SCIENTIFIC ABSTRACT BALASHOV, S. I. - BALASHOV, V. V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000103220008-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 3, 2017
• Document Release Date: July 27, 2000
• Sequence Number: 8
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

- - ---- - --- - - - -- -- -- ---- - -----------
ARSXNIYIIV, Lev Borisovich, Insh.; rIlATOV,
BAIASHOV, Sol*@ Inzh. , red.
*%N-I -
[Nxperience in building large panel
stya krupnopanalloogo shilogo down.
informs, 1956, 16 p, (Informatelia
rabotakh., Tana 310 no,1-56-101)
(Apartment houses)
A.I., Inzh.. Yedushchly red.;
apartment houses] Opyt strottell-
Moskva, In-t takhaiko-skont
nauchno-iseledoystel'skikh
(MIRA 11W
---. 0 -
Let's honorably fulfill the task* of the seven-year plane
Na stroi.Mook, 2 no,3:i-4 mr 159. (MIRA 12:5)
1, 2amestitell mchallnike, Olavmosstroya.
(Moscow-Construction Industry)
KALIMKp V.V.t Insh., rod.; BALASWV S.I., insh., red.; BOGATYKH,
Ya.D., insh., red. -red. - PAVLOV, S.H., red.;
KHUDYAKOV, A.K., red.1 PETROVA, V.V., red. isd-va; IFTIM,
G.A., red. isd-va; KOHAROVSKAYA, L.A., takhn., red.;
RODIONOVAv V.H., tekhn. red.
loations and regulatioul Stroitel'We
[Construction spoof
norwy i pravila. Moskva, Goestroiisdat. Pt.3. Sec.A. ch.7?
(Basic principles for qrSoxising-labor (SViP 111-A.7-62)1 Or-
ganizatsila trudal oenovnys poloshenlia (SNiP III-A.7-62)
1962. 4 p. Pt.3. Sec.V. ch./+.(Regulations for production and
inspection of work in stone construction (SNiP III-V.4-62))
Kamennye konstruktaii; pravila proisvodstva L priemki rabot.
(SNiP III-V.4-62) ~963. 11 p. (MIRA l6t6)
1. Russia (1923- U.S.S.R.) Gosudarstvennyy komitst po, delam
stroitellet". 2, Gostroy SSSR (for Kalinyuk, Gribin).
3. Meshdu"dometyennaya komissiya Peresmotru stroitelinykh
norn i pravil(for Balashov, Pavlovr.~4, Nauchno-isaledovatell-
skiy inatitut organizataii, makhanizat6ii i takhnichaskoy po-
moshchi stroitelletvu Akademii stroitel'stva i arkhitektury
SSSR (for'Bogatykh, Khudynkov).
(Building, Stone)
(Constmotion industry)
At. A '.Orri' 1-%~ Inz!_
M
i oto r t tow k I t i. ni.
Dtl Vli VPX S).14'. ~!P::,
A I t KTH 1 11.1 W J
r
e
-tserizent -PIRMY MTV k-w,; tlk'ITI
1~ 111th., na
[Large-i.-ile Ailly convl.rG-ulv!l Jrj
o' - v
[Py] -evut'
BALASHOVp Semen Tegorovicb; SPITSUA, A.# red.1 SHlffKj, M., tekhno red,,
(Inculcating a feeling for the niv and progressive] Vospitanle
ohuvetva novogo, poredovogo. Moskva,, Moskoraboahii, 1961 73 P.
(MIRA Wl2i
1. Ukretarl partiynoy organirAtaii zavoda "Hoskabell I (for Balashov).
(Efficiewyo Industrial)
PARSHIIIII A.H.; PICRUPELKIN, A.S.1 BALASIUY, S*Tu.
Assambly Una for narkllii'out and examining fabric. Tnkst.
prom. 18 no.902-43 8 158, (KRA Iwo)
(Cotton nanufacturs)
USSR/Cultivated Plants - Potatoes, Vegetableso Melons. M-3
Abe Jour Rof Zhur - Biol., No 7, 1958, 29820
Author Balashov T,Ne
Inst
Title The Influence of the Type of Pistillate Flowers in Melons
on the fruit gets
Orig Pub Tro po prikle botan., genet. i selcktaii, 1957, 31, No 2)
189-190
Abstract Melon fruit setting was studied in relation to the type
of Pistillate flowers: 1) female, 2) monoecious with
fertile pollen on the stamens, 3) female with vestigial
stamens. It was revoo2ed as a result of the intervariotal
pollination of the large melon collection that the per-
centage of fruit setting in plants with flowers of the
first type is nearly twice as great as in the plants having
flowers of the other two typea (22.6 as compared to 14.5%)
A similar result was obtained in 1955 with the cross-
Card 1/2
US-`O/Cultivatcd Planta - POtatOOG- Vegetables. Melons, M-3
Abe "r * Ref zhur - Bio.,.. No 7. lorA
v T,N.
Varietal tnms Of EUrOPftn melons. Trudy po priki. -bot. . gen. - i,
Sol* 32 noo3t233-247 '59, - (MIRA 14'5)
(Melons-Variatise)
BALASHOV, T. N. Cand Agr Soi -- "Study of European melons as tstarting material
for solootions" 11ov, 1961 (Moo Order of Lenin Agr Aoad im K. A. Timirystev)
(KL, 4-61, 204)
'77
4M-
A- - o
Centralized repair of equipment. Prow.koop. noolo:26-27 0 15?.
(MIRA M12)
lslspolAya"hchty obyuannostl proylonlya arteli "Stankoremont,"
Leningrad.
(Repairing)
WCHATIV, Georgiy Kuslmich; NIWCHUNOVA, 0., red.; BAIABHOVg V.,
tokhn. red, - - - -, " - I
[Thiermistore in te"rature control] Tormosoprotivleniia
v te"raturnom kontrole. Xiev. Gos.isd-vo tekhn.lit-ry
USSRj 1959. 205 pithermistors) (MIRA 120)
-,IBALASIIOV, V.; FELIDMAN, A.; POWIOROV, A.
Now book on Pneumatic and hydraulic transportation of food industr7
bV M,14,Korobovs Fem,i apirteprom, 31 no.1%44 165. (MIRA 1885)
ROZENSOV, Isaak Samuilovich; BAJAS)IOV, V.A., red.
[Roving rrames]Rovnichrqe maahiny. Ivanovo, Ivanovskoe
kniahnoe izd-vop 1963s 54-po (MIIA 17:5)
Aloksancira Nikulayomn; V.A. p red.
[Sliver deliverlng machinco I Lentoolinye mavI&W. lvanavo,
Ivanovokoe knirhnou Izd-vo, 19(,4. 41) p. (NIRA i7i-.8)
WN Uol3fili , Aleksandr Fadeyovichk BLI '41;1,OVI_ V.A. , red.
[Scutchors) Tropalltiya mashitor. Ivarlovo, lvanovskoe
knizlinuo izd-vo, 19641- 55 v-. (MIRA 17:8)
DONSKOY, ALV., doktor tekhn. nauk, prof.; DONSKOYI, An.V.1
DRMINt S.V.) IMSKrY, G.V.1 KUYJITIII, A.M.; LErblli,
Yu.V.; MONDRUS, D.B.; SOLCFAKHIII, I.M.; FRUMKIN, A.A.;
BALASHOVI V.A,p retuenzent
[High-frequency olectrothervW; a handbook] Vysokochastot-
naia elektratemila; spravochnik* v,,oskva) Mashinostroenle,
1965. 564 P. (MIRA 18:0
I.DCHIN, Te.D,, kand, takhn, naukj BAWHGVv V.D., Inzh.
Building approach canals to industrial enterprises. Rech,
transp, 22 no.9s23-24 S t63. (KMA 16tlO)
--BALAMiOVP--V*-r*-- - - I I
Xsehanising the removal of wastes from betneath a oupola. Ut.proizv.
no,,9W S 162o (NM 15111)
(Cupola flurnaces-Equipment and supplies)
7-
A940;R0-32489 souRcE coDE: UR/0413/66/000/01T/0030/0030
INVENTOR.- Alekseyev, alanhov, V. A...--Gershonok, Me I.; Grachav, I. M.;
P. A.;
yegorov, Ire A.; Kobyllnitaka T--Kozlov D. A.-. Lifshits, A. I., ~bndrus, Do Be;
79 .72 S
Parshin, N. A.; Rashevskiy, A. L.; Rivkin, A. E.; Tallgren, A. A. -. Khansuvaroyl A, A.
ORG: none 1<
TITIE: Device for high frequency soldering of lead-acid storage batteries. Class 21,
No. 185368
SOURCE: Izobreteniya, proaWshlennyye obraztsy, tovarnyye znaki, no. 1T, 1966, 30
TOPIC TAGS., tietal soldering, storage battery
ABSTRACT: An Author Certificate has been issued for a device for high-frequency
soldering of lead-acid storage batteries. The device containsm h-f generator with
on Oxtornal tank circuit, a multiloop Inductor with open ferrite magnetic circuits, a
conveyor with n lifting tnble, a control dosh, and tin asromblinc'-soldoring former
equipped with a magnetic screen fnstenod on it non-rut;:.natic Sane. Orig. art. hall:
1 figure.
-- - -- - - --- - --- -- -- 3
V r)j.
Fig. 1. 1 - 11-f ganarator-, 2 - external tank circuit;
3 - Inductor; 4 - conveyor; 5 - lifting table;
6 - control desk; 7 - forr.*r; 8 - screen; 9 - base*
10,13 / SUBM DATEs
'WN t I 'T1
-AC-C NRo
Ap6015699 0) SOURCE CODE: UP,/0413166,/00010091009T,/0098 :2,
INVENTORt -Bala shov., JA___A Doteenko, A. M.; Kornilov, A. V.
ORO: none
TITLE: Method of studying the development of fatigue cracks. Class 42#~
No. 181361
:9,
SOURCEI Izobre~eniya., promyshlennyye obrazteyo tovarnyye znakil no,
1966s 97-98
TOPIC TAOS: cracking, crack propagation, fatigue crack
ABSTRACT% This Author Certificate Introducea a method of studying the
development of fatigue Aracks by applying a sensing element to the area
,of possible gr&cklng.. Whe sensing element consists of several parallel
conductors with a giv n law of variation or space between them, The
conductors are arranged perpendicular to the possible direction of
-crack propagation.j.In order to obtain diagrams showing the reltjtJ.on,-
ship between the length of the propagating crack and the number of load-,
ACC NR' AP6015699
ing cycles automatically, electric signals proportional to the spaces
l
,between the conductors of the sensing element are arranged to be trans-
mitted to the recorder which simultaneously receives the periodic
sequence of eleatrio pulses from the oycle.oounter, The time between
these pulses is proportional to a specific number of loading cycles of
the test piece
see Pig, 1). Orig. art. has: I figure. [Translation
[LD)
Fig, 1, Device for study-
ing the propaga-
tion of fatigue
cracks.
1-Sensing element,
2-automatic
recorder; 3-0yele
counter
SUB CODR: 20/ SUBM DATM 2714ar65/
BkIASHOVf V.l.p podpolkm*~ moditsinakoy sluMbyj USANOVAl A.-V.
Influensalike fom of food tocinfootion. Voon.-sod.shur, no-4186
Ap 160, (FOOD POISONING) (MIRA lrtl)
BAIASHOV. V.Ij_ARGUNOV, R.S.1 SOXOWV, I.A.; ROGOZ11IN, V.A.; WSANOVA, A.V.
Outbreak of food toxicoinfection caused by two types of Salmonella.
Zhur.mikrobiol., epid.i iwm. 32 no.M114 D 161. (KRA 15: 11)
(FOOD POISONING) (SALMONULA)
KRAVCHENKO, A.A., starshly nauchikyy sotmdnik; MIROMOV, D.I.;
--BAIASHOM, M.I. r-
emometry in hypertanaives. Trudy
Vestibulometry and
MNIKI np.51115-131 16:4 (KIRk 16 s4)
1. Otorinolarlngologicheakayn klWka,?bekovokogo oblastnogo
nauohno-isaledovateltakogo klinichea&ogo Instituta (direktor
zaalushennyy deyatell nauki, prof I.Ta.Sondullskiy),
(HYPERTENSION) iVESTIBUIAR APPARATUS)
(BLOOD-OXYGEN CONTENT)
KHOLOWK, Ye.D.; NlKlrFOROV, I.V.; RAYSURADZE, L.I.; ALEKSANDROV, K.I.;
BAIASHOV$ V.I.
Now metbodo for gravity surveying under the conditions or a dense
-forest* Sboroluch.rate.predl. pts 2:4-5 1639 (MIRA 170)
1. Ukhtlnakoye geologicheskoye upravleniyes
M-, I I f , ',$I i .,! ~-' :I .;I .
flew princ.1ple.; of rvouluLln
contInunon caltivut!un Qf
73-78 Ja-.-' 105.
1. Inatitut, m1krobiclor,11 AN
i .;.. ; I ... . I
I I I;..p . .
~ - ccriportItion of Ll~n vAAtur. In 1!.,,
%o-oreantsion. MikrobiologMa 34
"6014018
ACC NR - At 5MIRU' CODF- UR/0220/65/034/001/0D73/00778
AUTHOR: _1pruaa1ims,%siy, N. D.-Ierusaliraslq, X. D.; Shaforostova, L. D.;
-Balashov,
_/0
MG1 of Vacroblology,, AWSSSSR (Knatitut, mikrobiologii AN SSSR)--
TITLE: New principle for regulating the accnposition of media used in continuous
culturing of microorganisms
SOME: Mikrobiologiya, v- 34, no. 1, 196ort 73-78
TOPIC TAGSt microbiology, Coll, physiol~,e;y
ABSTRACT% In flow-typo apparatuses based tin the chemostat principle, sooner
or later 6 dynamic equilibrium is established between the multiplication of
calls and loss thereof in the liquid flowing out. The population and growth
rate of the cells, their morphophysiologic4il properties, and composition
of the culture fluid become stabilized at come constant level. Any change
in the flow rate entails a change in the ccmposition of the medium. Yet
for precise physiological investigations it is important to be able to vary
only individual external factors, leaving the others unchanged. To achieve
this purpose, the suth,*,ra propoaed a new device (here described in detail
and illustrated) permitting independent regulation ot the atuount of several
solutions making up the medium. It worked efficiently in continuous culturing
of Bac. megatherium for 2j months in a medium consisting of glucose, N&M,
MgS0 0 K211PO4. sodium eitrate, ammonium suctinate. NH4C!, Com 0 Mns , and-,
4 2 04
Card 1 2 VDC; 76. 8,Q2L3,___j
ACC NR, AP6014018
6up W-A~ur. Thij IMOm 1,aLv A,%, t"ic
Such indiceu of the process as optic: densit the culture and content of
~",KIIU~ifd
remainod stable at each flcw
residual nitrogen mid sugar in the culture
rate. The pil was virtually unchanged. Okg. art. hast I figure and 2 tabIps.
(JPRS)
SUB OODE: 06 SUBM DATE: OlFeb64 ORIG REF: 002

L~ard
KIV.1XV, B.P.; HALASHOV, V.L.; KOWHIN, A.A.; LFBFI'FV, V.V.
Separation of barium and strontium by the exchange method In
the system amalgam - solutions, Radlokhimlia 6 no. 1t114-
1.17 164, (MIRA 17,6)
- - - -KISEIXVP--BO-P*-l - BALASHOV, VA. - - --- - - - -- -- - - - -- - - - -- - - --- -
Texperature dependence of the separation coefflcient of strontium
and barium in amalgam exchange, Radiokhimiia 7 no.2044 165.
(MIRA 18t6)
W,A,SHGV0 V. V.
PAIASHOV, 1). 14. - "Localization axyl Removal of Foreign
Human Tissuea.w Sub 26 Mar 52, Acad Fed Sci
for the Degree of Candidate in Medical Sciences).
Bodies From
(Dissertation
SO: Vechernaya Moskva January-Deceml~er 1952
'IT) r-.- -f~rldd
licrvou-- fy
s yrtL-, - Ccntrri ll(,rvcut Syr-tc-.
Abs Jour iAcf Zhur - Biol., No 12, 1958, No 55065)
Author I-141?~r-hovl V.m.
Inr,t t I--osco--v1-bMTi4-lnvtltutc of M,;dicln,;.
Titlc tThv Rolctionchip of Narvo 0611P rnd Ccpillrrior Ifithin the
luolcur of tho Fteirl Norvo.
Orig Pub iUch. zvp. 2-Y Meek. mod.in-t, 1997, A, 96-99
Abrtrrct sBoth errotid crtarie-, of 5 evts undor n-rcostr vom fillad
vith indien ink i-ix-.d with FArtinc. Tho brrin vra then
hiLtclo:jcvlly exrrincd (the ttrininr wee parfon-cd recordint
tc the nothod of Niucl). On tho rdproracd vroculrr nctmork
the pritirry root rnd tho nuelcur of tha P-cirl nurvc (FN)
c.ppccr. Tho danrity of th,-j ctpillpry nctvork in the princry
root of FN is tirnifictntly ;:rllcr thrn in tho nucleus,
r1though it vrrior In the FN too, The rrurtort nu-ibcr of
c-pilltrior ir to be found rround the ncrvm! coll bedlor#
v,hich c-rc rrr-nrod in groupr. Two Eroupr of collF ;:,Py be
Crrd 1/2
WSR/Ihn~irn rnd Antriel Porphclojry ("cr--rl rnd Frtholo-jcrl) b-3
Narvown Systv - Cantrrl Ncrvcur Syvto-
Abe Jour t iic^L 4!ivr - Bi(,l.p No 12, IW, No 55W
diitin,pI:hLdI 1) rt r distrnc4 of 25A frot- th,- ccll body the
Icn,(,,th of tha c,pill!,ry network cuountr to (thu
-vor,-,-~ ',,Bang 286), the c-pillericn rdjoin the cell body for
1/4 - 1/2 of itr cirew.,foronco, 40 porcont of tho ccllt hrvo
cont.-et vqth tho cell body, th-; rizo of the cell body rrountr
to 22.-4QA.- ; 2) -t r dietf-ma of 2'j-,, the lcr.~th cf the cc
ill-'ry nct%-crk mcunt! to 110-180.A%. (thc rv,~r^,,zc bcinZ~ 2003-,
the c,-pillcrice rdjcin the call body for 1/4 of Itf circur-
fcronco, 10 pcm%nt of the ccllr hrvc centect with the ccll
body, the riv.,-o of the cull body rrountr to 13-26A%. . The
l,n,-th of the c-pillrry mtw,.~rk it not -Iviryc dcUrrinod by
the c-inu of the cell bodiec, howcvQrl for in thu ftret, -P
voll ra in tho racond prnup, girnt cullr hm.; inrifnific-ntly
short ncti-orks while thu reverse rry hc. truo in otharr.
Thorcfcro, it hre bcon vurravtc4 thtt in the r~;lrtionEhlp of'
ncrv,. ccllt end crpillrricr within th,~ Fli nuclLur, functicnpl
retivity dotarrinor thL ch-rrctQrirticr of fori wrictionr.
Cerd 1 2/2
YEV, V.I.; SALASHOV, V.M.
--------------
Study of the conditions of hydrogenation of geraniol to citronellol
!r, a bmtch-type autoclave. Trudy VNIISNDV no.625-14 163.
(KRA 17:4)
V.C.; FILYAND, A.I., !IWRT!~,EVP V.A.; BALLSHOV,
KUMICIMV, V.A.; YDSIIXTN, M.I.
Ilrocans of the lipid phase soloctive hydrog"n-t1kion of aranial
!r, a flcw system. Trudy VNIISNT)V no.602P,141 163. 1WRA 1714)
---- - -BAUSHOY YoN. (Leningrad, rurskina, 1/3, pavillon 26. kv. 66); BORISOV'*
- *wi#wt-1;;inCrad, Institutekly pore, do 5, f 1. 7, kv. 62-a)
The 50th anniversary of the Department of Normal Anatomy at the
Leningrad Medical Institute of Sanitation and Hygiene. Arkhowat,
gist. i embr. 35 no.6illo-113 N-D 158,, (MIRA 12il)
(ANATOMY, education,
hilt$ In Russia (Rua))
GUYANSKITO O.A.1 BAIAS Ih. N.
!~!Waty
Using emission radiography for studying the paragenetic rolation-
ship between minerals and the composition of ores containing elements
with a high atomic number. 'Geol, rude mentorosh, no65tI23-124 8-0
16o, (MIRA 13110)
1. Brednessiatekly asaahuo-isaledovatel'okiy institut geologil i
minerallnogo syrtya, Tiashkent.
(Radiography) (Kiuaraloff)
BAIASHOVv V.N.; POLYAXOV, A.K..
Experimental radiometric assaying in an antimony Ming.
Sov.geol. 5 no.W64P169 A 162. (KM 15:2)
1. Srednea-lataUy nauchno-issladovitellskiy institut
goologil i minerallmogo syrtyat
(Ores-Sampling and estimation)
(Antimony ores)
BAUSHOV,q V.N.j HOIGUNOV, V.S.
Gamma-quantum analysis for heavy elements, Biul.nauch--tekho
inform,VIMS no,100 160. (MM 1535)
L. Srodneasiatskiy nauchno-iseledovatel'okiy inatitut goologii i
minerallnogo eyriyap Tashkent,
JG&mms rays.-Industrial applicationa)
(Ores-ZA=3 I and estimation)
L 53736-65 EVF (c)AMAPA(s) -2/EWT(a)/rdP(i)/VWT(b)/W(s) P,j-4/rr-VPs-4/Pt-?
u"Itwir
ACC=1011 WRi
666.109.211
AMOR:S~kojlnlkoy, YR. A.1 Polik 8 'M I Karakhmidi, N. 0.1 Ivanov- P~ K.1
I ~ay b
-jjLtUL.XL-L. I - - et
1. Ye.4 OaLjX1LY-&j-jm-.JLa Yefinova, H. 1.1 8 yes
.2 ~hayev&~Yj. $,.I -
D!yIL_XP. i Nobstay. V .1 P~vqysvskftya' to A.1 Kukin. so Do-I
TITLEt Oless forjj!a fibers.,~Clua 32, No. 170369
SOURCE1 ~Yulleten* izobrtt*nir I toyarrWkh snakov# no* go 1965v 119
TOPIC TAM glass, glue fiber
AWWRAM An Author Certificate has been Issued for a glue suitable r as
glass fibers. To increase cheulW durability, to prevent corrosion o SUCY of
aluntnum and other light metals, and to improve proctuability, the glue Is for-
aulated to contains 58-60 8101, 2-V D20j, 6-61 A1201# 0.5-1.51 ?j0jj, 4-6S
U01, 6-8% C&O,'12-13% N&IO, and 1.5-0 K20. (SH)
AWOCIATIONs none
PAIASITOV) v. p.: maoter Tech Sci (dine) -- "Nveatigation of trannvorne forcea
,A8. 27 pp (Min HiOier r-&uc tSM,
in the movement of bridge craran". Moacow, lc
Moscow order of Tonin and ordor of IAbor RAd Bonner Hl;)ier Technical School im
w. E. Bauman), 15o copieo (xL, no 4p 1959, V5)
NIKMAYXVMIY, G.K.. kand.takhn.nauk; SN&SARXV, G.A., kand.takhn.nauk;
BALASHOV, V.P., kaud.tekhn,nauk; AXMIOV, I.P,, kand.takhn.nauk;
kand*tokhn.nauk; SPITSTMA, 1.0.. kand.takhn.mauk;
ZORIM, Z,X., insh.; VOROBKOT, G.N., Insh.; IVASHKOV, I*I., kand,
tekhn.nauk; OSIPOVA. L.A., red.isd-va; MODILI, S.I. takhnered,
Dtaign of crane mechanisms and parts of hoisting and conveying
machinery) Raschaty kranovykh makhanisuoy I detalsi podlenno-
transportAykh mashin, Isdo2s, perers I dop. Koskys, Gom.nauchno-
takhn.isd-vo mehinostrolt.lit-ryo 1959. 493 p.
(MIRA 13.-I1)
1. Koscow. Vassoyusnyy nouchno-looledovatellakly institut
pod'youno-transportoogo mashinostroyenlys.
(Crones, derricks, etc.) (Hoisting machinery)
(Conveying machinery)
BAIAStIOV, V.P.. kand.tekhn.nauk-, TYLIS, I.G.
Using single-rim running wheels for crane trolleys.
Test.mash. 40 no,9:12-14 8 160. (MIRA 1319)
(Oranes, 'Orricks,eta)
ULASHOV, V.S., red.; MATVXYEVA, A.U., takha. red.
(Metals; methods of meahwdcal and service testing)
Metally: metody mekhanichaskikh i tokhnologichookikh
ispitanii. rad.ofitsialince. Moskva, Standartgis.
1%3. 214 p. (MIRA l6s8)'
(Metals-Testing)
BALASHOVp V.S., red.; HATYRUTA, A.19., toMm.red.
(Cokel classification, specifications and methods of test-
ing) Koko; klassifikatsiia, tekhnichaskie trabovarLila I me-
tody lopyUnti. Isd. ofitsiallnoo. Moskva, Gos.isd-vo
stondartov, 1963. 135 p. (MIRA 16s10)
(Coke-Ztandards)
BAWNSHU, V.S., red.
(Fastenings. Bolts. Screws. Nuts. Itivetn] Kropezhnyo
lzdeliia. bolty. VinLy. Gaiki. Zaklepki. lzd. ofitsictll-
noo. Moskvap lzd-vo standartov, 1964. 241 p.
(MIAA 17.8)
I
b;~ ! ko;!`Iv , V' S . ) rf3d a
v -
fhefractories aM refractory yroau.-7-B] (.,~Tleufxry i ortle..
,.Itpo lzd. ofitvial,rce. Moskva, 17,d-vo
,.yWe izdellia.
atandartov, 19(4. 467 p. (MRA 1-, :7)
EELYANIN, Petr Nikolayevich, inzh.; CHERMKO, Zhan Sergeyevich,
kande tc-khn. naukj SUTUGIN, G.S., kand. tekhn. nauk,
retsenzent; BAIASHOYj__~fq,,_inzh,, red.; GRIGORASH, K.I.,
red.
(Aircraft filters and cleaners for hydraulic systems] Aviatsion-
rqe filltry i ochistiteli gidravlichaskikh sistem. Moskva$, Ma-
shinostroeniep 1964. 293 p. (MIRA 17W
tp
"Nuclear Binding Energies and Excitod States In P4 Shell,"
paper Included in the program of the All-Union Conf. on Nuclear Feactions In
Medium and Low 4nera Physics, Moscow, 19-27 I.-ov. 1957.
Moscow StateUniversity
BALMHOV) V.V., S111110KOV, Yu.1m, ~7rlx - - - - ---- --
"Application of the Second Quantleation Methods to the Nuclear Shell
'Iteory,91
paper included in the pro&Tam of the All-Union Conr. on liuclear Reactions
ft. IV.-(Mm ard lxv 1~ncra P"ica^14cow, ISI-27 Nov 1957.
Wscow State University and L-abcdev Ph-,Dies Inst. Acmd. O"cl. tUAi
)_~A , , -r_ - - _F".-. - , 7, -
F
L1'J I
DAIASHOVt V'V. , MACIFET '-*k! I C. - . p
~Mr,"C7,OV, Yu.M. 'AMIRN V !", and
I it) I Y11 - I
"14--thod of the Light BaCI&I Levels Wculatlon,"
paper submitted at the All-Union Conf. on Nue3car ReactJcno In Medium and Low
Ener&r Physics, Moscou, 19-27 110v 57.
ft)scow State Univ. and Lebedev Physics, Inst. Acao. Sci. U5319
AUTHOR ~IROKOV, JU.M., DAWOV, V.V., TUWOVI K.A. PA - 2081
TITLE On a Method of Direct Computation of the Nucleon-Nucloon AoqAction
Hamiltonian on Basis of Experimental Values for the Levels of Light
Nuclei (0 metode nopo3rodsvennogo vytiolenija gamilltoniana nuklon-
nuklonnogo vzaimodojstvija po eksperimentalInym znaaenijam urovn*j
lechkich jad*r).
PERIODICAL Zhurnal Ekaperimentallnol i Teoret. Fiziki, 1957, Vol 32, Nr 1,
pp 167-168 (U.S.S.R.)
Received 3/1957 Reviewed 4/1957
ABSTRACT The here discussed method for the inv63tigation of data concerningthe
nucleon-nucleon interaction of nuclei is based on the following con-
ditions. A)Forces in the nuclei are pair-like. B) The average velocity
of the nucleon in the nucleus has the order of magnitude of O~l c or lose.
Besides, the isotopic invarianco of the actual nuclear interaction in as-
sumed and the difference of the proton and neutron mass is neglected.
The wave function of the nucleus' of the atomic weight h is divided into
products of A self-function3 each, belonging to a frequency of the nucleon
in a threadimensional oscillator well. Into this oscillator representation
of the different nuclei only the SCHROZZINGER-equations are set up in
which not only matrix elements of nuclear interaction but also develop-
ment coefficients of wave, functions are known. The coefficients can be
eliminated by putting up the secular equations for the different levels,
In these secular equations only the matrix elements of the pair-like
nuclear interaction are unknown, because self-values of the energy are
Card 113 known from the experiment. If the development of the wave function con-
PA - 2061
On a Vothod of Direct Computation of the Rucleon-Nucleon Interaction
Hamiltonian on basis of Experimental Values for the Levels of Light Nuclei.
verges rapidly, secular equations can be cut off. The system of cut off
secular equations obtained in this way is solved with respect to these
matrix elements.
The fast convergence of the wave functions of the nucleus according to the
oscillator functions guarantees the satisfaction of the condition B. The
oscillator problem is the problem of the determination of W a roA
AxR Her* denote the average values in the given state,
r0 the basic frequency of the oscillator. Computations
for HO with U 1,2.10-13 cm lead to the value W-1. For heavier nuclei
up to oxygen analogous computations furnish the value W- 3. In the ana-
v3is or wave functions of the nuclei H3, H63, W, only the original state
3f the oscillator with n ft 0 playm an important part, in the case of
heavier nuclei up to oxygen only the first two states with n a 0 and n a 1
are important. The contribution of other states excited is insignificant.
The kinetic energy of the nucleon is computed as a whole from the complete
Hamiltonian. The Hamiltonian in the center Of Mass system is then obtained
and the self values of the Hamil nian are then the energy levels of the
nucleus. This Hamilton-operator tPis given explicitly and is discussed.
Finally, numerical results are given in the roughest approximation (n a 0).
Card 2/3
PA - 2081
On a Method of Direct Computation of the Nucleon-Nucleon Interaction
Hamiltonian on Basis of Experimental Values for the Levels of Light Nuclei.
ASSOCIATION
FRESENTED BY
SUBMITTED
AVAUABLE
Card 3/3
Moscow State University
Library of Congress
MASHM, V. V..- Manter Phyn-nith Sol (di9a) -- ".on the theory of intAmction
of shell nuoloono in light miclet". Wscowp 10. 7 pp (Mmcow State iT im
~ )qj 121~j
M. V. Imonooov), 150 copies (XL, wo 60 IT
21(8) SOV/56- 36-2-4 1 /63
AUTIPMS: Balaphov, V. V.,-Tulinov, A. F.
TITLE: On the Problem of Collective Effects in Light Nuclei (K vopr.-
su o kollektivnykh effektakh v legkikh yadrakh)
PERIODICAL: Zhurnal ekoperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, Nr 2, pp 615 - 66 (vsn)
ABSTRACT: It is interesting to discuss some general considerations
concerning the collective effects in nuclei which are not
connected with the concretization of the mechanism of
collective intensification of the electric quadrupole
transitions and, thereforet with the addition of any further
parameters. In contrast to the one particle operator, the
operator of the quadrupole transition (which in connected
with a collective motion) cont!tins only a scalar component
with respect to isotopic spin. There are therefore no
collective effects in the E2 trannitionn with exchange of the
isotopic aping and it may be assumed, that the shell theory
will give the correct values of the probabilitien of these
trannitions. The verification of this statement in especially
Card 1/2 interesting in the region of light nuclei. Within the
On the Problem of Collective Effects in Light Nuclei SOV/56-36-2-41/63
p-shell, only a small number of pure E2-transitione with
variation of the isotopic spin can be obverved. The increase
of the probability of the quadrupole trnnsitions found is
due to collective effects and such effects are actually ex-
cluded in transitions with variation of isotopic spin. Un-
fortunately experimental data are nvailable only for the
cane 16.1(Ci2). Pinally, the nuthorn nug,,;ent the following
experimental investigationn: ,) ilicasurement of the tirle 'r
for the transitions 3.58 -4 1.74 Mat and 4.77 -4 1.74 Vey in
B10. This can be carried out either according by the method 10
of the Doppler shift (for examplet in the reR(,tion C12(d,(,)B
or by measuring the relative prolvalilities of the transitions
from the states 3.56 and 4.77 MeV to the 1 .)wer states. b)
Measurement of the relative probkUiti;Fn in the mixed MliE2
transitiois, especially in the trannitfon 17.63 -42.9 MeTj
in the Beg nucleus. There are 1 table kind Q references, 2
of which are Soviet.
ASSOCIATION: Inctitut yadernoy fiziki Moskovskogo gonudtirstvennogo uni-
vercitata (Institute, of Ruclenr Physien of Morcow State Uni-
vernity)
SUBMITTED: June 27, 1958
Card 2/2
24(5)
AUTHORi Balashov, V. V. SOV/56-.36-4,25/70
TITLEs The Nuclear Forces and the Levels of Li-Isotopes
(Yadernyye oily I urovni izotopov Li)
PE,'ZIODICALt Zhurnal ekoperimentallnoy I teoreticheskoy fiziki, 1959,
Vol 36, Nr 4, pp 1123.1128 (USSR)
ABSTRACTs The present paper suggests- an improvement of the Intermediate
ooupling,model of the nuclear shell theory by taking Into
accuunt spin-orbit Interaction between the nucleons, It
is shown that by investigation of two interacting
nucleons according to the method developed by Talmi
(Ref 10) it is possible to characterize the potential
S. L S and L denote total spin
;2 12) ( 12 12
and orbital momentum of the relative motion of two
nucleons) by means of two independent parametersi by
to(, ando(2' For the P-- and D-state the follow*.rg holdst
1eP'4*'jV (1 2)1 > - 20L4 /-'D.',*IV. (1 3o(
Card 1/3 81 0 1 &1 7
ee"jV,l(1.2)j) - OL4 OYVIV 0~21) CK.?
.4 81
The Nuclear Forces and the Levels of Li-laotopea SOV/56-36-4-25/70
< V (1,2)1'> .- CA. V ( 1 2 )1 >
91 al
For the amount of the spin-orbital splittin g-up of the
interaction between the y-nucleon and the 4 shell it
holds that A (Ph.,py. 'AOY (9). The parameters 6
rA4 ci%and 6 are then.calculated for the levels of LI
and M7 (Tables 1 - It), and in diagrams E(C~j the curve
families for various cf-s-values are represented (Figs
2 - 4). Figure 5 shows a level scheme. Summaryi
Consideration of the pairwise spin-orbit interaction between
nucleons in a not filled-up shell leads to a considerable
variation of the parameters describing the central
interaction of nucleons, From calculations it follows
that a composition of central and two-particle
spin-orbital. forces gives good aFprcximation of the
I&nteraction of nucleons in the nucleus. A level analysis
of the lithium isotopes gives the following values for
Card a/3 the parameters of pairwiao nucleon interaction (in Mov)o
The Nuclear Forces and the Levels of Li-Inotopes SOY/56-36-4-25/71^
A. - i.98.-J., - 0--43. C42 a 0-23- F, - -.3,12, F 2 7,18,
F5- - 1.28, F 6 - -3-55,
The parameter values ofA (P.%,, -p-A) andcX* agree well
with the equation (9) obtained by means of oscillator
functions for s- and p-nucleons. The relation
Fl/F2 m F5/F6' which holds forc,44-0 andd-,,-O. is not
in accordance with the above parameter values, which
Indicates the existence of various radial dept-.ndunces
of nuclear forces with different exchange character.
The author finally thanks Y,i. Mv Shirokov for his constart,
interest and for his advice, and he further thanks
A. A. Samarskly and V. Ya, Golldin for their advice in,
connection with calculations, There are 5 figures. 3
tables. and 13 references. 4 of which are Sovie*
ASSOCIATIONi Institut yadernoy fiziki Moskovskogo gooudarstvennigo
universiteta (Institute for Nuclear Physics of Moscow
Card 3/3 State University)
SUBMITTEDi September il, 1958
24(5)
AUTHORs Balashov, To V. BOV/56-36-5-12/76
TITLEs Consideration of Phase Shift in the Transition
From "Particles" to "Holes" in the Theory of Nuclear Shells
(Uchet fazy funktaii pri perekhode ot "chastits" k
11dyrkam" v teorii Yadernykh obolochek)
PERIODICALa Zhurnal eksperimentallnoy i teoreticheskoy fizikit 19591
Vol 36, Nr 5, pp 1387-1392 (USSR)
ABSTRACTs In an earlier paper (Ref I)Balashov, Tumanov and Shirokov
used the method of second quantization for the purpose of
calculating the matrix elements of the single-partiole-(P)
and two-partiole-(G) operators for the general case of
mixed "particles''- and "hole"-configurations of the
nucleons, in the nucleus. In the y~ress*.paper several
further formulas are derived for the matrix elements of
the F-oper&tore for "hole"-oonfigurationa, which were not
obtained by reference 1. They are used for investigating
the connection between the parental coefficients
corresponding to the beginning and the and of a nuclear
shell. For the purpose of setting up the wave function
Card 1/3 for a nucleon state that corresponds to a filled shell,
Consideration of Phase Shift in the Transition SOV/56-36-5-12/76
From "Particles" to"Ifoles" in the Theory of Nuclear $hello
it is possible to operate with the representation of
spatial and isotopic rotation groups with J a 0 and
T w 0 and the symplectic group with (&) a (00). This
state may be considered to be a particle "vacuum", and the
nucleon state in which only one particle is lacking for
the closed shell, may be considered to be a "hole" in the
"vacuum" state. Transition from the nucleon annihilation
operator b in the state J,m,lv- to the hole-production
operator is described by b(j,m.,r) ft (-I)j4M (-1)1/t+T
C+(J,-mt-T). By making use of the results obtained from
reference 11 transition of the "particle" function to the
"hole" function, and by means of the derived matrix
elements and the parental coefficients, the shell
configurations are described, and the problem of phase
shift variation in transition from "particle" to "hole"
is inveatigated. Selection rules concerning the symplectic
group are formulated for the case of electromagnetic
nuclear transitions in the case of jj-coupling. 1n an
Card 2/3 appendix the parental coefficients for two different
Consideration of Phase Shift in the Transition SOV/56-36-5-12/76
From "Particles" to "Holes,, in the Theory of Nucleex Shells
configurations are tabulated. The author finally thanks
V. G, Neudachin for valuable discussions. There are 2
tables and 10 references, 3 of which are Soviet#
ASSOCIATIONs Institut yadernoy fiziki Moskovskogo gosudaretvennogo
universit s" (Institute of Nuclear Physics of Moscow
State University)
SUBVITTEDa September 11p 1958
Card 3/5
aAj~A-01'44' vvv. -- ---- - -
04ucloar Shell Model"
Y*port submitted for the UM Conference on Nuclear Reactions at low and
rntemediate Energiest Moscow, 21-28 July 1960e
-B&TASHOV-V--
On the %7 Isotope. Atom.energ. 9 no.1:4f" j, #60.
(Hsllulb~lsotopes) (MM 13t7)
1
8/048/61/025/002/001/016
B117/B212
AUTHORS: _3&j&&hwAr.*vw*r"*ud&chinj V. 0.9 and Smirnov, Yu. F.
TITLE-. Structure of light nuclei
PniODICLL: Izv tiya kkademii nauk SSSR. Seriya fisicheakeyat v. 25j
no. 64 j 1961, 170-188
TEM The prosent'paper was read at the 10th All-Union Conference on Nuclasr
Spectroscopy (Moscow, 1960), and also at the 11th Annual Conference on Nucle.
&r Spectroscopy (Rigap January 25 td~Fbbxuary 2, 1961)9 The authors eum-
marize the progress in the development, concerning the theory of light nuclei
and mainly deal with two aspects which underly their description of the
theory of light nuclei: 1) Utilization of a modern shell model to calculate
the characteristics of ground states and least excited stateal 2) The ques-
tion of consistency of various models of light nuclei. The first chapter
deals with the manybody aspects of the shell theory. A theoretical argu-
mentation of the shell model is not givenj the model is only treated as a
semi-*mpirioal method providing a simple explanation of experimental datag
and at the same time furnishing a means for predicting lower-excited nuclear
Cqrd 1/5
8/048j61/025/002/001/016
Structure of light nuclei B117/B212
states. The authors discuss various elementary questions concerning the
formalism of the rhell model, i.9., introducing concepts and symbols which
are generally iii;cJ in publications v.i this aubj ot but have not yet entered
the Russian The first chapter deal: wRh the following ques-
tions; Construction of wave functions belonging to the shell theory
(Refs. 2-7), application of the shell model to calculate energy spectra of
light nuclei~(Refs- 5-8)1 electromagnetic moments and transitions in light
nuclei. (Re66. 16-22). The a cond chapter dsals with the alpha association
and shell model.(Refe. 2023-MI it is shown that the alpha-particle model
of nucleus and the shell,model are much closer interrelated than has hither-
to been assumed, and that they do not exclude each other. In chapter three
~Collective motion and shell Model")# the authors mention papers (Refs. 29-
40) which deal with the creation of now and more complicated models. They
had to be developed from the collection model (drop model) and the shell
modell since the range of application of the two aforementioned models
alone is tather narrow. Finally, the authors deal with a number of experi-
mental problems. The solution of such problems has become urgent since the
theory of light nuclei develops steadily and rapidly. In order to clarify
the characteristics of nucleon interactions it isp above all, neoeseary to
Card.2/5
S104 61/025/002/001/016
Structure of light nuclei 3117YB212
perform a systematic investigation of light nuclei. This is necessary for
a precice explanation of the shell model and a dotermination of its relation
to other models. At first, such an investigation might be limited.to a
anall number of nuclei, but the results obtained should be very complete.
From a, theoretical point of view, and regdrding the present experimental PCs-
sibilitieaiothe nuclei atthe end of the p-ahell with A - 13, 14 and 15, and
also the B nuclei, up to now already thoroughly enouCh studied, are of
special interest: According to the authors, the following special pro leme,
seem to be promising: 1) Levels in.Li7i 2) calculation of levelsin Li~;
1 12 16 20
3 nature of the excited 04' levels in C , 0 , No , and other nuclei;
4~ investigations of E2-transitions near ITS when T is chLngrad; 5) experimen-
tal spectrometric roblems which are of interest for the theory of photo-
(d,p) and (d,n) reactions formirg
nuclear reactions Nef. 44); a) atrip~inf:
single-body laval.s of the final nualeusl b) inverse strippine*(p,d) reac-
tione during which the nucleon is "pulled out" from the inner'shell of the
nucleust i.e., Mg24 eta., a) elastic proton scattering on up to 8-Hev nuclei.
Ref. 45 brings an example for such experiments. 0. Lipkin, Yu. M. Shirokov,
K. A. Tumanov, V. Yu. Goncharp Ye. V. Inopin) and S. P. Tsytko are men-
tioned. There are 2 tables and 45 references% 11 Soviet-bloc.
Card 3/5
S/046/61/025/002,1001/016
Structure of light nuclei B117/B212
ASSOCIATION: Nauchno-iseledovatellskiy institut yadernoy fiziki
Mookovskogo goo. univeralteta im. M. V. Lomonosova
(scientific Research Instituto of Nuel ar Physics of Moscow
State University imeni M. V. Lomonosovl
.1. 7 0 eleare Una Pies"" ano r. r
1/2 pf, I*."p-1, N111 Vs DU 111. 111 P1431:22P.J. p1j.-st, 'is
lice 0.1 p2j2j.*IS, Aj.01 cis 0.0 P91441:11s, A.:00

L16
t.0
)0121:1631 .10
0'
- 'it,
P'1441):"pv,
Py,:112 111
Lit p'13J."P.J. it NH 1.0 p'914421:12S, p "I.: 10
Iwo 0,0 P4141:11s, P.41.:00 NU 119. 'is j0j443j-."P.,j p2/ -1/t 1/0
it, oil 0,0 1014441:1% :OD
3,0 )A14110% e.1;30
Legend to Table Is
1) Nucleuej 2) class-
ification in the IS-
schemej 3) classifi-
cation in the
scheme
Card. 4/5
Structure of light nuclei
AV, T. I 1 POAR"ACT I Pf) i l 11.2p0 7,JF i ftAll"A" 1 $41
Lit (P./.)9 Ill. Ili 3.79 3.04 pt
' Ili. Ill 2.79 2.;9
not (P-0-8 'h. 61. -t.01 -1.16 11gis (dv~ IllM, -1.91 --0.64
(P:1 1-1 3,70 3.79
" (d.1,
6 4.79 4.70
nil -3 Pj
'to
3.79
304 Al (d 1, 4.79 3.52
Cis
1/0
0.64
0:64 Im
C
(d1l
0,13
0,20
Nil 'Is -0.26 -0.26 Cl" (d.-, 1) 0.13 0.13
01? )1 '/1. '/1 1
-1,91 '
-1'91
Stu w" Ih. Ill 5,79 Me
Legend to Table 2: 0 Nucleuej 2) configurationj
3) Psingle particle
S/048
,/61/025/002/001/016
B117/B212
Card 5/5
S/056/61/041/006/039/054
B109/B102
AUTHORSo Balashov, V. V,, Shovehonko, V. G., Yudin, N. P.
TITM Giant resonance in Pb208 photodisintogration
PERIODICALs Zhurnal eksperlmentallnoy i teoreticheskoy fiziki, v. 41,
no. 6(12). ig6t, 1929-1933
TEXTt The cross section for the dipole absorption of r-quanta by Pb 208
nuclol. has been calculated by using the shell model. The application of
the diagonal approximation (taking into account only the diagonal terms
of the interaction of the particle with a "hole") to the photodisintegra-
tion of Pb206 does not bring about an essential change in comparison with
the single-partilole model of Wilkinson. In this approximation, the curve
of dipoie absork-t-ion is characterized by a wide maximum in the range of
5.5 - 8 Nov (experimental range 13.5 - 14 Nov). The energy levels J - l-
and the corresponding wave functions were calculated by diagonalizing the
interaction matrix, using the single-particle states shown in Table 1.
Th 0 pool tion of the single-particle levels was determined in agreement
Pard 1/jP I"
208 8/056/61/041/006/039/054
Giant resonance in Pb 14. B109/B102
with experimental data on the neighboring nucleus and extrapolating
calculations according to the single-particle model. Ass2pin
-interaction between the nucleons V -9 [ (I --A) + , r
12 5(r, - -2
and an interaction qmplitude of 1220 Mev. (see W. W. True. W. T.
Prinkston, J,. C. Carter. Bull. Am. Phys. Soc., 1, 243, 1960), the values
given in Table 2 and Fig. 2 will be obtained for &( - 0.135. A relevant
calculation with the Wigner force resulted in values which deviated
considerably from experimental data. It is concluded that a consideration
of the residual interaction in Pb 208 leads to an isolated "dipole state"
whose position corresponds to the experimental energy value of giant
resonance. The occurrence of this state is caused by the high density
of the single-particle dipole states in the nucleus under consideration.
It is pointed out that high density cf single-particle levels is not a
sufficient condition for the occurrence of an isolated and strongly
correlated dipole state (Brown-Bolsterli effect). It is assumed that the
6..ant -esonanoe of photodisintegration can be explained by the use of a
shell model and by taking into account the mixing of configurations. The
Card 2/Vd
208
Giant resonance in Pb as.
3/05 61/041/006/039/054
B109YB102
results of investigatione of Pb 208 are believed to be valid for any
other nuclei. Thero are 3 fifiures, 2 tables, and 7 referencesi 1 Soviet
and 6 non-Soviet. The four most recent references to English-language
publications read as followso G. Brown, M. Bolaterli. Phys. Rev. Lett.,
4.72, 19591 E. G. Fuller, E. Hayward. Intern. Conference on Nucl.
Structure, 1960, Kingston, Ontario, Canada# J. M. Soper (to be published)l
G. E. Brown, L. Cactillejo, J. A. Evans. Nucl.Phys., 22, 1, ig6i, w. w.
True, W. T. Prinkston, J. C. Carter. Bull. Am. Phys. Soc., 5, 243, 196o.
PSSOCIA;IONi Inatitut yadernoy fiziki Moskovnkogo goaudaretvennogo
universiteta (Institute of Nuclear Physics of Moscow State
University)
SUBMITTEDt July 12, 1961
Table 1. Energies of "zeroth approximation". Legende (1) single-particle
proton stat ftl (7)(7ingle-partiole neutron states.
Table 2. L:gendj itotal mb. Mov.
Card. 3/1
BJMMOV# Y.V*; MTAnfft V*B~: IRAXZHTAN, R.A.
[Calculation of tvo-mucloon correlations In the theory of
apture by light nuclei] Udhat drunutlonyth korreltateli
~
;:3orHA-sakhvsAa logtimi iadrami. Dubna, ObOoditennyl
In-t ladernykh 19:1*dovanii, 1962, 11 p, (MMA 1512)
(Nuclear re otions) (masons)
8/048j62/O26/Oi 2/002/0 16
BM/B186
AUTHOR: Balashov* V. V.
TITLE; The nature of collective di,pole excitation of atomic nuclei
PERIODICAL: Akademiya nauk SSSR. Izvestiya. Seriya fisicheakaya,
v. 26, no. 12* 1962t,i459-i469
TEXT: A survey is made of the results of cork started two years ago in
the field of dipole excitation theory at Moskovakiy univereitet-(Koecow
University) with the collaboration of N. P. Yudinj V. G. Shevchenkog R. A;
E:ramzhyant V. M. Chernov (UGU), K. V, Shitiko*a (Urallskiy politekhn. in-
(Ural Polytechnic Institute)), V. B. Belyayev.and B. N. Zakharlyev (OiYaI).
The results showed that the usual ooncepth resulting from investigationo.!of
nuclear properties suffice to present a microscopic picture of nuclear ',I
dipole excitation. Dipole excitation can be explained in terms both of
collective model and of a shell model. The dipole-dipole component in
nucleon interaction acquires particular significance when dipole states
are set up in nuolei,beqauee..Qf the shift it causes in the giant resonance
-which Is large compared to the single-particle value. The width of the
Card 1/2
S/048/62/026/012/OU2/016
The nature of collective dipole ... Bli?/B166
giant resonance depends on the"friction" occufting in dipole excitationt
There are three causes of the litter: 1) disturbed deg:n7rjo~,of the single-
particle levels (spin-orbit splitting, anharmonic pote t a a 2) all the
multipoles having residual interaction, with the exception of ~ - i,
particularly the quadrupole-quadrupole 4nteracti,,ov 3) deviation of the
dipole-dipole interaction from the ideal form (T Ir2 ) ('~l e2 The generator
method is proposed as a simple means of quantitatively describing the
characteristic features of giant resonance U. V. Balashoy, Zh. eksperiso
i toor' fiz., 42, no. 1, 275 (1962)1 K. V. Shitikova, Zh. eksperin. I toor.
fia., ;2, 868 (1962)). This method can also be used to describe other
collective excitations. This paper was presented at the 12th Annual
Conference on Nuclear Spectroscopy held in Leningrad from January 26 to
p*bruary 2, 1962. There are I figure, 3 tablesland 23 references.
ASSOCIATION: Fizicheekiy fakul'tet Mookovskogo goo. universiteta im.
M. V. Lomonosova
(Division of Physics of the Moscow,ptate University imeni
M. V. Lomonosay)
Card 2/2
S/056/62/042/001/041/048
B102/B108
AUTHORi Balashov, V. V.
TITLEs Relationship between
of dipolo excitations
the collective and shell descriptions
of atomic n%iclei
PERIODICAU Zhurnal okeperimentallnoy i tooreticheukoy fiziki, V- 42,
no. 1, 1962, 275 - 281
TEXTa The collective model of A. B. Migdal (ZhETF, 15, 81,0945) is
modified and f-eneralized by introducing shell model represeptations which
permit better description of nuclear dipole excitation and decay of dipole
states, as well as simple calculation of the position of-the giant
resonance, its width, and the total photoabsorption cross sections. Also
the various branches of photoaboorption and the character of the energy
spectra of the photoproducts. can be described. The model is based on the
experimental fact that all nuclei poetess narrow energy bands of dipole
absorption (giant resonance). The wave function of the nuclear dipole
state is T dip " (N Lyo) Tho dipole-state generating operator
Card 1/4
3/056/62/042/001/041/048
Relationship between the collective ... B102/B106
is given as the sum of proton and neutron eingle-partiole operatoral
b=2 4- e a14. cij.,.
W
/P in- 14.
ajP and aip are the proton production and annihilation operators, ain and
are the neutron single-particle states. ?dip a% IV The aA,
crre iroportional,to the single-partiole matrix elements of the electric
flpolo moment ,k' The energy of dipole excitation is obtained as
EOk I 0A + 2 E *I GA.- EOJ'Vjj' + YJ
E E.& 11'4- Y, a
)2
G-ince 7 (H E > , whore is the mean energy cr
dip 0 dip
the aipole, State, E - . The total photoabsorption cross
0 0., . 0
E 2:1(d)X12 , the corresponding expression i -n the
Car) ibi dip X
1111017
8/056/62/042/001/041/048
Relationship between the collective ... B102/'B108
2
single-particle model is a .%or E I The present molel explains
abs k ON X
the major part of the fast photoprotona in the photodisinteeration spcctm,
as reoultinG from the superposition of low sinele-particle states over the
dipole state. The width of the giant resonance in
At ~ (I IE) < W,,, I(h - E * - Ej1p)" (1) Ee) I 4'd,,>
(7d.-VI(ft-EIIIIVdip) -(E,,P)I. (15)
E. I r,,,
so that
A' 5% E'k- (El I *A Or
(16)
if V Nk, " 0. For V kN' / 0 and E ON E ok' const, A - 0. The formulas
obtained are applici to calculate E p and a abs for 0 16 , Ca.40, Pb 208 and
12. -P -
C The results are compaid with those of exact cnlculation and with
experimental data. AgrPoment is very good. V. G. Neudnehin, V. G. Shev-
C,Ard 3/4
7
3/056/62/042/031/041/00
Relationship between the collective ... D102/B108
chonko, etn(l N. P. YuAin are thanked for di3cuaslona. Thore arp 1 figure,
I tablos, tind ~) referencent 3 Z;oviet and 6 rion-ooviet. The four refer-
encen to English-lant-,ungo publications rend as followal J. P. Elliott,
B. H. Flowers. Proc. ROY. Soc- W, 57, 1957; 1). M. Brink. Nucl. Phya. ~j
215, 19571 G. Brown, 4M. Bolaterly. Phys. Rev. Lett. 3, 472, 19591
". Fuller, E. flarwttrd. Intern. Conf. on Nucl. Structure, Kingston, Canad
1960; R. Summers-Gill et al. Cnna(l. J. Phys. 319 70, 1953-
ASSOCIATIONt Inotitut yadernoy fiziki Moakovakoj;o goaudaretvennogo
univergiteta (Institute of Nuclear Phynica of Yloacow State
,niveroity)
SUB1.11TTEDt August 19, 1961
Card 4/4
ACCESSION XRt AP4024061 8/0048/84/028/002/0359/03-70-'
AUDIOR: Dalashov, V.V. IDoyarkloa, A.N.
.TITIX: Quaslelastlc scattering of fast protons by light nuclei with knock-out of
deuterons Zieport, Thirteenth Annual Conference on Nuclear Spectroscopy hold in
Xlev 25 Jan to 2 Yeb INZ7
SOURCE: AN SSSR. lavestiya. Seriya fisicheskays, v.28, no.2, 1964, 339-370
TOPIC TAGS: quastolastic proton scattering, elastic proton scattering, scattering
by light nuclei, scattering reaction, light nuclei, p shell nuclei, knock-out re-
action, nucleon cluster, deuteron yield, deuteron knock-out
ABSTRACT: in a previous study (Zhur,oksp.i toor.fin.43,117,2962; Nucl.Phys.38,629,
1962) the authors discussed the possibility of a "spectroscopic" approach (approach
basod on analysis of partial transitions) to description of the processes of quasi-
elastic scattering of fast protons by light nuclei with knock-out of on* nucleon.
It was shown, using the example of the NJ4(p,2p)Cl3 reaction, that, using shell no-
del wave functions for the ground and excited states of the nuclei, one can charao-
terize, In detail the excitation spectrum of the residual nucleus in agree-
card 1/3~
:A = SSION NR: AP4024061
:ment with experiment. Recently, X.Dietrich (Phys.Letters 2,139,1962) carried out
analogous calculations for a number of other lp shell nuclei. The present study is
an attempt to apply the same "a pact roscopL c" approach to description of reactions
:with emission of complex nucleonic clusters. The simplest of these, of course, are
deuterons. In view of the fact that the available experimental. data on knock-out 0,
'fast deuterons% In the process of quasielastic scattering are extremely scanty, the
purpose of the present calculations Is not so much to compare theory with experimat
*as to arrive at some general conclusions and inferences that may prove useful In
,planning and chocking future experiments. The consideration is restricted to lp
shel.1 nuclei and there are considered only states with a complete Is shell. The cal-
culations are carried out in the framework of the shell model, taking Into account
nucleon correlations and the requirement for commutative symmetry of the functions,
following from the Pauli principle. Thus the lightest nuclei (A n 5 to 7) are des-
cribed In the framework of the theory of supermultiplets, heavier nuclei - in the
!framework of the intermediate coupling approximation. The radial single-particle
.wave functions are assumed to be oscillator ones. All the characteristics of the
reactions are calculated In the momentum approximation In which the principal reac-!'
tion mechanism Is knock-out of a deuteron by the Incident proton. (A competing pro-'
coss, Involving knook-out with the Initial spin is mentioned, but In view of the
Catd 2/3
LAOCESS 10M_ NR.- -AP4024061-
Inck of any valid Information on the characteristics of this process and certain
other factors, it in neglected.) Folinwing derivation of the appropriate tomulas
there are comouted the deuteron distribution in momentum parameters for proton ro-
actions on Li , U7, 1)69, C12, N14 and 016,and the resultant values are compared
with what experimental date are available. In many cases the agreement in satisfac-1
tory. In general, however, the available experimental data, as noted above, are
14till too scanty for adequate comparison with theory* Son* recommendations are made;
concerning possible modifications of present experimental techniques stood at ob- I
taining results that will be more revealing from the theoretical standpoint. "The
authors are grateful to Vo.O.Noudachin and Yu.F.Sairnoy for d1scussions." Origearta;
hast 18 formulas,' 7 figures WW 3 tables.
'ASSOCIATIONi none
SOMITTEM 00 DATS ACQc OSAPrG4 RMM 00
:SUB CCON, NS NR REP SOVa 004, OWR: 008
Cafto/3
X
B/056/62/042/005/035/050
B102/B138
Au~ 211 Oaj Bmlashov, V. V-t Belyayevv Ve BegZakharlyev, B. N.
Dipole excitations of nuclei according to the suporfluld
.,.:OD1C.'.L: Zhurnal eksperimentallnoy i tooraticheakoy fiziki, v. 42,
no. ), 1962, 1365-1370
'A*Ihe nuporfluid model has proved to be one of the beat to explain
nuclear ijecaliaritiou. Now it is used to investigate the poosibilitien of
di,lolo excitationt- The dipole state of a nucleus is conBidered an a
sui;erpositio,~ of a great number of two-quaoipartiole excitations. The
energy of this otato ic virtually unchanged by taking account of nucleon
p;Arint; in comparison with the values obtained in the aingle-particle
::,00 Ol .7110130 estimates (Wilkinuon model) yield, however, far too low
valim, of the giant resonance of photoubsorption. The dipole energy can
bo raised by introduction of dipolo-dipole interaction, in addition to
the pairin&-type interaotion. It is shown that the effects of
collective intencification of dipole tranaitiona'and the presence of an
Clard 1/3
S/056/62/042/005/035/050
Dipole excitations of nuclei ... B102/B130
enerj;y chift of the dipole state with respect to the cingle-particle
valuo tire. catioed by nucleon correlations of dipole-dipolo type. Long-
rande correlations of other multipolarity contribute to the dispersion
of the (11pole excitation. The increase in dipole excitation energy is
iiroportional to the nu,;ibor of states in the last filled shell. In
.
,~reezent with the shell modol this offoot is fundainental-for heavy
ae
ro,~cloi -and uni-."Aportant for light ones. Pairing-type excitations have
only a woulk effect on the dipole excitation. It raican the energy of the
dipole state only to the extent required for a destruction of the pairs.
The contribution of pairinj; to the dispersion of the dipole excitation
2
.s of the order of c . The r9sulto indicate the direction of further
development of the shell model of the giantresonanco in deformed nuclei
(S. C;. Nilsson, B. IN. :,,ottelson, 21ucl. ?hys., 13, 281, 1959). Allowance
for :)airinj; does not elininate the main disadvantage of the model, the
Alar too loA vuluo of giant rononunoo. This can be done by considering
the non-diajonal dipolo-dipole interaction between Nilsson-type single-
particle &tatos. Results of this will be published in later.., papers.
".-'udin is thanked for discussions. There are 2 figures and I table.
Card 213
S/05 62/042/005/035/050
.-Apole excitationo of nuclei B102YB138
Inntitut ya'dernoy fiziki 11-lookovokogo gooudarstvennogo'
univerni'veta (Institute of Nuclear Physics of Moscow State
Univorsity)
December 23, 1961
Card 3/3
A U 7 1CR 6 Jalashov, V.
......................
T ~410 nriiclautic
hole excitations
6/056/6-2/0413/001/018/056
B102/2108
V., Boyarkina, .1.
scattorinr of fast ~)rototm ,nd t:~e u,)cctru:.-; of
4
in Cow , 1 nucloun
Zhurn;tl c1coporimentallnoy i tooretichcsk-oY fizzlki, v. 4~,
no. 10), 1962, 117 - 120
T*.-.'.'.'A Th,, cnlculAted the hole excitation a-pectrum fol, "-;e fast-
P r ~) to ni:. reaction 2P)CI3. T li a i r. V C at i C',,, '. i on -.;,, ~~ . - . c -,. o 'I i n d
I - - do oxist and thy they have not been
Out if tha love's 1/2 , 3/2 and 5/2 V
Aiscovered up to noy- The calculutions wore carried out on "ne basis or
the ;:model of inter;-.cdiatc coupling, takinf: account of the currelation be
twm the nucloons and usine Kurath's data for central and s~)J.n-orbi'Cal
forces (Phyo. Rov. 101 , 216 1 1956). Nzae 03 level vxc.~t%tiun .~-.,obabilitior,
"ro in the levol scheme (Fic. 1). The exci.tation curve conutruc-
t C. d .A-reament rith experimental data (Nucl. Phys. 10, 119~)6j 2-3 ve.-.v
1-100d. The lovels invostl6ated havo not yet bo,n obsurvcd in 'nC")
3qattorinC oxporiments bocauso thuir roduced width'is very a,-.all and their
61056/61/04 310011018/056
-~iulaatic ucnttc-"InL; 1002/5106
i urc fo~-b4~Ajen. Thaac levels lrxvc
a" ono
0 13 in'luced lby pickup rcaotions,
t i s:)o-l n'6cd o,,a t. t in n, any liCht nuclei such
stateu ;:Acht uxist; their stability i3
to b,~
1113 e.
alinommily
to the
- i:1
,,tabllc
forbill-
al," their --~cc:~citationc;. The're are 2 fi,-urcc. and 5 t~ibblcl~
C !.V.' US %ln.3titut yadernoy fizilU *,:os),,ovsko,o
sitcta ~Instituta of Nuoleur Physics o,. :..'oncov. JI-ate
ty)
December 23, 1~61
14
~0,?000
3/056/62/043/001/032/056
B104/B102
AUTHORSj Balashov, Ve Val Chernov, V. U.
TITLEt Effect of phonon excitations of a nucleus on the character-
istice of giant resonance in photoabsorption
PLI.IIODICALt Zhurnal):kaperimentallnoy i tooraticheakoy fiziki, v. 43,
no. 1(7 1962, 227 - 229
TEXTs The effect of surface (phonon) excitations of a nucleus on the
position and width of the collective dipole state is studied. It'is
assumed that a unique photoabsorption shell level exists and that this
level in connected with a unique single-phonon state by particle-surface
interaction. It is shown that phonon excitations are one of-the
principal causes of "friction" accompanying p-n dipole oscillations of
nuclei. From a ?b 208 nucleus it is deduced that (1) the phonon excite-
tions of the nucleus do not affect the position of the giant resonanco in
photoabsorption 1 and (2) the consideration of phonon excitations is
easenti,al for determining the width of giant resonance. These excitations
zake'A contribution to the dispersion of the dipole state in the order of
Card 1/2
S/056/62/043/001/032/056
Effect of phonon excitations... B104/BiO2
the square coupling oonstant. of the particle with the nuclear surface.
LSSOCIMILIXONt Inatitut yadernoy fitiki Moskovskogo gosudaretvennogo
universitsta (Institute of Nuclear Physics of the 11.0scow
State University)
SUBMITTEDi February 13, 1962
Card 2/2
.%!~Ti.roli6:
',:1ODIC,,,1,:
S/05 62/043/002/046/053
BIOOYBI02
Balashov, V. V., Tulinovo A* Fe
(riant resonance of spin wave excitation in atomic nuclei
Zhurnal eksperimentallnoy i tooreticheakoy fiziki, v. 43,
no. 2(8), 1962, 702-705
A-XT: In inelastic scattering of fast protons from light nuclei a
char,-.c'eristio peak similar to the giant resonance peak in photoabsorption
be"n observed. The fundamental properties of the collective spin
wave excitations cauving such resonance have boon studied. Becides, also
an optical Ziant resonance appears. The giant rosonlance of nuclear spin
wave excitation is more smeared out than the optical resonance. This
gives some insight into why the width of the inelastic scattering peak
is usually greater than the width of the photoaboorption curve. There
are 2 tables.
ASSOCIATION: Institut yadernoy fiziki MoakovGkogo goeudarstvennogo
universiteta (Institute of Nuclear Phyaico of Moscow State
Card 1/2 University)
S/056/62/043/002/0/,6/053
Giant resonance of spin wave , B108/B102
OUBI.'ITTED: March 31, 1962
r,~rd 2/2
U237
3/056/62/043/006/040/067
B183/B102
AUTHORs Balashov, V. V,
TITLEi Mechanism of inelastic scattering of e-quanta from nualsi
PERIODICALt Zhurnal skeparimentallnoy i teoret-ioheskoy fisiki, Y. Ot
no. 6(1'2)9 1962t 2199 - 2203
TUTs When beep hole states are excited by S2 absorption of r-quants,
do-exoitation occurs in several steps, i.e., moot of the g-quanta are not
elastically scattered. This is due to the shell struot ure of the nuolous.~
An analysis of the corresponding inelastic scattering of ~-quanta in the
20-Mey region show& that the nuclear shell structure can be confirmed in
this way up to very high exoit;lion energies.* for all nuclei the (rr)
re4atlon delivers two maxima o ithe effective cross section as a function
of the excitation energy. The first maximum can be explained by excita-
tion on related levels near the threshold. The second, which ooours at
about 20 Vevt has no satisfactory thoorlticil explanation at present. It
in a phenomenon of resonance in the absorption and emission of X-quanta.
According to the statistical nuclear model the second maxima# if due to
Card 1/3
S/05 62/043/006/040/067
Mechanism of inelastic soatte~ringsoe B183%102
eient resonance, should be expected at 14 - IT Meve Based on the model of
independent particle" the f9llowing can be stateds In the case of El
transitions, the- residual dipble-dipole interaction between nucleons leads
to a giant-resorenoe energy shift toward higher energies amounting to about
Is5 times the single-partiole'shift. It is assu6ed that the quadrupole-
quadrupole component of residual interaction playa &'jsimilar role not fully
clarified. Its effect in E2 absorption Is weake'r than that of the dipole-
dipole interaction in Ei absorption and of opposite sign* The single-
particle model leads automatically to the occurrence of the v2O Mey group
of excited levels in E2 absorption of t-quents. which is characterized by
anomalous stability against nucleonic decaye The radiative decay of such
states is studied here, After E2 absorption, only,some of the do-excita-*
tions of the proton to the initial level occur directly. There is much
greater probahility of Ei cascade transitions (inelastic scattering). A
certain percentage of these transitions leads to isomeric states, The
example of the 49 InI15 nucleus supplies a rough quantitative picture. Out
of 25 mb-Mey for the differential total aboorition arose section, about
19 come to inelautio scattering to the ground stator 4 to isomeric yield$
and less then 0.5 mb-Mev to elastic scattering. '.The one-partiols model ie
Card 2/3
8/056j62/043/006/040/067
Mechanism of inelastic scattering... B1831D102.
unsatisfactory as it takes no account of tunnel effects and of a number of
factors that increase the isom,erio yield. A rigorous theory of inelastic
scattering seems har4ly practicable at present. There are 3 figures and
I tables
ISSOCUTIONs Institut yadernoy fisiki Moskovskogo 4osudarstvennogo
universitets, (Institute of Nuclear Physics of the Moscov
State University)
SUBMITTEDa June 30,k 1962
Card 3/5