SCIENTIFIC ABSTRACT GUREVICH, A.A. - GUREVICH, A.G.

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
• Document Release Date: March 20, 2001
• Sequence Number: 10
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

A, 01revich (K. A. Umlryamw Avr. Anid. M,wm),
_P11u1TT_;Mv7"Xjak, S.S,S.R. 91. 12'2)J --Th,!
mWind It li~invft on the of It frrom
VINITNU1,11CI (11) to ii~~ITANLQI)j (III thitt Iq se-m&
tited by chlaraphyl! (1). The linaL. 01 v-1,(GjC*IIlNIICJN
t krifflA to dctd. wlarlmettiltaty. va, wo. ut%d conwia,
10 nt. I In 30% Ric., 6 drops or coned. N11i and I nil ' of
ToavoidtfindecreMcof
fluiintuin yield hy depletion of H donor unit the Interitunct
of light allwMtion by M, the exposuTe imut LLA only till a
ytry wittz brown color devlops, FmqtO ItUsi ninst be
'Intulla yield
URCAtuawkillimettight. The conitancy or qv~
In difleount fl,.tro of sWtrutu was not ctleckal, butIn prob-
able. The vwtlott yitJd Is ropo owl 0
the Itght InIcnAt

"*A photoansilizer In the pi cross of yhoto-
A,A. Gumvi-A (Lab. Plant Physiell. and Ifl-
-A--Tjh- 'AZr. Ac3A.. Moscow). Trudy
J;. . it -
ritst. ~rWd. miloeva ins. K. A. Timiryamla 3," No. 1.
amatmAtion wa5 achleved fQr (lie
AvsjjIx.,ttkm activity of chlorophyll. proposed
j(t" 61 phaqor
by T(nih-Y-Alev (0b Umviiii Sids Rdslrldro) .I St. PaAers.
botrg. 1675). Said. aq. soln. of o-dinitro!muenc (1) in
voluldrod(m witiq youuX wheat or Eladra plant5, iturnemd
vaqWfy irtio, libe solit.. nadement reduction the Went of
Vhkb vadoill with the extent of aeration (air expostin-) (If
~the PUM.- Uader cimulition of illumination I midergoc* re-
'dwitim im tb.--Vftrs pArtig of the plant at sti-h a high fit-
-.- hydro-Aylarnine h- not
'tC:jk Wt the cam:ipcoalb
,,,etyamed OU6 toal:- place only with high level of meratia
1311)
.1" the P"Waft or ahsence of Cos in the atm. dots not
Aftct t1m mdowflon, Thu3, the mitiction is tict a part of
iCOs rettetion tystoin. Lipts. with tht green -,listids of
chick-%vel:4 wA shniLtr plants showed definite reduction of,
1: the usact Wisfactory method of following the reaction
-d In I Ili Ht!O then
was by rue=s of filtcr-paper strim sol-AL
ldfk0l. stich suipo Weill: placed in the reaction cells contg. Olt
;iweds ItMicet. tll~n StMwCted to light introduced through
theopposi(O wool the couta."Im.
-,uall aniounts of a-ititroaviline
,by-*Aw tests. amialned
WX1 =W ntA of (~ititroi,Lcnyiliydroicylainine,
tam
Mot ~.i Ili thft dat L, or at liest a very strall
ion t
r
,trmwat. oll todStednit prndtwt~ ivas Immol in long vxpts.
(3 _Tkus; 1i (lie iiiota-id' vikwl Illi,
reaction terids to, stiolp at the hydrnTyiallillim Ili
dw rk'Ttl leal-the mdurtimi to go I I i i la iiii r l I miliol.
stage. Thc illmil"'ll"Ited plAMI& 111,11;'110im III t1w I'll-!
0' 11 Inol. 0 willf-11 i4 "qrNi'l If,ttt 140 tif
the inedium. A Me. v)ln. of dilotolivIlAwIlivil ~'illk 1 :11111
expwed to fir'llt in t1ke jjm~Lllce of VhKIINHI q
viyo3rowi 1-ciinetion of I to Or. 1:qi ; ill tie,
d3rk no maction tvijk place tjnk_-;r. 1,011 ,i t~nd.j,ll
to the Inixt'; In tll~almmccof 0110rollilvIl or 111INHWI! r"
mactimi took plave. Tlti~, tujit 44
by-direel: nltrat,imi fif A r'-acdo.l
wt ich I;j%L($jVC4I PhNIINIIi.ftCI, III,:. CT--.111rophyll ,All, :ltA
a ft%v dropq of Nltl,Off idso ji0iled sonje My-
droxYlainine. (detected by red t-)Ior in all- io 11.). "1 l1v
paral-sanwr is redliml more rtmilily th.-L-1 UIC 0rI1lOi-ntTWr.
Whell ascorilic 20d 1%as 11setl al 3-1 dolloIr, the solil. o* 1 :110:
chlorophyll treated with N11.011, sitnihr mlncilfm W L
occurred an illitinitiation. It itppeat,~ Iliat chlamphii: in
the natural state i's -L photocAtalyst Ivilich al-tivialf"s If. I
COU fict CaIL,f pI-bAehy(Irngt:nma:. ClIlotopliyll simil.-rfv
I.'S (.-III. r4hi.) tn I ill
limsence of light. Tlte. rca~tim~ns yield Ili-! hydi-mv! i,livo
deriv. M. KwoLlpolf
X

k~~ u il~ " ~v I ". ~ t " i-A -~ I -
GUREVICH, A. A.
Plont Physiology
Dissertation: *Invostigation of the Biochemical Transfer of Vydroeen
in Plants in Connection with Respiration and Photosyntheals.0 Dr
liol Sci, Inst of Biochemistry Imeni. A. N. Bukh, Acad Sci USSR,
I Apr 54. ( Vechernyaya Foskv~-, hoscow, 17 Rur 54)
SO: SUM 213, 20 Sept 1954

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0 C I U N1 T It Z Y Al
CATE GORY 'PLANIV PHYSIOLOGY. pl,

jiBS. JOU, R. :PEF ZHUR - 810L.(GYA, NO. 4, 1959,

ALTYHOR K0, 15242
Gurerich A,A.

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in th~: -Fresemte of

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s b. : Pairi, a t i a Ic ri d . N. A. Vaksluwva. M. I
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-1957, 21-,2-2L1
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~
w me -"It iii a piixture
of vmter -Y
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0.1 f~ solutioll

e d wa t r . Lo
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iit
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IC was adde
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nclant -a
r
All at.
11
in dire,:~t ratlio '.13 IJO
CARD,
C' UET2Y
F?Y
:.1L.1,NT PHMOLOCY.
Nn-. 4, 1959; No, 15242
AU T TITO R
T.-Dw
GPIG. PUB.
T
and Pro- ressed at the e-cj:)en:3e of the
P.
-0tc
ctOcildc-ai acti-,ration of if 2 C, e w a e 7,
-ne.work w.--:ts accomnished lc~t i;he Tin.-,
kcademy.--
CV RD: 2/2
SOV/20-126~5-60/19
GolOsoval I (0b
acorbic ~kc'( f rasuo9o
170) rurevicho Reduction 'WithAl etilOvogo
KUTHORS'. -Inc ed Us thylene Red novieniYel
JUC reakts" Vossta
TITLE-. ,,,t,irovannOY lotoy) j-zOr 5, py
askorbin0voy kis 1959, 70'
3)oklady kkademii nauk SSSR9 orthO dinitro-
PF -DICkL: the Y ac-
'RIO (,USSR) at the reduction of --sent'all rog-11
-t .. Proved th ascorbic wanox.vgen or hYcl- 180
lhydra4ine or oleoular O'e donor a
J?OrtmerlY henY .. hydr green
influence of the M Janus
A6B5TRJkCT: benzene With P.he _, this,reactiOn be used.
,elerated by t 1 2). ethylene re .. can
acoevtor,U organic
Oxide (Refs rogen dUCable olor 0 not run
per . e and 1368 hyd, represents
cyStein irreversible re -hange Of c
other lace With C not uni ue u itle.
and some ns taking I it is ~s jn t e t he easy
resct'o donor. Therefore be ca'lled E part Of t
These hich may hydrO-
thout hydrogen f a certain
0 the molecular
V1 n type reaction sctivates by the Jrre-
a certV-1 reaction the Oxidation 6rt to Jed to
such a of the donor hydrogen Per 'it wes tr
the other
movable hydrogen Of In this pape
gen the transmission acceptor,
r,arcl 1/4 versible reprod"O"ble

Induced Methylene Red Reduction With Ascorbic Acid SOV/20-126-5-60/69
determine how the movable hydrogen of the donor is distributed
between the acceptor and oxidator in the concerned reaction.
As hydrogen donor ascorbic acid was used, as hydrogen acceptor
methylene red. As catalyst copper sulphate and ferrous sulphate
were used. The methylene red molecule is reduced to a colorless
leuco compound (Ref 3). Methylene red behaved in the previous
tests quite analogously to the ortho dinitrobenzene (Ref 1).
Out of the fact that the reduction of I molecule methylene red
requires 2 hydrogen atoms follows that only 1/5 - 1/3 of the
atoms of the movable hydrogen of the amount of ascorbic acid is
used for it. The ascorbic acid is oxidized at this reaction.
The remaining movable hydrogen of the donor is oxidized by H 202'
This utilization coefficient does not depend on the concentra-
tion of the reaction participant. The ferrous sulphate operates
at the said reaction only in presence of the H 202 and not of the
molecular oxygen. But the latter operates in this sense only on
the catalytic effect of copper ions. The corresponding experi-
ments gave an analogous result as above, but showed a smaller
consumption of ascorbic acid. This can be ascribed to an
Card 2/4 exacter titration possibility than it was possible in the first

I.
Induced Methylene Red Reduction With Ascorbic Acid SOV/20-126-5-60/69
case. The said oxygen consumption was in oxygen stream 4-5 times
greater than on adding H202* A b o u t t h e m e c h
a n i s m o f t h e i n d u a e d r e d u c t i o n
The strong peroxidase effect of iron- and copper ions is known
(Ref 4). The copper ions also strongly catalyze the oxidation
of the ascorbic acid by the molecular 0 2 whereat H202 results.
On this the idea of the formerly described (Ref 1) induced
reduction can be based: the H 202 introduced from outside or
formed as above is activated peroxidaselike by copper- or iron
ions. This H202 oxidizes the ascorbic acid monovalently. There-
by arises its free radical - the mono dehyd-.ro ascorbic acid
(Ref 5). These radicals are a very strong reducing subetance.
Therefore its single movable hydrogen atom gets the capacity to
let transfer itself more intensively to the more difficultly
reduceable acceptors with a low redox potential as methylene
red, ortho dinitro benzene, and others. In this way the oxida-
tion of the first movable hydrogen atom effects the activation
of the second atom of the ascorbic acid and induces thereby the
Card 3/4 reduction of the acceptor. This is only possible in the presence

Induced Methylene Red Reduction With Ascorbic Acid SCV/20-126-5-6o/6a,
of copper atoms. At the presence of H 202 this reaction takes
place also in the presence of iron ions. The activated H-atom
of the mono dehydro ascorbic acid can of course be transferred
also on an active oxidator. Therefore, the utilization coef-
ficient of the movable hydrogen of the ascorbic acid does not
equal 5-d' but it is much smaller. The reason is that the ascor-
v70
bic acid oxidized by 0 2 is only the oource for H 202' The arising
of free radicals of the ascorbic acid was proved b A - I' Drokin
(Krasnoyarsk Institute of Physics of the AS USSR~ on Para-
magnetic way. There are 8 references, 7 of which are Soviet.
ASSOCIATION: Institut fiziki Akademii nauk SSSR g. Krasnoyarsk (Krasnoyarsk_,
Institute of Physics of the Academy of Sciences, USSR)
PRESENTED: March 16, 1959, by A. L. Kursanov, Academician
SUBMITTED: December 8, 1956
Card 4/4

V339
S/19 62/000/006/127/232
D256YD308
AUTHORS: Gurevich, A.A., and Golosova, N.A.
TITLE: Effect of ultrasound on oxidizing and reducing
reactions of hydrogen transfer
PERIODICAL: Referativnyy zhurnal. Avtomatika i radioelektronika,
no. a', 1962, abstract 6-5-42 n (V sb. Primeneniye ,
ulltraakust. k issled. veshchestva, no. 12, M., 1960,
147-150)
TEXT: To explain the oiological effects of ultrasound it is oft
interest to investigate the effect of ultrasound-on the oxidizing
and reducing reactions. One of such reactions is the transfer :)f
.-_ydro,gen _Lrom the donor (ascorbic acid) to the acceptor (the itiethyl
red) in the presence of ions of copper as catalyst. It was found
that ultrasound of a I-equency of 8bO xc/s and 7 vl,/cm2 intensity
considerably accelerates the transfer of hydrogen in this reaction.
[Abstracter's note: Complete translation-j
Card 1/1

GURXVI GOLOSOVA, N.A.
--LR~CH~
ek
Iffect of aeration on methemoglobin reductioa by ascorbic
acid. Dokl.AN SSSR 133 no.6:1458-1461 Ag 160.
(KIRA 13: 8)
1. Inatitut fisiki Sibirskogo otdoleniva Akadsmii mu
SSSR. Predstavleno ahmd. P.A.Rebluderom.
(NNTRWGUSIN) (ASCOnIC ACID)
(MIDATION4UMG?ION RUCTION)

_!~4AEVIGRq,-AA.-; GOLOSOVA, N.A.
Effect of aeration and hydrogen peroxide on methemoglobin reduction.
Dokl. IN SSSR 137 no.11211-2i-2 Mr-Ap 161. (MIRL U;2)
1. Institut fiziki Sibirskogo otdeleniya Akademii nauk SSSR.
Predstavleno akademikom P.A'.Rebinderom.
(Hemoglobin) (Oxidation-reduction reaction)

, GUREVICH., A.A.
Catalytic effect of peroxidaso on the induced reaction of ortho.-
dinitro-banzene reduction by ascorbic acid. Dokl.AF SSSR 145
no.2.443-446 Jl 162. (~MU 15:7)
1. Institut fiziki Sibirskogo otdeleniya AN SSSR. Predstavlano
akademikom P.A.Rebinderom.
'(Peroxidase) (Benzene) (Ascorbic a cid)

GUREVICH, A.A.
Demonstration. experiment on photosensitizing action of
chlorophyl. Nauch. dokl. vys. shkoly; biol. nauki no.3:
154-155 '64 (MIRA. 17:8)
1. Rekomendoirana Institutom fiziki Sibirskogo otdeleniya
AN SSSR.

ACCESSION NR: AP4036729
S/0020/64/156/002/0457/0460
AUTROR: Gurevich, A. A.; Trubachav, 1. N.; Rarberg, M. S.
TITLE: On the effect of hydrogen peroxide on nitrate reduction in green pjants
SOURCE: AN SSSR. Dolclady*, v. 156, no. 2, 1964o '457-460
TOPIC TAGS: nitrate reduction, hydrogen peroxide, algae, chlorella, nitrate,
ammonia, amination, nitrogen, biosynthesis
ABSTRACT: The authors investigated whether an external introduction of a physio--
logically admissible'concentration of hydrogen peroxide, under certain conditions,
would affect nitrate reduction in a plant and, so, produce an increase in ammonia
formation. The experimental subjects were one-called green algae (chlorella vulgaris.
a thermophylic, variant). From some of the experimental results, it was shown that
the addition of hydrogen peroxide to the nitrate solution, under either night or
daylight conditions, increased ammonia production from the plant to the surrounding
environment by an average of more than 1-1/2 times. When the nitrogen wag depleted,
however, the chlorella did not give off ammonia. It was concluded, therefore, that
for green plants, the biosynthesis of albuminous matter from nitrates was accomplish-
Card 1/2

;ACCESSION NR: AP4036729
ed with the assistance of the induced reduction reaction. Orig. art. has: 2 tables
ASSOCIATION: Institut fiziki. Sibirskogo otdeleniya. Akademii nauk SSSR
(Institute of Physics, Siberian Branch, Academy of Sciences SSSR)
SUBMITTED: 04Sep63 DATE ACQ: 16Jun64 ENCL: 00
suB coDE: LS NO REP SOV: 002 OTHER: 001
Card 2/2

it eluc ri on ef nl ir, by a
157 rin,
akudo..,akom

GUREVICH, A.A,, Jnzh.; ZAKS, A.V., inzh.; KASPAROV, G.H., in;,h.;
MUCHNIK, M.M., inzh.
Automatic control of vacuum driers. Mekh. i avtom. pro'kzv,
18 no.10:37-38 0 164. (MIRA 17:12)

is
6 .0 --6 --~f g-j P IT at IiW P "t /1 11 P
IL
MI/2531/65/Goar, vnAima
I
1 INT- AT-5019957
ACCESSTIOL
AUTHOR: -G-arelvich it A Loomv V. A.
TITLE The Un~oblpw of frictloavally d 191kn~ ~Mlalrv
--A
WURCH- MnIngrad. Glavmyag-eofizielmiihya~ab~eivato'rlytu' *mdJ ilog 177 Agos'
Atmosfernoye~elekLrichestvo (Atmospheric electricity)-, 61-89,
T
-PIC TkGS*. luminophor charge abrai;iv~ charge, friction,!
0 char :e!i Aerosol LOr- f~
ticle charge
4,5
ABSTPACT.-, Simultaneous measurement of the particle charge iLhd soe~~of _-ju~~,*hor's and:'~:,-
deve
abrasives has been carried out on the PZK-1 device,, 1OP& 8~ the Glavaqw. geoftziobes-
Abel
Imya observatorlya im. A. L. Voyeykova (Mon Geophysical Observatow.yh as dea:cj'. I
inthis.article. Charges and dimensions were obtained from. the trajebtory parwlieters.of
particles failing freely between the vertical plates of a plane parallel capscitor. tests,
yielded quantitative measures characterizing the totality of observed charges of a: I=Lnopnor_:
The ob-I
(70% ZnS with 30% CdS) and an abrasive (99% of At -)owrler form.
P3) in, mic-riaL
served symmetrical charging of luminophors during the use Qf glal;s ivid.P:_;Vt
atomizers anti sharply asymmetric charging In tne me of metglltc Oiu* .,era s in good
agreement with the resuUs obtained by Kunkel (L. Iteb, Statichoskaya. eMctrizataLy-ap

SHISHMAN, D.V., kand. tekhn. nauk; MEXHOVA, N.N., inzli.; GIMEVICH4. A.A.,
inzh.; IKHTEYMAN, F.M., inzh.; Prinimali uchastiye: ROZET, Me.,
inzh.; KAPLAN, G.S.; KAZIMIR, A.P.
Light-weight RVO-35 valve-type discharger. Mekh. i elek. sots.
sellkhoz. 21 no.3:60-62 163. (MIRA 16:8)
1. Leningradskiy filial Gosudarstvennogo isaledovatellskogo
elektrokeramicheskogo Institute. (for Shisbman.,Mekhova, Gurevich).
2. Nauchno-issledovatellskdy institut mekhanizatsii i elektrifikatsii
sel'skogo khozyaystva Severo-Zapada (for Ikhteyman).
(Electric protection)

SHISHMAN, D,V,, kand.tekhn.nauk; GUREVICH, A.A., inzh.
Experience in using "vilite" arresters, Elek.sta. 33 n0.12346-51
D 162. (MIRA l6112)
(Electric protection) (Electrio power distribution)

VOLKOVA, I.B.; NALIVKIN, D.V.; SLATVINSKAYAj Ye.A.; BOGOMAZOV, V.M.;
GAVRILOVA, 0.1.; GUREVICH ',-A-&; MUDROV, A.M.; NIKOLISKIY, V.M.;
OSffURKOVA, M.V.; PETREN I A.A.; POGREBITSKIY, Ye.O.; RITEMBERG,
M.I.; BOGHKOVSKIY, F.A.; KIM, N.G.; LUSHCHIKHIN, G.M.; LYUBER,
A.A.; MAWDONTSOVp A.V.; SENDERZON, E.M.; SINITSYN, V.M.; SHORIN,
V.P.; BELYANKIN, L.F.; VALITS, I.E.; VLASOV, V.M.; ISHINA, T.A.;
KONIVETS, V.I.; MARKOVICH, Ye.M.,- MDKRINSKIY, V.V.; PROSVIRYAKOVA,
Z.P.; RADCHENKO, O.A.; SEMERIKOV, A.A.; FADDEYEVA, Z.I.; BUTOr-Aq
Ye.P.; VERBITSKAYA, Z.I.; DZENS-LITOVSKAYA, O.A.; DUBARI, G.P.;
IVANOV, N.V.; KARPOV, N.F.; KOLESNIKOV, Ch.M.; NEFEDIYEV, L.P.;
POPOV, G.G.; SHTEMPELI, B.M.; KIRRIKOVIP V.V.; :LiVROV, V.V.;
SALINIKOVY B.A.; MDNAKHOVA, L.P.[deceased); MURKTOV. M.V.;
GDBSKIY, I.I., glav. red.; GUSEV, A.I., red.; MOLCHANOV, I.I.,
red.; TYZHNOV, A.V., red.;,SHABAROV, N.V., red.; YAVORSKIY, V.I.,
red.; REYKHERT, L.A., red.izd-va; ZAMARAYEVA, R.A., tekhn. re4
(Atlas of maps of coal deposits of the U.S.S.R.]Atlas kart ugle-
nakopleniia na territorli SSSR. Glav. red. I.I.Gorskii. Zam.
glav. red. V.V.Mokrinskii. Chleny red. kollegii: F.A.Bochkovskiy
i dr. Moskva, Izd-vo Akad. nauk SSSR, 1962. 17 p.
(MIRA 16:3)
1. Akademiya nauk SSSR. Laboratoriya. geologii uglya. 2. Chlen-
korrespondent Akademii nauk SSSR (for Muratov).
(Coal geoloam-Maps)

GOR, Y!j-l . ; 6UREV 1,-,i: , -*~. D. ; "A , ;',. 1 ~
Ana."Lovugs of the Kume'.5k Iri 1,he, Ncxil~jk ri~~ric)n. lzv.
ALN S~;"3111. Ser. geol. 30 no,,6:92-94 je 165.,
(MIMA 18:6)
1. LaborntorJya geologal uglya Instituta. geologil I L?-nfizik.L
Sibirskogo otdeleniya AN SSSR, Novosibirsk, i Instilut geologii
'.rkt,iki Leningrad.
.4

GUREVICHY A.P.
Paleogeography of tile Norillsk region in the Tate Paloozoic.
Uch. zap. NIIGA. Reg. geol. no.2:30-48 164.
(1-11IRA 19: 1)

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-ling rin the W content) with :1 4 cc. tit !di% HCI
= 0
with tlrt)pwiw adft. of HNfh and then hod tor 2-3 min.
0 Pil. the win. with hot water and filter. Wasilt the beaker
3 times with hot water, and cliswAve the ppt. in the filter
4111 Into the -W"W beaker with I ie. of hot 5% NSOH. Wit'll 0
ve the fillef.1 .1 tim" with hot water and evap. the WCh a4it.
00 on a water bath to about 0.5 m. After the Aildn, of 0.5
cc. H,PO. K 1-7) and 3 cc. of concil. HCJ, treat thtsoln. roe
of with 2 cc. of the SnClj win. (obtained by &q*4vion .5 x. of
grantilated So in Hit) cc. ofA0% 110). After III - IS nihi.
make up the solo. to 10 cc. with water &nil compare the 0
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front st"t'k of kit wn W cmtent-t. cha't. Ohmic
roe
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1. N. V. lxvr andil. rGu"redvich. Zavoilskap Lah.
it. N.P. 1. It IT(Im)-sell. twiw4d# inclusismis ill I&
Iftl .6111pit by anodic MAU.. trandcr the rievilolytic Ir'i-
Ito froul Abe culloilim 1*8 tog"her with the dLvU(Avtr
.1 beAer. decomp. the dectrolyticNinOt by adding 2 J
a. oc-Na " taitmatc. beat to 51)-W*. k2 mand at tbi~
ICpmp. for I hr filter nub with cold water until so lemc-
16. 1. so.-I m tran4rr the Pvt. and fill" 1'. a
beaker, mist 111cm W a fir water. then Im Ild"4 lict
0:5), beat the An. to boiling. kcwp on a water luth I;ir
W20 law., OW Alter Into a DW-ca. Inmurind 4-k.
O"live the arl. Litipwitim mW temm Cl - in uuc-trtitb,A
the vAtt. by homating with INSO, anti H.N(h unid S),
atid dot Mn by the pnoulfaic imthmi.
kecak 17,011. content to Silts, dcdlsct tile ck"Itent'-f S
bound lu.%Infrtxn the total commit of Sin the steel sautpic
anti cmic. FeStmusbemidualS. Fight rvicrencrs.
W. it. lienn
ma low Now I.I.J41 -am*
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""CIIIIS ANO
A.Vorshunov..M-N-
Stat
Z, V~l I "d of the
Cl- with 3-6 nrd~. of ale. to make the
content of ale. at the equiv. point ciloal to 55-GVO'.
transfer the soln. to an clectrolyzer equipped with a ttibe
for passing III, and titratc with PbMa)i solo. of a conen.
2-3 times that of the Cl-, pouring the titrating soln. into it
tnicroburet with its end immerse([ it, the clectmlyzer. A
const, Potential of approx. 0.9-1.1 v. is kept throughout
the titration. Measure the diffusion curTent after each
addn. of 0.1 mi. of the titrating soln. and tuix the con-
tents of the clectrolyzer by a current of If, or some other
gas. Plot the no. of rul. of Ilb(,NO,)- u%ed for the titraflon
on the X-axis and the diffusion current on the Y-axis. A
const. diffusion Current indicate% an excess of Cl- in the
soln. which binds the Pb ion in the ppt. Deviations from
this position indicate the -appearanec of free Pb ion, i.c...
theendoltitration. Aimallexces,.iofPb(NOl)tl.-;adifcd
anti a correction for the current due to the soly. of PbC1 -
is made by drawing a straight line parallel to the X-*.xis
on the Ph wave fit satd. PI)Ch soln. from the horizontal
region of the diffusiost curretit to the intttsection Nvith tht
titration curve. The abscisna of this point corrcipoiull
n
to the no. of nil. of Pb(NOj)x used to rcuch the equiv. poi t.
X - 58.4(ion/m (X Is the Content of NaCI in ml., is the
titer of Pli(INO)), solo., n the no. of mi. of Ph(N(N)t
used, anti its the no. of tnl. or NaCl used for the analysis).
W. R. lkru~_.
4.
Jill

0 0 0 0 0 0 0 0 0 * 0 0
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USSR/Sclid State Physics - Phase Transformations in Solids, E-5
Abst Journal: Referat Zhur - Fizika, wo 12, i956., 34687
Author: Leve, N. F., Gurevich, A. B.
Tnstitution.: None
Title: Tnvestigation of the Effect of Heat Treatment of Steel on the Composition
and Wature of the Nonmetallic Inclusions
Original Periodical: Collection: Svoystva i term. obrabotka transp. metalla,
KharIkov, metallurgizdat, 1955, 205-222
Abstract: T11o eTfect of soaking at 900-1,3000 on carbide and sulfide inclusicms in
various steels and on ferrous oxide in armco-iron is studied, Chemical, microscopic,
amd metallographic analysis methods were used.. It is shovn that heat treatment of
specimens at 900-1,3000 for 30 minutes does not change the composition and the shape
of a sulfur and oxygen inclusion in carbon steels or in alloyed chromium and nickel
steels, and leads to a noticeable spheroidization, starting with 1,0000,_of ferrous
oxide Im armco-iron. As a result of a longer beating at 1,3000 (15 hours and more),
there is a partial spheroidization of the sulfides in steels and a contamination of
the nonmetallic residue by oxides of iron and chromium. -In steel alloyed with
1 of 2 - 1 -

USSR/Solid State Physics - Phase Transformations in Solids.. E-5
Abet Journal: Referat Zhur - Fizika, No 12, 1956~, 34687
Author: Leve;, N. F., Gurevich, A. B.
Institution: None
'Pitle: Investigation of the Effect of Heat Treatment of Steel on the Composition
and Nature of the Nonmetallic Inclusions
Original Periodical: Collection: Svoystva i term. obrabotka tranBp. metalla,
Kharlkov,, metallurgizdat, 1955, 205-222
Abstract: chromii= and tungsten (up to one percent)., the spheroidization of sulfide
inclunions is clearly seen vhen heated to 1,3000 for 30 minutes. The carbides of
iron and manganese beccime transformed as a result of similar heat treatment into a
solid solutien, and the contents of iron and manganese In the nommetallic residue of
the. hardened specimens diminishes sharply.
2 of 2 - 2 -

Determitutti" sullideis and oxides at mangaaesifM,
---Hock f
wbon steel and theEldeow 4M manganese cartilans.
and apaskaya IA&. 21110*~
QW"N14 c1tratif dbL401VO NNIC
t do not break up the double cartildo of Mr4C anti F4C
Tilectrolytit treatment of C-Mn steels with an att6lyto of
-tilmlyle 01 10"ts
XDr contg.,10% citric acid and a c 'I
CUSO, and subsequent treatment with 10% Na c1trate sit,
witia(KH.W.dissolvedonlyz pirtof thecitrbidm- 30 369,
Afn,C and 51.9 F? Fete in the 1st golvelit and' Rmv,
h(ii,,C anti 43.76% FeC in the Nil Eolvent from a hitilt-lifil
Steel (C 1.24. Mn 9.00, S 0.000%) nitil 111.20% NNIC and
SS.32% Ft!tC by the Ist solvent and 23.4(1% IWIC and
46.60% Fe,C in thc 2nd solvesit from a Nrrutrianpriese steel
Thus the existence of (Mn,C),
1: FcjC), is substantiattA. Tht rmal treatuactit at OWO arid
juenching in ft%O brings the earbides hito it solid StAn. with
SU115; JlCat the MMI)IO (0 '")' for J() 211111. 111111 (11jench in
HtO tit I.3W' does not affect tht: results). Dis-
("- 21
solve and1l. lyr in a neutral soln. Filter and wash the res-
idue free ,I the chctrolyte. Stir with IM in). of 10'7~
(NI-14).SO~ for I hr. tit roorn teinp. Anti filter. (a) Mic tit-
irate contains the "unstable- hInO (th,firittl ns that NftiO
which is sat. in I(W. (NII.),M). Theterni).lannimlortant
factor since at higher temps. such comptis. as Mri silicattli
May dissolve. (b) The rtsidus- is boiled wilik 100 mt. HrSof
(1:3), filtered, evapd. with 5 ml. IINOI and 10 ml. lIsSO, it)
1
the appearance of S% futnes. cwlktl, dild. to 250 ml., and
MnS Llctd. W The hisol. residue is fused with Na,C(h, dii-
sq)ved in IlCl, and MuO detil, 1. Berstowitz

/-"o'A
Tra ris la tion froin: Referativnyy zhurnal, Metallurgiya, 1958, Nr 5, 1) 327 (USSR)
A UTHORS: -Gurevich, A.B., Kalina-Zhikhareva, V.I.
TITLE: Employment of Cationite5 and of Trilonometric Titration for
Determination of Arsenic in High-arsenic Alloys (Opredeleniye
mysh*lyaka v vysokomyshlyakovistykh splavakh q primenemyern
kationitov i trilonometricheskogo titrovaniya)
PERIODICAL. Tr. Nauchno-tekhn. o-va chernoy metallurgii. Ukr. resp.
pravl. , 1956, Vol 4, pp 127-130. Comments, pp 131- 1137
ABSTRACT: As is separated from Fe by means of passing a solution of the
alloy through an ion exchanger containing 60 g of sulfocarbon or
40 g of KU-2. The As is precipitated in the solution by a mag-
nesia-ammonia mixture. MgNH4AsO4 is filtered out and is dis-
solved in HC1 (1:1); after adding NH40H, a buffer solufion, and
an indicator (acidic, dark-blue Cr), the As is titrated with a
solution of trilon B. Another method of titrating As with trilon
B is also described. The results of determination of As in fer-
roarsenic are presented in a tabulated form.
1. Arsenic compounds 2. Arsenic--Determina-uion P. K.
Card 1/1 3. Titration--Applications 4 Ions--Applications

16(l) PHASE I BOOK EXPLOITATION SOV11818
Gurevich, Avigdor Berkovich (Viktor Borisovich), and VaBiliy
Pavlo i-ch MinorskTy--
Uchebnik analiticheskoy geometrii dlya vtuzov (Textbook of Analytical
Geometry for Vtuzes) Moscow, Fizmatgiz, 1958. 163 P. 35oOOO
copies printed.
Eds.: R.Ya. Shostak and V.A. Solodkov; Tech. Ed.: S.N. Akhlamov.
PURPOSE: The book is intended as a textbook on analytic geometry
for students at vtuzes.
COVERAGE: The book is written according to teaching programs which
include 360-400 teaching hours for mathematics. The book contains
a brief, but complete and accurate, presentation of the methods of
plane and solid analytic geometry. The fundamentals of determi-
nants and vector analysis are presented, and are applied to the
study of analytic geometry. No personalities are mentioned.
There are no references.
Card 1A1

25(l) PWR I BOOK KXPL40ITATION SOV/2132

X17ev. Ukrainskly Nauchno-loolodov4tel'skly Institut ast4llOv
?ekhnologlys proizvodatva I avoystva charnykh metallov, obarnik
(The Manufacture and Characteristics of Ferrous Metals; a collection %
of articles) Khar-kov, Khar-kovskiy Som.unlv. lm. A.M. Oor'kogo, 7
1951- 271 P. (sort** Its: Trudy, vyp. 4) Errata allp In-
sorted. 1.000 copies ;rlted.
Zditorial Staff of this back, P.A. Alsksandrov, D.3. Xazarnowakly,
N.I. Kur'"nov, X.F. Lave, V.P. Onoprlyenko, V.A. Tikhovskly, and
To. A. Shneyeravi
Id.i S.S. Liberman, Tech. Ed.t K.O. Gurin
PURPOS93 The book Is intended for the scientific personnel Of
Institutes and for engineers and technicians of metallurgical
enterprises and other branches or the industry.
COVKRAGX: The collection of articles reviews the work carried On at
the ljnfttltut* of Metals on the technology of blast furnaces, Open-
hearth furnaces, and rolled stock productlon. It
with problems In notallography, heat treatment of ferrous metals
and methods for their study. Particular attention L: devot!d
tol
the preparation of charges and blast rurnace practic with In refta0d
c
Sam pressure, open-hearth production with oxygen blast anti rolllng
of light profile$. NO personalities or* mentioned. References
accompany each article.
TABIX OP CONTENTS t
3C=Wj OF UTALS AND IMAT OMTA.L TREATMENT
gur=nqy_ R..Z.. and a.Q. Sa2ov'yaV4.IBPOrtanc& of Resilience Tests
rd-r-l-vaji-astion of Shiet-Steal Quality 221
~tsedln ?tT- causes For Formation of Plakea in Steel 233
Dyubln, X.P., D.S. XszarnOvA1ay,-K,%. Klimov,
T.G. augulsphtlll' ftEd_'O_R-1%=An . r.vention of
Flakes In 25 01-WAfle mdo7of Open-heirfh 3t*ol 243
MMODS OF STUDYING TfUt qUA.L1TY OF METAL
Love X P. and A- - The Composition of The Carb-'d& MSG@
aw 6arbon &md jev_&lloy steel$ 257
Un&ljoy~
XLkitinas Gel_ P.O. _Lklyar~ and Z_jQ. Miroohnichen P.
LOW 'ConcentrationA of Slaments in Stool.by Sp4ccral Methods 261
AVAILABIZI Library of Congress (TX 60T.T4)
TX/60
card 616 9AI/59
j"r

GUREVICH, A.B.
Lithology and coal potential of lower Carboniferous sediments in
the Belgorod-Oboyan' area. Izv. vys. ucheb. zav.; geol. i razv. 1
no.12-.17-37 D 158. 09RA 12:12)
l.Leningradskiy gorWy institut.
(Belgorod Province--Coal geology)

IjVZ, N.F., prof.; GUREVIG A,#,B..,-kand. khim. nauk
Constitution of the carbide phase in low-carbon unalloyed and low-allov
stools. Trudy Uk:r. naii6h.-issl. inst. met. no.4:257-260 '58.
(ERA 12:3)
(Steel-Ketallography)

KUR~WIIOV, M.I., kand.tekhn.z)auk--, LEVE, N.F., prof.; SOLOVIUM, G.G.,
inzh.-, MWICH, A.B., kand.khim.nauic
_W_
Effect of arsenic on the reversible temper brittleness of
alloyed steels. Trudy Ukr.nauch.-issl.inst.met. ao.5:202-211
159. (MIRA 13:1)
(Steel--Brittleness) (Arsenic)

3/137/60/000/02/08/010
Translation fromi Referativnyy zhurnal, Metallurgiya, 1960, No 2, P 261, # 3887
AUTHORS- Kurmanov, M.I., Robruskina, Sh.R., Leve, N.F., Gurevich, A.B.
TIM.- Phase Distribution of TitaniumAnd Its 9ffect on the Properties
of High-Strength Low-Alloy WAIOT (15ODYuT) -)Steel
PERIODICAL: Sb. tr. Ukr. n.-i. in-t metallov, 1959, No 5, pp 212 - 222
TEXT: Investigations were carried out into phase distribution of Ti and
Al in 15GDYuT steel and into-the effect of these elements on the steel properties.
Specimens were cut out of hot-rolled 24-rxn thick sheets In the'after-rolling and
after-normalization state at 8000- 1,2000C. The steel was composed as
follows (in %): C 0.10-0.13; Mn 1.20-1.34; Si 0.13-0.17- ~U 0.36-0-.39; Titot
o.o86-o.o8l,- Altot 0.11-0-053; N 0.024-0.038. It was established that In hot-
rolled steel 85% of-the total Ti amount (0.1%) was contained in the carbide phase
and 15% in the solid solution. In steel normalized at 8000, 900o and 1,00000, the
Card 1/2 V13'

GUREVICH, A.B., kand.khim.nauk: URUM, O.M.. inzh.
Phase analysis of titanium steels. Trudy Ukr.nauch.-isel.inst.
met. no.5:249-256 159* (MIRA 13:1)
(Titanium steel-Metallography)
(Phase rule and equilibrium)

30)
AUTHOR: Gurevicn, A. B. 51 C 7 7 - 3 ~ //5 8
TITLE: On the Lower Carb-oniferous Deposits of the Belgo-rod-Oboyan,
District
PERIODICAL: Doklady Akademii nauk SSSR, 195,-j, Vol 127, N" 5,
pp 1074 - 1077 (USSR)
ABSTRACT: The district mentioned in the title is situated in the soAth-
western part of the Kursk magnetic anomaly ( Mal) in the iron-ore
district of Belgorod. The deposits mentioned in the title were
discovered by prospecting in 1953. In the South they overlie
denosits of Proterozoic iron ores and in the North and East they
contain workable coal beds. The author investigated these Ade-
posits in detail in 1956-58. Lower Carboniferous is represented
also in this case by the Visean stage which contains the follow.-
ing horizons: Stalinogorskiy, Tullskiy, Lleksinskiy, ',"ikhaylovs-
kiy, and Venevskiyq furthermore in the South also the Serpukho,,rs-
kiy lower stage. These deposits are stratified on a considerably
structured surface of the pre-Cambrian fundan-,ent and are covere6
by I'desocenozoic deposits (290-470 m thick') . From the structural
point of view the Lower Carboniferous deposits form the northern
edge of the Dnepr-Donets depression.. They slope to the South---West
Card 1/2 at an angle of 2o-35'. The horizons mentioned above are dividc-d

On the Lwver Carboniferous De-;osits of tte Bel-~orod- SOY / 2o- 127 -5, -39/5 5-
Oboyan' District
into 3 sedimentation cycles. These cycle3., their flora (SpDres,
determination by K. 1. Inosova), and their fa-ana (Fora.-manif era,
determined by Ye. V~ Fomina; Brachio-poda, determined by P, Dona-
kova) are described. They are compared with other parts of the
Russian platform. There are 5 Soviet references,
,kSSCICIATION: Laboratoriya. geologii uglya Akademili nauk SSSR (Laboratory of
Coal Geology of the Academy of Sciences, USSR)
PRESE1,TIM.- llvlarch 21, 19159, by D. V. Nalivkin, Academician
SUBMITTED: March 18, 1959
Card 2/2

GUMNICH9 A.B.
Lower Carboniferoun of the Voronezh antealise. Dokl. All SSSR 135
no,3:682-685 N 160. (M-4 13:12)
1. Laboratoriya geologii uglya Sibirskogo otdeleniya Alkadeudi naWc
SSSR. Predstavleno akad. D.V. Nalivki--qym.
(Belgorod Province-Geology, 9trati'.--,ra5hic)
(Kursk Province-Geology, Stratigraphic

GUREVICA, A.B.; TURUBINER, L.M.
Acidless separation of oxide inclusions from carbides and
sulfides in carbon steel. Zav.lab. 29 no.3:28Or282 163.
(MIRA 16:2)
1. Ukrainskiy nauchno-issledovatellskiy institut
metallov.
(Steel-Analysis)
(Oxides)

5/032/63/029/003/005/020
B117/Ble6
AUTHORS: V1rAU~4L,_A__" Kirzhner, 0. M., Sandler, N. I., and
Murav'yev, V. N.
TITLE: Determination of cerium-containing inclusions in alloy steels
:..~PERIODICAL- Zavodskaya laboratoriya, v. 29, no. 3, 1963, 283-286
TEXT: Cerium compounds formed by introducing small amounts of cerium in
alloy steels were investigated. Steels containing 0.05 - 0.12% Ce,
0.60% bin, 0-30 - 0.40% C, and 0-3~a S were-used. The nonmetallic phase
was separated by dissolving the steel specimens in the usual iron sulfate
electrolyte with complex formers. The anode alime'was first treated with
30% copper ammonium chloride solution containing 1% FeSO and 5~ ammonium
4
citrate, and then with iodine solution in potassium iodide; subsequently,
the slime was studied petrographically and by x-ray anal sis. Cerium
compounds were found in the form of sulfides (CeS, Ce 2S 3~ in the steels
investigated; no oxysulfide compounds were detected. Since cerium sulfides,
soluble in hydrochloric acid, are insoluble in iodine solution, they can
Card 1/2

S/032/63/029/003/005/020
Determination of cerium-containing ... B117/Ble6
be easily separated from iron and manganese sulfides. The amount of
cerium inclusions in the steel was independent of the total cerium content.
This was due to the high degree of liquefaction of cerium sulfides and
their irregular distribution over the cross section of specimens. The
electrolyte residues contained much more cerium than the sulfide phase.
Cerium was irregularly distributed in the sulfide and the carbide phase.
In the carbide -ohase, it was contained in the cementite lattice which was
confirmed by x-ray analysis. There are 5 figures and 3 tables.
ASSOCIATION: Ukrainskiy nauchno-issledovatel'skiy institut metallov
(Ukrainian Scientific Research Institute of Metals)
Card 2/2

17 " " ".I
SAITLEI", GURVIG"i. A.B.; NA'iRfj7lr~',' !--"!: !.'I. _,, 7 - ! : J.- -',~ ~~ *, . ~ 1 - . :, T , - ,
L.M,., XfRZHkJ'ER, rLM .
Phase d.JstrlL-.-i+imi of veLnadl--,Lm: and -il
lo-w-alloy stesl5, Sbor. tvi~:. ~114LMnc.904.9-'zi~ '~,'
I -- .1 J-
, - 4 " s 4 --,, ')
I

GUREVICH, A.B.
... - - I
Distribution functions and the Darboux property. Dold. AN BSSR
9 no-12:725-787 D 165. (MlIful 1~: 1)
1. Belorusskiy gosudarstvennyy universitet imeni Lenipa.

ARAKELOV, A.S..t BORISOV, V.A.; GALIPMUN. I.I.; GURETICH. A.G.; DOVZHU,
G.T.; PARS IF, R.N.; SOKOLOVSKIY, S.M.; SIMIKHOV, V.L., SHIFRIH,
D.L.; ETKIN, H.V.; GETIYE, V.A., red.toma; YELIN, V.I., red.toma;
SOLDATOV, K.N., red.toma; SVYATITSKAYA, K.P., vedushchiy red.;
TROFD40V, A.V., tekhn.red.
(Equipment used in the petroleum industry] NeftianGe oborudovanis;
v shesti tomakh. Moskva, Gos.nauchno-tekhn.i2d-vo neft. i gorno-
toplivnoi lit-ry. Vol.l. (Compressors and pwTul lompressory i
nasosy. 1958. 234 p. (MIRA 12:5)
(Petroleum industry-Equipment and supplies)
(Pumping machinery) (Compressors)

GURTVICH, A.G.
Use of plastics in some branches of the machinery InduBtry.
Biul. tekh. Skon. inform. no.9:86-90 '59. (MIRA 13:3)
(Rachinery industry) (Plastics)

GUREVICH, A.G.; STRONGIN, M.A.
Regulating the amount of materials used in tire manufacture. Kauch.
i rez. 19 no.6:45-47 Je '60. (MIRA 13:6)
1. Hauchno-iseledovatellskiy institut shinno7 promyshlonnosti.
(Tires, Rubber)

(A
AUTHOR: Voronova, A.V. and 'Gurevich, A.G. 109-4-5/20
TITLE: Nvaluation of the Propagation Constants of a Rectangular
Waveguide with Ferrite Plates. (~ascfiet'pqstdyw=kh ras.-
prostranona.ya v pryamougolnom volnovode s ferritovyml
plastinami)
PERIODICAL: Radiotekhnika i Zlektronika, 195?, Vol.2, No.4,
pp. 401 - 407 (USSR)
ABSTRACT: Two waveguide phase-shifters are considered. One of these
comprises a ferrite plate of thickness H , which is placed near
one of the narrow walls of the guide. The second phase-shifter
comprises two ferrite plates which we parallel to the narrow
walls. The longer walls of the guide )xave a length a , and
the plates are magnetised perpendicularly to the axis of the
system. The plates are characterised by a permittivity e and
magnetic parameters IL = 0.9 and a ; the permettivity and
the permeability of the guide were assumed as co = 140 = 1.
The propagation constant y of the guide with one ferrite plate
can be found by solving:
Card 1/4 x Ctg xh + x ctg x 1, + 0 (2)
u 0 0 UU
109-4-5/20
Evaluation of the Propagation Constants of a Rectangular Waveguide
with Ferrite Plates.
where: 2 2
0
2
x0 2
k6 2
y
k
0 ~j 2 Vr
C )6
Q2
1126.0 IL

and
t a
h.
7
Similarly, the propagation constant of a guide with two plates
can be found from:
x ctgh x - x0tg x1Dj 4. CLY 0 (3)
Card 2/4 it,,

109-4-5/20
Evaluation of the Propagation Constants of a Rectangular Waveguide
with kerrite Plates.
,Bquations (2) and (3) are given without derivatJpn; they are
presumably takenftm a paper by V.V. Nikolskiy LlIef. ~J. The
equations were solved numerically by the Nowtonra matho-d by.
employing a fast electronic computer. The calculations were made
for two directions of propagation (or two directions of the
magnetising field), corresponding to the propagation constants
Y+ and y_ ; and for the following values of the variable
parameters: a 0 to 0.5 0 a 3 to 11 h = (0.08 to 0.26)a
and X = )LO I X , where XO :0 1.39a and$ 4XV = 0*05 The
calculated results of y+ and y_ were used to evaluate the so-
called non-mutual phase-shifts
I = (y,. - y_)a (5)
and of its frequency coefficient:
Card 3/4 1101 - 110?- X0
101 2 A%

109-4-5/20
Evaluation of the Propagation Constants of a Rectangular Waveguide
-with Ferrite Plates.
Where qo, was calcu2ated for hi a ho - A and nw for
X2 = XO + AX2 - The values of q and I are *plottad as
functions of all the above variables for both the phase shifters
(single-plate and two plates). Altogether twelve sets of graphs
are given. By comparing the results obtained with a single plate
(?I,, and Kl) with those for the syptem with two plates (12 and
~2) it is seen (Pigs. 9 and 10) that the latter gives a band-
width about twice larger than the former.
There are 6 references, of which 3 are Slavic.
MMMITTED: Octobe~r 25, 1957.
AVAILABLE-. Library of Congress.
Card 4/4
4 - C_
109-7-13/1?
AUTHOR: Gurevich, A.G. ipsoid with Tensorial parameters.
TITIR: Internal Field in an Ell ametrami)
(Vnr~ren ellipsoide s tenzornYmi Par
epegwRoltev)
r1 e I m ka, 195?, V01-II, NO 71
MIODICAL: Radiotekhnika i Xlektronj pp. 93? - 939 (UiSR)
'= is situated
ABSTRACT: An ellipsoid having tensorial PerWbility 11 um having
in an external uniform magnetic field Ho in a medi
scalar permeability 40 . It is shown that the internal field
of the ellipsoid is given by:
_V - 'MW (1)
HO 4 is the tensor
where I is magnetisation of the EEJljpsoid~
*of the de-magnetising factors. The internal field is also
related to T--and % by eq. (2). Consequently, the external
field can be expressed by:
-0 ~ 1# (3)
R - IM6
Card 1/2

109-7-13/17
Internal Ifield in an Ellipsoid with Tensorial Parameters.
in which the tensor lam is given by eq. (4) where I is unit
tensor, and 0 is expressed by eq. (5). If the tensor # is
expressed by means of its diagonal components N. I N y and N.
then the tensor I is given by eq. (6), which is the solution
of the problem.
There are 3 references, I of which is Slavic.
SUBMITTED; January 11, 1957.
AVAILABLE: Library of Congress.
Card 2/2

AUTHOR: Gurevich,-.A.G. 109-8-3/1?
TITLE: Quadratic Relationships for the Media with Tensorial.
Parameter5. (KVadratichnyye sootnosheniya dlya sred s
te"ornymi parametrami. )
PERIODICALt Radiotakhnika .1 rllolctronika, 195? Vol.II Na.8
P-P. ~60 - 968' (USSR').
ABOTRACTz The purpose of this work is to derive the principal,
qua&rabic 1ctraliata f'or tfie medla represented by tensorial para-
meters and 'to analyse certain corollaries resultino- from tbem.
These aro of interest in -the ultra-high frequency techniques.
The basic quadratic lemmata can be derived from the Maxwell
equations for two electro-magnetic processes occurring at -two
different frequencies and having different external currents and
tensorial parameters. In the Gaussian system of units, the
Maxwell equations can be written as shown by equations (1), (2),
(3) and (4). From thesef the quadratic relationships are
eiressed in terms of complex amplitudes, by equations (5), (6)
(9 and ('10). These represent a generall*zation of lie quadrat-.1.c.
lenhiiata, as formulated by Kisunko (~ef.lj, in particular, for
the media witli difl'oront and tensorial paramell-ers. For t1he case
of equal parameters of the media and equal frequencies, the
Card 1/41emma is given by equation (11) which is a generali,_,ation of

Quadratic Relationsbips for the Media with Tensorial arameters.
the known Lorentz lemma. I'Ihen the media are reDI-Csatited by
anti-symmetrical tensors, equation (11) leads tothe atandard
Lorentz lemma as given by:
(14)
47 div (E 1 x H2 - E2 x H1) + jCM2 El - jcm.122 = 0
where El, F2, H1 , H 21 icm. 1 and J CM2 are tile clectric and
magnetic fields and the currents, respectively. Ex-,ression (14)
is also a differential formula of the 'Icnown
principle. ini.2gration of the equation (1'~) over a voluil-10 V
limited by a surface S , expresses the reciprocity irinciple in
an integral form as given by equation (1'/). The combination of
the lemmata expressed by equations (9) and (10) for the case of
equal tensorial parameters, frequencies, fields and currents
leads to:
c iW 0 (24N
- div(I x H*) + -~--(H - 4H - B i*E4) + JCM
4r 4Tr
Uard 2/4where the asterisk refers to conjugate quantities. Equation (0-4)

Quacb.,atic Relationships for tile Media with Terujorial.
is a generalization of the Umov-Poynting theorem fo~~
represented by tensorial parameters. Tho basic, quadratic
lemmata can also be employed in the derivation u2 the perhi-H)ail~ L(:_!1i
formulae. It is assumed that an e le ctro-mar---ne tic phenomenon
which is represented by the indices 2 in -the expressions for
the lemmata corresponds to an unperturbed conditicii of the systein,
while a perturbed state is denoted by indices 1 ' The most
important practical case is when the system in its initial st,)te
is represented by scalar and real parameters and the ext(--:rnal
currents are absent. Formulae (6) and (9) lEad then to
equations (28) and (29), which can be regarded as the basir!
perturbation lemmata. These are applied to three fundamental
boundary problems of the electro-dynamics of hollow systems:
1) determination of the propagation constant of a regular wave-
~uidei 2) calculation of the transmission and reflection coeff.-_*,~-
ients at the discontinuities in a wave-guide and 3) the ~ieter-
mination of the natural frequencies of a cavity resonator. In ail
cases, it is assumed that the metallic surfaces licaitinG the
above hollow systems are ideal conductors. The author expresses
his gratitude to the Correspondin~j Member of the Soviet Academy
card3/4 of Sciences A.A. Pistolkars for the discussion on tile results

1.09-8-3/1'/
Auadratic Relationships for the Media with Tensorial Parameters.
of this work.
I There are 16 references, of which 9 are Slavic, and 3 fiCures.
SUBMITTED: December 6, 1956.
AVAILABLB: Library of Congress
Card 4/4

Q-,
V
pwx I Doot unoignum SM/1503
Akadeodya u&uW_33aR._ Inatitut palu-proybduLkov/
PoluproTodnikl v nauke I takhmike, t. 2. (ammiconduatore In Science
Md Tsol*mology, Vol 2) Rosoov, lad-vo AN 33M, 1958. 658 p.
17,000 copies printed.
loop. Zd.s A.F. Ioffe; ?*ch. Id.1 R.S. Pev=or.
PURPOR& This collection of articles is Intended for scientists, en-
gineers and technicians.
COYNDUals The collection, published by the 3432100nductor Institute.
Acada:ay of Sciences, MR, under the supervision of Acade-Ician
A.P. loffe, contains Parts II and III of a two-Volum* work on semi-
sonduators. Part Il completes the material an semiconductor devices.
bogun lit Volume 1. and Part III demarlbes various owalaonductor wa-
torlals. Lack of space did not permit Inclusion of such vubjocte
as crystal counters, thermoelectric generators, atomic batteries,
lunduophores, amicanductor catalyzers. materials for accaplex cathodes
and various other applloations of semiconductor*. laffe points out
AzerLO&n. scientists V. Johnson and E. Lark-
RorcvItx an semiconductors at low touperatu"s deals with a subject
hardly covered In the Soviet literature. Slallarlys the article by
the Swiss scientists 0. Busch and U. Winkler fill@ a gap In the
Soviet literature on methods of Investigating staicanductor charac-
t*rlatloa. Th*so subjects will be dealt with exclusively In a pro-
posed third volvate. References appear separately after
TAWJ OF COMMUs
Ch. 20. Soolonakly, a.&., and A.G. &Aravloh. forrOM44patin
Seala*oduotors - 349
ft* author discuss the application of fsrrO&&&n~tIG sealaondu4_
Ure In multichannel telephony, radar, else troscous ti as, also-
troule counters, cores or induction coils, transformers and MI.
term, permanent sagnets, nagnOtOstrIction transducers, Memory
almost@# @to. They explain the crystallography of forrItes and
the theoretical fundamentals Of boaccopenosted antirarromagootlam.
Card 619
1hey also discuss problems of --90*tlG saturation In fem*It6s and
their bahavlour In &-a aLCnetiq fields and at very h1gh rrequanolos.
Special chapters cover such subj"to as slootMMAgnotia oacIll-tions
is ferrite@ and nonlinear Processes Occurring at very h1Z:' rr*,Zugc-
also. The concluding aAaptora deal with the electric PrOP*rtI*8 Of
forritev and with ferrite watorials and their. selection. There are
53 reforamoss, of which 33 art Ingl1ah and 20 Sovist.
Ch. 21. Q-A-, =4 V.A. Iou~pov. SaIgnetoeleCtrIO
Materials 425
Mis authors expl#An the alffor*nass and Similarities bstw**n
-galgeatoolootrIo. piezoelectric and forroassnatic materials. They
present a historical survey of saignotooleatrialty and provId4 data
tables of asignotoolectrIC Mukt~riLls- Ths au=Ors explain th* fUn-
daxsntals of the microscopic theories an seignetoolt0tric Ph*ccadn&
and discuss In detail the cryStal lattlOs structure, physical pro-
pertios and problems of producing various seignatO1100tric materials.
-They briefly 449arlbs antloalanstladlectrIC mAtar,210 and draw att*n-
tloa to recently adopted applications or the** mini-
&turt capacitors. nonlinear capacitors, PlOzO9100-ats and memory
alestato. There ars 35 references, of vh1ah 210 are SOV18t. 23 JM&Ush
card 7/9

;~OV/1J )-5-1-3/20
AUTHORS:Gurevich, k. G. and Boo-omaz, 14. A.
TITLE: Non-Reciprocal Phase Shifts and the AUtenuation Coefficient
lor a Waveguide vjith a Ferrite Plate (1,v'evzaimrTje fazovyye
sdvip,i i Icoeffitsiyent zatuldianiya v vol-novode s forribovoy
, k
l" Siinoy)
p
PERIODICAL: Radio bek.-inika i elektroni-ka, 19158, Vol 3, Nr 9,
(USOM)
ABSTIUCT: The calculated results of an accurate comoutation of the
Dhase constant and the attenuation coefficient for a ree-
uangular wa-veguide with a transversely magnetized ferrite
plate are re.ported. The calculations were made by means of
a fast electronic computer. The calculation of the propa-
gation constant y in the waveguide (see Fig.!) was done
on the basis of Ea.(l), where k 0 is the viave no-mber in
free space, s is the pom.,iittivity of the ~plaze and 1-1
-and a are the complex components of ti-Le a ic permitti-
vity tensor whilst _h a t are the d0imensions
nd (see
Fig.1). The i--er-mittivity tensor is defined by the determin-
arit on 1) 1134. The non-reciprocal difference of phase sii-iftus,
i1 wos calculabod without ~akiii,7 inU~) ail-count ~hc attenua-
Cj
Card 1/4 tion. The differonce 71 is defined 'by:

llon-Re,~,, i- _L U
procal Phase Shifts and the Atte-nuation Coefficaent -or a
Wave.-uide with a Ferrite Plate
TI = Y~ - Y, (2)
where y.,. and y_ are the propaSation constants for tiro
nronaqati -~n directi.-)-ns r)f' "ne waves or for two directions of
U
the magnetization cf the plate . The dependerice -if n on the
,uaveiength X is illustrated in Fi!--.2 for vari-.)as values
U
of The bandwidth of the waveEztide-ferrite system can
CD
be charact_-,rised by a frequency coefficient defined by:
OL 0 -A%) - q(% & + X0
(7,0) 2A%
%~,,hare 4% is a certain fixed q antity; in th-Js case it was
u
assumod t-dat AkAo = 5%, . The dependence of -.1 and K on
r" fDr various values of h and E are shovm in Figs.3, 4,
Card 12.-/~-

)n-Reci-procal Phase Shifts and t-',%e Au"ternia'l-ior C,efficie-nt for a
I
N
Vlave-aide aith a Ferrite Plate
5 and 6. Since the atUonuation cocfficient in -the ferrite
was c,)!,v,1arativeI,,/ small, t 110 4 rq, '
.L part of the propagat-
i.-.)n cons'Ga~Lkl,- could be determined froM the approximation formula:
Y11 = 3-(1 E; It + a Y By, (Y11 (4)
OE;' I~L aa,
TLI).(, c ale t--.1a results Givine, tho, valucs of Vie derivatives
of Eq.(4) for tuiie two directions, of pro-pa-'atigia, as a funct-
L)
ion of !~- and h are sho=_ in Pigs.7, 8 and 9. The atten-
uat-~_ill Co--.LCfieio,1t, as a function of is illustrated in
Fi,;-. 10. In the ref.~,,ion of ferroiaai_~netic resona.,.Ice the phase
constant y' and the attenuation coeff'i-cient
U - j" can be
deter.-Iiined by findias the cora-.-.lex roots of E 1) for com-
-ie parant~,`ers ~L and a
,ley- values of Ii mid a TI Ij .
w,-.re eWUIU~Aed and (9) respectively; for the
"UI-.-Ode Of IG VMI3 L~L;,iU U'lie ma,rno Liza t -
-,,)n curve for bl-Le ferrite plate woj ia Lh,':- s*io~ln_i in
Fis.11. The calcuiau-A.Dns, wz~!rc d-)nc for a frequency of
w/211f = 9-:5?5 TI'lie phase- a _J a-LenuaUji-)n
-D CL G as a function
Cal-d 3/4. of U~ie -,!la~netizing, field H 0 for vari..)us values of the

lk)--Rcciprocul -1-Iiiase A)IIi-L'b-S ~Itld t'ILf-! for o.
Lv---u.- wi t1i a Ferri Pla -e
'do U
U
loss 6 :-,,re sIIJW'fI -'S . 12 ";irl-ilC~" GUrVCS
--iven in and 14 !Dutu- biwisz) the pliase wid Ule
j
aGUenuation for wrious VCLlUeS Of w-id IL The quality
factor of the wave-mide-ferrite non-X-eciprocal phase-
Q -
shifter can be defined by: 4-
Y(., p
An e YH
re-oresents
c D
ted values of Q as a
or vari)us values of
and 15 rcf,,~rcnccs, of
SUBI',iITT,ED: Septe!.-iber 20, 1957.
the avera,,-e attenuation. Tille calcula-
C )
function of are s~ix;n in Fil-;..15
h Die oonta-..ns 15 fi-Gures,
,111lich 8 =.e and 5 arc Govict.
Card Lj-/LV

AUTHOR: Gurevi SOV/109-3-12-6/13
TITLE: Resonators with Tensorial Media (Rezonatory s tenzornoy
sredoy)
PERIODICAL: Radiotekhnika i Blektronika, 19158, Vol 3, Wr 12,
pp 14?1-1484 (USSR)
ABSTRACT: The work deals with the problems of the general theory
of cavity resonators filled with tensorial media. The
method of analysis is based on the application of the
eigen functions of a cavity resonator which was proposed
by Frankell (Ref 7) and used by Kisunlko for ieveloping'
a resonator theory for the case of scalar media (Ref 8).
The principal concepts of this theory are here generalised
and extended to the case of media with tensorial parameters
First, a closed volume, V , limited by a3i ideally
conducting surface S and filledKith a medium. whose
tensorial parameters are V' and 4 is considered.
The parameters V and V are arbitrary functions of the
co-ordinates (Figure 1). For the case of free undamped
oscillations in the resonator, the complex field amplitudes
for the m-th type of oscillation 0hould fulfil the
uardl/5 Maxwell equations:

Resonators with Tensorial Media SOV/109-3-12-6/13
rot H iwMCZ
+-114
rot iW '9H
m
and the boundary conditions given by Eq (2), where no
is a unit vector normal to the surface 8 . The field
vectors can be represented by Bqs (3), where e and h
are complex amplitudes which are related by Bq (4). Fro
the above, it follows that the eigen vectors and F
im m
of the resonator should satisfy Eqs (7) and (8), where '
WM is the eigen frequency'of the resonator. This can be
expressed as a ratio of two volume integrals, as is shown
in Eq (9). The orthoganality condition for the electrical
eigen functions of the reso-hator is given by Eq (13),
while that of the magnetic eigen functions should satisfy
go (14). If the medium is not lossless, the tensors
7- and V are not Hermitian functions and the eigen
(;ard2/5 frequencies of the resonator are complex and can be

Resonators with Tensorial Media SOVi09-3-i2-6/13
expressed by:
W~ + iW11 Wt + i
n n n ~n)
where nI/2w" is the quality factor of the resonator
Qn = W n
for the n-th eigen oscillation. In the case of forced
oscillations-in the resonator, the Maxwell equations are
w3itten as Eqs (18) to (21) and these should fulfil the
boundary conditions given by Eqs (22) and (~3) (Figure 2).
The field of forced oscillations of the system is in the
form of series expressed by Eqs (24) and (25), where
I
Em and -9m are eigen functions of-,the resonator, as
derived in the earlier formulae, while the coefficients
em and hm and the functions ~o and q) a-re to be
determined. It is shown that ~o can be determined from
Eq(26) and (P from Eq (29). On the other hand,
Uard3/5 coefficients em and hm are expressed by Eqs (39) and

Resonators with Tensorial Media 6OV/109-3-12-b*/i3
(40), where F m and I m are given by EqB (3?) and (38).
If the losses in the medium are comparatively small,
they can be taken into account by substituting the
frequencies in Bqs (39) and (40) by the complex frequencies
of Eq (l?). In this case, the coefficients e m and hm
are expressed by Eqs (41) and (42). From the above, it is
seen that the field of forced oscillations in a resonator
with a tensorial medium can be determined, provided the
eigen frequencies and eigen functions of the resonator are
known. In a waveguide resonator with a scalar medium,
the eigen frequencies are given by expression (43) where
I is the length of the resonator, n is an integer and
Y(w) is the propagation constant of the waveguide which
can be regarded as a known function. In the case of a
tensorial medium with non-reciprocal propagation constants,
the eigen frequencies of the resonators (which are
similar to those shown in Figure 3) can be determined from
Eq (46), where y and y- denote the propagation
constants for two opposite directions.
Gard4/5

Resonators with Tensorial Media SOV/iG9-3-12-6/13
The author expresses his gratitude to A.A. Pistol'kors,
Corresponding Member of the Ac.Sc.USSR and N.A. Kuzlmin
for their valuable Observations -fa discussirW this Work.
There are 4 figures and il references, 6 of which are
Soviet and 5 English.
SUBMITTED: February 21, 1957
card 5/5

GUREVICH, A.G.
UsItc structures with honeycomb fillers. Biia.tekh.-ekon.
inform. no.1:93-96 059. (MIM 12:2)
(structural frames)

GUMICH,,,A.G., GUBLER, I. Ye.
Ferromagnetic resonance in yttrium ferrite single crystals. Piz.
tver.tela 1 no.12:1847-1850 D '59. (MIRA 13:5)
1. Institut poluprovodnikov AN SSSR, Leningrad.
(Yttrium ferrate-Magnstic properties)

GUREVICH, A.G.; GUBLER, I. Ye.; SAFANTIYEVSKIY, A,P,
Superhigh-frequency properties of yttrium and luetetium forrites
with structures of the garnet type. Fiz.tver.tela 1 no.12:
in62-1865 D 159. (MDU 13:5)
1. Institut poluprovodnikov AN SSSR, Leningrad.
(Yttrium ferrate) (Lutetium ferrate)

-24W
AUTHOR: Gurevich, A. G. SOV/48-23-3-16/34
S r
TITLE: Ferromagnetic Semiconductors in High-frequency Fields (Ferro-
magnitnyye poluprovodniki v polyakh sverkhNysokikh chastot)
PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheskaya, 1959,
Vol 23, Nr 3, PP 361-371 (USSR)
ABSTRACT: The work under review deals with magnetized materials which
are used in practice. To begin with, the properties of ferro-
magnetic semiconductors were investigated in small alternating
fields in the range of superhigh frequencies. Tensor character
and ferromagnetic resonance of the semiconductor are the mostv
important characteristic features of the magnetic susceptibil-
ity T. Figure 1 shows the components of the tensor of magnetic
susceptibility of a polycrystalline ferroma~,-netic semiconductor.
Within the range of superhigh frequencies P. nct compensate,_~
antiferromagnetic behaves, like a feTromaSretic 1-he magnetiza-
tion of which is equal to the sum of magnetization of the
sub-lattices, and which has a factor of spe,;trascopJ_c split-
ting up g eff* Figure 2 shows the procession of magnetization
Card 1/4 in the non-compensated antiferromad-netic. In connection with

Super
Perromagnetic Semiconductors in/-High-frequency Fields SOV/48-23-3-16/34
the consideration of the waves of =6-netization it is neces-
cary to take into account the so-called spin waves (Ref 10).
A spectrum of the spin waves in the unlimited medium is
given in figure 3. Under certain conditions they are connected
with homogeneous oscillations and exercise a considerabls~
influence upon the processes takinC place in ferromagnetic
semiconductors within the nuperhigh frequency range. An
explanation for the observed course of temperature and the
duration of relaxation r is given by the theory (Ref 20)
which brings the relaxation processes with spin waves and
magnetic heterogeneity into connection, especially with the
non-ordered distribution of the ma6-netic ions in lattice
point. It was found that Ir as well as the g-factor can be
exactly measured only on monocrystals. The effect of the
domain structure is also of outstanding importance. The
results found for unlimited media may also be applied to
bodies with limited dimensions if the tensor T does not hold
for the external but the internal alternating field. Un.-
fortunately, it is only possible to solve a very low nlimber
of boundary problems. Of the approximation methods, on-I.,-, '7~m of
Card 2/4 the coarsest (least accurate) are used at the present- time.

Super
Ferromagnetic Semiconductors infiffigh-frequency Fields SOV/48-23-3-16/34
the method of"infinite space" (Refs 49P50) and the perturba-
tion method with a quasi-Btatic approximation of the internal
field (Refs 51,52). Apart from theory, also apparatus were
developed during the past 6 years in the case of which it is
possible to make use of the properties of ferromagnetic
semiconductors for the solution of practical tasks of super-
high frequency. The principle of such apparatus is funda-
mentally clear (Refs 56,57). The main problem is now the
supply with auitable materials and the necessary parameters.
In the short;..wave range of superhigh frequencies it is
relatively easy to fulfill the requirements. Considezable
difficulties arise, however, in the case of lloner -,vave:,.
In the case of low frequencies the ranges of natural roso-
nance and the resonance in the external field ovt~rlap 0,'ii; 4).
This-is the reason why semiconductors with small an.1z:ot-ropy
and saturation magnetization were developed for the l3n-S-,7e_7e
range. The combination of a small saturation magnetization
and a sufficiently high Curie point is the E-5reate-.1.diffic--aty
in this connection. Spin waves play a considerable role i~l
the theory of non-linear losses. They pass the energy
Card 3/4 produced from homogeneous oscillations to the lattice, which

S~Iper
Ferromagnetic Semiconductors in/AL'Ligh-frequency Fields SOV/48-2~7-53-1 6./":"4
causes an increase in losses. This phenomenon o':)viously
occurs in all ferromagnetic semiconductors. Only the values
of the threshold field vary. The non-linear comDination of
homogeneous oscillations and spin waves does not on-'.y exnlain
the higher losses, but may also be used in non-14-1--ear fer.1-1.
magnetic generators and amplifiers of superhiL,,h frequen~_;t:;.
There are 7 figures and 76 references, 23 of which are Soviet.
Card 4/4

PHASE I BOOK EXPLOITATION SOV/4433
Gurevich, Aleksandr Grigorlyevich
Ferrity na sverkhvysokikh chastotakh 11-rrites at Saper-High Frequencies)
Moscow, Fizmatgiz. 1960. 407 p. (SevAst -F1Mk*-p*1nprovodnikov i
poluprovodnikovykh priborov). Errata slip inserted. 10,000 copies printed.
Ed.- Ye.L. Starokadomskaya: Tech. Ed.: V. N. Kryuchkova.
PURPOSE: This book is intended for technical personnel and scientists working in
the fields of radio physics, radio engineering, physics of solid bodies and
the technology of magnetic materials. Its purpose is to convey a general
understanding of the subject, rather than to be a review, or serve as a handbook.
CO'VERAGE: This book is an attempt to generalize theoretical and experimental data
gathered during the processing and utilization of ferrites in the super-
high frequency range. Part I of the book exwnines the magnetic properties of
ferrites in the weak fields at the super-high frequency range. Part II deals
with the electrod-ynamics of media with tensor parameters to which belong magne-
tized ferromagnetic semiconductors, Part III is concerned with the nonlinear
C&=1_V_6_

Ferrites at Super-High Frequencie-
SOV/4433
processes occurring in ferromagnetic semiconductors at high amplitudes of
the -variable magnetic field. The coverage is limited to a small number of
ahs,racter'st4c phenomena, which are exposed In detailwith the rala;ting of
Intermediate computations being given in most cam-n. The author thanks;
G, A. Smolenskiy, Doctor of Physical and Mathematical Sciences, V. V.-RIC611-
skly,, Candidate of 11behni-il Sciences and A. I. Pil'shchikov, Candidate of
Physical and ILathematlcal Sciences for their valuable advice. There are
1169 references: 326 English, 123 Soviet., 10 German and 10 French.
TABLE OF CONTENTS:
Preface
PART I. MAGNETIC PROPERTIES OF FERRITES IN WEAK
SUPER-HIGH FREqUENCY FIELDS
6
Ch. I. Isotropic Ferrites Magnetized to Saturation 13
1. Susceptibility tensor. Pbrromagnetic resonance 13
2. Ferromagnetic rescnance in. unbaaaaced antiferromagnetics 26
3. Spinning wavei3 36

NIKOLISKIY, Y.Y.; GMVICH. A.G., kand.tekhn.nauk, retsenzent; KMIK.
A.R., red-
[Theory of the electromagnetic field; manual for students of
radio engineering) Teoriia elaktromagnitnogo polia; uchobnoe
posobie dlia studentov radiotekhnicheskogo fakulltets. Moskva,
Goe.energ.izd-vo. 1960. 43o p. (mi-RA 14:1)
(Radio-Hondbooks, manuals, etc.)
(Electromagnetic theory)

GURSVICH, Aleksandr Grigorlyevich; STAROKADOMSKAYA, YO.L.; KRYUCEIKOVA,
V.N., takhn.red.
(Yerrites at microwave frequencies) Verrity na sverkhvyaokikh
chastotakh. Moskva. Gos.izd-vo fiziko-matem.lit-ry. 1960.
407 P. (MIRA 13:7)
(Ferrates) (Microwaves)

GT,/* Pm
gvgT PJV3
95
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L95 -W ;UV
-AQvr*q :d
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:
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4vA-u9v=- ui suatqojd '.C%j-raTn?uvp*j wwvuw%uodo 3uj-4jqjq"
sm-2mcs, 027;4jal 2u&uodmczT3-,= ;,uv tdool sisajo-42AU Jvjngut,3~oj
"U.; TU co-21.1.20i j0 goTpn-Is 'goalijej ja clacTrul IVOTC04"o
-.sZVd put lwz-..2142 014,4 uT cz.-,qwd Islarlatio rEguls onTijej jo
tj%~042 Mn JO DDIPWAS JO 90;2416d"d l'C26UffVWUVAtlll
put ivot.:,4Daza 'cuoiiv=ojsuv-:2 nistl2ta tni;iq -tvap g-Ajodoj stu
'W6-5 utzra-woraq I)ICUTW al Dreg V*21.wag urc aouoa juco uaTuA
-Ity pjlvZ vql 3v P6,4uasaid azzodba guTv2uoi 7,ooq Z jZDVVWo
lw~IsAtvs Put 1421LAId
'20;u*J2~OTO 0TP9J u1 909--ncz PODUVAPV ul aluapn2s Aq Dean eq
jo min put uo;2*npwd sq%
;,jw 'Ra-suOus soluoijoato CTPWJ
a oviod jmzTtmz~.
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pug -j~.uaJVLIoMG 'w *r, !92~uf)los Put TVOTB446
j0 alvp,;puv3 q,4.1cqs -g -K 'Zoovejoij "CTAIrualows 'y 'D .1jossaj
'A *V -..IoatojoQ !A6u'l&-;TQj 'm -3 :-logrojoia 'Alms
"laloal 'Aclog -a 31 !V= caouslog jo 4MOPUDY
Puo)l r
-a4 !jo& --p2 -dtaH :P.Ivoa jvjJo2jPl
jo u,"PIZI-prov
.1issu NY Ao)-,-.~DoAojdnjod ; VT&j 02OP-19A2 TATZTJ
mzjjau?v= od -4a-AOI "ujj"Tg -.Colou*Sy gulloguod
lop,40
poluTid cvgdoo 000"A
-po-Aaavu-, djTg uzujjz 'd '1=9 NY c"P21 ')I%uTW
(4%-ijod,7)J -tal2JOdO-2d put ITOTIatza Iso.4lmaj)
prljoC -vtorgoAo T qATmgs,401zT;
656T, 'Mvuiw
~VAICICOAV "T"-IJ od Q4jUVL40tjV0A0 'CouWOCREA
E69t,/Aos 7009 1 EM.1

-:bI T.,
GUMICH. A.G. [translator]; NAMIMSON, I.G., red. ; POIZAPM)KOVA,
Te.S., te-REn. red.
(Perrites in nonlinear microwave devices; collected irticles.
Translated from the Buglish] Yerrity v nelineinykh everkh-
vysokochastotnykh uatroietvakh; abornik stntei. Moskva. Izd-
vo inostr. lIt-ry, 1961. 6~4 p. (Kin 14:5)
(Yerrates) (Microwaves)

AUTFORSi Gurevioh, A. G., Gubler,
TITLEz Temperature dp-ei-Maence of
and relaxatior. processes
PERIODICALt Fizika tverdogo tela, V.
89271
S/181/61/00,'/001/003/042
B102/B212
I. Ye,, and Titova, A. G.
the width of the resonance curve,
in ferrite single crystals
3, no- 1, 1961, 19-31
TEM One of the most suited methods for studying relaxation processes
in ferromagnetic materials is based on the analysis of the temperature
dependence of the width (24H) of ferromagnetic resonance absorption curves
in ferrite single crystals. This paper reports on such measurements.
Spherical yttrium-ferrite single crystals with a garnet structure, and
manganese and magnesium-manganese ferrites with a spinel structure served
as specimens; the measurements were made in the range from -1960C to the
Curie point of these ferrites. The growing of the single crystals is
described briefly. A standard method has been used to determine 2AH at
9100 Me. Altogether 6 specimens have been investigated, and their charac-
teristics are given in a table. Fig. 2 shows 26H as a function of.
temperature for these 6 specimensi Fig. 3 shows Al' (T) for specimen no. 1
res
Card 1/7

89271
9/181/61/003/001/003/042
Temperature dependence of the ... B102/B212
(All denotes the imaginary part of the diagonal component of the lloxtornalll
res
susceptibility tensor at the point of ferromagnetic resonance). 2AH is
determined in ferrite single crystals by the following processes: Inter-
action of homogemous precession with spin waves; relaxation processes, in
which magnetic impUrity ions with a stron frequency 5spirlattice relaxa-
tion take part; excitation of spin waves fwith k,-10 -10 cm-1) as a result
of scattering of a homogeneous precession from microscopic magnetic fluctua-
tions which are caused by a random distribution of magnetic ions among the
lattice sites; a widening of the resonance curve, caused by the roughness
of the specimen's surfacel and incoherent relaxation processes due to
thermal fluctuations of the magnetic moment. The latter effect entails a
rapid increase of 2&H when approaching the Curie point. When analyzing
the 24H - f(T) curves, it is assumed that n processes that influence 2AH
are additivet 2,&H A detailed discussion is then given of the
n n
effect of the roughness of the specimen; of fluctuations near the Curie
point; of rare-earth impurities; and of impurities and magnetic disorder
in spinels. The results of the investigation lead to following con-
clusionss 1) The component of 2AH, due to the roughness of the specimen,
Card 2/7

89271
S1181 61/003/001/003/042
Temperature dependence of the ... B102 B212
is approximately proportional to the magnetization; the factor of propor-
tionality is not a function of the ferrite composition. 2) The relpation
frequency of rare-earth impurity ions in Y-ferrite grows from 2 .10 to
6-1013 when heating the specimen from -1960 to +200OC; at room temperature
it has a value of 3-1013- 3) The relaxation mechanism characteristic of
spinel-type ferrites leads to a 2AH component of several oersteds caused by
a spin-wave excitation; therefore it is possible to measure resonance curve
widths of less than 10 oersteds in single crystals of such ferrites. 4)
The 24H component caused_by, thermal fluctuations of magnetization increases
in proportion to (T.- T) 172 when approaching the Curie point. 5) Due to
the fact that the latter component grows with increasing temperature, while
the components caused by impurity ions and by the roughness of' the specimen VK
decrease, all 2AH . f(T) curves have a minimum above room temperature.
Position and distinctness of this minimum is a function of the values and
temperature dependence of these components. Increasing roughness, e.g.,
brings about a shift of this minimum to higher temperatures. The authors
thank Professor P. A. Smolenskiy for discussions; F. M. Samigullin
participated in measurements. N. N. Parfenova and Ya. I. Shtreys ~)f NII
Card '4/7

S11 81/61/003/001/003/04 2
Temperature dependence of the ... B102/B212
tokov vyabkoy chastoty im. V. Vologdina (Scientific Resenrch Institute of
High-frequency Currents imeni V. Vologdin), and E. Ye. TL-lezhkina and
M. A. Zaytseva of VNII abrazivov i shlifovaniya (All-Union Scientific
Research Institute of Abrasives and Grinding) are mentioned. There are
8 figures, 1 table, and 19 references; 7 Soviet-bloc and 12 non-Soviet-
bloc.
ASSOCIATION: Institut poluprovodnikov AN SSSR Leningrad (Institute of
Semiconductors, AS USSR, Leningrad)
SUBMITTED: June 17, 1960
Card 4/7

89271
61/003/001/003/042
B102 212
dependence XB
Temperature
Ix
of
/01
x
4
----------- 280
110 goo
-40 40
Card 5/7
Fit)

W It"'. T,
- ~~Jj- " I , w 1, .~ R
gum=
S/1 81 /61/003/001/00 3/042
B102/B212
Temperature d.ependence of the...
Legend to Table: 1) Number of*speci' men; 2) composition;.3) diameter (mm);
4).grain bize (R) of abrasives, with which -the specimens were finally
polished; 5.) magneViza-tion (.o*auss) at 200C and H- 3250 oe; 6 Curie pointy-
(00, 7) 24h.-(oer"steds) at .-1960C, 200C, and minimum value; 6~ minimum
temperature.
WNP k 00
'6
XPUBOO, DPGT~
COME
U
04
x W 0 oil
XX
I
1 0.47 1-3 Iso
2 290 14 2.2 1.6 170
Y3Fesolt 0.55 60
3 1 290 26 10 6 240
0.49 1_~ - - 165 8.5 3-9 230
:4
5 Mnj.o3FejxO4 0-60 1-3 320 SOO 101 16' 12 150
0.58 60
148 41 26 260
6 M9oz2sMnom3FejsjOd 0.76 1-3 23o 333 46 9.5 &S
A 100
Card 7/7..

25686
B/181/61/003/007/008/023
B102/B202
AUTHORSt Gureviohp A. G. and Starobineta, S. S.
TITLEs Instability thresholds in the case of farromairnetic reso-
nance in yttrium garnet single crystals
PERIODICArLs Fizika tverdogo tela, V. 3, no. 7, 1961, 1995 - 1998
TEXT: The authors present the results of a study of ferromagnetic
resonance in yttrium garnet single crystals with different content of
rare-earth admixtures and different surface treatment. It has been found
before by experiments (and also theoretically) that the rebonance
susceptibility X r1les decreases with increasing amplitude (h)'of the
variable magnetic field. The studies were made only for small values
It (h) in a large h range in different
of h. The authors studied z res
yttrium ferrites. The measurements were made at 9370 Me/sell, (in pulsed
operation, the reciprocal of the pulse duty factor was 4000) in spherical
specimens (diameter,.,,0.5 mm). The three specimens studied had the
following characteristicas
Card 1/4

Instability thresholds
No
purity of the
initial yttrium
oxide
grain size of
the abrasive
25686
3/181/61/003/007/008/023
B102/B202
24 H for
h-*O,
oerst.
2,61~ 241,11",
k
oerst. oc--rst.
m
max)
gauss
1 1 99-995 3 2:3 20 =1.2 18
2 99-995 10 4 7 24 - 17
3 99-95 3 7.6 49 9.8 1 24
The best curves of measurement are obtained if Iles
Ir h 2 is plotted as a
function of h. This is shown in Fig. 1 where the diagram b shows the
first part of a) on an enlarged scale. In all curves a series of linear
parts follows the first part (with ~ " - cons t) t -'i " h2 - mlimh + pp
res 4, res
where m li, and p are constant quantities for each part. m lim is the
11
limiting value of the variable magnetization-k res h (for a given part)
at h4oo, p characterizes the velocity of the approach of it h to m
res lim
with an increase in h. It is assumed that m lim is the critical amplitude
Card 2/4

25686 3/18-1/61/003/007/()08/023
Instability thresholds ... B102/B202
of magnetization of the homogeneous precession for the first linear part
for which M M pltm k holds theoretically. M is the constant
or 0 0
0
magnetization, 26H k the width of the resonance curve of ~the spin waves
which become unstable; (these calculated valu,6s -are also-given in the
table as 248H ') Assuming the magnetization at the &beginning of the first
k
linear, part,as magnetization threshold, a,value-which is given in the
table under.2AH" is obtained for 2AH These vaaues can be divided into
k k" ' ..
an intrinsic plus an impurity part (the spe'cime~s'l and 3 differ in their
impurity con'tent by one order of magnitude)-; the following values were
obtainedt
No 1. No 3
2 H" 17 + 3 17 + 32 oe
. k
2 H" 4.7 0.5 4.7 + 5-1 oe
k
All curves showed three linear parts. With increasing concentration of
the rare-earth impurities the slope of the first two parts considerably
Card 3/4

25686 3/181/61/003/007/008/023
Instability thresholds ... B102/B202
increased. The slope of the last one was the same for almost all
specimens. -For-specimens which differed only by their surface treatment
it was eaual. Hence, the limiting'amplitude of the homogeneous
precession depends neither on the rar-e-earth concentration nor on the
roughness of the surface at sufficiently high alternating field strengths.
The maximum values of the amplitudes of the homogeneous precession m max
are also given in the table. Ya.Loos is'%mentioned. There are 2 figures,
I table and 6 referencest 1 Soviet-blo6 and 5 non-Soviet-bloc.
ASSOCIATIONt Institut poluprovodnikov AN SSSR Leningrad (Institute of
Semiconductors AS'USSR _14eningrad)
SUBMITTED: November 25, 1960 (initiallyl February 4, 1961 (after
revision)
Card 4/4

j C)
7, 1 S/04r3/6i//O25/O-,1/Q
2 L) ti B108/B158
i~7S Gurevich, A~ G, and Starobinets, S. S,
TITLE~ Ferromagnetic resonance in ferrites in strong variabl-a
magnetic fields
PERIODICAL; Akademiya nauk SSSR. Izvestiya,, Seriya fizicbeskayaj v.
no, 11, 1961, 1357-1360
TEXT: In order to study ferromagnetic resonance at hd,-h power
authors measured Xf'
res' 2&H, and H res of single yttrium garnets The
measurezuents were made at a frequency of 9375 MCPS with a pulse gi~ntra-~r.
The specimens in the shape of spheres () 5 mm diameter ivere piaced ~n ih~~
magnetic field antinode of a TE -mode rectangular cav-,t:t 7" i ~ h a
106
v all the measurem,.-,nts
ur~cision attenuator at the input end of the cavit,
could b- maJe at constant power output, III was determined from the PU*-'J'_r
absorbed in the sample as shown by the attenuator, The method of
measurement has been described in Ref, t (Fizika Tverdogo tela, 71
1995 (1961)) by the authors as well as in Refs. 2 and 3 (Spe below, 'r h
Card 1/3

3006'
S/048~61/025/011/010/031
Ferromagnetic resonance in ferrites in-, B106/BI38
advantages are that the magnetic field amplitude is the same at any point
on the resonance curve, and that the results do not depend or, the crystal
dqtector characteristics, The results nhow that, bo%h at roc-m and
nitrogen temperatures, the power absorbed Is, after a short initial.
section, linearly dependent on h,, The rise in the resonance losses
observed with decreasing temperature is attributed to the effect of rare-
earth impurities which favor resonance absorption, The anisotropy of
the resonance losses increases considerably with field ampli-,udce Th.:,
resonance field H res is connected with the angle 9 bet*e~,-n [ooij axis and
(110) plane through the relation H - ~) .lKil f(G) (I), W'Iere
res 7 M
f (0) cos2Q oosO . The intersec tion c f the sL.raight line
16 4 76
with the ordinate axi3 yields the g-factor.. At room temperature, this
g-factor increases with rising power level., At 77oK, the pg-faotor is
independent of power level down to field strengths of about 3 oersted.
The cbserved decrease of the product J" -2AII hirb ris:Lng f;~~Ild amplitudv
.res
indicateR reduction of permanent magnetLzation as it recult ef incroa'Al .n
lard

S/04)8/61/025/011 '010/0xi
Ferromagnetic resonance in ferrites in.., B108/'B13'8
spip wave amplitudes. This paper was read at the Conferenc,:- o-.1
lerromag-netism and antiferromagnetism in Leningrad, May 5-11, 1161.,
I - 90
There are 5 figures and 7 references: I Soviet and 6 nen-Savie-,- The
t'ho most recent references to English-language publications read as
Weiss M. T , J. Appl, Phys-, 31, N 5, 778 (196c); Green J J
SchlOmann E, IRE Trans. Microwave Theory and Techn., 8, N ?, (1~960).
Card 5/3

30066
S/048/61/025'/011/011/031
'2 Ll -'1 5 C) 0 (10. Yl/,3 B100102
AUTHORS: Gu~i- Saffintlyevskiy, A. P.. Soloviyev, V I
and Sher, Ye. S.
TITLE,: Effect of induced anisotropy upon ferromagnotic ro:ionttriesz
PERIODICAL: Akademiya nauk SSSR. Izvestiya., Seriya fizi..,hL~~skaya, v- 25,
no. 11, 1961, 1361 - 1367
TITLE: The authors studied the effect of electron-induced anisotropy of 0
polycrystalline yttrium garnets upon ferromagnetic resonance from 4.2-300 K.
The measuring technique used in the temperature range of 77 - 3000K had
been described in aprevious paper (A,. G, Gurevich et al,, Fizika tverdw~o
tela.. ~, no~ 1, 19 (1961). A square rooonator was dipped into liquid
helium. with the specimen between 4.2 and 770K.. With waves the
resonance rield H res and the width M~H of the resonanct curve were deterndied
from the dependence of the reflection fnctor IV) on the magnetic field, as
recorded by an z3flfl-09(EPP-09) voltmeter, An example is illustrated in Fig.l..
Manganese-free specimens annealed at high temperatures showed a rapid in-
crease of 2AH with decreasing temperature, For an initial yttrium oxide
Card 1/'O~

30066
5/048/61/025/011/011 1.1/0~s
Effect of induced anisotropy.- B104/B102
with a purity of 99-995~c, the said rise cannot be attributed to rare-earth
impurites. Present results show that the induced anisotropy of polyarystal-
line yttrium garnet is due to Fe24, ions, To clarify the establishment of
induced anisotropy with time, the authors determined the time dependence of
in when the specimens were rotated through 900 within --'O,l soc. 1[11 did
not change noticeably above 1300K., At lower temperaturea, 11"I changed
abruptly during rotation, and then returned to its original value (Fig,
Sign and amplitude of the jump were found to depend on the constant fleld'~0
It is believed that induced anisotropy is not yet fully established immedi-
ately after rotation through 900 and that the resonance curve at i given
temperature shifts by Hc toward stronger fields relative to the static
curve. lie 14 550 oersteds is obtained at 770K, and Ht' :z 200 oersteds at
900K, It follows from a discussion of this result that in additicn -.o the
processes that are observed after rotation, also other processes -.ake place
which have time constants considerably smaller than the time o-f rotations,
These processes are held responsible for the major Dart of the induced
anisotropy field.. As is shown,,~-iuperposition of several procenses~ with
different time constants and activation energies of the order of 0.05 ev
Card 2X-3

GUBEVICH. A. G.
Dissertation defended for the degree of Doctor of Physicomathezatical Sciances
at the Institute of Metal Physics in 1962:
"Ferrites at Ultrahigh Prequencies.0
Vest. Akad. Nauk SSSR. No. 4, Moscow, 1963, pages 119-145