SCIENTIFIC ABSTRACT V.I. CHECHERNIKOV - Y.S. CHECHET

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000308220018-7
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 12, 2000
• Sequence Number: 18
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

'36603
/u L, S
/126/62/013/003/019/023

E039/El35

AUTHOR: Checherpikov,

TITLE: The
magnetic susceptibility of the rare-earth metals.

Ho, Dys Tb and Gd

PERIOD
ICAL: Fiiika metal;ov i metallovedeniye, V-13, no-3, 1962,

,
458-46o

TEXT; The study of the magnetic properties of the rare

earth~metalz is of interest inasmuch as the magnetic effects of

the
electrons lin the 4f-shell are well screened by external

electrons
from the.influence of other atoms. Previous

investig~ttions-have been
limited mainly to the low temperature

region. This paper describes the
results of an investigation of"

the temperature dependence of the
magnet~lc ounceptibility of the

polycrystalline metals Ho, Dy, Tb and
Gd in the temperature

range 300-1500 OK. The metali were 99.5% pure
and their magnetic

susceptibility was measured in an apparatus based
on the

~araday-Sixsmith method. The apparatus was calibrated by means

of electrolytic Ni and a NI-Al alloy (5 wt.% Al) for which the

Card
1/3

D

S/126/62/013/003/019/023
The magnetic susceptibility of ...
E039/E135
data are well known. It in shown that the metal Ho follows the
Curie-Weiss law over the whole t',emperature range iuve~tigated.
This agrees with the results of other authors. From this are
obtained values for the Curie temperature (88 OK) and the
effective magnetic moment (Pj = 1o.6 In the case of Dy
there is a slight deviation from the Curie-Weiss law at
temperatures over goo OC. Its Curie temperature is 148 OK.
Gd, which is ferromagnetic, is studied near to its Curie
temperature'(17 OC) and it in found that there is no transition
region at the ferromagnetic transformAtion point. Gd obeys the
Curie-Weiss law for temperatures between 300 and 650 OK. Of the
metals investigated only Ho followed the Curie-Weiss law over
the whole temperature range 300-1300 OK; the others deviated at
h:Lgh temperatures. This may be qualitatively explained by the
theory of Van-Fleck which suggests -that the magnetle
susceptibility has two components, one of which in temperature-
dependent and the. other, a high frequency term, which is not.
There are 3 figures.
Card 2/3

The magnetic susceptibility of S/126/62/013/003/019/023
E03,19/E135
.,ASSOCIATION: h'6zkovskiy gosudarstvennyy universitet.imeni
M.V. Lomonosova
(Moscow State University imeni M.V. Lomonozov)
SUBMITTED: july 8, 1961

lumestigation of nickelWaftlum forrites In the transition
region. VestJb&kvn.S*r.3.Fiz.vastrOj. 17 no.2t2O.23 Mr-4p,
162, (MM 16 s2)
1. Kafedra siagmetismia NDskovskogo, univeralteta.
(Ferrates-4bgnetic proportion)

3709%/056/62/04 2/004/005/037
1?4 B1 02/t1 04
ADTHOR: Chechernikov, V. I.
TITLE: Anti~erromagnetism of iron-nickel alloys
PERIODICAL: Zhurnal elcaperimentallnoy i teoreticheskoy fiziki, v-
42,
no- 4, 19629 956-958
TEXT: The temperature dependence of the paramagnetic susceptibility
t of
Fe-Ni alloys was measured at T>Qf (of - ferromagnetic Curie point)
with
specimens containing 4-7) MY 14-4, 19-3, 27, 29, 30-9, 34.9, and
36.84.
Ni. Special attention was paid to the y-phase of these alloys. The
susceptibility measurementa were made in the range 300-15000K by the
Faraday-Sucksmith method in an argon atmosphere. The curves 11X, -
f(T)
of the specimens with 27, 29, and 30. Va show a step which is
indicative
of an ar,?y transition. The 2V alloy has the highest step (at 82&K).
k of the 34-9 and 38.8% alloys satisfies the Curie-Wei8 law in the
whole
temperature range (no phase transition). Of the lower alloyed
specimens
only the y-phase was investigated; 1/7L - f(T) is a straight line.
Also
the magnetic moments P and the paramagnetic Curie points 9 of the
Card 1/2 P . P

S/05 2/042/004/005/037
Antiferromagnetism of iron-nickel ... B102YB'104
y-phases were measured, depending on the Ni-content. PP of
alloys with
more than 500/16 Ni decreases linearly with increasing
Ni-content. OP is a
non-linear function of the Ni-content. It has a broad maximum at
about
601jl~ Ni; in the range 30-4Vt'o it decreases rapidly, and at
20% Ni it changes
its sign, i.e. the y-phase of the alloys with less than 20i". Ni
and also
the phase of iron have a negative paramagnetic Curie point. This
is due
to the fact that, because of the negative exchange interaction
between
the iron atoms in the y-phase, the number of antiparallel spins
increases.
By extrapolating to pure iron, F P - 7-4 and Op a -30000K is
obtained.
This agiees with the Sucksmith-Pearce results (Proo. Roy. Boo.
A167P 189,
1938). 'The result that,in the I-phase at 4 2011 Ni, negati,/e
exchange
interaction occurs is in agreement with the theory of Ye. I.
Kondorskiy.
There are 3 figures.
kSSOCIATION: Moskovskiy gosudarstvennyy universitet (,Moscow
State
University)
SUBMITTED: November 4, 1961
Card 2/2

3948o
S/01!6 1652/U3/~02/3 /053
')3104
10 v
3
AUTI-10,28 Chechernikov, V.__ Afonina, L. N.
13 TTv Antiferroma,-netic pro-jerties of the gamz:ia ohaue of 2a
an
Fe-Co alloys
?ER 10DICAL: Zhurnal eics-3erirent-allnoy i teoretichesiro'- i z
V.
no. 2(8), lcl;62, 429-431
TEXT: The teriperatire dependence 'X(T) of the susce--)tibility
of 1e-111tiand Pe-Co.corkta-Lning- 3.08, 4.80, 6.066, 8.71,
10-90', 13-30, 22-70,
and 30.00 at;;'~ Pt-, and 5.1, 106.2, 25.0, and 34-9 at'/;tO Co
-aas investi3a-Led t-,
-P a "latent" antiferromagnetism in'the gamma phases
prove the presence o-
assumed by Ye. 1. Kondo-zski and V. 11. Sedov (Zh!:T-F, 35, 1579,
1953)
2de-NTi alloys. )C(T) of each of the alloys was measured -in the
rankle
S50-15000K uhere both groups of alloys show a linear course of
1/-/, f (T)
The parama8netic Curie -poi'it (G P ) and the af"fective magnetic
moment ? ue:~-a
also --ensured in each case. In alloys containing Pt e- 14 at"'i
and Co < 106 at','.
0 is less than 0. P drops slizhtly with increasing percentalge of
IFt or
P P
Card 1/2

Vo 5 0/0 53
Bl D2/
Antife.-roma8netic PrOpOrties Of 'he ... 3104
Co. Por e.c. pe+3.08 at,/l'o Pt, 1? =06.26 g. and 9,,- -1500-1--i.
There are
p
3 fi-frures.
ASSOCIATION: Yoskovskiy osudarstvennyy universitet State
University)
SUBMITTED: 1..Iarch 1,/*, 1962
FROP6~eL Y)6,ucul-q
Card 2/2

HERNIKOV VU:k ano_ ich, red.;
CHNG vj~7yich; KONDORSKIY, Ye.I.,, prof.,
.A. A
~--M-Z ", - . r
ORSEVA. C i6d.; CHISTYAKOVA, K.S.,, tekhn.red.
[magnetic measurements] Magnitzwe izmereniia. Pod
red.
B.I.Kondorskogo. Moskva, Izd-vo Mosk. univ,, 1963.
284 P.
MIRA 17:3)

5162
S/198/63/000/001/003/014
B104/B102-
'AUTHORBs Chechernikov, V.,Ieg Lyubiitin, 10 -5.
TITLE: The temperature dependencevf the,magnetic susceptibility and
of resonance absorption in Cr 03,.-*no,a~md Nio
2
PERIDDICALt Moscowe Universitet.. Vestnik.; Soriya III. Fitika,
astronomiya;, no.,.1, 1963., 20 23
T.T,,XT:Astudy was-mad~ of the temperature-dependence of the
magnetic sus-',~:
c4ptibil-ity (100 - 13000K) and of the resonance absorption (3,.!-qp
range)
in
the polycrystalline an',;iferromagnetic compounds Cr 0 MnO, and NiO.
The
2 39
samples made available by R. Z. Levitin were of 1 mm diameter and 3.
mm
high. Measurements were made in an argon itmosphere.. The magnetic
Bus-
ceptibility of Cr 0 has a sharp.maximum at 3140K; that,of NiO a ~rosd
2 3
maximum at 640 OK. The lower thatemperature'lies uider the antiferro-
magnetic Curie point (Q f OK) the strongoz~is the dependence of the,
susceptibility of Cr 0 on.the magnetic field. For T > 9 the
suicepti-'-.'.:
213 af
bility decreases with increasing tempqrature; this dependence is less
Card 1/3

Y
S/188 63/000/001/003/Ofl4
YB
The temperature dependenceof the ... B104 B102
pronounced in the ferromagnetic region. The susceptibility of NiO
decream
with increasing field strength. This is explained as due to the
existence-,,
of ferromagnetic impurities. The susceptibility is independent of the
field strength only above 1040 OK. It in assumed that 9 of Cr 0 is 4n-
af 2 3
dependent of the magnetic field strength and that,Q of NiO becomes
lower.'
af
with increasing field strength. Study of the temperature dependence'of
the..
susceptibility in the paramagnetic region shows that the Curie-Weiss
law ii~',
-valid. The paramagnetic Curie point, the Curie-Weiss constant and the
magnetic moment (Table) are determinede Por tomperatur9s below 0 the
af
stant value. The
resonance absorption of Cr 0 falls steeply to a con
2 3
decrease of the resonance absorption of MnO'begins already-in the para-
magnetic region. The half-width,of the resonance absorption in CrO
re---;,.
3
mains constant in the paramagnetic-'region; it rises steeply at 0
MnO...
af
shows similar behavior. The following values were obtained for the
g-factors: g 1.87 (Cr 0 and g 1.90 (MnO). There.are 4 figures and
2 3
1 table.

i/188/63/000/001/003/01

The temperature dependence of the

BIOJJ~102

ASSOCIATIONs Kafedra
magnetimma

(Depprtment of Magnetism)

SUKiITTED:
May 8,
1962

Table. Paramagnetic

Curie point

(0
p
0 0
K).1 9 K; Curie-Weied constant;'
&f

magnetic moment.

-~

Table

60., K

O;r !K
-C. rpm
-PA Ij,

Ii
4510

-2m

314
3
4
2
2

Sa
-
7

-

640
8
5
4.

ADO

-227

1220

06
3. 4.9B

dard 3/3

L 18327-63 EwP(q)/zw(m09Ds AFprc/AsD JD/JG
4 (0126)
E-M-9 C 9 N R AP3002854
AMORSt Cbechirni)=T, V. To;_Pop# Tulin,
ITTM -Relation of tesperaft" to paramagnetic suseeptibility ot
-Od-T-alloys
lovedeniye# v. 15 no. 6, 1963 19-4
OURCEs FizlkR metallow I metal 13V
IOPTC TAGS: Gd-Y alley, magnetic property.. electron structure
ABSTRAM The Gd-Y alloys with a general compositions 25. 509 65j 75
and 90. 6t.%
ied at temmratures of j00-1500K.I~q These samples were chosen becaime
tr
they form a continuous series of solid solutions In the whole
interval of e0neen
tion,and they have the some hexagonal close-spaced lattice. The
purpose was to-
Investiff ate the magnetic properties, the electron structure and the
nRture of the
Interaction between these rare-earth metals which have an open
4f-shell. The
.results sh3wed that the reciprocnl of the specific suiceptibility
followed the
Curie-Weiss law Rlonp, the whole temperature interval of the
investigation, i.e., it
had a linear* relatton to temperature. The effective magnetic moments
per alloy,~.
atom and per Gd-atom as wall as the pnrnnagnetio Curie points were
calculated on the'
basis 'of these dhta. The increase in yttrium content caused a sudden
drop in the
Curie point and a decrease in the effective moment of the alloy. The
authors
ic

L 18527-63
ACCEMCK WRt 03002854
conclude that a gradual change in. Gd-Y magnetic Weperties occurs
with the Increase
in yttritm content. 'The gadolinium atom may be regarded an being In
afree state
the ancy. rts, magnetic properties are determined basically by the
spine of
electrons located in the 0-shell. Orig. art. beat 2 figures
IASSOCTAITCRt Voskovs)dy gosudaretwenny*y wilversitet In. M. V.
lazonosova (Noscow
IStats Univer
SUBMT72M MoY62 DAIS ACQs 23J0163 INCLS 00
SUB CME: IAL NO REP SOFs 001 OTMRs- 006
2/2

CHECHFM4IKOV V I. BUROV, I.V. ; SAVITSM, le.He
Magnetic properties in tho system iron - gadolfiniuva- Fiz.
int.
i metalloved. 16 no.3:324-328 S~ 163. (NIRA 16:22)
1. Moskovskiy gesudarstvamiy universitat imni Iomermava i
Institut wtallurgii iwni A.A,,Baykova*

CHECHERNIKOV, V.I.; KASHLINSKIY, A.I.
Temperature dependence of resonance absorption in
nickel-zinc
ferrites. Vest. Moak. un. Ser. 3.-Fis., astron. 18
no.5:49-53
S-0 163. (MIRA 16:10)
1. Kafedra magnatizma Moskovskago gosudarstvennogo
universiteta.

ICHUNIM V.I.& IULIU FOFj HAUNKINp 0J.; TERMOVA, V.F.
===A-:m~ -
Mapetic proportion of ocaudium. 2b=. eksp. i toor,
fize 44
no.1 J67-389 Ja 263. (MM 1635)
1, Moskovskiy g9sudarstyemW universitet J., ~Wtitut
mtanurgii
AN M& I (Swadiuw-YAgn9tic properties)I

CUCHERNIKOV" Me;
Some magnetic properties of gadolinium single
crystals. Zhuro
Wwp& i teor. fize 45 no.4 :867-869 0 163. (KMA 16:11)
la Moskovskiy gosudarstvennyy universitete

CHERNIKOVI V. I. land POP, I.,
Nagnetic Properties of Some d- and f-Metals."
report presebted at the Symposium on Ferroelectricity and
Ferromagnetism,
Leningrad, 30 May-5 June 1963.,

paramagnetism of the Curie-Weiss type* Orig. art. has: 6 figures.
COM

Lj~96 ~,Z5 DIT(M))Fod~~~)/i~~id)/EWP~(t)/EWP(b) ID -0
OAV JDIJGIMLk
0)dF
ACCESSION NR: AT4048695 ?I MOO 0'0_9jSR/j'8 070
00W
'the op I Nau kIn,:O. P.
AUT MR;. chernikov,, V~ I.., V M
TITLE: Magnetic of.monocrystal1ine and polycrystalline 5candium
SOUAC.Ei., :Vsesoyuznoye soveshchantye ~o;splavam redKikh metallov,
Iq630'V'oprosY--'-
An
teori-i-~F-primeneniya. redkozemel y*kh-metal 4ov- -(Problems
Jn-the-thwor-y-and-use Z
rare-carih.metals);.Maieeial'y*-'~oveshthanlya. Moscow, lzd-vo Nauka,
1964,..67-70,
:TOPIC TAGS I seandium, d
noo ymium, scandlum single crystal, polycryst0line licandiumo
scandium'magnetic property
.:ABSTRACT, The.magnetic.propprti6sof most paramagnetic transition
metals havelbeen
studied in detail over a wide temperature range. Scandium, however,
has not been
-:-due to the difficulty of obtai
tested -for magnetic properties, ning pure scandium.
Investigations of the magnetic-prop rties of scandium will provide
important in
e
formation on the degree of localization of d-electrons and the
distribution of
electrondensity in the Iattice.- In the present.work, the magnetic
susceptibility
'was measure in a vacuum between 77 a-d )IOOK by the Faraday-Seksmit
method, in:
d n
which the force acti n9 on the sample Is measured.by a thin elastic
ring made of
beryllium brohze. Two reflectors are placed on the ring and a light
beam is re-
from the first reflector onto the second and into a cathetometer.
-Deflec-

L 14963-6 . ... ..
..ACCESS I ON NR: :AT4o. 8
4 695
IF them r n accur acy .of 0 00). mm Si nce sca
~t ion o* ay. i s determined. W th'. a ndium i s a
-M is p: I a,y-, an
'd -important role -Tests show that-lncreas-~
weakly agnetic.met6lj:a mixture
-;in the'metal purity changes the Magnetic'moment from 1.65 to 1.42,
while the
paramagnet i c Curie point-changes from-080"Ito'._700K. The Curie
point was negative
for all samples. it is possible,- therefore, that scandium' shows an
antiferrite
'exc ange ow er,
h interaction- H e4 thls'~requlres further testing at lower
temperatures.-
No investigations have-been re orted.on.the:.magnetic properties of
monocrystalline
P
so
since it.ls very difficult to obtain scandium single crystal
e jo wa on e vacuume:
~In the Or sent work this sA e by r crystallization annealing in a
high.
:This,method results in,the -lowest quantity of admixtures. The
sample of mono-
crystalline scandium was.placed-in a holder-in such a way that the
magnetic.field
wa's directed either parallel o perpendicular to the c.axis.
The.temperature
r
~dependenca of magnetic susceptibility was-investigated in both of
these directions..
-The tests,showed that,the-mmignetic,sus6e tibility wac higher in a
parallel field
P
than in a,perpendicuiar field*, This,sh6ws that the magnetic moments~
are oriented-
* t
_C ' 1300K in the parallel magnetic field and
aj,ong the c.axis... The urI6.poln was
-900K in the perpendicularfielA. Similar relationships betweenthe
Curie points
of monocrystalline,and polycrystalline scandium were obtained with
neodymium b
Y
D. R..Behrend, S. Le9vold and F. H. Spedding They also found that
neodymium was
antiferromaqnetic~at Io'w temperatures.-Orig: art. has: 3 figures and
i table,
Card
2/3~

PDP, IuliuL-Cq~I,Xovf- V.I.
Pendulum type magnetic balance with mechanical
compensation.
Prib. i tekh. eksp. 9 no-5:180-182 S-0 164. (MIRA
17:12)
1. Fizicheskiy fakulltet Moskovskogo gosudarstvennogo
universiteta.

ACCESSION.MRs AP4034069 8/0126/64/017/04/b636/0638'~
AVMORSs Chechernikay, V* Iol Pop, Iuliu
TITLEt Antikerracametism. in Ni-Cr alloy's
SOURCEs Fizika metallov L metallovedenlyeg ve 179 no- 4. 19649
636-638
TOPIC TAGS: antiferromagnetimp nickel alloys chromium alloy,
smanetio
susceptibility# temperature dependence
~.,ABSTRACTs An wMerizental study was carried out an the
temperature dependence of
~the paramagnetic susceptibility )C of Ni-Cr alloyaq which
contained 3-4t 5-0t 8-75"
11.1 at. % of Cr (hereafter referred to an 19 29 39 and 4
respectively).. For
cast samples the curves of IM as a function of temperature T for I
and 2 increased
linearly up to about 10OOK and satisfied the Curie-Weise'Aaw in the
form
x=. + i where W is the texperature-independent part of the
sunceptibiliii
k
C -is the Curie-Veins oanstantq and 9 Is the taqwature of the
paramagnetic Curie
p
P
int. Curves for the cast.woples of 3 and 4 were definitely nonlinear
0 and.
followed more closely the KAI law I I " T` For arnealod. Miles au
rard 1A

'ACCESSION MRs AP4034069
the curves satisfied the 141 law for T above 500-650K. At lower
temperatures the
dependenoe of the eumooptibility on the magnetio field intensity
predoninsIted,
,Ebtporimental values for the parameters occurring in the above
equations are given
..for each curve. Neutron diffraction studies show tb&t for Ni-Cr
alloys in this
,region of Cr conoentration the mastic moments of the chromium and
nickel ALtoms
are oriented antiparallel. Consequntlyp it is conoluded that strong
antiferro-
magnetio exchange Interactione wdst for this systems Orige arte
base *2 oquationst
-3 diagrams, and I toble.
ASSOCIATIONs Moskovskly gosvidarobvenV*1 universitet Im.
Lomomosovs, (Noioow State
Phiver
sity)
'SMKXT=s 20W3 IMCLS
00~1-
CMER 110 3W BOVI 0014
Oln=$
/*
7

ft wYi w
C S10126/64/018/0'33/0369/0367
C"ESSION .,NR, AP4046089
A
P
rniko
AUTHOR.
V,
TITLE: Magneile pr'opertie~j Of-. gmolinitrio-cerlwi alloys
SOURCE -I"zik no.. 3, ~1964 363-367
I a metallov- i rnetallo'Vedeniye, v. 18,
TOPIC TAGS: xi~agni tic aE~,r~ "s gadolin'lum corlurn alloy, ~ij
a-ra m a g z i e t i e rrvj-_~- r-y s' Curie Weiss, la'w
-na
ABSTRACT: - The authors haveylli vesitig'ated.the -maganetic prope
rties~of effloys of
7-177
t Ic- gaaollnluln-~:Cerium tern:X Mtie Tcr~y"Illwe-st-m la-'
on the relative a' uunts~of Gd'ainid Ce,:~andltheir magnetic
propertle s could be-
IM
expected to vary accordingly. The magnetic suscqlib ility was
inea-sured as a
lunction of tem-perature u to 1000 X for alloy kvith Gd and Ce in
various propor-
tions. It appeav'S from the res -iffis that the -gllovs- Iwith more
than 607o of gadolinitrn
byweight. are in the ferro-anti- and paramagnetic statess. The rest
of the alloys
are anti-ferrornagne tic at lovi ternperatures, and at higher
temperatures t`rtere is

' NIR RET SOV, 005 OTHER.006

~ACUSSICK XR: A S/0O48/64/028A*"74kM7SQ
CbedLeralkav, V.I.; ftp# Iullu
'~TXTM magmetie properties of mom d and 9 imetals (single crystals
and pDlycrysta
~Zffeport, Symposlum an Feravoegastlam and Ferroelectrielty hold In
lonlegred 30 Ifty
to 3 June M17
SOURM AN SSSR. Isv. S*r.fla.g v'*28g no*49 19640 746-750
;'TOPIC TAGS:- magnetla susceptibility, temperatv" variation of
susceptibility, Mg-
netization isotherm , scandium, yttrLuap godollnium, d transition
metal 0 9 trawl-
tion metal
!ABSTRACT: Where" the magnstle properties of scat trawltion d metals
have by Mv I
been thoroughly studied In a wide temperature range, little Is
1known regarding the
!magnetic properties of metallIc scandlum and yttrlum, particularly
In the torn of
single crystals. This is due partly to the difficulties of preparing
high purity
Sc and Yt. Yet their properties are of particular Interest in view.
cc the fact that:
Sc and Yt have one uncompensated eloatrola spin is the 3d and U
shells v respective-;
ly. In the present work there vas determined the temperature
depandeme ad the re-
Cord

AMWICK HS: AP40306W
c1procal suseeptl1billty for several polyar3nitallbw specimens of
scandim of diffe-,
rent degrees of purity. The results are shows la the figure
(Saclosare). However,
primary attention van given to Investigation of the magnetic
properties at Se am
Tt single crystals. After conelderable experimentation, cubic
crystals suitable for
.measurement were finally prepared by the method of
"recrystallIzational anneal" un-.
der high vacuum. For susceptibility measurements these were mounted
In the holder
'with the c axis either parallel or pexpe Icular to the field. It
Vag found that is*
go the susceptibility In Us parallel ;field is greater than In the
perpendicular
one; thei opposite is true for Tt. The temperature dependences of
the reelprocal mum-
ceptibility were obtained ffbatraot*rls note: no results are
described only In vs-
ry general termRg In view of the fact Ahat in Se and Tt, as Is many
ram earth me-
tals, there may obtain antiforromagontle exchange Interaction In a
certala tempera;--
ture range. It was deemed of Interest to Investigate the magnetic
ps opertles at ga-.
dollulua; Wasurements of the nagnatIzatlon lseOmw were carried out
on single
crystals - (a a3ds pamllel and perpendicular to 09 field) and
polycrystallime sea-
ples :in the rafte from 17 to 1000OCe The sagastisation Isotherms
am proseated in.
figures* 7M brea3m evoiced In. 'Aw curves aro emktagous to tbase
sapofted tar other
ram sank messla Sa Wo r"Iss et wassamee st a belleass aga
seaftgarasamt, to
Amid"

ACCESSION NR: AP4030656
is concluded on the basis of the experimental kesults obtained for Be,
Yt and ad
that a complex azktlferrGmgwtlG structure obtains In those wtals.
Orig.art.han:
:4 figures.
1ANOCIATICK: Moskovskly gesudarstrsaWy valversitet Oftscor Rtatis
UUversity)
:SUMTM: 00 DAIR Aft 3CApM 23=4 01
im cani: M MR w am$ 000 01MM 004
A
4
/

ACMSXQN NRz U401921H 8/006/64/046/00~/0444/0446
AUTHDRSt Ch*chsz~hAXqv_#.. Ve X91 Popt lialiul Terekhova,-V. F.;
Koleanichenkove, Ye.
TITLE, Magnetic proporties of iingle-brystal and polycrystalline
I- yttrium
SOURCEs Z.
hurnal sksper. L tisorl. fix-* V. no. 2s 1964, 444-446
i Topzc TAGes yttrLus, aLngle crystal y~triume polycrystallLne yttrL-
um, 1 Curie reLss Xaw*. paroWnetic Curie temperature, magnitic sus-6
ceptibility, sunceptibUity-texperature dependonci, transition metal
d band e1ectrqv%, a band electron
A~WTRACN' The mWetLe suseeptibilLtyiof yttrium was studied for
e of cbtaLnLnV now Lnfozmtion an the rol
CM purpos e of d and a
'Aloctrons; in the mWeUe prap*#Lea of weakly magnetic transition
metals -Tbs. 'temperatu;* 41spendincis of the magnetic
susceptibility,

A 4
ACCUSION MR: AP4019204
was Imeasured between 77 and.1004'Y. by t~* Sucksmith method. In the
isinglercrysital yttrium the magnq~ic su0ceptibility was higher when
measured at right angles to tbs',-j--axis,`than parallel to this axis.
J,The tes"rature dependence of thi ouselptibility'is attributed to
,.the presence of collective-statiOlOctFOns of the d-s band and elec-
,.."trons of the d!-,bande subjected t~o spat4al localization. use of
the
C!2ri*-Weiss law yields for the paramagiketic curie p;oint values
-510KO -330Xt a -396K* It is suggeste&
P
ep-L :P-Polyqro
Vthat in view of the below-sero CIari;m t4pporature an antifer:Fomag
"In conclusion,
Inetic interaction may exist in netillic yttrium.
i r
P.the authors mTress theLr-gratitude to*Prof. Yo;. 1. Kondorskiy fo
-.invaluable isparkse" Qrigo art. bass I figure and 3 formulas.
,.Aj;SOCIATIONs 'HoskovskLy qosudariitvenny,*y univ*rsitet (Koscow
state University]
'OSMG3 Dwq) ACOS ;7Mar64 ENCL: 01
OUB. CODE v PH 90 BOVif',.002 OTHERs 04~-
0
P-A

S/00s'
1ACCESSION NR: AP4031143 6/64/046/004/1226/12271
AUTHORS: Chechernikov, V. I.; Pop, Iuliu'"
-TITLE: Magnetic properties of lutecium
SOURCE: Zh. eksper. i.teor. fiz., v. 46, no. 4. 1964, 1226-1227
TOPIC TAGS: lutecium, magnetic susceptibility, paramagnetic Curie-
temperature, Curie Weiss constant,.effective magnetic moment,'eloc_
..tronic state density, electronic specific.:heat
ABSTRACT: Continuing similar studies on scandium and yttrium
(ZhETF v.-44, 387, 1963 and-v. 46, 444, 1964), the authors measured-,
f6r the first time the t6Werature dependence of the magnetic sue- i.
ceptibility of metallic lutecium in,the rang* from 77 to 1000K.
Bother magnetic characteristics (effictive magnetic moment P , Curie-
P
!Weiss constAnt C~, ~nd..the paramagnotic,Curis twperature.'O were
P
142

I

:;on the cohcentration.and magn6tic*field.intensity. The temperature
the paramagnetic'susceptibility of Gd-Er alloys was
-investigated.to detei-mine:the effective magnetic mome nd
also nt a
the paramagnetic,Curie point. 'The magnetic moments of the Gd-Er
alloys increase fr - 0 .for pure Gd to 9.52 Bohr.
om 7.95 Bohr magnet ns
magnetons for Er. The paramaghetic.-Curie point shifts to lower.,
temeratures when the erbium content is increased but remains posi-
tive*.at all erbium ntrations. It d that the.de-I
conce is conclude
penderice -69--the maghe ti:es-.-of --these -alloys- on
the-tempera-----------
tic- roper
Cord 2/3

L12?m-66 EWT (M)/EWP (W)/ETC (F)/tWG (a)/T/EWP (t)/W (b) IJP(c)
RDW/JD/JG
ACC NR- AP6001230 SOURCE CODE: UR/0363/65/001/012/2138/2139
AUTHOR: Chechernikov,, V, 1, ; Pedwnpikov, A. V. , YareMbash, Ye. 1.
; Kalitin, V.
mow
ORG- Moscow State. Univeisi!j Im. -N. V. Lomonosov (Moskovskly
gosudarstve .nnyy univers-
Itet);
Institute of General and Inorganic Chemistry I N. S. Kurnakov,
Academy of Sciences,,
SSSR (Instifut obshcRy-i neorganicbeakoy khImil Akademit nauk SSSR)
7
TITLE.- Magnetic propertAeo of praaeodymium selenides
SOURCt-. AN SSSR. Izvestlya. Neorgntcheak6 materialy, v. 1, no. 12,
1965, 2138-2139
TOPIC TAGS: praseodymium compound selenide magnetic moment, magnetic
susceptibility
Cvrie point
ABSTRACT: Vie magnetic r. ea. of the selenides PrSe, Pr SeV Pr-,Se..,
and PrSe7 were
studied. The magnetic susceptibility was measured in the 80 - 900K
range. Above room
-4
temperature, the measurements. were made In A. 10 .. mm Hg vacuum to
prevent oxidation.
'Fig. I sbows the reciprocal magnetic susceptibility versus.
temperature. The Curie-Weiss
law X = C/(T - go was obeyed by all the samples. If the paramagnetic
Curie point 0 Is
determined from the experimental data, and the effective atomic
magnetic moment R is then
calculated, it Is found that these values change in proportion to the
praseodymium, 4t;nt.
The magnetic moments correspond to the magnetic moment of Pt+ ion,
Le. , 3.;3~,6. The
Curie point 9 Is positive in Pr 41 Pr2 Se3, and PrSe7s and negative
in PrSe and 13rSe.; this
is due to the RY;Darance of anwrromapetic interaction in the latter
two compounds. It is
rd 1/2 UDQ 546.6661231:538.11

card 2/2

39712-65,"

ACCESSION NR. AP500613

ENCLOSURE:. 01

Inverse~-sus
1
Fi

.,
g.

2
25
5

ceptibilit
y.,as a

function of tempera

erbium (I
turefor

and alloys.. 2

3--3.96; 4-9.81;

-at

6 T

5-

61V M

"/I

;,L 1358-66 EWT( WPCw)LEY4(g) WPZb) 1JP (c)
AVE

"ACCESSION ME: APS021942 UR/0126/65/020/002/029910301

546.65~:538.214

erekhova
AUTHM.
arnikov,
Mach V.~.; Spsianski-Y. N.M NaRj2v

~-1:,
TITLZ*. Magnetic proElrtie f
Imn-naodaigg alloya

-

SOURCI; Fialks, ustallov I UstallavedenLys v# 20, n0s 2, 1965, 299-301
~j

alloy, neodymium containing alloy,-sagnetic propertie
TOPIC UGS: iron containing.

.."z
constitution diagram, ferromagnetic
region, paramagnetic region, Curie point, anti-

tic interaction, three
sublattice structure
nape

ABSUACT: Pure carbbny iron (99.9%) and neodymium metal (99.5%)
vere smelted to-

gather in an arc furnace with anonconsumable tungsten
electrode in a purified

-400
helium atmosphere under a prQs*ure of 300 mm Hg. The resulting alloys
contain'

i different proportions of To to Nd were remelted several
times to assure homo-~~

seneity and annealed in evacuated
quartz.ampoules at 600 and 900*C for 130 hr.

Subsequent microstructural
and,l-ray onalyses of the sphere- and rod-shaped speci-i'

Sens showed
that most of the obtained alloys are of two-phase kind and represent

mechanical uixtur*a of solid soliltione (based an pure components)
with chemical

compounds .(Fel7N2"and re2") Such 6: type of constitution
diagram largely deter-

rd 1/1

L 1354-66
ACCESSION NIL: AP5021942.
pa anagnatic properties were nves-
sines the magnetic pro rties,of these alloys. Th i
tigated with the aid of the magnetic scale described.by V. L
Chechernikov (Vestnik
7 4
WA far., fiz., 1937 no- 1, 47),- at first ia' the ferromagnetic
region. It turned
out that in alloys containing from 10. 52 to 85 at.% Nd, below the
ferromagnetic
Curie point Of there exists a temperature range in which
magnetization decreases to
The 4
a minimum whereupon it again rises, and then againdrops to zero at T
- ef*
t
investigations were also carried out in the paramagnetic region,
where they made i
possible to calculate the effective magnetic moment P and the
temperature of the
paramagnetic Curie point. The temperature range of Avestigations in
both the fer-
romagnetic and the paramagnetic regions was.300-13000K. It
is.concluded from the
-Nd-allay,system there. *exists, alongwith-the ferromagnetic
findings-that in the Te
rramapat c- taraction~ case
A 80-. AS i icb- W~: t: clearly.manifes ad a ihs:
o the -on* 7 Vd__ -:As- f :experiments revealed, in: the regi - f
-P on
f Mee compour e17
existence of this compound the magnetic moment of alloy reaches a
minimum. and the
paramagnetic Curie point is much lower than in pure iron. It is
possible that a
three-sublattice structure exists in the Fe-Nd system, with positive
interaction
.,Iexisting between homogeneous atoms and negative interaction
between the atoms of Fe
and.Nd. The magnetization of Fe-Nd alloys*throughout the temperature
range-inves-
Itigated is conditioned by the Fe atoms; it is-not completely
compensated, since the
~Uapetic soment of. the Fe etooftesede that ot the. NO atwo: "In
conclusion tim
Caid. 2/3

L 1718-66 EWT(m)/EWP(t)/~WP(b) IJP(c) JDA
ACCESSION NR: AP5021943 UR/0126/65/020/002/0302/0303
539.292; 538
A 91
AUTHOR: Cheche
rnikov, V. 1.*,-Nefedov, A. P.; Sokolovskaya, Ye M,.
TITLE: Magnetic properties of V-Ta alloys
~T7
SOURCE:. Fizika setallovi metallovedeniye, v. 20, no. 2, 1965, 302-303
.~TOPIC TAGS., magnetic susceptibility, vanadium containing alloy,
tantalum con-
taining alloy, homogenized alloys electron system) sigma phase
ABSTRACT: The authors present.the results of an investigation of~the,
temperature
dependence of the magnetic suacep;4bility of V-Ta alloys made of
99.63% pure '4
vajaadium ano/199.7% pure tantalumilli4ong with small percentages of
Fe, Al. Si,
N2, C, 02s no Tit W, and Mo. Physicochemical investigations of the
annealed ape-
cimene (inicrostructuralexamination, determination of electrical
resistivity,
X-ray structural analysis) revealed that the -homogenized- alloys form
monophase
systems, while alloys subjected to additional annealing are two-phase.
The mag.;
netic'susceptibility of the alloys was ne'asured at temperatures of
from 77 to'
lloO*K with the aid of A pendulum balanco. It was found that at room
temperature
1/4
Card - ---------

L 1718-66
ACCESSIOWNR: AP5021943,
the susceptibility,of the hoviogenized alloys varies smootbly
thr3ughout the range
of concentrations. For pure vanadium it is maximal (4,10-0 g-cm- ),
and it de-
creases with increasing Ta contentuntil, in the case.of pure Ta, it
drops to
0.95.10-6 9. -3
cm . At different temperatures,_ throughout the entire temperature
range investigated,-for.homogenized alloys, the temperature dependence
of.specific
susceptibility 1/X is linear (Fig. 2). The slope of the curved, which
is nearly
independent of alloy composition, indicates a certain localization of
d-electrons
in the alloys,investigated. The imost interesting results were
obtained-for alloys
containing 34 at.% Ta (curves 6, 7).Thus while the susceptibility of a
specimen
subjected to a single heat-treatment operation varies markedly with
temperatures
the susceptibility of the compound TaV2 Is nearly independent of T
(curve 7). This
indicates that, in this compound, the principal part of the
d-ele.6trons undergoes
a considerable collectivization, forming together with a-electrons a
common elec-
tron system. It is this electron system that largely determines the
magnetic
properties of the compound TaV2- It may :be assumed that thio'compound
is an.
CF-phasev whichl' as is known, exists in many vanadium alloys and
is-by nature an
electron compoundo Furthermore, these findings confirm the phase
diagram obtained
by Refedov at &I* (Zhurnal neorg. khtaiip 1964p 9p 4p 883), Orig. art*
has% 2
figures*
Cewd-Alk-

JVIJU
-A_ffUTff:_ AP5027907 SOURCE CODE: UR/0189/65/000/00,r,/0042/0047
7=-Z Z----
AUTHOR: Nefedov, A. _E; s4WOLy- at Ye.'M.; Grigorlie A. T Cher.
--Sokolova,.~- G4; Guzey, I.,
ORG: Moscow State Unf~ersity (Moskovskiy gosudarstvennyy universitet)
75
TITLE: Solid-state phase transformations in vanadium-tantalum alloys
_64-/
SOURCE- Moscow, Universitet. Vestm'k. Seriya H. Xhimiya, no. 5, 1965,
42-47
TOPIC TAGS; base transition, vanadium alloy, tantalum alloy* vanadium
compound,
p
tantalum compound
ABSTRACT: The paper is devoted to the determin
mnature of the. intermediate
-Touf.P
V~
phase of TaV and boundarieW of its existence in V- a ste . The
magnetic
2
susceptibili* was measured as a function of composition and
temperature. The
temperatures of the start of fusion (solidus temperatures) were
determined. Data were
obtained on the differential thermal analysis of alloys of the V-Ta
system, and on the
microstructure, hardness, and crystal structure. The results were
used to plot a phase
diagram of the system (see Fig.
1/2
UDC: 536.7.
Card

1: _7_932m66_ 7
ACC, NR, AP5021907

It is found that in the region of the

stoichlometrid
composition where the ratio of

the components (at. %) V ! Ta--- 2 ! 1,
prolonged

.2AZ
-

stepwise annealing (lasting over 1600 hr)

induce s
transformations which may be regarded

~as a Process of ordering with
the formation of the

Intermetallio compound TaV . X-ray analysis

2&V
-

showed that TaV has a hQ~nal structure

I&V

similar to that o? an MgZn
-type Laves phase,

a to.,a)

058 0. 005
and lattice parameters a - A;

fW0
M 0 00 G~ a a

c = 8.250 � 0.005 A; c/a
= 1. 631, with four

1 9 00 0 0*000' ato

Vormula units per unif'de-H.
Orig. art. has:

T

7 figures ind 3 tables.

j
~

M4d
0 60 0,
-

79
AV A9 W .59W &V M 109'

Pig. 1 Phase diagram'of the,V-Ta system

based on
data of this, study

SUB CODE: TvIM'SS SUBM DATE. 07Jan65 /'O'RIG REF:
005 OTH REF: 002

2/2

,
C,,d

L jUP(Z)/EWT(2)/fWP(b)/AWP(0 IMP) JD/Z4/JG/)UVt4)
ACC MR: AP5018871 SOURCE CODE: UR/0126/65/020/001/0157/0159
AUTHOR: ChechernjjMy,,V,.I.; SjLeranskiy, N. M.; Terekbova, v. r.,
Rozhkova, R. S.
ORG:.,Moscow State University im. M. V. Lomonosova (Moskovskiy
gosuniversitet)
167
TITLE: Several magnetic properties of Ni-Eu alloys
SOURCE: rizika metallov i metallove3eniye, v. 20, no. 1, 1965, 157-159
TOPIC TAGS: Europium compounds nickel containing alloy, magnetic
property, paramag-
netic susceptibility
ABSTRACT: Temperature-de3endence (300-10000C) of paramagnetic
susceptibility-using
~the Faraday method at 10- to .10-4 m-m Hg was studied for specimens
contaiping 0.77,
.2.0, 31.26, 3.6 and 6.38% Eu. Samples of electrolytic Ni of 99.9%
PuritylAnd Eu not
containing more than .2% total impurities were castand remelted under
15 atm of
helium 3-4 times in a tungsten-are furnace and then homogenized for 100
hrs at
11000C. Microstructural examination showed the presence of a eutectic
Mi(a) +
,Nil7EU2, which increased with increasing Eu. The eutectic
transformation tempera
,ture was-1190 1010C. The solubility of Eu in Ni does not exceed 0.77%
atA Eu.
Qrd UDC: 546.661 538.214

ACC NR: AP5018871
'The compound Eu Ni (Th7Ni '10 was indexed at c/a 0.968 giving lattice
17 tYr,
A =T31Tand c~=,8.09 and intensiiy measurements indicate an hexago-~
nal structure. The hardness of the~compound was 271 kg/mm2 as compared
with 70
kg/RM12 for pure Ni. The'variation of the reciprocal of the
susceptibility I/X with~
;temperature is shown in fig, 1. The Curie-Weiss equation gives the
susceptibility
~where ~k is the,temperature insensitive susceptibility.~ The
susceptibility of Ni
16.38% Eujs almost an order of magnitude greater than'for pure nickel.
The magnetic
!moment RR is almost independent of the composition a small increase
in ~R takes
!place at 6.38% Eu., The paramagnetic'Curie point OR drops initially
with increasing~
:Eu and then from 3.0 to 6.38%,Eu* remains constant. Orig. art. has: I
figure and 1'
i formula.
~ISUB CODE: MNI SUBM DATE: 240ct64/ ORIG,REr: 000/ OTH REF: 000
Card 2/3

-.kCP7k,-66Ai - - -
5018871

Fig.l.
Dependence of 1/~ on T for

j
A

specimens with varying.Eu content.

j

1 Ni;
2 - 0.77; 3 - 2.0; 4 - 3.2
at.

(upper temperwture scale); 5 - 3.6;

10

-

6 6.8
at. % (lower temperature

scale).
Lower right shows the depend--~

ence of
RR and OR on Eu content.
8

6

.

~Pl

.300

200

100

Ivi

104P .600,

ew /Xv.

1200

JOV YOL~
WO

Cara 3/3

CICE CIERNIMAT , V. !. ; SPEWANSKIY, IN.11
1,1--*,-l;l,'c)V.! , E.V.
Magnetic rzoperties of. iron-neodymium alloys.
Fiz.,met.i n, etalloved.
20 no.2:290,-301 Ag 165. 18:9)
1. Moskovskiy gosuda--stvenyW universitet imeni
14.~.Lcrmonosova,

CIECHERNILKOV, V.I.; NEFEDOV, A.P.; SOKOLOVSKAYA,
Ye.14.
,~
Mgnetio properties of V-Ta.a-lloys. FJz.metoi
metalloved. 20
no.29302-~.303 Ag 165. (MIRA 18:9)
1. Moskovskiy gosudarstvemyy -universitet imeni
M.V.Lomonosova.

CHECHERNIKOV. V.I.; PECHENNIKOV, A.V.; YAREMBASH,
Ye.I.; KALITIN, V.I.
Magnetic properties of prasoodymium selenides. Izv. AN
SSSR.
Neorg. mat. I no.12:2138-2139 D 165. (MIPA 18:12)
1. Moskovskiy gosudarstvennyy universitet i Institut
obahchey
i neorganicheskoy khimii im. N.S. Kurn"ova, AN SSSR.
Submitted
July 12, 1965.

BALANEVSKAYA, A.E.; BERGER, L.I.; PECHENNIKOV, A.V.;
CHECHERNIKOV, V.I.
Magnetic propertieg of a series of ternary
semiconductor
compounds of the A'B-T' CyTtype with chal.copy-rite
structure.
Izv. AN SSSR. Neorg. mat.j no.12:2165-2166 D 165.
(MIRA l8sl2)
1. VoesoyuzM7 nauchno-issie6ovatellskiy institut
khimicheakikh
reaktivov i osobo chis 4khimicheskikh veshchestv.
Submitted
July S. 1965.

WMDOV, A.P.; SOKOLOVSKAU, Ye.M.; GRIGORIYEV, A.T.; , I .
SOKOLOVA I.G.; GUZEY, L.S. Fll,- . _- I
p ~~ -2 ~ _~ -

CHECHERNIKOV, V.I.; SPERANSKIY, N.M.; WiLYSHEV, Nel.
Electric, thermal and some mapetic properties of nickel-
cadmium ferrites. Vast. Mosk. un. Ser. 3: Fiz., astron. 20
no.5:45-48 S-0 165. (MIRA 18.U)
1. Kafedra magnatizaa Moskovskogo universiteta. Submitted
Vay
.128 1964.

CHEqEWL(3y,_j.I.; PECHENNIKOV, A.V. :; KALITIN, V.I.;
YAREMMSH, Ye.I.
Magnetic properties of single and polycrystalline
praseodymium
diselenide PrGe2. Zhur.eksp. i teor.fiz. 49
no.5%1399-1401 N 165.
(MIRA 19g1)
1. Moskovskiy gosudarstvennyy universitet.

-
0121 rd-'w P-01'i4:'--L"('U0UU'QE"UUU'
~~v I-- - __ . -1 - - - -1 UUVI vv i J.'r vv -.0 1
AUTHORS: Chochornilwy.-j"..; Spqranskiy_,__Y~_4__;.
.ORG: none
TITLE: klagnetic.~ thermal, and electrical_p?~_qpq_*ies of
nickel-cadmium ferrites
SOURCE: Vsesoyuznoye soveshchaniye po ferritam. hth, 11-11insk.
Fizichesk .iye i
fizikok1iimichovkiyo svoystva. ferritov (Physical and
physicochovacal properties of
forritas); doklady sovoshchaniybL. 111insk, Nauka i takhnika, 1966,
'11-75
-TOPIC TAGS: ferrite, electric resistance, magnetic susceptibility,
heat conductivity~
nickel compound., cadmium. compound
JkBSTIZACT: Specific electrical resistance, heat conductivity, and
mgnotic 3uscepti-
bility of nickal-cadmium forrites have been studied as functions of
tomorature
within a temperature range up ti OC. The chemical comoosition of the
specimens
is listed ip Table 1 Uhemical 5nalys S,k
specim
F'.0' Nio rajo
1 6.1.2 '24 4 10.11
2 63.4 20:8 15,3
3 61.8 17.5 20.7
4 61.4 14.3
,
5.4 1 XT
Card 1/3 ~.6 55,4
T 'I f%74). A7

ACC NR- AT6028976
At these conditions it is possible to observe the variations of
physical properties
in ferrites changing from a normal spinal structure to mixed and
reversed structure.
The effect of temperature upon the heat conductivity ~ and upon
specific
electrical conductivity (D of various compositions ol this ferrite
system is
illustrated in Figs. 1 and 2. A definite correlation was established
between the
.3 c al
jjcj
A x 1-2 3`3 5 6 Fig. 2. In.
oe'
for Ni-Cd
forrites as
5 1 a function of
W C
(500
Table for
30 jig 500,
ZO composition)
Fig. 1. GoefAcient of thermal
conductivity for Ni-Cd forritea
as a function of temperature
(zoo Table Xor composition)
Card
0

IACC. NR. ATI"026976'
invostigated proportios, especially a regularity botwoon the
ILemporature and
composition of the ferrite, on one hand, and the specific
eloctvrical resistivity and
heat conductivity, on the other. The obtained data indicate thatt,
the decisive role
in determining these properties is played by the electrons located
in apices of tho
crystal lattice. Orig. art. has: I table and 4 figures.
SUB CODE: 3.1,* 20/ SUM DATEs 22Dec65/ ORIG REF.- 003

-1-:07113-67 EWT (1) W/EOPWAti iip(c)
AP6029107 SOURCE CODIt UR/0048/66/030/006/0937/0961
ZhdazWVqGqG.-. lbralnov,XIe131i3[3&x Inin,R.H,; Chechernikov.Y.1
ORO: Physics Department# Moscow State University Ims
RV'1Am*nosov(F1x1Ch"k1y
fiiillltet Moskovskol gosudaretvannogo universitsta)
TIM: The Mossbauer effect In the IntermstallIc compounds Coll ASn mW
N13L 48A Isepo"
All-Mion Co ~er*w~eoh~e Physics of Ferro-and Ant1terroffilwatims
held 2-f July I
In Sverdlovsk7 z
SOURCE: AN SSSR, Izvestlyse Seriya fixlch*skaya, v, 30, no. 8~ 1969,
957-961
'TOPIC TAGS: Mossbamer spectrus, Wasbauer effect, magnetic
susceptibility, cobalt
allay, nickel allcy-,$ntermeta~41c cowpound
ABSTRACr:,Jhe present study.was undertaken In conjunction with the
growing Interest
In In IntermetallIc compounds, in particular those can-
taw- W&~%W,"'-Speciflcally, there was studied the Mossbauer effect
In C0l.4Sn d 11,48n. The compound specimens me" prepared by vacuum
melting of the
components, followed by homogenizing anneal In sealed tubes (30
hours at about 8000W.-
and then slow cooling to room temperature, In the some manner there
were prepared
spe I xtures of the two above-wentioned compounds* I.ee,
representatives Of
C
the CT0?x3f?-rYstez6 Am" the last only samples with the NOW stmoture
wpil 1002190t4k
for iie-iois-t or The Mossbauer effect was'studled on a 2=261
1/2

L 07113-67
ACC NRi AP6029107
In specimens with 1."timr thickness of 9 mg/cmi2.~ The source of the
2398 k~V gamme
rays was a 5 mg/ca thick sample of Wgion. The measurements were
performied -with the
source at liquid nitrogen t*mperatur*e The Mossbauer spectra obtained
for Co On at
f l Bn
different temperatures of the absorber and for a series o 00 .4
-N13L.48n 90111
solutions (0,9,25,50 and 100% C01.48n) are reproduced In figures. Also
presented In
graphics are the temperature dependences of the
reclprocal.musceptibility as obtained
by the authors and taken from the literature (M*Asanum, J.1ftys.Japan,
17, 300, 2962);
the agreement for C02.48n Is better than for Nil 48n. The temperature
variation of
shows that quadrupole spliHing persists up to the taimperature
the Mossbauer spectra
Of the phase transition, that is, up to the temperature of the Nook In
the reciprocal
susceptibility versus temperature curve; above the transition point
there 10 obsox.
only the sInglet Mosobsuer line. The results are discuss" briefly and
reasoWwn
hypothesized for the absence of ferromagnetIms In the studied
Intermetall1c compowedso
Further investigations must-be weft before a full Interpretation of
the prebefit re-
sults can be offerode Orig, art, has: 4 figures.
80 CGDZz 20#07 amt 00 Ono, am: 005 am RMS 006
LC

T, 01052-61 EW (m)AA-dP(t)ATt IJP(c)- JD
ACC -144, -AP6030956 SOURCE CODE- UR/0181/66/008/009/2594/2597
AUTHOR: Ka shlinskiy A. I.; Chechernikoir s
V. 1. Venevtsev, Yu. N.
ORG: Moscow State Universi!Z im. M. V. Lomonosov (Moskovskiy
gosudarstvennyy
universitet)
TITLE: Investigation ofelectron resonance and magnetic properties in
solid
solutions f the system
SOURCE: Fizika tverdogo tela, v. 8, no. 9, 1966, 2594-2597
TOPIC TAGS: electron spin resonance, electron spectrum, EPR
spectrum, solid
solution, bismuth ferrate, barium titanate
ABSTRACT: The spectra of electronic resonance in solid solutions of
the i5ystem
bismuth ferrate barium titanate have been investigated. The clearly
defined
anomalies in the spectra are determined, corresponding to the
d.jelectric and
magnetic transitions in solid solutions in conformity with
tetragonal and rhombo' -
hedral modifications. The data on changes in the EPR spectra are
analyzied in 'k.~
relation to the properties of solid solutions under study. Orig.
art. has: 2 figures.
[Based on authors' abstract] INTI
SUB CODE:. 20/ SUBM DATE: 14Jan66/ ORIG REF: 0091
,-LCard 1/1

ACC Nit, AP601690
AUTHORsl Chechwakova V. I.1 FecherAdkovs As Ve; luliu POP
ORG: Moscow State University In He Ve Lowncew (Kos1wvs1dr
gosuniveraltst)
TITLE: Magnetic properties of cerium-acwWdim alloys
14.
SOME: Fizika metallov I metallovedenlysp v;*-1.' no* 6# 19669 937-939
TOPIC TAGS: magnetic alloyp magnetic susceptibility, cerium bass
alloy, scandiUll
ferromagnetism, antiferromagnotim
ABSTRACT: The magnetic susceptibilities of seven cerium-acandium
alloys are
investigated as functions of tempersturee The subject in of interest
as it was
noticed earlier by Vo I. Chechernikov and Iullu Pop (FM., 1964v 18t
363) thatp at
certain temperaturesp cerium alloys exhibit coex1st*nc* of ferro- as
wall as
antifarromagnetism. The temperature interval chosen for the study was
77 to 1100K
'which Includes the region of polymorphic transformation. Before
measurements were
taken., the alloys were annealed at %W for 240 hours* The magnetic
susceptibility
was measured by balanced s"les with mechudcal compensation described
by luliu Poyr.~- -
and,V. I. Checherakor (PTZ,, 196kp moo 5j, 180)o' The results of the
investigation
are shown in Fig. 1, Apparentlys, tbs magnstlo properties of alloys
with high
UDGa 538.224A.65+546AU

ACC NRt AF60189$0
7 1 Fig. I I/A an function of T
for C94c alloys a I - 9j -
2
41 3 - 411 i 4 491
65j., 6 - 60;. 7 90 ate % I
-;f Saj raudader consists of Goo:
e
4L
V~.
-j-
r
cerium content are determined by localized 4f electrons* 'Orig.
arta. Wwt'2
fipres*
SUB CCIDEs 31,2.0/SUBK DATICit MecW QUO MWz' 003
Cwd 212

ACC NR: AP7002734 (A) SOURCE CODE: UR/0126/66/022/oo6/c,839/0842
I AUTHOR: Shafigullina, G. A.; Chechernikov, V. L; Markova, L A.
----------
ORG: Moscow Stat University im. M. V. Lomonosov (Moskovskiy
gosuniversitot)
il T1TLE: Magnetic properties of Dy-Y alloys
SOURCE: Fizika metallov i metallovedenlye, v. 22, no. 6, 1966,
839-842
TOPIC TAGS: dyskosium compound, yttrium compound, magnetic
property, magnetic
susceptibility. Curie point, magnetic moment
ABSTRACT: The article presents the results of an experimental
investigation of magnetic
properties of Dy-Y alloys throughout the range of concentrafions
in the temperature interval of
from 100 to 1000% in the presence of magnetic fields of various
intensity. To this end, 9 alloys
of this system, containing 5.7, 11.9, 18.7, 26.6, 35, 44.1, 55.8,
68 and 83 at.% Dy (with '~f
as the remainder) were obtained by multiple remelting in a
helium-aftnosphere are furnace
and vacuum annealing at 10-6 mm Hg for 70 hr at 850*C. Magnetic
susceptibility was measured,
pe-
by the conventional ponderomotive method on using a magnetic
balance. Heating to high tem
ratures was accomplished with the aid of a platinum resistance
furnace, and the temperature
1/6 UDQ 669.85186:538.214

ACC NRs AP7002734
was measured by means of precalibrated Pt-PtIth and Cu-constantan
thermocouples. The
quartz cup containingthe specimen and the thermocouple junction
were in a uniform, tempera-
ture field. The magnetic balance was calibrated in advance with
respect fo pure holmium, Qor
< 70VX) and nickel (for 700-UOO-A). Findings: magnetic
susceptibility x and crystal lattice
constants a and c change monotonicaUy over the entire
concentration range (Fig. 1). The pat-
tern of temperature dependence of reverse susceptibility I/X is
linear. (Figs. 2. 3) thus makir
IA,
X./D#
t Fig. 1. Magnetic susceptibility y. (curie 1)
t
and lattice constants a (curve 2%
3 and c (curve 3) as functions of
z composition of the Dy-Y all(iy a~t
room temperahwe
L
UD j0
Y, 'at.%
j Card 2/6

ACC NR' AP7002734
x
12
6
S
6'
.2
2-
!00.470 M 4100 TOO tOO 700 $00 OO/W49/we w
Fig. 2. Temperature dependence of reverse Fig. 3. Temperature
dependence of re-
susceptibility of Dy-Y alloys: verse susceptibility of Dy-Y
1- 5.7 at.%Dy; 2 - U.9 &L%Dy; 3 -18.7 auoys:
at. % Dy; 4 - 26. 6 at. % Dy; 5 -36 at. % Dy. 1 - 44.8 at.% Dy; 2
- 68 at.% Dy; 3 -
(RenOdWer: Y) 83 at. % Dy (Remainder; Y)
Card

ACC NR. AP7002734
it possible to calculate the effective atomic magnetic moment p
of the alloys as well as to,de-
termine, the Curie point 0P (F%. 4). Within the Oestigated
temperature range,
!AID
Fig. 4. Effective atomic magnetic moment
pp and paracutgaetic Curie point ep
as functions of alloy composition
Dy, at. %
the magnetic susce ptibility of Dy-Y alloys follows the
Curie-Weiss law. and 8 of the a]
Pp p
Card 4/6

ACC NR:
AP700273-1- -
vary monotonically As a function of the alloy composition, and the
magnetic moment calculated
1 per atom 6f dysprosium corr~esponds to the trivalent ion of this
element in fundamental state.
In the low tcmperat~re range there occurs a transtion from
antiferromagnetic to paramagnetic 1
state, which shifts in the direction of low temperatures with
increase in 'the magnetic field' I
intensity (Fig. 5). k1 this indicates that the magnetic properties
of DrY alloyii are chiefly
2
2S
Fig. 5. Temperature dependence of suscep-
tibility of alloy no. 9 (83 at. % Dy,
remainder Y) as a function of magne-,
tic field intensity H:
I - 17, 400 oe; 2 - 16, 100 oe; 3 - 14, 600 oe;1
4 - 12,440 oe; 5 - 10,050 oe; 6 - 7550 oe
OA'
......
j
00 ja 24

ACC NR: AP7002734
conditioned by localized 4f-electrons, while In the
antiferromagnetism region there apparently
exists a spiral-Me magnetic structure resembling the structure
observed for pure dysprosilimi
"In conclusion the authors wish to express their gratitude to
Professor Ye. L Xondorskiy for
his valuable commeAU. 11 Orig. art. has:- 5 figures.
SUB CODE: 11, 20/~ SUBM DAT.E; 29Mar66/ OTH REF: 004
Cwd Y6

TMTKOVA. A.F., inzhoner; CENCHMIAU, M.N.. inshoner.
Good results from the u:=90f =00as ~W, bout shuttles for flax
weaving*
'Poksteprom. 17 no.2:34-35 7 157. (Km 10:2)
1. Gosudarstvemiyy prMktoly inatitut-1.
(Loans) Oplax)

- --- ------
C=HgRsyliy Alekiaz~r Isayevich; FILOOT, N.P., red.:
KOHYASKINA, A.D.,
telchnred.
[How to prevent fire& in the how] Yak uberech' Shilishche ot
poshare.
Moskva, Isd-vo H-va ko=un. khoseRSMO 1957. 32 p. (MIRA 110)
(Dwellings-4ires and fire prevention)

D.M., inzh.,- ZBOSKIY, S.G., inzh.;
CHERNETSKIY,, V.1),, irzh.- CHECHFARSKIY,',
SOWIMP ltvyc,.p
Complex lnocul&nt for iaatit iron. Mushinostroenle no.3.,
2 ,z -6 (MM 18 6)
my-js 165.

GORBU(N.B.P.; CHICHN'T.z.
Calculating the backwater of ground water under conditions of
Intensive evaporation. Trudy Inst.soor.Al Ux.SSR no-5:91-96
154. WRIL 8: 10)
(Soviet Central Asla-Vater, Underground)

CHECHET.-Yu.S., dolctor tekhn. nauk, prof. (dec.eased);
LOPUKHINA, Ye.M.,
Acihd. tekhn. nauk, doteent
Optimum parameters of motors with
no.39:55-59 162.
hol Trudy MEI
(MIRA 17:6)

C,jjFCJJ-n~-1) jqr~V_.o, I 1 0) A. a
__grggypVj#.., prof.( 894- 9( ',- TITUNIN, e.
Y .,
red.
(Miniature electrical irachines of automatic
sYs-Lems]
Elektri.cheskie mikromashiTly avtomaticheskikh
ustrolstv.
lzd.2., ispr. Mosk-vaj Energiia, 1964. 423 p.
(',LIRA

KOSTENKO, Mikhail Poliyevktovich, akademik,
PIOTROVSKIY, Lyudvik
Marlyanovich; CRECIIET Yu j,., r
. Rof.j retsenzent;
USSERY A.s.- 12~ff, ~Le-'11~"Off'nauk, red, t
VOLIDEK, A.I.,
doktor tekhn. naukp red.; PRUSS-ZhUKOVSKIY,
V.V., nauchn.
red.; ALEKSBYEVA, Ye.A., red.
[Electrical machinery]*- Elektricheskie
mashirq. Izd.2.,
Moskva, Ener.-iia. Pt.l. 1964. 547 p. (1,.IRA
18:1)

ACC NR& AM5010318 MCUDGWII UR
bechets Turly Sergey c Professor; Doctor of Technical Sciences;
Deceased)
Electric micromotory of automatic devices (Elektrichookiya
mikromashiny avtomat-
icheskikh ustroystv) 2d od.p rev. Moscow# Izd-vo "Enorgiya"#
1964. 423 p.
illus.p biblio. 25#000 copies printed.
TOPIC TAGSs automation# synchronous communicationp servomotor#
tachometer# trans-
former# computer technologro computer componentp automatic
control.
ou&rroror- ^",vroz
PURPOSS AND COVERAGEs This book describbe the basic types of
micromotorep Including
serromotorep tachometer generatorop rotary transformers# and
synchronously operating
machines# for automatic devices. It also liescribee the theory
and application of
.micromotors in automatic control pysteSSA~\The book is intended
as a textbook for
students in elictrJkal engineering and power engineering
universitiesp as well. an a
*cool for engineers and technicians working in the field of
autonations talemechanical
jind computing technoloj6,. The author thanks N. A. laylinskiy
for his valuable
(W CWTENTS [abridged)i
TU. S. Chechut, [G. N. Petrov, Professor, Corresp6nding Member
MSW] - 5
Foreword - - 7
Introduction - - 9
UDGs 621.313.3s6a.313.2
rd 113
CH 57

ACC NRs AM5010318
PAN 1. Servomotors
Ch. I. General theory of a-c motors for servosystens - - 14
Ch. 11. Theory of "ideal" induction motors used in servosystems - -
59
dh. III. Theory of a real motor' with amplitude and phase control -
- 73
Oh. IV. Theory of a motor with a capacitor In the mitinj circuit.
Comparison of
various control methods - - 115
Ch. V. Direct-current servomotors - - 138
.Ch. VI. Electromechanical time constant of servomotors - - 157
PAW 2. Tachometer generators
Ch. VIL Alternating-current tachometer generators 164
lCh. VIII. Direct-current tachometer generators - - 189
PAff 3. Rot,az7 transformers
Ch. IX. Design of rotary transformerss, their use and working
prinaiplq 298
Ch.-I. Theoz7 of rotar7 transformers with four windings - - 215
Ch. 11. High-precision windings for rotary transformers - - 254
PAFG 4. Idaromotors for synchronously operating eyetems
Ch.,XII. Sinchranous. motors - -i.292