near future.
Card 1/5

L 44711-56
ACC NR, AP6C
z
8
IC
8

so
Fig. 1. ElongqtLon vs the number Fig. 2. Relative diameter in-
of cycles.,' crease vs the number of cycles.

A.471 1-66
ACC NR& AIW30743
The correlation between the theory of plastic loosening and dislocations,
together with their role in plastic deformation, are briefly discussed. It
is necessary to bear in mind that the formulas expressing both criteria.
which are taken as initial equations in this investigation, describe
quasi-static isothermal deformation. It must therefore be considered
that the cyclic deformations proceed at a slow rate. The po%;sibility of
extending the results obtained here to the cases of fast alternating loading
can be decided after a special Investigation, although the qualitative aspect
of the phenomenon should apparently be valid also In the case of fast
cyclic loading.
It is believed that the final deciqion on the applicability of simple
mechanical models used in the theory of plasticity can be made only in
the future on the basis of the statistical theory of solids, which accounts.
'for their structural defectq; regrettably, the theory is now in A* state of'
.initial development. Orig. art. hast 2 figures and 5 foraiUs. fF_SBz v. 2' no.
SUB CODE: 20 / SM DATEt 29mar65 / ORIG REF: 012 / OM RM 007
he

L08072-67 JD/EM
ACC NRi AP6034146 'SOURCE CODE:_ __U1(/04_2-4/66/0_0_0/005/0103 /0111
!AUT110R: Novozhilov, V. V. (Leningrad); Rybakina, 0. G. (Leningrad)
JORG: none
The outlook for establishing a strength criterion under
'TITLE: _~m 1 ~ex
iloadina
SOURCE: Inzhenernyy zhurnal. lickhanika tverdogo tela, no. 5, 1966,
~103-111 I
> m. In the case of a non-
+ av
central field 6(V + F(1 2))/a
(pE/2n) 7 T d
2 2 a ;k
is found for the virial theorem.
ASSOCIATION: Not given
PRESENTED BY:
SUBMITTED:
AVAILABLE: Library of Congress
CARD 3 / 3

We V.
IIOVOZUWV >and TULUB,, A. V.
"Functional Method in Quantum Field M.Leory,," Uspekhi Fizicheskikh Nauk, Vol 61, No i,
Jan 1-06p PP 53-102.
SUM: 136o p 16

ffHZ VARIATIONAL PIIWWLE AND TRU VIRIAL
THWARM FM TH2 CONTINUOUS
S
t
92S-30(1967
t
JET P 4
e
ov
Me,
,
J
y
.
A gcivorWzation of the variational principle for all
ocAtterift Amplitudes to, the case of the-Dir" equatim

4- '--to prVientol, jm4 tht6 drivil Lheorop farThe mUnuou
Dir ~pettrurrv is doriv*d~ Thor results cxi be uj4Mcd -to
Pic
the twry of Mgh-enorgy al"trort Scattering b)~vuoet.
-(L.T-W,)

. . . . . . . . . . . . . . . . . . .

. . . . .- - - - - --
7-
Jt7-:

101"VP TIIJ-
Variational principle, scale transformation and the r1rIal. theorem
In relativistic quantum theory (with summary in Znglish, p.1511.
. Teste Lea. ux. 12 noo4:5-24 157. (MM 10:4)
(Quantum theory)

AUTHOR NOVOZHILOV YU PA - 2083
;~
k~
~~~a
TITLE *
ae
~f
tjo~n aid the Virial Theorem in the Quantum Field Theory
(Masshtabnoye probrazovaniye i teorema vJ-riala v kvantovoy teorii polya).
PERIODICAL Zhurnal Eksperimentallnoi i Teoret. Fiziki, 1957, Vol 32, Nr 1,
PP 171-173 (U.S.S.R.)
Received 3/1957 Reviewed 4/1957
ABSTRACT Scale transformation here means the trarisfo rmation of the coordination
scale with simultaneous inverse modification of the mass scale x (A --~ AxIA,
m -+ m/A- , M +.M/,L ; here A is real and positive, m denotes the mass of the
mesons, and M the mass of the nuclei. For reasons of simplicity here neutral
meson and nucleon fields are observed. The author here investigates two
cases connected with the group of "scale transformations": a) invariance
of the field equations with respect to this transformation group and the
relations resulting t~.evcfrom, b) the virial theorem which is derivec- by
means of scale variatiun- Tric field eouations for the meson and the nuclecn
field run as follows. D(x,M)y(x'M) Y~ro-/
axt` + M) i'(x'M) - gy5'f (x'm)f (x")'
"
,
( 13 -m
) y (x, m) - - g ~ (x, M) y5 y (x 9 M) 4h 'r (X,M)
These equations conserve theIr form in Lhe case of scale trArtformation if
field operators transform themselves as follows. %y1(x,Y,) =A3/2qj(A,x,m/,k)
?I (x,m) -A Y (A x,rp/A ). The terip, f, 3 is the only nonlinear term that can
be added to the meson equation without destroying the scale invariance of,,.
the field equations. The relations between transformation of the producing
operators a+, b+, and c+ and the absorption operators a, b, c are then
explicitly given. From the invariance of the field equations with respect
Card 1/2

FA - 2083
Scale Transformation and the Virial Theorem in the Quantum Field Theory.
to a homogeneous "extension" x - Ax of the space-time-continuum and from
the proportional curtailment of the mqF-es results the invariance of the
transformation function Ula = (T (-,)). Here 41(4s) denotes the
Heisenberg state-vector, In tnc, -!.,cM-'aase of e:6 -+ +- and i5lL -*. -- the
transformation f t.on Uja is transformed into the scattering matrix
st a . IV An )- In the case of a BETHE-SALPETER-equation a relation
to the nucyeus Q of the equation results from the constancy of the field'
equations with respect to the given scale transformation. The virial
theorew In the case of the presence of exterior fields the constancy of
the above field equations with respect to the scale transformations given
in the beginning, is destroyed. Variation of the scattering matrix 6SIa
, ( - infinitly small) a relation
id then not equal to zero. With ;L a 1+ F
for the summation over the impinging and scattered particles is found. The
integral expression here has the form which is typical for a "virial"
theorem of the quantum theory of the field. "i'lithout illustrations)
ASSOCIATION
PRESENTED BY
SUBMITTED
AVAILABLE
Leningrad State University
4. 10. 1956
Library of Congress
Card 2/2

V~
AUTHOR
TITLE
PERIODICLL
-AMMIL"Ju __V -
56-5-55/55
On the Reduction of the Two-Nucleon Problem to the OLe-Nucleon
Problem in the Nonrelativistic Domain.
(0 avedenii dvukhnuklonnoy zadachi k odnonuklonno7 v nerLlyatl-flst-
skoy ablasti -Russian)
?,hurnal Eksperim.i Teoret.Fiziki,1957,Vol 32,11r 5,PP 1262-1264(USSR)
iBSTRACT The paper under review invatigates the interaction of two nacleons
fixed in the points _?i and ?I and attempts to express the (renorma-
2
lized) two-nucleon martrix elementa by (renormalized) one-nacleon
matrix alements.In this context,the author of the paper under review
bases himself on the.previously published investigations by G.Chew
and F.Low (Phys.Rov.,Vol 101,P 1570(19R,3)) as well as by G.Wick (Rev.
Mod.Phys.,Vol 17 339095 The energy operator has the furm
ii PAI - 0 . aa
H-H +U +U Vo (A)e arfVj.+(A)e_i rk a+ .(A-1,2). Here V4
0 1 2' UA_ ~ e k k
contains the operators OA and T^ which are related to the nucleon A;
the other denotations are the same as in the first of the above pa-
pers.The state with two physical nucleons in interaction with
other 76 is an eigenstate of the Hamiltonian HTC~(1920-~)mrn 0+F,:(
In this context,E denotes the self-energy
0
the nucleon and E,?Q) stands for the static interaction energy of the
nucleons.The sign d-(I41S"I,',S3') characterizes the eigenvalues of
the total spin, of the tctal isotopic &Din and of their third projec-
Card 1/2 tions.As main fanction a,-:item thu axthor of the paper under review

On the Rdduction of the Two-Nucleon Problem to the One- 56-5-55/55
Nucleon Problem in the Nonrelativistic Domain.
selects the Zroducts of the one-nucleon state vectors
Fa(1,7)FB(2,a) J_ with a and 8 denoting the spin char6e indices-The
quantity Fa(lsa,) describes a nucleon with a mesonic cloud and it is
the solution of the Schroodinger Is equation(Ho+u )F(i '7)=E F( 1 T)
At Q-ioothe ap-ove liste4 products are solutions .o1 the'equa?ion
HYCI(19297)- L2Eo+EC(~) 1 17,(1,2,19), (Q_r1-12),and they have the fol-
lowing property of orthogonalitj: (F,8(1,2,T),
But at firde products these products are nonorthogonal and they are
a function of Q. The author is looking here for T. in the form
%Va+ld. it is assumed that the nucleons of the cloud enter with
I
to eirl nucleon into by far stron:,-er interaction than with the o-
ther nucleon.Finally,the paper under review contains a step-by-step
discussion of the computation of the relevant matrix elements.
(ilo reproduction) .
ASSOCIATION Leningrad State University.
PRESENTED BY
SUBMITTED 23.2,1957
AVAILJ,'tBLE Library of Congress.
Card 212

56-4-11/54
AUTqORS Novozhilov, Yu.V.
TITLEj Nuclear Forces and the Scattering of T -Mesons
(Yadernyye sily i rasseyaniye Ir -mezonov)
PERIODICAL: Zhurnal Eksperim. i Teoret. Fiziki, 1957, Vol. 33, Nr 4,
pp. 901 - 909 (USSR)
ABSTRACTs The interaction of two rigidly connected nucleons in the pseudo-
scalar mesotron theory with pseudoscalar interaction is investi-
gated. The main part of the two-body problem is represented in
form of a one-body problem. Only the states without real mesons
and with one real meson are taken into account. The method to
renumber the two-body matrix elements into one-boy matrix ele-
ments is further developed. These are then calculated according
to the method given by Chew, Low. The potential a-2R which con-
sists of 2 parts is calculateds one part is f4 proportional
(f .... interaction oonstant), the other part depends on the
phase of the scattering of 11- -mesons on the nucleon.
Card 1/2

Nuclear Forces and the Scattering of qj- -Mesons
ASSOCIATION: Leningrad State University
(Leningradskiy gosudarstvennyy universitet)
SUBMITTED: March 30, 1957
AVAILABLEt Library of Congress
56-4-11/54
Card 212

AUTHOR: NOVOJILOV,JU.V., TULUB,A.V. PA - 2042
TITLI: The Method of Functionals in the Quantum Theory of the
Field (Russian).
PERIODICAL: Uspekhi Fizicheskikh Nauk, 1957, Vol 61, Nr 1, PP 53-102
(U.S.S.R.)
Received: 3 / 1957 Reviewed: 3 / 1957
kBSTRkCT*. The present survey is arranged as follows:
I. The method of functionals in the Quantum Theorv of the Field:
Introduction: Art Ij The quantum theory of the field and the
functionals. Art: 2 FOX'S method of funotionals: Idea of the
Method, the deducing functional for the probability amplitudes,
the method of the functional and the titatistics by FEW, the
equations for the functional of state. Art. 3) The deducing
functional for the anplitudes of the new method by TAUX-DANKOV.
tivisti
ana runctional integration:
Art. 4) The deducing functionals for -the relativistic functions:
The T-function and the deducing functional, 78Y1flW 13 ampli-
tudes and the deducing functional, th-t function Q.
Art. 5) The space-time treatment of t:29 quantum theory of the
Card 1/3 field and the functionals: The basic aquations for the fourdi-

The Method of Funotionals in the Quantum Theory P1 - 2042
of the Field (Russion).
mensional state vector, the generalizing YOK functional, the
functional FOURIER transformation.
Art. 6) The variation of the operator and the functional
integration of the FERMI field:
In contrast to other methods functional methods permit strict
formulation of the equations for tho field functions and
make it possible to find a formal solution of the problem of
fields that are in interaction. Thin special feature of the
method of functionals is important for investigations of a
basic character and also for the W03?king out of ap roximation
methods (which differ from the perturbation theory5 for the
solution of field equations. At prenent work connected with
the method of function&ls can be subdivided into two groups
(from the point of view of using tho functional apparatus):
works ooncerning the investigation of deducing funotion&ls,
and works that are connected with the use of functional
integration. The idea of the method of the deducing functio-
nal was brought forward for the firat time by the member
of the Academy V.A.FOK in 1928, and was worked out in detail
Card 2/3

The Method of Funotionals in the (juantua Theory
of the Field (Russian).
PA - 2042
in his work of 1934. Thia method van then used for the
olution of st*,eral problems in the course of the years that
;
ollow*d, but it was not applied a=d developed on a large
cale until recently. The most Imlortant development of the
:ethod of funationals is connected. with the introduction
of the funotionals of the exteriox sources by SCHWINGER.
ASSOCIATION: Not given
PRZSBNTED BY:
BTJBNINXD:
AVAILABLZ: Library of Congress
Card 3/3

AUTHORs N oY-aZhk10v-;--M V-.- SOY/54-58-3-3/19
VITLEs On Asymptotic States of Dressed Particles (0b asimptoticheakikh
soatoyaniyakh oblache W kh chastits)
PERIODICALs Vestnik Leningra dskogo universiteta, Seriya fiziki i khimii, 1958,
Mr 3, pp 21 - 23 (USSR)
ABSTRACT: In the present paper the author describes a method according to
which equations for asyr,itotic states of dressed particles with
consideration of the vacuum polarization can be deduced. According
to the Hamiltonian of the meson and nucleon fields, the vacuum of
the interactingYz-fields, and ty means of the creation operators
0
A A' of the dressed particles corresponding to the equations
1 2
1H Ail - E iAi a system of eilgenfunctions H can be composed:
V fA+ H (E + E + . . .)
12-.' A 1 21 2 Y12- .
The operators A + depend on the creation operators
i
Card 113 and ~(-)(x) as well as on the absorption operatorsf

On Asymptotic States of Dressed Particles SOV/54-56-3-3/19
The function Y12_ also depends on the distance R ij
between the particles. If however R ij -300.- it is not transtormed
into a product of the creation operators of the naked particles
which act upon the mathematical vacuum. It describes the Iressed
non-interacting particles. If B i j--), -42 for the asymptotic functi-on
A+A + and tt-us also for the asymptotic creation
12__ - 1 2 0
operators A+, A of the dressed particles, equations can
1 2
be found by employing the cond:.tion that IY12.,. is an asymptotic
function of the H E E R --)04as well as
(H 1) 2 ij
of the total momentum P. As examples were investigated the case of
2 fermions (creation operators A+ and A+) and of 1 boson and I fer-
1 2
Card 213 mion (creation operatora C* ard A+).

24(5) SOT/54-58-4-9/18
AUTHORSt Novozhilov, Yu. V., Frokhoroy, L. V.
TITLE: On the Forces Acting Between Nucleone and Hyperone in Accordance
With the ifeson Theory (0 ailakh mezhdu nuklonami i giperonami
soglasno mezonnoy teorii)
PERIODICAL: Vestnik Leningradskogo universiteta. Seriya fiziki i khimii,
1950, Nr 4# pp 80-92 (USSR)
ABSTRAM This paper deals with the vontribution of P-mesons to the
nucleon-hyperon-potential trithout making use of the perturba-
tion theory. for the investigation of the hyperon-nucleon-poten-
tial the following conditions are important: the computation of
the potential ought to be Possible within the scope of the non-
relativistic theory. It is assumed that in the case of scatter-
ing of 7r-mesone on hyperons the cross section has a resonance
character and that the latter is very considerable so that it is
possible to neglect the not-resonance cross section; if there is
no maximn- of the scattering cross section ofTj-mesons in the
non-relativistic energy range this theory is not permissible in
this case. Furthers the potentials differ with respect to the
Card 1/2 degree of their decrease with growing distance; the velocity-

SOV/54-58-4-9/18
On the Forces Acting Between Nucleons and H,yperons in Accordance With the
Meson Theory
dependent terms in the potential are calculated vith linear ap-
proximation. The meson cloud is of quasi-static character. With-
in the framework of this the3ry of scattering of the dressed
particles, expressions are set up for the nucleon-hyperon
adiabatic and the velocity-dapendent potential and simplified
for the non-relativistic cas-3. The asymptotic expansions of these
potentials are Gomputed. In continuation of this the properties
of the operator 0 are investigated and the possible r9sonant
condition of the scattering of pions and hyperons is determined.
It is not possible to obtain the two terms W 06 and W., by the
perturbation theory. W 09 contains the pion-nucleon scattering
cross section 6'1 or the pion-hyperon cross section 6 2 linearly,
whereas W6,61depends quadratically on 6 i' There are 9 references,
3 of which are Soviet.
Card 2/2

24(5) SOV/54-58-4-10/18
AUTHOR: Novozhilov, Yu. V.
TITLE: Dressed Particles in Quantum Field Theory (Oblachennyye
chastitsy v kvantovoy *eorii polya)
PERIODICAL: Vestnik Leningradskogo universiteta. Seriya fiziki i khimii,
1958, Nr 4, pp 93-106 (USSR)
ABSTRACT: In the introduction different interpretations of cloud particles
are mentioned in brief (Refs 1-6). It is the aim of the present
paper to generalize a method already previously suggested by the
author to introduce independent fields for various "clouds"
taking vacuum polarization into account. The attempt is made to
set up a scheme of scattering in quantum field theory based upon
the concept of dressed particles. Part I of the paper deals with
the general form of introducing independent fields for the de-
scription of dressed particles and groups of particles not in
interaction. Part II gives a description of the dressed particles
with the "free" Iluailtonian being diagonal. This theory is also
applied to the connection of the asymptotic states (van Hove,
reference 1), with the states 9f the dressed particles not in
Card 112 interaction. For this investigation independent meson, nucleon,

Dressed Particles in Quantum Field Theory SOV/54-56-4-10/18
and antinucleon creation and annihilation operators were intro-
ducel for each particle cloud and the basic functions were de-
termined in terms of this operation (6). The expression for the
S-matrix has to contain the weight operator (equation 15). The
"effective" nonhermitian Hamiltonian (16) was obtained. The term
of interaction H12 (equation (19), (20)) describes the effect of
meson, nucleon, and antinucleon exchange between the individual
dressed particles. The S-matrix can be set up in a quite analogue
form to the scattering theory with operator H 12 as perturbation.
A representation, in which the Hamiltonian of the "free" dressed
particle H is in diagonal position, was introduced. It is pos-
sible to d8velop the perturbation method in the "dressed parti-
cle representation" in which perturbation containa only the in-
teraction of real particles. There are 7 references, 1 of which
is Soviet.
Card 2/2

24(5) SOV/56-35-3-271/61
Noyozhilov, Yu. V.
WTHOR:
TITLE: On the Scattering ofIlDressedilParticles in the Quantum Field
Theory (0 rasseyanii "oblachennykh" chastits v kvantovoy
teorii polya)
PERTODICALs Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1958,
Vol 35, Nr 3, pp 742-749 (USSR)
kBSTRACT: In the present paper the author discusses a scattering theory
in which the virtual clouds surrounding the particle are in
all cases taken into account with exactitude. The theory is
based upon the use of so-called basis functionals J, which are
represented as the products of single-particle functionals.
For the purpose of introducing the f-functions the author pro-
ceeds from the total Hamiltonian for n nucleons and anti-
nucleons (which interact with the meson field)
H = H + [H,(i) , Ujj, where H denotes the Hamiltonian of thi,
Card 1/3 free meson field, 11N(i) relates to the i-th naked nucleon anail

SOV/56-35-3-27/61
On the Scattering of Dressed Particles in the Quantum Field Theory
is the interaction operator of the i-th nucleon with the meson
field, which is set up as linear function of the meson-produc-
tion and -&""JhI1&ti0n )perators a+ and a. For the wave function
in a system. of n non-interacting dressed particles in depend-
ence on the meson field ~ it holds thad~(1,2 .... n; a-) =
- J(1,2,...n; a+)Aot where A a is the vector of state of' the
vacuum (The physical vacuum here coincides with the mathemat-
ical vacuum). For the wave function of the system of non-inter-
acting dressed particles the following equation is finally ob-
(1,2,...; a+)A, a F (l,a+)F(2,a+) ....
tained; fa cc a
ap. .
From this e~aation there follows for the basis functioni
- a+ a .... f ; A w (qI9 ; a). A
A q, q2 a q2 ...
The application of the formalism of the scattering theory (ac-
cording to reference 2, S-matrix), in the case of an invest:L-
Card 2/3 gation of the scattering of dressed particles immediately leads

SOV/56-35-3-27/61
On the Scattering of' Dressed Particles in the Quantum Field Theory
to a system of nonlinear integral equations ;or the scatter.119
amplitudes. If no vacuum polarization exists, the equation.~
for the maLrix elements are automatically renormalizea anl ne
matrix elements can be expressed in terms of tte single-
nucleon matrix eiements. In an appendix a formula of tnis ,paper
is discussed. There are 8 references, 1 of wnich is :Oviez..
t~7FOCI:%TION: Leningradskiy gosudarstvenyy universitet (Lentngrad '-tate
University)
UBMI I TTED April 10, 19~8
Card 3/5

NCVOZEaWV, Yu. V., Doc Phys-Math Sci (diss) -- "Cloud particles in the quantum
field theory"a Mscow, 1959. 10 pp (Lenirgrad order of Lenin State U Im A. A.
Zhdanov), 1-50 copies (KL, No 23, 1959, 159)

21(l) PHASE I BOOK EXPLOITATION sov/2825
Novozhilov, Yuriy Viktorovich
Elementarnyye chastitsy (Elementary Parunles) Moscow, Flzmatgiz,
1959. 184 p. 15,000 copies printed,
Ed.: G. F. Drukarev; Tech. Ed.: 0. V. Speranskaya.
PURPOSE: This book is Intended for the general reader with a back-
ground in secondary school physics.
COVERAGE: The text reviews the field of elementary particle physics.
Concepts are presented without the use of mathematics. Recent
findings concerning mirror symmetry, the antiproton, the anti-
neutron, the neutrino, and the nucleon are discussed. No person-
alities are mentioned. No references are given.
TABLE OF CONTENTS:
Foreword
4
Card 1/4

Elementary Particles (Cont.) SOV/2825
Introduction. What Is an Elementary Particle? 5
Ch. 1. On the Threshold of the World of Elementary Particles
Conservation 1,~ws 13
Familiar particles and measures 23
Photon 28
"Hunting" the elementary particles 32
Characteristics of the world of elementary particles 41
Moment of the quantity of motic'n and spin )J9
Ch. 2. First Step3 In the World of Elementary Particles
Discovery of the positron 55
Particleg and antiparticles 61
Conservation of energy or another particle? 65
Beginning of th- struggle for high energy particles 71
Ch. 3. Particles Necessary to Explain Nuclear Forces
Characteristics of nuclear forces 1-6
What Is interaction? The virtual photon 78
Card 2/4

Elementary Particles (Cont.)
SOV/2825
Nuclear forces and nuclear mesons 84
In search of the nuclear meson 89
Continuation of the struggle for high energy particles 96
Mu mesons and pi mesons 101
Ch. 4, First Results
Particles and interactions 108
Charge independence and mass difference 114
Isotopic spin 118
Ch. 5. Strange Particles
Invasion of elementary particles 122
Strange particles 128
Classification of strange particles 131
"Strangeness" 139
Ch. 6, Recent Progress
Mirror symmetry, or the "right" and the "leftit 146
Antiproton, antineutron and the neutrino 154
Card 3/4

21 (7)
AUTHOR: SOV/54-59-2-1/24
TITLE.- Setting up an S-matrix for Dressed Particles (0 postroyenii
S-matritsy dlyA oblachennykh chastits)
PERIODICAL: Veetnik Leningradskogo universiteta. Seriya fiziki i khimii,
1959, Nr 2, pp 5-13 (USSR)
ABSTRACT: An S-matrix for dressed particles is set up on the basis of
Hamilton's formulas but without the use of the hypothesis on
the adiabatic introduction of the field interaction. Thus,
this is the problem of setting up a function for noninterac-;ing
dressed particles or - which means the same - the
of the complete Hamiltonian 9 into the "free" Hamiltonian
which comprises the effect of proper energy and the operat-7
of interaction of dressed particles. The wave function of ',-E;
0 can be interpreted
noninteracting dressed particles f n
the form of the derivations of the generating operators of tae
physical particles, A +, IL+ , X+ , h+ applied to the phy~!--;--l
N R x B
Card 1/3 vacuum T 0. The permutation relations of the operators A~

Setting up an S-matrix for Dressed Particles SOV/54-59,.2-1/24
with the absorption operators 1% have a general form. In gunern-,
the state of the noninteracting particles can be set up by
means of the operators of the physical particles. In the the7y
of dressed particles, however, the existence of an equation
of motion for the field operators which is otherwise mios-L~g
for noninteracting particles is presupposed. As the
consideration of this case is most difficult, a simplifiers
case is assumed where for the calculation of the S-matrix
0 need not be known and simpler functions +(t) with the
Yn
same asymptotic behavior as ?(t), f 0 are sufficient. In this
n
way, th~ author considered in a previous paper (Ref 2) the
scattering theory of dressed particles of which the present
article is a continuation. In � 2, the theory of dressed
particles is considered from a slightly different standpoint
than in reference 2. The metric operator I is introduced here
which plays an important part in theory. In � 3, the explicit
A
expression for the operator G is found, and the equation is
Card 2/3 set up which determines the operator 6 from the effective

Setting up an S-matriz for Dressed Particles 307/54-59-2-1/24
interaction operator 0. Besides, the assertion made in
reference 2 that the structure of the S-matriz is only
determined by the operator U is confirmed. In an appendix,
T'
the formulas for the operator U are derived which in the
mentioned previous paper had been set up without any proof.
There are 5 references, 2 of which are Soviet.
SUBMITTEDs February 5, 1959
Card 3/3

24(5)
AUTHORS: Novozhilov, Yu. V., Terent~yev, 1. A. SOV/56 - 36-1 - 18/62

TITLE: The Two-Nucleon LS-Potential in ti.,e Nonrelativistic Meson
Theor~ (Dvukhnuklonnyy LS-potentsial v nerelyativistskoy
mezonnoy teorii)
PERIODICALs Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, Nr 1, pp 120-139 (USSR)
ABSTRACT: It is of interest to investigate the question as to what
potential that is dependent on velocity can be derived from
the meson theory wi Vout using the perturbation theory. In the
present paper the'Vg-potential is derived within the framework
of a meson theory which is nonrelativistic with respect to the
nucleons. Short mention is made of several arguments against
such a theory. However, in the case of the two-nucleon problem
the here discusse,.'. .:,,nrelativistic method of dealing with the
problem is perfecL_,,, Justified. A favorable circumstance is the
resonance-light behavior of (Tr- N)-scattering. Therefore, the
center of mass of the matrix elements "or ~X- li)-scattering is
not in the nonrelativistic domain, and it is just these matrix
elements that occur in the velocity-dependent two-nucleon
Card 1/3 potential. As to the interaction Hamiltonian, the Pere discussed
.4

The Two-Nucleon LS-Potential in the Nonrelativistic 30'1/56-36-1-18/62
Meson Theory
method of calculating ths potential does not depend essentially
on the type of interaction. In the present paper the potential
caused by pseudovectorial binding is investigated. Calculations
were sarried out on the basis of the theory cf the scattering
of "clouded" particl-es.,Ref 6). He-ormalization ir. calculations
carried out without ~c:rrurbat'_(_r* theory presents considerable
difficulties whic~a, however, do rot arise in the present paper,
because here only the linear approximation with respect to -~
velocity fa used. The probl'em car. then be renormalized in the
same manner as in the st-atic ::ase. The first chapter deals in
full detail with the -initial formulas for the potential, and
in the second chapter the potential is calculated. Details of
calculations are not discussed because of similarity with
potential calculation in the static case. The last chapter
gives a short account of an aeymptotic development for this
potential Wt~. The expressions found for this potential for
the first time make it possible to form an opinion as to the
extent to which the representations cf the nonrrelativistic
Card 2/3 meson theory for (N - N'-scatte-ing ir. the range of low

The Two-Nucleon LS-Potential in the Nonrelativistic SOV/56-36-1-18/62
Meson Theory
energies are correct. The authors thank Member of the
Academy V. A. Fok for valuable indications concerning the
problem of asymptotic potential development. There are
10 references, 2 of which are Soviet.
ASSOCIATIC,i: Leningradskiy gosudarstvennyy universitet (Leningrad State
University)
SUBMITTED: May 26, 1958 (initially), and September 27, 1958 (after
revision)
Card 3/3

S/026/60/000/012/004/C09
A166/AO27
AL'THOR: Novozhilov, Yu.V., Doctor of Physics and Mathematics (Leningrad)
TPTLE: InTo the Depths of the Microworld
PERIODICAL: Priroda, 1960, No. 12, pp. 47 - 52
TEXT: The article Is an attempt to explain to the layman the significanc..e
of Academician Vladimir Aleksandrovich Fok's theory of quantum electrodynami*cs,
as laid down in his monograph "Works on the Quantum Field Theory". The work was
mainly concerned with creating a mathematical model of the quantum field theory
and an approximate method of calculating atoms. For the work Fok was awardedthe
1960 Lenin Prize. Fok developed an exhaustive theory of secondary quantation tc
describe the processes of the birth and decay of elementary particles. An ac-
count of "Fok's C:)lumn", the Hartrey-Fok method and the method of Fok's functic-n-
als is given, together with an explanation of the need for Dirak-Fok-Podol'skiy's
multitemporal formalism. Fok's theory of quantum electrodynamics has subsequent-
ly been polished up and some difficulties removed, but the basic tenets remain
unchanged. His theory of the interaction of electrons with an electromagnetic
field has proved accurate to within millionths when checked by experiment. Thegr
are: I photo, I diagram and I Soviet reference.
Card 1/1

86904
S/056J60/039/005/021/051
k15-o o B006/BO77
AUTHORS: Braun, M. A., Novozhilov, Y4..L,
TITLE: Some Properties of Dressed Particle Operators in the Field
Theory
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 39, No. 501), PP. 1317-1322
TEXT: The authors examined the properties of operators of dressed
particles, which are determined by single particle states produced when
acting on a vacuum. First of all the local relativistic-invariant operator
Q(x) of dressed particles is defined, aqd also the in- and out-operators
and some relations between these are given. It is further shown that
besides a strong limit at large periods (t-*t w) for the production
operators of the dressed particles (which has already been demonstrated
by Haag (Ref. 1)) such a strong limit exists also for the annihilation
operators of these particles; i.e., the annihilation operators of the
dressed particles tend, with t-+� aD,to the in- and out-operators of
annihilation. The examination of the properties of the operators Q,(x)
Card 1/2

86904
Some Properties of Dressed Particle Operators S/056/60/039/005/02-I./051
in the Field Theory B006/BO77
shows that if the expansion in a series for the coupling constant is
possible, Q (x) cannot satisfy the causality conditions in their usual
form, i.e., the commutator of Cx) is not equal to zero on a three-
dimensional surface. The proof for this is based on the perturbation
theory. All considerations are limited to scalar particles of the same
type. There are 5 references: I Soviet, 1 US, 2 Italian, and 1 Dutch.
ASSOCIATION:
SUBMITTED:
Leningradskiy gosudarstvennyy universitet (Leningrad State
University)
May 25, 1960
Card 2/2

3/054/62/000/001/001/011
B102/B112
U7HORS: Trifonov, Ye. D.
uzhoab
TITLE; Axiomatic method in the quantum-field theory and the proper-
ties of symme-~ry of elementary particles
PERIODICAL: Leningrad. Universitet. Vestnik. Setiya fiziki i &himii,
no. 1, 1962, 5 - 10
T2XT: The symmetry properties of elementary particles are studiej, wnicn
result when the following two postulates are added to the ordinary postu-
lates of quantum mechanics and relativistic invariance (I and II): It is
assurned that there is a unique, relativistically invariant, uniform empty
space 10 > (III), and that the energy B,~,ectrum is positive (IV). A
quantum theory based on postulates I - iV has been developed by
A. S. Wightman et al., whose functions are used in the representation
4
W9 ..... 9. (C." - -C.-O S-I'(AC) W,__ .(Ac;~_., Aj._,)-
Card 1/4 S-1 (A) ?(AE)= U(A),?(E) U-'(A),

SIQ') 41621000/00110V-1110 I I
Axioma t ic _,f tnod in the ... B1 02/3112
resulting from the invariance under the complex proper I,Drentz
LI(C) . 9, 9n refer to a f ield with sdin, and U(_'~) is a unitary r,.,-
presentation of the homogeneous Lorentz Group in the Hilbert s-)ace. FroM
the invariance of the analytic continuation of the Jightman functions
under the complex group L+ (C) 4-t follows that the physical theory '-s oil
higher symmetry than would follow from the invariance of the *dit_,htman
functions under the space group L 1.11 1..... . are in-
91 ..... Yn ~n-l
variant under L only in the complex region. In Drder to ascertain
whether there exist symmetry properties of W in the coiplex reCion,
which could be reiresentedas additional symme j properties of 'N in
the physical region, a transformation group R is ietermined, which is
different from L (C) and for which W
+ 91 ..... Yn (RP lpn-1)
flL R(,Pi)",[ q)l .... 9n (P1 ...... Pn-1), where pl = Rpi are Jost points. it Is
ohown that R nan be roprononted as a product of the reil LorenLz --roup
Card 2/4

S/Oa 62/003/031/0jr,1/--11
,xiomatic method in the ... B102yal 12
and of a ~,-roup R0 ; R - L +/Ro, whero R 0can be found with the K o~,ora-
tors of 01) H + F + HI + F1 [H+F-HI-F'I,
(2)
L 4JH - F + H'- F1, K121 JH - F - H'- Fj.
f3
11 1 (M32t M13t M21), H'= i (N,2, N13, N21),
F (Mol, M02, M03), F'=(NOj, No., Ng3)-
0with Euclidean
M and N ~Lre real. Thus, for example, R 1 1 metrics (rotation
in four-sDace) reads D (c) = i + ix(i)- + iK (2)8, , where ~' are real
1 C11 2
parameters; in )seudo-Euclidean metrics (RO) D (Y) + it, Y
2 2
where y is an infinitely small complex jarameter. Thus, the physical
transformation R is achieved by two independent tr4nsformations: (1) the
real proper Lorentz transformation, and (2) Ro which refers to internal
i
degrees of freedom only. It is shown that R can be identified with the
Card 3/4

S/G54/62/ODV0/1-J3
Axiomatic method in the ... B102/B112
four-di-ension~3.1. isospin group. Academician V. A. Fok s t-an,'~e .
1iscussions. There are 5 non-33viet references. T-,,e reference tj t-.e
English-lan~-,uaage publication reads as follows: A. S. '.7ightman. Phys. R,~V.,
101, 86o, 1956. (S. S. Schweber. Introduction to the Relativistic ~,-Iuanvu~.
Field Theory. Row, ?eters3n and Co, 1961).
SUEYITTED: December 20, 1961
Card 4/4

NOVOZHIIDV, Yu.V.; TRIFONOV, Ye.D.
Axiomatic approach in quantum field theory, and
properties of elementary particles. Vest.LGU 17
(Quantum field theory)
the sy=etric
no.40-10 162,
(MMA 15:3)

MVOZHII,OV, Yuv,
Axiomatic theory of the s7umetry properties of elB--entar7
Ow.
particles. Vest. LGU 17 no.16.-5-19 (MIRA 1-5:9)
(Q=tum field theory)

AUTHORs
TITLEt
/62/147/001/012/022
81020
B104/BI02
Gage invariance and axiomatic &ccewto the-quantum field
theory
RERIODICALs Akademiya nauk SSSR. Doklady, v. 147# no- 1, 1962, 80 - 83
TEXT: The problem is whether it is possibLe to obtain a non-zero electric-
charge operator by the transformation A - A + af/ax 9 9j___,~ 91 + iaq f9i
OW tul I", i
on condition that the quantun mechanical axioms are fulfilled, and that
the axiom of relativistic invariance, the axioms of positivity of the ener-
gy and of the uniqueness of the vacuum are valid. The electromagnetic
field A is represented as sum A 1 + Ao gene* the-wightaan functions
W ix,A 11. Here V
9~x,A~ can be represented as sum W 91x,Ao~ + W 9 9~xoklj is
1 0
'the boL.ndary value of the function W 4z,A A describes a spin-0 field,
1 9t i. A,
A., a spin-1 field; f, an arbitrary function of x is an infinitely small
operator and qi is a Heraitean antisymmetric matrix, eq i the charge. The
Card 1/2 1

S/020/62/147/001/012/022
Gage invariance and axiomatic ... B104/B102
complex Lorents group L +(C) is studied thoroughly. It is shown that the
vacuum expectation value in space-time transformations transforms according.
to the K* representation of L+(C). Furthermore, it is shown that Al is
1. 1X_
an M and an M vector simultaneously, and that ~~ is no scalar with respect
to transformations by the generators 9- of L+(C). Further considerations
based.. on these results give 4 a 9- + coast for the charge operator. Thus
12
the charge operator proves to-be anuoperator of a rotation about axis "3"
in the isospin space. Thus, the field A' is the projection of a pseudo-
vector onto axis "5" of the isospin space.
ASSOCIATIONs Leningradskiy gosudarstyennyy universitet im. A. A. Zhdanova
(Leningrad State University iaeni A. A. Zhdanov)
PRESENTEDs June 11, 1962, by V. A. Pok, Academician
SUBMITTEDg June 5, 1962
Card 2/2

S/02o/ 162/147/005/0~10/027
B104 B186
.'UTHOR. L'Iovozhilov, ".1.U. -V.----
TITLEt The group of the four-dimensional isospin and the hypt,rcharge
in axiomatic quantum field theory
PLRIODICAL. Akademiya nauk 665R. Loklacly, v. 147, no. 5, 1962, 6cG - 605
TE.XTs Assuming the conservation of spatial parity, the author enquire3
which symmetry group exists in axiomatic quantum field theory which is
based on the quantum mechanical axioLns, on the axiom of relativi6tic in-
variance, on the axioms of positive energy and of uniqueness of the
vacuum. It is demonstrated that in gauge invariant theories only a
generalized reflection has any sense, and that conservation of thV spitial
parity of the reflection operatur P, of the spatial coordinatt~s requires
L
also conservation of the isospin parity of P L* Transition from. thi group
of the three-dimensional isospin to the group of the four-dimensional i~ic-
spin is possible only whtn tht; isospin parity and, consequently, '%rlen tht
spatial parity is conserved. The charge T + I v is obtainea as s
2
Card 112

The group of the ...
S/020/62/147/005/026/~,17
B1001~36
consequence of tne invariance, of gauge invariance, anG of
the possible transition frcm pseudocuclide,,n inner space to eucl,-aean
space. Y is the hypercharge which is an iroscalar commuta~ing witi,
T3 , 21 Z2-
ASSOCIATION: L~-ninwgradskij gosz~darstvennyy universitet im. A. Zhd,rova
(Leningrad state Univrrsitj imeni A. A. Zhdanov)
PRESENT-',~'D: June 23, 1*/-62, by V. A. Fok, Academician
SUBMITTLI)s June 14, 1962
Card 212

NoMiMjg,,UM,.Vikto"ch; DRUKAREV, G..F-,v red.; LUKIYANOV, A.A.,
W.~ -
--- EeRnno rou.
[glementary particles] Elementarnye chastitay. Izd.2., dop.
Mo7kva, Fizmatgiz, 1963. 204 p. (MIRA 16:9)
Particles (Nuclear physics))

_~ OZHILOVI rueve
Axiomatic theory of the symmetry characteristics of elementary
partiolea. Vest. LGU 18 no.4:7-14 163. (MMA 160)
(Particles (Nuclear physics))

KOVOZHILCNo YU-V-; TERVIVYWO I.A.
The i7ftmawncur-POW, -) grOUP In theory of elementary particles.
..Vest. 147.20- 'nor. IOT5-~i 0650 (MIRA 1g.-?)

NOVOZRIWV Yw-k VIk .0 "Ayk , doktor VIZ.-Platoln. Tilluk, Prof.,
-, t
I L J, . .0 karid. fiz.-matem. rviuk, nauchn. red.
("4LIb-rIt,UM field theory and olemontary particles] Kvantovaia
teoriia polia i elementarnye chastitsy. Leningrad, Ob-vo
"Znanie" RSF,9R, 1965. 39 p. (MdRA 18:10)

NOVOLHILOV, Yu.V.; TERENTOYMI, I.A.
Symetry, of elementary particles in the theory of inhamogenaous
groups. Dokl. AN SSSR 165 no.3:530-5)3 N 165. (MIRA 18:11)
1. Leningradskiy gosudarstvennyy urdversltgt im. A.A. Zhdanova.
Submitted February 10, 1965.

S L ok, PI SER
~.TP.A -~9
-2)
8 L" :7y m. d o no v a

HCVCZEITDV,Ag A. D.
"The Effect of Subliminal Irritation cn the Excitability# Absolute
Refractory Phases ard ChronmW of Muscles*" Cand Biol Sets Moscow State
%dagogical rnst,, moscov, 1953. (R2hBiol,, No 5. Nov 54)
Survey of Scientific and Technical Dissertations Defended at USSR Higher
Educational Institutions (11)
SOz Sum. No. 521t 2 Jun 55

NOVOZHILOVAY A.D.
Effect of direct current of subliminal intensity on the
excitability and absolute refractory phase of nerver nnd
the muscle. Uch. zap. MGPI 16c)',I'L-28 162.
Effect of subliminal rhythmicL,~ excitation on the funct,-,nal
state of the nerves and the mu,cle. Uch. zap. !IG&I 169011~-40 162.
~,'-;,UiA 17~5)