SCIENTIFIC ABSTRACT NAZARENKO, U. P. - NAZARENKO, V. A.
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December 31, 1967
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SCIENTIFIC ABSTRACT
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NAZARENNO Ustin Petrovich; kFANASITEV, N.A., red.; BULIDTAYEV,
_-, ~_.40 "A '
IT. . , tAhn. 'red.
(Operation of piston-type air compressors] Ekopluatatalla
vosduahnykh porshnevykh kompreanorov. Moskva, Gosenergo-
izdat, 1963. 63 p. (Bibliotaka elaktromontern, no.99)
(MIRA 16sio)
(Air compressors)
"I'll T- "I, b..&A
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j-A
k,i: I y7Tr7 -.-.
~.W_ m v To,
".. - - ;7 'n2"
O't% .."I
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19
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--Tsqiwl -0 .1
'ACT 'D Vt '-T%-*J
ft'd)c.,.T tJ*d)u" . -4
11STI.-I tyl ... 1.J."
"T"r.
-%i-~ 'A
A,..Oq
- --A
.11-12 .341. %-34
SIM
111.14-rwo
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-lop"
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T r .1. W.Tv_ "%lot*
1z"n. J~ '664.2bel 00,
P".q
-vt ... 4 '_'t.~ "I So
r:..4 Ou =Tzwtv
Tr.11 acimu
'M it
24 6200,24 640-0#211.6500, 77001
24:6600,24:6700,24.6510 SOV/56-37-6-J1l/4j5
AUTHORSs Lobashev, V. M Nazarenko, V. A. and Ru3inov, L. I.
TITLE: Letter to the Editor. The PolarizqL~ional 13 -
Correlation In the -Decay of CoOu
PERIODICALt Zhurnal eksperimentallnoy I teoreticheskoy fiziki,
1959, Vol 37, Nr 6, pp i8io-i8il (USSR)
ABSTRACT: As was predtcted by A. Z. Dol Jnov (cf., Zhur. Eksp.
I Teoret. Fiz., '35 178 1958~ and H. A. Tolhock (cf.,
Rev. Mod hys., 26, 27~1 195 ), a transverse polariza-
tion of -electrons escaping in a plane perpendi,!ular
Aear spin, takes place dur
to the nu Ing the decay
of polarized nuclei. The authors have investa'ated
the correlation between the transversely polarized
electron and circular6y polarized Y-quanta formed
in the Xdecay of CO U( ^,100 tL Cu). A case was
studied where the electron momentum P lies In the
plane perpendicular to the momentum Tt of Y -quantum,
which possesses circular polarization 0- The spin
Card 1/3 of electron s was anti-parallel to'R. Measurements
Leqer to the Editor. The Palarizational 77001
J'5 -60 Y -Correlation in the Decay Sov/56 -37 -6 -ji 1/55
Co
were made of the degree of the circular polarization
of quanta, which coincide with r~-electrons.
The Zir-cular polarization of -/ -quAta was determined
from the compton scattering forward on magnetized iron.
The substitution of the results in the equation
a ~- 2 (11 - 12) / (11 + 1:!). lj,~ = R, / RpR,;
gave (0-50 + 0.18)%. The calculation with the
aid of the equatlon
IV (o) - 1 + Ac. (1)
Card 2/3
yielded A = 0.32 + 12. The theoretical value for A
is 0.24 (cf., A. R. Dolginov, loc. cit.). This work
was performed under the guidance of A. Z. Dolginov;
Lelter to the Editor. The Polarizational 77001
IV -Y, -Correlation in the fl-Decay SOV/56-37-6-41/55
of C060
ASSOCIATION:
SU04ITTED:
0. V. Saltykovskly, V. S. Andryukevich and A. V.
Kurakin participated in the experimental part of this
study. There is a schematic diagram of the setup;
and 6 references, I Soviet, I German, 4 Ty S. The U.S.
references aret H. A. Tolhock, Rev. Mod. Phys., 280
277 (1956); H. Schopper, Phil. Mag. 0 2, 710 (1957
F. Bohem, A. H. Wapstra, Phys. Rev, 10 456 (19U~;
N. Sherman, Phys. Rev., 103, 16ol ( 1956.
Leningrad Phys.-Tech. Inst. Acad. Sciences USSR,
(Leningradskiy fiziko-tekhnicheskiy inatitut, Akademil
0n%
nauk SSSRj
August 14, 1959
Card 3/3
89197
S/or-6/61/040/001/002/037
20-6610 B102 B204
AUTHORS: Lobashov, V. M., Nazarenko, V. A., and Rusinov, L. I. (De-
ceased)
TITLE: Py-P:)larization correlation in the P-decay of Sc46
PERIODICAL: Zhurnal eksperimentallnoy i. teoreticheskoy fiziki, v. 40,
no. 1 , 1961 , 10-12
TEXT: Within the framework of experiments made for the purpose of verifying
the T-invariance of the 0-decay, the Py-correlation in the decay of polar-
ized neutrons and the Py-correlations in the decay of orientated nuclei has
already been measured, and it was found that (with an accuracy of 4
15-3CV6
no imaginary part occurs in the 0-interacticn ffamiltonJan. The amount o~
this correlation in these experiments depends on the imaginary part of the
interference VA termsj as, howeverp an S- and T-admIxture could hitherto
not be excluded, this should also be teken into account. This was the pur-
pose of the present paper. By trying to estimac the amount of Im(VT, SA)f
the correlation between the transverse polarization of the electron and the
circular polarization of the gamma quantum were experimentally determined.
Card 1/5
n(II n-7
U7.L7 f
SIO 5 6/61/04 0/001 /002 103 7
Py-P.7larization correlation B1021B204
The experimental arrangement is shown in Fig. 2. A theoretical study of
the correlation coefficient K for allowed transitions (according to
A. Z. Dolginov) shows that K depends on the degree of interference of the
Gamav-Taller and the Fermi matrix elements. Thus, Sc.4 was chosen aB a
source owing to its high degree of interference of the matrix elements. The
electrons goming from the source (S) are collimated on a bismuth film
(0-5 mg/cm4), scattered through -1350, and recorded by means of a scintil-
lator, which is connected with the photomultiplier via a light pipe. Owing
to the azimuthal asymmetry, which is connected with Mlott scattering, the
,,, r-O _v
beam of the scattered electrons is polarized in the direct P P P,
1 #21 1 ( 'a
the momentum of the electron before, and P. that after scattering). In cr-
der to increase counting intensity, Circu lar geometry wqs used. The circu-
lar polarization of '-,he I-quanta was measured by means of the method of the
Compton forward scattering on magnetized iron. The outputs of the photo-
multiplier of the 0- and y-detectors were connected in fa3t-slow coincidence
with 2-v . 1.8-10-8 sec. From the measured results A - 2(1 1- 12)1(,1+,2)1
11,2 ~ R coinc /aPRIwas calculated, and thus K - 41P IPP was determined, whem
Card 2/5
d9A.Y
S/056/61/040/001/002/037
Py-p-larization correlation B102/B204
P and P Pare the efficiency of the y and P-pclarimeters. One obtpined:
6 (+0-15 � 0-11)~, and herefrom the correlation coefficient was found to
be K - 0.00 + 0.06. The experiments were repeated ty means of a thick
scatterer ('5mg/cm 2), from which it followed that the experimental arrange-
ment had no eaymmetry. Thus, it was found that, as
K - + 0.04 with Im(VT,AS) - 0
K a r+ 0*23 with a maximum Im(VT,AS)
tr 0-15
is Im(VT,AS) . 0 with a statistical accuracy of- 30~j. For the purpose of
checking the exper mental method, also Py correlation experiments were
carried out on sc4~ and C060, and results were obtained, which showed good
agreement with those obtained by other authors. The authors finally thank
A. Z. Dolginov for discussions and for his interest, 0. M. Saltykovskiy,
V. V. Andryukevich, and A. V. Kurakin for the experimental assistance.
There are 2 figures and 5 references: 2 Soviet-blo,7 and 2 non-Soviet-bloc.
Card 3/5
8Y197
S/056/61/040/001/002/037
py-p)larization correlation ... B102/B204
ASSOCIATION: Lo nin~radskiy fizl.ko-tekhniche!,kiy institut kkademii nauk
SSSR Leningrad Institute of Physics and Technology of the
Academy of Scienaes USSR)
SUBMITTED: June 22, 1960
Legend to Fig. 2: S - sourcel 1) electron scatterer, 2) plastica
scintillator, 3) light pipes, 4) vacuum chamber, 5) outlet window for
y-quanta, 6) magnet of the y.-polarimeter. 7) photomultipliers.
Card 4/5
3/056J61/040/001/002/037
PI-Polarization correlation B102/B204
2,
Fig.
Card 5/5
LOBASHOV, V.M.; NAZARWO, V.A.
Studying the docay of PrW+ Irl the &-correlation wthod.
Zhur. eksp. i teor. fiz. 4.1 no.5:1433t-1J.37 It 161. (MBUL 14:12)
1. LenlWadskiy fiziko-tokhnicheskiy institut AN SSSR.
(Praseodymium-Decay)
(Quantum theory)
3~635
Lo
(Z' ri 7 1 C, n, the (,-re n
Cf (
ri
r c
r. a I
A L
c oe
or
.
A' r
, u" cl .
P.- a !I-,M ;j on
:3
rt
FA S
64 )1:7
k
a mcln
d e fl
,
a s f r cz, a r, r," rey - e T) e n
r
o un o
r a T m v, r
-
r c i e n,,
.
iv t:G
f a3 2
I T
F~ kk~ 07)
s t 7!
AA ,3 1 r
1 3 n
N
r, i k r in-I F
lie r Ft I n H H 1* r 0 f,
r~ n ir j -t
Ll
3~'056/62/042/0012/006/05
Inve.,itigation of the dcpendence ... B1021BI38
Morita. Nucl. Phys. 14t 106, 1959.
A S!7 OC IAT I ON: Leningradnkiy fiziko-teklinicheskiy JnAtitut Akademll nmuk
SSSR (Leningrad Physicotechnical Institute of the Academy of
Sciences, USSR)
SUBMI TTED: July 21, 1961
LeE,end to Fig. It (1) Source, (2) stilbene crystal, (5) NA(TI) crystal,
~4~ light pipe, (5) lead collimator, (6) lead shield, (7) dinperning MRejlPt,
8 jacket of Armco iron, (9) Permalloy jacket.
Card 3/3
5/0 5 6/6 ?/04 2 j"0, r) ~" /0 1
AUTHORS; Lobashov , 7~ M, . NazarenkoL 11
TITLE. Py-correlation in Mn 50 and F20 0-dt'L;iYq
PERIODICAL. Zhurnal eksperimentallnoy i teoretichenk~)-., ftz,~ki %
no. 2, 1962, 370.374
TEXT. From the #ell-known Mn 56 _7 Fo 56 decay the ~-traruj', t. ion wi th I iri.4 ttu!
spef~triva energy of 2.86 Mov was atudied in detail , Thic tranaltiori tak-r!
plac.e to the first excited lovel of F956 which goes cuer to thp Frnilni
atate with emission of an 845-k(.-v gamma quantum. (3' -4-2* -Y---'>C';
log ft . 7.2). The angular correlation of this (alloved) tran3itori va,-3
measured with an apparatus similar to that described by Steffen (see rel W
The source was obtained by irradiating Mn55F-, on an Al ba,ikin~:, with
1~1013 neutrons/cm -2 sec -1. The Velectron8 were detf-cted *~th a atil~en-
oryatal and an PJ-36 (FEU-36) photomultiplier, the gamma quanta witK -n
NaI(TI) cUstal and an 13~-13 (FEU-13) multiplier. Both multlpiis~rq hikd
Armco and Permalloy housings. The NaI(TI) crystal was lead shi-11ed,
Card 1/3
56 S/056/62/C-i'!-/CC,,/C!
Py-correiat..on in tin a nd B102/B!3b
against scatfer-id ~;amma rays The multipliers were c,~nn,--
c~oincidence circuit with a time resolution of 6. 10' 9 ai~ - .
,oincidence background was '-(~; An anisotropy cf the ;~ir,-7jlar
tion was observed. 'H(g) - I + A2 cne4U. the ariisotroj,y fi-t,jr na6
A2 - +(0,,022 f 0.005); 9 Is the an(;Ie between P-electron and ,amzn judo
momenta. Inner br,~msstrahlung and multiple scatte-ing are
-0,20 The
,orre-."ion for asymmetry due to yy-coincidences wari
tion between O-electron emission and circular polarizati---~n o" thf~
quantum was determined for the same O-decay component The -orrelq~--r
factor for the Gamow-Teller transition was found to be f~-' ~L-
soquence of spin levels, the nutaeri,-,al value was -,'0.80 - C,C6 vP- r~
angular anisotropy and the anomaluu3 mat,;nitude of the
tion car, he explained from estimates of the seccnd forbidder.
Measurements were alao made of the pclarization ypy correlati7-r. In
F20 P -decay. For the F 20 ground atate. spin and p,rity w,~r,4 fri,ind
the correlation factor was -,alculated as -0.,12 10,2' its Mearju:--el J'-'1 I-
-0"!(),
0~14 + 0.07 Professor D, M. Kaminker is thanked for inte:-ev~ V V
Card 213
56
Py-correlation in Un and
S/056
,/62/042/002/010/055
B102/B136
Andryukevich, G. D. Chuklin and V. B. Belyakov, W~ V. T[mofeyev and V. I
L'vova for help. There are I table and 15 references: " Soviet and
13 non-Soviet. The four moat recent references to English-language
publications read as follows R. M., Steffen. Phys- Rev. Lett., 3, 277,
1959~ J. 11. Hamilton, B. G. Petterson. Bull. Am. Phys. Soc., 9, ')~ 1'1')9'
M. Morita. Nucl. Phya., 14, 106, 1959- P. Dagley, M. A. Grace. J M,
Gregory, J. S. Hill. Proc. Roy. Soc., ?50, 550. 1959,
ASSOCIATION; Leningradskiy fiziko-tekhnicheakiy institut Alkademii nauk
SSSR (Leningrad Physicotechnical Institute of the Acadpmy
of Sciences, USSR)
SUBMITTED: August 8, 1961 (initially), February 5. 1962 (after reviaic6
Card 3/3
8/05 62/043/005/005/058
B163Y3106
AUTHORS: Lobashov, V. X., Nazaranko, V. A., Sayenko, L. F.
TITLE: Determination of the spin of Eu152m
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 43,
no. 501), 1962, 1579-1581
TEXT: The 0-t' correlation between the mom6ntum of the P-electron and the
circular polarization of the 1.327 May/'quantum in the allowed branch of
the Eu152m 0-decay with a O-electron end-point energy of 560 key is
measured. This P-decay, whose frequency of occurrence among all decays of
152m 152
EU is 1.2%, leads to the 1.515 May excited I- state of Gd . The
measurements were made with an apparatus described earlier (V. M.
Lobashov at al., ZhETF 41, 1433, 1961), then used for investigating the
similar Pr144 decay by an analogous experimental procedure. The Eu152m
souroe was made of about 1OOpg/CM 2 europium oxide on an Al backinl/foil,
irradiated in the FTI AN SSSR reactor. The value of A -201 12 (11+1 2)
Card 1/5
i 52m S/056/62/043/005/003/058
Determination of the spin of Eu B163/B166
is found to be +(1.6 ! 0.4)% where I R /R A ; H and Rj,
1,2 coine Y 0 colne
denote the counting rates for coincidences and single pulses of ther
channel respectively,and 4 P is a correction factor for the influence of
the magnetic field on the 0-channel (0.03%). The subscripts I and 2
respectively correspond to different magnetization directions in the/-
polarimeter. From this, the correlation coefficient A 1is calculated
taking into account the-background of casual coincidences; also the
geometry and the efficiency of the/polarimeter; A +(0.40 :t 0.10).
- 0 - r +
For the transitions 0 , I ~ 0 a correlation coefficient of +1.00 is
to be expected, but for the transitions I- P, I- r,O+ a correlation
coefficient of the observed magnitude is possible. It is concluded that
spin and parity of the Eu152a isomeric state are 1- instead of the pre-
viously accepted value 0 . The reliability of the applied experimental
procedure is confirmed by the fact that Or, correlation measurements in the
0 decays of Co 60 and Au 198 (V. M. loobaohov et al.t ZhETF 42, 358, 1962)
Card 215
I 52m s/o56/62/043/005/003/058
Determination of the spin of k;u B163/B186
have given results in good agreement with those of other authors. It is
important to know the spin and parity of the Eu152m isomeric state in
connection with the experiment of Go.Ldhaber et al. (Phys. Rev. 109, 101r),
1958) whereby the polarization of the neutrino from the K decay was
measured. Goldhaber's main result i. e. his conclusion on the chirality
of the neutrino, is not affected, but the expected greater accuracy from
152m
further ouch experiments with Eu to dete'rmine the polarization of the
neutrino is diminished. There is 1 figure.
AOSOCIATIONs Fiziko-teklinictieskiy institut im. A. F. loffe Akademii
nauk SSSA (Physicotechnical Institute imeni A. F. loffe of
the ikcademy of iciences USSR)
SUBMITTED: April 26, 1962
Card 3/3
-7rT--
MMIN
or L~,cd I pnen~, t7p,! Zhur ELn a I r.,~
1. Institutu. ct lrlr~rt-!Lnir (A-.Pr-,it;try, I-cwitmmy
Sclencer, in rde.,%ga.
~,, -). M.; WBASHOVP V. M.; V. A.; SAYEMO, L. F.; KhAEUCEVICH, j.
Y3, oROI A. I.
"Relative asuremeM of J~g langityMnal Polortzatioa of Electrona in beta
Z'ecay of P!ra and Zn , Ho and Re , ."
-eporr subtaitted for All-Union Coaf an Nuclear Spectroscopy,, Thilial, 14-22
Feb 64.
2TI (physico Teci~-tical rnst)
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N,WltYEN~O, V.A., I XPVi'!' KAYA.
or I
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Od 0s
I; Iltz"11.701 ITO p V.A. ; FI,IA.':TlKO'/A , G. V.
lolunetric detrmination of In t~.(! "01-.1 rA,
germanic acids. M-r. zhur. 30 rio.7t/62-7UI t 64
(IMILA I F, '. I )
1. In.,,titut ob~hchey I neorpriiclic,.,.~.Oy ~hlml 1 -AT Ukr3ISTR,
1;iborntorli v Odenno.
16~~97-6,r- EP! T O-n
n (r,
67n~
V!, TF) PS -Karminker,12. M.t, Lolbashov, V. 1-1 .bT a z a rn1ko, VA .
TV:UI: Relative measurement of the longitudinal polarization of
.lectrona in Beta decav
C~.QUV'H: Zhurnal E-Ysp-rim(n--, r~(),'. i rizkl, 47,
no., 5, 1964, 1668-1671-11
TOVINC rAGS.- beta decay, electron polarization, electron enerqy,
-i!-r-AL,~ir po)arJAxF'It ion, structu-e
ES TP , ACT: T(-, --hc-c!< ~-)-n thf--a advanc r-~d to f~~Cplajr, !,rime
thM. the i-nternal stru crure o, U-1- t') h'kj:)eI-
-~orrections, the authorc3 att--,~-,nptod to --aqcertAin the -lependence
Card 1/4
ACMS-E'100 NNU AP5000311
meas~*irements of the long itud i nal polarizatio,i Dif electrons, were mea-
-1 41.1 dec,-jy of p32, 111", -1142 166, iB8
sure, - 110 a n d 11 at energy
Ep 1-250 keV. Tha exprLrimentU., comE-~isLed of imeasurinq the Clrcular
~)f th- p-ro--3ucel by deceleration of the
vj Uie z;o-
f elcctrons in a lead tarqp-i-, ur3it '-L~J) J.n j?j'4. 1. C;f
L 1-w- i-mcloliure. The circulai. pol-a-rization of the bre-insstranlung 'Y
quanta of the 1P. electrons of InI.14, Pr 142, F.0166, and Re'88 was com-
r~"-tved '.'tith the circular polarization of the bremsstrablung 'y quanta
r t r nn 5~, Tlir- -nen~rxl wat, (Jeter-nined with the aid
T ,-I
of a maqnetic lens epectra-fter-er.. h, t-- v a 1 (--j 1-
32
I Ma
'u"'inal. polarLzatlon reiative to that of P were 0.960 + 0.0015,
.9 14 +- 0.015, 0.9,~2 + 0.015, and 1.005 + 0.016 for In liz, Pr142
n C! Re rcsPefJ V~' 17, f Or'vj'a-
'.i- tt
A
1-1'rf'ill il-ructure of tht., nij,-
2/4
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L 1 60915-65
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I ab, da a 0
jon,jitudinal p-nlarization do not corrc~latO Vith W-ail -e t n
L r a r) s i or. s, T e
(,-)f the s, p ec t r- a po
'k
i t ho r s, tiank V_j Ltj(n _LiZ. - a n
y
Chuklill for help i~l 1, r, I -p, I I
a 1 --1 o A , Tlmo)-bin fnr part i,:-Liparinq in nrepar,t~ ion r-r tl)e P-
~i,,, d JnlJ,4 sources." Orig. a-.L. hds,: I figure-
ASS()CIATION: Fiziko-taklintcheakiy institut inn. A. F. loffe Akaderaii
nauk SSSR (physicotechnical Institute, Acadcmv of Science!3 SSSR)
SUMUTTODs 23May64 ENCL: 01
SUB CODE: NP
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Semi-wicbochemical. analysis of minerals and ores Moskva, Goa. aauchno-tekhn. Izd-vo khIm.
lit-ry , 1950. 189 p. (51-24966)
QE364.N3
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16, 536-8 150. (an 6:4)
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