SCIENTIFIC ABSTRACT IOFFE, B.G. - IOFFE, B.L.

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000618620014-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 10, 2001
• Sequence Number: 14
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

Iomp ~ - -- .. . .
Why children got lick. Rabotnit" )3 no,2.,29IF 157. (MUL41:10:4)
(Children-Cwm and hygiene)

IOM, Blyume Georgiyevna
[Care of the sick child] Ukhod so bolln" rebeakom. Isd.Z.,
Moskva, Medgis. 1938. 21 p. ~ (KIRA 13:3)
(GHIUWW-CARE AND HWLM) (PIRDIAIRIC NURSM)

-n-~ 58
;Z:, ~,j
742/5;~~EFFEC~T OF RADI THERAPY OF THE DIENCEPHALO-HYPOPHYSEAL
T
REGION ON THE EXCRETION OF 17-KETOSTBROIDS AND CORTICOSTER-
OIDS IN ITSENKO-CUSInNG'S DISEASE (Russian text) - loff e B.I. and
Zakharycheva A.A. All-Unionlywt.ofE%p.Endo:tM.-,-M-os-e-o~Wl-
PROBL.ENDOKR. 1956, 2/6 (12-0) i
The effect of X-ray therapy of the diencephalo-hypophyscal region in Itsenko-
Cushing's disease on the excretion of 17-ketosteroide and oxysteroids was investig-
atcd. In 8 out of 15 patients with a normal initial level of excretion a 17-keto-
t:r id a dose of 800-2600 r. was followed by a reduction. in the excretion of
t roid:: However, in patients with low excretion rates. the same dose led to an
:
Increase in the excretion of 17-ketosterolds. In I I patients iviih an initially rained
level of 17-ketosterolds, a reduction was observed after therapy. but subpequont
investigation of this group 6-8 months later again rev6aLled a high rate. The change
in the excretion of oxysteroida was similar to that of the 17-katosteroids. No can-
nection could be demonstrated between the mechanism of excretion of the hormones
and the therapeutic effect. Dilman - Leningrad (G)

IOFFEP B.I.

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SS43
FORMATM OF QUANTA AND Or NEUTRAL MES0148
DUWW CAPTURR OF ir 14930113 BY DzUTMONS.
-42
00
lodw A ROM' SOWL, MwevalikovidL Dok!!ft AkM, n4t
-iftw
W
7l.
W10u). (bottiew'd
to at* 44 as 3 "ViAmits (9) d 6 it' -~ ~q
A. Wd 4 i* -4 4 a * y'"dis) d R 4 It's vs. As~,~fi- 090
ft,#* W 604 of 1, Is w0. tm scalar WA tm patsdoi.
WAS"a Ord slow cWtared., walls for ow maut
ma~ $4 (1) is dt(tuy forbidden (uw colittars, twirw
"WOW (Q PMOVII front 00 2 k"1). in the Cm of th*' satim
p"Wosew" W*0011 (1) will "Imp"s W10 (2). Howevir_4 i
co"Pimiss 9141) wwd prq%ftt taiinjdallbif djffjCUjjjtj.L
moo
since it immW reilstre the knowlefts of Um *&" justij,
of tM witain tm raftir Of w"Ion of Wiser foirctis.
A calculmlift in stiods of tlw prolabiltues of (2) &M (31,
PfftifirbStion tredMW of tits several nripinth tit
see
Um mesime theory 09 "to-spin particlm

sivi
1 9 9 q I 4m 01 0 'S w ag
10 on I
u *Aria isiol, 41 It I
0 S
0 1 41 ; 0 0
o a 4 0 0 9 o 0 0

I(MO B. L.
qil-
"*oimation'of Gamma-Quanta and Neutral $09ond Dur-,
ing Capture of "neg pi mesons" fv%~-MeO "s by Peu-
t7erons. .1j" B.I. loffe, A.'P. Rudik, lit',M.
mushkevich, Acad Sci USSR
"Zhur Pksperi Teoret Fit" Vol MI. No, 1,~pp 11~,Qq
A brief exposition of results.'~ of preseni,~ vork. ~~wis
published in "DokA)u~ Muk:: SSSR" Vol: LXMI, 195
403,- CalculateVthe probability. of "9Am1m's~+quazt%
formgtion during capture of, j('6!mesdhs bj~;Aeu*000'~~
for-varioue variations:of the *sso t of
ticles with. zero spin. , co6iidilisl the *,ture
pseudoscalar mesons an lit c pture~.ofid"iiar'!,!~
d t
mesons. ubmitted. 22,Marw: $I.

~ - - il.
~- .-I
I
I I
I I . . ~i . I I I ~ ~ I

R. 1", Taffe a~d
I VR zur.
of rxen wtions ',ir tbt! pWopmructfcr.,t of ~hnqLd v. cati-
uu-e I.-f T- by ff. wut ic"tes('Ir of as-M.e.r. ~- by -,T (Aso
the mxvitude 4 the r~ UFetinle ~IG` Ste.) coflfd VO be

ed
fitt hl TQvrCSt Wder V-,rtitrbatioci tlte~ry by- u4n.:r j'*ruN-
M-M -i-A tnty tint kind it cuxililinx. but tustrAt
;,-.1doialkir coupcinc :,Mx I affd
K, L. C.

1 ,
Eloctrium produCM4 In tho tlqtjyib of g-M o"m [Ala otduk,

' BE ~L7% Rksp.!, 411
IL ii
C
R
Nil.

A 4W=s~. __21 _.jiakL 52
"Decay of theW. -Hesou:" B. Ioffe, A. Rudik
-DOk Ak Nauk SSSR- Vol L=CII,..Ko 31 350,- -~60
V16- CICICO~AL-U ]J13r11J1mb:Mt7'of 112j&W
vith eadssion of game-quantum and fligll~t.qf.
of decay vithout exp4lsion olf 6~
q=ntktft as a fU=tiM Of the ratio Of A to Ro$
vbwe is the flisbt distance of ,o -meson -d&-U4
the demyj7-?,v+ v. From tbeseone gets the
foLlowing values for the consts:,u 21T U.Ia,IAA.-~- 2T6
wd ~ a a 0. Submitted by Acad L. D. ZAAUU
i Noy 51. - Acknowledges the Interest of Prof 1.
Ts. Pannandbuk during discussion of subject
t' 7 J b

Iol~PE-j B-0 - L-.- - ---- --- - - -- - - - - -
v
I c

j. g~ "IL
-~,ldv Ak,J
x;, mole r
-imflo-
,,.I I 1-1c le kjrTt:,I f. A :1 V n t Ir. ;Iod
1,L., X~." N~ the one-ii,scleon Green s iunclmo j&
4 !it'fR'e Of an e:tternail riucleon sourcv-detisit~ J (4) thij
fxic ronal dt,-rivative eiluatioln rllym.
4 5, 4 5 4 9
til
q i rv
"I Vi ,)kl%cvrt ~A tima

JL
NJ

SUBJECT USSR / PHYSICS CARD 1 / 2 FA - 1517
AUTHOR IOM,B.L., OKUNJ,L.B.
,TITLE bn tie Bui~ing-Up of Fuel in Nuclear Reactors.
PERIODICAL Atomnaja Energija, 1, faso- 4, 80-91 (1956)
Issued; 19-16-195C-
The present work describes a method for the oomputation of this burning.-vup
in consideration of the capture and the multiplication 6f neutrons in the
course of the process of slowing down. In the course of computations the
burning-up of V 235 as well as the accumulation and the burning-up 6f 1fp239
PU239' Pu 240, Pu 241 and of the fission fragments (poisons) is taken into
account. Here the change with respect to time of the reactivity of the reactor
(dynamic of burning-up) in the case of the high burning-up of the fuel for
systems of natural uranium with heavy water as a moderator is investigated.
The work is arranged as follows: Multiplication during,olowing down, the dyma-
mic equationst changes of reactivity, computation of the burning-up of~the
fuel in reactors with natural uranium and heavy water as a moderator.
Summary: The numerical computation of the systems of natural uranium and heavy
water as a moderator show that with a decrease of the reactivity of the
reactor the accumulation of pu240 as a result of the great resonance &b-'
sorption by the level at 107 eV lays an important part. The duration of the
operation increases considerably foompared with the case that the entire
reactor is cleared out at one and the same time) if the reactor operates.9tead-

Atomnaja Energija, 1 fasc-4, 80-91 (1956) CARD 2 / 2 PA - 1517
ily, i.e. if the channels are cleared out continuously and if at any time there
are channels of any burn-up degree in the reactor. The channels must 6n this
occasion be distributed evenly over the various burn-up degrees. By this the
operation may be prolonged from 1,5 to double its length.
In the case of the here investigated reactors with uranium and heavy water
burn-up degrees of from 3000 to 4000 megawatt per day/ton may be attained if
operation is steady. If only the duration of the operation is intended to be in-
creased, it is not allowed to use the lattice with the greatest probability of
resonance capture corresponding to the given volume of 'tbe reactor. It is more
advisable to leave a certain reserve,in the multiplication coefficient. Hereby
the performance of the reactor is, of course, reduced.
The parameters of the lattice (e.g. the cell spacing), which determine the,
amount of resonance absorption, must ther7%fore be selected in consideration of
two competing factors: prolongation of the duration of the operation (which, of
course, entails a decrease of the quantity and a deterioration of the quality
of the plutonium obtained on this occasion), and decrease of the performance
of the reactor.
In an appendix the cross sections of the fissioned isotopes and the dbsorption
in fission fragments is nomputed.
INSTITUTION:

0 1A
SUBJECT USSR / PHYSICS CARD 1 2 PA - 1868
AUTHOR IOM B.L
TITLE ii~~on Wations,for Scattering and Phatoproduction.,
PERIODICAL iurn.eksp;i teor.fison,fasc-4s 583-595 (i956Y
Issued:' 1957
The present work-investigate* mathematically the diepo'rsioh relations for~thq
scattering of pions by nucleons, the photoproduotion of pious on nucleons, an
well as the scattering of nucleons and antinuoleons by nucleons and,arrilres
at the following important conclusions; The here dencribed:method fcr~the de-
termination of dispersion relations is actually based~npou;,the follo Iwing
assumption: signals cannot propagate witg a velooitk that Is greaterthan that
of light. All other points of view of the investigation we.Te only of a stoona-
ary character and could, if deeiredg be replaced by 6ther,oonsideratione which
are not based upon the $-matrix in its present form.:;,The following -problem is
therefore of considerable interest: In it possible to demand that these con-
ditions be satisfied for microscopic distances or is~it possible to be content
with macroscopic distanceiihere such conditions without doubt hold good ? The
present derivation furnishes several arguments in favor of the latter possibil-
ity. In this case it is actually assumed that the range of propagation of inter-
action is not limited by the cone of light, but that it reaches a little beyond
it. The author assumes here (and this is important) that,a condition that de-
stroys causality is imposed upon an interval. Thus#1the following expression
would apply e.g. in the case of the scattering of pions by nuoleons:for'the

V
Zurn.sksp.1 teor.fis,.;1jfasc-4,562-595 (1956) CA31) 2 2 PA 1868
amplitude of scattering in a forward direction: ik'j
dird djK+
f + (0j ) /r
2 2 2
+
In the model,under investigation the disturbance of causality in a sitilAo-
main does not disturb the entire course taken by the 'roof;~ Howevero'a differ-
P
ant choice can be made with respect to the condition that disturbs 68~lsality
in that it is not imposed upon an interval, In this w y it may generally'be
expected that then the dispersion relations no longer hold.
The following.oonclusion is thus arrived at: If the experimental data are-in
contradiction to the dispersion relations, this probably Misans that, the signals
propagate at short intervals with supersonic velocity. However, agressient with
experimental data as regards dispersion relations therefore by no means excludes
a disturbance -of causality in the case of short distances. The extension of
Interaction in above all possible between two points which are loce,14d not with-
in the colne of light but within a hyperboloid.
INSTITUTION.,

T F F
SUBMT USSR / PHYSICS CARD 1 / 2 PA - 1S95
-AUTHOR OFFE,B.L., POM3RANCUX9I.JA.v RUDIXtA.P.
TITLE The Diip-ersion Relations for the Scattering of Pious byMiuterons#
PERIODICAL lurn.skspi t7orofisq.Ltfasol.4,1~2-713 (1956)
957
The present work investigates the elastic soattering of pioAs;by dsutoioni Vith
the scattering angle 0. The dispersion relations whicli~oorrospond to ih;Ls 'pro-
coos differ &# follows from the dispersion relations for the scattering of
pious by fro* nqol*ous: Firstly, the dispersion relationa depend on the polar-
isation of deuteron; and sooondlyt only one single disporei6n relation, for the
sun of the scattering amplitudes of positive and negative pious is olitained if
COULOINDIS interaction is neglected.
Let the real- and imaginary parts of the amplitude ofthe 60attering'of pions
with the energy &j by deuterons whose spin projection onto,thQ direoll Ion of the
motion of the pious is equal to ml be denoted by Dm(6j) and AM(W ) rie.speotiT#ly.
By using the connection between the real part of the amplitude of scattering in-
to the angle 0 and the total arose section JLM(W) - (k/4X)11M (CO ), (orhore'
2 2 2
k 'CO _4~m applies and 4L4 denotes the mass of the meson), the following equation
ac I '&c'
is obtained by the ordinar method for the determination of dispersion relations:
DM(W Dx(eL (2k2/ (.' W + (k2/2x2 m
(_.5(wj"2_ 4j 2) 2_ 2
fkl
0 ki

Zurn.ekspA t9or.fisq31,faGo-4P712-T13 (1956) CA" 2 2 PA 1895
For the determination of the contribution originating from the domain.
0 4 the following expression is used:
A (CO X T111. (W I f 26 [ Cjt 2/4M) _ f2
0 - (k Al - Rove if
denotes that.matrix element which corresponds to the aa'ptur* of a pi6xil by:a
deuteron in the state m with the production of two homogeneous nucleons &Ad,.no-
montum f of the relative motion. This matrix element is explicitly wirittei
downlit differs essentially from zero only in the domiin f:- k/2. Alto the
nMILTONIAN of the interaction between two nucleons, which is requir,od here,
in written-do*n in a general form without taking tensar forces into account.
The dilap*rnion relations determined by means of this UMILTOSIAIT for dents-
vans which are polarized parallel# antiparallel, and vertical to the inciding
bundle are written down. They.oontainp apart from the"constant g, certain
effective values of the potential energy of the interaotioi between two
nucleons in different states. It in from these offectiYe values that ~.ho~
amount of the pole term for deuterons which are polarined vertical to in-
aiding bundle depends essentially.
INSTITUTION:

---- r- -~c _;F--. 1-1 -111-11-1.11
.~ n - E y
., s: av., v. B., J~ 1, ~TUDT .1
._11, L,.) -1 i.
(Acad. Sci. USSR

CZECHOMVAKWNuclow Physics - ftelftr Power and Tvchnolofi7:
Abe Jour : Ref Zhur - Fizikap No 31, 1958j, No 509
Author : Joffe B.Lop Olnmp LB,
indit rwrffv~*~,,
TLt1s On tM Conomption of Fuel In ftelear Rmwtors.
Orig Pub Jaderns energies 1957j, 3* No Op 160-177
Abstract Translation from the Awlane See Went z1gur nakap "195T.-
No 4. 16710.
Card

ImAV E 1,11 V P!.!'2 11

J-0mr 11-T.- [Ioffe B LO); OKUNO L.B. (Oli,mj, L.B.); BOHALp L... inz.
[Irans tor
Bulming out oi%#Win nuc3.ear motors. Jaderna onorgie 3 no.6:1 68-
177 Je 157o

USSR/Theoretica Physics - Quantum Mechanics. B-4
Abs Jour Referat Zhur - Fizika, No 1, 1958, 162
Author loffe, B.L., Okun', L.B., Rudih., A-1P,
inst
Title Concerning Nonconservation of Parity in Week -,im I-actions.
Ori g Pab Zh- eksperim. i teor. fizW,',1957, 32, No 2,;tk1-397
Abstract It is indicated that if invariance with respect OR* charge
conJugation takes place in the case.of veak 1A ions
theu the effects noted by Lee and Tang (Refer~t A-Lur Fizi'-
ka, 1957, No 6, 16485), in -wtich. nonconservation -f-, ]*rity
appears, vanish) since the dbrresponding
terms vanish. By vay- of coWles, the auth6ri ..;o4ider
the decay of hyperons and the beta-decay.9f zed nu-
clei and shov that the invariant requirement with respect
to the 6arged conjugation leads to a vanishil g i-);'iail the
effects connected with the nonconservation, 'of -!u;Wtyp It
is noted that experiments by Wu et al.
Card 1/2
.. ............ .
Abs Jour Ref Zhur Fizika No 1~ 1938) 182
(Referat Zhur Mika, 1957, No 12, 29853) are J i e. M-7e
aminst the conservation of 'charge parity in Visak It
er-
actions.
Card 2/2
i Ai
1019;oe
USSR/Theoretical Pkwics QuantunP, MacbWics- B-4
Abs Jour Referat Mur Fizika, No 1, 19.58p
Author Ioffe, B.L
Inst
Title C"Ceraing Two possi-tin SdtAsimea of Parity N(Zd,onsft~yation
in Weak Intewactions.
Orig Pub 27a. eksperim- i teor. fiziki,, 1957P 32, No 5) 1246-1M
Abstract 3:t, is shomm tbat in t~~P- first approximt-ion iA vesk inter-
action, in the cac-e 1&em time parity is cow6i.-Tv.,di I:rOversal
f the sigas of all tt-,:~ M=Znta =d &. :~~Oj ~tions
o th eptt ec
causess the. real:, pd-rt o:!f -the mat-c-iX elemea-t 'to change its
eiga, w~Lile tale t-mgirw~v p&rt does not &Leage- its sign.
-if cbw,ge paxity is howeveri exalpgous changes
I -lull te Ice. upon dbange:of sigm of
iri the Matrix cli~:Ilf PI-9
Oaiy tue Spin P?~-0-14--tCtior---. On the bilaia of th.ese.-Conside-
rations, thF. typ(-.,s of angulw,- diatz:,ibutions of pol&'rized
particles w.,e fc-yr- AO pe-rticle dK-ays, 9'Qr Won
Card 1/2
L

IOMO B.L.
rw~~ aftp6ie Of PoWsed 14 -inesons by nualet, Zhur. _~~Np, i toor, ~Ivo
o (XMA 10t9)
0-1008-309 JI 057.
n
(masons-captilre)

AlutliOR IOFFEpB.L# 5&7-W66
TITLE On the Capture of Polarized Negative Jdyons by, Ifucl0i.
(0 zakhvate polyarizovannykhdZ-mezonoy yadrami - bt4ssian)
PERIODICAL Zhurnal Eksperim.i Teoret.Fiziki,1957.-i Vol 33, ffrlp PP 308-309 (Ussit)
ABSTRACT The theoretical investigation of the capturej;:of polarized negative
nyons is interesting because it is possiblel.:%7hen;comparing theoreti-
oal with experimental results, to draw conclusions with respect to the
character of the weak interaction of myons with t~e nucleons.The auth-:.
or here investigates the capture of a totally polarized myon by a nuc-
leus. The Halmiltonian of interaction is here written down in form
of a totality of 'all 5 varieties of the interactjontH*-(1/2),E.1gi
(TnOiTp ) (Ty (1- O)Oje, )+ herm.conj. (i-k SpV,T :FA*P) ii ..,.
The neutrino is here considered to hivre two components. By !taking
the four varieties S,V,T and A. into account it i,s possible,to go over
to nonrelativistia approximation with respect to' the nucleans..The
pseudoscalar variety vanishing in thenonrelativistical approximation
furnishes a contribution only if the coupling oonstant g is =ch
greater than the coupling c6netants of all1iother varieti s-. An exp-
ression for the Diatrix element, which is coiaput~ed by using the above
expression, is given. The share of this matrix element is"then Com-
puted. The author here investigates the moot frequent of all cases,
Card 1/2 i.e. that in w1hich on the occasion of the capture of the negative

zed Negative MYOnS by Nuclei- 56w7-WfA
On the Capture of polari . vron-s pro
3leus are create&. The neu,
ron and a recoil nU4 is inversely
myon one neut of this capture (their~moment'llm the same (or
ducecl on the.occa8ion he neutrino) must mainly have theiangular
directioned to that of t -hat Of the spiu'Of the myon. For
3posite) direction to t I _a cose, where 0 denotes the
01 as dwAQ - the.neutron alld the
distribution the formUltion of the emission or p,, eudo -
the direc ect rial, and-
ngle bet-Keen he soalars v 0 Lnd exially
a, mycn. In the case of t ho-tensoVial 0 c1 by
spin of the 13.,j. In the case Of t .not be 006-2utc
vectorial varieties, val-me of 6 can, in generalt the. a,-
riety the iven here. Fxperiaental measuring Of
vectorial va formulae 9 ,in the upper.part of the spectrum)
means of the th an energy legative my ons in light
9.1., distribution (w! capture 4 polarized I
n the I Occasion of the tinguish betWeen the different 'Va-
0 leons.
nuclei makes it possible to dis and r-uO
tivO myons
between nega
riants of interaction
(Ijo illustrations)
A,SSOcIATION Not Givens
PRBS~;IjTLD BY
SUBuITTED 25.4-1957
jibrarY of Congress
Card 2/2
A/.z
ISO
Olt
59
iq lass
of
as sp
01 so
'too 0
~1.54
Do )-o" v"4,
6-T, t of
lot 080
.6a4v - %t0
ale t"to v.0
resl& so 0,
;016
Sao 664- 1 00* ti
Vo
0
0041 6% 0
eto
0
6$!o
lem
A40 9 0010 6. 5160
PT Voo-
o .16 ~41?! ) 6`6
* "~l %a , ;i
'910, irVr ! !~;
6 0% ;~. -~~ ,
. I ~ 0 jj~,60
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to, 60000 0
30
vols
oil,
co~
010~ v4et
-4hande of
Ar
a
"partj6le 0an Is*I
4 to a
~bse"ed-.'The uthors of the
-all deal with the t1oatlering ~f
r, --inb field of the nuclous. i The Intera;1bi
'form of V (Z02 on
fs The
41itude Is deriYed in nonrelativi s tig *Born appro-
differential cross ge0j;jOn has the following~form,
--the spin of the A -particle equals 1/2):
CAU 2/3

TOFFE)B.L.
"Homogenous Natural Uranium Reactor With Recyclinji of Plutonium
Produced", ( a paper to be presented at 1958 UN "Atoms-for-Peaqvill Conference,
Geneva., Switzerland.).

0.11401111111fts
r r Fi
-Rompnews atural'uranium- Reactor With Recycling of nutadus Producei
paper to be presented at ftd UN Intl.' Coa. cc the PMefUl uses of Atomic
Ifterfai, Omwal 13 Sept 58.

BMWTETS?aij V. B., ICFFE, B. L., RUDIKI A. P. and TER -MARTIROGYAN,.K A
(Acad. Sci. USSR)
"f3-Decay and Non-Conservation of Parity," Nuclear Physic-S, Vol- 5, No- 3,
Feb 1958 (No. Hollzmd Publ. Co., Amsterdam)
Abst:, Effects due to non-conservation Of parity such as longitudina.Iand transverse
polarization of 0 -electrons, angular distribution of 19- electrons ~from an or*+,ed
nucleus (including the case when the direction of the recoil nucleus momentum i's fiYed)
are examined in the prexent paper for the cases of allowed /3-transitions and first'
order forbidden transitions'. It H shown that owing to the influence of the Coulomb
field the magnitude of these effects for forbidden transitions in li~alq and intermed-
iate muclei is the same as for allowed transitions, perceptible deviations are
observed in light nuclei (Z 20). In the particular case of a 0-0 transition
comparison with experiment my yield important data on the ccutribution of pseudoscalar
coupling. Unique transitions ( A.7*= 2, yes) for which the electron angular di stri'l-
butioa of oriented nuclei essentially differs from that for allowed tmnsitions are
considered separately.

1211 f a jearx0mallr2we Now.---
-1 U T H 0 H.`~ Ioffe, B. L, Lyublmov, V.. A.
TITLE! Conclusi-ns Yrom the Two-Component *-,"I e~i:lron "lip r ac; t e rin
0-Tnteract-lonr, (0 v-1-odatviyukh 17, d-iijkkikomponeti'tnouti 4) 1 a k
trona v 8-v-zaimodeyatviyakh)
N-MIODICAT.- Zhurnal ekpperimentallnoy t teorotlchell~oy J*ilnki 1958.
Vol, 34. Yr 5s PPO 1321-1-3-2i (US-3H)
ABSTRACT: Most recent measurement's (fiefu 1 1)4' thil 1O.n91t0d1nr.L
polarizavion of electrons in the P--dtv:jiy 8K.0i thq% the
amount of the long1tudinal polarlzation
An analysis. revealed that the nonuniqueness of the
solution may be of the nature of virti~al or the
Breit-Wigner levels. K. A. Ter-!'-Martirosyan, A. X.
Logunov, and.Yu. A. Oollfand participated in the
Card 3/4 discussion of the subject. There are 6 references,

Analyticity and Unitarity in the Scattering 76993
of Scalar Mesons on a StaticlNucleon SOV/%-37-6-W55
2 Soviet, 4 U.S. The U.S. referpnc6.sare-, M. Gell-
Minn, Proc. of the Sixthkn. Roch. Conf., 1956;
S. Mandelstam, Phys. Rev., 112, 1344, 1958; L~~
Castillelro, R. Dalitz., F. Dyson Phys. Rev., 101;
453, 1956; T. D. tee, ?Ws. Rev.,' 95P 1329,
SUBMITVD: July 10, 1959
Card 4/4

MM

83736
S/056/60/038/004/0?~/'046
B000050
AUTHORs Ioffe, B. L.
TITLEt Renornaliza ion in the arity Won-connervation Theory
PERIODICALt Zhur nal okeperimentallnoy i teoraticheikoy finiki, 19601
Vol. 38, No. 4, PP. 1263 1275
TEXTt Already several authors b&Y* dealt with qu:sticns!r9latingtO
renormalization in connection with the non-causer &tion afiparity, but as
the author of the present paper says in his introduotion~ this was done
either with a lack of sufficient conpleteness or oUtorrectuess. Therefore,
the present paper again deals with these problens,xix. in a form t.hat:is
as general and as comprehensive as possible. In thicass~of non-con~serva-
tion of parity, the free equations may have a for& that deviates from the
usual one. The author therefore (in part I of the ps'per), first investi-
gates the properties of these free equations (the equations of motion of
the free particles). In part 2 the renormalizition,tachnique (for the re-
normalization of asset charge, and wave functions) 'in developed. As inter-
action with parity non-conservation, the interaction of a charged spin..
zero boson with a fernion field is investigated. In the.l&st part of the
Card 1/2

83736
Renormalization in the Parity Non-conservation S/z/60/~.08/004/0.29/048
Theory BOO /B056
paper, the technique is applied to a concrete example, via. for the pur-
pose of calculating the asymptotic behavior of the dreen'function aid the
2
vertex parts with large p . The "three-T-approximation" equation i:o:use.d
for the vertex part. The results obtained are finally an al~Zed. A diffi~-
culty arisen above all in putting the ronormalized Ohargq *qual to scro,s
The renormalized Green function ham a nonphysical singularity. In the
following, the meaning of equation (3-12) in, above'all,;dealt with and
several details are discussed. The author thanks I. Y&. Po!1trLnch
A. D. Galanin, and G. M. Gandollman for disaussions.,L. D.-Undau is
mentioned. There are 15 references, e Soviet, I British, 3 Italiano and
3 us.
SUBMITTEDt lovembqr 69 1959
Card 2/2

83bG4
S/056/60/038/005/037/050
BOO6/13o63
AUTHOR: Ioffe, B. L.
TITLE! The Range of Application of the Theory, of WeAk, Interacition J?
~PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fiziki, 1960,
Vol. 38, No. 5, PP- 1608-1614
TEM The question as to whether the type of four-fermion interaction in
the theory of weak interaction is conserved at high eneF~gies~' and, if not,
At which energies the type of interaotion,begins to deviate from thatwe-
vailing at weak energies, is to be answered primarily by way.of experiment.
An investigation of the energy dependence of the arose 'sections of weak
processes must, if the type of int'eraction does not va ' with growing~ener
2 2 ry,
give a-g E )curves (g Fe, 10-5/Ml is the weak interaction cotistant, M fig th
nucleon mass . Another possibility is an analysis of rddiati*s lossesifor
various effects observed at low energies. A consideration of, the dimezisionv~/
shows that the weak interaction at F,,l/)fg- - 103 Bev passes over into,a
strong interaction. When the radiative losses are calculated from the weak
Card 1/3

8360
The Range of Application of the Theory of Weak B/056/60/038/005/037/056
Interaction M6/Fo63
interaction, integration-after pulses can be carried out.up to.pulses;
A - 1/fg. Assuming that the weak interaction retains I to form up to
pulses A , the adthor estimates the upper limit of A by making use of ex-,
perimental data. The following effects are particul&rly:suitible for thiS
purpose: the equality of the constants of the vectorial interaction in
and p-decays, the p -a. e + y and P-1~36 decay. The first effect is first
analyzed and the correction of first order in.gA? to th 0 vertex part in the
anuon-decay according to the graph of Fig. 1 is determin ,ed. 90~ first-orde'r
correction to the vertex part results for a P-decay according to the graph
of Fig. 2,,and in the case of a muon decay there Is only ona~if there
exists one of type (;V) ;a) and interaction (Fig. 3) instead of
a (59)(~e) interaction ~Fig. I)* The upper limit of A w,as estimated to be
A~~ 120-Bev. If,the last-mentioned types of interaction, do not exist, a:
contribution to the vertex part is only made by the graphs of Figs 6 and 7.
Besides, the charge renormalization in second approximation isi
carried out by use of Ward' a theorem. A A 400 Bev is obtained in this case.
Next, the author studies the process p --b, a + I which, According to experi-
ments, probably does not exist. By use of th + graphs of:Figs. 8 and 9 the
author obtains A 4 50 Bev. The op, + e- d'eollay of ~ the lowetit
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83604
The Range of Application of the Theory of Weak B/056J69/038/005/037/0.50
Interaction Boo6jn63
2
order with respect to gA (graphs of Fig. 10) gives a value for the upper
limit of A , which is close to 400 Bev- All of these are
carried out in first perturbation-theoretical approximation, .are not
very accurate for the estimate of. A I the error of.A may be~cf the orde~r
of magnitude of this very A-value. I.-Ya. Pomeranobuk a.nd &A, jer-
Martiros an are thanked for.discuesionew L, Be Okun' is mentibned. Theiie
Y
are 10 figures and 10 references: 2 Soviet, 6 US, I British, :4nd 1 Italian,'
-SUBMITTED: December 219 1959
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378,92,
8/056:,62/042/005/043/050:
B 108 %%B 13 8
AUTHOR: loffe, B. Le
TITLE: Violation of the principle A4 AS in leptoti:decay prgqessos,,
no
of X-mesons and thebehavior of weak iitera~tio at high
energies
PERIODICAL: Zhurnal eksperimentallnoy i teoretioh~enkoy fiziki, v-~ 42, i
no. 5, 1962, 1411-1413
'o transitio
TEXT: Experimental data led to the conclusion that the k0 n
0 +
can proceed in two ways, namely K -1W n + a + and
0 +
K + a- + T The theory of weak interactions can be: appiled, to
these processes. From the difference observed between the masses Pt t4s
0 0
K and K mesons, it is conoluded either, that weak' interactions or, the
1 21
leptons cease at energies of.tho.order of,the nual~:6n m4iss# or at t1he
integral (along a closed.path) over the leptons (F nzi"~~ graphs c6 i tai he
no quadratic divergence. There is I figure.
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3,7895
t,-7
B/056/62/042/005/047/05D
B108/B138
AUTHORS: Cribov, V. N., Ioffe, B. L., Pomeranchuk, Id' Ya., Rudik, A.P.
TITLE: Some consequences of the pole shift hypothenis for high-
energy processes
P3RIODICAL: Zhurnal eksperimentallnoy i teoreticheakoy fisiki, v- 42, 1
no- 5, 1962, 1419-1421
TEXT: Some of the relations between the asymptotic values of the total'
cross sections of various processes are established Using the theory of:
the reaction (R) matrices in the annihilation channel. It was found that
in the spin-zero two-particle problem the ratio between any twolpartial'
amplitudes T. is uniform (t - square of total energy)'. inelastic
1k(t)
scattering of two particles yielding one unstable particl *e in the final'
state is considered. The behavior of the amplitude.is determined by the
last pole righthand in the 1-plane. The system 1i + 21", may pass over
into a "quasi-vacuum" state wit 'h isotopic spin T - 0, total momentum
0, 2, 4,..., and positive parity. The state where the pole shift
Loard 1// 3

S/0 56/62/042/005/047/p~o
Some consequences of the pole shift ... B108/B138
I (t) determines the total and elastic cross sections at-high energiest
0
lies between these states At h' energies,the amplitude of the process
* 10M
considered is f(s,t) = r t s 1 (0) - 1. The cross'section of this
0
2));.
process in proportional to -const/(c +-ln(,s/4m he constant c.can be
evaluated from experimental data. In accordance with this-theory,1' .. J.
NX-scattering shows D 3/2 and F5/2 resonances in range 1,0,- 27 A
Bev. No P 3/2 resonance with isotopic spin T - 3/2 was-observed. .Within
the framework of this theory this must be due to the absence of
"quaai-vacuum" states. The arose section of resonance eta-be productions
in processes passing a "quasi-vacuum" state does not'decrease with
increasing energy. This means that such resonances can also be detects Id
at high energies. For nucleon-nucleus scattering processes the relaitio*n
0 2 is established. In general, 6- 2/3
NA NA --A (A atomic nuin-er)
A
but a dependence in proportion with A would not contradict the abo7a
relation either.
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S/056/62/042/005/047/050
Some consequences of the pole shift ... B108/B138
ASSOCI;~TIOlf: Leninqradskiy fiziko-tekhnicheskiy institut;,Akademii nauk
SSSR (Leningrad Physiootechnical Institute of the Acade~wyplf
Sciences TJSSR) (V. N. Gribov); Institut teoreticheskoy.i.
eksperimentalino,y fiziki Akademii nauk SSSR:(Institute of:
Theoretical and Experimental Physics or the Academy 6f~
Sciences USSR)
SUBI~,ITTED; March 21, 1962
Card 3/3

S105616210431001105010'56
B102tB164
AUTHOR: loff e, B. L.
TITLE: The AYL-resonance
PERIODICAL; Zhurnal ekeperimentallnoy i teoretiches~by fiziki, v. 43, :J
no. 10), 19621 341-342
TEXT: The resonance nature of.the N(E)-dependonce~bf the'q mason pro-
duction in the.reaction K_ + P -)A + YL (Bastien et al~' Phy6. Rev. Lett. 0.1
8, 114, 1962) is discussed. If the energy E (expressed in a. m. sj
surpasses the threshold energy (mA + m -166o mev).,~of this reaction bV,
20 Mev the production cross section dyL 0.63+0-'11 mb, ana If
E-(m,+m,, 60 Mev, d