SCIENTIFIC ABSTRACT SMOLENSKIY, B.L. -

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
• Document Release Date: August 31, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SMIY14SKIY ~ B.L., ROMIENUKO, ~LA.
Sendaut!j:aatic control of the dinking and cogging of Belf-
centering nut slots. Kuz.--shtam-Proizv. 5 no.7:40~41 J:L
163. (IURA 16.9)

ROKHLFNKO~ M.I.; SVIOLENSKlY, B.L.
New dynamometers. '~~sl-Lincstvroitell no.7:24 Jl '63. (MIRA 16:9)
(Dynamometers)

SMOLENSM, B.L. [Smolenslkyi, B.L.], inzh.
Head of a cutter. Mekh. sill. hoss-o. 14 no.9:13 S 163.
(MIRA .17: 1)

SMOISNSKIY, B.L.; ROKHLENKO, M.A.
--- - --------------
Power wrench with a pulse-percusaion mechanim and pneumatic
drive. Stan.i instr. 31+ n0:.1:41-43 Ja 163. (MIRA 16:2)
(Wrenches)

ROKHLFNKO, M.A.; SMOLENSKIY, B.L.
Hand vacutm suction devices. Stan.i insti-. 34 no.7:37 J1 163.
(MIRA 16:9)
(Implements, tools, ate.)

SMOLENSKIY,B. L. GOSPODARCHUK 1. L.; ROMUNKO, M. A.
I
Automatic machine for countersinking chamfers. Mashinostroital
no.12r7 D 162.' (MIRA 161l)
(machine tools)

SMDLENSKIY B L
nnt~~~
Mechanized dividing head for milling slits.
no.3:29 Mr 163.
machines-Attachments)
Mashinostroitell
(MIRA 1634)
(Milling

IWKIILENKOP M.41.; SNOUNSKIY", B.~~.
Manual pneumatic clamps for power riveting. Kuz.-shtam. proizv. 5 M-1:
42-43 Ja 163. (MIRA 16:2)
(Pneumatic tools) (Rivets and riveting)
I?-

ROKHLENKO~ M.A., inzh.; _gMOLEI!~KIY, B.L., inzh.
Checking the "optics" of sight glass. Stek. i ker. 20 no.4:
29-30 Ap '63. (MIRA 16:3)
(Glass--Testing)

SMOLEZISKIYI B-.-L.; ROEIUENKO, M.A.
~bdernization of a laying~out milling maeh=e. Stani instr.
34 no.2:39-40 F 163. . . (MUU 16:5)
(I.ttlling machines)

SMOLENSKIY, B.L.; ROKHLENKO, M.A.
Tool holder with quick-change holders. Stan.i instr'. 34 no.5:39-40
My 163. (KERA 16:5)
(Metal-cutting tools)

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AUTHORS: Klemeshov., G. A., Panasenko, F. L., 32-3-50/52
SmolensViy., F. A., Shvarts, S. Y.
TME: Standard Laboratory for Fadioactive Isotopes (Tipovaya laboratoriya
radioaktivn.ykh izotopov)
FERICDICAL: Za-vodskaya Laboratoriya, 1958, Vol. 24, fir 3, pp. R6-379 (U35R)
ABSTRACT; This paper contains a short description of a laboratory project
designed forz;a larre metallurgical plant. In this laboratory it
is intedded to use isotopes of carbon, sulphur, phosphorus,
silicon, manganese, calcium, iron, cobalt, iridium, etc. Particu-
lar attention was paid to special sanitary protective measures
in the working, distribution, tiansport, etc. of isotopes. For
this reason the laboratory project was worked out according to a
three-zone system. This system includes hermetically closed rooms
which are radiologically Itcontaminated". Isolated from these are
the "half-clean" roomsp and, completely separated,, the "clean"
rooms. In the first-named rooms preparation-, purification-, and
repair work etc. is carried out, for which purpose special
Card 1/2 clothing is worn, or, for aerosol work, hermetically closed

Standard Laboratory for Radioactive Isotopes 32-3-50/~2
chambers are used. A schematical drawing of a hermetically closed
furnace, in which it is possible to melt radioactive isotopes in
the vacuum, air, or inert gas atmosphere, is given. Conveying
radioactive preparations from one chamber into another is brought
about mechanically by means of a conveyer band, whilst a special
air conditioning system is used for the purification of air. A
ground section of the laboratory shows the arrangement of rooms
as well as other details. Thus, the building also contains a room
for gamma defectoscopy with an adijoining chamber with radiosc6pic
devices of the typerj n -Co-5-1,rj n -Go-50-1 and KC-6; these de-
vices are remote-controlled. There are 2 figures.
ASSOCIATION: State Institute for the Planning of Metallurgical Plants
"Giprostall" (Gosudarstvennyy institut po proyektirovaniyu
metallurgicheskikh zavodov "Giprostall")
AVAIIABLE: Library of Congress
Card 2/2 1. Metaliurgical laboratories-Characteristics

le, a
pri Y,
V,(p s ~,4-59
'-'T-7 U I: .0's r;"e-J.
3 '0 U"OPIS' 35 1. )L)

--al .,fi-th a ~kiall "ammiona-turee Dependence of the Diel:-etzaic juscez~-
tlbilit~r,ll Zhur. Tf,,!..',,. ilz., 15, Do. ), 1945; "Ifew Ple-zo--lectrics," Dok. A , 70, No.-
31 1950; II.Pio:~0'..-loctrimi rmi~!itioo of Ciertain Titanates and Zirconates of Bival.-!nt
ti of the Perovoldtf,- Ty-c," ~'Z-Mr. Tekh. *i,,., 1,11o. 2,
~, -urture
a
stion o~l GriEdn of ~iezooloctrlciLy,ll Dok. -ldl, 7", 1.10.
1950; "On ue 1951.

r1
.1 "hot,,X1.1"Al.2N im,
0. A. u ;;16'N;~ 7,17-TJ
.4tod tak Ia.
A
A Sk log *b=04 with II&M cow-
(190).74 cumv.var clay .
Old 0. vWvv" vbW
1. Iko cmmpd N" '60W in
imt at 12-15%04 to,,= is Ikeol Im
~,vkftll. W"bw .1 0. dbkc- WO' *
tz vow o# O.W6 ontedus temp
aded!:r 1330-1.W.
tl;~2% gaC(h did 004 ~~
10- ,,Iy goo kS./sq.
,j "ARCO can i;~ be
0 a cga. by
Tbt produc _j&W kg./Iq
This Wes to tuskVC0110'. . t
goltbc felwhK m at I
it at 2r " WO W-70%.
I 'ad-
I.q.
tbe T is the
t arcom. (0 b
as the bit ./@q.
sifen tb V 6 , " 030a as
ol t lit" I an"W4 to 35 by
(VI the &W, ti,
ag to . of 4 tb- aW--Utltc
wt.). cd vitrams pbw may fired Prod-
wbicb do 0, esad 3-7 p 10 -then c-ditio"-
(1 30 p), Upd- tb by the all"
tba=~-tite cr= wiw P;,W
the cem" dmn ww abseff"d in
j"A less Can ;WAmd prOcticsoy
of foing- Ww"arrelocius)- Y tite
.tit tbe tyw ON mus (as of the cWW-st.8
AM to the
'"CHMIUSt,44:10min ugo. "04.
Ti., effects of Ilawlts. at AIA- sdodlts- Wen *"W is
..d VOI WM lt'"t ~.:W " .k lot iee~_ OW ,
5 6;--d tba
,mt,. of 1-15% t. Zro, ,And aw $bowed bio
LVM ts* *conla steatite to
stem, fidng tcmp.
Ar.09t Of jUtjtc had a jA t$#
I a, Igo kg./sq. CM-#
t
1220
-A 0..

Feb 50.
uiaOhysics - crystals, Piezoelectric
Titanium Compounds
"Plezoelectrical Properties of Certain Titanates and
r--Zirconates of Bivalent Metals Possessing a Structure
of the Perovskite Type," G. A. Smolenskiy., 11 pp
"Zhur Tekh Fiz" Vol XK, No 2
Studies dielectric permeability of subject titanates
and.'zirconates. Establishes CdTiO3, PbTiO PbZrO
L (Sr, 9)
and'also: solid: ~ solutions 6f'(Ca~- Pb)TiOI an
MO are " seignette- electrical" (piezoe' ectric), like
Ro2elle salt crystals'. Curie temperature of these
156T107
...........
--USBR/Physics Crystals, Piezoelectric Feb'.50
(Contd)
piezoelectrics is determined considerably by
degree of covalent character of bond in lat-
tice and by dimensions of octahedron in vhich
titanium ion is located. Establishes piezo-
elect-rics of this type possess below the Curie
point a tetragonal lattice. Submitted 9 Mar
4~.
156=7

USSR/Ptiysics - Piezoelectric Jan 50
Titanates
"New Piezoelectrics," G. A. SmolenskiY, 3 PP
"Dok Ak Nauk SSSR" Vol LXX, No 3
Considerations on ionic lattice structure of AB03
(where A can be Sr, Ba, Cd, Pb, etc., and B is Ti, Zr,
Sn, Hf, Th, Ce, etc.) indicated that titanates other
than barium titanate should be piezoelectric. Experi-
mentally shows titanates of calcium, strontium,!::admium,
lead and lead zinconate are piezoelectric. Submitted
22 Nov 49 by Acad S. I. Vavilov.
158T89

Mectroulbrictim pram!" I~ comicaunic
Fee.
C. ' A. Soossolenooki . ha . ,*A
a_*C-AA6.7M.-Corffs. offinear rispectessiorta a a . ileold'
to; Anterritt RaTiOo (-IOU to 160*). PbTi% (-Iuu to
tM*). and PbZrO. (- M to 3001). Since the vol. V of a
~cignmttoelec- is a function of both the internal field inten.
_'i R anti the stories. T. 4iv - (OVjaK)'slR + (OV/
Vw'r. gm the other hand, K Is a functlim of T and of the
I.Jalitalkni 11; lirnir 111. - (Olt/4),W)" + (W'371rdl'.
III, jivr' ftx - or - (9/11, XE) VI"WOR141TV - W. whark.
.' - VA I*X-3V/i)1')m - cocil. of On skm I
etsim. E (including F - o). and op - tr/. V';ras;/b-j-)Ja
% twfl of Nurser expention at concol. x1mrstanvous polmerization.
Sill" > 0. slif-pignal. 64101.1. bylbermistoul Ilse
,,d WVON)r. lilriesurionoruts ths"o , "Our
Its, Ogriv 1.0jit (*liver the vffrvl of virroespoirilon I argue-
"t), .6 sluirp Olin. of a for IMTA and rwlrlo~. alit) : A&VID
1,rzils fur Mroo. Consequently. In DaTA wid PloTA
YIA. elect real rirtlon is PCs., anti in PbZrO# It Is owe. Thk
mrr"j,ort,14 to the shift (if TI Inim, let INTIO~ and PliTKh.
lot f 1w ifit,- I Iwi -4 oiss, of I he oploolitor" fits () lanq. whirb give.
..d I.UW ,W.. at W*): In I'WrOs. it wMM MAI that
Zr lost are Allied okww she a axi*. and t1a < 1 (11.9111111 at
2W). In MTA, the & Is, very jornmi)) f- 2 X 10-l!
deVw) In the feesep. racist frorn -21) to + 275% lbb Is due
tocompenceatices of the thertrial citisoonsitiot Isycompremaimarr-
soulting hous decreasing clectrustriction. S.-issimettorlectirk1%
with very minall ser Practically no electrostriction can be ob-
talned by "llif Wn. (it components with ekrttvafli"iung t4
upwommicl Wgiss. r.o. PhTIO, and Ilbb(lm. Inawarnommork a-
roccirmuicilve strwissres must Inhibi( dialokcronimete of ismems It'
-y-'k linaftion. rwhiolve (so the evater of the elinsismostary
cell. the die1w. consit. at& salenettuelp, Andlitirrosawswith
-decreassing elotcumtrictints. lifeamurier"ents of thominewil tit-
poinalm havo vie led no phsw transition* in the lem-tormt,-
roissims 1% 1144t0a down to - IWI'; In PIMO.. a
trionewithism to foommood tit Vow that reamm. u%Nd withs-
Ptw4m_sAIlft4b_s,4Tkh them only a vwy todat Wor-lenip.
tormsessillim. wool thick disclose. acenst. and pieweirlac. immodulto
cho!togir restitinuously between -40 and +*I*. N. Theirs

Ch-
C41 ibe probim of the orWa of evigsisill!"WeIrift. 0. A~
. tolemkil and N. V. Kotheynikova. DokWy Abad.
.A-.Wf-YS.S.R. 76, 3ll)-2:XMl); cf. CA. 44. 376le.-
,%4jrv-" ill the cr-y*ta6 showing wignettorlec 1" (1)
,fluTicl.. MTRI, OMO, S4TA, lilt
I.' el)SIV N.T.4 )~. k F., h. N.NIA N, KNIAIZI 1.*I.,-.,-,.
I-'-~1100 1",t% to ihr%-uvfu~i~m 'hat ti, link-I with cv"t^lt
in which the 0 ticlah"Irons are partly tw whWolly pMopulated
by callous forined from atoins with an incomplete next-to.
,niterniost %hell. having an inert-ga% clectrmic structure, a
,urge charge, anti amnall ratlins. Spontaneott%polturimustion
Arl". mmg to the dipole M.Mrot, 'bre to 46plAcetrient of
Ihr- c;tlimiq triativr it, the crutrif of the aclahetIrons.
,it '~ixileltv tit, ill And fit KlllA.%Ot. this qvivia-
tutmm. 14 (file to rich diliplaaviticitt of It I lons.
I he mint Invorable oructurr for appearance of I Iv that
"Itcrrin the octahedrons mect in corners, as in pmvsMte%,
~tnictu'e, with coutnuctit edges are it-" favorable, find still
Ift%, structures with common facts. The coewdination no.
is itint"irtunt from the point of view of the dimensions of the
-1,41s-lmn: fit 1wrovAlle. lonq with the cormlinAlfort riot
III C4111 rAlmmi life t.1011rdr.-I con-14"Ohly. Frm" thr
I.Out t.1 Vie. if Ofarde "fill rit'llu., the "is V...
Cf", %lo." I""" will 140" It they ityr Ivallf lnt,,
""' "d constitute uitahlr cem" atorm
I of the crystal. In aMn. to the known wigntitmelft,
ke. LuTON. AxTd(h. AuTaM,,:".'I Rhvm)4' CMINIA
x-NI". AuNtO, (it of IWm%--k IItleturrl mrs lie V%
ted to exhibit I Imarct~r at "t.j,j Ily estlitl
efts. of the tbennAl expunsicit; corif , The structure. am~f
he lattice parminmeters. RbT&Ot (jimmovskite-type, tetrallonall.
d - 3.92. c - 4.51 A.) Is a seignettorlectric. with a Curit
point of -&ID'K,. and possibly also MoO, (anstalle struck
(tire. it# whic! every ~W octake,11ram IaM. along the tituater.
nmy ririi of ruble v1~ livirking. h unovempi'A. a - 3.,A).
6 - 13.94. r - 3AI A.) with a Curie I-i"t ,Mkl*K "r
Curie point of KTI(h shoulil lie bellfw, IhAt 44 RbTlth.
contrary to Malthias and Menfrika, (18hys Now. To. ISM
(1949)); NaTiO, mmt probably h not A eignettMecirk-
in the ratile-type tetragoilsil famn of Fe(SbOv)v Anti Fr-
MOA, spontaneous tion may be courittiac td by
Fe I I ionif In the octa=, anil the tintr applie, In ..
rvrti greater I.Pre 141 t'l"I'W' N Thmit

SMOLENSKIY, G. A.
USSR/M4tals - Structure 11 Jun 51
"Ferrites of Divalent MetlalS," G. A. Smolenskiy
"Dok Ak Nauk SSSR" Val LXXVIII, No 5, pp 921-9211
Studied solid solns of ferromagnetic (NiFe2O4,
MgFe204) and nonferromagnetic
C,uFa2104, MnFe204,
i,'I7nFe20L., CdFeo04) ferrites Graphs relations
betwQe7i concn of nonferromagnetic ferrite in some
solid soln6 and certain properties of these solns,
such as Curie point, magnetostriction on satura-
tion, magnetic permeabilities, coercive forces
and hysteresis losses.- Submitted by Acad I. V.
Grebenshchikov 16 Apr 51.
184T92

SHOLENSKIY, G. A.
USSR/Physics - Piezoelectricity 1 Jul 51
"Piezoelectric Properties of Some Solid Solutions,"
G. A. Smolenakiy, M. A. Karamyshey, K. I. Rozga-
chev
I'Dok Ak Nauk SSSRII Vol LXXIX,'No 1, pp 53-56
Authors investigate temp dependence.of coeff of
linear videning of solid solns. At low temps,
points of phase transitions of solid solno are
shifted-lower, with increased SrTiO content,
than the Curie point. Authors are 3 indebted
to Prof'P.P. Kobeko. Presented by Acad A. F.
Ioffe 7 )ILY 51.

Th* theory of solgaeftelectricity. G, A. Smolenskil and
E. Paxynkt)v jSdicate Chem. Inst.. Avad. Sci. U.S.S.k..
Moscowt. Dekl4dy Ahad. Nauk S.S..V.R. 79. 431-4
(1051 j; cf. C. A, 45. 3675j.-The thermodynamic Potential
'If A perovskite.type seignettodec. substance near its Curie
point is written down as a function of the compattents a( the
polarization vector. the elec. field strength sector. the defor-
mation tensor. the elastic coasts., and consts. depending
on the temp. and pressure. Partial differentlelioa with
rtxpect to the polarization and the deformation components
yields a system of equations permitting Investigation of the
different states of a one-domain single crystal. As a reswt
of deformation of the crysW in the absence of an elec. field.
below the Curie point. the discontinuity of the hest capacity
~aad the rate of growth of the spontaneous polarization in-
~a~ with decreasing temp. In an elec. field. deformation
And piexorJec. moduli L.-e opposite signs in BaTi0j and
in PbZr0,. The shift of the Curie point of a stiancttodec.
substance under stAtic pressure depends on the sign of the
vol. clecirostsiction A.; in the case X. > 0 (BaTi0j. Pb-
TiLh), the Curie point moves to lower. and in ine cww of
X, < 0 (PbZr0e) to higher. trUIPS.; with tern electrmul-
tion, the Curie point is indePeadcut Of the Pressure- The
potArization. at a given temp.. decream with increasing
pre- sure in the can ~. > 0. increases Witlk X. < o, &ad re-
1111L7
tax unchamgcd with x. - 0. Of the existing theories of
seignettoelecuicitY. that Of Mason and Matthias (C.A. 4J.
2a,,,sd) lead* to the conclusion that in DaTio~ the transition
point is close to the Curie point, which is In cOnfilict with
expti. data; the treatment by M. and 34. at the model in
which the Ti- ion form cov4eat bonds with the 0 - - ions
and the elementw7 cell contains 6 Minims Of Potent"d
energy, is legitimate only in the cam of the Potential barrier.
w., between the ininima, futfilling the inequality 14 ~Sp F 0
(where F . internal field. It = clec- moment of the tienten-
It actually me - F P. Th. theories of
MIZUbill-VerAn"". 1-,7sa) and Stater (C.A. ", 811111W),
under which the Curie Point is deld. by the dimensions of
the central ion and the Octahedron. are unable to account
for the decrease of the Curie Point IT- PbTiO, to B^TiOs
and from Pbzro. to BaTi(16. S. Thott

SMOLENSKIY, G- A*
The Nonmetallic FermmagneticB - Ferrites, G.A.Smlenskiy, Inst of Chem of
Silicates, Acad Sci USSIR, Iz Ak Nauk S55R, Ser Fiz) vol 16, rio 6, pp 72P-738,
Nov/Dec 52.
Analysis of ferrites of the type TIFe204 (where M is a divalent metal), which
were obtained by reaction method in solid-phase state. The properties of the
ferrites were studied and plotted on graphs and tables. Indebted to Ya. G.
Dorfman.
251T24

USSR/Physics - Dielectric Lose Jan 52
"Polarization and Dielectric Losses in Zirconates,
Stannates and Certain Titanates of Bivalent
Metals," G. A. Smolenskiy
"Zhur Tekh Fiz" Val XXII1f No 1, PP 3-11
Investigates dielec permeability, its temp de-
pendence and tangent of the angle of dielec loss
of zirconates, stannates and certain titanates of
bivalent metals. Establishes that in zirconates
and stannates with structure of the perovskite
type the dielec permeability increases with in-
crease in the radius of the bivalent cation and
its temp coeff's sign changes. Shows that it is
2o6T97
USSR/Physics - Dielectric Loss (Contd) Jan 52
necessary to consider also anharmonics in order
to explain the decrease in dielec permeability of
BaZn03 and BaSn03 with increase in temp of osc ,il-
lation of the central ions in these crystals. Sub-
mitted 1 Jul 51.
2o6T

,
-0ft-, IW-olr s~iae
96. F ~Iliitik- -in
er
L-Ak _SSS
r&A
"5~-7 (1952) ImAitilai't.-
R46ults aim aud dis4Lisod -of (.avewpti~~J
-
-
,"
loglinniffivity. WI
On dw A ~_i~adcocc of
pl~~ t
SeriO.-CM0,. PbTiOj -in .tn, a . crat
40 ~oi,M'K.,'Staiq tats 4
Paw ure- liana Qt 2
ric
vxm of sow l2lutim BaTiolo-Bazro haV6 guiwa

ropmwa of the Wter
Wf, JU tft.p
wool
piczo-ifiodultis of. these sol
scs. to xfw
~ of,
MIR liwaer
.
ftZloilit twin tem b uch lesl Chip t4i
'
of BaTid, '
the expennients . Ava~ ijoCco the
chanvi- of -azio of 131,00,-
.for -Pb Yom
60 f coinWratia"
7 Yna
Is to
Vte.tc~mgwl stivdWe -afar P4ZrOS W Irel-to'l,
JW~plevl - - Z_ .
and Abstril 4952
:7
wtte
t
.

-77777
:A.

7 w-,

R.~R. akov :bar., EkSP11.1-i T -24-,69-77
eoY4~ Fm
'
e P trAW311ion from ca bleftwaWsucticileo
.
-
'

t f
A ay te!n-O
o,tetiago!iaL(seigvejt0le&) Is caled. s
,
o
&
l
b
i

ie
d
tained rc
at
ficas'll
o
mp
bgu
and the 6anges of. tb&zfiWY of
tion to the polarizatloa veiitpFl th
li~rejectrmrktw_
,
c -and to c6effs.-of Uni '.-and presOirez-, d
onsts.; -A' t'scussidu
~-
-
Rhowi thit. in In.creme- in spotitaneous~
of thek equations-
defortnation of the~.cr~stal.below th6 Curie 'U1t1d
Crt=3
City and the speed of gowth -of poh~
the rise in heat capa
tioKwith failing tezap. ~'Aiolutloa for w
elec. fields swis a correct matrix of coeff,-of tke riction-
t Is-11
a piet -.moduli-.~--Thi Curk

depend
nd otlic
k BaTiO
r
T4
"
xp
ent on p
emure"
e
e
s
Curie point -is displaced i the v
pj;c4lte dirc~_~. if th
-
the
t
d W
A
i
T
bu
t direc
e
ong
s.
x
not, isotropic
s
pression ~ is
y
ee. perineability. of, a- fall Is
cry
Tbe die)
as -v.O)issmaIIcrth4nW,a ree, crys

Y. LUXASjM -' - .
.A" . I

jy

SMOLENISKIY, Georgiy Anatollyievich.
Inst of Chemistry of Silicates Acad Sci USSR. Academic degree of
Doctor of Physical and ~Iathematical Sciences, based on his defense,
22 November 1954, in the Council of Physics Inst imeni Lebedev, Acad
Sci USSRY of his dissertation entitled: I'Segnete-electrics with a
Structure of the 'Perovekit' (?) Type."
Academic degree and/or title: Doctor of Sciences
30; Decisions of VAK, List no. 14y 11 June 55, Byulletsn' MVO SSSRy
No, 15, Aug 56, Moscow, Pp. 5-24, Uncl. JPRSINY-537

S R 537MU 621.315.612A
le propug" or AM NOW101115 d!
wv-l barium Stamiste lit WAM tiftate. - 0.
A. Smom-,',
mat AD V~ A. 1Wpo_v. 2h~ 1d*h.'F1z 24 No. 9 -
A
137S4 954) In Russian.~ 7Z
The vchunctric clectrostriction of solid solutions,
With snail barium s4amte content is greater than
j.1
1:1n the Curie mnp--::'SoUcf - 9616flons ~ with 'Small
electrostrictfort (10-irlo Bajjo~ htye hign
nimdmum,
e
'
iPchiattivitY in weak fields
thdr
relationship between
.
,
,
perrnittivity and field itrength is sharply dermed... no--

ity of golid solutions baflum
.with high
3tannato content. ch~ngcs:. considerably with mill -
temptinturc change~q. Tha Curie temperature of solid
solutions decreases when:badum stanhatc content r
ImeaseL, At the sam fitme lo;Ai-timperature phase
transfarmadons rnove towards hijbir temperaturm.,
A chanse of structum from cubic. to 'rhombohe",

occomon Wollng 3011d~3~lutlom mialning > lr/,, N
of bari stannate. Nezo-osciltatiorm occur in solid
solutim-Mth sufficfimd~~ high barium stannate 00*~
tent at temperntures hltgher by W-39'c . than: corro-
sponding values ror maximum dielectric pennittivitk. -
blid solutions have no single CU
S rie ternperuture but
'
a range of Curie ternivraturm, which can be explained:
The resonance ...-
by considerable Internal - striessm
~
frequencies and consequently the niodulus or rigidity'.,
of the solid solutions investigated increase wi
barium stannite content. 1. rijkmUmm

-A,
0S'/L,,hj-;i(1s Piezoc=lectrics F D-716
Card 1/11 Pub 146-14/18
Author Smolenskiy, G. A., and Kozlovskiy, V. Kh.
Title Thermodynamic theory of antipiezoelectrics
Periodical Zhur. eksp. i teor. fiz., 26, 684-695, Jun 1954
Abstract Discusses phase transitions from an antipiezoelectric state into a
paraelectric one or a piezoelectric one. 7 references, including
3 foreign.
Institution Institute of Silicate Chemistry, Acad. Sci. USSR
Submitted October 12J, 1954

Yt_
411111111a~
fi gLes of certain aolid solub
Phase c a Ions having eiii6rical
;p1opelues UL Aucaeue gait.. Q..A_SMUkUqUand V A-
Duktady A k
Isupov. ad. NaUrT."S = 6, 53-4(1054).~rclrr;
Eonstitutiond &graw for BaTiOBaSnO, shows that
up to 12% BaSn% the solid-soln. field is divided into
areas
;of cubic, tetragonal, orthorhombic, and rhombohedrid
'crys
gals, and only one transformation can be observed on
ssing the Curie point in the presence of 12% or more of
W
ISnO3, namely from cubic to th=63hedral. Aningi~4N
In
BhSnO, content reduces elec. owep estroys s
o"ri- 'on defined by the dipol;g~ traction, at
Pth. C.','- point. Shifthig of low-fil4o. phase chamiii. ii
Icaused by sispultuntown unidi -.1 S.
tit
&m1 movements
and 'thin individual dorpais occuff Ing at definite
Ti ious wi
BaTiOs conens. at -temps. 6det4he Curie point; -16~ls
move with it great t f d the 11111 and with
es - U,
most' diffictil onen. moves
n
the transformation 1; temp. R.:, of
VaMO-BaZrOpsystemsbiltsa Io'3'v temps. more slowly thai
iln the BaSnOBaTjO&systvrt, 11isiscausedbydifferent
characteristicsof bondsof thc&ndSnio..witb thoseetO.
Tin Ions move.to'a lesset exjejit in respect to the center of
the lattice than do Zr idiii. A higher BaZrOj concrt; also
moves the trausforniatitimpoint higher, and at 18% or more
lOnly the rhombohedral pVAqe is present. In the BaTiOrw
;SrTiOssystem, the transfdri~ation poititshifts towards lower
temps. with higher SrTiOj content mori slowly, than ~docs
i t4e Curie poizi t.
Z!
~.L 7

USSR/Physics
Card 1/1
Authors Smolenskiy, G. A., and Arganovskaya, A. 1.
Title Orgination of spontaneous polarization in lead-stannate and lead
tantalate.
Periodical Dokl. A14 SSSR, 97, Ed. 2, 237.- 238P JulY 1954
Abstract Experiments were conducted on lead-stannate to determine the conditions
under which it would have, if any, segneto-electric properties. The
atomic structure of lead containing crystals is analyzed. The possibiu-.-~*~'.~'.
ties of obtaining spontaneous polarization of every crystal, which 'may
contain lead (Sn), was.anticipated because of the atomic structure. Two-'.-
graphs are given showing temDerature-dependance of di6lectric conbtants
on lead-stannate and tantalate. Four references. Graphs
Institution Acad. of Se. USSR,.Che mical Institute of Silicates
Presented by Academician A. F. Ioffe, March 22j 1954

OL8XSKiy,

OURnIld RAItletrig., (1161 On)-,

I
I
,
iI
I
`
k
!
.
_
Zhior. Eckh. Fiz;. 25,
I
:
L
II
Is
ity and ilic dimipation fachw were mt-asitredIrmi-1) to
30)'. fit witisi. llte-t~tnps. of phase Inniskiwis fur lite.
V;triotis compils. alf-It. hisictlun 4if eampri. wcm dettiz The
rcstilts Show that.the sulid will'. (Ills, Pb)sno, (1) crysudlizes
Wills is peravAlte 'pinteturc iind posseKscs
propcrtics. Thm solos. diffi-t frolit other mignUtoeJec.

coinfid!5. in that the i
- -entnt( atsixwtfes not have Lite at,
structure of-it volile gas. The triallsition temp. of I de-
cmaks as lite Jla&A content incrmses. The soM solus.
Pb(Ts, Sii)%aod 111)(Zr,- Sn)O.:(JI) sbows high trisissilmiji -
temps. if the 1wrctiatige of PbSuOs is high. Its 11two
pht~ transition were discoircred. Weriter Tacabsuit

die

'i z

:S
I
7
.:7 ,
J

'
V
A

e
h
inetal n

ans a
~

Category :USSR/Electricity - Dielectrics G-2
Abs Jour :Ref Zhur - Fizika, No 2, 1957, No 4143
Author Smolenskiy, G.A.
Inst Institute~~f Chemistry of Sblicates, Academy of Sciences USSR
Title New Ferroelectrics and Anti-Ferroelectrics of the Oxy-Octahedral Type
Orig Pab Izv. AN SSSR, ser. fiz., 1956, 20, No 2, 163-177
Abstract Survey of the properties of new ferroelectrics and anti-ferroelectrics
with a structure of the perovskite, ilmenite, pyrochlorine, and
rhenium-trioxide type. Generalization of the experimental data make
it possible to establish that spontaneous polarization can occur
in crystals, the oxygen octahedra of which are f)illy or partly pop-
ulated with cations, having the electron structure of a noble gas atom
after the emission of s-and d-electrons'. a high chaarge, and asmall
ionic radius. Exceptions are crystals that bind lead ions Fb2j' owing
apparently to the influence of the strongly polarizable lead ions on
the character of the bonds in these crystals. Bibliography, 38 titles.
Card 1/1

v
OSTROUMOV, Andrey Georgiyevich, inzh.; IOFFE, A.F., akademik, red.;
SOMINSKIT, M.S., kand.fiz.-mat.nauk, red.; MASLAKOVETS, Yu.P.,
doktor fiz.-mat.nauk, red.; SMOLENSKIT, G.A., doktor fiz.-mat.
nauk, red.; SHALTT, S.S., dokto7TtY:~:-:iWt'-.'nauk, red.: REGEL', A.R.,
kand.fiz.-mat.nauk, red.; SUBASHITNV, V.K., kand.fiz.-mat.nauk,
red.; SHAGURIN, K.A., inzh.; ACHKINADZE, Sh.D., inzh., red.;
FRBGER, D.P., tekhn.red.
[Piezoelectric substances] Plezoelektriki. Leningrad, Leningr.
dom nauchno-tekhn.propagandy, 1957. 30 p. (Poluprovodniki, no.16)
(MIRA 10:12)
(Piezoelectric substances)

PASYNKOV, Vladimir Vasillyevich, dOktor tekhn.nauk; IOFFE, A.F., akademik,
glavnyy red.; SOMINSKIY, kand.fiz.-mat.nauk, red.; RASLAKOVETS,Yu.P.,
doktor fiz.-mat.nauk,.red.;,19),~PX!~45NIY..G,A., doktor fiz.-mat.nauk,
red.; SHALYT, S,S., doktor fiz.-mat.nauk, red.; HEGEL', A.R., kand.
fiz.-mat.nauk, red.; SUBASHIYEV, V.K., kand.fiz.-mat.nauk, red.;
SHAGURIN, K.A., inzh.; ACHKINADZ-B, Sh.D., inzh.; FREGER, D.P.,
tekhn.red.
[Nonlinear semiconductor resistors; varistors] Nelineinye
poluprovodnikovye soprotivleniia; varistory. Leningrad, Leningr.
dom nauchno-tekhn.propagandy, 1957. 35 P. (Poluprovodniki, no.5)
lectrir resistors) (MIRA 11:1)
_i

MIRLIN, David Naumovich: IOFFE, A.F., akqdemik, red.; SOMINSKIT, M.S.,
kand.fiz.-mat.nauk, red.; MASLAKOVETS, Tu.P., doktor fiz.-mat.
nauk, red.;'~M-OYZY~~iT doktor fiz.-mat.nauk, red.;
SHALYT, S.S., doktor fiz.-mat.nauk, red.; R-WEL, A.R., kand.fiz.-mat.
nauk, red.; SUBASHIYEV, V.K., kand.fiz.-mat.nauk, red.; SHAGURIN, K.A.,
inzh., red.; ACHKINADZE, Sh.D., inzb., red.; FREG19R, D.P., tekhn.red.
[Semiconductor bolometeral Poluprovodnikovye bolometry. Leningrad,
Leningr.dom nauchno-takhn.propagandy. 1957. 36 p. (Poluprovodniki,
n0.4) (MIRA 10:12)
(Bolometer)

PHASE I BOOK EXPLOITATION 676
Smolenski2r., Georgi-y.Anatollyftvich, Doctor of Physical and Technical Sciences,
Isupov, Vladislav Aleksandrovich, Engineer
Segnetoelektriki (Seignetoelectric Substances) [2d. ed., rev. and eal.] leningrad,
Leningradskiy Dom nauchno-tekhnicheskoy propagandy, 1957, 43 P. (Obshchestvo
po rasprostraneniyu politicheskikh i nauchnykh znaniy. Poluprovodniki, vyD. 15)
15,000 copies printed.
Sponsoring Agencies: Akademiya nauk SSSR. Institut poluprovodnikov, and Lenin-
gradskiy Dom nauchno-tekhnicheskoy propagandy.
Tech. Ed : Freger, D. P.; Editorial Board: Ioffe, A. F., Academician (Ed. in
Chief~, Sominskiy, M. S., Candidate of Physical and Mathematical Sciences (Asst.
Ed. in Chief), Maslakovets, Yu. P., Doctor of Physical and Mathematical
Sciences, Smolenskiy, G. A., Doctor of Physical and Mathematical Sciences,
Shalyt_q S. S., Doctor of Physical and Mathematical Sciences, Regell, A. R.,
Candidate of Physical and Mathematical Sciences, Subashiyev, V. K., Candidate
of Physical and Mathematical Sciences, Shagurin, K. A., Engineer, Achkinadze,
Sh. D., Engineer.
Card 1/4

Seignetoelectric Substances
676
Ch. III. Preparation of Seignetoceramics and of Single Crystals of
Barium Titanate 13
1. Production of seigni5toceramics 13
2. Growing single crystals of barium titanate 14
Ch. IV. Basic Properties of Barium Titanate 16
1. Crystal structure 16
2. Domain structure 17
3. Dielectric hysteresis and spontaneous polarization 20
4. Specific inductive capacitance and losses 22
5. Piezoelectric effect 24
6. Volume resistivity and electric strength 26
Ch. V. Properties of Certain Solid Solutions with a Barium Titanate
Base 27
1. Solid solutions of barium stannate in barium titanate 27
2. Solid solutions of lead titanate in barium titanate 29
3. Solid solutions of barium meta-niobate in barium titanate 32
Ch. VI. Anti-seignetoelectric Substances 33
Card 3/4

SUBASHIYEV, Vagan Kasparovich. kand. fiz.-mat. nauk,; IOPTE. A.F., glavnyy
red.; SOMINSKIY, H.S., kand. fiz.-mat. nauk, red.; MASLAKOVETS,
Yu. P.. doktor fiz.-mat. nauk. red.- SMOLENSKIY. G.A..doktor fiz.-mat.
nquk, red.; SHALYT, S.S., doktor REGELI, A.R.
kand. fiz.-mat. nauk,red.; STIAGYRIN, K.A., inzh., red.; ACHKINADZE,
Sh. D.10 inzh.. red.
[Transistor diotes and triodes; point-contact diodes and triodes]
Poluprovodnikovye diody i triody; tochechnya diody i triody.
lemingrad, Leningr. dom nauchno-tekhn.,propa.gandy, 1957. 52 p.
(Poluprovodatki, no. 7). (MIRA 11:11)
(Transistors)

SCKINSKIY, Monus Sa~uilovich, kELnd.' fiz.-mat. nauk; IOM, A.?., almdemik,
glavu~7 red.; MASLAKOVINTS, . Yu.P., dokto ri fiz.-mat. nauk, red.;
SKOLANSKITI GoA., doktor fiz.-mat. nauk, 'red.; SHAWT, So$&',
dofc~-o -. nauk. red,;' M64W, Ao"Ps, kand. fiz.-mat;,nauk, red.;
SUBASHIM, V.K., kand. fiz.-mt. na,~k, red.; SELMIN, ]C.A..
in2h.; redo; ACHKINA Sh.D. inzh., red.; FMIM, D.P., tekhn.
red,
[Photoresistors] Fotoooprotivioniia. Leningrad'. Leningr. dom nauchno-
tekhn. propagandy, 1957- 54 p. (Poluprovodniki, no.6).(KM 11:91
(Photoelectric cells)

SUBASNITXV. Vagan Kasparovich, kand. fiz'.~-mat nauk.; IOFFE, A.F., akad.,
glavrxv.v red.; SOHnISKIY. M.S..knnd. fiz.-mat. nauk,red.; NASLAKOMS.
Tu. P,.dciktor f iz.-mat. gauk, ~ red.; j)JOLIVSXIT,,.-G",, dok-tor f iz.-mat.
rAuk.-red.; SHAWN. S.S.. doktor fiz.-mat. nauk, -r'eil.; REGELI.
A.R., kand. fiz.-mat. nauk, red.;SHAGURIN, K,A.#iu;h.i"d.',-
ACHKIMADZI, Sh.D..inzh.,rsd.; FRMYM. D.P., takhn. red.
[Photoelectric converters of solar energy)'Fotoelektricheskie
pisobrazovateli so'Inechnoi anergil. Ianingrad. loningr. dom nauchno-
tak"ha. propagandy, 1957. 61 p. (Poluprovodniki, no. 9). OIIRA 11:12)
(Solar batteries)

GELIAM, Isaak Khaimov ich, inzh.; "SKIN, Bamull Semenoylch,inph..~IWFE. Aj.,ftademik,
red.; SOMINSKIT, M,S., kand.fiz.-mat.nauk, red.; MASLAKOVETS, Yu.P.,
dok-tor fiz.-mat.nauk; SHOLENSKU.- A., doktor fiz.mat.nauk;
SHALYT, S.S., doktor, fiz.-mat.nauk; REGEL', A.R., kand.fiz.-mat.
nauk; SUBASHIYXV, V.K., kand.fiz.-mat.nauk; SHAGURIN, K.A., inzh.;
ACHKINADZE, Sh.D, inzh, red; FRMICR, D.P., tekhn.red.
[Semiconductor contact rectifiers] Poluprovodnikbvye vypriamiteli.
Leningrad, Leningr.dom nauchno-tekhn.propagandy, 1957. 94 Ir.
(KIRA 10:12)
(Electric current rectifier)

ZHUZE, Tladimir Panteleymonovich; 1OFFE, A.F., akademik, glevnyy red.;
SOMINSFIY, M.S., kand.fiz.-mat.-nauk, red.; MASLAKOMS, IV.P.,
doktor fiz.-mat.nauk, red.;-.W1OIMi.SKIY, G..A., doktor fiz.-mat.
nauk, red.; SHALYT, S.S.. doktor fiz.-mat.naulr-, red.;
A.R., kand.fiz.-fmt.nauk. red.; SUBASHIYEV, V.K., kand.fiz.-mat.na-nk,
red.; SHAGURIN, K.A., inzh.. red.; ACHKINADZE, Sh.D., inzh., red.;
FRXGER, D.P., teldm.red.
[Semiconducting materials (semiconductor elements)i Poluprovo(Ini-
kovye materialy (elementy - poluprovodniki). Leningrad, 1957.
101 -D. (Obshchestvo po rasprostraneniiii politicheskikh i nauchnykh
znanii RSFSR. no-17) :'(MIRA 12:4)
(Semiconductors)

AUTHOR Smolenskiy, G.As 57-8-18/36-
TITLE On the Appearance of Spontaneous Polarization in Cristalsq
(K voprosu vozniknoveniya spontannoy polyarizatsii v kristalm
lakh.)
PERIODICAL Zhurnal Tekhn. Fiz., l.957, Vol. 27, Nr 81 PP. 1,778-1783 (U,95R)
ABSTRACT A surrdy is given on the ideas prevailing at present. The critics
on the development of ROCHELLE salt electricity are investigated.
The problem of ROCHELLEsalt-mactive ions and the problem of the
nature of the chemical compounds in ROCHELLE-salt electrica and
anti-ROCHELLE-salt electrics are discussed. Some data on the cons
struction of electronic shells of ions being present in oxygen
octahedrons- of ROCHELLE-salt electrics (which contain no hydrogen)
are given. The author shows that hydrogen compounds, with the
presence of which the development of spontaneous polarity in some
compounds containing hydrogen is-connected, in all. ROCHELLE-Wffalt
electrics, containing hydrogen or notp are not pure ion compounds.
(With IL table and U. Slavic references).
ASSOCIATION Leningrad Institute for Semiconductors of the Academy of Sciences
of the USSR. (Institut poluprovodnikov AN SSSR, Leningrad.)
SUBMITTED Feb.1, l-957-
AVAILA,BLE Library-of Congress
Card 141
Tqui)ov, V. A-, A.~,,ranovskaya, A. I-~J-7-11-15/33

il~'THCK SMOLENSKII G.A.,, ISUPOV V-A-,.AGRANOV3KA1A A.I., PA' - 3o4l
TITIS --?nMT-TrW2r1t1-6s in Beignette-Eiectric SoAd Solutions on the Basis
of Strontium Pyro Tantalate.
(Fszovyyi perekhody v segnetoelektricheskikh tyerdykh raBtvorakh na o9nove
.pirotantalata strontsiya ~Russian) I
FERIODICAL Doklady Akademii Nauk SSSR, 1~57, Vol 1-13, Nr -4, PP. 803-8o5 (U.S.S.R.)
Received 6/1957 Reviewed--7/1957
ABSTOZT The solid solutions of the seignette electrica. of thii type investigated*
up to now.are enumerated Ln short. The present paper investigktes other
solid solutions of seignette-electric niobates and tantalatea-and gives
som data on the solid solutions In the following system : Sr 2~~2"7 +
+ 13a2Ta2 0 andbr2Ta2O?.4 %U207. Hitherto the sam-
8r2Nb207, Sr2Ta207 7
ple have not been investigated radiographically, but the distinct shifiing
of CURUt's tamherature is indicative of the creation of solid solutions.in
.alimited concentration interval.,The samples were produced according tothe
usual ceramic method and were annealed for-6ne hour at a temperature*of
1480%. An 'increase of the CURU temperature of the.solid solutions of
Sr2(Ti,Nb')20 was expected on the.occasion of the replacementcf Ta-ions
by Nb-ioxa. Le presezt paper confirms this expectatioti, as may be seen
from the attached diagrams of'the temperature dependence of the dielectri-
city emstant of the solid solutions in the system 5r2Ta2(~+Ur?Nb207. Tile
dard 1/2 CLMS temperature increased by about 320 on the occasion of an .increase of
i

~.UTHCR- 5MOUNSKIL G.A., ISUPOV V.A., AMV1CP1SUYA A-I-, PA - 3c&-
TITLE' fh-esoTrd-S61Utions of Metaniobate a-Lid Ketatantalate of Bar!:.~M in
Barium-Titanate which Have Seignette -Electric Properties.
('fverdyye rastvory metanio'bata i metatantalata bariya v titanat-e barlya,
obladayushchiye segnetoolaktricheskimi svoystvami -Russi.-M)
PERIODICAL Doklady Akademii Nauk Szia~ 1957, Vol 113, Nr 5, pp lo53-1056
Received 6/1957 Rev-iewed 7/1957
ABSTRACT The authors investigated various compound systems BaTiOa - B&0s5'1FOQ5
and BaTiQ3 - Bao,~TaO,3 With a content (of up to lo mol.-pereent) of
BaO15UbO3 and Bau'5TaO3. The polycrystalline samples with a low degr~me of
open porosity-were produced in the usual manner. The introduction of bari-
um-metaniobate into the,' barium titanate modif ies the t r
o7pe ature dep~~adance
of E and tg 6 considerably. With a content of 1 mol.- 0 Bao,5NbO3 theE ~
peak.vanishes at Curie point and there remains only a salient point in the
curve L = f (T) . If the 13&6,5ND03 content increases,, this salient point be-
comes less pronounced, and with more than 5 mol-0/0 Bao,5NbO3 it vanishes
entirely. In scild solutions a maximum of E is found to ezist in the domain
of the pha:se transition from the tatragonal to the orthorhodbic structure.
If the coheentration of bariumpmetaniobate increases, the maxima of the cur,
vas 9 - f(T) weaker and more washed out, on which occasion they shift to-
wards lower temperatures. The position of the maxima and of the salient
point-s of th'e curve 6 - f(T) does riot depend on frequency in solid sclut3.cns,
Card 1/2 In solid solutions with a high content of barium metaniobate tg 6 chan,:q

~S M 0 /_ E, N Y,
24( 0) FILAM I BOOK EXPLOITATION SOV/1180
Vsesoyuznaya konferent'siya po fizike dielektrikov, Dnepropetrovsk, 1956.
Fizika dialektrikov; trudy konferentsii... /(The Physics of Dielectrics; Trans-
actions of the All-Union Conference on the Physics of Dielectrics) Moscow,
Izd-vo AN SSSR, 1958. 245 P. 3,000 copies printed/
Resp. Ed.: Skanavi, G.I., Doctor of Physical -Mathematical Sciences; Ed.: Fillp-
pova, K.V. , Candidate of Physical-Mathematical Sciences; Ed. of Publishing
House: Starokadomskaya, Ye.L.; Tech. Ed.: Astaflyeva, G.A.
Sponsoring Agencies: Akademiya nauk SSSR. Fizicheskiy institut, and Dnepropet-
rovsk. Universitet.
PURPOSE: This book is intended for scientific research workers, professors,
industrial engineers and laymen who are interested in the study and use of
j
dielectrics and dielectric materials.
COVERAGE: /This volume publishes reports presented at the A1.1-Union Conference
on the Physics of Dielectrics held in Dnepropetrovsk in August 1956, sponsor-
ed by the "Physics of Dielectrics" Laboratory of the Fizicheskiy institut
Carc 1/.0

The. Physics of DielecLrics (Cont. ) SOV/1180
ABSTRACTS OF REPORTS READ AT THE CONFERENCE AIM PUBLISHED IN THE
JOURNAL "IZVESTIYA Ail) SSSR, SERIYA FIZICRESUYAn, Nos 3 and 4, 1956
Kseadzov, Ya~M. The Inflizence of Admixtures on the Electrical Properties of
Ratile 5
Finkel'shteyn, B.,N. and N.C. Fastov. (Moscow, Institut stali (Institute of
Steel] The Rela-xation Theory of Electrical Polarization 5
Skanavi, G.I., Ya.I.-Kseadzov, V.G. Prokhvatilov, V.A. and Trigubenko.
Non-Seignette-Electric Dielectrics With High Dielectric Constant 6
Smolenskiy, G.A., V.A. lsupov, A.I. Agranovskaya and Ye.D. Sholokhova,
1,-H3_ngY.:Fu1, -Institut khim:Li silikatov AN SSR ( Institute for Silicate Chem-
istry, AS USSR] Polarization and Dielectric Losses in Several Solid Solutions
of the First and Second Classes 7
Glauberman, A.Ye. [L'vov, Gosudarstvennyy universitet (State University)
Theory of Systems with Non-Centralized Vechanism of Particle Interaction. 7
Card ~~P_
.02

48-22-3-2/N
Polarization and Dielectric Losses in Some Solid Solutions of the First
and Second Type. Theses of the Lecture. The Complete Article is I`ublished
in ZhTF, 1957, fir 27, p. 2528 and DAN USSIR, 1957, N.,. 113, pp. 803 and 1053
3) The system of the solid solutions BaTiO -LaA10 was
3 3
investigated.
4) Solid solutions of the fiz-st type: (Sr, Ca)2Ta.20V
(Sr, Ba)2Ta20V Sr2(Ta, Nb )207 were investi.1-ated on the
basis of strontium-pyrotanta-late.
5) The results obtained by the provisional investi-ation of the
solid soli!tions of the second type are -iven: BaTiO
BaTa206 and BaTiO~-BaNY6.
ASSOCIATION: Institut khimii silikatov Akademii nauk SSSR (Institute of
the Chemistry of Silic--tes,AS USSR)
Card 2/2 1. Crystals--Polarization 2. Alloys--Dielectric properties

24(6 A= 1]3rWX2ATICK SCYA503
Akadectlys. nauk SSSR. In#tjtut poluprovodmtkov/
P0luYr0v0dn1k:L v nauk* I takhnike, t. 2. (5--goonductors In Science
and Toohnology, Vol 2) Moscow, Izd-va AN 333 , 1956. 658 P.
17.000 copies printed.
Kemp. Ed. I A. F. larfe, Tech. Sid. % R.3. Pevzmor.
FURPWXi This collection of articles is Intooded for scientists, on-
51nears; and technicians.
COVERAaRl The collection. published by the SemIcanductor Institute,
Academy of Science*, U33R, under the suporvIsLan of Academician
A.F. iofre, contains Parts II and III of a tvo-volume work on semi-
sandu4tors. Part 11 completes the material on semiconductor devices,
begun In Volume Is and Part III describes various semiconductor ma-
terials. Lack of space did not permit lmc2umlon of such subjects
as crystal counters, th aMae I..tric gall erxtors, a tomin batteries,
luadnophores, swAlcondua tor catalyzera. materials for 00--Pl*x cathodes
and various other applications or somicoodu*zors. lorfe points out
tl~,~ American scientists V. Johnson and 1. LArk-
SorovItx an semiconductors at low tomperattxres deals with a subject
hardly covered In the Soviet literature. Similarly. the article by
the Swiss scientists 0. Busoh and U. Winkler r1lls a gap In the
Soviet literature on methods of InvestisatIng sealconduotor charac-
torlatics. Theme subjects will be dealt w--th exclusively In a pro-
posed third volume. References appear separatoly after *&ch AWwM.
TABLE OF CON=Mt
Ch. 20. a 2 ,a and 1,0o "'Ich. Terrostavatic
'
0. Onlutr.
emloomMuo ors 349
the author 41scuss the application of forraime4potic samicanduo-
tore In multichannel telephony, radar, eloctroaccustion, oleo-
Sronla counters, acres of induction coils, transformers and ril-
Sera. p&rwsment magnets, 1004vie too trio tion tramaduc*rso memory
elmments# @to. They explain the ar7stallozraphr or forrites and
the theor*tieLl fundamentals of nonccmponaazwed antiferromagnat-ism.
cam 619
a discuss problems or magnetic sAtUxItiOn In ferrite& and
They gas
their bahavicur in &-a magnetic fields szd at very high frequencies.
Spsois.l chapter$ cover such subjects me 4lsztr1%maXn*tic Oscillations
In forriten and nonlinear proos3ses oG4U=Im9 at vary high rrequen-
Ojos. The concluding chapters dena with the electric properties or
forritag and with ferrite mAteriman and th&Lr -sale* tion. There are
53 references, of wUah 33 are English OX4 210 Soviet.
Ch. 21. and V.A. Isupow. 3eIgnetooleatric
-maze 425
am thora explain the dIfferences and a1xL2&rLtiss between
.&sign a tooloo trio, plazools4tric and forromagmatic materials. They
present a historical survey or salznot0qj*ctrIcLty and provide data
tables of seIgne tool** trI a materials. The authors explain the run-
&Lmcntals of the microscopic theories an 41a,1gnatc*joc trio phenomena
and discuss In detail the crystal lattice structure, physical Pro-
perties and problems of producing various aftlCle toolea trio materials.
they briefly describe antissignatooloctric m.&tqrjLls and draw atten-
Uon to recently adopted applications of t-hose materlolele.C., mini-
ature eapaoltors, nonlinear capacitors, P18=02emOnto and memory
slemests. There are 35 reforenass. or which, 20 are Soviet. 13 English
0=4 7/9

AUTHOR S. Smolenskily, G. A. . Agrano-skayaa. A, 1, 071/57. 23--7-21/35
TITLE Die! 7. -Eric. Polarization and Losses of So-me Com.-lex Compounds
(Dielel-Aric-heskaya polyarizatsiya i poteri nekotorykh soyedi-
neniy slozhno-o sostava)
PERIODIC2,L; Zhurnal tekhnicheskoy fiziki, 1958; Vol,, 28, Nr 7.
pp. 1491 - 1493 (USSR)
ABSTRACT.~ The authors investi-g-Ae by the example of oxygen compounds with
perovskite structures the possibility of obtaining compounds
of complex composition. In this case the [;eneral formula reads:
(A.'', .- A ) (B -~B,)O The conditions necessary for-the
k 3*
ions A, and B. are written do-an. Considerin& that the ions tend
1 1
co a certain coordinate number it may be assumed that the possi-
bility of the forination of a number of coriipounds (k,jA 2)(B,~B 2)03
vrith perovski-te structure is riot impossible. In an analogous
way also the possibility of the formation of solid solutions of
com-~,ounds -aith complex composition and perovskite structure, as
viell as of compounds and solid solutions of other structures
Card 1/3 can be investif-ated. A number of such compounds and solid so-

Dielectric Polarization and Losses of Some Complex 50'~,57- 29 -7 -21/35
Compounds
lutions were synthetically investigated on this basis. It was
shown that of the investigated compositions with perovskite
structure Pb',(NiNb I and Pb3 (MgNb2)0 have a high dielectric
2)09 9
constanz. Pb 3YgNb 209 is a ferroelectric substance with a Curie
temperature of-100C, The high dielectric cmAant of Pb 3Hillb 209
is dependent on the relaxation mechanism of polarization. It is
possible that the relaxation mechanism in Pb 3Nillb2 09and in some
other compounds and their solid solutions does not depend on
ion processes but on electron processes. It is assumed that a
ferro--electric phase zransition exists in the "relaxators" at
sufficiently low temperatures. The difference in the -mechanisms
of dielectric polarization in the compounds Pb 3 Mglfb209and
Pb3NiNb 209 in the investigated temperature interval proves the
important role played by the structure of the electron shells
of the ions and the character of the chemical binding. Thus a
ferroelectric substance with complex composition was discovered
Card 2/3 for the first time. The authors show ways for searching ferro-

Dielectric Polarization -and Losses of Some Complex JUY/157- 28-7-21/35
Com.dounds
electrics, and moreover of compounds of complex composition as
wellasof solid solutions with irit(~reating electric and ma6nietic
properties. R.A.Zvinchuk ansiated in this work and supervised
the determination of the lattice parameters of elementary cells
of the investigated compounds.
It could not be fDund which of the formulae was correct, that
with or that rithout brackets. One of them must be a misprint.
There are 1 figure, 1 table,and 1 Soviet referan2a.
ASSOCIATION: Ir-stitut Doliiy)rovodnikov All SSSR Lenin1:--r---(i (Inutitute for
Semiconductors. AS USSR, leningrad)
SUBMITTED: JanuarY 7, 19~8
Complex ions- -Po larogr aphic analysis
Card 3/3

C.-T.: -:0
J 0
mo -f t--n:-' K 1.7% gr-,i novck a y a, :Oupov,
T T New Ferroelectric `u bota tic es of Compit-x
r,egn,-.-z,,,elektrl.ki slozntiogo sostava
T T . Pb Fe NoO, and -rb YbNbO ( I I -l'b 4't,
a 2 6
'Lhjrna! teKnninnaskuy t'izii-i'Vol 28, ~ir
Com-po,!, ion ovy y C
NO N b C)
op '21:`-2-211t-A
CT - Thiz pai)er cover.; ar, o, zne Oyiitnet-lc p-odoc,.ion cf
polycrystaliine sampl~!s Of lb 2~, e NbO6 and To Y OJ b 06' T 1, ey 7i r e
D.Y11MCCized by a rt-action in solid phase accoraing to conven-
tional vowder-metallu.-,S-ical me-thod-j. -Trie Pb 1; FeNbO6samples were
at the ;'b
sinr,ercd , ;~ I bNbC.)6aT, C. It was -~sLabiished
b,,,: X-rjuy structural analyses tf-.fit the cumpounds produced have a
thk,. riiob-ium-, yr,,.erb-um-, ,jnd iron inz-:
occupying octshedric positions. The dieiectric constant of
Pb2 FeNbo 6 sampies passes tirough a maximum at 112()C. Pronouncea
r6 1/2 dieiFctric hysteves.in. lcofm -. .-t-- hit,irid Ft room terjper:i!ur.~.

!'prroeiectric '~ubst-,nce8 of a Corn:)Iex Comoosition, SOV/57-O-)c-s.4,~,
IT
'Lli r, C: d b b i b G
6
j3 a I'erroelectric s~ibstance. Th~ maxim,"rn, r..,' ~h~
-;-,ctric cc-nzitan-. o.` ',;b
NoO, h i c n i m -a 1 Coun d a t a
rr, c t ihiK,,ier valoc!, at e~,,iO C. ThE curve flT exhlbits a kink
n, . r -:-' 4
Iq : eQaals 0.)i at room ternDerat-ure and a frecuency
Key. 1L auickly Jncr ns,~,; a
L lleating, pa.,4-inp thrcugh a not
v 1 - [-.v -,"Inimum aL about ~40 C, and increasing again nence-
,.,j-th. 'Phe, `c-lectric con-~tan~~ v-rsus temnera-ure funczi~~n
1~'PIL,il 01* dint- - ferroeleczric i;Ab~-,*u5n,,-,-,S, ao,,t?ncc- -)f* a
ond tqe ;mai i ci,itc-rion t
-~t.,-,ntiate tht; an,';omul ion t7 a L
subz 11
b."I bNO.'. s a. n
ure ref erenc ea.
-i-ch re et.
n -
2/2

SMOLENSKIY, G.A.; ISUPOV, V.A.; AGRAITOVSX&YA, A.I.
Dielectric polarization of solid solutions in the system (Ba,Sr)
Ta,Nb)206, Je '59. (MIRA 12-10)
l.Institut poluprovodnikov AN SSSR, Leningrad.
(Solutions, Solid-Blectric properties)

SMOIZNSKIY, G.A.; AGRAMOVSKAYAt A.I.; POPOV, S.N.
Polarization mechanism in Pb3NINb 0 solid solutions.
IFiz.tver.tela 1 no.1:167-168 Iya ?; ?9Nb209 (MIRA 12:4)
(Solutions, Solid) (polar*ization (Electricity))

SMOLENSKIY, G.A.; ISUPOV, V.A.; AGRANOVSKAYA. A.I.
New group of seignettoelectrics with a laminated structure. Fiz.
tver.tela 1 no.1:169-170 Ja 159- (MIRA 12:4)
(Ferroelectric subatances)

SMOLENSKIY,.G..A.; ISTJPOV, V.A.; AGRANOVSKAYA, A.I.
t3 es) 0(
New eeignettoelectics of complex composition of the type P1634) IT 0
Part 1. Fiz.tver.tela 1 no.1:170-171 Ja '59. (MIRA 12:
(Ferroelectric substances)
( q#-2( +36+5
2 8 1 11)0(.)

SNTOLENSKIYO' G.A.; ISUPOV, V.A.; AGRANOVSKAYA, A.I.
Seignettoolectric properties of solid solutions in the system
FbNb206 - BaRb206 - SrNb206- Fiz- tvar. tela 1 no-3:442-449
Mr '59. (MIRA 12:5)
l.Institut poluprovednikov AN SSSR, leningrad.
(Solutions, Solid) (Curie point) (Ferroelectric substances)

SYOLENSKIY, G.A.; AGRAI;DVSKAYA, A.I.; ISUFOV, V.A.
Pb
New seignettoelectrics of complex comPosition. Part 3: 21006,
Pb3Fe2WO9. Pb2FeTaO6. Fiz. tvar. tela 1 no.6:990-992 Je 159.
(MIRA 12:10)
1.Institut poluprovodnikov Akademii nauk SSSR, Leningrad.
(Forroolectric substances)

66336
_2~ 2*7?06 SOV1181-1-10-11121
AUTHORS: Smolenskiy, G. A., Agranovskaya, A. I.
TITLE: Dielectric Polarization of a Number of Compounds of Complex
Composition
PERIODICAL: Fizika tverdogo tela, 1959, Vol 1, Nr 10,
PP 1562 - 1572 (USSR)
ABSTRACT: The f-- and tg8-values were measured at room temperature and
I kilocycle by the usual methods for a number of polycrystalline,
synthetic complex compounds. The results obtained for 19
samples (such as Ba(Ta, Al)O 3' Ba(Nb 0-51 Al 0.5 )031
Pb(Ta, AI)O 39 Ba(Ni,Nb)o 39 etc) are given in table 4. Table 3
contains the exact compdsition of the various samples, the
prelimi,riary and_fina,.l annealing temperature and annealing
time. 8 of these saiiples belong to the perovskite minerals.
The structure of one sample was indicated by I. G. Is-
mail-zade. Further results of measurement are shown in dia-
grams; the temperature dependence of the e- and tg6-values of
Pb (Mg,Nb at I.,kilocycle (Fig,!); trie -E Zi i1nd ~.tgb -values
3 2)09
Card 1/3

66336
Dielectric Polarization of a Number of Compounds of BOV/181-1-10-11/21
Complex Composition
of Pb3 (Ni,Nb2)09 at 1, 45, 450, and 1500 kilocycles (Figs 2-3);
the E- and tg6-values of some more samples (Fig 4), and the
F_- and tg6-values of the sample 1-10 at 1, 450, and 1500 kilo-
cycles. Theoretical considerations which have been discussed
in detail in the introductory note and experimental results
permit the following conclusions: 1) Certain complex compounds
of a particular structure as well as their solid solutions can
be predicted on the basis of the condition of electric neutra-
lity, the specific nature of the crystal structure and the
tendency of ions to subordinate themselves to a certain coor-
dination. The phase diagram of the corresponding multicomponent
system need not be studied. 2) Among the investigated perov-
skite samples, Pb 3 (Ni,N*b2)09 and Pb 3(Mg,Nb 2)09 have the largest
dielectric constant. The compound Pb 3 (Mg,Nb 2)09 is a Seignette
salt. The dielectric polarization of Pb (Ni,Nb )0 is character-
ized by relaxation and piezoelectric prgcesses~ 12 is assumed
here that the activation energy of relaxing particles be
very small within the region of phase transition. The results
Card 2/3
4V

66336
Dielectric Polarization of a Number of Compounds of SOV/181-1-10-11/21
Complex Composition
of this investigation were published at the II All-Union
Conference on FL-rroelectricity held at Rostov-na-Donu in 1957.
There are 5 figure3, 4 tables, and 11 references, 6 of which
are Soviet.
ASSOCIATION: Institut poluprovodnikov AN SSSR, Leningrad (Institute for
Semiconductors of the AS USSR, Leningrad) L~K
SUBMITTED: August 4, 1958
Card 3/3

66337
2A7900 SOT/181-1-10-12/21
AUTHORS: Smolenskiy, G. A., Isupov, V. A., Agranovskaya, A. I.
TITLE- Ferroelectric Solid Solutions of Substitution With
Subtraction
PERIODICAL: Fizika tverdogo tela, 1959, Vol 1, Nr 10,
PP 1573 - 1582 (USSR)
ABSTRACT: In order to complement publications by many Western authors
and the Soviet scientists Skanavi and Ksendzov, the authors
studied the #wroelectric properties of the following systems:
BaTiO -Ba 0-5 NbO 3; BaTiO,-Ba 0.5 Ta03 ;BaTiO,-La 2/3 Tio3;BaT '03-
-BaO;NiO; BaTiO3-WO 3' BaT '03 -BaO:AIO, .5 ; BaT '03 -NaT '02-5-
The samples were prepared by the usual ceramic methods. For
burning temperatures of the samples see table 1. The temper-
ature dependence of the E.- and tg6-values for the individual
systems is graphically illustrated in figures 1,2,4, 5, 6 and
10. Figure 3 shows the temperature dependence of phase trans-
formations occurring in the solid solutions of the systems
Card 1/3 BaTiO 3-La 2/3 Tio3and BaTiO 3-LaAlO 3* The temperature dependence
ql*"

66337
Ferreelectric Solid Solutions of Substitution SOV/181-1-10-12/21
With Subtraction
of the specific elongation of the solid solutions of
BaTiO -Ba 0.5-YbO3 is depicted in figure 8. Figure 7 repre-
sents the dielectric hysteresis 10OP3 of the solid solution
of the system BaTiO 3-Ba 0-5 NbO3as dependent on the BaNbO 3
content. Figure 9: temperature dependence of the dielectric
constant of the solid solutions of the system BaTiO -Ba 0.5 NbO3
as dependent on the Ba 0-5 NbO 3concentration. Final digest: 1)
The ferroelectric solid solutions of substitution with sub-
traction may be divided into two groups: a) In the first group
the maximum of the dielectric constant at the Curie point
is retained even if the solid solution contains a high per-
centage of the second component. b) The maximum of the di-
electric constant of the second group is suppressed already
by a small percentage of the second component. The first group
includes the solid solutions of La 213 TO3 in BaTiO 3' whereas
the solid solutions of Ba 0.5 NbO,, Ba 0.5 TaOVand BaO:NiO
Card 2/3 in BaTiO3 belong to the second group. 2) The properties e

66337
Ferroelectric Solid Solutions of Substitution SOV1181-1-10-12121
With Subtraction
of the solid solutions (second group) of substitution with
subtraction may be explained by the perturbing effect of
electrons and holes located-near the vacancies of the crystal
lattice. The first report on this investigation was delivered
at the All-Union Conference on''Ferroelectricity held at
Rostov-na-Donu in 1957-The Soviet scientists Yu. N. Venevt-
sev, A. F, Ioffe, Devyatkova, and Stillbans are quoted in
this article. There are 10 figures, 1 table, and 9 references,
4 of which are Soviet.
ASSOCIATION: Institut poluprovodnikov AN SSSR, Leningrad (Institute for
Semiconductors of the AS USSR, Leningrad)
SUBMITTED: August 18, 1958
Card 3/3

88695
'7-43-00 loq~- Il-'TS) S/058/60/000/0io/004/0i4
A001/AO01
Translation from: Referativnyy zhurnal, Fizika, 1960, No. 10, P.,054, # 27014
AUTHORS: Smolenskiy, G.A., Agranovskaya, A.I., Sholokhova, Ye.D.
TITLE: Ferroelectric Properties of Solid BaTiO3-LaAlO 3 Solutions
PERIODICAL: Fiz. sb. L'vovsk. un-t, 1959, No. 2 (7), PP. 101-- 106
TEXT: Ferroelectric properties of solid solutions in the BaTiO LaAlO 3
system were investigated. In this system solid solutions are formed WN~ the
structure of perovskite, possessing ferroelectric properties at the high content
of barium titanate. The Curie point and dielectric constant in the peak of solid
solutions are sharply decreasing with an increase in the content of lanthanum
aluminate. No spontaneous polarization occurs in lanthanum aluminate and in solid
solutions containing more than 16 molar % LaA10 . These experimental data corrob-
orate the viewpoint that central ions in ferroeiectries must have the structure of
inert gases after losing s- and d-electrons, i.e., must form from atoms with the
card Card 1/2

IOFFE. V.A. [ translator] ;_ ~! ~01.~#SKIY,__!I.A. . 7d.; BURTSRV, A.K., red.;
KORNILOY, B.I., tekhn.red.; POTAPHNKOVA, Ye.S., tekhn.red.
[Dielectric spectroscopy; recent studies onithe propskisa of
-certain ferromagnetic semiconductors and diA-ectrics: relaxotion
processes, electric conductance, losses. and the role of structural
defects. Translated articles] Dielektricheakeis spektroskopiia;
noveishie issleaovaniia evoistv nekbtorykh forromagnitnykh-polu-
provodnikov i dielaktrikov; relakestpionup protsessy, elektropro-
voanost's Poteri i roll aefektov struktury. Sbornik statei. Pod
red. G.A.Smolanskogo. Noskwaq Izd-vo inostr.lit-ry, 196o. 362 p.
,(MM 14:4)
(Spectrum analysis) (Dielectrics) (Semiconductors)

tW& *. bDOX ElPLOITATICC SOV/1079
Vosacirusnaya konf,reatslys I- fisikv diolektrik- Zd, 1951
risika dlel.~ctrikiv; trudy vtoroy voes3risnoy konferentali (Phynics of Diolutri-,
T,.hs-t1,ns of the 24 A-11-U.1- C,tf-mc. on the Physic, of
M-m, lzd.vo A SaSR, 19~0. 5]2 p. Errata slip InserteJ. 5,0D0 copies
printed.
'Ap..
, oftj-. Ae-tcy, n..k SXR. F1.zIth.sk'y L-tit.t i-1 P.M. We's
r1d, of Publisb!ng Hillsit T%.L. Sterokadmekeye, T-.h. FA.: 1,9. DcrtlahAn.; W-
torial Boordi (peep. 14.) C.I. SkansvI, D~ctor of Physics -1 11.^th-tl~s
0- .... d), and 1.7. Fil_FP__.' of Phy'le. end ?Uth.meu...
KILP03E, This colla~,tic. of r.p~rta is i.t.odd for adi-tist. lb-ItIC.-I.J
the physic, or dielectrics.
COVCRAGS~ Th. S"ccJ C~.Nlvnc, to the Phys-tv .1 D.,l._t,Ic, held in
M-ow at the F121chsskI7 Izetttut I=#1i P.I. let,.d- t?hyci~. Institute L-ni
P.R.
Lebod-) In 1953 - stt#~I~J by r.pr ....... ti,~_, of the
scientific c,.t.rg or ttwe U.13R end .1 .... -1 cth. r , -his c,,I-
lft~.ou contain. vlst of' tb* reports prosett-d at tho conference end -ribs
of the dia4usalc:ij which n9 recrIx In this collection deal with
dielectric propert4os, 1-fl, atd ;c,l&riutjon, and with q;ecific ".I.Acti-
of try,tels. ".p'-d.. am
slactrv-j, farr~1e,trt: cryatals, end -t- rel"t%an -d irr4dlatl~ of-
feet. cn dI.l,ct.!cs are j.,.stgetel, The ,l_~ list of ther
p^p-rs Nasem ed It he Coof'ron 1...... .
-4 d*ollvC with polArIcati
br-kd-ce of d141Wr1ca , hit% .,:. V.,bli.ttd it the S_,tly. 0
WSR , serlya W2. "4:,% 1q. ptra.call-., are menti.-d.
Referent,.. a.-cc%;,ny .,~ t-,crt.
G..1.7 A.I. ker.=,.k~,ya, I.A. Isupo, W'j S I. P. V.,
Q
of Ss.i ... 3~ tort
AS USSR] 339
X.22L6X-1a. Geometric Model For the Nocription of Poly=rphous Phcis
Transition. ~Cystala (Phymics Di,I,J.n, M~s.cw Stale Co~!,.r.lty J..bi
M.T. Lomono2OT) )A7
I.M. S_-jLrjj-=A_&nd Dooml, Struo-
_VM~# 'and Certain Fhjsri_xT_Pr:,pertiss of polarized Trl;lytina -ulfat* C.'7at-ls
11"tituts, of Crysts.11c,iraphy, Academy of Sciences U33R, Moscow) )51
M-A.S., end Zh.%!_- _Z-.4-Som, CrIstell.ebaulcal Problems or F.-
x "t'ric Crystla-Wi-th a Hrlrog.o Bood Clutit.t. of Cr7.t.1l.graphy, AS U31q,
. oscov] ... ..... I - - .1 )66
_Y.rb ff-t of Chromic,
L.S. Stolt,y`c.A. E.
Z-jds on the Z1,at'l rcp.-t to
on -or 372
CharnZj, BA - 6CcZrO3e System
Electrical Proportion of the B&T103
NnWf-p-~ro;'1A'i!y G-s-lexat..,vy uni-rsite. U-prop,tr.- St.t.
ty) 385
X
I.S., I.S. Raz' A.S. Socdn' V.I. Gilikly, V.M 11.%Zerl'~~ V'A-
trf.-Prop-ti.' of G_~'_'I-Al " fn-=-
(T-'.-.r. .-I. lab?r.toiy 'Yetot.k.--niki. (C,.-
tral. Scientific-Re, 1.;y~
:Irch Laboratory of P ..h.- Institute of Crystnllo-
gr.phy, AS USSR, M 393
jLnZjLk=.1-'L. and O.A. 51-jg-. L!'fect of ~S~ll Allition A~,,ntl an
1
.1 Electrical No;-ties of PolycrY3t4l B&7iO3 [Dnepro;etrovak State ~hi-
1* ity]
are
G-~-Ich. Problem of the Conoettion Between Electric
Conducti,itj of rr,;sl~~,ii~i~ Cry,talLecd F::-*a'--.r-cI.j [Central Sol-
tLf-c-Re-ch Lb.-t-y of PI-L.C l.q M.11-j 410
C--d 11/15

SIROVA, N.N., akademik, otv.red.; BELOV, K.P., prof., red.; KONDORSKIT,
Te.I.j prof,j rod.; POLIVANOV, K.M., prof., red.; ULSOIN, R.Y.,
prof., red.; SMOLENSKIT, G.A., prof., red.; SHCLITS, N.H., kand.
fiz.-mat.nauk, red.; WOLTARENKO, E.M., red.; BASHKIROV, L.A.,
red.; KHOLYAVSKIY. S., red.izd-va; VOLOKHANOVICH, I., tekhn.red.
[Ferrates; physical a 'nd physicochemical properties] Ferrity;
fizicheakie i fiziko-khimicheakie avoistva. Doklady. Minsk,
Izd-vo Akad.nauk BSSR, 196o. 655 P. (MIRA 13:11)
1. Vsesovuznoye soveshchaniye po fizike, fiziko-khimicheskim
svoystvam ferritov i fizicheskim osnovam ikh primeneniya.
2. All BSSR (for Sirota).
(Ferrates)

86444
S/181 60/002/011/032/042
Boo6 Bc6o
YB
AUTHORS: Smolenskiy, G. A., Isupov, V. A., Agranovskaya, A. I., and
Popov, S. 7~'
TITLE: Ferroelectrics With Blurred Phase Transitions
PERIODICAL: Fizika tverdogo tela, 1960, Vol. 2, No. 11, pp. 2906-2918
TEXT: This is the reproduction of a lecture delivered at the All-Union
Conference on Ferroelectricity which took place in Moscow in January, 1960.
A report was made on studies conducted on polycrystalline specimens of
ferroelectrics with blurred phase transition and belonging to the two
systems Pb(MgjjjNb2.jjO 3 -Pb(Nilh Nb,13)03and Ba(Nb, Ta )206 - Sr(Nb,Ta) 206'
These ferroelectrics exhibit a relaxation polarization in the region of
phase transition. The technique of the specimen preparation has already
been described by A. I. Agranovskaya (Ref. 6); and the method of measure-
ment in Ref. 2. Investigation results are illustrated in diagrams and are
discussed in great detail. Fig. 1 shows & and tang as functions of
temperature for Pb(Ni7h Nb,,,)O, in weak fields at frequencies between 1 and
Card I /~

86444
Ferroelectrics With Blurred Phase Transitions S/161/60/002/011/032/042
B006/BO60
1500 kc. Both curve groups exhibit a maximum between -150 and -100 0C, the
precise position and height of which is somewhat frequency-dependent. The
maximum loss angle is the larger the higher the frequency. Fig. 2 shows
the temperature dependence of E and tanS on Pb(mgl/,Nb,/,)O 3 in weak fields
at frequencies between 0.4 and 4500 kc. This compound as well exhibits
loss angle maxima, lying between -50 and OOC and which are the higher, the
higher the frequency. The E-maxima (between 9000 and 12000) are the higher,
the lower the frequency. At 0.4, 1, and 45 kc they still lie at negative
temperatures, but already at positive ones at 450, 1500, and 4500 kc. The
ascending part of the E(t) curves is frequency dependent, but not so the
dropping part. Figs- 3 and 4 show oscillograms of the hysteresis loops of
these two compounds at -90 and -1960C, respectively, taken at varying
electric field strengths (E max ~ 20 kv/cm and 60 kvlcm). Fig. 5 shows the
temperature dependence of total polarization on Pb(Mg1j,Nb2.(3)03'
Pb(Ni,I,Nb,13)0,, and solid solutions xPb(Mg,,,NVO 3 + (1-x)Pb(N~j,Nb2j3)OY
the x-values being given near the curves. Fig. 6 shows, for these speci-
mens.. the spontaneous polarization as a temperature function, Fig. 7 the
Card 4~

86452
S/181/60/002/011/042/042
B006/BO60
AUTHORS: Smo G. A. Isupov ` V. A., Agranovskaya, A. I.,
3~Ln ~Krayvnl
TITLE: New Ferroelectrics of a Complicated Composition. IV
PERIODICAL: Fizika tverdogo tela, 1960., Vol. 2, No, 11, pp. 2982-2985
TEXT: This is a report en the discovery of now perovskite-t e ferro-
electrics, which may be described by the empirical formulas YrB 11 0 5Na 0 51. r1o3
and[Bi 0-5y'0-51 TiO 3' The Curie temperatures of these compounds ar; 3206
and 3800C, respectively. The compounds were prepared by mixing the initial
substances Bi 203' TiO 2'K2CO,, and Na 2CO .3 in a stoichiometric ratio, and
by sintering them in the air at 1120-1140 (Bi,-Na) and !0600C (Bi-K) for
an half an hour to two hours, The pe.-ovski4te structure of the compounds
thus obtained was established by X--ray.-. The parameters of the elementary
cells of the two compounds were found to be a = 3.88 and 3.94 A,
respectively,. In the said compounds. the authors determined ~, tang
7~
Card 1 /10

864-52
New Ferroelectrics of a Complicated
Composition, IV
S/181/'60/002/011/042/042
BOO6/Bo6o
the relative longitudinal expansion 61/11 and the coefficient of linear
expansionr~ as temperature functicris, Results are shown in Figs. 1 and
2~ A study of polarization revealed that sodi_um bismuth titanate has a
well-shaped almost rectangular hysteresis loop, whereas that of potassium
bismuth titanate is far from 8aturation, The first mentioned compound has
at '1160C a spontaneous polarizatiofi Of 8.,Opcoul/cM2 and a coercive force
of 14 kv/cm., It was further establ;shed that a1sc INa 0.5 BiO.5]Zr 03
and [K O~5 Bio. 51 ZrO3havE U perovskite-type crystallization, There are 2
figures and 18 referencesi 15 Soviet, ! US, and 2 British.
ASSOCIATION: Institut poluprovodnikov AN SSSR, Leningrad (institute of
Semiconductors of the AS USSR, Leningrad)
SUBMITTED: June 30, 1960

20151
j,q3oo ~akd 1/47) //Sy 1"5-9) S/181/61/003/002/049/050
B102/B201
AUTHORS: Smolenskiy, G. A,, ChanC Tsung. and Stankevich, A~ K
TITLE: Effect of electron diffusion upon the radio-frequency
dispersion of the magnetic permeability- of garnet-type
ferrites
PERIODICAL: Fizika tverdogo tela, v. 3. no. 2, 7961, 663-667
TEXT: In weak electric and ma-netic fields.. certain ferrites display relma-
tion processes which are correlated with electron diffusion. The mechanism
of these relaxation processes has never been fully clarified so far. In
this connection, a study was made of the complex magnetic permeability and
the complex dielectric constant, as well as of the dielectric and semicon-
ductor properties (the latter were studied by Ya. M., Ksendzov and V~ A. Sto-
gova). Concerning the study of the dispersion of the magnetic permeability
a report has already been given at the 3rd All-Union Conference concerned
with physics, the physicochemical properties of ferrites, and the physical
bases of their application (June, 1959. Minsk) The polycrystalline spec-
imens were prepared by the usual ceramic technique, using analytically pure
Card 14 5,

20151
05C
S/18 61/003/002/040/1j,,~
Effect of electron ... B102Y3201
10 6 and 107 ohm-cm. *Vfhen the specimens were heated in oxygen current, the.
2-. ity inc~_eased. Fig. 2
concentration of Fe ions was reduced, and resistiv
_sl,ows the frequency dependence of ~L' and ~Pl at room temperature and H~,I moe
14
of polycrystal ~ne specimens prior to (curves I and 11) and after (2, 21)
xy vas added to some
~heatinE; in o. -,e'n current (15 hr at 10000C). 1-2~,, of CuO
1'e. of 'he specimens (curves 3 and 3) , their 'resistivi-ty ranged bet~,.reen
10 11
10 and 10 ohm-cm at room temperature; similar results were ob-tained on
specimens with 1 -25'0 Mn 203 addition (4, 4'). For a comparison, Fig. 2 shows ,
moreover, the frequency dependence of g' of single crystals (curve 5). The
single crystals had a resistivity of 10 12 ohm-cm. A study of the three
abovementioned solid solutions showed that PI is reduced with increasing A131-
concentration, and that the maximum of P" is shifted toward higher frequen-
cies. The iIntroduction of Cr3+ increases pl. The magnetic and electric
spectra (i.e., pl(f) and V(f)) of the ferrites investicated have a similar
course. in all cases where there arises electron diffusion,. p' and El at-
'high values at small frequencies. A final clari, ct
fication of the effe
o`L' electron diffusion upon the dispersion of magnetic permeability requires
further studies. V. A. Iof-Pe, A. G. Gurevich, and i. Ye. Gubler are men-
Card 3A5

20151
S/181/61/003/002/049/050
Effect of electron B102/3201
tioned. -There are 2 figures and 8 references: 5 Soviet-bloc and 2 non-
Soviet-bloc.
A330CIATION: Institut poluprovoanikov All SSSR LeninGrad (institute of Semi-
conductors of the AS USSR, Leningrad)
SU3MITTED: September 3, 19601001
Fig. 1
Card 411

20796
s/161/61/003/003/022/030
3 0 0 3 6 j /I VS1- /I V71 //5 B102/B205
AUTHORS: Smolenskiy, G. A., Isupov, V. A., and Agranovskaya, A. I.
TITLE: Laminated ferroelectrics of the oxygen-octahedron type
PERIODICAL: Fizika tverdogo tela, v. 3, no. 3, 1961, 695-901
TEXT: In an earlier paper (Ref. 1: FTT, 1, 1, 169, 1959), the authors have
uttered the opinion that compounds of the general formula ABi 2B20 9
(A - Ca 2+ ) Sr 2+ , Ba 2+ , Pb 2+ , Bi 3+ ; B = T14+, NO+, Ta5+) have ferroelectric
properties. Now they report on the proof of these properties and the
manufacture of the new group of ferroelectrics. In the lattice of these
compounds, perovskite-type layers (AB 207 )2- consisting of BO 6 octahedra
alternate with 1( Bi202)2 Ix layers. Such crystals have face-centered,
orthorhombic unit cells which, in first approximation, are considered to be
body-centered tetragonal cells. The specimens (8_1 0 mm diameter, 0.5-2 mm
thickness) were made of powdered oxides or salts of the corresponding metals:
PbO, SrCO 37 BaCO 31 Bi203 trade-marked "Ma" (pro analysi), CaCO,V TiO 2
Card 1_4*
/_7

20796
S/i 81/61, 100310031022103C
Laminated ferroelectrics ... B102/B205
trade-marked 0411 (pure), Nb2 05 (containing Nb 99.4%, Ta 0.2~6, Fe m6%,
Si 0.04%), and Ta 0 (TiO < 0-*25%-, Fe,O 0.18%). The specimens were pres-
2 5 2 C_ 3
sed from the Dowder mixtures, heated to 7000C (for 4 hr) in air, again
powdered and heated to temperatures which are listed in Table I (holding
time: 1 hr). The losses in weight (in lead and bismuth oxides) are given
in %. The X-ray structural analysis was carried out by I. G. Ismailzade,,
The temperature dependence of the initial values of F, for some of the
compounds is shown in Figs. 2 and 3; the course of E(T) on heating and
cooling is shown for PbBi 2Nb 209* tan 6 of these compounds at 1 kc and room
temperature was equal to 0.01. It is seen that some compounds show a
monotonic increase of 6 without an extramim1while other compounds have broad
or sharp maxima. The highest value of E is reached by BaBi 4Ti4015- Fig- 4
shows the temperature dependence of 6 and tan 6 of the solid solutions
(Pb 1-x BaX)Bi2Nb209 at 1 kc, and of the compound BaBi2Nb20 9 at I kc (contin-
uous line) and 450 kc (broken line). The figures beside the curves are
the values of x. Fig. 5 shows the x-dependence of the temperature at which
Card

S/181/61/003/003/022/030
Laminated ferroelectrics B102/B205
Creaches its maximum for (Pb I-X Bax)Bi2Nb209at 1kc (1) and 450 kc (2), ~.nd
for (Pb I-x Srx)Bi2Nb209at 500 kc (3)- 'The chemical composition (1) and the
temperatures of the phase transition (2) of niobates (a), tantalates (b),
and titanates (c) studied are listed in Tables 2 and *3- It may be seen that
all compounds of the new group of ferroelectrics have a comparatively high
phase-transition temperature. This fact is attributed to the presence of
Bi 3+ ions. Concerning the selection of the ions A and B, it is necessary
to follow the instruction given in Ref. 8 (G. A. Smolenskiy and A. I.
Agranovskaya, FTT, I, lo, 1562, 1959) for the manufacture of such ferro-
electrics. The fact that the radii of the.ions A 2+ and B13+ vary consider-
ably is held responsible for the disturbance of the arrangement of the ca
tions forming the compound CaBi Nb 0 in several compounds with a lamini~at;d
2 2 9
structure. This explains the width of the phase transition (blurredness)
and the occurrence of relaxation polarization in BaBi 2Nb209' There are
5 figures, 3 tables, and 8 references: 7 Soviet-bloc and I non-Soviet-bloc.
Card 3 41

20901
S/1811/61/003/00--/028/030
6 B102/3205
AUTHORS: Smolenskiy, G. A., Kraynik, N. N., and Agranovskaya, A. I.
TITLE: Antiferroelectric properties of some solid solutions on the
basis of PbMg 1/2W1/203
PERIODICAL: Pizika tverdogo tela, v. 3, no. 3, 1961, 961-990
TEXT: Antiferroelectrics of the perovskite type have so individual proper-
ties that no "typical" compound (such as BaTiO 3 in the group of ferroelec-
trios) can be found. When investigating antiferroelectric effects, it is
therefore necessary to compare the properties of solid solutions.
with various antiferroelectrics as basic material. One of the most
important problems in the field of antiferroelectrics is the stability of
the ferroelectric and the antiferroelectric phases. A study has now been
made of this problem with the aid of the new antiferroelectric
PbMg 1/2W1/20 31 and the effect of a substitution of the ions A or B in this
compound has been studied (A denotes the ions contained in Derovskite-type
lattices ABO 31 in sites with the coordination number 12, and B denotes the
Card 1/8

2C801
S/181/61/003/003/028/030
Antiferroelectric properties B102/B205
basis of PbZrO3 and NaNbO 3' 2) Solid solutions with BaMg 1/2W1/203and
CaMg1/2 W1/203showed no ferroelectric phase. A new, obviously antiferro-
electric phase appears in solid solutions with CaMg1/2W1/203' 3) In the
antiferroelectric phase of solid solutions with PbTiO3 and PbMgl/, Nb2/3'3
at a concentration of the second component of 5-7 and 20-2y/., respectively,
a forced phase transition into the ferroelectric phase, occurs in a strong
electric field. The critical field within which this phase transition
occurs, increases with a rise in temperature. 4) In solid solutions on the
basis of PbMgl/2WJ/203' the phase transition from the antiferroelectric
into the paraelectric phase is accompanied by a reduction in volume. Thus,
the occurrence of the antiferroelectric state may give rise to a reduction
in volume of the primary unit cell (solid solution on the basis of PbZrO 3)
or an increase in volume (solid solution on the basis of PbMgj/2W1/20 3)
as compared to the paraelectric state, 5) Certain compositions of solutions
with PbTiO3 and PbMg 113 Nb2/3'3 show both ferroelectric and relaxative
properties. 6) Experimental data on the relative stability of the ferro-
Card 3/0

S
TITLE
P F R LO D A
t 11,1
n
n F- e
TEXT,
1, U t ed by
of d r e
fa! S th e
j()f S titc, tIr'.1-
t ,
x n b i t ed
":)n S 1, 24,
s.,) b ish e d Sa'
b e c s a ccl ~empera-uure ar"
~1.c I Mt m the. t ~ne
bAlity~ a
-e
1 e ed
polycrystall !11e S 21P n ue d
p ap-
ti 'i r~i ~-;lk The -authors c)f t ht! e s'~'n
ri --; ~) Z r, or Cd
f I ~i~-riOU S ,:; 0 Lq,,:, C, U n d s s,"'stem
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an
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F
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e ~t I L M I S l' E! 0
x x 2 111x I i "5 1 "-
-1 jA ort t i n uou 6 r t) s, Al I i s c. I t o r. -
F, 'o 44
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lyz e T i Z r
2x
i cin t i )n f(jr x
SI,
e rl
lit
r:: Lit 1 t'l 1'0 ii Tl 1 -1 t IiL I
L'M I ~tf Cj J e 3 ;--3 fl-C Ni I
t firl s for t he rodu c t rl i f f ex e I-- f: A
gI t j~ im, e4el 1
o e ~i !I -w? t 'b 1 T h E-;f r ma t o ri o
n -va i c a y 1 A Ir
i ,T, e T h -2 -p
1Y
r m, e b ri!~"-- az:
11 f Th 'inn,-% t b;~, ex
~.T
rr, d U h,~
se f a I ris v a j t e
Z

S/181 61/003/006/020/631 -A
24923
~!errimagnetic materials with.v.. B102 B201
zt,
been sh'bvn by studies of e temperature dependence of v0, that the 7N
maximum' value of 110 rinen wi~~`,itha oontent of diamaanctic ionn. The.
NP
consequence
q','~;,Authors. believe that an-if) txopy
wit 0 and magnetootriotion drop in
'
'3'
.
~ X;

"M -

I
.
4- -. .
4
I . - , ~
i.- f a'diminution of the.content~of magneticallyaclive iona. The value of
d
F. ~4 . i etermined by shifts o the domain boundariea. K. P. Belov and

N

5
At: Pom f f re, 'I table, and 6 refer-
enko are mentioned, There are 1 gu
"U
"
',
no e a a -bloc. The -reference to the
5 Soviet-bloc and 1 noh Sovi
--e.- Engl i'sh-lan guage publication rea a as
d follow a ~S.
Geller-J. Appl. Phys
.
1960

polu~~rovodnikov AN SSSR Lening~ad (Institute 'of

Semiconductors AS ttSSI
R, Leningrad)

SUBMITTED January 17, 1961
'
l Id.
-~,to the Table -"I cont ent."of second component. in mo
e 2, last

/cm3 m4ximum temps.rature; 5, holding
3, density in g 4,
ime in,hours;.'6,,apparent density; 7,,density in %,of theoretical values;'

f ".t '20*0 and f 04
.,
Y p0 Cps Y-
'
a
d 3/

t
,
.

2 q, ?goo 30060
S/048/61/025/011/004/03' 1
2 L1,920D B108/B 158
AUTHORS~ Smo.lens-kliy, 1supov, V, A., Kraynik, N, N., and
Agranovskaya, A---i-
TITLE, Coexistence of the ferroelectric and ferrimagnetic states
PERIODNAL, Akademiya nauk SSSR. Izvestuiya. Seriya 'Lizicheskaya,
v. 25, no~ 11~ !961, 1333-1339
TEXT; This paper was read at the Conference on ferromagnetism and anti-
ferromagnetism in Leningrad, May 5-11, 1961, The authdrs studied substances
having both ferroelectric and ferromagnetic or antiferromagnetic prcuerties.
Among the crystals known so far only the perovskite-type structures include
greater number of ferroelectrics and substances with magnetic ordering,
,
a , 0
If a perov,skite-type crystal AB03 contains a definite concentration of 'ions
of transition elements with non-compensated spins, magnetic ordering may
arise Ferromagnetic properties will arise when the A and B ions have high VY
polarizability. In perovskite-type crystals, ferrimagnetism may be
achieved by a certain ordering of the ions in the B sublattice in solid
solutions. The latter are assumed to have the structure
I
Card 1/~'/I

30C.60
S/048//61/025/011/004/03';
Coexistence of the ferroelectric and... B108/B136
(I - x)AIBIO 3 - xA"B Oo5 PIBO ; 5'1103 where the first compound is antiferro-
magnetic and the second paramagnetic. x denotes the concentration of the
serond component (mole per cent), The saturation magnetic moment of one
ABO3 unit is calculated under the assumption that the exchange interaction
w1thin the B sublattices may be neglected. It was found as
m 0. 5(m, - mjI') 5 1(m' x) ~m"xl[l - E(k ml X) II - E(k
~0' L
m and m ii are the magnetic moments of sublattices 1. 11, respectively,
m~ and m" the moments of the ions BI and B", k I and k Ii the contributions
of nonmagnetic ions to the overall ion number in the sublattices I and 11,
5 6 -,
E(k) =6k . 5k Is the probability that a magnetic ion in one of the
sublattices has not more than one nearest neighbor among the magnetic ions
in the at),.er sublattice, In the considered case, k I =0 and k IC x In
particular the authors studied the solid solution
)0 xPb(Mg )0:~ -Ahich was obtained by sinter,-ng
2/5W'/3 3 - 1 /2 WI; /2 _;
the oxidn4 at 900-92c)!~;,~- lay phase :~nalvses were carried out by
arq