SCIENTIFIC ABSTRACT KIKOIN, I.K. - KIKTENKO, V.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000722520009-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 14, 2000
• Sequence Number: 9
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

87400
S102 60/135/006/01~/o37
/003) B01 9YB056
AUTHORS: Kikoi Academictan, and Lazarev, S. D.
TITLE: The Isotropic and AnIsotropic Components of the Even
Photomagnetic Effect
PERIODICAL: Doklady Akademii nauk SSSR. 1960. Vol. 135~ No, 6.
pp- 1371 - 1373
TEXT: When light is perpendicularly incident. upor. a seml,~cnduetor
lr~cated in a magneti',~ fieldi an electric field is known to be formed. In
the oase of the even photomagnetic effect, the emf is usiially measured
In parallel with the direction of the magnetic field (contrary to the odd
effect, the sigr of the emf does not change in the case of the photomag-
netic effect when the direction of the magnetic field is revers'E-d). it
has been found already Parlier that the even phctomagnetic effect In
single crystals of Ge is anisotropic. The formula
E - L e ri H + L H,n H -i L n H 2 (2) was suggested for a phen:,meno-
I 'kl k 1 2 k k 3 1 i
logical desoription of th- photomaCnetic emf. Here, L1, L V and L3 C1 11 t~
Card 1/3

87400
The is)tropi-, and Anisotropic Components of the 81020 60/135/006/015/037
Even Photomagnetic Effect B019i/BO56
,,orotants chararterizing the somiaonductorl eAl in all llntisynlwet~-Ical
tensor; A are the components of the internal surface normal of the
sem-'conductor; and Hi~ Hk' and H, are the components of the magnetic
f.-.ald. The last term in (2) des,~ribes the aniaotropy of the phetrimag-
r,etAc effect, indicating that the even photomagnetic effect may be ob-
served not only in the direction of the magnetic field, but in any direc-
tion, especially perpendicularly tc the magnetic field; this is the ~,.ase
even if 0 - V2, where 0 is the angle between the surtace normal and *.h.,-.
magnetic field. The au"bors verified these reaults of the phencmenolo-
gical theory, using a .isk-shaped single crystal of Ge out out perpen-
dic.ularly to the (11:3 axis. From the results obtained the auth-irs co-n-
clude that formula (2) may be used, no~ only for weak, but alsl- for
stxong magnetic fields; however, the rioefficients.L1 and L2 must be con-
si.dered to depend -.,n the magnetic field, It further turned cut that ths
isotropic and anisotropic components of the photomagnetio -.mf depend cn
the magnetic field, and may have different signs. The authcra thank
Card ?13

KIKOIN, I.K.; LAZAREV, S.D.
---
Anisotropy of the odd photomagnetic effect. Zhur.eksp.i teor.fiz.
41 no.4:1332-1333 0 161. (MIRA 14:10)
(Photomagnetic effect)
.xv.17-

26722
S/056/61/041/005/037/038
'21 B109/BIO2
, ~' 9- 4o 0
AUTHORS: Kikoin, I. K., Nikolayev, I. N.
TITLE: The photomagnetic effect in a p-n junction
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 419
no- 501). 1961, 1692-1694
TEXT: Studies of the photomaguetic effect in semiconductors suggested a
photomagnetic effect in the blocking layer between semiconductor and metal
contact when the contacts are illuminated. In order to elucidate this,
the following experiment has been made: A piece of n-type germanium
(10 by 4 by 4 mm) had a diffusional p-n junction(due to diffusion of
indium) on the one front face (4 by 4), and an ohmic contact (tin) on the
other. The photomagnetio e.m.f. was measured between these contacts. while
the sample was illuminated and exposed to a magnetic field. This e.m.f.
consists of the voltage along the homogeneous part of the sample and of
the potential difference at the p-n junction. These two portione can be
distinguished because the voltage along the homogeneous part depends on
the area of the illuminated surface, which, e.g., may more or less be
Card 1/3

AUTHORS:
TITLE:
PERIODICAL:
S/056 62/043/006/063/o67
B141 B102
Gridin, V. A., Kikoin, I. K.
The nonstationary photomagnetic effect in germanium single
crystals
Zhurnal eksperimentalinoy i teoreticheskoy fiziki,,v. 43,
no. 6(12), 1962, 2315-2317
TEXT: The time sequence of the photomagnetic effect for pulsating
illumination was investigated and the emf was measured as usual.
Specimens of single crystal-n- and p-type germanium in the shape of disks
(30 mm diameter) were placed in a field of up -to 30 koe, and light pulses
were produced by a Kerr cell; the pulse length could be varied between
5 and 2000 Itsec. The maximum light flux passing through the Kerr cell was
about 1017 quanta/see. The depth of modulation of the visible particle of
. Q -'
light was 81j. The emf of the photomagnetic effect to be muasured was
recorded simultaneously with the voltage pulse on the Kerr cell by an
OK-17M(OK-17M)synchronized double-beam oscilloscope. The oscillograph
Card 1/2

S/056/62/043/006/063/067
The nonstationary photomagnatic... B141/B102
curves show the dependence of the uneven emf on the time at an illumination
pulse of 1 msec. If "he ill,umination is switched off at the moment when
the emf passes throuEh a maximum, it drops to zero without change of sign.
The type of illumination also f:overns the shape of the curve. It is shown
that the dependence of the photomagnetic effe6t on time depends strongly
on the surface recombination rate, which can be explained by the fact that
the emf is proportional to the difference in concentration of the minority
carriers on the illuminated and nonilluminated part of the sample surface,
whilst inversely proportional to the conductivity. The change in sign of
the emf on samples having identical surfaces when the illumination is
switched off is caused by the dependence of the surface recombination rate
on the intensity of.illumination. There are 2 figures.
SUBMITTED: September 29, 1962
Card 2/2

-KIKOIN, Isaak-Konstantinovich; KIKOIN, Abram Konstantinovich;
MARGULIS, U.Ya., red.; AKMLIROD, I.Sh., tekhn. red.
[Molecular physics) Molekuliarnaia fizika. Moskva,
Fizmatgiz, 1963. 500 P. (MIRA 17:2)

KIKOIN, 1. K.
Igor' Vasillevich Kurchatov. Atom energ. no.1:5-9 Ja 163.
~MIRA 16:1)
(Kurohatov, Igor' Viasillevich, 1902-)
4w

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4- of, trii "no :to" -dauteron.plasna
-TITLE
Us i un
ti
SOURCE:~-~I:.Zb.: ekspei.---c"tiore fiziki' V -45, no 3t*,1963 428'-43
-do
TOPIC VACS ute-ro.a. oma-ldeiisi 'toroidal dio'charge chamber~,,oj,,.
'Asmal',deusity, p asms.
Plasma p1
_:V2
Mea a
BSTRACTA 'A: method' of a dauter,on, plasma, by' idea
f f 3 des'cribed
:a beaw :.6 plasma i
o
Th thod is based:.ow.rocovding eioadar~_partlcles.ies',~ltiu
a me
4''
re ti n D(tOn)Hi~p'cAu$cd b :,the;.collision of accelerated
from ac. 0 .: ~y
-thi *1 The energy
r .~p asma por.
t,LtLum,lono with ticles. 6f the inject d
tritons was appro*Lmatdly~"160~Ktiv,'and~the energy of the neutro
and alpha:particles produced' 14 and 3.5 M Ievo respectively. The-
A;ard

167,9
~~_i
OWNRi AP3
nV -a*- t c r a a: We
estlgal~-ifig~devllca vat o iidaV`dLs'hi'9e.1ch mber,ln.
The rincipal"di*meter;of the' t~ioll
p
i was -.750 mm #~ the. inner, Alame,ter'-olf ._th4,:..dis charge chamber, aboutt I I
-210. mm the intensit If:'ih magnet C:. 200-w-700 oas~ andi~ 6'~'
field
0 7 q a': 11 . . . .! ;. I-
maximum,discharge-eurve "Wo -kamp. The discharge timc. in
er was'
the chamb -approximstily'!~600 Post the pulse duration of,1he
&6u approiffmate 17'."I'doo use c :A
rce, V nd-the time delay between
the start ~of the disc ArItk'Am-th ch
h, amber and the start of,th"
e epu
of the source current'' 1~41000 - usec. Measurements were carried
out with the- discharge,icha-mAer',filled vith deuteriu and,as
m ai col
.-Iasma,density over the whole
trol, with hydrogen a.- ~he:;,aver.sge_p,
m
7 path of a ltritium'beam jvas:~~-,deter inedo.. Although,the plasma de6i!"
s~ greater af ter'dischirgei~`thi, -increase cannot. be. regarded as! a
result of iplasma.comp ~ssion arely a a result :of the liberati
r
0. a 'dis'
f 03 fvom~ the chamberiv llt~,dltrr ng, ch.4rge, Orig art. has.
F 8 figures.;
C
ASSOCIATION
'63 -AC 9;- 0806t63' ENCLs 00.
SUBN=ED: 07 Mar
SUB -C
SOVs-1 002
ODSt PH 10 (YTHER.- 000 i
Car4,2/2

KOZYREV, Yu.P.
Fffect of a magnetic field on recombination radiation from
Ge and its quenching by infrared light. Zhur. ekBp i teor.
fiz. 45 no.5:1393-1395 N 163. iMIRA 17:1)

ACCESSION NRt AT4025309
0/0000/63/000/000/0193/0198
AVTHORSs Moin, 1. K-j C;okbbercjt B* Hot Nalltnevs Ve V*1 Otrosh-.
ebenko, 0. A. I Knyatyatovo A. 0.
TITLEs Probing a deuterium plasma with a tritium been
SOVRCE: Diagnostika plazmy* (Plasma diagnostics)l ob. statey.
Moscow, Gosatomizdat, 1963, 193-198
TOPIC TAGS: deuterium, tritium, plasma density, plasma ele*ctromag-
netic property, neutron yield, discbarge plasma
ABSTRACT: The method is based on the registration of the number of
reactions between the incident tritium nuclei and the deuterium
nuclei of the plasma, making it possible-to investigate the varia-
tion'of the deuterium density independently of the degros of ioniza-
tion of the plasma and of the impurity contents. The investigation
was made in the "Igla" toroidal chamber.(Iarge diameter 750 mm,

ACCESSION NR: AT4025309
small diameter 200 mm, maximum capacitor bank energy 35 kJ, maximum
discharge current 100 M). 7be ion current and the position of the
beam were monitored with thermocouples distributed over the channel.
The tritium beam source is described elsewhere (1. 1. Afanas'yev et
al. "Atomnaya energiya* v.' 13, No. 8, 135* 1962). The. investigation
of the neutron yield from the ion collector located on the inside of
the cUscharge chamber has made it possible to draw certain conclusiono
concerning the absorption of the working gas (deuterium) by the walls
of the discharge chamber. However, in the case of high-frequency
ionization of t-be gas (preliminary ionization) the walls are c4able
of absorbing a very large amount of gas. Investigations of the vari-
ation of the deuterium plasma density during the discharge time show
that the plasma density increases by several times during the dis-
charge, as a reault of interaction between the plasma and the walls..
When deuterium in used in the discharge chamber, the yield of neu-
trons decroaies immediately after the discharge, ared with the
yield in the ibsence of dischargeo Jn the case of hydrogen# the op-
Cwd 2/3

ACCESSION KRt AT4025309
posite takes place. a control experinent has shwwn that the increase
-AeA the netutron yield is not due to a dLmplaa-ment of the ion beam
during the dLechargee 0rLq* art. hant.4 figuran.
ASSOCIATIM None
GUBMITTEM 190ct63 DATE ACQt 16Apr64 ENCLt 00
SUB CODES ME 'NR REP BOVs 002 OTHERs. 000

ACCESSION NR: AP4012524 S/0056/64/046/001/0067/0070
AUTHORS: Kikoin, I. K.; Igosheva, T. N.
TITLE: Hall coefficient and electrical resistance of ferromagnets
SOURCE: Zhurnal eksper. i teoret. fiz., v. 46, no. 1, 1964, 67-70
,TOPIC TAGS: f4rromagnet, Hall co"effici6nt, electrical resistance,
magnetic component of resistance, ferromagnetic Hall coefficient,
odd galvanomagnetic effect, even-galvanomagnetic effect, Curie point,~
magnetoresistance, Hall effect
2
ABSTRACT: Since the formula R = Ap which Karplus and Luttinger
F
(Phys. Rev. v. 95, 1154, 1954) proposed for the connection between
the ferromagnetic Hall coefficient and the electric resistance p of
a substance was never confirmed experimentally, the authors show
that it is physically more justified to relate R. with the "magnetic"
Card 1/,8;1-

ACCESSION NR: 'AP4012524
Part PM of -the resistance, broug.qt about by spontaneous magnetiza-
tion, and show by analysis of the experimental data that the formula
R - R a where R is the'value of R at 01K, holds true for
F FO Pm'-. FO F
temperatures both above and below the Curie point (with possible ex-
ception of very low temperatures). The variation of the reiistance
of several alloys in a magnetic field (in the paramagnetic region) i
is also shown to be proportional to the magnetic resistance.. It is
therefore concluded that the magnetic resistance p is the quantity
M
with which both the odd and even,valvanomagnetic effects should be
compared. Orig. art. has: 3 figures and 7 formulas.
ASSOCIATION: None
SUBMITTED: lOJul63
-DATi ACQ: 26Feb64 ENCL: 01
SUB CODE: PH NO REF SOV:. 003 OTHER: 006
Card 2/~:~-

KAROL', 1. L. : S. G.; KIKOIN I. K
. - - - -?- -- --
"Use of isotopes for quant !tat ive invest igat ion of' atwssj-,~ Lre "
report submitted f'or 3rd Intl Conf, Peaceful Uses of Atomic E,-ier;,,,.- Geneva,
31 Sep 04.

ACCESSMA NR: AP4037618 S/0056/64/046/005/1923/1925
AMOR:_ Kikoin, I. K.; 1goshava, T. N.
TITLM Mametic variation of the rcsistance of fcrTQmagnets
SOURCE: Zh. eksper. i teor, fiz., vo 46, no. 5, 1964, 1923-1925
TOPIC TAGS: ferrcmagnetj ferranapet resistance, fctyowgnetic Hall coefficient,
anomalou:3 Hall coefficient, spontaneous magnatizatiai, galvanomagnetic effect,
resistance in maMetic field, para process, Curie point
A15STRACT: In analogy with the simple connection they previousi.y obtained (Z"ETF
v. 46, 67, 1964) betwedn the ferTarvipletic Hall effect and the ma-pictic, resis-
tance, the authors establish a relatic.-I for thc change in the rcsis-~-an..,e of a
fen-r-,-,o,Sn,at in an external magnetic field. 'Llie con5ideration is l-'17,-LJL4-2d to fields
and te,-,,-'-)eratux~-5 at which the P~a-ra-pr-c"C'35G ti-ii-'es plac-e. The relat C'.1% i2stablished
is in the form,
Coro A
ACMS~;jo,,, NP: AP4037618
-:1gnetizatio:1' J and k7
x)T-.-\-iIq wi~R t- I - 1111, 111
cratures) tInd r "t given and ;"('1N'3
il) I th;~ su'll';talice" 3110w5 it to !)~2 th.-
1110 fact t"It t11(! c 'fficient A in the e,
CW
41:0 0-5 + 0-1 rather than ur-tity is difficult to ex "s
deterlainat n-of entails C011F n1lain Aj-1 experimcntll
W, dderlable difficulty in'view of its
t'v'ty to --mall ermM in J and J far from the Curie Point. Orig. art. has:
G
5 formulaz and 1 f-ij,
ASSOCIATION: None
SUBIUTTMY
SUB CODE: JECtFM
NR REF SOV: 004
ENCL: 02
MIER: 002
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L 00755-66~ W (1)104T (m)/T/3R(t)/3iP(b)/3iA.(h) IJP(c) JDIAT
ACCESSION MR: AP5021730 UR/0386/65/002/002/0075/0077
AUTHOR: Kikoin. 1. Ki% Lazarev,_.S. D.
q Y,
TITLE: Anisotropy of ihe odd-parity photomagnetic effect in germanium strong
effective magnetic fields
SOURCE: Zhurnal eksperimentallnoy i tooreticheakoy fiziki. Pialma v redaktsi
yu.
Prilozhenjje, v. 2, no. 2, 1965, 75-77
TOPIC TAGS': photomagnatic effect, germanium semiconductor, s!~miconftctQr jmspart-h.1
s.emiconducior theory
ABSTRACT: ~,Previous studies have shown anisotropy in both the even- and odd-parityll
photomagnetic effects in germanium. A microscopic theory for anisotropy of the
pbotoma Ic effects was recently developed by Kagan and Sobakin (Yu. Kagan, V.
Sobakinner! Phys. Chem. SoWs, 261, 1965 [in press]). According to this thecry,
when w (w is the cyclotron frequency of the carriers and x is relaxation time),
a unique atiomaly should be observed in the anisotropic component of the odd-parity'
photomagnetic emf V as a function of the angle 0 between the direction of the mag-;
netiefield and the normal to the illuminated surface of the semiconductor. The
_Curd 1/4

L00755-66
ACCESSION NR: AP5D2173C
authors measured the odd-parity photomagnetic emf in n- and p-gemanium at 770K.
The angular effect on odd-parity photomagnetic, eat in various field strengths for
both types of germanium is shown In fig. 1 of the Enclosure. The odd-parity an
sotropic photomagnetic eat is given as a 'function of magnetic field strength H at
various values of the angle 0 for both types of gemanium in fig. 2 of the Enclo-
sure, The experimental results show extremely good agreement with the Kagan-
Sobakin theory,, "The authors are grateful to Yu. Kagan and V. Sobakin for fruit-
ful consultation." Orig. art. has: 2 figures,
ASSOCIATIONt none
SUBMITTED.- MayO ENCL:, 02 SUB CODE: SS, 'M
NO RCF SOVi ..002 OTHER: ~001
CAM A

I I
f
I
i
rig., 1 -1 ~ I !

oo755-66
'ACMSGION MR: AP5021730
'wit
EMMOSURE: 0
00106

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E-

41

d 4/4.
Ca
r

t 003h5-66 t In (0)
~DW- JU
ACCESSION WRI fno.19224.11 UR/000/65100/00i/0124/0.126.
Af-1;5
AUTHOR: Main 1. 1C.1 i Senchenkovt Aq I'mans Es V'6 Korsunskiy, M, Ms;
Waurzakoy P
TITLEt Electric c2nd~~Yit~ and density of metallic vapor
Iq 'S~
SOURCE* Zhurnal ektperiment1licy I teoretitheskoy fitiki, v, 49, no. 1, 19659
,124-126
.TOPIC TAGSt mercury, electric conductivity,, pressure effect, temperature de_pendence~llp
high temperature research
ABSTRACT: The article describes an Investigation of the electric conductivitylof
more In the transcritical range of temperatures and pressures. The experiments
ere carried out in a chamber in which pressures up to 4000 atm could be establish-
ed by means of gaseous argon compressed with a thermal compressor. The mercury was
contained in a capinary whose mid-section could be heatL-.1 electrically to 2000C.
The transcritical conditions were established only In the middle part of the'capll-~
-.1arye The mercury vas activated in a reactor before the experiments,, and its den-.
'sity was determined by measuring tube y radiation from the 11j203. The measured
quantities were automatleally recorded with multichannel automatic plotters The,
I Card 1/2

.L 00345-66
ACCESSION NRs AP5019224
family of curves platted at different pressures made it possible to determine the
flelectr'ical. equation of state" r w.f(Po T) and the thermodynamic equation for the
density p - #(P, T).(r as re-sistivity, P - dennityl T = temperature, P - pressure).
The critical temperature of mercury was found to be 1450 1 50C. The measurement
accuracy was insufficient to deter.mine.the.temperat.ure coefficient of resistivity,
but it was found to be negative at densities below 7"4 g/cm3 and close to zero at
higher density, A more detailed description of the results and of the experiments
vill be published elv~wheres -0rigs arts hast 2 figureB;-
ASSOCIATIONt None
,PMMII-PTED t19Feb65 ENCLs' 00 SM CODE t EM, TD
NO REF SOV: 001 003
Card 2/2

L 8125-66 ZWT(1)/ZWT*~/EXP(b)/ZWPW UP(c). JO
ACCESSICH NRI UR/0181/GS/007/008/2564/2565
9111 -5. 41
ALITHOR: gh?i
:.n_,_I. K*; Lazarvvq S* D*
TITLE*. On the anLs9trqpy of the even pbotomagnetic effect Milk p--gerwniun in straq
wagnetic fifadd
SOURCE: Mika -wrdogo telag v. 7% no. 8t 1965j 2664-2565
~2)' If I/ f ~~