SCIENTIFIC ABSTRACT MANENKOV, A.A. - MANENKOV, P.V.

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SCIENTIFIC ABSTRACT
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M.ANEMKOV, A. A. MAKENKOV, A. A. - "Paramagnetic rearnance in certain cr;m-v@unds of elementa in the iron and rare-earth groups". @oscow, 1955. Acad Sci USSR, -h7sics Inst Imeni P. N. lobedev. ( Dissertatinn for the Degree of Candidate of Physicommthematical Sciences.) SO: Knizhnaya Letopi,91 No. 46, 12 fl@-.vember 1919. Moscow [@Cj F i I' -V' E- N r, U'4 F@ I fj . USSR/Physics Paramagnetic resonance FD-2366 Card 1/1 Pub. 146 - 31/34 Author Manenkov, A. A., and Prokhorov, A. M. @iws .Nwimw@ Title Fine structure of the spectrum of paramagnetic resonance of Cr34' ion in chromium corundum Periodical Zhur. eksp. i teor. fiz. 28, 762, Jun 1955 Abstract The authors investigated the spectrum of paramagnetic resonance in the solid solution A1203-Cr203 (chromium corundum) for concen- tration of chromium of 0.05%, which compound was earlier studied by S.-Kh. G. Kashayev (Dissertation, Molotov University, 1954) but without successfully explaining the observed spectrum. They in- vestigated this compound at two frequencies, 11970 and 8960 mega- cycles, and at room temperature. They note that paramagnetic resonance of chromium salts have been best studied in alums (V. Bleaney, Rep. Frogr. Phys. 16, 108, 1953). The authors observed two lines at 8960 and four lines at 11970 and in agreement with theory find that the relative intensities of the lines depend upon the angle between the axis of symmetry of the crystal and direction of the radiofrequency field. Two ref. Institution Physical Institute im. F. N. L-ebedev, Academy of Sciencea USSR Submitted February 26, 1955 AAMMOV, A. A., and PROKHOROV, A. (Moscaw) "Fine and Superfine Structure of the Paramagnetic Resonance in Bivelent Europium," a paper submitted at the International Confeeence on Physics of Keggdtic Phenomena, Sverdlovsk, 23-31 May 56. aT k I . -- I 4 - I Ii 1-12 JSSR / Radio s, Application of Radio-Physics Me' iods. ,kbs Jour : Ref Zhur - Fizika No 3, 1957, ":,,) 713'ti Abs r@ract - riftt:irai frequency -,' :;he resoDitur, -"-!F) !'ru@"Vm;t' _", W,c- ;-If,,110- rator, and Irl,"C's j@j the !,esoriant f' .-oqtieric... o' Li-e ,i" -netic I'lield. Card : 2/2 - @11 - 51-4-10/25 AUTHORS:-Manenkov, A.A., Prokhorov, A.M., Trapezaikova, Z.A. and Fox, MqVf' t4l, TITLE: Application of the paramagnetic resonance method t5y-study of the activator state in phosphors. (Primeneniye metoda paramagnitnogo rezonansa dlya issledovaniya sostoyaniya aktivatora v fosforakh.) PPERIODICALOOPtika i Spektroskopiy-',' (optics and Spectroscopy), 1957, Vol.2, No.4, pp.470-474 (U.S.S.R.) ABSTRACT: This paper was presented at the 5th Conference on Luminescence in Tartu, June, 1956. From the nature (or absence) of the paramagnetic resonance spectrum of a crystal it is possible to deduce the valency state (and changes of that valency staLe) of paramagnetic ions in crystal. This is more difficult for powders when the paramagnetic absorption lines may be very broad due to relaxation or anisotropy. These difficulties are particularly pronounced for the case of ions whose paramagnetism is due to unpaired d-electrons. Results are reported for powdered SrS:Eu, SrS:Gd and for artificial CaF2:Eu monocrystals. Measurements were carried out at 9340 Mels and at room temperature. The apparatus used is described in Radiotekhrlika i Elektronika, Vol.1, 469, 1956. Some of the present results were reported earlier Card 1/3 (A.A.Manenkov and A.M.Prokhorov, Doklady Akad. Nauk SSSH, .51-4-10/25 Application of the paramagnetic resonance method to study of the activator state in phbophors. (Coat.) 1 107: 402, 1956). In SrS:Eu and-CaF2:Eu only the Eu2* ion 1 19 1/i-state).is effective; Eu3+ i 41on-magnetic. For-Eu2+ ( S7 the.# ectroa,sPia is 7/2 and therefore 7 electron transitions are possible due to ckystal electric field splitting. In SrS:Eu only one of these transitions 1/2 war, found; the.others could not be observed due to anisotropic broadening. This one transition was split into 12 hyperfine structure (h.f.s.) components by the interactio4 of the nuclear spins of the two Eu isotopes: EulA and Eu153 with the electron Spim. The SrS:Eu paramagnetic spectrum confirms that'the europium activator is in the Eu2* state. In the'fluorite (CaF2:Eu) spectrum all 7 electron transitions, each with 12 h.f.s. com- ponents, were observed. From the h.f.s. of the paramagnetic spectra of BrS-.Eu and CaF2'Su the ratio of the magnetic moments of the Eu151 and Eu153 nuclei was found to be A .1 gl/ A153 +2.24 t 0-03 huclear magnetons. Frequency of the a sorption lines for CaF :Eu monocrystals was found to depend strongly on the crysM,orientation with respect to the applied constant Card 2/3 magnetic field. This indicates that the crystal electric-field @UBJECT: USSR/Luminescence 48-5-53/5A, AUTHORS: Manenkov A.A., Prokhorov A.M., Trapeznikova Z.A., and Fok N.V. TITLEj Application of Paramagnetic Resonance Method for Investigation of the Activator State in Phosphors (Primeneniye metoda para- magnitnogo rezonansa dlya issledovaniya sostoyaniya aktivatora v foeforakh) PERIODICAL: Izvestiya Akademii Nauk SSSR, Seriya Fizicheskaya, 1957, Vol 21, #5# p 779 (USSR) ABSTRACT: The paramagnetic resonance method was applied to determine the valence state of an activator in crystallophosphors and to detect the changes of valence during the excitation of phosphors. The paramagnetic resonance was investigated in the phosphors SrS-Eu; CaF 2-Eul SrS-Gd and SrS-Tb at the room temperature by means o a superheterodyne radioapectroscope. It wag estab- lished that Eu in phosphors is in bivalent state (&V+), and Gd and Tb are in the trivalent states (Gd3+ and Tb3*'). The ratio of nuclear magnetic momenta of Eu 151 and Eu153 Card 1/2 nuclei was determined to be 2.24 1 0.03 by observing the 48-5-53/56 TITLEs Application of Param W etic Resonance Method for Investigation of the Activator State in Phosphors (Prizeneniye metoda para- magnitnogo rezonansa dlya issledovaniya sostoyaniya aktivatora v foaforakh) superfine structure of Eu 2+ and gd3+ ape a, The values of nuclear magnetic momenta of Gdl5D and GdM were estimated to be approximately equal to 0.2 of nuclear magnetons. One Russian reference is cited. INSTITUTION: Physical Institute im.Lebedev of the USSR Academy of Sciences. PRESENTED BY: SUBMITTED: No date indicated AVAILABLEi At the Library of Congress. Card 2/2 'AUTHORS: Manenkov, A. A., Prokhorov, A. 14. 56-5-5/46 TITLE: A Determination of the Nuclear Moments of Gd155 and Gd157 From the Hyperfine Structure of Paramagnetic Resonance (Opredeleniye yadern.vkh momentov Gd155 1 Gd157 iz svorkhtonkoy struktury par&- magnitnogo, rezonansa) PERIODICALt Zhurnal Eksperimentallnoy i Teoreticheskoy Fiziki, 1957 Vol. 33, Vr 5, PP. 1116-1118 (USSR) ABSTRACT: The gadolinium spectrum was recorded by means of a superhetero- dyne radiospectroscapa at 9383 MHz. The magnetic field was mea- sured by means of the proton resonance. A SrS-Gd preparation was used for measuring the paramagndtic resonance, in which case Gd155 or Gd157 respectively, were found accumulated in enriched state (-93%) in the test pieces. The following results were obtained: I - 3/2 for Gd153 and Gd157 J@(Gd155)j : j/)A(Gd157) I = 0,73 + o,o3 From a comparison of the decomposition uf the hyperfine structure of SrS - Gd3+ and SrS - EU2+ results: Card 1/2 1@,(Ju_151)I - J@C(Gd157)1 - lo,6. + -,-3 A Determination of the Nuclear Moments of Gd'55 and Gd157 From 56-5-5/,46 the Hyperfine Structure of Paramagnetic Resonance. Let @t be assumed that 316 is the (theoretical value) of /j@Eu 51), it hence results from the ratio measured: l,k(Gdl55)1 o,25 atomic magnetons J@.(Gdl57)1 604 atomic magnatons There are 1 table, I fi&ure, and 11 references, 3 of which are Slavic. ASSOCIATION: Physics Institute imeni P. N. Ltbedev of AN USSR (Fizicheskiy institut im. P. N. Lebedeva AkaGemii nauk SSSR) SUBMITTED: M&,Y 11, 1957 AVAILABLEi Librarj of Congress Card 2/2 . - zJZrAlp c7V7ET9 OL.NTHE NUCLEAR BPI, NO SIA -MUROMP-THE @;Z-YEAIC RADIOACTUE. IS OTOPE I-TuE.5, -12 fri*hafd@t Aka spWttr f. T@a mmlear w. Itz 2.03 nultlear wg ot parr-@ tud es t. thc@-Or4@ dtfst- ta by cout nlnjil@ Year x., taral-minare- Eu .2@ irra Thf-4 lrr,,d Man producc-3 dated by iC4@p@ @eqtjvo lp rom Kit m for cousidersh-re y"Diud-radlo &Lie Fit- T@ wl.- nkITENKOV, A. M. (FLU, MOSCOW) "Molecular Amplifiers and Generators". report presented at the All-Union Conference on Statistical Radio Physics, GorIkiy, 13-18 October 1958. (Izv. vyssh uchev zaved-Radiotekh., vol.,.2, No. 1, pp 121-127) CONPMTE card under SIFOROV, V. I.) SOV/56-34-6-50/51 AUTHORS: Zverev, G. 11J., Korniyenko, L. S., Manenkov, I.. k., Prokhorov, A. M. TITLE: A Paramagnetic Amplifier and Generator on the Basis of Chromic Corundum (Paramagnitnyy usilitell i generator na khromovom korunda) PERIODICAL: Zhurnal ek3perimentallnoy i teoreticheskoy fiziki, 1958, Vol. 34, Nr 6, pp. 166o-i66i (USSR) AB@,TRACT: The spectrum of Cr3+ in corun um was investigated in previous papers (Refs 6-9). The ion Crg+ ' within the corundum is placed in an axial electromagnetic field which splits up the spin quadruplet of the lower singlet orbital level into 2 dublets with the distance 2D - - 0,3824 cm-1 between them. For the construction of the paramagnetic amplifier the authors use the levels which (in the case that the crystal axis is orient- a.ted parallelly to the external constant paramagnetic field) are characterized by the quantum numbers M - 3/2, + 1/2. If the crystal axis is turned the states are intermi)@e_d and the Card 1/2 transitions between all 3 levels are allowed. The levels SOV/56-34-6-50/51 A Paramagnetic Amplifier and Generator on the Bats of Chromic Corundum M = - 1/2, 1/2 are used for the amplification and the auxil- iary radiations excitate the transitions between the levels 11 = 1/2, -3/2. The frequency at which the amplification (or the generation) is carried out is equal to -3000 mega- cycles and the frequency of the Suxiliary radiation was equal to - 15000 megacycles. At T - 2 K the system was excitated by itself and changed over to the function of a generator. The exact data concerning this amplifier will be published later. The authors thank A. I. Shallnikov for his help in carrying out the experiments at low lemperatures. There are- I figure and 10 references, 6 of which are Soviet. ASSOCIATION: Fizicheskiy institut im. P.N. Lebedeva Akademii nauk SSSR (Physics Institute imeni P.N. LebedevAS USSR) SUBMITTED: April 1, 1958 Card 2/2 5'(4 AUTHORS: Rode, T. V., Manenkov, k. A. SOV/76-33-2-43/45 TITLEs Letters to the Editor (Pistma v redaktsiyu). 0 *n the Problem of the Valence State of Chromium Ions in Compounds Formed in the Thermal Decomposition of Chromic Anhydride (K voprosu o valentnom sostoyanii ionov chroma v soyedineniyakh, obrazuyushchikhsya pri termicheskom razlozhenii khromovogo angidrida) PERIODICAL: Zhurnal fizicheskoy khimii, 1959, Vol 33, Nr 2, P 503 (USSR) ABSTRACT: It has previously been found (Ref 1) that in the thermal three chemical compounds form, and at a decomposition of CrO 3 pressure of 250 atm CrO -s formed in addition. Chemical 2 analyses showed that these three compounds are the decachromate, dichromate, an,'. monochromate of chromium. Since it was possible that because of a disproport-Jonation of the chromium "wet" analyses had yielded incorrect results on the valence states investigations using the method of electronic paramagnetic resonance were carried out here. The measurements were taken Card 1/2 at a frequency of 9375 megacycles. In CrO 3 no electronic Letters to the Editor. on the Problem of the SOV/116-33-2-43/45 Valence State of Chromium Ions in Compounds Formed in the Thermal Decomposition of Chromic Anhydride paramagnetic resonance was observed, while decachromate and dichromate showed absorption lines corresponding to a g-factor - 1.9 and a width of about 100 gauss, which was attributed to paramagnetic resonance of the trivalent chromilm ion with an electron transfer M = 1/21@ kT .If ha2l\@, kT, n n A exp/c, t)+(n n with T =_1/aj@@, 1/W W is the probabilit 5- 2 = A @ 1 3- 2)eq 1 31' ik Y of a transition E i-,@E.. In this case the temperature dependence of the relaxation time is very .,ieak and at hi) 3@ kT it vanishes. (b) E 3- E2@@ kT, '&-T. For hL., ",/', kT, f .or the 21-1 transition n _n @ Aexp(a t)+(n - n 32 2 1 1 2 @re =_1/aj:-t1/W 251 i. e. the temperature-dependence is strong (exponential). :',id-resuits indicate that the temperature dependence of the spin-lattice relaxation time depends on the relation between level splitting and kT. .63cc TION Fizicheskiy institut im. P. N. Lebedeva Akademii nauk SSSR (Physics Institute imeni P. N. Lebedev of the Academy of Sciences USSR) SUBIdITTED: December 26, 1961 Card 2/2 6/053/'62/077/001/001/003 B-117/B112 @.'J'THORS: Zverev, G. M., Karlov, N. V., Korniyenko, L. S., Manenkov, A. A. , Prokhorov, A. IM. T I!, Application of paramagnetic crystals in quantum electronics lzli!ODI'AL: Uspekhi fizicneskikh nauk, v. 77, no. 1, ,962, 61 - ioa yn : I @:estern and Soviet studies during the period 1952 - 19062 concerning @he -,roCress in th@ application of paraua@net4 @c crystals for building C''U.-nium devices are reviewed. In these devices, which are used in the fields of radio and optics, negative temperatures are produced by auxiliary radiation. The following problems are discussed- energy levels of paramagnetic ions in crystals; relaxation phenomena in paramaanetic crysTals; (paramagnetic) quantum amplifiers of the radio range (para- magnetic resonance amplifier :;7,lj (Iq@U), paramagnetic progressive wave amplifier (PUBV)); quantum generators and amplifiers of the optical range (optical quantum generators with ruby and fluorite, quantum ampli- fiers, (@ui_,ntum counters). Finally, the great progress achieved in quantum electronics during the short time of its existence is pointed out& "ard 1/2 1 3/053/0'2/077/001/001/003 Application of paramagnetic... B117/3112 estaolisnment of highly accurate frequency stanr@ rds 'or various purpose3; -a ,eve--oiment cf love-noise paramagnetic amplifJers of the radio range and of optical 6anerators havin- a 'h_J,3h degree of coherence and hi6h spectral radiation density. The quick progress of quantum electronics and Zts nro- zisinJ prospects,are the consequence of its development on the 3a sis 0f already existing. technolo.zy. Progress was first achievea-in the radio range, ana later in the optical range. At present work is in progress in developing the entire range, including the submillimeter- and distant infrared range. There are.27 figures and 134 references: 45 Soviet-bloc and 99 non-Soviet-bloc. The four most important English-language refer- ences are: J. R. Singer and S. -11'ang, Second international Conference on a n. Lum, Electronics, Berkeley, 1961; W. G. Wagner and G. Birnbaum, Second 7ntcrnational Conference on @uantuz Electronics, Berkeley, 1961; H. Hell-aarth, Phys. Rev. Lett., v. 6. 19 (19061)i A. L. Schavilow, G. Devlin, Phys, Rev, Lott*,, v. 6, 96 (1961). Card 2/2 5/18 63/005/001/036/064 B I 08YB 180 AUTHORSt Lushchikov, V. I., Manenkov, A. A., and Taran, Yu. V. TITLEi Dynamic polarization of protons in lanthanum-magneBium binary nitrate PERIODICALt Fizika tverdogo tela, v. 5, no. 1, 1963, 235 - 236 TEXT: Earlier work on the dynakc polarizdtion of protons (FTT, 5, 5503, I.961) is continued he're. (La,Ce)2Mg,(NO,)12-24H20 single crystals were gycrwn from a saturated La (NO solution with an appropriate addition 2Mg3 3)12 of Ce2Mg3 (NO 3),2, The sample was placed in a resonator so that the hexa- gonal crystal axis was always perpendicular to 5Ho the external maenetic field. In this position, g., - 1-83 for the Ce + ion. The increase in the polarization of the protons in the crystal on saturation of the epr was det@.rmined from the Jncreased amplitude of the nmr signal from the proton. With fixed epr frequency typical polarization peaks were observed at H + AH, which corresponds to the forbidden transition at the frequency 0 2 Card 1/2 S/18 63/005/001/036/064 Dynamic polarization of... B108YB180 Vexc nucl* The greatest increase in polarization was found at 1.60K in a field of 3700 oe for a crystal with 0-5@4 Ce, In this case, the proton polarization was 170 times greater than in thermal equilibrium. This de- creases somewhat when the temperature falls to 1-50K. MeacurementB of the coefficient of dynamical increase in polarization in dependence on the power of epr saturation showed good agreement with the simple phenomenological theory of spin diffusion (0. S. Leifson, C. D. Jeffries. Bull. Am. Phys. Soc., 6, no- 3, 1960; Phys. Rev., 122, 1781, 1961). The same ap3lies to the nuclear spin-lattice relaxation time in dependence on the Ce I concen- tration in the range 0.2 - 1@@ (at constant temperatures between 1.5 and 4 1.70K). Between 1.5 and 1.70K, the relaxation time is proportional T_ at any Ce3* concentration. There are 3 figures.and 1 table. ASSOCIATIONi Fizicheskiy institut im. P. N. Lebedeva AN SSSR, Moskva (Physics Institute imeni P. N. Lebedev AS USSR, Moscow) SUBMITTED t August 6, 1962 Card 2/2 S/181/63/005/002/009/051 B104/B186 AUTHORSs Kessenikh, A. V.# Lushchikov, V. I., Manenkovj and Taranp Yua V. TITLE. Proton polarization in irradiated polythene PERIODICKM Fizika tverdogo tela, v. 5# no* 2t 19639 443 - 454 TEXT: The aim is to find materials suitable for polarized proton targets, and to investigate the physical properties of irradiated polythens. To this end the studies-of dynamic polarization in high-density polythene irradiated with fast protons (V. I. Lushohikov, A. A. Manenkov, Yu. V. Taraiat --FFT, 3o 35039 1961) were continued. The dynamic nuclear polarization wail measured at 77, 4.2 and 1.60X in a magnetic field OfAJ3400 06 using a device desoribed in a previous paper. The 1799-6 mm test pieces were placed. in the coil of an autodyne n.m.r pickup, with the axis of the coil per- pendicular to the long side of the resonator. H102 oscillations with a frequepcy of 9440 Ho/s were set up in the resonator. The dynamic polarize- ijon factor of the protons was determined from the amplification factor of the n.m.r. signal at saturated e.p.rof the free radicals formed when the Card 1/3 S/m 63/005/002/009/051 Proton polarization in... B104YB186 polythene was irradiated. Resultat In the He temperature range, the oross- relaxation under conditions of non-uniform e.p.r. line broadening plays an important part in the dynamic polarization of the nuclei. This can be used to explain the increase i-n the broadening of the dynamic nuclear polariza- tion maxima as the temperature decreases, and the fact that the dynamic polarization factor does not depend on temperature. The time dependence of the n.m.r. lines is described as the sum of two exponents with relaxation times of T 1 and T.. The nuclear relaxation depends lineaily on T 1 and T 21 this result being contrary to theoretical predictions (0. S. Leifoon, C. D. Jeffries, Phys. Rev.f 122, 1781, 1961). it io explained on the assumption that the action zone of the paramagnetic centers is equalized at the expense of fast spin diffusion. The dyncmio polarization coefficient diapends linearly on the molecular weight of the initial material. There are 6 figures. ASSOCIATIONs Fizicheskiy institut im. P. N. Lebedeva AN SSSEk (Pbjaioo Institute imeni P. N. Lebedev AS USSR)j Nauohno-issledovatel'sMy fiziko-k4,Wheakiy institut im. L. Ya. Karpova, Moalcva- (Boientiflo,.Fhysiooohemical Research Institute imeni Card 2/3 L. Ya. KarWv, Moscow) 8/181/63/005/002/009/051 Proton polarization in,.* B104/BI86 SUBMITTE.Dt August 69 1962 1 I j Card 3/3 i@n i i6 6-ti i@ if ,e.@p Oe@brogd: f ng -d" lex nal. raI 3 uriLt-I p b cc xati ant 26- e-n re uiiiitidte 4f@'Ithi &-d" atib@ ga_ 4/i imuia @-cond no or. - ----- ---- -00 Q94 S. nam 96' Do a am-, nud ry.t@Mas U'- nA" to;" G-"; Etsir-@--:A 22 7811 T. 1@6 io i RITUS, A.I.; MANENKOV, A.A. Splitting of the paramagnetic resonance lines of' Cr3+ ions in ruby in an external electric field. Fiz. tver. t!li 5 no.12:11590-3593 D 163. (MIRA 17:2) 1. Fizichaskiy institut imeni P.N,Lebedava AN SSSR, ?4oskva. 4- -@ , - " - ' ".-! .-.-..-I MANENKOV, A.A.; POLISKIY, Yu.Ye. Relaxation processes in paramagnetic resonance of Gd 3* ions in CaF crystals. Zhur, ekBp. i teor. fiz. 45 no.5:1425- 1-429 & 163. (MIRA 17:1) 1. Fizicheskiy institut imeni P.N. Lebedev@L AN SSSR. ACCESSION' YR: AP4019845 S/0181/64/006/003/0827/0830 AUTHORIS: Kessenikh, A. V.; 14anenkov) i. A.;_Tyatnitskiy, 0, 1, TITILE: Discussion of experimental data on dynamic polarization of protons in irradiated polyethylenes SOURLE: Fizika tverdogo tela, v, 6. no. 3, 1964, 827-830 TOPIC TAGS: polarization,@polyethylene, ultra high frequency irradiation, ma,@netic resonance magnetic property AASTFUCT: The authors have investigated samples of polyethylene of high density., conn,aini,ng 1016 - 1019 cm-3 polyene radicals: CH2-(CH)a,_,-CH2, where 1-1 >2* Studies were made at 77, 4.2, and 1.6K. The frequency of the ultra-high-frequency generator was kept constant, but the magnetic field was varied., and the intensity of the nuclear magnetic resonance signal was measured in its relation to the magnetic field. It was assumed that the relations between the probabilities of different spin transitions, during iatra-high-frequency irradiation of paramagnetic centers with irremlarly ekpaaded electron paranagnetia Card 1/2 ACG-;'SS701%1 NR: APLO198L5 resonance lines, are determined by the relations among rates of establishing equilj:brium within the spin system and equilibriwii of spin with the lattice. The dynamic polarization of protons was found.to decline very ra@pidly (negative values) Q with increase in magnetic field, reach a minimum, then increase very rapidly tpassing tilirough zero) with further increase in field, reach a maxim.La, and then decline again. Theoretical values were found to correspond closely. to experimental values in values of mtgnetic field where tihe minimum and maximums @occur, but the theoretical values of,the minimum and maximum, proved to be numerically greater than the ez/.2eririental values. The authors point. out that it is possible to compute, within the framework of the model they employ, the effect of combination spin transition saturation ca electron polarization, which cannot generally be neglected in calculations. Orig. art. has: 2 figures and 3 formilas, ASSCICLkTION: FiziIko-Ir:himichesIdy institut im. L. Ya. Karpova, Moscow (Physico- chemical ::nr,-zitWve) SUBI@=ILD: 02SeP63 DATE ACQ: 3314ar64 EXL: 00 SU3 GODEE: SS, EG NO RL? SOV: 004 OTHER: 003 Card 2/2 AM @,MT3 -13ftd 3 MED -'ZUG 00 Lf, _aM CODE NO R& - ()TIM]a i-00 8 CaM 1-1 KARLOV, I.V.; MAKENKOV, A.A. Quantum paramagnetic amplifiers; review. Izv. vys. ucheb. zav.; radiofiz. 7 no.1:5-45 164. (MIRA 17:3) 1. Fizicheskiy institut imeni Lebedeva AN SSSR. L 11949s.% -,.ACC NRi AI?6M. 737 -'the;,trans tibi fiel4' at- -the rr Mve sh --of equeiM. v, on,, 'irv;ea.A.r6"sJL ex on '-thatz hie:@xelAjt&t ugir- _p@!Pu. gqted doncent, of a-A-turat n' Pul I_'g. _ses@ - - a conf rins o@@, ppen& tru '6_@:are, Ao-v rc *Ahkt- ther 64 elaxa 01' dt CPzTe The i qpq@ O'sjin@]Attt6i, iel i@mtlon trans t 2-vas Auv6stlgiektd&@"' :-frequ'e'ncy,@-v_,-'i of tb or parallel entation e litivi external Amagneii .6'_-z field be), me he.@ ao 3+ br@c ertain Cr corl- ti 't f fr r. oncium 1-pbsei 'me.- eldxa ea- eveda: a eqiqeiqcy 'Ot t Ana! -40,@b' h i *@,, ibe-- eIAjAt! ons.- These vd- pro@.:: porroppouqi sp n7 "Cross@ r t epara, lhg-@ th Oe4@qndence'-.of he'-ftrm' of, - --relaxation'*.@' the e-,durat: ib@d2@'df@@tbe ' tea-*rature 6iikv6s':on -- th* i6h - of- the- sati@iatW Abes - reatig4_ PI 1A A' 6'r4",' h t @ _@4 @@ Tit rival-T .4i, i- 0 .2K at:all n- V ,a Om, es'-whatever- e.ve a n. at large Con@ _t id: itiln@.lat k' em _tI 't V_Ii,@6Oiaiid,6d` t @f dene'd - tM e .-.cen'. ra iom-@ + - fko@6" ect pib66"dso fe .-..ex arige@ -etween't e -sy f nergy, sp n._ stem -tii*e,---,-c-on-:ceiitriti~ii-~iii*,d-'ni tlie ri3imatio n ter of dence of rate indicates -Abit--'thii@ke-': are, _tw,6:@ dif , erent- -effect nt n iecfia-'. i eractio 7p on0h if ti _p q :coiq@e ra qn@ responsible.-+, NatPo*: At, low: .66nceutiAidni - (