SCIENTIFIC ABSTRACT KOROLKOVA, O.S. - KOROLYUK, I.K.
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December 31, 1967
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SCIENTIFIC ABSTRACT
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SOV/48-22-8-19/20
Data Concerning Industrial Photoelectronic Multipliers for Scintillation
Spectrometers
with a sensitivity better than 20p A lm- multiplier sen-
sitivity at 2400 V better than 10 A 1m-1 teroidal dynodes
ofANg K alloy). An FEN with a bismuth-silver-cesium cathode
was aescribed in reference 3. These multipliers give a good
amplification. The amplitude resolution of 10 specimens of FEM
with NaJ-(Tl)-arystal with a diameter of 20 mm and with
C8137 was within the limits of 12 - 14%-
There are 5 figures, 1 table, and 3 referenoeB which
are So-Viet.
Card 3/3
85863
S/04BJ59/023/012/006/009
Boo6jBo6o
AU~HORS: Iferkovskiy, A. G., Breydo, I. Ya., Koroltkovat 0. S.-,
Leytevzen, T., V,
TITLE: Some Characteristics of New Photoelectronic Multipliers
Y
PERIODICAL: Izve3tiya Akademii nauk SSSR. Beriya fizicheskaya, 1959,
Vol. 23, No. 12, pp. 1517 - 1519
TEXT: Two new types of photoelectronic multipliers PY-35 (FEU-35) and
~)Y-29 (FEU-29), as applied to scintillation spectro6ters, were worked
out by the authors. Full particulars are given of FEU-35, less of
FEU-29. The cathode diameter of FEU-35 is 25 and 34 mm for 108 mm length.
To improve electron-optical properties of the input a focusing cylinder
(of. Fig.1) is applied. This cylinder permits better combination between
the axial-symmetric inlet of the multiplier and the inevitably asymmet-
rical first cascade of the multiplier system. The new inlet system
secures a good energy resolution. As much as 600 FEU-35 devices were
checked for amplitude resolution (Fig.2) and for the amount of the
energetic noise equivalent (Fig.3j. Fig-4 illustrates the average
Card 1/3
8
6
58~
Some Characteristics of New Photoelectronic S 048/59/023/012/0013/009
Multipliers Boo6/Bo6o
amplification and the sensitivity of the multiplier as well as the de-
pendence of the dark current on the supply voltage.'The linear depen-
dence of the output signal amplitude on the y-quantum energy is secured
up to amplitudes of the magnitude 10 v for 50 k92 and 10 pF. The sensi-
tivity threshold is about (6-8)-1o-12 lm for a resonance amplifier band
width of 20 cycles and for a resonance frequency of 80 cycles. The
second multiplier (FEU-29) suitable for y-spectrometry has a cathode
with the dimensions 38-48-190 mm. Its amplitude resolution is given
with 7.5 - I(YI.. it exhibits an especially low noise level (1 - 2 kev)
in the 50 iMP/sec level. To test the stability of the photoelectronic
multipliers under work conditionmea special device was constructed,
.1tting measurement of the change with time of the Cs 137 photopeak
perms.
level by means of a Nai(Tl)-crystal. This device consisting mainly of a
one-channel analyzer is described. Fig. 5 presents the photo of one part
137
of the record chart of the photopeak amplitude stability of Ce for
4 FEU-29 multipliers. The horizontal multiplying factor was 0.4% of the
pulse amplitude, the vertical one was 30 minutes. Displacement with
Card 2/3
71494
4/s-o 9/109/60/005/010/017/031
2033/3415
AUTHORS:
Breydo, I.Ya., Gla*61*v 'V.P., Glukhovskoy, B.M.,
Le;teyz*n,
Korollkova, O.S. and
L.Q.
TITLE: Investigation of the Stability of Multi-Stage Photo-
Electron Multipliers
PERIODICAL: Radiotekhnika i elektronika, 1960, Vol-5, NO-10,
pp.16 98-1702
TEXT: This paper was presonted'at the 9th All-Union Conference on
Cathode Electronics, Moscow, October 1959.
The stability,of the output signal from a photo-electron
multiplier depends on a number of factorsi the voltage, the
current, the time of operation*and so on. The purpose of this-
article in to clarify the effects of these factors on multipliers
with emitters of different materials. Since multipliers are
widely used an scintillation counters, the multipliers were tested
in a special set-up which approximated to oserational'conditions
with crystals of NaJ(TI) irradiated by Cal 7 on the cathodes of
the multipliers. Block diagrams of the test apparatus are given
and the apparatus is described'. The output current, which
depends not only on the amplitudi but also on the frequency of the
Card 1A _z:-
S/109/60/005/010/017/031
Investigation of the Stability ... 2033/3415
pulsess i.e. on the intensity of irradiation of the crystal by
y-rays, was also monitored. The results show that there are two
types of instabilitys 1) smooth change in the average value of the
amplitude of the pulses over a period of time and 2) oscillation
of the amplitude about a mean value, which shows as a scatter of
the recorded points for a given curve. The deviation of the
points is approximately 0,3 to 1% of the value of the output pulse.
Early tests showed that the stability depended to a great extent
on the previous history of the multiplier. The "settling-down"
time in different for different specimens and'for the same
specimen the settling-down time on the first day can be very much
longer than on following days. This "training effect" made
investigation of individual specimens impossible and statistical
tests on a number of multipliers were necoaxaryo The results on
80 multipliers of the 403Y-35 (FRU-35) type with Sb-Cs cathodes
and emitters are presented graphically by histograms of percentage
change in pulse amplitude against numbers of multipliers for output
currents of 0.1 to 2.5 microamps, 0,3 to 0.5 microamps and
0-55 to 6.0 microampo. The maxima of these distributions show
Card 2/4
21594
5/109/60/005/010/017/031
investigation of the Stability 0.0 Z033/9415
greater percentage change for larger currents. The results for
60 antimony-cosium cathode and emitter multipliers were similar.
It is concluded that during the first hours of operation the
stability is directly related to the output current and reduction
in the current density improves the stability. The absolute
maxima of the changes in the output current of the multipliers did
not exceed published figures for multipliers with Al-Mg, silver-
magnesium and antimony-cesium emitters. The settling-down time
was found to be proportional to the output current. Testar on
multipliers 1#3W-24 (FZU-24) with aluminium-magnesium alloy
emmiters showed'that they also have, appreciable settling-down time,
but the output current has little effect on it, except that it is
reduced with high currents. For example, a batch of multipliers
with Al-Mg emitters and bismuth-silver-cosium cathodes had an'
average settling-down time of 10 to 20 min, after's rest-poriod
of 12 hours with output currents of 20 to 30 microamps. To
clarify the effect of activation by cesium on the stability of
alloy emitters, a multiplier with a thermo-cathode was prepared.
The stability of the emitter was chocked directly in a vacuum with
continuous pumping before and after cesiation. The relative
Card 3/4
rN, R
21594
S/iog/60/005/010/017/031
Investigation of the Stability ... 3033/9415
changes in the secondary emission coefficient for thermo-
activation and for cesiation, for one stage of a copper-beryllium
alloy with 100,V and 0.3 mA output current are shown graphically.
It in seen that the presence of cesium leads to an increase in
both the nettling-down time and also in the magnitude of the change
in the secondary emission coefficient. There are 7 figures and
2 reforenc*ms 1 Soviet and 1 non-Soviet.
SUBMITTED: December 21, 1959
Card 4/4
143Y till 11 J ~A y v I"r i"', IY f J
yy
T Ul' r
3T3- 1'~;
KOROLINJVA, T. A.
23596.
0 BYSTRM KOLEBANIYaKh
USILIVAYuShchlEh BESEDY
BIBLIOGR: c. 307,
S-- LETOPIS' NO. 31, 1949
I EUKTROENTs EFALOGRAMMAKh I NEKOTORYKh. USLOVIYaghs, M
(PO EKSPERIM. BIOLOGII). T. I. TBILISI, 1949, C. 301-11--
LIVANOV, M.N.;XOJkOLIKOVA, T.A*
-- -WROMI"Pl-,
Effect of inadeqmate stimlation of the skin with inducing current on
blooloatric cutaneous rhythm@ and on conditioned reflex activitys Zhe
vysehei nerv. delat. Favloya 1 n0.3%132-346 Kno-June 1951- (CUL 23.-2)
1. Moscow.
ri~
LITANOT, M.N.;KOROLIZOVA, T.A.;FRIMLI. O.K.
AWMWMOI-W~i
Is
Blectrapb7stological examination of the higher nervous function.
Zh. vysshet nery. doiat. Pavlova 1 no.4:521-538 July-Aux 1951.
(CLKL 23:2)
LITANOT. M.N.; XOROLIKOVA, T.Ae
Bloctropbysiological stu4 on disorders of the hlgbor nervous function
In rabbits. Ir. ls*solus. obah. f Isiol.. no. 1:31-16 195,2. (CLKL 24%1)
1. Daliv*rod 27 September 1950, Mucow.
m n,
KOROLIKOVA, T. A.
KOROLIKOVA, T. A.: "The effect on the cerebral cortex of r;.bbits
of rhythmic irritations of varying frequency". Moscow, 1955.
Inst of Higher Nervous Activity, Acad Sci USSR. (Dissertations
for the Degree of Cahdidate of Biological Science)
SO: Krizbnaja letol2ig', No. 52, 24 December, 1955. Moscow.
KCROLI MDVA. T.A.
-
Iffect of drug-induced sleep on one of the pathological forms of
electrical activity In the cerebrum of rabbits. Trudy Inst.vys.
nerv.delat. Ser.fisiol. 1:308-319 155. (KIRA 9:8)
1. Is laboratorit slaktrofistologit usloynykh reflaksov. saveduyushoMy
K.N.Livanove
(CIBURAL CCRTM) (BLACTROPHYSIOLOGY)
(SL=F-THff4PjwTIC USA)
ICROLIKOVA, T.A.
Study-Ing the physiological mechanisms of the vormation of rhythms
reflecting the respiration rate in the cerebral bioelectrical cur-
rentso Trudy Inst.vys.nory.delat. Ser*fiziol. 2:181-282 '56.
(MLFA 10:1)
lo Iz laboratorit alektrofiziologii uslovnykh relfeksov. 'ifav. -
M.N. ILvanov #
(Y"CTROMSIOLOGY) (HNSPUUTION)
7A,-
KOROLIKOVA, T. A.
Blectrophysiological study of the effect of ionizing radiation on
the functional state-of the cerebral cortex under norml and patho-
logical conditions. Trmd~r Inst.vys. nerv. deiat. Ser. fiziol. 3:
121-135 139. (MM 12:3)
1. Iz laboratorii elektrofiziologii uslovnykh refleksov, sav. -
M.N. Livanov.
(RiLDUTION--PHYSIOWGICAL M7ECT)
(CIRIML CORM )
KOROLIKOVA, T.A.
Investigation of the significance of rhythmic processes in the
cerebral cortex of rabbits following the extinction of conditioned
reflexes. Trudy Inst. vys. nerv. deiat. Ser. fiziol. 5:21-32 060.
(MIRA 13:10)
1. Iz Laboratorii, elektrofiziologii uslovnykh refleksov, (zav. -
M.N. Livanov) instituta vysshey nervnoy dayatellnosti.
(CEREBRAL CORTEX) (CONDITIONED RESPONSE)
GLIVEMOp Ye.V.;,AP~OWKOVA, T-A-j KUZ14ETSOVA, G.D.
Integral picture of the correlative relationahips between
biopotentiale of the rabbit cerebral cortex. Fi2iol. Shur.
48 no.4084-388 Ap 162. (MIRA 15:6)
1. From the Institute of Higher Nervous Aotivity and
Neuropbysiology# U.S.S.R- Academy of Sciences, and the Institute
of Controlling Electronic Yfachines., Mosco'Ve
(CEREBRAL CCRT&X)
(EIaMCENCEPHUOGRAPHY)
-P
KOROLIKOVA, T.A.
Standards of physiotherapeutic service for the urban popula-
tion at the existing level of the general incidence of di-
sease and hospitalization. Zdrav. Roo. Feder. 7 no,10:12-17
0163 (MIRA -16:11)
1. Iz otdela, organizatsii zdravookhraneniya (rukovoditell
doktor med. nauk V.D. Bogatyrev) Moskovskogo nauchno-issle-
dovateltskogo instituta gigiyeny imeni F.F. Erismana (dir.:
A.P.Shitakova).
GLIVENKC,'Ye.V.; KOROLIKOVA T.A.; KUZNETSOVA, G.D.; LUCHKOVA, T.I.;
TRTIBNIK(YVAP
Physiological evaluation of the averaging method for the derivation
of biopotentials. FiZiOl. 2hur. 51 no.8s943-951 Ag 165. (MIRA 180)
1. Institut vysshey Idjol 1411nosti i neyrofiziologii AN SSSR I
Inatitut elektronnykh upravlyayushchikh mashin, Moskva.
R ~716
VASILIKOV, Igor' Afanaslyevich; XQ.~qLIKTLA, T.Ye., red.; GORINIA,
V.A., tekhn. red. -r__
[With a motion-picture camera in the world of insects; scenario]
S kinoapparatom v mire nasekomykh; stsenarii. Moskva, Iskusstvo,
1962. 133 P. (14IRA 15:12)
(Notion pictures in science) '(Insects)
Z
KOROLIKpqk,~A,; KAYUSHEVA, I.V.
Pulseless disease. Klin.-- d. 38 no. 2:141-142 F 1601,
Pw
(Am.taw.-DinnsEs) (MIRA 14:1)
S/271/63/OW/003/021/049
Ao6o/A126
AUTHORS': Keropyan, K.K., Korol'kova, V.A.
TITLE: On a method of electrical simulation of plane movable frames
PERIODICAL; Referativnyy zhurnal, Av-tomatika,.telemekhanika I vychislitellnaya
-eekhnika, no. 3, 1963, 6, abstract 3B32 (Tr. Rostovsk. inzh.~-stroiU
in-ta, 1961, no. 23, 49 - 70)
TM: A new method is proposed for solving problems of electrical simula-
tion of movable frames. The method is based on the application of well-known in
their mechanics approximate methods of analysis for the preliminary determinati(n~
of the displacement of the frame nodes with the subsequent introduation of these
nodes into the electrical simulation circuit in the form of emf imitating the
angles of Intersection of the struts. The proposed methed is Illustrated by ex-
amples of analysis of single-level plane multi-span frames with varied strut at-
tachment; by the simulation of monotonic symmetrical multi-level, multi-span, i
frames bearing a wind load, and-by the simulation of plane movable multi-level
frames. Expressions are cited for estimating the errors in the values of the
Card 1/2
S/271/63/000/003
/021/049
On a method of~ electrical simulation of plane .... Ao6o/A126
moments actinj:, at the ends of the-struts on aooount of errors in the determina-
tion of angles. The experimental results are presented of a verification of the
described method in the analysis of several plane movable frames taking horizon-7
tal loads, using the si mlator MCC -5 (04SS-5). There are figures and 6 ta-
bles.
1. V.
on
[Abstracter s note: Complete translati
Card 2A
A4
11. T
K07tCl I K97A,
1 5
662.5
T.,8i
Elektrobezopasnostt na pronyshlenriylch predpriyatiyakh (~;afetr measures
naustrL, I entarprl Tzd. 2. Voslcva, Clborongitr., 1 5
ait-, olectricit~ in 4
315 p. Illus., dia-rs., tablen.
AB5205r6.
1. K011OLtKOVALk; V.I.
2. US3R (600)
4. Electric "ngineering - Safety Moasures
7. Wimarks to V.I. i(orollkovaials book "Safety riea3ures for electricity in industrial
enterprises.", Eng. M.A. Savin. Prom.energ. 10 no. .4, 19153.
9. Manthl List of Russian Accessions,.Library of Congress,
APRIL
1953, Uncl.
ICOROLIKOVA, V.I.; TIMOVEYEV, T.G., spetaredaktor; VRUMINA., A., re-
SIMKINA, Te., takhnicheiskiy redaktor.
[Practical manual for technical inspectors from trade-union-central
committees] Pcsobie po prakticheskoi rabote tekhnicheakikh inspekto-
rov TsK Profsoiuzov. Vol. 3. [Safety measures in the realm of
electricity] Xektrobezopasnost'. (Moskva) Izd-vo VTsSPS Orofizdat,
1954. 179 P. (MLRA 8:1)
(Electricity, Injuries from) (Electricity---Safety measures)
KOROVIOU,- T-I-
instanstions; instructional
to
EssfetY engineering in 0106t stj * elektroastanovk2kht uchebuys
pisoardal fekhnike besoPIMO '(MIRA 10:9)
GODOMMI1.124-vol 1956. 27 plates
tablitay. N09k" , jon..8afety measures)
(Illectric power distrilb'd
RAKITIII, GA.; VLASOV, A.F.; GLAGOLIVA, T.A., kandidat tekhnichaskikh nauk;
,XWCLIMNA T.I., kandidat tekhnichenkikh nauk; TO.J.;
Irandidat tekhnichask1kh nauk; PROPWOM, A.?.; IRO-
NUCHERIb ; Toys
TSTANOV, LJr., professor; DUNWA, A.B., redaktor: KERWOFA, N.A.,
takhnichaskly radektor.
[Labor rotection] Okhrana truds. lid. 2-os, isr. Moskva lid-vo
VTsSPS KofizdAt, 1956. 278 p. (Km 9:5)
I.Moscow. Mookovskaya vyeshaya shkola profdvithenlya. 2.dhlen-kar-
respondent A"demli weditsinskikh nauk (for Zhotoranov).
(TWWRIAL HYGIM) (INIKWRIAL SAMY)
AMOLIKOVA.-Vera Ivenovna, kandidat takhnicheakikh nauk; PAZHITNOT. D.?.,
lalbener, retsenzent; SAVILOYST. T.M.. in2hener, reteenzeat;
XONSTARTINOV, N.A., redaktor; MUMMA, F.G., isdatellskiy
redaktor; GIADKIKH, N.L. tekhnicheskiy rodaktor
[Safety measures in Industrial enterprises] Blektro-bazopasnost'
as promyshlonnykh predpriiatiiakh. Izd. 3-e, dop. Moskva, Gos.
12d-vo obor. promyshl., 1956. 447 p. (MLRA 9:10)
(Industrial safety)
(Ilectric engineering--Safety measures)
STROKTATNIKOV, I.A.; GRUDINSKIT, P.G.; PWROV. I.I.; KOROLIKOVA, V.I.;
S]IRBINOVSKIT. G.V.; BOLISHAM, Ta.M.; LIVSHITS. D.A.; FAYXRKAN. A.L.
NAYFILD. M.P.; ZHIVOV, M.S.; ONKIN. A.K. (Moskva)
Candidate of engineering L. P. Podollskii. Blektricheetvo no.1:96
ja 158. (MIRA 11:2)
(Podollskii, Lev Petrovich, 1867)
SOV/105-5,r--10-22/25
Korollkova, V.I.t Candidate of Technical Sciences
TITLE; ?~i-~dical-tcchnical Confereywo on Protection From Electricity
P3 1 *1 10 D I C.L L EL~htrichc:3tvo, 1"'71, Nr 10, p 8" ( us S
., J., I
ADS T: A medical-tochnical conference -aill bo Reld this year. It will be
attended by representatives from medicine and technology. The
conference will deal with problems of protection from electricity
and prophylaxis of oleo trotramiatism, and present a scientific
foundation for the standards of protection from electricity. The
study and Generalioation of experience collccted in electro-
therapeutics nay be of special importance. Toots on nionkoys nust
plair the decinive role. Investi,3atioiis of thooe problems aro to be
!:lade a'- the SW-chumslkaya mediko-bioloCicheolk--ya- stantsiya AM-T, SSJS7.~',
- 11 .0
(Sul-diumi ladical-bioloCical Station o-f the JU!S of the USS-11)
to-r,other with the collaborators of the Academy vho are ,-reatly
experienced in tests on moWceys.
Card '1/11
GRIGORYAN, Grigoriy Makarovichp prof., doktor tekhn. YEGOIROV,
Valerian Nilcolayevichp dots.# kand. takhn.nauk;
KAIASIMIKOV, Konstantin Artamonovicb, inzb.-polk.;
LIKOVA. Vera -kand. tekhn. nauk; POLOZKOV)
L I
PRO J=M&
Vladimir Tikhonoviohj, dots.p kand. tekhn. nauk;
SARKISOYANTS, Gayk Arkadlyevichg prof. Prinimal uchaBtiye)
SMMOV, V.M., tuh.-podpolk.; KUSBEIEV., Vladimir Pavlovich,
red.; ROMM, Miron Yakovlevich, red.; YEEMIOVA, T.D.,, ved.
red.; KLLMIENOVA,, K.F,, ved. red.; VOROBIYEVA, L.V., tekbn.red.
(Fundamentals of safet, engineering and fire prevention in the
petroleum and gas industries) Osnovy tekhniki bezopasnosti i
protivopozharnoi tekbniki v neftianoi i gazovoi promyshlen-
nosti- LBy] G.M.Grigorian i dr. Mosk7a, Cos. naucbno-tekhn.
izd-vo neft. i gorno-toplivnoi lit-ry, 1962. 222 p.
(MIRA 15:2)
(Gas industry-Fires and fire prevention)
(Petroleum industry-Fires and fire prevewUm)
Undustrw hygiene)
KOROLIKOVA, Vez4-Ivanovna, kand. tekhn. nauk; KRYAZEVSKIY, B.A.,
-------------- IE-a-xZ tekhns nauk) dots., retsenzent; TUBYANSKAYAS F.G.,
red. izd-va; ORESHKINA, V.I., tekhn. red.
[Safety measures in using electrical equipment in industrW
enterprises] Elektrobezopasnost' na proryshlenrWkh pred-
priiatilakh. 4.., dop. izd. Moskvap Oborongiz, 1962. 527 p.
(KTRA 15:7)
(Electric engineering-S&fety measures)
11 -3
T 2z
IVASHKOVA, V.K., kand.takhn.nauk; Prini-Ii uchastiye: KOROLIKOVA, Ye.A.p
starshiy inzh.; IEBEDEV, VA, laborant;
SWIM., S.M., tekbn.red.
(Using electric models to s-tudy the Thermal propertiR.9 of the
enclosing elements of buildings] Issledovanie teplo Itekhnicbes-
kikh svoistv ograzhdaiushchikh kbnstruktaii zdanii metodom
elektromodelirovaniia. Moskva, Gos.izd-vo lit-ry po stroit.,
arkhit.i stroit. materialam, 1960. 135 p. (Akademiia stroitell-
stva i arkhitektury SSSR. Institut stroitellnoi fiziki i
o,rgrazhdaiushchikh konstruktaii. Nauchnoe soobahchenie, no.1)
(MIRA 15:1)
(Walls-Zlectromechanical alalogies)
L61615-65
-AT5017499
AOCESSION Nit.
2
-28C. Tho.arctic summer har. a smooth temperature variatton which change by
5 S, only
tenths of a degree during.the wtumest indatlis. -In,autunin there is a rapid decrease of air:
temperature from month to month 2i)-25C in tvo 6r Oiree moriths. The entire Arctic
is divided into five -regions-in which the beginning and end of the climatic seasons differs
in time-. Atlantic, Siberian,, Pacific, Capadian-Greenland, and central Arctic bas-I . The
specific character of the climatic sensons for each of these regions is described. The
climatic seasons were defined as-follows- '-Western Atlantic: winter -. mid-November. to
March; spring - April-May; summer _.iune-late August; auturnn - September -mid-Novem-
ber. Westeru.partof Atlantic. December-March: spring -April-
_Y
ernb&: autumn ember.
late May; summer - Jtin.e-mid Sept uAd-September-early Dec
Siberian region: winter - Idue November-March; spring - April-May; summer - Junev
September; autumn - October-late November. Pacific Ocean regiom Nvinter - early De-
cember-March; spring - April-mid-Ifune; summer - mid-June-miet-September; autumu
mid -Sept ember -ea rly December. . Central Arctic, western sector: winter - niid-Novem-'-
ber-111arch; spring - ApiHl-rvlay; summer - June-August; autamn - September-mid-NGvem-1
ber. Central Arctic, eastern seotor: vftter - December-March; spring - April-May:,'
stunmer - June4utplst;_ fluxtumil - Orig, ral., lias~ 6 figurea and
Uible.
SKOTHIEVA, K.K.; KOROLIKOVA. Ye.M., master
Experience In achieving waste reduction. Tekst.prom. 19 no.4:
76-77 Ap, '59. (MIRA 12:6)
1. Smennyry Inshener Soenevsko7 otdelochno7 fabriki Iment Samoylova
(for Skotnikova). Otdal takhnicheekogo kontrolya Soanevskoy otdelochnoy
fabriki Imant Samoylova (for Karallkova).
(Textile fabrics) (Clothing Industry)
SOV/54-5B-3-8/19
AUTHORS: Marinin, V. A., Polyakova, L. V., Korollkova, Z. S.
- ---------------- _~- --- ---
TITLE: Electric Double Refraction of Polystyrene Solutions
(Elektricheskoye dvoynoye lucheprelomleniye rastvorov
polistirola)
PERIODICAL: Veatnik Leningradekogo universiteta. Seriya fiziki i khimii,
1950, Nr 3, pp 73-77 (USSR)
ABSTRACT: In the present paper experimental data on the electric double
refraction in polystyrene solutions are given. The solutions
of 7 polystyrene fractions were investigated. Carbon tetra-
chloride served as rlvent. As the experiments showed the
dependence A = f (E ) remains linear in the domain of the
concentrations used. The Kerr constant was computed for all
measured polystyrene fractions according to the diagram A
versus E2 (Table 1). For reasons of comparison the Kerr
constant of styrene (Table 2) was ascertained too. The Kerr
constant of the solutionj of various polystyrene fractions
(molecular weight 4.0-10 500.106) is,evidently,within
Card 1/3 the errors of observation, of similar magnitude as the Kerr
N
Electric. Double Refraction of Polystyrene Solutions SOV/54-56-3-8/19
constant of styrene. The behavior of the polystyrene solu-
tions in a constant electric field is analogous to their be-
havior in a magnetic field (Refs 2, 3). As a comparison the
molecular Kerr constant of benzene was examined. Measuring
m3ults of this constant in carbon tetrachloride at various
concentrations are given in table 2. The quantities K 2 for
styrene and benzene were determined from the diagram plot-
ting K12 versus C 2* The coefficient of the angular de-
pendence K12 - f (C2) permits to determine the quantity K 2
for infinite dissolution. The computation showed that the
molecular Kerr constant of styrenes is by about two times
higher than that of benzene. It was found that the Kerr
constant of the polystyrene is independent of the molecular
weight. Its sign is positive and in its magnitude it r3-
sembles the Kerr constant of styrene. These facts prove
the conclusions made by the authors (Refs 2, 3, 7). The
authors exprees"their gratitude to V. N. Tsvetkov for his
interest. Ther6 are 2 -4igures, 2 tables, and 7 references,
4 of which are Soviet.
Card 2/3
~V~7
KOROLM317, V. V.
W6Lding tip for welding plastics. Kh1m. I neft. mashinostr.
no.509-40 N 164 (WRA 1822)
-Kf!qj,q_y,_8.A.; KUKOSH, V.I.
Experience in using suturing apparatus in cheat surgery. Trudy
NIIEXRI no.5:19-22 161. (MIRA 15:8)
1. Iz kliniki gospitallnoy khirurugii Gorlkovskogo meditainskogo
instituta im. S.M.Kirova,
(CHEST--SURGERY) (SUTURES)
RL ...
SIM11MI, G. L., DUWIIK, A. G., XMTSIMM, P. V., GRMjIGG, A. B. YOFfZq;, 1. A. _:-
"The High Speed No Dead-TimB Frandng Camera 'A4s-1 -
report prenented at the 6th Intl. Cong. of High-Speed Photography, The Hagm,
1T-22 Sep 162
KOROLOWA, S.
Vitamin i1 as a drug inducing labor and IncreasiM labor pains. Przegl.
lek., Krakow 8 no-7:199-201 1952. (GIKL 23:4)
1 Of the Obstetric-Gynecological Department (Read-Docent M. Seidler,
M: D.) of the Holmital Imienia G. Naratowics. Krakow.
KMOLOkFA, Stafania.
2h9 problem of prolonged prognancy in obstetrics. Gin. polska
28 no.2:189-196 Nar-Apr 1956.
1. V.Oddsialu Ginskologicsno-Poloaniesego Sspitala in. G.Iara-
towicza v Krakovie. Klerownik: prof. dr. N.Seldler. Krakdw.
Kielecka 27.
(PBBMWCY
prolonged (Pol))
KOROLISKAYA, G. A.9 CAND AGR SC,Iq "PECULIARITIES OF THE
PROCESS OF TILLERING AND DEVELOPMENT OF SHOOTS IN WINTER
WHEAT AND WINTER RYEYIN CONNECTION WITH THE FORMATION OF
THE HARVEST." KHARfKOVj 1961. (MIN OF AOR UKSSR. KHARlKOV
ORDER OF LABOR RED BANNER AoR INST IMENI V. V. DOKUCHAYEV)-
(KL-DV9 11-619 225).
-213-
KOROLYFOV, A-M-
Vyazkosty nekotor-jkh metallov 1 splavov v svyazi s ikh
fizicheskimi svoystvamA...
report submitted for the 5th Physical Chemical Conference on
Steel Production.
MOSCOW ~O JUN 109
Korolyu4, A. F. 1111ouroT-sycholon,ical. dist wbanen in into-,:icution In- tetraet'--I !;--ad,
Tnidy KWrb-~shavsk. r,,0,,;. M~A' in-ta, Vol. 1, 101~!~p P. 95-104
SO: U-2"81, Leflo ris Mromalln-71rh Statcy, No. 1, 10,49.
t.w ~n
AUTHORS: Galkinp A. A.,j~ Korol~mk 56--34--4,-49/60
TITLE: The Dispersion of Bound Velocity in Metals in a Magnetic Field
(Dispersiya skorosti zvuka 7 metallakh v magnitnom pole)
PERIODICAL: Zhurnal eksperimontallnoy i teoretichookoy fiziki, 1958,
Vol- 34, Nr 4, PP- 1o25 - 1o26 (USSR)
ABSTRACT: The dispersion of sound velocity in hard metals predicted
by R. A. Alpher and R. I. Rubin (Ref 1) has hitherto not
been observed, apparently because of the smallness of the
effect. The present report describes experiments conneeted
with the discovery of this phenomenon. An apparatus was
developed and built for the investigation of slight varia-
tions of the sound vibrations which, in the case of favorable
condit'ons. takes it possible to measure relative deviations
of about '10- from sound velocity. The principle of the
measurements is based on the comparison and the measuring of
the phase difference of the vibrations passing through the
sample to be investigated. The block scheme of the measuring
apparatus is shown by a diagram. The high frequency voltage
Card 1/3 originating from a generator (stabilized by means of quartz)
56-34-4-49/6o
The Dispersion of Sound Velocity in Metals in a Magnetic Field
ia transferred to the radiating quartz which on one side wao
stuck on to the cylindrical aample, The receiving quartz is
then stuck on to the second front face of the samplev and
the voltage produced by it is then transferred to a phase-
meter. At the same time a voltage is directly transferred
to the phasemeter from the radiating crystal. For the investi-
gation of the ultrasonic vibrations quartz plates (x.--seotion)
of a diameter of lo mm were used. Cylindrical rods of a
length of 2o cm and a thickness of 14 cm served as samples.
A diagram shows the results of these experiments, which were
carried out at room temperature in a field vertical to the
axis of the sample. The experimental points fit well on the
theoretically calculated straight lines. Sound velocity thus
in--,reases proportionally to H in the magnetic field and
the intensity of the effeot corresponds to the predictions
of theory. It is interesting to learn that in bismuth no dis-
persion of the sound velocity was observed at room temperature.
Finallyv the authors thanked Professor A. I. Akhiyezer and
S. V. Peletminakiy2 who had directed their attention to the
discussed phenomenon. There are 2 figures and 2 references,
Card 2/3 1 of which is Soviet.
The Dispersion Of Sound 56,-34--4-49/6o
Velocity in Aletals in a Magnetic Field
ASSOCIATION: Inatitut radiQfiz-Lk! i elektroniki Aka&---emii nauk Ukrainakcy
SSR
SU]3,'AITTL?D (Institute of RadiOPhYsics and Electro.ic. AS Ukrainian SsR)
JanuarY 14, 1958
Sound--Pefraction
2. Mata*1s__.Ac'ou3tic properties
Card 3/3
240), 240)
AUTHORS: Galking A. A., 1rorolyuk, A. P, SOV/56-36-4-52/70
TITLE: Anisotropy of the Absorption of Ultrauonics in Metals in the
Magnetic Pield (Anizotropiya po.-loshcheniya ulltrazvuka v
metallakh v magnitnom pole )
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, TTr 49 PP 1307-1309 (USSR)
ABSTRACT: It has already been shown that for longitudinal sound the
absorption coefficient in tin depends on the ma~,-netic field
in ouch a manner, that if the latter is vertical to the wave
vector, a weakly marked maximum of absorption occurs in
certain fields; a similar phenomenon is observed in poly-
crystalline copper and in indium. In the present "Letter to
the Editor" experiments are discussed in which the influence
exercised by the magnetic f5eld on the absorption of ultrasonics
at low temperatures in polycrystalline samples of very pure
metals was investigated. Tin with a rosidual resistance
1 1.6.10-5 and zinc with R 4.2/R300 ~ 2.10-4 was investigated.
The samples had a diameter of 12 and a length of 12 and 15 mm
Card 1/3 respectively. The absorption coefficients were determined by
Anisotropy of the Absorption of Ultrasonics in sov/r-6-36--4-52/70
Metals in the Magnetic Field
means of the well-known pulse method at frequencies of 17.,'A,.
23-3~ 51, and 70 megacycles, Figure 1 shows the results
obtained by measurements r;arried out at 4.20 K with a magnetic
field that was vertical to the wave vector. The curves plotted
at higher frequencies show already two maxima, Thusj zinc at
70 megacycles showed a minimum at about 500 Oe, the first
maximum at about 800, and a second flat maximum at about
2,000 Oe. If the magnetic field rotates in a plane that is
vertical to the SaMDle axis, the curves are found to va-ry
essentially-, The absorption of the maxima and their amount
varies~ in the case of certain directions these maxima vanish~
and in certain cases the maxima exist only within range of the
angles of 15-200. Figures 2 and 3 show such diat;rams at
70 megacycles. Here the absorption coefficient for ultra-
sonics shows a tendency of assuming a saturation value at
5,ooo-6,ooo Oe. This limiting value depends on the orienta-
tion of the sample in the field. The diagrams for the limiting
value in the case of stron.-, fields describe the anisotropy
of electric conductivity in the magnetic field, There arc 3
Card 2/3 figures and 6 reforoncon, I of which is Soviot.
Anisotropy of the Absorption of Ultrasonics in SOV/56-36-3-52/70
Metals in the Magnetic Field
ASSOICIATION: Institut radiofiziki i clektroniki Akademii nauk Ukrainskoy
SSR (Institute for Radiophysics and Electronics of the Academy
of Sciencesi 19krainskaya SSR)~ Piziko-tekhnicheskiy institut
Akademii nauk Ukrainskoy SSR (Physico-technical Institute of
the Academy of Sciences, Ukrainskaya SSR)
SUBMITTED: December 12, 1958
Card 3/3
24 (1)
AUTHORS: Bezuglyy, P.-A., Galkin, A. A. BOV/56-36-6-61/66
Korolyuk, 1. P.
TITLE: The Anisotropy of the Absorption Coefficients of Ultrasonics
in Superconductors (Anizotropiya koeffitmiyentov pogloshohoniya
ulltrazvuka v averkhprovodnikakh)
PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fiziki, 1959
Vol 36, Nr 6, PP 1951 - 1952 (USSR)
ABSTRACT: By the investigation of the absorption of ultrasonics in super-
conductors it in possible to determine the size of the energy
alit at T a 0 an well an the dependence of the alit width (Ed
on temperature. The experiments carried out in this connection
are in agreement with theory. By means of experiments also the
influence exercised by the isotope composition and the homo-
geneous lattice deformation,upon T k and on the width of the
alit was investigated. It may be imagined that lattice aniso-
tropy leads to more visible results than isotopic composition.
In the present "Letter to the Editor" experimental results con-
cerning the absorption of ultrasonics (frequency 70 kilocycles)
Card 1/2 in superconductive and normal media are published. (Determine-
K,
The Anisotropy of the Absorption Coefficients of SOV156-36-6-61166
Ultrasonics in Superconductors
tion of the absorption coefficient in the C2- and C4-ax's of
a spherical tin sample). The results, which were dealt with b
the method developed by Bardeen, Cooper and Schrieffer (Ref Z
are shown in a table. It was found that the temperature de-
pendence of the ratio of the absorption coefficient a $/an is
different in the two directions. The case of sound propagation
along the C -axis agrees better with the isotropic theory of
4
superconductivity. There are I table and 4 references, I of
which is Soviet.
A330CIATION: Fiziko-tekhnicheskiy institut Akademii nauk Ukrainskoy SSR
(Physico-technical Institute of the Academy of Sciences,
Ukrainskaya SSR)
SUBMITTED:
Card 2,2
April 7, 1959
24 (1)
AUTHORS: Galkin, A. A., Xqr,.~k ~A-~ BOV/56-37-1-53/64
TITLE: Oscillation of the Sound Absorption Coefficient in Lead at Low
Temperatures (Ostoillyatsii koeffitsiyenta pogloshcheniya zvuka
v clove pri nizkikh temperaturakh)
PERIODICAL: Zhurnal eksperimental 'no i teoreticheakoy fiziki, 1959, Vol 37,
Nr 1, PP 310 - 312 (USSR~
ABSTRACT: It has already been shown (Refs 1-3) that the absorption coef-
ficient of ultrasonics in metal does not change monotonely with
the m W etic field, but that it has a special anisotropy. The
authors of the present "Letter to the Editor" investigate the
latter at an ultrasonic frequency of 70 megacycles and give a
report on the results obtained. Investigations were carried out
in a spherical monocrystalline lead sample Of 15 mm diameter.
Planes were out off from the sphere, to which the ultrasonic
sources were applied. The perpendicular lines of theme planes
were parallel to the axon of 2. and 4- order. Absorption was in-
vestigated for longitudinal sound, the wave vector k of which
was parallel to the axis of 2. or 4. order. The sample was ro-
Card 1/3 tated in the magnetic field-1, with the-z_7ector remaining per-
5
Oscillation of the Bound Absorption Coefficient in SOV/56-37-1-53/64
Lead at Low Temperatures
pendicular to -9. Figure I shows the course of th amplitude in
dependence on the field strength (45 - 1000 Oe) :t T w 4.2'0K,
for sound propagation along the axis of second order; i was
parallel to the axis of 4. order. The curve has a manifold of
marked maxima and minima (of V. Gurevich, Ref 4)- Prom the os-
cillation periods the magnitude of the limiting momentum of the
electron was estimated at P - 5-10-20 9.em/sec. Figure 2 shows
the dependence of the projection of the limiting momentum of
the electrons on to the plane (001) as a function of the angle
between the axes of 2. and 4. order$ developed according to os-
cillation periods. Figure 3 shows several results of measure-
ments of the absorption coefficient in dependence on the mag-
netic field voltage and the angle of rotation f in the (001)-
plane. Figure 4 shows the angular dependence of the absorption
coefficient at H - 7.103 Oa and with rotation of the field in
the (001)-plane. The investigation of sound absorption in a
Itl V'shows that the curve a(H) has singular points. Ac-
field H
Card 2/3 cording to the theory by V. Gur3vich, the magnetic field in
Oscillation of the Sound Absorption Coefficient in SOV/56-37-1-53/64
Lead at Low Temperatures
these points satisfies the condition Hi - oonst/n, where n is
an integer number. There are 4 figures and 4 references, 2 of
which are Soviet.
ASSOCIATION: Institut radiofiziki i elektroniki kkademii nauk Ukrainskoy SSR
(Institute of Radiophysics and Electronics of the Academy of
Sciences, Ukrainskaya SSR)
SUBMITTED: March 25, 1959
Card 3/3
86749
S/l2o/6o/ooo/oo6/025/045
9041/9521
AUTIORS: A.A. and.- roly". A.P.-
TITLgt InstrAmeat...for .3t4dying. Ultrasonic Absorption by
Metals at Low Temperatures
.PZRIODICALt Pr:Lbor-y-i-.tokhnika-eksporimenta,-.1.960, No.6, PP-99-103
TZXTa 'The greatest Interest lies in the &Wsprption by magnetic
materials under conditions where the mean free path of a conduction
electron is significantly greater than the wavelength of the sound
in the material', while the Larmor radius of the jolectron is
comoarable with the latter. The absorption coefficient varies
periodically with magnetic field strength and the period is a
measure of the electron impulse at the Feral. surface. The present
article describes a method of recording automatically the propagated
signal strength as a function of magnetic field in a series of
monocrystals. Fig.1 shows the block diagram of the experimental
arrangement. A pulse generator .260 (261) drives simultaneously a
modulator and a delay circuit. The modulator switches a high-
frequency generator connected by coaxial cable to the transmitting
crystal a. The crystal can be watched to the generator by varying
Card 1/4
86749
sA2o/6o/ooo/oo6/025/045
zo4l/9521
Instrument for Studyi=&_UUxaso"c~, Ab4wrptlow -by Metals at Low
.Temperatures
the cable length. The' receiving c'fkfiital b in similarly joined to
the receiver whose output is gated in the pulse selector drive by
another generator 261 from the delay circuit. The selector output
is peak detected, the selection of the appropriate pulse being made
by varying the delay. The detected output goes to a recorder )r1n -og
UPP-09) which is a two-dimensional self-balancing potentiometer
plotter. The field strength in measured by a'germanium Hall-effect
pick-off. Fig.2 to the circuit of the modulator and high-frequency
generator. The latter oscillates between 50'and 250 Mc/s. The
receiver is in two parts. The high-frequency part in an ordinary
television receiver front--end working over the bands 50-100 and
160-230 Mc/s. Other frequencies are covered by heterodyning. The
intermediate frequency amplifier circuit in in Fig.4. The crtre
frequency in 32 Mc/s, the bandwidth 3 Mc/s, amplification 10
sensitivity between 5 and 10 microvolts. Fig.4 in the delay
circuit providing delays between 0 and 250 microseca. Fig-5 is
the pulse-selecting gate. Fig.6 is a cross-section through the
Card 2/4
86749
S/l2o/6o/ooo/oo6/O25/O45
E041/E521
Instrument...for.Studying.Ultrasonic.Absorption..by Metals at Low
Temperatures..
crystal. Fig,'7 shows how the sample is mounted. The sample may be
rotated in the field. The magnet current is controlled from 0 to
8 amperes by the circuit of Fig.8. Fig.9 is an example of. a record
taken on a monocrystal of tin. The 'Bound frequency was 220 Mc/s,
parallel to the (101) axis. !The H-vector lay in a perpendicular
.plane and made an angle of-about 360.to the (100) axis. The two
.curves each took 3-4 minutes in recording. Manual methods would
have taken 15-20'times as long. The overall error in measuring
either coordinate---does-.not. -exceed a -few. percent. There are
9.figures and.8-r..eferences:.4 Soviet and 4-non-Soviet.
ASSOCIATION: Inatitut radiofiziki J. elektroniki AN UkrSSR
(Institute of Radiophyiics and Electronics, AS, UkrSSR)
'SUBMITTED: October 13, 1959
:Card 3/4
850575
d'84,00 (32,01, /Ofy/ 2#0o)
VA00
S/05 60/038/006/017/049/XX
B006YB070
AUTHORS: Galkin, A., A,, Korolyuk, A. P,
- 4~~
TITLE: Absorption of Ultras~cnics ~in ~Inc' ~ Low Temperatures
PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fiziki,
1960, Vol. 38, No. 6, pp. 1688 -- 1694
TEXT: The oscillation of the ultrasonic absorption coefficient a
with a change in the magnetic field has been studied several times in
the past; the theory of this effect is due to V.. L. Gurevich. Also
two of the earlier papers of the present authors (Refs. 1, 2) were
concerned with problems of the same nature. Now, the behavior of a
in a strong magnetic field is studied for the case when 1)X) r
mean free path of the electrons; r-cp/eH is the Larmor radius;
ultrasonic wavelength). The behavior of a Is essentially related
to the asymptotic behavior of the electrical conductivity tensor,
A theoretical study of this was made by Gurevich and E, A, Kaner
(Refs. 9, 8) who showed that data on the topology of the Fermi surface
Card 1/5
856 7 5
Absorption of Ultrasonics in Zinc S/056/60/038/006/017/049/XX
at Low Temperatures B006/BO70
can be obtained by studying the anisotropy of a in a magnetic field,
The experiments described here were carried out on single crystals of
zinc by the method of Obreimov-Shubnikov. The metal was 99.9996% pure,
and had a resistivity ratio R 4,.2/R 300~ 2,10-4., The techniques of
preparing the specimens, of producing the ultrasonic waves (60, '00;
180, and 220 Me/sec), and of the measurement are described in the
introduction, The periods of oscillation of a were measured for different
orientations of-A which could be rotated in a plane perpendicular tot
Fig. 1 shows one of these oscillation curves at 220 Mc/sec.. Fig., 2
shows the number of oscillations as a function of 1/H for different
directions ofO in the (10fO) plane, In Fig, 3, a, b, and c show the
angular dependence of the extreme direters of the Fermi surface
(perpen-dicular to -A) on rotation of and the planes (1120), (0001)i
and (10fO), respectively. Fig, 4 shows the de endence of the difference
of a-values with and without a field (7000 M on the direction of
It, a: k 11 F~0011 ; b: k 11 [10 ~0] ; c: k 11111 ~0] . T= 4, 20K; 60 Mc/s ec,
According to the theory'(Ref'. 6), a change'in the diameter of the
electron orbit in relation to ~k corresponds to each oscillation of a
Card 2/5
Absorption of Ultrasonics in Zinc
at Low Temperatures
65675
S/056/60/038/006/017/049/XX
B006/BO70
in the magnetic field.. The relation 1--r-N(n+~) holds for the mean free
path of electrons in a weak field., Another possibility of determining
1 is to measure the component of the electron momentum perpendicular
to I and ft (P,.), and the minimum field in which oscillations appear
(PL/r max- eH min /c),, The following path lengths were determined by
these methods:
direction Path length [mm] Temperature
according to the according to FOKJ
number of oscillations pi
~00011 0.5 o.6 1-65
ri 0 i0l 0,22 0.2 4~2
[11 ng 0,,27 0.24 1,65
Thus, the electron path length alsr shows anisotropy, The results
are discussed in the conclusion. The values obtained for the extreme
diameters of the Fermi surface show that the law of dispersion of
Card 3/5
-n'
M
85675
Absorption of Ultrasonics in Zinc
at Low Temperatures
S/05 60/038/006/017/049/XX
B006YB070
electron energy deviates largely from the quadratic form It- is con-
cluded from the anisotropy of a in a strong field that the Fermi
surface of zinc is an open surface of the sixth order in the direction
of the symmetry axis. E, A. Kaner and M. I.' Kaganov are thanked for
discussions,and V.. I, Bogatov for supplying l1quid helium., There are
4 figures, I table, and 11 references: 7 Soviet 3 US. and I British
ASSOCIATION: Institut radiofiziki i elektroniki Akademii nauk
Ukrainskoy SSR
(Institute of Radiophysics and Electronics of the
Academy of Sciences Ukrainskaya SSR)
SUBMITTED
January 10, !960
Card 4/5
82594
'1) 9 00 S/056/60/039/01/01/029
".5-4 0 0 B006/BO7O
AUTHORS: Bezuglyy, P. A., Galkin, A. A., Korolyuk, A. P.
TITLE: Investigation of the Anisotropy of the Energy Gap in
superconducting Tin
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 39, No. 1 (7), pp. 7-12
TEXT: The authors investigated the temperature dependence of the
ultrasonic absorption coefficient in different directions of single
crystals of superconducting tin. They describe the methods of investi-
gation and present the results. The method of energy gap investigation
is based on the determination of the difference between the curves
ces/,xn - f(T) when the ultrasonics is propagated along a binary (C2) and
a tetragonal crystal axis. From this difference the anisotropy of the
energy gap may be determined. aL. and oen are the electronic ultrasonic
absorption coefficients in the superconducting and the normal state
respectively. They are related to the width 2 6 0 of the energy gap by
Card 1/4
82594
Investigation of the Anisotropy of the Energy S/05 60/039/01/01/029
Gap in Superconducting Tin B006YB070
the relation ae Van =2/(e Eo/kT + 1). To investigate the influence of the
lattice anisotropy on the energy spectrum of electrons in a semiconduc-
tor, the temperature dependence and absorption coefficients of longi-
tudinal supersonics was investigated by means of an apparatus described
here in detail. Fig. I shows a block diagram of the measuring device.
The generator works at 70 Me/see, the quartz emitter receiv9s
2500-3000 pulses per second for a duration of (1 1-1-5)-10- sec. A small
sphere of single crystals of tin was used as a sample. It had a diameter
of 13-15 mm, and on it, cut surfaces of 5-6 mm diameter perpendicular
to the crystallographic axes were produced by electrocorrosion. Onto
these surfaces quartz emitters and receivers were cemented in vacuum
and on them small plates of brass of 5-6 mm diameter and a thickness of
0.2-0.3 mm. For very pure crystals of tin the condition that the mean
free path of the electrons be large in comparison to the ultrasonic
wavelength was very well fulfilled at helium temperature. The temperature
dependence of ultrasonic absorption coefficients was measured simultane-
ously in two different directions at temperatures down to 10K. Fig. 2
shows the Dewar for helium in which the measurements were carried out.
VY
Card 2/4
82594
Investigation of the Anisotropy of the Energy S/056/60/039/01/01/029
Gap in Superconducting Tin B006/BO70
The temperature of the sample was determined from the saturation vapor
pressure of helium. The results are shown in diagrams. Fig. 3 shows
lxs/c~n between 10 and 40K taken along two mutually perpendicular C2 axes.
The measured values (full and empty circles) all lie on one line which
shows that the physical properties are the same in the two directions.
Fig. 4 shows the same for C. and C 4 axes. Here the anisotropy of the
energy gap is clearly seen. ieasurements made on two samples gave uniform
results. For the absolute value of the electronic part of the ultrasonic
absorption coefficients in the normal state in the neighborhood of T.9
the following results are obtainedt(Xn - (47.6 + 0.2) decibel/cm -(C.),
and c(n - (21-4 1 0.2) decibel/am -(C 4)- Fig- 5 shows log(ce./M.) - f (Tc/T)
From the slope of the straight line portion of the curve, the energy gap
width at absolute zero may be determined to be (3-5 � 0.2)kT a for the
C2-axis and (3.1 + 0.1) kT. for the C 4-axis. Besides the anisotropy in
the temperature dependence of the absorption coefficients, an anisotropy
Card 3/4
82594
Investigation of the Anisotropy of the Energy S/05 60/039/01/01/029
Gap in Superconducting Tin B006YB070
of the transition temperat-are To is also established. For the C2-axia TC
lies about 0-0040K higher than for the C -axis. The authors thank
A. I. Berdovski and E. I. Ponomarenko fir cooperation in the measurements
and V. L. Karpachevskiy and B. 1. Aleksandrov for help in the preparation
of the sample. There are 5 figures and 13 references: 5 Soviet,
6 American, I British, and I Dutch.
ASSOCIATIONi Fiziko-tekhnicheskiy institut Akademii nauk Ukrainskoy SSR
(P!Msicotechnical Institute of the Academy of Sciences of
the UkrainB-kava SSR)
SUBMITTED: January 12, 1960
Card 4/4
88423
S/056/60/039/006/007/063
,Z4-.7700 Boo6/BO56
AUTHORS: Galkin, A. A., Kaner, E. A., Korolyuk, A. P.
TITLE: Investigation of Ultrasonic Absorption by Metals in a
Magnetic Field
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheakoy fiziki, 1960,
Vol. 39, No. 6(12), pp. 1517-1528
TEXT: The characteristics of ultrasonic absorption in metals at low tem-
peratures under conditions at which the mean free path 1 of the electrons
is very large with respect to the acoustic wavelength I have already re-
peatedly been investigated both theoretically and experimentally, above
all the periodic change in the ultrasonic absorption coefficient a as a furio.
tion of H-1. The first theoretical calculations are by Fermi and V. L.
Gurevich. In the present Daper, the theoretical and experimental results
are given, and compared for tin and indium. First, the magnetoacoustic
resonance and the oscillation of a arf investigated for a strong magnetic
field, as well as the conditions wave vector) and Xtt,2nr tl.
Card 1/3
Wt "l 0-.
88423
Investigation of Ultrasonic Absorption by S/056/60/039/006/007/063
Metals in a Magnetic Field B006/BO56
For tin- and indium crystals typical oscillation diagrams are shown and
,liscussed. Two different types of oscillations are said to occur in tin:
Anharmonic resonance oscillations and sinusoidal oscillations. Those of
the first kind are ascribed to the existence of an open Fermi surface;
the period of the open surface, calculated on the basis of oscillation
periods, is in agreement with crystallographic data. A study was made of
the anisotropy of ultrasonic absorption in a strong magnetic field and
when the condition r