SCIENTIFIC ABSTRACT ZYRIN, N. G. - ZYRYANOV, P. S.
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S
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100
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December 31, 1967
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SCIENTIFIC ABSTRACT
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~-BE ITSYNA, G.D.; OBUKHOV, A.I.
Ufect of the current strength of a carcon are on the evaporation
and the radiation Intensity of microelement~ in a spectrum
analysis of soils. Pochvovedenie no.54.123-127 Bj, 162.
(MRA 15:6)
1. Moskovskiy gosudarstvannyi universitet.
(Soils-Analysis) (Trace elements)
ZYRM~11 A-.; -BELITSYIM ---G. D-. -; -0--BU-Y-J-l-O--V-, A. 1.
Characteristics. and aucce!;:Jcn.o.~Ahe intalca of elements in the
flame of electric arc in OpectIVA-001 wlyalls. .-Al6brov0denia
no.10.:88-92 0 161. 14-.9)
~.l Moskovskiy gosudarstvennyy universitet im6ni M.11.' Lamonosova.
(spectrum analysis) (Soils-An&lysis)
Concentration of trace elomenta of the iron :tamil:r in come s 0~ils
of the U-8-S-14 Vest. Moak. un. Ser. 6: Biol., poohv. 16 no *5-.
59-71 8-0 161. W-10)
ls Kafech-a poclivovedeniya Maskov kogo gostWArstvamo univer~siteta.
(TEACE EIZ14ENT MWEruls IN. SOIL) 60
j:
ZYRRI S.F.
Concerning the assortment and quality of linen fabrics.
Tekst. prom. 24 no.9t6-9 S 164- i
(MM ~7111)
1. Nachallnik upravleniya linyanoy, promyshlennosti, Gosudarstven-
nogo komiteta po legkoy promyshlennosti pri Gooplane S88R.
ZYRIN N.G.; BELITSINA, G.D.; OBUXBOV.,.A.I.
Possibilities for using absolute blackoningalin the quantitati1re
spectral analysis of soils for microelements Nauzh. dokl. vyv:
shkoly; biol. nauki no.2tl85-187 162. (MIRA 15-5)
1, Rekomondavana kafedroy pochvovedeniya Mookovskolgo gosudar6tvennogo
universiteta im. M.V.Lomonosovao
(SOILS-ANALYSIS) (TRACE SM4EkS)
(SPECTRUM ANALYSIS)
ZYRIN, N.G, KORNBLMI, E.A.
CharacterIiatica of the tehavior of iron in Soils n-r the Amur
flood plain. Dokl. AN SSSR W no..1:200-203 ja 1621. (MIRA 14:12)
1. 'Moskovskiy gosudarstvennyy universitat im~,M.V., Lomonosova:i
fochvezinyy institut im. V.V. Dokuchay8va AN SSSR. 11-i-edstavlano
akaddmikom LV. Tyurlmym.
(Kmnara reg'ion-4oils-Irori contimt)
_RRFj,,NUolay, prgiyevich;ORLOV Dmitriy Sergeyevich;
KOROBTSOVA red.
(Physicochemical methods of studying soilsl Fiziko'.-
khimicheskie metody issledovaniia pochv. Mo~~a, Izd-o
vo Mosk. univ.,, 1964. 347 p. (MIRA 17:1~0)
BMVA, L.N.; ZYRIN, N.G.
Role of the roots of her'baceo-us vegetatiomIn the nitrogen and
mineral cycle. Vest.Mosk.un.Ser 6: Biol.,Ipochv. 15 no-3;
67-75 MY-Je 160. (MIRA 13:7)
1. Kafedra pochvovedenlya Mookovakogo universiteta,
(Roots (Botany))
(Soilb-composition)
DUBBOVOLI IT-~G.Tv;-Z7RIN--&G-0-
%WSW
Some feat-area in the geography and chemistry of bottom-land soils. Test*
Moak. un. Ser. biol., pochv., geol., geog. 12 no,3rl29-135 157.
(KIRA 10:12)
1. Wedra pochvovedeniya Moakovskogo gosudarst-wennoga universiteta.
(Alluvial lands)
11 W
4POPIMM. M!" Mm
M-9--m-41 TIT,
ZYRIN, N.G.; OVCHINNIKOVA, M.F.; ORLOV, D.S.
Amino acid composition of humic acids and ful,ric acids in some soil
Vpes. Agrokhmiia no-4-'108-120 Ag 164. (MIRA 17:10)
--G-6-unt-ry : USSA-____
Category Soil Science. Physical. and ~Cliemiqal Pro'yer~-
-ties of~sollad
Abs Jour RZhBioloq~No 6,~19.59.,,No 2460,6
Author
G.,
in No Go; Orlov, D. So
pini
Inst
j ,,
io
sc,ow=
m
Ve
oscow n versity.
Title Determination Methods of the.Activity of So-
dium Ions in Soils and Soil Solutions*
Otig:Pub Vest a Mosk, Izi-tal Ser. biol.,~ pochvovedeq pol.49
geogr*2 1958, No. 11 71-80
Abstract The activity:,of so dium -ions An soils and.soll
solutions may.-be V' 7
y a , special; gl4ss
electrode with Na-function v;ith.the
j aid of .,
a,
,
,
..lamp,: potent Iometer6 The magpi~ude::of activ#y
~_is:clogely connected withthe!--genetie PeCU14-
rities. of,.,certain soils andm~y servo as a
method for an approximate diagnosis of solo-
netz and saline soils. For these purposes, it
.-Card 1 2
22
ZYRO, Y.; 'el'ORIEKIAN, F.
Stamping anO extrusion of sockets from polyj~ronal blar;R5, p. 14,1. (Mechanik,
Vol. 30, No. 4, Apr 1-0,57, Wars,3w, Poland)
SO: Monthly Lint of East European Accession5 (EE;1) LC, VoI. 6, No. 8, Aug 10,57-t Uncl.
WISNliwxi,-Henryk;-WRZOLKOW-,--,Teresa;-ZYRO~ISKA.
2 cases of-cerebellar myeloma in adults. Ne=ol. nomrocUr. pdlychlat.
pol. 12 no.4:501-508 162.
1. Z Zakladu Neuropatologii PAN.Kierownik: of dr A. Xunicki-~z
Zakladu Anatomii-fatologicinej AN w GdanskJrIer4=Uki prof, dti
W* Czarnocki-Z Kliniki Neurologicznej AM w Gdiimsku-,KIerownik-..
prof. dr Z. Majewska.
(MYELOBLASTOMA) (CEREBELTAR NEOPLASMS)
WISNIEWSKI, Henryk; WRZOLKOWA, Teresa; ZMOMSKA Monika
Two cases of medulloblastoma of the cerebellum in adults.
Neurol neurochir a
,psych 12 no 4:501-508 'J1-Ag 162.
1. Zaklad Neuropatolofii, Polska Akademia Nauk, Warazava,
Kierownik:,prof. dr &.Kunickl; Zakldd Anatoall Patologiamej,
Akademia Medyczna, Gdansk; Kierd,~nikt prof. dr W. C.aarnocki;.j
Klinika Neurolojiczna,'Akademia Modyczna, Gdamak; Kierownik:
prof. dr Z.Majewa6.
,I -,.cl- a ',,,!a nda ; F~', rl -,'-7.11 !'1 41 1 , - *~~) I ~ T, , --, .
_ C~ I - _1,1~41~jrj % j
N!; Mon i ka
rruc- of angi.--neurotlc Inflarrimat4ary rcar7.tion oC I.IN-, con-'ral
nentri'a*3 SYBI,~~ty, in a 1--year-Old glirl. fledlat. flol.~ 19
831-8314 Je 164.
1- '! III 51in-Al Padiatryczriej Akadnmii M~,Aycrln~e~ ul Va f,
i.1, erawn.1k., pru'. dr med. T. YI~n;ki
Neurologiculej Akadertil M,,-,dyczrc-j w Gdrtnai~v
dr mod. 7, 1 % Zakladu Anatom,~i 1,01,01.0git'nei
Al-adnmii Madyc:~.-.ej w Gdansk-u (Kierowniki prot,, dr- imetz,
WO Czarnocki) .
HIJU-13KA-FRYDRYCH, 111(mika
Thrombo-emb6lic complication3 in acute vascular diseases Of -the
brain. Pol. tyg. leke 19 no,41U1533-3-535 5 0 v64
1, Z KlAniki Chorob Nerwowych Akademli Modyc=61 w Gdansku
(Kierownik." *orrif. dr. Z.Maiptiaka),
~YRYANOV, A.A., master
Device for checking the springs of the socket contact of a VIC-133
switch. Energetik 12 no.S.-20-21 Ag 164. MIA 17:9)
ZYRYANIOV, A. I.: Master tied ScL (diss) "Prolbi.e!!is of activa imzzlni-za~ian
against dysentery under experimental conditions". Kr"noyarsk, 1959. 14 pp
(Tomsk State tied Inst), 200 copies (KL,No 12, 1959, 132)
RLT47, Ye.G., gorayy imphener; M*---R7l-YAWV, V.I.. gorWy tekhnik;
gornyy tah-hnik; M11MYS11, 3.V., gorr*7 tekhniV.
ConvArisort of W-506, TP-4 and MY-4 rook- drilt Derforminnec.
Gor shur 09 10:9)
TO,
(R'Ock triiis)
BOBY,LZVI I.P. (st.A&W, Sverdlovskol, dorogi); ZPYANOV, Aje, (st,Aducrp
Sverdlovskoy'dorogi); MELUZOVp,V.G. (at.Advy,'Sverdlovskoy dorogi);
SINTMIN, F.T. (st.Aduy, Sverdlovskoy dorogi); TALIBULINA, R.G.
(st.Aduy, Sverdlokvskoy dorogi); FATKHA-LISLAMOVp G.,(nt.Aduyp
Sverdlovskoy dorogi)
Inadmissible procedures, Put' put,khoz. 8 ao.2t4l 164.
(MIPA 170)
-FIDYU KIN,-D.-L~-:--ZYlffANDV, B-.A:;---,-KORDTKOVA-.A-.A.
Instrument and method for hardness tests on sponge rubber.
Kaucb. i res. 17 ne.11:36-37 N 158.
~ .; (MIRA 11:12)
1. Naucbno-ioaledovatellskiy institut rezinovftb i li~tekarqkh
Welly.
(Rubber--Testing)
AUTHORS: Fedyukin, D.L., Z SOV/138-58-11-12/14
Korotkova, A.A.
p.
TITLE: Apparatus and M thod for Testing Foam Rubber Products as to
Hardness (Pribor i metod dlya ispytaniya Subchatykh,izdeliy
na tverdost')
PERIODICAL: Kauchuk i Rezina., 1958, Nr 11, pp 36 - 37 (USSR)
ABSTRACT: Hardness is measured by the apparatusi showa in the illus-
tration by penetration of a steel cylinder,59 mmdia under a.load
of 1415 g. This gives a specific pressure o n the s amlle o f
50 g/ci2 which is the average pressure on the seat of a man sitting
down. The hardness tester is mounted on a disc 280 mm dia, and the
whole unit weights 2.3 kg. The cylinder is held'before measurement
by the detents so that it is just level with the surface of the foam
article. Hardness is expressed as the deflection measured 30 ' see
after zlease of the cylinder. MeasureWent should be made at con-
trolled temperature between 15 and 25 0. 'The hardness indicated
varies according to the thickness of the spe imen, and for control
testing standard thickness specimens must bo used.
ASSOCIATION: Nauchno-issloLdovatellskiy institut rezinovykh i lateksnykh
izdeliy (Research --lastitute fdk Fdbber and Latex Products)
Card 1/1
1e.,, -ZYRYAITUV Ij_.Y*
POPOVA, T.S., inzh.
Color stability 6f the illuminating kerosene produced-by the hydro-
genation. of crude oil; ". i tekh. topl. i masel. 6 no.lOsV, '. 16
0 161. (NDA 14: 3-1)
(Kerosene)
PODKI-ETHOV, N.Ye.; ZYJIYANOV, P.F.
Catalytic reforndng of Sakhalin gavoline. Xhi,m.L tekh.topl. i
manel 10 no.1:2E-27 Ja 165. (MIRA 18:4)
1. SakhalinakLy kompleksnyy nalichno-IssledovittelInkiy Institut
Sibirskogo otdeleniya AN SS,9R.
_L 22113-c4 piT k m) / 1 VIS
AM HR, XP _6012993 --~O-URCE COME: TO 0 i; A 755W00170QF670027!
yanov B. F.
AUTHOR: Podkletnov, H. Ye.; Zyr
ORG., Sakhalinskiy KNII SO.AN,SSSR
TITLE: Catalytic reforming of Sakhalin gal~361ine
SOURCE: Khimiya i tekhnologiya topliv-i m~s 1,~~ no.i.1 i 6,5 2
matir,.* hy"arbon~ batalytia c~ackimg
TOPIC TAGS: catalytic reformings gasolxne~:aro
a ne 7a vl~
lumina, platinum, catalyeiss .,xyle r. benzene nonmetatir- or hie deri~aft
ABSTRACT: In order to determine the possibilI4 Or.. !us' In the lis~ht
B 01\
s as petrochemical a ri 00 4 ,the
portion of Sakhalin stock .7 ~400~
line obtained by straight run. distillation of , VIdiabf nska-y-d-76 ri
nd t-6--talytio ref orming:' over a p :a i4dt.i ~The 13-i7o
, arwen a 1--ti-num!qAt, i
u
gas-oline fraction boiling at 97-1509C undekiw67~F;Oatihliblc re6rml-
Ing on an experimental apparatus with2circuldt,1119 Wrogen-eoiitalm-
Ing at a pressure Pexc = 40 ks/om , a bulk:flow rate of 2A
hourRls, and a temperature of 5050C., Forty ml'o~f AV+56 aluml ' -
platina catalyst was placed In the reaotor enoll~osedllh an aluolmm
block.' Temperature measurement In the catalydt; laydir was madj3 at
three points. The experimi8b lasted 48 hours, The resultjUg
catalyst had a density ?t, = 0-8158, refraction index n - m it4740*
a 72,2% by weight aromatid hydrocarbon contento, Tito cataTysate
yield was 84% by welot with ,rec e 't to'gasoltio. Toluene ~r6do'i.
ard 1/2 ~.665.i534.- 665 5~li2(571,64)-
i-C
. ........ "FEW;
jig lull L[ILM11F1111hallij
L 22113-4
ACC NRt AFTO~12993
-contexit. ofA9."j%,O. -the C 11 b
minated in the catalysate, at
vvr9qa~ on*:.
-a
t "n be ~ 7 .
In the initial gasoline and In the qatalysate~, deeh 1~
that B-70 gasoline differs from theicat4ly~ate; in highei:gas6ti~a;.
content and In lower xylene eontent. In addit.iOn to P648- hy
carbonsq the following derivatives of benzene, 0. the' C C 6 MOO--;~
.sition were detected In the.eatalysate~ wl th c e stibs'MUnt I
nk
n-propylbenzeney Isopriopyl anzene, be*"butylbe'~~'6ne:~" 1(rith twd~
OY One'
substituents -- 19 2-s 19 3-, and l' ''.4-methyl . 1b' neq
1-methyl-4-isopropylbenzenev Isith three substlt4pntj - 1j. 20 3-!V:'
19 2j 4-t and lt 3, 5-trimethylbanzents The h6 lial'!"Ible tulror."_..
content in Sakhalin gasoline and th'a high *raugoto Oydro6aiftA
yield upon its catalytic reforming makes this sasoltna a pranid-
ing crude for catalytic cracking. Orig. art* has: I tat-Ile. -1apm]
ZYRYAMT,---Bi;P~;- KAULSENUOTA, m.r,; ORWHKrIf,- DJO --
Hydrofining of the "galosha" gasoline distillate* Truly
Vost.-Sib.fl.AF SSSR no.26:141-146 159. (MrRA 13:6)
(Gasoline) (Hydrogenation)
ZYRYANOV) E. YE.--"Study of the Mechanical Efficiency of a Steam Hqpine
on Redistribution of the Power on the Cylindera.W~D
For Degrees In Science and Engineering Defended at U
Higher Educational Institutions)(29) Odesaa Inst of
Engineers of the Maritime FleetP Odessa, 1955
SO: Knizhaya Ioetopis' No 29, 16 JulY 1955
For the Degree of Candidate in Technical Sciences
"M iff"I"WRIPTIMM". ~Im " ~1111 11~1VII"Ir"Il I I IN IIIIII
i3l MHi
'11,41 Wfrm-k Lim-
-1401
Developing productive forces in the northwestern part of
British Columbia. Prob. Sev. no.51-130-3-45 163,
JMIR'A 16:11)
1. Sovet po izuehaniyu proizvoditeltnyi& sit pri Gosplane
SSSR.
Ila,
"IFNIR
vm
Plant for the direct reduction of iron In Gamda. Retallurg
5 no-3:38 Wr 160. (NIM 13: 7)
1. Sovet po izucheniyu proizvoditellmykh oil AN SSSR.
(Canada--Metallurgical plants)
0.0000
AUTHOR:
TITLE:
PERIODICAL:
ABSTRACT:
ASSOCIATION:
Card 1/1
7805~3
SOV/130-60-31-22/23
Zyryanov, G. A.
Metallurgy Abroad. The Plant for Iron Production
by Direct Process
Metallurg, 196o, Nr 3, P 38 (USSR),
This article de'scribes the ~Ilu
new meta rgical plaht to
be built by the "Quebec South Steel Corporationil'in
the vicinity of Montreal, Quebec, Canada.
Council for Study of Productive Forces, Academy of
Sciences of the USSR (Soviet o izucheniyu
proiz,voditellnykh sil AN SSSR3
R.P.1 ~DROXJJI, A.I.; ILYKOV, A.S. j SALANSKIY, QRYABGV;_,~~.,I.
Temperature hysteresis of the magnetic permeability of magnesium-
manganese and nickel-zinc ferriteo. Izv. vys, ucheb. zav.; fiz.
no-404,39 '63. (MIRA 16:9)
1. Inatitut fiziki Sibirskogo otaoleniya AN SMER.
(Ferritas (magnatic materials))
24(6)
AUTHORs Z7rYarI6-v,_G_. SOV/57-56-12-2/15.
TITLEs Variation of the Contact Potential or ;Cadmium Sulfide When
Illuminated (Izmeneniye.kontaktnogo,potents'lala sernistogo,
kadmiya pri osveshchenii)
PERIODICAL: Zhurnal tekhnicheskoy fiziki, 1958, Nr 12, pp 2657-2668 (USSR)
ABSTRACT: The aim of the present work was to eyplain'the nature~of the
photosignal obtained from a cadmium sulfide layer lacking'
activating admixtures according to the method of the.dis-
placement of characteristics. It was found that the reflection
of slow electrons with an energy from.1 to 10 eV from'the
semiconductive layer does not take place manotonously,but
,.that at certain electron velocities maxima and minima.exist.
A comparison between.the reflection coefficients of the slow
electrons with I to 10 eV on,Pt, Ni, and CdS shows that the
reflection coefficient-of the-semiconductor is somewhat
higher than that of,th.e metals. The eXistence of reflection
minima at 2.5 and at 5.0 eV-permits to assume that when an
electron is transferred to the zone of conductivity an
inelastic collision takes place. This provides an opportunity
Card 1/3 of determining the width of the forbidden 4one according to
Variation of the Contact Potential of Cadmium Sulfide SOV/57-58-12-2/15
When Illuminated
the reflection curve of slow electrons on siemiconductors.:
The time- and spectral-characteristics I and -the infrared
attenuation of the photo-displacement *show that the kinetics
..of formation and of the decrease of the photo-displacement
(shift of the current-voltage characteri;ti 'r, in volts) is*the
same with photoconductivity and.that the emission of electrons
takes place at the same levels. A general formula isipresented
for the increase of the photosignal when the illumination is
switched on and for its decreaseafter the'removal of the
illumination.'From this formula exponentialland~hyperbolic
relations are obtained for specialized cases. The dependence
of the photo-displacement on the intendity of illumination
is logarithmic, i.e. an analogy with the-DeMber effect exists.
It is shown that the experimental data may*be expressed by the
known formula for thephoto-e.m.f.,,and-thip without the
assumption made by G. Wlerick (Vlerik)(Ref 1) that on the
surface of the cadmium sulfide layer a film of adsorbed gases
in found. The estimation,of the coefficienta from the
experimental formula for the photo-displace.ment by means of
Card 2/3 comparison with the theoretical formula leads to a "quantum
Variation of the Contact Potential of Cadmium Sulfide SOV/57-58-12-2/75
When Illuminated
yield" of the order of~103
. The investigation of the
dependence of the photo-displacement on the thickness of
the CdS layer shows-that-the phenomenon takes place.in a
.thin (10-5 cm) layer on the surface of the semiconductor.
The possibility of employing the diffusion theory for the
,explanation of the results is investigated.
A. A. Lebedev, Academician,-suggested the theme.
IR. Ya. Berlage supervised the work,
There are 12 figures and 16-referenees, 6 of which Are Soviet.
ASSOCIATIONs Leningradskiy gosudarstvennyy universiiet Kafedra
elektrofiziki (Leningrad State Univ6rsity Chair of
Electrophysics)
SUBMITTED: December 129 1957
Card 3/3
,,-,,ZYlffANOV, G.K.
Taking the diffraction image as a basis,in detgrmining the
energy of slow primary electrons by which a dielectric is
being bombarded. Vest.LGU 20 no,22:166-169 165,
(MIRA 18:12)~
ZYRYANOV, M.N.; SINAKEVICH,, A.S,,; NADOLISKIY, A.P..
ZIRYANCV, Mikhail Nikolayeviohj ~_SINMVICHI -A.S.)_ red,;_ 13011ELIDER, E.Ya.
- ----- -KARAS'f-V.D*- tekhn-,- red-
red
(Dispersed rare elements; propertieop arewof use, production
dynamics prices, raw matorial'oourceol toolmology:o.f pro-
parationi Rasseiannye rodkie elementy; svoist'vnipoblanti primenuniia,
dinamika pralzvodstva, tsergp syrlevye istoohn*i proizvodstva,
tekhnologiia polucheniia. Pod redo A.B.SinakOvicha. Irkutsk Ir.
kutskoe knizhnoe izd-vo, 1960. 201, p. (MIRA 15M
(Trace elements)
,9/137/52/009/006/059/163
A052/A101
AUTHOR: Zyryanov, M. N.
TITLE: Thermodynamic analysis of sulfating reactions of some oxides, sul-
fides and metals by means of bivaltintl 1ron pulfate
PMIODICAL: Referativnyy zhurnal, Metallurgiya, no. 6, 1962, 19, abstract 6014'1
C'Sb. nauchn. tr. Irkutskiy n.-i. In-t redk. met.", no. 9, 1961,
1055 - 171)
TEXT: The results of thermodynamic calculations of sulfating Pb, Zn, Cd,
In and T1 compounds by means of FeS04 are reported. These'results substantiate
the necessity of investigating the sulfating of Pb-powders. There are 8 ref-
erences.
[Abstracter's note: Complete translation]
Card 1/1
--ZYRYLNOV;--M.-Ii.;-NADOLISKIYp--A.-P.-
Complex treatment of dusts from the lead Industry telth a high
selenium content. Trudy Vost. Sib. fil. All SSIM no,1+1:12e-131
162, (MIRA 15310)
1. Irkutskiy nauchno-isaledovatellskiy insti tmt redki kh metallov,
(Lead industx7-By-productz) (Fly ash)
Mikhail Nikolanvich; SUIIKIN, A.N., red.; BATOTSYMNOVA,
D. B.', tekhn. red.
(Rare metals,, their discovery and use] Redhemetally, ikh
otkry-tie i primenenie. Ulan-Ude, Buriatskoe knizhlloe izd-vo,
1962. 50 P. (HIRA 16:6)
(Metals, Rare and mirtor) (Rare earth metals)
now" "Imm"Immm"O. mff""
S/137/62/000/006/049/163
AOo6/Alol
AUTHORS: Sinakevich, A. S., Z M anov, M. N.
TITLE: Application of the ccntinuous chlorination method to lean oxidized
molybdenum raw material
PERIODICAL: Referativnyy zhurnal Metallurgiya, no. 6, 1962, 17, abstraA~60131
C'Sb. nauchn. tr. Irkutskiy n.-i. in-t redk.Allet.", 1961, no.,9,
184 - 192)
TEXT: The practical possibility is shown of applying the method of~con-,
tinuous chlorination with gaseous C12 to lean, oxidized Mo-raw material. The
optimum dimensions of granules for continuous chlorination are 2 - 3 mm; chlo_~
rination time is 1.5 hours at 4300C, with addition of 8% pyrite concentrate and
560 - 620 kg/ton C12 consumption, Conditions are given for the selective con-,
densation of sublimates and their processingto commercial products. Mo extrac-
tion was 80%.
0. Svodtseva
[Abstracter's note: Complete translation]
Card 1/1
214570 81137161100010051009r,-60
A006/AI06
AUTHORS: Sinakevich, A..S.P ZManov, M.N.
TITLE: Chlorination of oxidized molybdenum compounds with vaporous, bhlori-
des
PERIODICALt Referativnyy zhurnal. Metallurgiya, no. 5, 1961,,18-19, abs .tract
50145 ("Sb. nauchn. tr. Irkutskiy n.-i. in-t redk. met!'), 1959,
no. 8, 220 - 229)
TEXT: The authors studied the interaction of mol~bdates of Fe, Ca, Pb and
Cu oxides with CCI and S2C12. During chlorination of CC14 the temperature should,
exceed by 50 - 100 C ahlorination temperatures Of 8 C12 In order to attain an~
equAl degree of decomposition of the salt; or the 812 consumption at the,same
temperature must be increased. Chlorination Of CC14, SC12 or Cl with addition
of pyrite and solid coal makes full extraction possible at 35d - ~`OOOC. Chlorina-
tion Of C12 in the presence of pyrite and chlorination or CC14 should be prefer-
ably performed. The reaction produats are Mo oxychlorides, mainly M002CI~, MbOC14
and chloride metals contained in the comnepsition of the compounds.
[Abstracter's note: Complete translation] G.S.
Card 1/1
Moll
~--.M~111 W M-111. I I'm M..
N.D.; lyttyAN-OV KOHOSTIELEV, P.V,; GOUN, V-Nl-
SIIAIA-UNOVY I
." L6
Production of cast# pipe-ro2ling equipment, no.'LC109-10
(Y. T
0 164. -RA 1814)
IKFNG, Pikolay Petrovich;-MIYANOV Mikhail-Yegorov~o~h- TSMMOV,
Grigoriy Artemtyi-vi~c; KASIHTANOV, F., red,;IMIOLIVKO) V.p
tekhn. red.
(Conveying system for the transportation of.'Pece freight]
Konveiernaia ustanovka dlia transportirovaniia shtuchnykh
gruzov. Minsks Cos. izd-vo BSSR. Red, proizvodst,7emol lit-
ryp 1961. 52 p. (KIRA 15:2)
(Railroads-Freight) (Conveying machinery),
40
(tt
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02 "c'l qj
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SOV/139-58-6-24/29
janoiL P.S
AUT"HORS: Yeleonskiy, v.M. aad,~jr
TITO on the Theory of the Energy Speatrum of Systems; o:r
Interacting Particles~ (K teorii energetiohesiko-b
spektra qis.tem -uzaimodeystvuyushchikh chastits~
p&-RIODICAL:Izvestj_,YEj. V),sshikh Uchebnykh Zawdeniy, Fizikas~
1958, Nr Gr pp 152-157 (USSR)
ABSTRACT: In systGms consisting of a large number of interacting
particll,-s each paiticle intera~ts'with a larger Il'umber
of other particles provided the density is sufficiently
hiGh. In the so --alled collective, interactions,
COUV,nuous medium properties appear. ~Howeveir, aot~ all
the properties cf a system consisting: of diserete
p&:ticles can be approximated by the properties of~ a
C-Isat'inuous medium. The diseietemss of the aystem
Ld-11 appear in prooesses which ta.1w plaie in s 11'
spatial regions which am of the brder of -the inter-
particle distance. Hartree-Fook,eqpations. may te
nically s-o.ch collective
used to describe quantum mech&
interactions and a Goneralised fo'rM, of these e uativons
Card 1/3.~: covering non-stationary states is given by Bq,?].)O,
SOV/1300-~-58-6-24/29
On the Theory of the Energy Spectrum of Systems of Interacting
Particles
The plus sign applies to boson 5 and. the minus sign to
fermions. Recently, these e(rfati=s have Wen used both
in nuclear theory and the theo'ry of metals .(Ref. 3). It
follows from Eq (1) that the density matrix is given
by Eq (2). The discrete properties of the system can
be described in terms of the scattering problem
formalism. One of the properties of the non-linear
Eq (1) is that they have solutions inthe fom.of plane
waves, i.e. they have a solution ,,,orresponding to a
constant density of particles~,ia tha system*' It follows
that states of the system in which, the density.is almost;
constant may be desoribed by iwans of lineariseld
equations of the form (1) in the neigbbourhood of
solir'vionz with coastant, density. The present paper is
concerned with setting up thedispersion equations for
a system of interacting partir-les having small density
fluctuations. For this puipose izLstead of the complex
fun--tions *i(xt) real fuactions are introduced,by
Card 2/3 putting Pj3/2 (Xt),i1J-Sj(xt)h-1. The funations
S1)vi7,,9--5,5-,,6-.,24/29
On the Theory of the Energy Spect.rlam of Systems of Interacting
Particles
P i and Si are then f wind be, gi-7.en by Eq (3).
Idn-arisat'lon of the equations In the neighbourhood of
e
exact solutions:
Sj soj = --Eoit + pjx,. Vs J", P()"j IV() j
poj const
v
leads to the syst'jem of Bq W. The se relatJ,ons'are thbn
used to obtain dispersi.on ewaal;ionm for boson and feria-Lion
systems (Eq 6 and 3.2 :r-espel-Iti-wely),, There ana
7 references of which 5 are 2 Er.LF,1ish-
ASSOC IATI ON: Ural T skiy Politekbnicheskiy Inntitiit-, imeni S.M.Kirova
(Ural Polytechni~,,al Instital'-.e 'Lm,-ai S.M~Ydvov)
SUBMITTED: 20th Janu -rY 1958
Card 313
AccEssiar NR: AP043435 G/0050/64/006/W2/0401/01108
AUMOR: Zy*ryanov, P. Be
TM: Quantum theory of thermoga1vunauagnetic yhe
TI nonena in metals and
semiconductors
v. 6
SOLMCE: Physics. status solidi,, no& 2, 1964, 401-1108
TOPIC TAGS: quantum theory, quantized magnetic field, tbLermoGaivanonagnetiam,
semiconductor, semiconductor thermogalvaacmagnetism, electric energy opectr=,
relaxaticn mechanism, molecular current, ccinduction electica.. coaducticn cur-
rent, nondissipative density, dissipaticn density
ABSTRACT: Inasmuch as recent attempta to construct a quan th
t.UM theory, of e=101-
magnetic riiencmena contradict either the clasuical theory or the basic laws
of thermodynamica, the author offers an explanation of inherent dilpf icultics
throuah a calculation which shows that in a quantizing wagnatic field the vol- t
umetric current density of the j charge.. calculated vith tbo. aid of the denBity'
matrix,, does not coincide with the density of the coaducticn current jnp$ oving
to the appearance of Landau dimawpetiomp which causes a "molecularn a
current
vp
-A
al Ia- APIA3435
ACCESSI
rot M (M is the magnetization of the conduetioll ejactrolla) a, e oa-
long Vith th c
auction current in sterie nonuniform systems, but rather is defined by
j + c rot M. Similarly, Q rather than % alone (Q is the
np /C jnp M QT + %I
volme density of the energy current, T is temperature in energy units, (- In
the thermal current, 044 is the magnetic energy current, and ~ U the ch'L,12ca1
potential). On this basis the author derives fonnulan :Vor the nondissipative
density of thermal and electric currents in a quantizing magnetic field vith
electron spin taken into account. Ile also derives expreosions for the dissipa.
tion density of these currents on t%e basis of the elastic scattering apprcmi-
mation. Me results permit calculatim of any thermogalvanomarpetic effect
under conditions of a strong quantizing magnetic field (1Z * I VL io the cyclo- ,I
tron resonance frequency, and Via the relaxation time)# Origo art. has: A
formulase
ASSOCIATION: Institut fiziki metaUov AN WSR,, Sverdloyak (Institute for Physics
of Mletals)
SUBMIM: LIWWO~ "M41M. 00~
SUB dMR W, 68 NO F" S 0v f 005 .00 I'll
:,ca
2/2
L
1
2
-6 F(n)-2/li.~IG(k)/PWP(q)/EWT(m)/BDS~~- 1FFTCA$D/E$D-3/-
IJ~P~(CL)1/~SSD Pa-4/~;i7-4. JON
T
ACCESSION NR: AP3007497 /0181/ 76/25~?
S 63/0051009/25
AUTHOR:, Zy*ryanov, P. So
TITtEt The influence of phonon drag on the.lon:tlat~ al thermo-
electromotive force-of semiconducto-K and setni in longitudi-i
m
S
nal magnetic fields ?X
SOURCEt. Fizika tverdogo tela, v. 5, no. 9,, 19630. 2576-2579
TOPIC TAGSs phonon drag:effect,.phonon drag~i the'rMoelectromotive
force, thermoelectric power, Seebeck electromotiv f orce 'lonsi-
tudinal effect, semiconductor theory
ABSTRACTt The part played by phonon drag in~~the longitudi ~al ther-'
n
1 momagnetie effect is theoretically investigated by:lthe use of 'in
approximate solution of the problem for the inverse square'law;
electron dispersion. Formulas for the effect of the phono n dra
9
i on the thermoelectromotive force are worked out for both semicon-
ductors and degenerate semiconductors, and the case of vanishing
magnetic field intensity is considered. The~substantial part
played by phonon drag at very low temperaturao is indicated. Orig.
Card 1/2
---~--7- q
11111114,11 [Hill It IRI
SOV/126-7-1-24/28
AUTHORS: Zyryanov, F.S., Borisov, B#S. and Taluts, G.G.
TITLE: Propagation in a Metal (Oso,bennosti
rasprostraneniya zv-uka v metalle)
PERIODICAL: Fizika Metallov i MetallovedOniye~, 1969~'Vol.7y :Nr.l.,
pp 15.3-154 (USSR)
ABSTRACT: For describing the propagation of'sound,waves of;sufficiently
high enerSy-donsity (e.g. ultragonic waves) the;lattice
binding energies in a metal may be Ignored and the.metal
treated as an ionic plasma. The following relation will
then hold:
M 43 2 02
1 + X,
2
r2-, q
0
Here X is the amplitude of the ultrasonic wave and
the associated electric field potontial; M, 9 are respect-
ively the ionic mass and charge; 0 , q are respectively
the ultrasonic angular frequenoy and wave-nuxbor; finally
Card 1/4 to is a characteristic; angular fraquency of the':plasma,
0
SOV/126-7-1-24/28
Singularities of Sound Propagation in a Metal
given by: 2
4 r-. no
0
where n is the ionic density. Furthermore the acoustic
energy flux S in the z-direction may bo written~as:,:
where a is the sound velocity and
2
mnca X12 exp( -2,,r
_z)
2
with < denoting the sound absorption coefficient.A
relation between the acoustia and electric ener6y~fluxes
Card 2/4 which follows from the above is:
BOV/126-7-1-24./28
Singularities of Sound Propagation in a Idetal
C1 t x
where t is time and or is the ble'etrioal conductivity.
Now the left-hand side of this last~~equabion must clearly
equal div S, and from this follows.immediatel7 tha r6lation
between cc and V **
2
U) x
n(3
This shows that "anomalous" acoustic propagation
(acoustic absorption bands) will oocur under conditions
favouring high electrical conductivity: energy removed from
the sound waves appears as electric current. Such a current
will produce heating of the metal and th(a magnitude. of this
affect is discussed for some typical cases. Therg'are
Gard 3/4 3 references, of which 2 are Soviet and 1 English.
j1K
Singularities of sound Propagation in a Metal ;30V/126-7-1-24/28
ASSOCIATION: Urallskiy politekhnichoskly inst;ltutlimeni S.M# Kirova
(Ural Polytechnical Institute imeni S.M. Kirov);~,
:In6titut
fiziki metallov AN SSSR (Metal Physics Inotitute,:Aa. Be.,
USSR)
Card 4/4.
a r1 I HI. I IN H "11 If HOW If 11411HIIIII-11 If HIII
PU39 I BOOK EXPLOITATION SOV/4a93
Vxesoyuxnoye soveshchanlye po rlztke. fizlico-Ichimtchaskla 5v*Y8tvWX
rerritov I rizichesicia o3novam, 11th primenenlya. 3d, Minsk. 1959
P*rrltyt MIchasiclye I CIZIko-khImichosiclys svoy$tv4. Dokl4dy
Physical and Ph"Icochemical Properties. Reports)
XlA2k. Ixd-vo AM SUR, 1960. 655 P. ErrAt& 911P Inserted.
4.000 Caplan printed.
3poraoring Agenciest Nauchnyy aovet po magnetlxmu AN SSSR. Otdal
f1zlirl tvardogo tela I poluprovodnlkov AN BSSR.
19ditorlal Boardt Rasp. Zd. : N. N. 31rota. Academician or zr,*
Academy or Sciences ZSSR; X. P. Belov, Proressor; Ye. 1. Londar-
skl7, Professor; K. K. Poilvauqw; Professor, It V. Telesnin. Pro-
fessor,.G. A. 5001*"kly. Professor; X. M. Stwi -ts, Candidate of
2. N. 3001yezenko; azd
X. A. baswarov; Zd. of Publishing House: 3 . Xholyavskly; Tech,
Zd.3 X. TolokhmoovUh.
physical Chemists,
radio electronics engineers, and tachnicAl persorne, enVLgs4 In
the production and use or rerrOcAgoetlo materials. It may also
be used by Student* in advanced COUrfed in radio electronics.
and physic" ChealAtry.
COV12WASs ThO book contains reports presented at the Third All.
Union Conference an P.,Itgz hold in Minsk. BelorussS%n S31
.t.
The rGP=tx 4041 with uAgnetle transfor--ations, electrical and
Sal"AO"PtOtle Properties Of forrites, studies or the groth
or ferrite aina'a erystais, problems In the chemical and pftys..-
OCChNVICAJ WAlyniX Qf'fCrrjt4G. StUal&X of farritog haVIAg
ractafticular brat4reeLs LOOP, and Cult
'Itomponent rerrIte systamn
*XXIbit-tog spontaneous rectangullLrLtys problem In magnetic
attraction. highly cowrCive rerrltes, magnetic xpsCtrogc*:rY.
fsrrO"Znatlc resonextCe, sagnoto-optles, physical principles or
Using ferrite compon~ta in electrical circuits, "InotroP7 of
electrical and etIc propertles, ate. The Committat On Max-
natum. as MRIF V. Vfts"NklF, chairman) Organized the 4r~-
fareacw- -ROCtrances. "a0awy 144tvidual articles.
rarritos (cont.)
Parekallee, T. ft., and A. A, Aakothenskly. rnvostigation or
the Fsr~.gnet:4 Rdsonanc* or a cobalt ParrIte In an Internal
Field of Anisotro. p7
ara Z". V. Sicrotsicly.
%he
of%%Crrv~iz r-tgr-tl4 flt'dor=--C an the Optical
Properties or Yorroaus&natle and Paramagnetic Dielectrics
'
505
I.j OT, TU. A.
. and Q. V- Skrotakly. Magnetic Spin
X*80n"c6 In CO"uctlOn SlOctrOns In Alkali "4 PerrO-
W&gneclo Metals 513
gotywicy" N., ani A. X. Durnyaheva_ 7b& Ittfect of
Aalsot-optc Zlotstic Str*'&sqG.Qn forroOagottiv Resonance
lbscr7ttan In XIckel #*"It* S29
OuRbeh LeX. Z. X.. V. A. ftbrikov, and V. D. XWry*vto*v.
Temperature characteristics of Ferrite Components In SHP
Device*
card 1548
card 4Aa'
ZYRYANCV, P.S.
Quantum thoory of the excitation spectrum-of an electron gas in
a magnetic field. Zbur. eksp. i teor. fiz..40 no.4:1065-1071
Ap 161. (MIRA l4i7)
1. Urallskiy politekbnicheskiy institut.
(Electron gas) (Magnetic fields)
zmtyAmv, P.S.
v of acoustic osoilUt~ono of an OUatebn~-Ida!
Quantm theor
plasma in g mq tic field Zhio, iksp I teor,.fiz. 40 la6,5::
. pe
3.353-1-359 yq' I 61a. OM.14:7)
1. Uralrskiy'ndUtqkhnicbOskiy inatitut.~
ZPla#M- (laxazed gasips.))
(Mdgaetic-tields)
~-lLI-Nj V.P#
Integral of charged particle collisions a marmetic field.
Fize metj metalloved, 11 no,6*-955-957 A ~~61. (IIMI WO;
1. Ural'skiy politekbnicheskiy institut i,:Fiziebeskiy institut
imeni Pe He Lebedeva,
(Collisione(Nuclear physics))
ZYaYANOV, P. S.
Zyryanov, P. S. "Some Applications of the Method of Collective Inter-
actions to the Theory of Metals." Cand'Phys-Hath Sci, Moscow'Order
of Lenin State U imeni M. V. Lomonooov, 27 Jan 54 (VecHeFrqaY=aoskva,.
14 3an 54)
So: SUM 168, 22 July 1954
USM/Physics Conductivity FD-2872
Card 1/1 Pub. A6 - 9126
Author Zyryanov, P. S.
Title eory of the electrical conductivity of metals,
Periodical : Zhur. eksp. I teor. fiz., 29, August 1955,,193-2W
Abstract : The author calculates the fluctuations executed by the potential
of the internal electrical field In the electron-ion plasma of a
metal and also determines the electrical resistance which is due to
the scattering of the electrons during these fluctuations. Quaatita-
tive comparison of theory with experiments indicates the extent to
which one can approximate the properties of alkali metals by,the
properties of an electron-ion plasma.. He cites his earlier work:
ibid., 25, 441, 1953- Thirteen references: e.g.' Yu. L. Klimouto-
vich, V. P. Silin, ibid., 23, 151, 1952.
Institution : Ural Polytechnic'Institute, Sverdlovsk
Submitted : May 21, 1954
USSR/Phyrics Relaxation fluctuations FID-2969
Card 1/1 Pub. 146 - 10/28
Author Zyryanov, P. S.
Title Relaxational fluctuations in condensed systems
Periodical Zhur. eksp. i teor. fiz., 29, September 1955, 334-338
Abstract The author discusser. the problem of the separation of flu6tua-1
tions into "small-scale" (relaxational) and "large-scale" (vi-.
brational). He evaluates the role of rel~xational fluctuations
in electrical conductivity of metals. He thanks Professor V. L.
Ginzburg for his advice. Eight references: P. S. Zyryanov, ibid.,
29, 193, 1955-
Institution : Ural Polytechnic Institute, Sverdlovsk
Submitted ; May 21, 1954
Category USSR/Magaetism - Diamagnetism. Paramagnetism
f Zhur - Fizika. No 2, 1957, No 4026
Abs Jour Re
Author Z P.S., Yeleonskiy; V.M.
~;Tyanov.,
lust Uiair-PbUyEe-MnIc Institute, imeni S.M. Klrov,, Sverdlovsk) USSR
Title Collective Description of Magnetic Interactions,.
Orig Pub Fiz. metallov i metallovedeniyey 1956, 2, No 2t 2o6-a4
Abstract Discussioa of the problem of separating the magnetic interactions
into collective ones and individual ones ("fare' and,"'nearti). 4'.
method is described for introftaing the collective operator of
spin dewity and is ellustrated with an example in which -the Coulomb
and dipole-dipole interactions are calculateC
Card
:,1/1
B-4
USSR/Theoretical Physics
Abs Jour Referat Zhur Fizika, No 5, 1957, No 10W
Au~hor Yeleonskiiy, V.M., Z
Inst Ural' Polytechnic iMiNoe
Title Contribution to the Theory of Collective Motions of~
Particles in Quantum-Mechanicil Sy-steMS.
Orig Pub Fiz. matallon i matanovedeniize, 1956, 2, Ito 3~ ~6-2-563
Abstract A general method is proposed for separating out the collec-!
tive motions in a system of may particles,by introducing
additional variables in the vave fuaction of the system.
Upon suitable choice of the variables, one obtta:Lis the sa-
me Hamiltonians of the collective notion, as obtained by
D.N. Zubarev (Referat Zhur Fizika, 1955, 2627),:Bohm and
Pines (Referat Zhur Fiziks, 1955, 71,56), and Tomonaga
(Referat Zhur Fizika, 1956, 27839, 2784o)~ A mthod is
proposed for separating the collective mation in a system
bounded by a surface, for example) volume;,and surface vi-
brations in the nucleus.*
Card 1/1
ZYRYZNOV, P.S.; TALUTS, "R,
Weak excitation spectrum of electron systems in an intermittent
field. Fiz.met. i metalloved 3 no.3:547-548 156. (MIRA 100)
1. Ural'skiy politekhnichaskiy institut Imeni S.M. Kirovs, i In8titut
fiziki metallov Urallskogo filials, AN SSSR,
(Blectrons) (Pield theor7)
r
Category : USSR/Theoretical Physics Quanttm Mechanics B-4
Abs Jour : Ref Zhur - Fizika, No 2, 1957,No 2936
Author : Zyryanov P.S., Yeleonskiy) V-M.
Iust -.-Ur-kF ~iytectic Institute
Title On the Linearization of the Hartree Equations
Orig Pab Zh. eksperim. i teor. fiziki) 1956, 30) No 3~~ 592
Abstract Explanation of a method for describing the collective interactions'$
based on the linearization of the Hartree equations about soIntions
with constant density. The corresponding Byutem of equations nd
the dispersion relationships resulting from tbam are written down,
Card 1/1
--F 126-5-3-20/3l
AUTHOR: ZyrypAo
TITLE., The Theory of the Surface Tensions of Liquid Metals
(K teorii poverijanostnogo nactyazheni7a zhidkikh meItallov)
PERIODICAL: Fizika Metallov i Met allovedeniy6, 1957, Vol 5, Nr'~ 3 ,
pp 545-547 (USSR)
ABSTRACT: The earlier calculations of Frenkei, in~vrhich thIel surface
is considered to consist of.a doublY charged layer, are
extended by allowing for the thermal oscillations.of the
ions. These thermal oscillations are shown to fall off
exponentially with depth, and to have the effect of
reducing the thickness of the double layer. The initial
equations used are the equations of',continulty, Poisson's
equation and the Bernouilli-Euler equation; E is the
limitin- Fermi ener6y of the degenerate olectr8n gas.
The final formula agrees satisfactorily with experiment,
as is shown by the table, Which lists the.standard,
parameters of some metals; the last,two columns are the
theoretical and experimental valueslof the temperature
coefficient of surface tension respectively.
Card I
1/1 There are 1 table and 8 references, 6 of which are Soviet,
2 En l' h.
ASSOCIATI?N: jraTjski~ P9lijekhntqheskij inot't t *4ieni S.bl.Kirova
Ura Po yte hnica Ins itute me nph MKkirov)
SUMITTED: March 26, 1957 1. Liquid metals--Surface tension
Z S.
AUTHOR ELEONSKIY 'V U ZYRYANO F4 - 2964
'TITLE On the Theo;; o*l-t~MNUV~ective~gotions of Particles in Quantummocha-
nical Systems.
(K teorii kpllektl:vnykh dvizheniy chastits v kvantomakhanicheskikh
aistemakh -Russian),
FaIODICAL Zhurnal Ekeparim. i Toorot, Fizikij 19571 Vol ~2, Nr 3, pp 515-519.
Received 6/1957 Roviewed 1/19~)7
ABSTRACT The method of the separating th6 collective,mations in a system-dis-
cussed in the presefit paper is simple in-as-much as. voluminous appaxa-
tus of second-quantization and of unitary transformation are not r6qui-
red. This method is.based upon the transformation of the HAMILTONIAN by
the introduction of a system of additional variables Into the, wave'func-
tions of the system. Into the wave function.Arj~;;r I t) desckibing the
state of a system with the HAMILTONIAN H p, a + (1/2%6(?, i#Vr J)p
the authors introduce additional (Ilsurplusllj~ J
variable functions-,Pj(rj)-(j * l,2*oaN),vhich$ for the time being remain
arbitrary. Instead o 1p, the authors Investijate the new,wave function
(functional ofpi) t) The operator Itj is to
be replaced by the operator -ift,LVj +.(Vj;-fjWa191ii. Also the share;the
potential energy-'can be expressed by,the*16ctions -fj(~j). Next~ the func-
tions -pj (rj) are discussed. By )Pi. the coordinates of collective motion can
Card 1/2 be expressiM. The describtion of the -collective,matiopp wibbin the system
- - ------------
On the Theory of the Collective Motdons of PA - 2964
Particles in Cuanummechanical bystems.
will be better, the better the one-particle functions are selected.
Next, several special cases of the selection ofpi are discussed.'The
interpretation off (r~) (wave function of the steady state of the,j-th
particle in zero- A a prbximation) used'herc rendera the determination
of previously deriv6d HAMILTONIANS possible and shows possible vay~ for
3Alution of the boundary problems..The authors first put1f
th;2 j(rj)
expl-A&jI.This wave function describes the steady state of,'.k free
particle with the momentum t't. Nexts, another example for the "solution,
of the boundary problem is dealt with. The special cases of the selection
of the functio63)Pj(r ) dealt with here permit the generaUzation of this
method for other problems. (No illustrations).
AWOCIATION Ural Polytoohnical Inatito
PRESMED
SUBMITTED 21.1ol.956,
AVAILABLE Library of Congress.
Card 2/2
-C 4r i-4 N ~~ V
- T_~~
kUTITOU
, .
-56-T-54/66---
I: 1Y3 V-!J- ZYR'fA_';()V) P -~i
IMU On the ApplicatTon- of Mell-artrea-Pok EquatLonn tc a Systtim of
".Uasiparticles.
(0 primenerii uravneniy Xhartri-Foka k sisteme
PERIODICAL Zhurnal hiksperim. i Teorut.Fiziki,1957, Vol 33, Nr 7,pp 289-291 (Uffsa)
A33TRACT The states of a system with many particles rihich. are in strong inter-
action and are near a certain !frrourid state cin be describecl. by an a,3-
sembly of qaasiparticles near the oround state may be looked uDon 4a
insignificant and interaction among them may be di3reLrarded.Hovever,
in sy,9tems with strong "non-ideBlityll the number of quasiparticles can
be rather high, and their mutual interaction raust then not 13e neglec-
ted. The present paper de3cirbee an attempt, made to take interaction
among quasiparticles into account within the frp-neviork of the self-
consisting field. For a system, which has ~n average of 11 quasi~ar-
ticles per volume unit, the systei,,i of Hartree equations can ble -filritton
down as fol ows in dependence of tine;
r :p 2d'r r
i T + fGoje T Here G 0
2m
denotes the kernql of interaction among the particles. By:the iiub-
stitution T QI/2exp i S /hl these evations can be writt (en do'-un in
hydrocynamical from: 1 2 2
(r ')I d? '- -f-
S + (VS + fG(j Z
Card 1/2 Q,
j 2a 3. 4m
the-A-pplicati a n- o--the-1 a-rtroe-Fol, 1'q,,uati(n,_- -tc- a --56-7-54/66
System of
A'"'SOCI!,TION
PRIZEITTED BY
AVAIUBLE'
Card 2/2
Qj
ion with const I/V and eith S0=m(V,90,) r -Eo*t + const,
(Here V denotes the volume of the syst-E-m which iz here asB-aned to be
equal to 1). The energy spectrum of a syste~i wWch ia nearly in a
state with constant density can be determined fro;,i the just, written
down lincarized systeia of equations. A dispersion equation is given,
and also the equation resulting frora takin.- the exchange interaction
into account. A generalization of the here discuiised :aethod consists
in the develooment of a -scrieral T)rocess for the determination of the
quantity (VP ~)2 which occurs in the aforementioned dispersion equa-
tion.
('11o illustrations)
Ural Polytechnical Institute (Urallskiy polibekhnicheskiy institut)
Library of Congress
AUTHORS: Yeleonskiy, Y. M. and 7jyryanov, P. 13. SOV/126-6-1-21P/33
TITLE: On the Possible Effec':~-~ec~trom~agE-e-tie:Radiat ion
on Electrical Conductivity of Electron Conductors
(0 vozmozhnom vliyanii elektromagnitnogo izlucheniya
na elektroprovodnost' elektronnykh provodnikov).
PERIODICAL: Fizika Metallov i Metallovedeniye, 1958, Vol 61 Nr 11
PP 171-172 (USSR)
ABSTRACT: The interaction of longitudinal ana transverse vi brations
in spatially homogeneous electron plasma in conductors is
absent in the linear approximation only~in the case of
spherical symmetry in the electron-velocity distribution.
If, however, an electric current 11 ows through the ,
conductor7 the electron v-elocity dl .stribution will not
be spherically symmetric and this ~;ill lead to an
interaction between the transverse:ancl longitudinal.
vibrations of the plasma. in metals, electron
vibrations cannot be excited by therinal motion since the
energy of a quantum of such vibrations hw, is large
compared with the energy of thermal motion (kT)~
Card 1/2 However, if the metallic specimen is irradiated with
light whose frequency w is greater than w0 then the
SOVIL-26 6-1-~v24/33
On the Possible Effect of Electromagnetic Radiation on Electrical
Conductivity of Electron Conductors
transverse field in the specimen will excite longitudinal
vibrations of the plasina. The scattering of conduction
electrons on these longitudinal vibrations will lead:to
an increase in the electrical resistancd, The calculations
reported in the present paper are concerned with the
existence of such an effect. It isl Bhown that in, solile
cases the interaction between the longitudinal and
transverse fields does take place. A quantitative
estimate of the effect of electromagnetic radiation upon
the electrical conductivity of a conductor will be given
in a future publication.
ASSOCIATION: Urallskiy politekhnicheakiy institutlimeni S.M.Kirova
(Ural Polytechnical Institute imeni S. 19. Kirov.,
SWMITTED: March 26, 1957
1. Conductors-~-Eleetrical propertidb2Light--Electrical
effects 3. Electrons--Vibration
Card 2/2
AUTHORS: Yeleonskiy, 7. and S)OV/126-6-3-31/32
TITLI~: On Fluctuations in Spin Density in an. Electron Plasma. (0
fluktuatsiyakh spinovoy ~'Iotnosti v elektronnoy plazme)
PERIODICAL- Fizika Metallov i Pile tallovedeniYe , 195;B~ Vol (5: ITr 3,
Pp 573-575 (USSR)
ABSTIZACT: Pluctuatioas in the sj~in densilty ia a systea. of inter-
acting electrons are due to magnetiel(spin-spin -=d sbin-
0
orbital) as well as exchaqf,~,,e Coulomb:~interactions. , The
presence of these fluGtuat-ions leads to the apDearance of
electromagnetic fluctuation fields which have an effect'. UDOn
the physical properties of the system. (electrical canduct-i-
vity, specific heat, etc.) These interactions may be taken
into account by a method analogous to that Siven in (Ref.1),
using Pauli's equations. It is shovw- that interactions
associated with spin have only an effect upon the spectrum
of transverse vibrations. From the dispersion e uations for
fluctuations in the spin density, Eqs.(2Yand (3 , it follows
that fluctuations of spin density cannot have a very' great
effect on physical properties of metals, ~i-nce these flue-
tuations are not excitable by theri-,iaLmotlon or ara small
compared with the usual elastic vibrationd. Thero are
Card 1/2
BOV/126-6-3-31/32
On Flactuations in Spin Density in an Electron Plasma
2 Soviet and 1 English references.
ASSOCIATION: Urallskiy politelchnicheskiy inatitut~,-imeni S. 14. Kirova
(Ural Folyteelmical Instibute, im, S.Ail. Kir,ov)
SUBMITTED: March 25, 1957.
1. Metals--Physical properties 2. Electron gas--Density
3. Nuclear apijia 4. Mathematics--Applications
J
AUTHORS: Zyryanov, P. S., Skrotakiyj G. V. 56-1-32/56
.TITLE: On the Influence Exerted by the Electric Polarization
Upon
,
the Magnetic Properties of Forritea (O~vliyanii elektricheskoy
polyarizataii na magnitnyye evoystva forritov)
PERIODICAL: Zhurnal Eksperimentallnoy i Teoreticheakoy Fizikii 1956,
Vol. 34, lir 1, pp. 222-223 (USSRY
ABSTRACT: The taking into account of the spin-orbit-interactioh of the
d-elootrons in ferritea leads to the fict that the effective
magnetic permeability depends on the electrical polarization
of the electron shells of the atoms (i.- e. on theidie-
electric constant). in the ferromagnetio*metals this
dependence is not observed in thelmeasaroments on"the radio
frequencies due to the high polarizability of the.con duction
electrons. The following may be expected; In some'types of
ferrites the electric properties fiot only manifest them-
selves in the nature of the frequency-dependence Of the
effective permeability as well avin thewidth, shape and
position of the lines of the resonance absorptionibut also
in the dependence of these effects on the dimensions and the
Card 1/2 shape of the sample (which are not taken into account in the
.. . .........
On the Influence Exerted by the Electric Iblarization 17pon 56-1-32/56
the MaGnetio Properties of Perrites
method of demagnetizing factore)i The s2in-orbit interactions
can be taken into account within the fr'ame of the macroscopic
theory when starting from a closed set.of the modification ..
of this polarization of the totality of the interacting atoms
with an internal electromagnetic tield. The authors then
calculate the impedance Z by calculating by means of the
original set of equations the problem for the semi-infiniti
'te for the-case of a wave normally
1;6dy filled with a ferr-,
'inciding upon the boundary. The taking into account of the
electric polarization of the ferrite leads to a shift of the
resonance-frequency and to a widening of the resonance line
of the absorption. There is 1 reference vhich is Slavic.
ASSOCIATION: umi Polytechnic Institute (Urallskiy politekhnichelskiy
institut)
SUBMITTED: August 2, 1957
AVAILABLE: Library of Congress
Card 2/2
AUTHORt Zyryanov, P. S.
TITLEt
PERIODICALs
ABSTRACTt
Card 1/3
56-1-37/56
the.
Coulomb's Correlations
On the Influence Exerted by
Vpon
Oscillation Spa ctrum of an Eleetron.,Pl'aama (0 Vliyamii kulo-
novykh korrelyatsiy na spektr kolebaniV elektronnoy plazmy)
Zhurnal Eksperimentallnoy i Teoreticheskoy Fizikiv
Vol. 34, Nr 1, pp. 232 - 233 (MR)
By the author's opinion the problem 0ifthe influenIce of the
Coulomb correlations has.not yet been; determined IinIzany pa-
pers on the collective osaillatLons of.a plasma The solution
of this problem may be attackedAn different wj-,~s. E. G.~the
kinetic equation can be set up'with the taking i nto.account
of the correlation and with this equation the dispersion equa-
tion for the small oscillations ~of the density can then be
determined.L. The dispersion equation obtained in this manner
will then express the frequency~~4a (k) by parameter ; which
characterized the spatial distribution. The mdn charracteristic
of this state is the average energy of a particle with the
56-J-37/56
On the Influence Exerted by Coulomb's Correlations Vpon the Oscillation
Spectrum of an Electron Plasma
taking into account of all inte:xactione (kinetic energyj ex-
change interaction and Coulomb oorrelations). A seeond way
for the solution of this problem waslinvestigated by V. M.
Yeleonskiy and P. S. Zyryanov.(reference 1). The small de-
viations of the density from the homogeneous density are de-
scribed by linearized ffartree~(Xhartri)-equatiohs with a time
dependence represented in a hydrodynamic form. In this con-
nection the coefficients of the linearized equations are
expressed by the energy of the particles in the,grourd state.
The dispersion equation for the'cawofmak perturbations is
explicitly written down. Especially the expressionlocourring
in this equation for the average enera for thebcaqe of the
electron gas is specialized. Then the author givesan expres-
sion for the frequency cf the natural oscillatEons. -In metals
the exchange effects play a more important part th= the
Coulomb correlations, There arel reterences, 1,of which is
Slavic.
ASSOCIATIOUs Ural ?olytechnic Institute (Itrallakiy politekhnicheakiy
institut)
Card 2/3
56-1-37/56
On the Influence Exerted by Coulomb's Correlations Upon the Oscillation
Spectrum of an Electron Plasma
SUBMITTEDt September 27, 1957
AVAILABLEt Library of Congress
Card 3/3
AUTHOR: Z.'__~ryanov, P. S. 56-2-34/51
TITLEt Collective 11otion in a Systerj~of Quaoi-narticles
(Kollektivnve dvizheniya v aitewe kyazicbastito)
PERIODICAL: Zhurnal Eksperimentallnoy i Teoretic'iesko,f Fi-iUq 1956)
Vol- 34, JTr 2, pn. 100 - 509 032R)
ABSTRACT: In the approximation of the self consisting field,the tak-ing
into account of the stron, interaction leads to .3-dependence
of the enerjy of a sin,3le particle (conaidered here an quas--;-
particle) on the state of motion of the rest of the P~rticles
of the system, Even with spatial homogeneous distribution of
the particles of the system the takin.- into account of the
interaction leads to a complicate ,d dependence of~thelensr-
gy of the particle on its momentum. Firat anexpres3ion for
the Hamiltonian of the quasipartioles Le ,,,--;ven fo-- the case
of a spatially inhomogeneous diatribution. 'The first.term
here takes into account the correlitionlat a snall distance
Card 1)3 and the kinetic energy, and the second term takes into ac-
H111111111 IlM OWNS INIERMIUMMIMMIEM
56-2-34/51
Collective Motion in a System of Quasiparti.clas
count the distant interactions( 11artreu: field). :Then the equa-
tions of motion for P. are mentioned. .The author restricts
himself to the investijation of tbose states of.the system
which come close to the spatially homogeneous distribution
of the quasiparticles on the coordinates as well as of the
undirectional distribution of velocity: These states .are
close to the ground states In thio,caso the Momenta o .f Jhe
collective motions will be small and tf .lc operators
Occurrin... in the initially,nantloned 11:11ailtoniancan ic re-
presented in the form E (-ffo + Here denotes I the momqn-
tum operator of collecti4a motion (a small quantity) Knd -It,
denotes the operator of the momentum of: URIireotional:no- 0
tion. E - i2 expanded into a series to -P, the auithor,re-
strictinG Rimself toAthe squared terms in relatiop, to
Then a new variable I canonicallY. conjugated to *-It, is intro-
0 0
duced into the wave function. An equation obtained this way
only describes the~collective motion in the sYsten Of the
quasiparticles and the coefficients of this equation depend
L.quasi-
on the characteristics of the undirectional motion of
Card 2/3 particles in the ground state. The disperse equation result-