SCIENTIFIC ABSTRACT SMIRNOV, A.A. - SMIRNOV, A.A.

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SCIENTIFIC ABSTRACT
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A. A..,--BTjJTYLAiIK0, A. K. , DANM 'MKO, V. M. ?,',ILNAN, YU. V. , NAYDIC-H, YU. V. AIM-, BYBAK, S. A. Theoz7 of Electric Resistance of Alloys in Prof-rossim- Order Izv. Kivevsk,_poj~tel~hn- in-ta, 192, 1953, pp 18-24 'F"xperimental curves, expressing ratio of electric resistance of alloys in Pro-ressinq ol,der to compound and distant order, differ from theoretical ones b-y presence of rectilinear sections, sharp ma-Kinums and uneven variations. These peculiarities are theoretieplly explained in examples of alloys -,.ith cubic latticed. The axticle confirms A. A. Smirnov's theory Zhur Elks i Theor ZI& 17, 743 (1947) of veculiarities observed in PIloys in proCressin-a order. (RZhFiti, No 5, 1955) 9- Sen 55 SO: Surn No. 630., U:S 8 R 7 en. PIL. 2J.. or the ' us pubstitritional; i diffusion of tuarked atoms "I ni tmary, body-celitered cul ticy Lnech- nuism was ns5umvl,~Sn .:b Interactions d were considerpdi~ eq l 6 Wid soln.,-thcn th press^1 F fil to Rom to a ne-7h. tile pot ~:Al tj.~& Ajarzjer~j - to -awaItittawn oreortca., and bo, ing Oiffu~ 'M wa!f V L tion of the. final'),Ah(i ion' 6i~ ar a ?.Wideritd, and In ds4 activatioii~,,Cnoky-witb winpii~ or m&.W would be cube of,.jAjfj# illoy jim. actiikila~ -d to;~~!%~.tbrougli a rivix. it the alloy tendc4 to ord,~, d -deccanp. into -if tuid thiouik a saiii tile- alloy tell cd to j 1 A G. G.I PIMSeS r z' 777-7', 7 7~ 1) h S~R-qf 53 9.217 Muslim of extrallem Th f th I eory o e A RM lite prvcev;,,.of,,btdtdo9. 1. alloys ~KRtvoGEAz-lANt)lA A. S~mtlttvov. ~zk ASXF vr_ 24 NO, 4 41YJ ' prQblcm... thc~ diffusion of atorris I Diswsks: t~~ inkiled into thle fniersikes of lbe bodymc6tred crysla , )ys, e.j.. Aras~ dWng l1w ordcr~ ja(tk4t~ OfIl.11tlry OK , rations of thc all )y p"ime con"go ini proccss AI. ounding tW diffusi or_lN_- moms-_~urt ng.atows, ' trarmus cienimi are:talcefi into considcridoft.-. A .: dcri~;Ltion i3, prLsented 'of- theoretical dependence ofthe cocffickar cfdiffukiaii on remperaturt; and con-, t dowfor both tho ordered and disordcrcd tit, c ra of tile MIO. liv -- -- --- ---- - 6740 THEORY OF THF IDIFiJISION OF EXTHMEOUS ATOMS, - IN ALLOWDURIAG TH4 PROCESS 60.011DERING. ll.: Zhur.- Ekaptl'I M. A. Krivoglaz a4 Bra Mov, ' 1"- fcL F1z. 24 No,~ ea (in Russian)- The problem of the diffusion of items (nee rted-Into the Interstices of a face centered crystAl Intilco.of binary. - -o' alloys, e.g-AuCup during the disorder rder tr- altion 13 an ..;Jlsquss~ed. The ternkraturei andcowntrallon dependence. of the coefficient of diffusion I-4 jn4cattgated (o th U16 r be efreot of the ordered and disordered state of the alloy. lie- n:on the~co~fflctpnt or diffusion is disdrder-order ti-ittO -or for the face-centirid than for the body be greO found to , t centered alloy, lattices. (Science Abstrac 13) 1. Vi-MTOVI A. A, 2. USSR (600) 4. Alloys 7. Oxidation of alloys. Zhur. fiz. khim. 27, no. 1, 1953. 9. Month!X List of Russian Accessions, Library of Congress, Hay 1953. Unclassift -ed. SMIRNOV, A.A. Iffect of vacancies In crystal lattice units on electric resistance of an alloy. Dop. AN URSR no.4:250-2.55 '54, (MIRL 8:4) 1. Chlon-korrespondent Akademii nauk USSR. 2. Kiivafkiv politakh- nichniy institut. (Metallography) (Electric resistance) /-I- 7~ Ov USSR ,"Elf ect~i interstitial atoms an the self-Musion of a metal. M. A. Krivoglaz and A. A.' SmImov. DuAlady .4 kzd. Mauk S.S.S.R- 90, dependence of self-difruiiou of -f-Fe on C content is explained theoretically. 'The equil. no. of vacaucies with 0 1; 2 3 '4~ 5, and 6 jjelghborine latenititia) atonis Ivas ~alcd.'by a statistical method. Art expression for the diffusion coeff. D ofinarked matrix ittonia was then obtained in terms of the setf-dif- filsion coeff. Dj in pure tuatrix rn~tal A,~the conca. c of the IntcvititiA atom C, the interaction cnergy V of alorns A :and C at M diaEance ag/2, and the difference of interaction erjergi,~ !i for distances (Ar,9141)oo and ri,/2, where a. is the; latrice- cim5l. D. - DiIII(I - c))Il + 44HAV - 1)A4 (I -L -01AT 1 011. ~ Thim, D did not vary expant' tizally -~% ith I/ T. HowLvtr, approx., the rbiervtd. expt], valut~l Qf activatian energy and fiequeucy fath)r were ob-'. tained for B - OAS c.v, R - 6 o, ane. c - 2 to 5 at. The fR-quency factor decrea:,&d by a factor of 100 with iocrc-4se in c from 0 to ".5 at. A. C~.Guy J, It-i We* at *4 nod" V , Ra, A. A , - i i 87 4 di a m s; Absm ~~ tifi.-Z77j4 cffcaO hatef the 6*7. re a cf. C.A.'49,131 elm. reghtgri y With cub(c,aysw littice stiaic, li itin oelm. this rcs46uicle, WCS dft cOn-cnd as tkto-s of addat , COzKt, i , Tho mutlom tho Obtalaw OffLow, golumce Off r4ticuil. - , G( tho atmi to tu A94Y showl Chat 14 - oforder tho addid. MWAIACC biUW not ha voi: at Amf COUCO', swd lo #Wyo 6vable.of dJ4*t&,r suchi tar. - r _~M 0_0 th~ h06 -d=mse~ tbo' 0 &;e a., - - t _ , ta Tedd It iYoul4le -=b _~e mi".11fe tjf &=A Ulcawpu M effea Is r4ost.pmbable. If eA iff ljij t n d r 6w f b W d es Cs t cc ere . e o oL bec=i or App g or d ,~ of temo. il~ eke _0 USSR/Physics Diffusion in alloys FD-1072 Card 1/1 Pub. 153 - 8/24 Author : Smirnov, A. A. Title : Diffusion into penetrated alloys Periodical : Zhur. tekh. fiz., 24, No 10, 18o2-1811, Oct 1954 Abstract : The author calculates the diffusion coefficient of atoms penetrating into intermediate nodes of the body-centered cubic lattice of a binary alloy which may be in the ordered state. Institution : - Submitted May 3, 1952 SMIRhOV, A. A., KRIVOGLAZ, M. A. "The Effect of Admixtures of Implanted Atoms on Alloy Dissociation" an article in the book "Questions of the Physics of Metals and Metal Science", AS Ukr. SSR Kiev, 1955, 151 PP- So: Sum. No. 1102, 19 Oct 56 USSR/Physical Chemistry. Thermodynamics, Thermochemistry, B-08 Equilibria, Physical-Chemical Analysis, Phase Transitions. Abs Jour: Ref Zhur-Khimiya, No 5, 1957, 14683 Author M. A. Krivoglaz. A. A. Smirnov Inst Title On the Theory of Disintegration of Alloys Accompanied by A Separation of Chemical Compound. Orig Pub: Fiz. metallov i metallovedeniye, 1955, 1, No 2, 311-1-315 Abstract: The paper contains the thermodynamic computation of the general case of disintagration of an alloy of two metals, 4n the crystal lattice of which atoms of a third element have been introduced; thia diaintergration consists in the formation of a chemical compound of this third ele- ment T,,jith the metals and a solid solution of an altered composition. The computation of the first phase repre- ~sentin_- the so!--;d solution is carried out statistical.Ly i-.aking into consideration only the configuration part cf the free energy. It is assumed that the disintegrating Card 1/2 emistry, B-8 USSR/Physical Chemistry. Thermodynamics, Thermoch Phase Transitions. Equilibria, Physical-Chemical Analysis, Abs jour: Ref Zhur-Yhimiya, No 5, 1957, 14683. b Abstract: alloy has a face-centered cubic lattice and that t-e interaction energy of atoms does not, depend on the temper- ature and composition of the alloy. Card 2/2 -1 , 1) All) /' Ii - A) mecra foreign Wing cm thb r .11,y-. Al. A. Kriwaglaz and A. A. Saiknov- all 1955, No. 6, loi-l Tcc~ of sul, qllcutitle- Cf .1 3rd- elment; C ca tjj of an A~-Y N-li thc demnun., phzv~irof IvIlIc"i ritai~l the lat- eubic) ei-thc, ;Hoy alld IvIlt-11 ng 71 .1m -io;tot Ownlically 1; ii imalvzol bv ow, raluced byzilum'.- The divory It--tds to the conclL,'oa t t sniall quantitic, (it C E when th-~ AE ;Cotlca. of ~c appro=C4 em I'l rL t ' A -fiv tim ur 0 obtained, (vibm x; 7 ~tid x, , the coomi. 2 ~phases), Le. fcr the dt Una Z, cmiapa. curvc is rdfL-cti to the line- 711;-3 is ill ~agik-blcnt With the~mlition derived- by W76 ~)w!Ehoat. am =u~cm- 'USSR/Physics Diffusion in metals 10ard 1/2 Pub. 118 - 4/8 Authors I Krivoglas, M. A., and Smirnov, A. A. Title A theory of atomic diffusion inalloys Periodical t Uep. fiz. nauk 5513, 391-442, Mar 1955 Abstract I An explanation of the diffusion.plienomena is prIesented. Two theoriM 0ut, of three mentioned) on the atomic diffusion are discusse& One theory explains the diffusion phenomena as the atom movements along the lattice intzr-sites. The theory considers two types of cubical structure crystal 8: 1. f the -brass crystals with regularly and irregularly arranged atoms; Institution: 'Submitted 0 I . . ;author Srdrnov A A Stoyrnov, LA. Inst Eev iolytc nic In'stitute, USSR Title Influence of Injected Atous on the Ordpring of the Llloy Orig Yub Fiz. metallov i iret,~11ovedcniye, 1956, 2, 11Jo 3, 524-55o Lbstrv.ct The influence of edmixturo of injected atoms on the ordering of on alloy, having a volime-centered cubic lattice, was in- vestizated periodicelly. It vas shovm that the presence of an admixture of injected atons increases the degree of order- ina of the alloy anJ increases the ordering temperature. The possibility of ordering the disordered alloy by injecting admixture ntous into the interstices of its crystalline lattice is clarified. The distribution of the injected Ptcm-s of the adinixture over tho interstices of E different kind in the ordering of the c1loy is investigeted. Card 1/1 A4 i k /V 0 V'/ USSR/Electricity - C;nductors G-4 Abs Jour : Ref Zhur - Fizika, No 1, 1958, 1390 Author : Krivoglaz, M.A., Smirnov, A.A. Inst : - Title : Concerning the Dependence of the Residual Electric Resistivity of an Alloy on the Composition and on the Degree of Ordering. Orig Pub : 3b. nauch. rabot In-ta metallofiz. AN USSR, 1956, No 7, 115-117 Abstract : Without employing the concept of the Tnesin free path and without assuming the energy of the electron to be inde- pendent of the direction of the wave vector, 'but within the framework of the single-electron approximation, the known relations for the resistance of an alloy were de- rived for the following two cases: (1) for a Uinary ordered alloy without allawance for the correlation -- the dependence on the concentration of the component Card 1/2 SMIRNOV, A.A. Theory of the electrical resistance of alloys. Ukr.fiz.zhur. 2 no-3:211-225 Jl-S '57. (MIRA 10:10) l.Institut metalofiziki AN URSR. (Alloys--Electrical properties) DANILENKO, V.m.: iMIVOGLAZ, M&TYSINi., Z.k-, SHIR110Y. A.A. I la Theor7 of wave 01spersion by the crystal ttIce of solid so- 1vtions. Fiz, met, i metalloved. 4 no.1:28-35 157. (MLRA 10:6) L. inatitut "tallofisiki Akademii nai~c USSR. (Wave mechanics) (Crystal lattices) AUTHORS: Smirnov, A. A. and Stoyanov, I. A. 126-2-V30 TITLE: Theory of the residual electric resistance of interstitial alloys. (Teoriya ostatochnogo elektrosoprotivleniya Bplavov vnedreniya). PERIODICAL: "Fizika Metallov i MetallovedeniYe" (Physics of Metals and Metallurgy), Vol.IV, No.2, 1957, pp.228-231 (U.S.S.R.) ABSTRACT: Up to now authors have dealt mainly with the theory of the residual electric resistance of substitution type alloys (1-6). The aim of this paper is to investigate the relations governing the residual electric resistance of interstitial alloys as a function of the composition, the distant order parameters and the correlation parameters (which characterise the near order relations) between the substituted atoms of various types of nodes and interstices. The calculation was effected on the basis of the multi-electron theory, using a method which was described by this author and his team in other work (3-5). The following simplifying assumptions were made: the potential energies of the conductivity electrons differ little in the field of the ions of the differing Card 1/3 type which substitute the nodes of the lattice. and that the putential energies in the field of the ions which 126-2-4/35 AUTHORS: Dykhne, A.M., Matysina, Z.A,.,and Smirnov, A.A. TITLE: Theory of residual electric resistance of multi- component ordering alloys. (Teoriya ostatochnogo elektrosoprotivleniya mnogokomponentnykh uporyadochivayu- shchikhsya splavov). PERIODICAL: Fizika Metallov i lAetallovedeniye, 1957, Vol.5, No.2, pp. 220-229 (USSR) ABSTRACT: The theory of residual electric resistance of alloys has so far been developed only for certain particular cases. Nordheim. (Ref.1) evolved such a theory vrith single electron approximation, without taking into consideration correlations for disordered multi-component alloys and Smirnov, A.A. (Ref.2) evolved such a theory for ordering alloys with any lattice of the Bravais type in the disordered state. Ryzhanov, S. (Ref.3) has taken into consideration correlation for ordering alloys with a simple cubic lattice. In all the here mentioned viork the usLiaL assumptions of the single electron apDroximation have been made which are unjustified and ere as3ocii-ated with introducing the length of free travel, the character of the energy spectrum of the conductivity electrons, etuc., Card 1/4 which are not really required for deriving relations 126-2-4/35 Theory of residual electric resistance of multi-component ordering alloys. expressing the dependence of the residual electric resistance on the composition, the mrameter of tbe long range order and the correlation parameters (see Krivoglaz and Smirnov (Ref.4)). Within the framework of the multi- electron theory of metals, the residual electric resistance was calculated in earlier work (Ref.5) for binary ordering alloys, taking into consideration the correlation in the first coordinate sphere and in other work (Ref,G) for ternary disordered alloys, taking into consideration the correlation along all the coordinate CD spheres. The aim of this paper is to evolve a more general multi-electron theory of the residual electric resistance of multi-component ordering substitution alloys with any Bravais type crystal lattice in the disordered state,which.in the ordered state, have any number of types of nodes, taking into consideration correlations in all the coordinate spheres. The authors did not aim to determine the numerical values of the electric resistance and they limited themselves to Card 2/4 deriving relations expressing the dependence of the 126-2-4/35 Theory of residual electric resistance of multi-component ordering alloys. residual electric resistance on the composition and also on the parameters characterizinG the distant order and the :=relation in the alloy. Therefore, in the same way as in the earlier work (Refs-5,6), the authors succeeded in carrying out their calculations with a minimum number of model conceptions. In addition to taking into consideration the properties of the translatory symmetry, it was assumed that the potential energies of the conductivity electrons in the field of ions of a different type differ little from each other and that the potential of the electric field in the metal is so small that the Ohm la'w applies. Thereby, the calculation of the residual electric resistance can be carried to finality only if the atom concentrations of all the components except two are small. The subject matter is dealt with under the following headings: Calculation of the probability of transition of the system of electrons from one state to the other; determination of the dependence of the residual electric resistance of an alloy on its composition, the distant Card 3/Lp order parameters and the correlation parameters ail~i-taking correlation into consideration). There are 7 references, 6 of which are Slavic. SUBMITTED: May 3, 1956. ASSOCIATION: Institute of Metal Physics, Ac. Se. Ukral=ian SSR (Institut Metallofiziki AN USSR) AVAILABL~;: Library of Congress. Card 4/4 21-5-11/26 AUTHORS: Geychenko, V.V,(Heychenko, V.V.) Corresponding~!ember of the AN Ukrainian SSR and Smirnov, A.A. (Smyrnov, A.A.) TITLE: Study of Interatomic Interaction in Interstitial Alloys by the Wave Scattering Method (Izuchehiye mezhduatomnogo vzaimodeyst- viya v splavakh vnedreniya metodom rasseyaniya voln) PERIODICAL: Dopovidi Akademii Nauk Ukrainslkoi RSR, 1957, Nr 5, PP- 470- 473 (USSR) ABSTRACT; The authors consider the application of the theory of X-ray scattering by interstitial alloys for determination of some constants of interatomic interaction. The data obtained make it possible to find the correlation parameters in alloys with two kinds of atoms at the lattice points and one kind in the interstitial positions by the intensity of scattered radiation and making use of Fourier calculus. The authors consider a particular case of an alloy whose lattice points are occupied by atoms A and B and form a face-centered cubic lattice and interstices are partially occupied by C-atoms. The correlation parameters enable one to estimate the micro-nonuniformities Card 1/2 of the alloy. Formula 7 in the article can be applied to 137-58-6-13104 Translation from- Referativnyy zhurnal, Metallurgiya, 1958, Nr 6, p 274 (USSR) AUTHORS: Krivoglaz, M.A., Smirnov, A.A. TITLE: To the Termodynamic Theory of Second-order Phase Transi- tions in Solid Solutions (K t9rmodinamicheskoy teorii fazovykh perekhodov vtorogo roda v,fverdykh rastvorakh) PERIODICAL. Sb. nauchn. rabot In-ta metallofiz. AN UkrSSR, 1957, Nr 8, pp 65-69 ABSTRACT~ Relationships are obtained between the second derivatives of the thermodynamic potential 15 relative to the temperature T, the pressure P, and the concentration c which are generaliza- tions of Ehrenfest's relationships for solid solutions. Within the framework of the thermodynamic theory of second-order phase transitions, relationships of the degree of the lower- range order of Y1 were calculated relative to P and c close to the transition point. With T and P constant., 17 's ~-c o, while with T and c constant, ~rVTP--p, where c. and Po are the values corresponding to the transition curves. To deter- Card I/-- mine the slope coefficient of these relationships it is necessary 137-58-.6-13104 To the Thermodynamic Theory (cont.) to know the coefficients of the expansion of ~ according to powers of I I as performed in thermodynamic theory, and the derivatives 9TOIC)c or r,I Tolc9P, where To is the transition temperature. M.K. 1- Metals--Phase studies 2. Metals--Thermodynamic properties Card 2/2 18(7) PHASE I BOOK EXPLOITATION S011/2025 Krivoglaz., Mikhail. Aleksandrovich,, and Adrian Anatollyevich Smirnov Teoriya uporyadoclaivayushchikhsysL splavov (Theory of Ordering in Alloys) Moscow,, Fizzatgiz, 1958. 388 p. 5,000 copies printed. I Ed.: K.P. Gurov; Tech. Ed.: W.Ya. Murashava. PURPOSE: This book is intended for solid-state physicists and advanced students specializing in the physics of metals. C01TERAGE: The book aims to give a systematic presentation of the more extensively investigated aspects of the theory of ordering in alloys. The phenomenon is- studied from two points of view: the actual ordering of atomejand the effect thereof on the properties of the alloy. The author states that the theory of ordering makes it possible to determine the short-and long-range order estab- lished in alloyp of various compositions at different temperatures and to ex- plain the effect of-composition and heat treatment on the properties of alloys. Sufficient experimental data are included to illustrate the basic assumptions of the theory. No personalities are mentioned. There are 337 references, of which 153 are Soviet, 140 English, 31 German, 6 Japanese, 4 French, 1 Danish, 1 Dutch, and 1 Chinese. Card 1/ 6 theory of Ordering in, Alloys TABLE OF CONTENTS: Preface SOV/2025 5 Ch. I. General Informa;tion on the Phenomenon of Ordering in Alloys 7 1. The Ordering of atoms in alloys 7 2. Examples of the ci-jstal structure of ordered alloys 13 3. X-ray analysis of ordered alloys 19 4. Neutron diffraction study of ordering in alloys 34 5. Change in heat capacity and energy of alloys in ordering 41 6. Effect of the ordering of atoms on the electrical resistance of alloys 43 7. Kinetics of ordering 51 a. Effect of bombardment with fast particles on the ordering of alloys 58 9. Investigation of the relationship between ordering and the mechanical, magnetic, magneto-resistive, and other properties of ordered alloys 69 Ch. II. Thermodynamic Theory of Ordering . 10. Classification of phase transformations 85 85 Card 216 Theory of Ordering in Alloys SOV/2025 11. Thermodynamic theory of phase transformations of the second type 90 12. Thermodynaziie theory of nearly completely ordered alloys 109 13* Fluctuations in the long-range order and.composition of alloys 117 Ch. III. Statistical Theory of Ordering 127 14. Method of approach 127 15. Matrix methods 131 16. Theory of ordering without regard to correlation in the alloy (Theory of Gorskiy, Bragg, and Williams) 142 17. Method based on the expansion of the free energy in a power series of v (Kirkvood's method) 153 T, 18. Quasichemical method 165 19. StatistIcal theory of almost fully ordered alloys 172 20. Effect of the pdmixture of a third element on the ordering of alloys 181 21. Discussion of results of the statistical theory and comparison with experimental data 195 Card 3/6 Theory of Ordering in Alloys SOV/2025 32. Investigation of frequent cases of X-ray scattering 291 33- Scattering of slow neutrons by ordered alloys 301 34. Application of the method of fluctuation to the problem 7 of scattering '08 Ch. VII. Theory of Residual Electrical Resistance of Alloys 335 j5. Determination of the lirobabillty of electron scattering by the alloy crystal lattice 335 36. Derivation of formulas for determining residual electrical resistance 343 37- Residual electrical resistance of binary alloys 345 38. Residual electrical resigtance of ternary alloys 352 Ch. VIII. Magnetic, Magneto-resistive, Optical, and Mechanical Properties of Alloys 357 )9. Magnetic, magneto-resistive, and optical properties of ordered alloys 365 Card 5/6 GEYCHRIKO, V.V.; KRIVOGLAZ, M.A.; SMIRNOV, A.A. Studying atomic interac-t!6~~_in alloys by, means of wave scattering by the crystal lattice of alloys. Isal. po zharopr. sPlav. 3:140-149 1 58- (MIRA 11:11) (Alloys) (Crystal lattices) (Particles, Elementary--Scattering) DANILENKO, V.M.;JYj,VOGLAZ, M.A.; MATTSINA, Z.A.; SMIIUIOV. A.A. . I - _I- - '-" Thmory of slow neutron scattering In a . Inal. po zharopr. QPlav- 3:150-160 158. (IGRA 11:11) (Neutrons--Scattering) (Alloys) r 18(0)9 24(2) SOV/181-1-9-13/31 AUTHORS: Smirnov, A. A., Tikhonova, Ye. A. TITLE: On the Theory of Scattering of X-Rays and Thermal Neutrons by blulticomponent Substitution Alloys /? PERIODICAL: Fizika tverdogo tela, 1959, Vol 1, Nr 9, PP 1393 - 1400 (USSR) ABSTRACT: The authors investigated the influence exerted by geometrical lattice disturbancesq caused by different atomic radii of the components, on the X-ray- and neutron scattering in disordered binary and multicomponent alloys. Special attention is devoted to the concentration dependence of the scattered radiation intensity. The investigations,were conducted after the model of the Boris elastic continum for the special case of binary alloys* ~Moreover, they were made on the assumption of the displacements being superposable, without considering the correlations between the substitutions of the various lattice points by atoms. Calculations are made within the kinematic scattering theory-. The authors considered the scattering of a monochromatic radiation on a single crystal. First, the general theory of X-ray scattering in multicomponent alloys is Card 1/2 developed, and this is then applied to the special cases of a On the Theory of Scattering of X-Rays and Thermal SOV/181-1-9-131'31 Neutrons by Multicomponent Substitution Alloys binary and a ternary alloy. The formulas obtained can be used for the calculation of scattering intensity in alloys with disturbed lattice, and permit the investigation of the cor, centration dependence of the regular reflection and the back- ground intensity. There are 8 references, 5 of which are Soviet. ASSOCIATION: Institut metallofiziki AN USSR Kiyev (Institute of Metal Physics of the AS UkrSSR Kiyev) SUBMITTEDi December 30, 1958 Card 2/2 SWRNOV, A.A. [Smyrnov, A.A.]; TIKOZIOVA, Ye.A. [Tykhonova, 0.0.1 Contribution to the theory of X-ray and thermal neutron scattering by multicomponent substitutional alloys. Ukr, fiz. zhur. 4 no.3:322-333 M,v-Jo '59. (MIRA 13:2) I.Institut metallofiziki, AN USSR. (I rays--Scattering) (Neutrons--Scattering) (Alloys) AUTHORS: Yi-rivoglaz, M.A. and Smix-nov, A.,~L. SOV/126-7-1-23/28 TITLi,.. On the Possibility of Determining the Form of the Fermi Surface From the Angular Distribution of Y--Quanta Formed in the Trans- formation of Electron-Positron Pairs into Photons (0 vozmozhnosti opredeleniya formy poverkhnosti Fermi po uglovomu raspredeler-kiyu -~-kvantov, obrazovavshikhsya pri prevrashchenii elektronno-Dozitronnykh par v fotony) PERIODICAL: Fizika Metallo-v i Metallovedenie, 1959, Vol 7, Nr 1, pp 151-152 (USSR) ABSTRACT: In units of h/2rr (h being Planck's constant) the character- istic momentum vectors for the crystal lattice, electron, positron and resultant photon are denoted by a, y,, KI and p respectively. The transition probability for pair annhil- ation with photon production in the lattice is then given by the standard formula: 2 w u ull exp ( -2 -Tr i_~r) d7.' 2 Card 1/3 SOV/126-7-1-23/28 On the Possibility of Determining the Form of the Fermi Surface From the Angular Distribution of "--Quanta Formed in the Transformation of Electron-Positron Pairs int._ Photons U Here the u's are the particle wave-functions and of course involve the configuration vector r; eur is the unit of volume In configuration space- t7he dq1ta-term insurgs the conservation of momentum. The angular distribution of quanta may be obtaLried explicitly from this formula by writing r and its dprived functions in terms of polar co-ordinaTea r. r!, / and integrating out the redundant variables. The di3tribution is related to the Fermi energy surface through the latti3e and particle ventors, and in principle this surface could be determined for all values of .E by absolute intensity measurements of the photon dis- tribution at a large number of angles. In practie-,g it is feasible to make only relative intensity measurements at a few angles, and the note suggests how these angles be selected to afford the maximum possible information about the general form of the Fermi surfase. In particu.1ar, the theoretical interpr9tation is considerably simplified for angles correspondinS to the vanishing of one or other of the basic Card 2/3 vectors. SOV/126-7-1-23/28 on the Possibility of Determining the Form of the Fermi Surface From the Angular Distribution -o7f 1( -(duanta Formed in the Transformation of Electron-Positron Pairs into Photons There are 7 references, of which 4 are Soviet and 3 English. ASSOCIATION: Institut metallofiziki AN USSR (Institute of Metal Physics, Ac.Sc. UkrSSR) SUBMITTED: October 7, 1957 Card 3/3 AUTHORS: Nosar', A. I. and Smirnov A._&. SOV/126-7-6-2/24 TITLE: Theory of the Residual Electrical Resistivity of Binary Disordered Alloys with Imperfect Crystalline Lattices PERIODICAL: Fizika metallov i metallovedeniye, 1959, Vol 7, Nr 6, pp 8o9-8211 (USSR) ABSTRACT: The theory of the residual electrical resistivity of disordered substitutional alloys of non-transition metals was given by Nordheim (Ref 1) in terms of the one-electron model, without any allowance for correlation and static defects of the crystal lattice. For binary alloys A-B this theory leads to a parabolic symmetrical curve which gives the dependence of the residual electrical resistivity e on the relative concentration C of the A atoms in the alloy; this curve can be expressed as e = kcA (1 - cA). Further developments of the theory (Refs 2,3) allowed for various factors which affect P. The many-electron Card 1/3 theory of the residual resistivity was used by several workers (Refs 4-10) for binary ordering alloys. These SOV/126-7-6-2/24 Thecry of the Residual Electrical Resistivity of Binary Disordered Alloys with Imperfect Crystalline Lattices workers allowed for correlation but not for geometric defects of the crystal lattice. The present paper deals with the effect of lattice defects due to different dimensions of the alloy atoms on the concentration dependence if the residual resistivity of binary (A-B) disordered substitutional alloys of non-transition metals. The many-electron theory of metals is used but correlation between lattice substitutions in the alloy is not allowed for. Since the treatment is qualitative, in the sense that a numerical value of the electrical resistivity is not obtained, the defects are allowed for by means of a rough "elastic-medium" model, used in discussion of X-ray scattering in alloys (Ref 14). Dependence of the residual electrical resistivity on the concentration c A is obtained in the form (0= AcA(l - CA ) + BcA U - c A (a0 + a1c A) (105) Card 2/3 where a 0 and a 1 are functions-of A(cA ) and wB(cB ) and W's are mean volumes of A (or B) atoms, which depend on the SOV/126-7-6-2/24 'Theory of the Residual Electrl 100 A the edge of the. optical absorption is weakly pronounced., but when a - 1-3 Py the absorption curve is similar to that for bullqr single crystals., but is shifted in the-long-r e re ion. The temperature coefficient determined from this ratio dEWdT ev h X 103 V/gM wit '~deg, agrees with data for single crystals. An so field of 5 frequency 16 cps shifted the absorption range in the region of X 5100 A'by.an CaM V2 io 7- o I-"),