SCIENTIFIC ABSTRACT ZAYDEL, A.N. - ZAYDEL, B.M.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001964020017-1
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 15, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

S/119/62/600/005/005/005
AUTHOR: Seleznev, G. V.
TITLE: A programming pulse device
PEARIODICAL: Priborostroyeniye, no. 5, 1962, 24-25
TEXT: The device is to be used for time programming for any
multiple time*intervals and for producing pulses of fractions of
.a second to aeveral minutes' duration. The design is based on
coupling a coordinate grid to a step-distributor. The number of
produced commands is determined by the number of program apertures
in the coordinate grid. If larger capacity .4,a required two ouch
devices are connected in series. The commutating panel has ver'tica
bars Corresponding to 'units' from 0 to 9, horizontal bars for
Itens',- from 0 to 9, and plugs whose numbe:r corresponds to the
required number of commands. Diodes prevent-the reversal of our-
rent in the coordinate gridoet'which reversal might occur with
four or more combinations. The rev counter may be either electro-.'
mechanical or electronic,depending on the produced pulse repe-
Card 1/2

3/119/62/000/005/005/005
A programming oulse device D201/D308
titon 1requency. The 'program is set up simpl by ins&:-ting the
plu,,,?s (of which diodes-form an iniegral parts into corresponding
holeo-of the commutation panel. When the arrangement is switched
on, an electromagnet then moves a contact along the 'unit' bar
until it meets a 'ten' connection and so on. There are 3 figures.
Card 212
V, 14-IT 1-1

2~'M# 21 (1) ~
AUTHORs Zaydaltp A. N. SOV/53-68-1-9/17
TITLEt Spectrum Analysis of the Isotopic Composition
(Spektrallnyy anali2 izotopnogo aostava)
PERIODICALt Uspekhi fizichookikh nauk, 1959P Vol 68j Nr I p pp 123-134 (USSR)
ABSTRACTs In the introduction.the.author.diecusees in short the need of
a reliable analysis of the isotopic composition for research
.and industry, furthermore, he describes the mass
speotro.graph, its applicabilityt and the spectra with respect
to shift and splitting of the spectral lines. quantitative
methods of isotope spectrum analysis (atomic spectra) were
devised chiefly in four laboratorieso two of them
(unspecified) are in the USSR (investigation of H, Ego Uv Liq
Pb); He, Li$ Pb, U were investigated in France, and H) He, Li)
Hg, Ph, and u in the United States. In this article reference
is made to the publications of 1950-58. First, some spectral
apparatus are mentioned: for H- and U-investigation the
spectrograph ISP 51-A or the smaller diffractive apparatus
DS-11 figure 3 shows the scheme of an apparatus for the
photoelectric recordi -ng Pf the hyperfine structure of spectral
Card 1/3 lines (resolution up to 106).-The light-source used is then

SpectruN Analysis of the Isotopic Composition BOY/53-60-1-9/17
discussed in short, and the moot frequenily used cathodes as
well as the cathodeleas high-frequency d;soharge (water-cooled
cathode - Fig 4a, cathode cooled with liquid nitrogen - Fig 4b)
are mentioned. The author then de9oribee in detail the
intensity- and concentration measurement. In first
approximation it may be assumed that the intensity ratio is
equal to the concentration ratio of the corresponding isotopes.
Howavort thin ideal case in dtatiirbed, in particular by the
following factorni (a) light nottroat inotopio separation,
various Doppler broadeningn, transposition of the contours
of the components of the isotopic and hyperfine struotur6,
self-absorption$ Otol (b) spectral apparatust finite width of
the inetrume~ntal contourt dispersed light, They are discussed
in short) and the analysis methods and accuracion-are
demonstrated by the examples of hydrogen, helium, lithium,
lead,.and uranium and with the help of numerous speotrograms
and microphotograma as-well as two tables concerning lead
Isotopic analysis. The concentration determinations by the
mass-opectrographio- and the spectral method are compared to
one another. Finally, methods of calibration are discussed
-2/3 and -an apparatus -designed -for -absolute determination of -the

Spectrum Analysis of the Isotopic Composition SOV/53-68-1-9/17
isotope composition of lithium (Flg 10) is mentioned. In
this connection the Russian authors L. A. Tumerman, Y6. N.
Koren, Yu. I. Turkin, and G. V. Ostrovskaya are mentioned.
There are 11 figures, 2 tables, and 20 references, 13 of
which are Soviet.
Card 3/3

24(4)V24(7) S07153-69-1-10111
AUTHORSs Bogdanova# I* P.v Bochkoval 0. P.j
Zakharovaj V. M., Kagant Yu. M., K&ITteyevsklyl M. Y.~-Penkinj
N. P.# Chayka, M. P,~Shukhtin, A. M.p Lipisq L. V.
TITM Bergey Eduardovioh Frish (Bergey Eduardovich F~iah).
On the Occasion of His Sixtieth Birthday
(k sheatidesyatilatiyu so dnya rozhdoniya)
PERIODICAL: Uspekhi fizicheskikh naukt 1959, Vol 69, Nr I, ppl65-167 (USSR)
~ABSTRACTt On June .19th, 1959,the well-known Soviet physicist So E, Frishp
who made a name for himself eepecially in the field of
spectroscopic optics, attaineA the age of sixty, He began his
scientific work as a student at the fitiko-matematicheakoye
otdoleniye Leningradskogo universiteta (Phy9ico-mathematical
Department of Leningrad University) under Do Be Rozhdostvenakiy.
After completing his university studies he continued his work
at the Gosudarstvennyy Opticheekiy institut (Optical State
Institute). Since 1934 he held a chair for optics and supervised
work at the Physics Department, first as dean and later as
director of the Nauchno-iosledovatel'skiy fizicheakiy institut
Card 113 LGU (Scientific Research Institute for Physics at Leningrad

Sergey Eduardovioh Frish. SOV153-69-1-10111
~n the Occasion of His Sixtieth Birthday
----Atate- -univeraity).-In 1946- he- was -appointed -Corresponding
Remberp AS USSR, and.took active part in the work of the
Academy. He is deputy chairman of the spectroscopy Committee,
chief editor of the periodical "Optika I opektrookopiya" and
member of the International Committee for spectroscopy at the
UNESCO. He first concentrated his scientific interest an
atomic energy# the systematics of atomic speotrat the Zeeman
effect in the sodium and potassium spectrwz~ as well as upon
experimental spectroanalytical investigations. In 1930 he
started a cycle of workag which was devoted to optical methods
of investigating the properties of the atomic nuoleuse (An
investigation of the interaction between nucleus and electron
shell led to the disoovory of the hyperfine structure of
spectra)o He-Inve stigated- -the -hyperfi-ne etruoture of Ila and set
up a rule concerning the interrelation between nucleus-spin-
and parity. He further investigated the fine structure of
Isotope mIxtureej the excitation mechanism of the higher atomic
levelop and questions of the intoraction of elementary
Card 2/3

Bergey Eduardovich Frich. SOV153-69-1-10111
.O'n the Occasion of His Sixtieth Birthday
particles. Finallyp mention is made of his pedagogical
activities, especially his courses in ph eics (which are
partly hold together with A,, V. Timorova There are
I figuro and 42 Soviet roforencose

SOV/5090
PHASE I BOOK EXPLOITATION
Zaydell, A. N N. I. Kaliteyevokiyp L. V. Lipis, and M. P. Chayka
Emissionnyy spektralInyy analiz atomnykh-materialov (Emission
S ectrum Analysis of Atomic Materials) Leningrad,, Fizmatgl.z., 196o.
9
96 p. 8tOOO copies printed.
Ed, (Title paga); A, H, %aydell, Professor; Ed.: Yet Ya. Shreyder;
Teoh. Ed.: A. A. Zabrodina,
PURPOSE: This book is intended for specialists in optics and
spectral analysis.
COVERAGE: The book deals with the techniques of spectral analysis
used in the determination of the purity of atomic materials,
The work does not discuss determinations of components in alloys,
including Nb-U and U-Al used in reactor construotions and in
alkali metal alloys, nor does it describe the analysis of atomic
raw materials (ores and primary produoto of their processing)
since this type bf materials can be treated by conventional

Emission Spectrum Analysis (Cont.) SOV15090
spe~cvrai analysis methods. Ch. II,0 IIIO.IX,, X11p XIII, and XIV
,wege written by-A. N. Zay4oll; Ch. V1,. X and X1 by
N.J. Kalitayevsklyj Ch. VIX and VIII by'L. V. Lipis; Ch. V by
M. P. Chayka; Ch. I by A. N. Zaydell In cooperation with
H. M. Kaliteyevskiy; and Ch. V. by M. P. Chayka and A. N. Zaydell.
The authors thank S. E. Frish, A. A. Petrov, S. M. Rayskiyx
M. A. Yellyashevich, A. A.' Bashilov, V. V, Wallmovj and
Yes-Ya. Shreyder. Reforencea accompany Gaeh of the three parts
of the books.
TABLE OF CONTEMS:
Foreword
9
Introduction 11
PART 1. PRINCIPLES OF SHMRAL ANALYSIS AND THE APPARATUS
Ch. 1. Principles of Emission Spectrum Analysis
1. Basic conditions 17
Cax-d-2/45,

8/051/60/009/002/001/006
3201/3691
AUTHORS% ZaAell Ajl,and Ootrovsk:aya, G.V.
.TITLB s A Spoetroacopic Datemination of the IsotopioCcmpositillof Carbon
PERIODICALt Optik& I spoictrookoplya, 1960, Vol, 9, No. 2, pp. 1370-141
TS-XT# - The Isotopic composition of -carbon vas -determined using a spectroscopic
apparatua employed sarlier for the is.otopic analysis of hydrogen (Ref4. 3 and 4
The carbon 4pootra wore acited in-an elootrodeless -high.'froquenoy digehargo
and rocorded with a diffraction monochrcmator and a photemultiplier. The
lsotuic aciapasition wits deduced from the ratio of the Intensities of C130
and 0 20 L*nds at 4131.0 owd 4123*0 A ro3pontlyoly- Typie%l roiordlne -lio
CO bands at C13 concentrations of 56 and are shown in Figs. la'anl 16
respectively. Fire. 2 and 3 Mustrat* corrections of the intensity
readings. The dependence of the 11012 intensity ratio on the gas'pressurs,
in the discharge tube.is shown in Fig. 4. The band intongity-isotopic
cIomposition calibration graph is given in Fig. 5. The range of 013
concentrations was varied from 1.1 to 56%. At low C113 concentrations (1-,c%)
Card 1/2

S/051/&0/009/002/001/006
3201/Z691
A Spectroscopic Deteruination, of the Isotopic Composition of Carboa
the scatter of the resultA corresponded to & cooffi6iont of variation eq al
to 5-7%.' At C1,3 6ontenta amounting'to 5-60%*the coefficient of 7ariation.
vas 2-3%.' Oho Isotopic analysis requirod 0.1-O.Z =3 of-gas and it took.
10-15 min. " Acknowl*d&mont is made to I,,G. Gvartsiteli for supplying m*thans
enriched with 013. There are 6 figurom, I table &M 6 r*f*renc*a% 2 Soviot
and 3 Snglish.
SUMMIDs November 18, 1969
card 2/2

Ni-.'WTMFA, Z#N.; TAKIMOVA. P.P.; YAXDVLZVA, 5,8#
Spectral determination of rare earth elements axtraoted from
minerals and ores. Vast. 14V 15 uo,4:48-$q 160. (MRA Ila)
(FAre earthn--Speotrx)
(Yttrium-Speotra)

A 74 51 4
B/057/60/030/012/001/011
B019~BO56
AUTHORS: Afrosimov, V. V.1 Glukhikhp V. A.f Golant, V. Ye.v
-7aXdgl Komar, Ye4 G4 j Konstantinov, B. P. ,
Malyshev, G. M., Malyshev, 1. F., Monoazon, N. A.2
Stolov, A. M., Fedorenko, N. V.
TITLE: Plasma Studies With "Allfa" Resaarch Installation
PERIODICAL: Zhurnal tekhnicheskoy fiziki, 19607 Vol. 30, No. 12,
PP. 1381 - 1393
TEXT: A research installation for producing high-power pulsed dis-
--chargesin-a-toroidal chamber with an average diameter of 3.2 m and an
inne,^, arose-ooction-diametex of--l-m is described. The chamber is filled
with hydrogeno and dleoharge is obtained at-a pxessure.of about
2-10-4 mm Hg, and with an OXtgrndl magnetic fiold of 100-720 oe* Dis-__
charges are produced by 2-3 meec electric pulses coming from a OAPdeitOr
6
battery capable of storing 1-5-10 'Joules of energy. The entire installa-
tion is shown in a photograph, and is se hematically represented in Fig.2.
Card 1/01,

67h5h
Plasma Studies With "Allfa" Research 8/05700/030/012/001/011
Installation' B010056
The electric and magnetic characteristics of a pl4sma discharge are do--
scribed in detail, after which microwave studies, spectrum analyses~
and studies of the atomic flux emitted by the plasma are discussed. The
experiments hitherto carried out on "Allfa" show that the production
and character of a discharge do not correspond to the general concep-
tions of a selfcontracting quasisteady discharge, The authors formed
this opinion owing to the lack of a long plasma column, which follows
from measurements of the electric and magnetic characteristics, from
microwave studies, from the existence of a large azimuthal current,
from the asymmetry of dischargep from the occurrence of oscillations
thereiny and from a considerable inhomogeneity of plasma. Besidesq there
is an inhomogeneous hydrogen-ion distribution, which is indicated by a
large quantity of protons with energies exceeding 10 key. An explanation
of these effects is not possible as yet. There are 8 figures and 22 ref-
.erences: 13 Soviet, 3 Swedish, and 6 US.
Card 24

Plasma-Studies With "Allfa"-Renearch- S/057
.1601030101210011011
-Installation
B019/BO56
ASSOCIATION: Fiziko-tekhnicheskiy institut AN SSSR (Institute of
Physics and Technology of the AS USSR). Nauchno-
issledovatellskiy institut elektrofizicheskoy apparatury
(scientific Research.Inatituto of Electrophysical
Apparatus)
SUBMITTED,
Jul~ 15, 196o
F
Card 3/6
p

9/05TJ60/030/012/005/011
9/BO56
02
LUTHORS: Malyahev) G. M., Shreyder, Ye. Ya.,
Berezin, A. B., Belyayeva, V. A-0 Gla4uahchak, V. I.,
Skid4n, V. V., Sokolova, L. V.
TITLE: Spectral Examinations With "Allfall Reisearch Inatallation.
I. Study of the Character of the Spectrum and of th4 Ion
Temperature
PERIODICAL: Zhurnal tokhnicheskoy fiziki, 1960, 701- 30, No. 12,
Pp. 1422 - 1432
TEXT: The spectrum of the discharge was investigatod within the rang&
Of ~50-5000 A. The spectrum of 356-2000 A wan rocorded by a vitouUM
spectrograph,(600 lines/mm), the optical axis of the inotrument *so laid
in a radical direction. From 2000 A to 5000 A a quartz speotrograph was
boed. Fig.1 shown several spoctra recorded by the apparatus. For deter-
mining the ion temperature, the authors udod the rol4tion
1.95-10 12 I(-Axlx)2 (1), on the supposition th at 4 Maxwell velocity
Card 116
3-

87458
Spectral Examinations With "Allfa" Research 9/057/60/030/012/005/011
Installation. I. Study of the Character of B01-9/B056
the Spectrum and of the Ion Temperature
distribution and a pure Doppler broadening of the spectral lines exists.
From the data concerning the temperature of the impurity ions obtained
herewith it follows that, in dependence on the selection of the lineq,
from whose broadening the ion temperature is determined 6with (1)9 the
calculated temperature varies about the range of 0-5"10 - 15-10 OK.
The calculated temperature value is the higher, the stronger the charge
of the ion according to whose line broadening the temperature has been
determined. This indicates an independent motion of the Ions of dif-
ferent charges and a non-uniqueness of determining the plasmia tempera-
ture from the Doppler broadening of the impurity atoms. The authors
thank B. P. Konstantinov for discussions and N. I. Kaliteyevskiy,
A. N. Razumovskiy, and M. P. Chayke for taking part in the work. There
are 6 figureep 4 tables~ and 7 references: 3 Soviet and 4 US.
Card 2/4

Spectral Examinations With "Allfall Research W057J60/030/012 /005/011
Installation. I. Study of the Character of B019/BO56
the Spectrum and of the Ion Temperature
ASSOCIATION: Fiziko-tekhnicheekiy institut AN SSSR (Institute of
Physics and Technology of.the AS USSR). Hauohno-
issledovatellskiy institut elektrofizioheakoy apparatury
(Scientific Research Institute of Blectrophysical
Appa~ra.tue)
SUBMITT=: July 15, 1960
S07-
019
eO
-6:0 OV
702
-794.
Card--3//Wdji
6W

87459
S/05 60/030/012/006/011
BOI 9Y13056
AUTHORS; _Zayde1'i.A"-, Malyahey, G. M., Mookalev, Ye. I.,
Ptitsyna, Ye. A., Sokolov&, L. V., and Chashchina, G. 1.
TITLE; Upootral Yx&minttt1ors* Wtth "Allfa" lloaoftr0 Inotallat-ton.
II. Direoted Ion Movumonto
PERIODICAL: Zhurnal tekhnicheakoy fizlki, 1960, Vol. 30, No, 12,
pp. 1433 - 1436
TEXT: Directed ion movements in "Allfa" were measured by determining
the spectral line shift of ions caused by the Doppler effoot. Tho ex-
periments were oarried out with a low-disperston quartz spectrograph
and a spectrograph of the type AjJC--8 (M-6), having a diapernion of
D-- 6 A/Mm. The pictures were taken in tangential diroation andp part
of the spectrum is shown in Fig-3. The ion velooities calculated from
the line shift and the root--mean-square errorare given in Table 1. Aa
may be seeng the velocity of directed ion movement does not exoeed
6
10 cm/sea, and increases with increasing ion charge. There are
Card.1

87459
Spectral Examinations With "Allfall Research S/057J60/030/012/006/011
Installation. 11. Directed Ion Movements B0191BO56

3 figures, 1 table, and 5 roferences; 2 Sovi et, 2 US$ and 1 Swediah,
ASSOCIATION: ' Fiziko-tokhnicheakiy institut AN SSSR (Institute of
Physics and.Technology of the AS USSR). Nauchno--
issl edovateltakiy institut ele ktroftzicheskoy apparatury
(scientific Researeh Institute of Eleotrophysloal
Apparatus)
SUBMITTED: July 15, 1960
Card 2
unlit

S/057 60/030/012/007/011
B01 9YB056
.2 IoZo
AUTHORS: &aXdel-' &J", M%Iyshov, G. M.v Berezing A. B*p and
Razdobarin, G. T.
TITLE: Spectral Examinatione With "Allfa" Research Installation.
III. Time Characteriatios of Plasma Radiation
PERIODICAL- Zhurnal tokhnicheakoy fiziki, 1960, Vol. 30, No. 12,
pp. 1437 1446
TEM, Two methods are described for-reoording the time characteristic
of plasma: a photographic method with mechanical spectrum ocanningg and
a photoelectric method. The mechanical scanning of the photographic
method was carried out by means of a alitted disk rotating in front of
the alit of the apectrograph. The width of the disk alit varied from
0.5 to 2 mrai the speed'at which the disk alit moved past the alit of
the spectrograph was 5 M/seo. In the studies carried out on-this speo-
trograph-it--waa- f ound-- that -the-width~ of line6--dhitil-giid--a-u-ri-n--g- the ra4la-
tion of the plasma. The widths of the NIV and OV linoe and the dis-
charge current are both graphically represented in Fig.3 as functions
Card 1/

87460
Spectral EzamInations With "All.fa" Research $/057/60/030/012/007/01)
Inatallation. III. Time Characteristics of B019/BO56
Plasma Radiation
of time. In the description of the photoelectric method, measurement
of.speotral line intensity with the aid of a photomultiplier and an
oscilloscope is first discussed. By means of a two-beam oscilloscope,
the intensity of the spectral line and the discharge amperage were re-
corded. From the Doppler shift, the authors were ablo to prove an
ordered motion of ions at nuffinAently high speeds, %nd with the aid of
a divider shown in,Fig.9 for the spectral linea,-a shift of spectral
linen could biD determined with high accuraoy. "Wfa" did not show any
difference in the course of intensity of the two halves of t~e line.
Intensity oscillations of the lines having a frequency of 10 cps are
explained by a Doppler shift and by an ordered motion of the NIV ions
along the direction of observatlon. Laboratory Assistant V. V. Semenov
took part in the work. The authors thank B. P. Konstantinov for his
interest., There are 10 figures and 5 references: I Soviet, 2 Hungarian,
I British, and 1 Swedish.
~Aj -
elYY~
Card 2/w
ir

wg~'o jo nju..=
LY
"Ci 1 0 n a f v a -1"1;1.1 LY 0 s
&=n -U(. V",-. t"J.
rL 1; A A
rC _,.t3
I A 14 - I - 0e60 And n total convantrotion ot lithium in the solution
111he tipja naocisosary for a minglo anAlyniz in two
10 mx/litrat
Ao throo mihutea. and the...atnount ot isolution required is about
~7, 5cc. The accuracy of the method"which was represented by a
-,'variation coefficient" was found to be 0~6)6,, 12
-2 t- bles 'and'.'8 referenceat 5 Soviet 'and 3
Thero-are 8 figures, a
r non-Soviot..
Card
0,

20672

S/051/61/010/005/00i/oO
-,- Spectroscopic -De termination .... E032/E
SUT314ITTED iJune ,21, 1960
Legend ofFig.3
lip 1. radiation source (hollow cathode
discharge-tube)
V 2, 3. condensator lenses

.4. ' od lator dine
m U
---5 f lame - of burnor

4 6*, . 8.:monochromators

79 . omultipliera
9. phot
10, 15 Auned amplifiers
11, 14. recording devices
12, -16. sources of supply for amplifiers
15 7 6 13# 17. sources of supply for photo-
multipliers

20872
S/051/61/010/005/001/006
Spectroscopi6 Determination.... E032/E114

M
foe c
NO
Y /
y

- Fig. 4 Fig. 8

" 7
ar
C
.
:
-7 k

r - 1 ~ , ~, , : , - , ,, , ", , : ~, -:. : 1~ ,
*;, i ~-~ ; , I. -:
. i .; . ;: . . I . F

ZHIGIII-ISKIY, A.G.; ZAYDZL,I., A.N,;- WRYMINA) E,A.
Study_ of a direct aurrant are- at elevated pressure. Opt. i
spuktr. 10 no.6:697-701 J6 161. (MIRA 14:8)
(Electric are)

Z11101,114MY, A.G.; 2AYDEW, A.N.p- KVNDj G.G.
Au~ocollimution - 90tup for -tho --ph6tCmlectrlc recur ding - of -
hypOrf4w atruGtures Opt. i apektr, 10 no.6:792-796 Ja 061.
(MIRA 14:8)
(Interforometry) (Photoelectric' moaauremente)

s/o5l/61/oll/oo5/olo/W
E202/EI92
AUTHORSs ,4"delI.._A..X-, and Lazeyeva, G.S.
TITLEi. -Photoluminescence of solutions and crystals or
Sadolinium - salts -
PERIODICALs Optilta i spektroskopiya, v.11, no.5, 1961, 636-61a
TEXTS Photolumine8cence of crystals and solutions of
gadolinium chlorides and sulphates was studied by means of
excitation with light from the iron spark (2700-2800 X). it was
found that the intensity of fluorescence of the neutral nnd weakly
acidic solutions in reduced by exposure to the light of 'the iron
spark. The part of the spectrum responsible for this quenching
was in the region of short wavelengths -4 2600 The quenching
did not reappear upon addition of HCI or H202- -Only qualitative
observations were made in respect of the quenching. Details of
the fluorescence spectra of chlorides and sulphates were given,
including a number of new bands, the presence of which was
interpreted as the superimposition or the electron transition
frequency in the 4f configuration on the Raman valency vibration3
of the hydroxyl group. Unable.to determine with high accuracy

32050
Photoluminescence of solutions and
E202/E192
the absolute vAluts of the decay tints of luminescence for "ach
band, the mithorm compnrod I for d itorlon of wank bands of
luminescence and found that all these values are approxintataly
equal and agree well with the dicay time of the fundamental
electron transition. Finally, it was concluded that the thermal
equilibrium between the two outer excited states is reached in
time which is insignificant as compared with the lifetime of these
states themselves. N.V. Kozyeurova and Ye.V. Kondratlyeva
participated in the experiments. Ya.I. Larionov, G.P. Malakhova
and G.S. Lazayeva are mentioned in the article for their
contributions in this field.
There are 5 figures, 2 tables and 13 referencest 6 Soviet-bloc
and 7 non-Soviet-bloc. The English language references read as
followat
Ref-31 G.H. Dieke, L. Leopold. J.Opt.Soc.Amer., v.41, no.10, 1957.
Ref.61 G.H. Dieke, L.A. Hall. J.Chem.Phys., v.27, 465, 1957.
SUBMITTEDi November 24, 1960
Card 2/2

2563.9
Blio -05
AUTHORS: Zaylic,11, A. IN., Fktrov, A. A., and Ustin~-j,. V. B.
VIT Tilli tml) 1 0. d Id 01. f .4vj~% 'pi
tw k
PERIODICAL: Za-mdakaya la~or~atcxriya, v, 27j no, '96 "401 90?
TEXT: Reprodl.;cible mr-asjurament, 7-aa~,Its ;~f band
on the stable cperati~-:n of bigh,lrequen_;y
isotopir spectr-um armlys4-.s. flic. t%-, formrr au~.bf:,r* 0
a p ek- f r o a k o pl y a 9 ~, 6'1 a t a bl ! Ad a s t_r d rd n , c. e t
e xci ted 1-.Ly a T-W - 2 V h I gli f gf,;ne fv.. Q r f h 1-~,O M,~ r a o
the hyd rogqn a p,~t, truar nzt -,h co vn, jr- pl., I Well,
intenaitoiea of tbetsk-.o0,; -,irmal .4
(-I~. at T~,,/,Tv ~, 11 W-U~ crnly wt,h stq'biPn;:1 fwai-tding
The power aippl,;ed by t,~-a gii-eratr-- 1;~'th on al"G,clutc. ;r.
the mains voltage and rm gmaxat-,r cir-ult, F,,r highcist, ;ntlen-i;~y it, ,3
required; Ri F (I), wbrjxv R jnt~.4rnal generit#.or r-jaistanie. I? H ro-
L -Card 1/8
--4,v U2

-2
atilt) III zol 0
alstance of the disA~arg,-- t-j~-e. S i a d~-ponda nn L h~- g 3L a PZ~.3 U r C,
Ion2
is y flulf:.Iled with ;-~zta~n v-:7.1tag-- Thi~refora, ',r, this
cil-c-ait, 1~ptim%im gas
tion.3 ihow micimum Ptr-
intenolty wit)i ohqngjr~g -v-c1-.agfj. In the 1;G-2 th,J-
tangent, of thc, angle of th;, I f(U r*r )~~O"-'- is
minlm'lm' evien at ojjtlz-n-um g~.:Ls Th-.-i al;'~horrj d,~vt!lop-id the
3F'--3 (VG-3) wlth, 1t;x ~) witij
Fa-rt of the Light fr6m, 0)~-' dL'1,,iAarg-- tu1a- g-e-3 t-~ tbe
converter, It is am~lifi"d in tho fcredtack AT~oulit ', ard arrivqa as
modulation signal at. the high-frequ-~nlv generator. Th~is, a .1.1gh,
change effects a feeding -:.urrent change. The choice of transmission
coefficient and polarity stabilizes -,he lieht' intensity of the discharge
tube. The multistage (;,~nerator permits a rodiiotion ,if thu amplifying
coefficient of th,9 fendback c-ir~.Uft. The gen-iratar power is cortrollrid in
w,4'hou,, mains Currents. Thus, the feedbar:k ampl'fl- ~,ar.
the weak stage- -.1-
operate with direct rurrent and 'tow ampi-lf'ying (,oHff4'.,,%Jent. The 711
generator is built according. to 'he I.nduction circuit with 065 (6P6.) tu-oi.~.
Card 2/8

2563~
S/032/61/027/007/010/012
Stabilized high-frequency generator B110IB203
The-- M-O-d u--I-a-t-- e--d--- b-y- -a---, Yo It age change in the control gTid Of
theJ[2 tube. A 7oltage amf.144tude cf-'20 v is required for 100~1 moelulation.
The suboequent stag4-a .,,cmposed ofJT JT andi7r, tubos according to %n
3P V
ordinary punh-pull i-lrcult a,,-.t as power amplifiorn. The feodback
consists of the photoele,,,tri!2 converter and d-c amplifier, and the tubes
IT69 JfV '7TS' An4)3Y-1 (FEU-1) light amplifier fed by re:-.tM%1ra servez as
converter. For 50'14o modulation, the amplifying coefficient must be -300.
When testirg the ripparatue with hydrogen, the authorr, ~~itAk;ljahed a alight,
efrv~-t nr Owl V,:, on 11V Tho V(;"3 wonootltor With
higher stabiliy th-in VG-2, -;ven without feedback i.,o indt~rond~Ant.
excitation. In the niw g--nerator.. the Iomponsablj v~)ltac;- interval .-. -10,
In VG-~ with arkd qIthout feedba~-k (Fig,~ !)~ the grapha for the pre3rrjz'~,
ence ar ahow thq exlst!,~n~-.e of nPI-111-MijUl F,:-az~lires for mczt :;'ablt,
14
excitation oonrl-itjons-nf the spentr%.- -Tnthr-, new gene:-.::itor, th-zty ara
shifted in tbo cf high pr~-33nras. Th,e valuetil. JA Uentr i "1 1 y
hall' of fhat in IJG-2~ Tho rr~,:~ordtng, of the rliotocurrerit ob, aln,)d frorr, thti
Card 316
77=

S/03"161/027/007/010/012
Stabilized high-.frequency generator... 13110~B203
R lines in luminescence excitation showed better radiation stability fo7
the swttched-on feedba~~k. The high-value of --the --ra-riatlor -Coef f icient-
--(o.6%)- (Table)-le probably due to the instability of thi photoelectric
recording block. The apparratu3 Pan be used forin.3 iaotopic- analysis and
spectrochemical vaa ana!79is where a Gon-d-;~ompoavd apnctral light curre--nt
10 Used U 00htrCt 3ignal. ThA author.,j thank. Ye~ St Fedurkin who supervIsad
the conrsf-v~,+,Ion of th~i apparatua at tha experlmi-'ntal production workshops
of the NIPI LGU. There are 3 figvres, ! table ,and 5 references; 4 So-fle-
,bloc and I non-Soviet-blon. The reference. to the Enelish-language
publication.reads ae follows: Ref. 10; H. P. Broida, M. Silgin, H. J.
Morowitz, J. lies. Nat. Bur. Stand., 52, 293 (41950-
ASSOCIATION; Leningradskiy goaudarstvonnyy vni7ersitet im. A. A. Zhdanova
~(Laningrtid St-,%to University imoni A. A. Zhdanov)
Fig. 1. Dopenden,:)e of the relative change In intuncity of hydrogen lines
with changing feeding voltage of the generator.
Legend: (1) VG-2 generator, (2) VG-3 generator without feedback, (3) VG-3
generator with feedback.
Card 4/8

ZAIDEL fA.H.1 FILIPCIIUK, B.I.; BABKO.. A.K.; SHAYEVICHO A.B.1 DDLIR801K.37, T~.F.
On the lextabliahment-of standarda,ln the mathods.of presenting
oxporlmontal d&ta,__Z%v,lab, 27 no,,1012273-1278 1614
(141A& 34tio)
I* Fisiko-takhnichookiy inistitut AN SSSR (for Zaydell). 2. Vea-
noy=nyy nauchno-issledovatellskiy inatitut metrologii im D. I.
Mendeleyeva (for Pilipchukp Dolinakiy). 3* Inatitut obsbchev i.
noorganichaskoy khJull AN USSR (for Babllco). 4. uraalskiy pauchno--
issledovatellskiy institut chernykh metallov (for Shwevich).
(mathe=tical atatistics)

6/057/61/031/002/001/()15
/.P- 0 06, po, B020/BO56
AUTHORSt Zaydell A. N., Malyshev, 0. M., and Shroyder, Yet Tat
TITLEs Speotroocopic methods of studying a hot plasma
PERIODICAM Zharndl tokhnichookoy fizikip v. 31, not 21 1961, 129-166
TEXTt This is a review of articles dealing with spectroscopic studies of
a hot plasma within the spectral range of some ten to 7p000 A# Plasma
luminescence is characterized by the energy distribution over individual
wavelengths, which# in' turnt is characterized by the intensity, width,
and oontours of the spectral liney by the intensity of the continuous
spectrum, etc. From the width of the spectral lines# tbe.tomperature of
the ions, and from the shift of the spectral lines as a result of the
Doppler effect, the direction of the controlled ion motion is determined.
From the intensity of the spectral lines, the electron temperature in the
plasma may be determined. The concentration of the charged particle is
aeterminea from the intensity of the continuous spectrum of bremestrahlungp
the contour of lines, as well as the shift of the boundary of tho spectral
series. On the basis of the intensity of the spectral lines of the
Card 1/"

S/057/61/031/002/001/015
Spectroscopic methods of ... B0201BO56
impurities emitted from.atoms and ions, their preeenoo and concentration in
the gas, in which the discharge occurs, m4y,be determined. From the ratio
between the line intensitiles,_ also _the Aegree of-- ionization of the plasma
may be-doter-min-od.- Fig. I shows the contours of the line NIV
(A 3479 A) averaged over time and the radial direction by means of the
experimental values obtained by L. V. Sokolova in the device "Allfall.
Fig# 2 was obtained on the basis of the spectrogram recorded by the
apeotrograph ViCTT-28 (ISP-28)t and Fig- 3 on the basis of the opectrogram
made by moans of the spootrograph A~C -6 (DFS-6),, Fig- 4 shove the
optical scheme of an arrangement for measuring the velocity of controlled
ion motion. The velocity of plasma ions measured by means of "Allfall is
given in Table 1. Fig- 5 shows a diagram, from which it may be seen that
the main part of light energy belongs to the wavelength range 1100-1400 Ap
which was used for measuring the absolute energy losses by means of
thermoluminophoreas For this purpose, the-monochromator or spectrograph
must be calibratedt two pairs of lines being selected for each element
(Pig. 6). Further, the ratio between the main quantities of plasma lumines-
cence, was, dealt with. The most important method of characterizing plaama
Card 21V

-------------
Spectroscopic methods of . . .
lum`neac.-nce with respect to time is long-time photographing. An example
hereto is the spectram shown injig. 7, which was takon by moans of
"Allfa". Among the methods of investigating tho time characteris~Uclj' of
lino contours during the discharge pulse, the method of splitting spectral
lines is mentioned. Mention is made of A. A. Vaynshteyn, I. I* Sobellman,
S. E. Prish, Yu. 1-1. Kagan, V.'.1. Xogany V#- .-Do Kirillov,, Av Be h6rezit, -
S. Yu. Luklyanoyl and V. I. Sinitsyn, There are 14 figurest '2 tables,
and 119 refereneost 57 Soviet-bloo. and 55 non-Sovie't-bloc.
't' Fiziko-tokhni6heiskiy institut im. A. P. Ioffe AN SSSRI
ASSOCIATION
-Loningrad (Instituto of Physico and Tochnology imeni
J, A. P. loffe AS USSR,, Leningrad)
SUBMITTED: 86ptember 14; 960
Card 3/ 14

ZAYDEL'p A.N.; PRDKOFIYEV, V.K.; RAYSKIY, S.M.; SHREYDERP
pK.P., rOd*; KUZNETSOVA, Ye.B., red.; IMUM, X.F.t
takhn. red,
[Tables of opectral:lineo]Tablitay opektrallnykh IInIj. Izd.2*,
ispr. i dop, Hoskvao FismAttin, 1962. 607 p. (HIPA 161l)

S11691621000101210061093
D228/i)307
WT HOI
22 Z a de V A. 11 zhiglinskiy, A.G., and ~,und G.G.
y
TITLE: Isotopic spectral'analysis
1)EIZICII)ICAL'. 111-el"(1rativnyy zhurnal, Geofizilca, no. 12, 1962, 10,
abstract 12,.80 (Byul. Komis. po opredeleniyu absol-
yutn. vozrasta geol. formatsiy, XN SSSR, no. 5,
19621 60-62).
TEXT: The most prevalent, accurate, sensitiveland univcr-
sal method of mass-spectrometrically 4eteftining iaotopic composi-
~tion involves various difficultlen-of principle and technique.
Spectral methods based on the differences existing in the atomic
and molecular spectra of different isotopes employ the simpler-
equipment and require less time. I-A'ethods of spectrally determining
the isotopic coutpobition have been employed for a series of elements.
The authors are now uorleintf on new mathods for deternininZ~ the iso-
ij
topic composition of inagnesium, and oxygen. 'Equipment with a resolv-
ing power of up to 106 for studying atomic spectra generally con-
Card 1/2

Isotopic opectral analysin !;/1,69/62/000/012/006/095
U228/1)307
Gists of a light source (hollow cathode, high-frequency discharge
tube), a pre-analyzin(f monochromator, a Fabri-Pero interEerometer,
and a photoelectric recording photometer. This apparatus detcr-
mines -the isotopic Composition with a precision of from tenths of
a percent to several percent of the specific concontration. Equip-
ment for determining thc, inotopic composition from molecular spectra
does not require an intarlerometer but usually contains a spectro-
graph i:ith a rezolving power of - 104; an are serve; as the ligh4 ------
source. A new method is -ased for determining the isotopic composi-
tion of hydrogen and uranium, based on the measurement of the vapor'
,with isotopic composi-tion. Determinations of the isotopic composi-
tion. of strontium carried out by the authors gave an accuracy of
3-5%, and. lasted about hours. -i'dork by the authors on improving
the isotopic composition of lead increased the mea*surement accuracy
for all isotope concentrations by 2-30/1 of the content of each iso-
~tone. 27 references.
Z~~ibstractcrls note: Complete translation-7
Card n12

ZAYDELI, A#N,
Concerning I.S.Pominov?a article *Absorption spectra of neodyzitm
chloride in aqueous-a.Icohol-ic solutions at low teq3eratures.!R
Opt* i spektro N ne.6;804 Je 16Z (KRA 1515)

33431
S104616~16~61001100 /0
1
3 go-o 3 71 3 Cl 51!~ B125/BI04
AUTRORSt ZaydeP, A. R., Lazeyeva, G. S., Ostrovskaya, G. V., and
fa-kimovat P. P.
TITLEt Luminescence of gadolinium salts
PERIODICALi Akademiya nauk SSSR. Izvestiya. Seriya fizicheskaya,
ve 26, not it 1962P 74-60
3+
TEXTs ',The luminescence spectrum of the Gd ion has been thoroughly
invest'igated on GdCl 3* 6H 20 and on a 0.1-1% aqueous solution of GdCl 3;
Gd 2(SO4)3* 6H 20; Gd2 (SO 4)3 1 Gd2(SO 4)3 ; and Gd (C2H5_SO4)3 . The spectra
obtained from a synchronous spark phosphoroscope were recorded by a
high-power E-517 (Ye-517) quartz spectrograph at room and liquid-air
temperatures. Irradiation.with the light of the iron spark sharply
reduces the intensity of luminescence of the GdCl solution (concentra-
3
tion,-0.1-1%) in neutral and weakly acid solutions, while it is much less
decreased in acid solutions with H01 excess. The decrease differs with
Card 1/4

33h3l
S1048
/62/026/ooi/007/018
Luminescence of gadolinium salts B125/3104
different solutions. The luminescence.of solutions cannotbe restored by
boiling, addition of E01 or H 202' or by precipitation of gadolinium.
Solutions of normal luminescence are obtained from the precipitated
hydroxide after an appropriate treatment and dissolution in HC1. It was
not possible to clarify the mechanism underlying the quenching of
luminescence of the solutions. The two principal luminescence bands
(3ilO and 3060 R) of the gadoltnium. salts are very narrow even at room
temperature, and are split up into several components. The spectra
of GdCl 3* 6H20 and Gd 2(SO4)3. 8H20 crystals exposed for a long time also
exhibit a 'narrow doublet of 3002 and 3005 1 and a few weak diffuse bands.
Apart from the principal bands which are more blurred, ithe spectra of
solutionB of gadolinium chlorides and sulfates are similar to thoso of
crystals. Although the spectra of the individual salts show the same
bands, they differ in many respects. The significance of the individual
parts of the spectrum is shown. At liquid-air temperature, the structure
of some diffuse bands booomen more distinct, According to Ye. V.
Kondratlyova and 0. S. Lazeyeva (Optika i spektroakopiya, 132 (1960)),
Card 2/4
"P`U~ K 2 MAM P_ ~t
M

31431
S/048j62/026/001/007/018
Luminesce'noe of gadolinium salts B125/BI04
the photoluminescence,of gaaolinium salts has a lifetime Ir-10-3 sec and
is damped exponentially. The exact lifetime for the 3110 1 line is
2-10- 3 soot and that for the 3060 1 line had previously been estimated at
10-3 to 10-4 sec. The latest measurements of the authors with the
synchronous spark phoophoroscope have shown that for the two lines
mentioned before$ the lifetimemare consistent with an error of about 10f4.
The band intensity ratio for 3110 and 3060 1 is nearly equal to 20 at
room temperature. The damping times of the bands at 3470, 3220, 3160,
and 3145 1 do not considerably diverge from that of the principal
elootron transitiont whioh indicates that the bands are produced by the
superposition of vibration frequenoies-over the frequency of the
principal electron transition. There are 7 figuress 4 tables, and 12
referencest 6 Soviet and 6 non-Soviet. The reference to English-
langlaage publications reads as followst Dieke G. H., Hall L. A., J. Chem.
Phys. t 27'0 465 '(1957).
Card 3/4

M- ~Vi7
33431
5/046/62/026/001/007/018
Luminescence of gadolinium salts B125/B104
ASSOCIATIONs Fizicheskiy institut Leningradekogo goo. universiteta im.
A. A. Zhd&novv4 (physics Institute of Leningrad State
University imeni A. A. Zhdanov)* Pi2iko-tekhnichookiy
institut im. A. F. Ioffe Akademii nauk SSSR (Physicotechnioal
Institute imeni A. P. loffe of the Academy of Sciences
USSR)
Card 4/4

B/048/62/026/ool/002/(J30
B104/B136
AUTHO"S; Zaydel', A.' list Zhiglinakiy, A. Gap and-Karklina, E. As
TITLE: Study of the direct-current aro at elevated pressure
?T;R-LODICLL; Akademiya nauk SSSR. izvestiya, beriya fizicheakayap
v. 26, no. 7, 1962, 855-857
TEXT: A previous paper (A. IT. Zaydel' et al Optika i spektroskopiya,
2, 28 (1957)) contains the description of an experimental system designed'
to stUdy Li and Cu spectra in dependence on the pressure of the
a-+,-i!OSPIlere--Sur-rour4ding-the-arc-.-At-a-ailr ounding-CO p;-essure-of-7-atm.
er
thp Li 1 6707, Li 1 6103., Cu 1 3274, and Cu I 3247:31nes have much great
intensity than at 1 atm. The relative intensity of the Li lines was 11
times higher than that of the background. The plasma temperature is
anouined to increase with precoure. Tho,ratio between the emitting
11ton-1101(joul'o oollinion oroan nootiono doon not dapand on prconurol-and
the optical density of the layer absorbing.the two'JA linau remains
uijaltered. Thusp the light source described in the previous paper
provides a means for improving the accuracy of spectral analyses.
Card 1/2
5
W IV

_~AY-~ELIO-AAL PETROVO A.A.
Spectral-isotope method of determlnlng nitrogen in metals.
Zav,lab.- 28 no.5:552-555- 162. (KRA 15:6)
1. Leningradskly Cosudarstvennyy univeraitet,
(Gases in metals) (flitrogen-Isotopes) (Spectrum analysis)
T7 ~M
zz
3 F
RTRI

-i/057/62/032/003/016/019
B117/3101
?16 - -k
A UTHORS Konstantinov, 0. V., and Xalyshev, G.
02
TITLE: Spectroscopic meaaurementB of ionic energies on a etall-
.type plant
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 32, no. 3, 1562, 370 372
TZXT: The relationship between ionic energy and nuclear-charge number was
checked on the basis of,experimental data. A relationship between the
ionic ohargo and tho;width of npqotral linou of thone ionn had alroady
been catablished in the firnt 'investigation conducted on t1w "ZoVa" plant
(Ref. 1, see below). ;.-ost of the results were oatisfaotorily.descrfbed by
-the relations Li - Uz (1) or Bi - ~z 2 (2). The data determined recently
by Jones andWilgon'(Ref. 10, see below) on the same plant concerning
energies of ions with different mass and nuclear-charge numbers ivere ex-
plained by stating that the ionic energy as a function of charge was
purely accidental. They suggested the following relationst
Fji rv 2/,, -- Idi Iand E
z i constf
Card 1/3
""~2 0

S/057/62/032/003/016/019
Spectroscopic measurements of... B117/B101
too- lation formula E
and used a two-term interpo i E0 + (mi/blj~)e (3) to'
attain an agreement between experimental and theoretical data. They
assumed "thermaliz.4t ion" of the plasma. A calculation of the data given
in the paper mentiohki, however, showed that the experimental results were
aescribed equally~ well by the interpolation formula'(1) with only one
parameter as by formula'(3),with two parameters. Thus, the investigations
con6ucted on the %3e4all and "Alf_O.II_Vlants confirmed that the.energy of
ions increased with incr6a" .I charg~'n'- 1 , -M-~s
umbel. Pormlu a
pin; n4g I
found to give a deuteron tebpe ra.,.U.~ ;of- rAe.v#chanj.~p of jonic
N100 P, I
ic
acceleration by electrostatic f ld ,W'plaawa .tj~ 0
possible for the "Zeta" plant eit her, . presuppo4e a~duuteron temperature
below the e1 ectro~n,-*t-emperature (20 - ~30 ev), i.e., near the value of u in
(1). Thure are I t ,aA lo and. 13 ref oz~enoer; 1 2 Soviet and 11non-Sovicit.
'Oho four most recent 'refere'nces,to'E~gl!ish-la~gu&~e. pi#licat~pns read as
lollows: Ref . 1 R. C. Thonem~nn et Naturq,-,. 181, 217, 1958; Ref - 10-
B. 13. Jones, It. 7illpon.- Report no. 05T..-read al~,t .We Konferent3iya po
issledovaniy o yadernogo sinteza
am v oblasti fiziki plazmy i upravlyaye-MOS
(conference on InVe~tiza'tiona'An"-ihe. Field 4~,I?laswa Physics and Controlled
Nuclear Syntheois)i 5alzburg, 19611 A. S. Kaufma4 pt al..Proo. Phys. 5oc.,
76, 17, 196oi B. Berlnsteiin', R. 1:..Xtxlsrud. Phys-Fluids, 957, 1960.
Card, 2/3

S10571621032100310161019
Spectroacopic neazurements ofe 0 3117/BlOl
ASSOCIATION; Fi-iko-tokhnicheskiy institut im. A. F. loffe AN SSLIrtf
'j "
Leningrad (Physicotochnical In3tituto imeni A. F. Ioffe
AS USSR, Leningrad)
SUT141TUDi November 23, 1961
Card 3/3
am amp--

AUTHORS: Zaydel', A. N.; Maly*shev, G. M.; Oatrovakaya, G. V.
TITLEt Use of laoor for quantum diagnostics
~:SOURCEI: Diagnostika plazmy* (Plasma diagnostica)l ob, statay.
f,-"-MoscOw-I Gositomizdzkt, 1963, 31-35
TOP IC TAGS: plasma, plasma diagnostics, plasma diagnostics with
laser, laser, plasma electron density, plasma electron velocity
distribution, plasma noise, ruby laser, light energy threshold,
free electron scattering
hi
1,-~ABSTRACT: The range of electron densities and temperatures in w ch,
i Ythe scattering orf light from a ruby laser by the plasma electrons
be used to determine the electron density and the electron ve-
t
'locity distribution function is evaluated. The expressions obtained
-under some o
implifying assumptions are
W5,

AT40251*200
''~,14ACC99910N NM
130 w kV
no Ah
no LA jf251A
MV
11.~'.,'for the minimum and maximum measurable electron density, respective-I
:`ly. It is assumed!~that the threshold of measured light energy is J
;~.-determined by the fluctuations in the number of photoelectrons pro-
duced upon qcattering, and that the main sources of noise are the
.:,,,Plasma intrinssic radiation and the light scattered by the various
parts of the apparatus. While the latter cannot be evaluated in
t'._.general form, an estimate made for a specially-constructed small dis-
!-charge tube,sh6ws that the proposed method can yield Inew data even
ith currently available equipment. Orig'. art. hast 1 figure and
w
l
ASSOCIATIONs* None
190ct63 DATE ACQ: 16Apr64 ENCL: 01
.90 REF SOVs 002 OTHER
SUB CODEz PH z 004
Card 2/

-71M A G.; ZAYDELI, A. N.
"Ccntem;~orary Yethods for the Spectroscoloic Deterzdnation of the Isotopes
of the Elements."
report submitted to 11th Intl Spectroocopy Colloq.. Belgrade, 30 Sep-4 Oct 63.
Boom

ZAYDELI, A.-H.;-PEIRGVO A.-A. _7
.. . ......
"Spectral-Isotoptc Method for the Detemination of GaBes in Metalf3."
rep,ort submitted to llth Intl Spectroscopy Colloqo Belgrade, 30 Sep-4 Oct 63-
Physico-Technical Inst im A.F. loffe, AS USSR, Leningrad.

Rn

ZHIGLINSKIY~ A.G.1 A.~t~t; PETROV,-A,'A-,
Speetral analysis of isotopic composition (survey). Zav.lab. 29
no.5s550-552 163. (MIRA 16s5)
(Inotopes-Spectra)

ZAYDELI, A.R,; IVANOVA., T.Fa; PM07j, A,A,; FEDOROVP V.V.l
N.M*
Unes of.tba.spectral-lootOpi-o-method of,determination of gaoso
in metais. Zmv. lab. 29 no.6t693-~695 1630 (KULA 16ir6)
1. Fizichsakiy inlatitut laankmdiskogo paudarstvannogo uni-
veroiteta imani A.A. ZbdiaoTas
(Gasse in metale)-Aspoetrum analyoio)
Ndtotaotopos)
777777L,

V, T"
N.-: KORENNOYJ-
L
the method of
Determination of the isotopic composition of lithium b.
atomic absorption, Zavalab, 29 no.12:11449-1450 '63. (KRA 17t1)
SM~;4: MEN"

9/057/63/633/002/010/023
AIN110118: Z Malyahev, Oo got and Ptitaynap Y*# A.
TITLE: Spectroscopic measurement of the electron temperature in the
"Alpha" machine
PERIODICAL: Zhurnal tekhnicheakoy finikig Y. ~31 no. 2, 1965t 200-204
TBXT: The plaam~ electron temperature In the Alpha machino won determined
frow the intoneity ratio of ooveral paira of spoctral linva. pertaining to
different degreos of ionization of oxy6ant nitroijant and carbonq Tho
intensity ration were determined from the timo-baso awoep, of the spectra
(resolution Os3-0&4 Peec) taken under the conditions (1) 1112 a 100 00,
10 kv, n 350 pulses and (2) 1). 7, i6o on, U a 15 kv, n a 150 Pulecoo
in a hydro Igen plasma 1-10-4 Dim Hg) The results were evaluated with
the formula
Card -1/ 3

3/057/63/033/002/010/02~
Spectroacopio measurement Of B108IB186:
AE.
k7,-
A
foe V04
.7.3. *is Vitt
At,,
8.3 10K. fjs U.
oil
where the subaorlptsI and 2 Indicate the speatral lines from ions with a
degree of ionization of (L+1) and Is respectivelye A Is the transition
ki
-probability#fOk the osoillator strength# Yki the frequency# 2athe
excitation potential# I the intensityp ~, and the ionization
potential of hydrogen and of the given ions a the main qua4tum numbers
-~n the number of electrons an -the orbit with no The factor g accounts for
photorsoombination onshelle higher than at while fIand f2 are oorksotions
forthe oross sections of photorecombination and, impaot.104isation- The.
GaM 2/3

.8/051/63/033/002/010/023
Spectroscopic measurement of Bioa/BW
results.ohow,ed.that the electron temperature rises with increasing degree
of.ionization.. The oonsiderable deviations from the Maxw4llian velooity
distribution of the electrons Oda be explained by the simultokneaue
emission from ions of different degrees of ionisation. Also the varying
of-the emisnion.with--time may affect-the results. There are I figure and
ASSOCIATION: Fiaiko-tekhnicheskiy institut in. A. V. loffe AN SSSR,
Leningrad (Phyaicotechnical Institute imeni A* Fo loffe
AS USSR, Leningrad)
UBMITTED., February 23# 1962
Card 3/3

=ESSION NM APhOO5080 8/0032/63/029/M2/2a9A450
AUTHM s ZWdollq At He; Koronnoyp lot P,
TITLEs Determination of Uthium isotope composition by tho,gtomi* 4corptioft
method
SOUICE: Zavodakap laboratoriya., v, 29t noe 12,, 1963# 1449-WO
TOPIC TAGS: lithium, isotope composition, atomic absorption method, isotope
analysis,, atomic absorption spectrosoopy, absorption band methods lithium 6
lithium isotope composition., lithium iaotope,, atomic "otrums, lithium atomio
Tirum.
Gpoo
ADSTWTs Two mothods are presented for lithium isotope anolysins the aton,
J absorption method and the omission method, Two tynea of solutions were usod con-
nd 3.00 m~lior of lithium with lithium.
j taining concontrations of 75M&Aitor a
6
'isotope Li content varying from 2 to 45%. A h613Aw cathode containing pure L,6
served as the r&liation dischargo tubo in tho first method, The isotople oontaut
k. was datoxvdzod from
+
Corti 1/2

ACCEW1011 NRt AP4005060
whom --a Li6atom aoncentration#-n7 U7 concontrationp-and
6/(n6'n7 n6
absorption coefficient* In the second mitliod a torch fl=o was usod with UT
vapor for. aboorption. The jj;.T/In4 plot shows a straight line with a mazimium emor
concentrations@ Orig* art* hast' I equation.
of. 2% for 2to 91% 06
=OCIATION t Fiziko-tokhnichoskljr inatitut Akademil Pauk SSSR (P4vicotoehnical
Institute# Acadoqr 9Z Solonoes SM)
=MTEDs 00 DATE ACQj 19Dec63 ENCL 1 00
SUB CODE: XC Norm ISOV 1 002 OTHERs 000
;-Card2/2.

ACCESSION'NR:' AP4042989 S/0051/64/017/001/0129/0134
AUTHORSx Zaydol', A. N.-I Maly*shcv, G. M.1 Shreyder, Ye. Ya.
TITLE: On the Fiensitivity of spectral-analysis
SOURCE: Optika i spektroskopiya, v.. 17, noo 1, 1964, 129-134
TOPIC TAGS: spectrum analysis, light sensitivity, photometry,
photographic,cmulsion, photoconductive detector
ABSTRACT: lqie offect of the method used to record the apactrum and
of the parameters of the spectral instrument on the sensitivity of
a spe#ral analysis is investigated as a function of the character
of the" inten.,i ity-ine-asurement errors. It is shown that the nature
of the errors determinedthe requirements governing the choice of
the spectral instrument and the.registration time. The optimal
registration time in the analysis of small amounts of substance is
;estimated. If a photocathode is used as the radiation receiver,
the decisive analyzi(i error can be connected either with the fea-
tures of the ine-asuring circuit or with the fluctumtions e1 thi
:'Card
1/2

,,.ACCESSION Mt- AP4042909
!,measured. signal,, depending on the size ofthe noise background. In
the case when an erwulsion . is.-used, . the photometry, area . determines
;-the type of predominating error, although the fluctuation error is
;'decisive in the majority of cases. Regardless of the radiation
.,,receiver employe;.dr the sensitivity of the analysis shows 'similar
dependence on the i3pactral instrument parameters ouch an the spectral.,;
gap width, dia'ersion, and area of the dispersing element, so that
p
i,the dependence of the sonsitivity.analysis on these parameters is
affected primarily by the ratio of the two types of errors. The
aria-.
optimal registration time can be determined from the law of v
tion of the npactrial line an the sample in connumed, Orig. art, hasilt
14 formulae.
i ASSOCIATIONt "None
SUBMITTEDs 26Jul63, ENCLs 00
SUB CODE: OP~. -NR.REP SOV: 009' OTHER# 003
~-rd
2 2.

...Aleksand r fla t anovicb; ret), O$I'4OV6jUY
[Fund&menta-lo of spectrtm analysis) Onnovy spektra.11nogo
analiza. Moskyap Naukap 1965. 32.2 p. (MIRA 1834)

-AYDELI, A.NI.
Appraisal of taeaimrsmont errors. Usp. mu? e5 no.2091
F 165. 18:3)

Ald
-. R,
~Nz
E3

ZkYDELI) A:Lrkserdr Vatanovr-11
(jvnjuat!.on3 Of
eranil. MoskVili IFXI]knp 79
riyo otsonki oshlbOk lzu, (IKIRA 18-9)

I I ~ - -.-. ,..,-.-p -, -
a
z - , J, ., . . - , ..- ~ .: z~~ .
: ,, zl -i-F-~'l-,-.1-r~-~j- -.". " 4~~
- . i ~, , R t, I , , P 'I ; t " , ,
~'- : V ~ , ;'. , - . a
WIl . '7, ~~A ; 1,6 , ; ,
'Will A , , , 'I- ', ~;, . .

M'Mt0 "W

". - - -, ., - -I-ow-m -,f
~ ~=Ar-~ i~4~ '7- - iggg ~ 'r
I - ~n
'A -14~
. - - ll~f~ F2 ", - n~.;
f,fv'~- F- f, ~-.
- -T-wPF467 - I. 105~;~

WAS

I - I jF COL, 5

#--A 4 6'4'*
SOMICS CODS; 911
ACC NR p700 5
AUTHORI 4yt1oj'# A* No: Konotantinovi V* Doi Outrovulk, YU0 If
ON: PIWOico-tochnical Institute imo A. Fe loffe, All SSSR Miko-tokhrdehoaKy
institut W9_d_S_Sk_Y_
TITIBi _Lsuor poaolution moasurawnt
SOMCE: Zliurnal nauchnoy i prikladnoy fotografti i kinomatograf3A, vo n. no- 5,
1966, 381-382
TOPIC TAGSi gau 1nuort photographic film, photographic o'rftduion, lauor application/
Mikrat-600 photographio f i-In
ABS MICT: A brief description is given of an expeAmental use of a 6,328-3nja~trom
neon laser as a source of light to measure the resolving power of 14ikrat-600
"film by the interference inethod. The."resolvogramo" Were stwied by two methoda..
,examination under the microscope and eyamination as transparent diffraction
!gratings) the second method being preferred because of simplicity) greater senal-_
~tivity and the abiliiy to determine the frequency-contraat characteristics of
.cmacion3) vhcre by the ratio of brightness of the zero and the first diffraction,
maxima can,be used an a mccopro-gf.the contrast of the image,, and can be measured
directly. 'Tho autlioro'iflank To 116 L'ovanbarG ror consuItationao Orig* art** hast
2 figurolj# finis: 38,96-iT.
. / - ORIr 002 OTH REFs 001
SUD CODES 14f 20 Sum DATE i 29APr66 REFt
001 -535024*64"621#375.9
Cord 3-11

L 4"WA-4bf,
ACC NRt
-SOURCE CODE Xi
r
AUZIOR; henko. T. F., Zaydell A. If.; Oa!~r~
~Yevtus _21aya L y.; Chelidze, T. Ya.
ORG: ttY.!_i_02~_t~e_chnical Institut'e im. A. F. Ioffe, A14 SSSRI Leningrad QlziRo-
taklinicheakLy Lnutitut AN SSSR)
TITLE: Spectroscopy of a laser apark..T 1. Spark in helium 1
SOURCE: Zhurnal tekhnicheskoy fiziki, v. 36, no. 6, 1966, i5o6_1513
TOPIC TAGS: nonlinear optics, laser Induced breakdown, gas breakdown, helium, argon,
hydrogen, air breakdown , laser beam, spectroscopy, laser radiation spectrum,
spectrum analysis
ABSTRACT: Laser induced breakdown In pure and hydrogen-doped helium under pressures
Xrom I to 10 atm and In air and Ar-112 mixtures was Investigated spectroscopically.
i-c t ulse 30-40 nan see
ruby laser which was Q-switched by means of a rotating prism. The laser bean was
focused by means of an f:25 mm lens Into a metal chamber equipped with quart:. windavp
which could be filled with gases at pressures up to 10 atm. The spark could be
observed in the direction perpendicular to the laser beam. The magnified (1.6 times)
spark image was focused onto the slit of an ISP
-51 spectrograph by means Of (L
Jupiter-3 objective. Spectra obtained in this manner indicate the spatial d:lstribu-r,
tion of the spark emission. The temporal distribution of the spark was observed by
means of. an SPR photorecorder. A spectral analysis of the laser-induced spEL:rk in an

L U090-66
ACC NRt AP6028 C)~8
-12 mixture was made and photographs with the time resolution of various stages o.r
He 1
the spark development were analyzed. The dependence of the 11 line halfwidth an the
distance from the spark axis was shown, Tabulated data Indichte the effect of
pressure and the corresponding electron concentrations on linevidth broadening (see
Table 1). The relative error of tabulated data was 20-30%. The preliminary resulfs
table.l. Linewidths in a laser spark spectrum In pure and
hydrogen-doped helium at a pressure of 2 atm
I A Line,
e
lie 16678 lie 14471 25 05
90 '0
He 1 5876 10 1 1
His 1 W16 9 1.6 11 10 41.8
Ile 14713 5 05 14- 60 62
Indicate that the spark plasma goes through two stages. During, the first stage 3
(-100 nonoacc), the plasma has a high electron temperature and density ('10" cm-
during which an intensive continuous spectrum is emitted and a considerable line
broadening of the neutral and ionized atom occurs. The second stage, which lasts tend,
of psec, corresponds to a gradual cooling of the plasma, during which only the neutrfil
atoms radiate. The electron concentration in the Initial development stage of a
spark W He was found to be similar to that obtained for air breakdown elsewhere
Card 13

L L-1090-66
ACC NRz AP6028628
1964 (5.1017 cm-*I*,
(S. A. Rwmdcn and W. F. R. DaVits, Phys - Rev. Lett., 13, 22T,
cmd Is.
and S. L. Mandel'shtam, P. P. Pashinin, A. V. Prikhindeyev, A. M. ProMorov
Sukhodrev, ZhETF, 47, 2003, ig6h). A refined treatment of the present work vill
a (Y-&
'7 figures and 2 tables.
.ppear shortly, OriSo art. han:
SUB CODE: 20/ SUBM DATE: 22mar66/ ORIG REF: 0021 OM REF:' 003/ ATD PRESS:
1W
ad
U~G~M3

L 44722-66 EwT(l)
ACC NR, AP ,663-1276
AUTHOR: Konstantinov, B.-P.; Zaydell, A. N.; Konotantinov, V. B.; Ostrovskiy, Yu. 1.
ORG: Physico-technical Institute im. A. F. Ioffe ANI SSSR, Leningrad (Fiziko- ~7'f
tekhnicheskiy institut Ali SSSR)
y. xperimental techniques and the resoluticn of method
TITLE: 1!21S&Laph
SOURCE: Zhurnal tekhnicheskoy fiziki, v. 36, no. 9, 1966, 1718-1721
TOPIC TAGS: holography, hologram, laser photography, C4"~O~_
ABSTRACT: Experimental holograms of half-tone and two-_ALnd three-dimensional objects
were made by means of standard equipment assembled on aPOSK-2 optical bench.10 A
Zenit-3m c&.mera was used with a 35-mm Mikrat-600 emulsion, whose maximum response was
at 6400 X. -Resolution was not less than 1420 lines/mm. The quality of reconstructed
images was enhanced by suppression of nonaxial modes. The angular resolution of
5 x 5 mm holograms was 3 X 10-4 radians for high-contrast reconstruction. Apparent*
_quality _.de grktdation was observed in holograms which were 10 x 10 mm and larger. The
degradation was aitrlbuted to-effects-- caused by film-bending an~d_eMUl_sio_n surface
inhomogencitieu. Orig. art. has; 3 figures* IYKI -
SUB CODEA20/ SUBM DATE: 27Apr66/ Vial a F: 002/ ATD PFE881 5080
blK

A:CC: NR,_'Ak700l32l_ SOURCE e: W605T[6616_36[01ili~~I_i_2
ALITHOR: Zaydel', A. N.01 Ontrovakayap G. V,; Ootrovokiy, Yu. I.; Chelidze, T. '18.
ORG* Physicotechnical Institute im. A. F. Ioffe, AN SSSR, Leningrad (Fiziko-
tek;inicheakiy institut AN SSSR)
ITITLE: Holography of a laser spark with a temporal resolution
SOURCE: Zhurnal tekhnicheskoy fiziki, v. 36, no. 12, 1966, 2208-2210
TOPIC TAGS: holography, laser photographyl plasma photography, Sclilieren.photography
ABSTRACT; Shadowgraphs of laser-induced air breakdown were taken by means of the
3-beam setup shown in Fig. 11 using a method of spatial-temporal separation of light
pulses employing a system of semitransparent mirrors patented by one of the authors
in 1963. Shadowgraphe can be made of various stages In the development of a single
diucharge. The ohadowgrapho can be conoldered Gnbor hologrittan of a lAnor apark.
Image reconstruction was carried out by means of the system shown in Fig. 2. This
sys,tem is actually a Schlieren setup in which the image is formed by rays deflected
by the'phase inhomogeneities of the object, The electron concentration Ne in a plasma
was determined experimentally for different stages in the development of a plasma
during two dischar�es, The average Ne for the first 120 nanosec (accuracy 30-50%)
was 2.4 x 1019 cm:- which agrees favorably with results obtained from 1) displacement
of the interference banda (A. Alcock, E. Panarellas S. Ramadeng 7th Interne Conf.-
Card 1/3 UDC;_ 533.9.07,

ACC NRi AI?7001321
Fig. 1. Setup for obtaining shadowgraphs
Rotating prism Q-switch; 2 - ruby
crystal; 3 - glass plate; 4,5 - lenses;
6 - pgism; 7 - mirror (99% reflective at
6943 A); 8 - mirror (50% reflective);
9, 10 optical glass wedges; 11 film;
12,13 diaphragms.
Card 2/3

Raw
ACC NR,7,Wfo1Yf321
A' r -
2F -4
Fig. 2. Schematic for.hologram reconstruction
It hologrami LjjLj - diverging lenses; L - He-Me-
laser (6328 A);'I'-: image (real); L' - converging lens;
3
P film.
on Phenomena in Ionized Cases, 1965) and 2) a scattered laser beam (S. Rawiden,
W. Davies, Phys. Rev.'Letts., 13, 227, 1964). orig. art. has; 2 formulae and
4.figureso [YK1
SUBM 6ATE.-- 18 5110
SUB CODE: 20 May66/ ORIG'REF: 003/ OTH REF: 006/ -ATD PRESS 511
[Card- 3/3-

NIKOLISKIY, B.P., glav. red.; GpIGOROV, O.N., doktor khim. nauk, red.;
FORAY-KOSPIT-9. R,A.,doktOvMdOw; nauk,,r~FGMjISM�WMMj&-.
P.G., r()d.j FRIDRIKIISbERG,
jj.A.j kand. khim. nauk,, red., RABINOVIGHP V.A.p kand. khim.
naukj red.; RACHINSKIY, F.Yu., kand. khim. naukp red.; UYDELI
A.N., doktor fiz.-mat. nauk, rcd.j ZASLAVSKIY, A.I.t knnTthffm",-
'~a-uk, red.; MORACHEVSKIY, 'Yu.V,, prof., reds; GRIVA, M., red.;
KOTS, V.A., red.; TOMARCHENKO, S.L.., red.
(Chemist'B handbook] Spravochnik khimika. izd.j perer. i
dop. l4oskva) Xhimila. Vol.4. 1965. 019 (KIRA 19:1)
1. Chlen-lorrespondent All SSSR (for Nikollaklyj- Romankov),

ACC Mi DOURCR CODE,.--- UA/0413/67 /000/001/0002/0002
INVENTOR:. Teterko, A. Ya.; Zevdell, B. M.
ORO: None
t
T
TITLE: An eddy-current'method for detecting flaws in,nonferromagnetic metals and de-
terminine Itheir parameters. Class 42, No. 190049 (anpounced by the PhyaLcomechanical
Institute AN Ukrainian SSR (Fiziko-mckhanicheskiy institut AN Ukrainakoy SSR)]
!SOURQE: Izobreteniya, promyshlennyye obraztsy, tovarn'yye znaki, no. 1, 1967, 82
TOPIC TAGS: eddy current, flaw detection, electronic measurement; quality control
ABSTRACT: This Author's Certificate introduces an eddy-current method for detectin*g
!flaws in nonferromagnetic metals and determining their parameters. Gradiometer pickup
isignals are subjected to amplitude-phase analycia-and the variation -,n thevector of
Ithe vertical component of the induction gradient in the field of eddy currents on the
surface of the part being inspected is used for determining the depth and size of the
haw on the basis of experimental diagrams. Provision is.made for adjustments to ell-
~inate the effect of changes in the gap between the pickup and the part being Jnspect*4
11 d changes in electrical conductivity and to increase productivity in determining
,an
flaw parameters. The change in the vector of the vertical cmponent of the induction
gradient in the field of eddy currents is displayed on the scope of a vacuum-tube
Cc-rd 1/2 tme. 620.1-7q.3-4,4

ACC NRs AP1064166
Ivectometer in the'form of a hodograph of this vector i'
p1the complex plane. This cca-
Iplex plane is reproduced on the screen of a CRT with image persistence and the depth
land size of the flav are determined from the angle of inclination of the linear sec-
ftion of the hodograph to the polar axis-and from the maximum length of this linear
section.
UB CODi..3104
S
SMH DM: 1TDec65
Card 2/2