SCIENTIFIC ABSTRACT MILYAYEV, N. A. - MILYUKOV,, P. M.

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001134330001-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 3, 2017
• Document Release Date: July 31, 2000
• Sequence Number: 1
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

--XIMAYMP H*A*
-_ I
Magnetic field in the area covered 17 the drifting stations NIFOrth
pole 30 and 'North Pble 40 in 1954/55. Trudy AAHII 223:46-64 160.
(MBA 13: 10)
(Magnetism, Terrestrial-Diurnal variation)

3, 6/' /00 (,Pj6 'r-1 1/~a
o
UM'W
R: Hilyayev, N. A.
TITLE: Simultaneous magnetic
the Arctic.
PERIODICAL: Referativnyy zhurnal,
-stract 7G222 (Inform.
no. 30, 1961, 25-28)
402 E,~
3/169/62/06'0/007/147/14r,,
D228/D307
variations in the Antarctic and
Gefizika, no. 7, 1962, 33, ab-
byul. Sov. antarkt. ekspeditsii,
TTEXT: The author cites examples of the simultaneous emergence of
polar disturbances at a numbed of Arctic and Antarctic stations on
26 Pebruary and 18 May 1959. The greatest similarity in the form
of the disturbances was observed at stations situated on both po-
lar caps (Vostok, Mirnyy in Antarctica; and the drift stations
SP-7 in the Arctic). The disturbances recorded by the
drift stations are closer to those noted.by the Antarctic staitions
than to those in the northern auroral zone. /-Abstracter's note:
Complete translation.-,7
Card 1/1

IGNALTOV,, V.S.; IMILUYEV,_N.A.; NVOOLISKIT, A.P.
Results of geoplWalcal studies In the central Arctic, Probl,
Arkt.i Antarkt. no.U%65-?A, 062. (KMA 1612)
(Arctic re;ions-4kgnstism,, Terrestrial)
(Ardtic regiops-Ionosphooric radio wave propagation)

- MILTAIEVO N.A. ___
Latitude shifts in the
of the Swetle field In
no.Ils75w?g_,
062.
(Arctic regions-AkpotIsm,,
transition zone
the Arctic.
Terrestrial-Diurnal
of diumal variations
Probl.Arkt.i Antarkt,
(MIM 16j2)
variation)

MILYAYEY, N.A,
Variations of the magnetic field in the area of drift of "North
Pole-4" and "North Pole-5" Stations in 1955 and .1956 TTwW AANII
241 no.4s65-8o 62. (MIRA 15:8)
(Arctic regions--Magnetism, Terrestrial-Diurnal variation)

MILYAYE.V.,JI.Av,
Aban level of magnetid disturbance in the central Arctic. Probl.
Arkt. i Antarkt. no.12:91-97 163. (MIRA 16s7)
(Arctic regions--Magnetism, Terrestrial)

~W
2191-&_ EWT(I)l A h)
f42/05/000/003/0300/0310
_,ACCESSION MRt APS020921 UR/01
621.37 .4
'j, AUTHOR: HiYaYev. N*,Ao:
TITEX; Some Orablems of the theory of electron tube i0saillatore uLth =11near
driver,circufts
SOURCE: IVUZ. Radiotekhn4a., v. 8, no. 3, 1965, 300-310
TOPIC TAGS: pn junct on electric capacitance,.electronic oscillator
ABSTRACT: The capacitance of the closed pn junctionjo widely used in different
radio.components.-7,1ts reactance-is easy to control-and It has a wide range of
-The no linear dependence of its
ioperating.frequencies (up.:to 3 go and higher). _n
Icapacitance on the instantaneous voltage on the pn junction makes the.jpnction use-[.
ver circuit In an electron tube oscillator. This
'ful as the capacitance of the.dri
type of oscillator has received almost w i6ention4n the literature, The authors
-!examine the most general case,an'electron tube.self-excited cacillator.1n.which
ithe driver circuit,capacitafice is composed of a linear-capacitor~and the coed pn
'Junction'snonlinear capdatance In parallel with Jnduct.ive. feedback# Eq"valent
Card 1/4

L: 2191-66-
ACCESSION NR: AP5020921
circuits of two variants are shown in, figs. 1 and 2 of the Enclosure& Results of
the.analys5svindicatee. (I) distortion of the voltage wavefow is considerable at
high amplitudes, results from the nonlinear variation of the pu junction's cap&-
citance with applied voltage, and depends on the amplitude of the generated
oscillations and the nonlinearity of the circuit; (2) the frequency of the generat-
t4
ed oscillations depends,strangly on their amplitude and the nonlinearity of the
Icircuit. As amplitude Is Increased frequency decreases, in a strong relationship;
-.1therefore frequency stabilization requires, inter alia, a stable amplitude; (3)
jthe effect of nonlinearity ofthe capacitance somewhat reduces the amplitude of
Ithe oscillations; (4) a genaratortube operating in the.middle of the plate-grid
~characteristlc has a negative impedance compensatin -for system losses, and if tile
1Q is high enough it does not distort the generated waveform. Orig. art. has: 28 1
formulas, 10 figures.
ASSOCIATION: none
ISUBMITTED*. O9Apr64 ENCLt .02 SUB COW:' -EC
NO REF SOVe. 006 OTHER$., 000,
Card 2/

L 35993-65 M t% 1) 173WA (h AT
ACCESSION NR: APS007"I S/0109/65/010/003/04S7/0467
AUTHOR: Milyaggy, N- A-
TITLE: Eff-e`ct of the nonlinear capacitance of a reverse-biased P-n junction upon
free oscillations in a circuit Iq
SOURCE: Radiotekhnika i elektronika, v. 10, no. 3, 196S, 457-467
TOPIC TAGS: semiconductor, semiconductor junction, semiconductor device

&nod p-n junction a Ainear
capacitance consists of rove roe-bi hunted by a
capacitor. The free oscil.lations are descri'~ed by this diff-erential equation:
0+261+ aw +_ *ps S)
(I = s;(k + m F=7) 9 k + in-(f - x)*
is t circuit
where 9), is the relative a-c circuit voltage; '6 2z he
attenuation; 40W 4 IYL(-E+ re)'Ts the circluit natural frequency at a bias voltage E.
-A
i the circuit-capacitan6e honlinearity factori snd-~f*

at
_L 36993-65
,__~._[ACCE=ONNIt. AP5007091
the circuit -capacitance linearity factor. The functions constituting the above
equation are expanded into power series, linear and nonlinear terms are

SUBAETTED: 27J&n64
It EF
NO. SOY: 007
Card 2/2
ENCL: 00
OTHER: 000
SUB CODE: EC,
ATD PRESS: 3223

ACC NRI AT6037052 SOURCE CODE: UR/0000/66/000/000/0148/0171
AUTHOR: Milyayev, N. A. (Engineer)
ORG: none
TITLE: The theory of forced oscillations in a nonlinear circuit with a p-n junction',
capacitance
SOURCE: Moscow. Aviatsionnyy institut. Teoriya i tekhnika radiolokatsii (Radar
theory and techniques); sbornik statey, no. 1, Moscow, Izd-vo Mashinostroyeniye,
1966, 148-171
TOPIC TAGS: hysteresis, nonlinear differential equation, electric capacitance
ABSTRACT: An attempt is made to analyze the work of a nonlinear resonance
circuit (both parallel and series) using a nonlinear closed-loop p-n junction
capacitance. The solution of a nonlinear differential equation makes it possible to.1-
find the resonance curves of the nonlinear circuit and to determine the conditions
for the occurrence of a "hysteresis" zone. The regulation curves of the nonlinear
circuit are plotted as a function changes in the excitation amplitude and the bias
voltage. The relationship between the circuit frequency and voltage shape and the!
2 UDC: 621, 396, 216, 001(4)

ACC NR- AT6037052
amplitude of oscillations, as well as the type of junction and the degree of circuit,
nonlinearity is determined. Orig. art. has: 13 figures and 65 formulas. [GC]
12, 20/SUBM DATE: 15Jul66/ORIG REF: 006/OTH REF: 0011
2/2

MILYAYKV, N.A,
Annual variations of' the magnetic perturbation and elements of the
Arctic magnetic field, Problo Arkt. i Antarkt. no.16:63-68 164.
(MIRA 17:6)

IMILYAYF,V N ,,, red.; ANDREYVA, T.P., red.; STULICHIKOVAp N.P., takhn.red,
[Tables of observations performed at the drifting research stations
"North Pole-60 and North Pole-8" in 1959 and 1966-1--**60rialy
naboiudenii nauchno-issledovatellaUkh dreifuiushchikh stant9ii
wSevernyi polius-6" i "Severnyi polius-8" 1959/60 goda. Leningrad.
Arkticheskii i antarkticheakii nauchno-issladovatellskii institut.
Trudy, vol. 265. (MM 16:7)
(Arctic regions-Mgnotiomp Terrestrial-Oboorvations)
. (Arctic regions-Ionosphere-Observations)

1 31137-6 - E1!T(1)= G41
ACC NRt AT6012782 SOURCE CODE: UR/2561/65/000/021/0072/0080
AUTHOR: Mi?Zayev, N.
ORG: none
TITLE: Magnetic field disturbances in the vicinity of the "North Pole-8" drift
station,
SOURCE: Leningrad. Arkticheakiy i antarkticheskiy nauchno-isaledovatellsk!Y
institut. Problemy Arktiki i Antarktiki, no. 21, 1965, 72-80
TOPIC TAGS: magnetic field, geomagnetism, drift station
ABSTRACT: Personnel assigned to the "North Pole-8" drift station drifted across
the central part of the Arctic Ocean Basin in 1959-1961, where they made absolute
observations and continuous v tion recordings of the Z, H, and D components of
the earth's magnetic fi A19f of the station's route covered that of the "North
Pole-411 station (1954-1956) and of the "North Pole-T" (1957-1958); the former
travelled in a period of minimum sunspot activity and the "North-Pole-8" at a time
of high activity. Data obtained from both stations are compared. The average
magnetic declination varied from +25' in the southern section of the course to +90'
in the northern section; the horizontal component varied correspondingly from
6500 to 2000 y, and the vertical Z-component from 56,500 to 5T,500 Y. Magnetic
disturbances were measured by the hourly amplitude variation of the H-component ry
with variations in the mean monthly values shown graphically. At#-.f )ts to find aH'
Card 1/2 UDC: 550-386

L 31137-66
ACC NRt AT6o12762
connection between the frequencies of magnetic disturbances and sunspot activity are
discussed. Annual variations in differences in values of distrubances r showed
no definite pattern of difference between years with high and low a ~ ~ activity
in high latitudes during equinoctial periods; values of r~ passed through zero al-
most every half year. Moreover, even when the Wolf number varied by 175 and 152
units, the magnetic disturbance ry varied only by 13 and 4 y, respectively. During
the drift period, three types of Niurnal variation were noted: 1) a summer type
characterized by a marked morning maximum at 2300---AWbr World Time, a very weak
maximum near local midnight, and a comparatively large amplitude of variation some-
times exceeding 170; 2) a winter type distinguished by marked morning and night
maxima; 3) a winter type corresponding to an area of high geomagnetic latitudes
between 77-78* (Janudry-March 1961) which was characterized by almost no night
maximum and a very weak maximum at 2300 hr World Time, with small variations in the
level of disturbance of about 50-T0 y. Orig. art. has: 5 figures and 4 tables. [E
suB com o8/ Sum DATE: 13mar64/ ORIG. REF: 003/ ATD PRESS: '41-2 1~ 0
iv

STRAUSOV, Boris Georgiyevich; IKONNIKOV, S.N., kand. tekhn. nauk,,
retsenzent; MILYAYE~, N.A-, inzh., retsenzent; IVANOV-
TSTGANOV, A.I., red.; YARTEMIYANOVA, V.A., red.;
BARANOVSKAYA, K.P., tekhn. red.
(Measurements in electrical and radio engineering] Elektri-
cheskie i radiotekhnicheskie izmereniia. Moskva, Mosk.
aviatsionnyi in-t, No.l. 1962. 69 p. (mim 16:io)
(Electric measurements) (Radio measurements)

KILUTV P.M.; GOIIDIYMMO, I.P.
-", I-
Automtio control of the composition of the nitrogen and
hydrogen mixture In the ammonia synthesis section* From.
energ. 15 no.5:22 My 160. (KM 13:7)
(Ammonla) (Automatic control)

AUTHORS:
TITLE:
PERIODICAL:
2641a
S/056/61/041/001/006/021
B102/B212
Manenkov, A. A., Milyayev, V. A.
Relaxation phenomena in the paramagnetic resonance of
Mn 2+ ions in the cubic crystal field of SrS
Zburnal eksperimentallnoy i teoreticheskoy fiziki, v. 41,
no. 1 (7), 1961, 100 - 105
TEXT: Following a previous work (ZhETF, 40, 1606, !Q.61) the authors have
investigated the spin-lattice relaxation of Mn 2+ ions in SrS. In this
reference it has been shown that SrS will crystallize cubic-symmetrically
with a very weak splitting (-10-4 cm- 1) of the 6S state, Therefore, the
ground state of Mn 2+ in SrS has to be nearly a pure S state, and it may be
assumed that the spin-lattice relaxation time is already significant at
room temperature. This, however, is not the case, since at room temperature
it is.--10 -8 sec, and at liquid nitrogen temperature ~10- 6 see. The authors
discuss these results with regard to relaxation mechanisms.. Mn2+ ions are
Card 1/5

26422
S/056/61/041 '/001/006/021
Relaxation phenomena in the.... B102/B212
also very interesting with respect to the spin-spin cross relaxation since
they exhibit a large number of hyperfine-structural levels, which come about
through an interaction of the electron spin of Mn 2+(S - 5/2) with the nuclear
spin of Mn 55(1 = 5/2). These effects have already been studied theoretically
and experimentally. The authors have observed marked cross-relaxation
effects at liquid helium temperature in the Mn 2+ spectrum of SrS. The
studies have been made with polycrystalline SrS-Mn specimens (0-05 % YIn
A superheterodyne radiospectroscope (9300 Mc/sec) was employed. and
measurements were made at 300 0Kv 77 0K, 4.2 and 1.6 0K,, The measurements
were made at the lines corresponding to the electron transition M - 1/2--)-'A
for various hyperfine-structural constants (m - +1/2, +1/3, -+5/2),. The spin-
0 0'i fro -the II e broadening
lattice relaxation time T 1 was estimated at 3 0 m in
caused by spin-lattice interaction. The broadening was calculated by
comparing the lines at 300 and 77 0 K. At 770K T I was determined by tho
method of continuous saturation of the lines (ZhETF, 5-8, 729j 1960)9 and at
liquid helium temperatures the relaxation phenomena were investigated by
Card 2/5

26411
S/056/61/041/001/006/02"1
Relaxation phenomena in the ... B102/B212
the method of pulsed saturation of the lines. In order to separate the spin-
spin cross relaxation and spin-lattice relaxation effects, two types of
saturation pulses were used; "narrow" pulses (r - 0.1 - 1 msee) and "broad"
pulses (f' - 70 msec). For comparison, the relaxation times were also
determined by the method of continuous saturation at 4~20K, T 1 was
determined at 300 OK for the components m = 5/2. For both lines T 1 was
5.10- 8 see. At 77 0K the value was T I ~ 1.5-10-6sec. The spin-spin
relaxation time was found to be T 2 = 6.10- 8 sec, At 4-.2 0K it was fcund that
T 2.9-10 -2 if T had the same value as at 77 0K. If. however, a spin-spin
2
cross relaxation exists, than T 2 will only be 1/3 as reat as at 770K, and
the following results are obtaineds T, 0.10-2 sec. At 1.,60K T 2~1.ICF'
sec. All these data are valid for lines with m - +5/2,, As to the character
of the relacation processes of the Mn 24 spectrum, the following can be
concluded: In the range 4.2 - 1.6 0K one finds that T11_T' 1~ i., e., single-
Card 3/5

26411
S/056/6!/041/001/006/021
Relaxation phenomena in the... B!02/B212
phonon processes play the main role in spin-lattice relaxation- At higher
temperatures, T1 becomes a stronger function of temperature. Ti drops
non-monotonically (Ti ~T- n) at an increase from 4,,2 to 3000K.. At 3000K
it is found that T I--T2. The Ikin 2+ ions are found in the 3 state. and their
levels are only slightly split by the SrS crystal field. The spin.-lattice
relaxation is essentially determined by mechanisms other than Kroning's.
One of these mechanisms can be a modulation of the covalent bond between M 2+
and the surrounding diamagnetic ions. Marked spin-spin cross relaxation
occurs at liquid helium temperatures. The authors thank Professor A. M.
Prokhorov and Professor S. A. AlItshuler for discussion, and a. hL. Medvedev
for producing the SrS-Mn specimens. There are 2 figures and 9 referencest
4 Soviet and 5 non-Soviet. The two most important references to English-
language publicgtions read as follows: N. Bloembergen et al. Phys.. Rev. jjL
445, 1959; J. G. Cartle et al. Phys. Rev. 119, 953, 1960,
Card 4/5

264n
S/056/61/041/001/006/021
Relaxation phenomena in the... B102/.B212
ASSOCIATIONt Fizicheskiy institut im. P. N. Lebedeva Akademii nauk SSSR
(Institute of Physics imeni P. N. Lebedev of the Academy of
Sciences USSR)
SUBMITTED: February 25, 1961
Card 5/5

MANENKOV, A. A.; MILYAYEV, V. A.
"Investigations of the Spin-Iattice ReImtIon of Ions in S-state."
Report presented at the First International Conferdnee on
Paramagnetic Resonance, Jerusalent Israel, 16-20 July 1962

34230
S/181/62/004/002/013/051
B102/B138
AUTHORS: Manenkov, A. A., Mi
,~Iya.yev,V_ A., and Prokhorov, A. M.
3+ 3+ -
TITLE: Relaxation times of Cr and Fe ions in rutile single
crystals
PERIODICAL: Fizika tverdogo tela, V. 4, no. 2, 1962, 388 - 391
TEXT: The pulse saturation method (9400 NO was used to study spin-.lattice
relaxation for Cr3+ and Fe 3+ ions in rutile at liquid-helium temperatures.
The paramagnetic resonance lines mere saturated with pulse durations
between 100 and 0.01 msec, in order to find the reason for the existence
of spin-spin cross relaxation effects. With no cross relaxation, the
curves describe spin-lattice relaxation only and are independent of pulse
duration. The single crystals investigated were grown by the Verneuil V~
method,, In all experiments crystal orientation was such that the external
magnetic field was perpendicular to the a-axis and coincided with one of
the a-axes. With saturation pulses of 100-50 msec the relaxation curves
3+
of Ruth with Cr impurity were found to consist of two components:
Card Q~3)

34230
3+ 3+ S/181/62/004/002/013/051
Relaxation times of Cr and Pe ... B102/B138
t/Tj -tft~
I(t) - 10 = A 1 e" + A 2e 1; A 1 + A 2 10, where I(t) is the line
intensity at a moment of time t after the end of the pulse, 1 0 - equi 14 brim
line intensity. The-following spin-lattlee relaxation times were calculated
Por the Cr3+ ions:
4 2 K 1. 0 K
Transition '
T
IT A
/I T
T
I A
/1
7
1
, ,
. i ,
[
J ,
0
msec % .
m C

-2
4 1.1 36
9
8
2 60
5'e ------ ~,,4 2.3 0.5 13 3.3 0:
8 30
3 ____-p, A 2.2 0.5 24- 3.3, 1 60
The weak temperature dependence of the transitions 3/," and 3?"41 can be
explained if the lower levels 1,2 and 11,21 take part in these trans-Ations,
For the ~-_'>2 transition cross-relaxation was observed with pulseE of M5
msec duration. In this case, besides T and T, , the relaxation curve also
LX
lard 2/3

34230
Relaxation times of Cr and Fe
coritaIns a "fast" exponent T12