SCIENTIFIC ABSTRACT FEDOROV, D.P. - FEDOROV, F.I.

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SCIENTIFIC ABSTRACT
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Fed orov, A D. P. i se-i in ge mar) wrm !~ez,hvuzovs~,aya nauchno-tckhniche(k~ya e rk i kantaktnyyc ya%-leniya v T- - !n I germanium transistor authors s-,u&y the nelationship betw~c!,) -C--~Qr ilin-tions In P4 allayel- Junct .)f temperature on ncises in *hf:sr- t,- detr-: -in ine the c-,-nbine,~ n, ise o-f the ACCESSION NR: AT5020464 ir Iv ~n~levondfmt of tho rmprmont ,f -A A: ii, ~1~ I iRqi 0 L 3-133-66 EWT(l)/EEC(k)-21*Z/EWA(h) IJP(c) GS ACCESSION M AT5020479 UR/OOW/64/000/000/0328/0334 4 AUTHORS3 Kuznetsov V. I.j Shchevelevs M. I I Fedorov D. P. q.~ TITLE: Temperature dependence of parameters of plate silicon diodes SOURCE: Mezbvusovskays nauchno-tokhnicbeskaya konrerentelya flzlke po.~,qpr9yodnikoy (p2verkhnostrAyy9 I kontakt! vleni . TOM IWO , =L" L_" L Poverkhnostmyye i kontaktwjyo yavlaniya v poluprovodnikakh ce and- 0 tact I phenomena in semiconductors), Tomsk, Isd-vo Tomokogo univ.p l9u+j 328-334 J TOPIG TAGSs :volt ampere characteristic, silicon diode, electric curront / D202 diode, D20 diode ABSTRACTj Results from experimental investigation of the temperature dependence 'of tho back volt-ampere characteristics and break-through voltage of plans silicon high-voltage liodon of the typo D2(P--M051 *re reported,, P-mr-imters of -the diodes were meas&ad in,~he texperatwv interval of 20-1700. At low return voltages the current Increases with the temperature, while at high voltepa. the opposite takes place, leadl~g'to the increase of the break-through voltage of the diode. Figure I on the Enclosure shove characteristic curves for the temperatwe dependenob of the break-through voltage* It in obnaludod that two processes occur in aillcon diodes. , one of vhich leads to an iam-sase In the return ourr at with tesperaturs,, Card 113 L 3-133-66 ACCESSION NRt -AT5020479 the other to a decrease. The first process is related to the generation of beat in the current carriers and Is practically independent of the voltage on the transitions. The second pvassa is connected with the surface changes occurring on the silicon oxide,, due to.the changes in concentration of chemisorbed moisture with temperature., To support this latter aisumption, temperature dependencolof 30 silicon transitions on the break-down voltage was recordedi The transitions were then dried for 8 hours in vacuum at 2200p then maintained In moist atmosphere for 5 days, each time recording Vv(T), A detailed chemiftl exp1mustion of the process is given. Or1g, wt, bast .4 figures '31 ASSOCIATIONi am SUMITrEDs 06Oct64 ZWLt M SM 001XI Ba NO REF SOVt 003 OTHERs 003 Card 2/3 L 3.133-66 ICCESSION MR'S AT5020479 IVA n M -1.11, ~ - ~ '- ~- i I.- ,. - - i -. - i~ , 'I . . !- . - 1-1 ~ ... 1-.1 -R-. [lyi- --- -- -- - - - Fedorov, D.S., Temperature regime of ocean currents as an indicator of their variability, Tr. Leni~gr. gidrometeorol. In-ta (Works of the Leningrad Rydrometeorological Institute), 110 7, 1956, p 211-216; (RZhGeofJ,z 12/58-8872) FEDOROV D.T.(Chiia) A3.1'depote of the railroad boaame profit bringing units, Zheladoretranspe 45 no.2.-73-7/+ F 163. (min 16t2) 1. GlavVy insh. Zabaykallskoy dorogi. (R-ailroads-kreight) ACCESSION NRs AP4017788" 5/0083/64/0004002/0024/0023 AUTEIORt Fedcrov,, go TIM: Satellites and weather forecasting SOURGEs Kry*llya roditW*~ no.-2# 19&* 24-23 or TOPIC TAGS: mote ologyg telemeteringe v"tbAr satellite ABSTRACTs Ground meteorological observatories have the disadvantages of being located unevenly over the surface of the earth* with large areas covered very poorly (especially water areas); being able to penetrate only the lower layers of the air, so that upper air soundings are too scanty to be of much use in woathor forecasting; and are unable to transmit their observation data U central processing offices# in many oasest until they are too old to be of maxim= value. Weather satellites would not be subject to these disadvantageso Images of cloud cover over extensive areas obtained from satellites are especially valuable for forecasting storms mid cyclones. Tho heat balance of the earth is also easily measured from satelliteag as are the atmospheric temperatures at various alUtades~ the composition of the atmosphere# and the upper boundaries of cloud covert Active radar tracking from satellites can Card 1/2 ACCESSION XR: AP4(a"88 trace cloud movements and the nataro of prealpitation. Satellites may also be used as-co=,Wcatton r*LW points for observation stations located in remoto regions. Meteorological satellites should hAve orbits *Us* to a polar orbit so that they can cbserve alLlatitades of the slabs* OrU. art. has 2 diagrams. ASSOCIATION: none SUR-MTED: 00 AM nN&rf4 MMS 00 SUB CODEs AS* CO 30 MY SOVS 00 OMM: 00 Car,d 212 L __~--54 FEO-2/EVT(d'/FSF(h)/FS--,I , - -,. -,., -, - 'L r L A 14 ~IR: A, P 5 /FWI 13 "rom the COz-:MO,-. ~;uidi-ng airplanes e r, j f r3 a r tLa ~a Ba Ie 111 tea K7y]'ya rorliny, no, 2, 1965, 22-2) T`IFI,~ -AL'S: Inavi n satellitl~ navigation system, sr-tolil- -r-, aircraft gliidance equ i unO I ABSTRACT: New vistas in the realm of airplane nnvigation arq earthIq artificial satelllte6, Ajij7-,:I a --ror,i I nn `3 r r,F ma y b-ic mp u ?i"Cular (Ind q-~ a he~g~ L ACCESSION, INT.: AP5006235 The apVaratus in each ri-atal I I f and --In the plaiae-=at-b zym6ranized that the planar cowuter will cale-alate the coardimtos, course, velocity, and altltwie In rint only planes but a!,;,) Sy a !-~3m. rlis a -'1a S A36;,-),~ LAT WN t none SUB'1437"TZI)t 00 ENCLi SUT CC'r--- IrG OW OTHb 000 7XDOROT, NoTee 1, "' - gronlits 'ia'truvton In ths Tabs and 4rda Basin$ (KmnOYarsk Urrito27)o Nate TM11I Ob. my. soiSsI06-in J48o (Ni" USO (&onoprok UrritoW-Woultes) --., Devonian igneous aotivity in the Mimwinsk Basin. Trudy VSEGEI 58:125-133 161. (KM 15:5) (Minusinsk Basin~-Rocks., Igneous) TMJNOV, A., glavMy Inzhennr; IMMINNYT, L. . inth h. Converting to central control system at the grain elevator of the Kirov Milling Combine. Muk.-elev.prom. 25 no.6:9-10 je 159.~ (MIRA 12:9) 1. Leningradskly mellnichWy korbinat im. S.M.Kirova (for Trunov). 2. Odesekiy proynictno-konstruk-torskiy Institut Pishcheprom (for Reynennyy, Fednrov). (Grain elevators-zquipment and supplies) (,,kutomatic control) , 11 , "Rationalization Serves Pmduction.," Tokst. prom., 12, lio.43 1952 , ~. A, FEDOROVP F. A. "Mechanical ~Iethod for Rermving Droppirws from Under the 11fackling Machine," Tekst. prom.2 12, No.8. 1952 FIDDROV, P.A. Device for planlvg grooved metal rollers for spinning looms, Obm.tekh.opyt. (MLPJ no.20:5-6 '56. (14IRA 12:11) (Planing machines) M FEDOROV, f.A. Addition of 300-200-brand cement to tho BF-2 glua for in- creRsing Itn strength. Obm.takh.opyt.[Wj no.20t19-20 156. (MIRA 12:11) (Glue) FIDOROV. N.A. Improved design of T-uhaped brass clamps for fastening the R and D- system atomizers. Obm.takh.opyt.[MU] no.20:28-29 '56. (MIRA 12:11) (Spraying) FEDOROV.9 F.A. lap for repairing sliding oalipers. Tzm.tekh. no.3jl2 963. (Calipers) (MM 1684) 7EWROT 7 27, trollin pectors W99ti -.-..g,4oisting machinery. Besop. truda v prom. 1 no.407 Ap 157. (MM IWO (Hoisting machinery) TEGORUMIN, V.Te.; KRAMOMMKOV, N.A.; RA2XTSLOVICH, I.R.; FXWROVv F.F: - SMEMOVICH, P.V.; TSVYRKUH, N.A.; BUYLIN, G., 2-.&-T re , UU-CHITS, G., tekhn.red. (Handbook of a tractor driver] Spravochnik traktorista. Minsk# Gos.izd-To BSSR. Red.selikhos.lit-ry, 1959. 578 P. (MMA 1):3) (Highway transport workers--Handbooks, manuals, etc.) GOLOYNIT, I.F., kand.tekhn.nauk; PANOT, A.A.1 YICDOROT, F.F.; YUTACIIEVA, N.Ta.; TALAGINA, T.A., tekhn.red. (Press forging; bibliography with annotations for publications in 19571 Obrabotka metallov davleniam; annotirovannyi biblio- grafiohaskii sprovochnik literatiwy Sa 1957 god. Leningrad. Mo .1, [Haating and drop forging) Nagrev, kovka I goriachais shtampovks. 1958. 132 p. (KIRA 13:2) 1. Laningradskly dom nauobno-takhnichookoy propagandy. (Bibliography-Irorging) TATNTRAUB, D.A.; PANOY, A.A.; FXDOROV,_Y.V.,- TUTACHSTA, N.Ta.; TILAGINA., ?*A., takhn.red. (Press working of metals; annotated bibliography of publications for 19373 Obrabotka metallov davlanism; annotirovannyi bibliogra- ficheskii spravoohnik lit^ratury za 1957 god. Leningrad. No.2. (Die stamping] K61odnaia.shtampovka. Pt.l. 1959. 99 p. Pt.2. 1959. 77 P. (MIRA 13:3) 1. Leningradskiy don nauchno-tekhnichaskoy propagandy. Nauchno- tekhn1cheskqa bibiloteka. (Shest-metal work) RIMMYY9 Lavinzhs; YXDOROV, P.,insh. Devices aM eqnipment for the automatic control of 'various operations in grain elevators. Muk.-eleveprom. 25 no,2:8- 10 1 159. (KMA 12:4) 1, Odeaskiy proyektno-konstruktorskiy institut Pishchaprom. (Grain elevators) (Automatic control) FEL)C,ff)v, Theory of elautle itavee in cryBtalD. Comparison with an isotrople medium. Xrlsta-Uografila 8 no.2:213-220 Yx-Ap 163. (MIRA 17: 8) 2.. Inotitut flziki. AN BSSR. U . I)rlr. -1 !., -r i r , I, -k - Fedorov, F. 1. - 'On the superposition of physieal magatudesm, rzvestiya Akad. nauk BSSR, 1949v No. 2, p. 17-18. SOt U-411, 17 July 53, (tatopla tZhurnal tnykh Stateyl, No. 20, 1949). FEDOROV9 F. I. USSR/Physics - Relativity Wave Equation 11 Avg 51 "Kiniman Polynomials of the Matrices of Relativistic Wave Equations," F. I. Fedorov, Belorussian State U imeni Lenin "Dok Ak Nauk.SSSR" Vol LMX, No 5, PP 787-790 Purpose is to show that the condition' which states that among the states possible for particles those must be absent corresponding to energy density equal to zero' also permits oneessentially to limit the form of the minimum polyn of the matrices of the following equation: ik)P=O, where P repre- sents the psi-function. ted by Acad V.A. Fok 16 jun 5l. 21OT90 1 Genert. c I.S 18 ;03-733 tj "r Vk iF.4 mi" I? ut 10. Shi I U.6 "Pec or all c-,~st'.v'Co an t4 t4~ WSSR/Physics Crystallograpby, Optical 21 Jun 52 Parameters "Determining tl!.%e Optical Param terB of Monoaxla7 Cry a- tale According to Reflected Light," F. I. Fedorov, Belorussian State U iment Lenin "Dok Ak Nauk SSSR" Vol LXXXIV, No 6, PP 1171-1174 Subject investigation is based on the relations among the amplitudes of reflected and incident waves for the case of incidence of light from an isotropic medium or, to a monoaxial nonconducting nonmagnetic crystal. Designates the unit vectors of the wave Mormals of the incident reflected, ordinary and eXtraordinary waves; vectors of the elec and magnetic 223rI02 fields; Indices of refraction of the isotropic medium; ordinaz7 and extraordinary rays; =it vector of optical axis of crystal; tensor of dielec per- mobility; unit vector of normal to the surface of sepn. Submitted by Aced D. S. Belyankin 24 Apr 52. 223T102 --~ -1.1 .6 Use of the method of functionals In certain problamg of milatlon ** theory. Uch. sap. WU no.146-33-73 '52. (KIRA 11:W j0pautum theOr7) Pu a) PAnRIVICH. I.G., kandidat f iz Lka-matematychnykh rAruk, reclaictor; nMARAU 'I kaudydat fizika-matemstychnykh navak, redaktor; 1b., takl=edaktar. [Radio and its role in the davtlopmeat of culturer and technical progress) Radylo i itho Yolia u razvitstei kulitury i takhnichnaba pragresu. Minsk, Vyd-va AN BSSR, 1953. 30 P. (KLRL 8-.2) (Radio) r T F- I I YEDOROT, Fedor Ivenovich -PiDOROV, Fedor Ivanovich (Belorussian State U Iment Lenin), Academic Degree of Doctor of Phystoo-Mathematical Sciences, based on his defense. 3 Dec- ember 1954, In the Council of the State Order of Lenin 0 ptioal Inst imeni Vavilov, of his dissertation entitled: "InvariMle methods In :the optics of anisotropic mediums.1 For the Academic Degree of Doctor of ScIencas. SO: Byulletan' Kint" terstra, Vysshego Obrasovantya SSSR, List No 20, 8 OctoUr 1955, Decision of Higher Cartifteation Commission Concerning Academic Degrees and Titles. MARAU,F. 1. - - 0. - O~! 0- RM; , Invariable Indications of the polarization of light. Testsf AN BSSR no.6:78-91 N-D '54. (KIRA 8:9) (Polarization (Light)) 11 1 : -,:: I- - . ~ ~ - - .;; ~ 1. :-1 ~F- - t, -;, . ; ,~ .. - - . .. , , '. - -. 4' , , V " ; -, , ... - - :, ~ r ~-. :1,)7,1i.~1 '. ~;, - I j ~ ; ;. . - ~i-- I .I USM/Physics Elect. magn. wave polarization QU4 1/2 Pub. 22 - 17/49 AnVion I Fedorovi F, I* Title S About. the polarization of electro-magnetie. waves Periodical i Dok. AN SSSR 102Am 69-71, May 1, 1955 Abetraot I An anAlysis of electro-magnetie-wave polaiitation is preserdood, Monochro- Matic homogeneous " non-homogeneous waves are considered. Two m6thods for analyzising the ho=geneous waves are suggested. 1he first method starts from a consideration of the wave ariplitude in the fom E a 1~ + iE . where the real vector parte E~ and 3 are conjugated semi- damet6rs of2~he ellipse of oscillations. ilia pecoRd method consists in the consideration of the complex vector E = E0elf , where is a phase Institution The Acad. of So., USM, Physico-Technical Institute Presented by t- Academician A.A. Laboday, December 13, 1954 Card 2/2 Pub. 22 - 17/49 Periodical i Dok.,AN SSM 102/lp 69-71s M&Y lo 1955 Abstract I of the oscillations. A consideration of the nen-homogeneous wave polarization is suggested# starting 4ith the reduction of Fammll's equation to the following formt JxHj, "H a [mEj As a result of such a treatment of Yjmell's equation a series of properties of non-homogeneous slectro-magnetic waves is listed. Two referencess 1 USS and'l Oem. (1929 and 1952). -f _i-__ - --_ - .- - - - I . j Crystals. B-5 Abs Jour: Beferat. Zhu=al'Xhiziym,, No 3, 1958, 7082. Author ?.I. Fedorov. Inst, Title "Transfer Principle and General Theory of Optical Pro- Parties of Absoxting Crystals. Orig Pub: Oj?tiki% i spektroakcpiya~ 1956, ls No 6s W7-W8- Abstract; Me lack of foundation for the "transfer principle" is enoa- sized. According to this principle,, all the relations of optics of transparent crystals my be transferred to the cases of absorbing ned'a (aouiprising mmonlilmi a and triclinic crystals) on condition that corresponding magnitudes receive coaWlex va- lues. Cited conputations show that the tensor of dielectric permeability has not generally three ova linearly independent vectors, it has not even ccMlex vectors.. consequently, the theory based on the "transfer principle" cannot be applied to Card 1 1/2 .27- -4w 17 I . . ff-~- ill 1~ t3l I YEDDROT, : ~ - - - Determining the optical parameters of absorbing crystals. Isr.A)i SSSR Ser.fis.ac.5064-369 056. (KI2A 9:9) LInstitut fluild i matematiki Akademli saidt BSSR. (Crystallography) USSR/Theoretical Physics B-6 Abe-Jour Referat Zhur Fizika, No 5. 1957s No 10898 Author Inst Institute of Physics and Mathematics, Academy of Sciences, Belorussian, SSR. Title Reduction of Wave Equations for Spin Zero and One to the .Hamiltonian Form. Orig Pub Zh. eksperim. i teor. fiziki, 1956s 31,, No 1, 140-142 Abstract A method is given for the reduction of the equation for particles with spine zero and one 019 VA -I- Y to the Hamiltonian form. The method is independent of the actual choice of natrixes(3 k and is based only on Eq. (1) Card 1/2 nwiRov, T. I. Certain dot-product representations of tbree-dimensional tensors. Trudy Inst.fis. i mt. AN BSSR no-2:230-234 1 57. (MIRL 12:1) (Calculus of tensors) AUTHOR: Fedorov, R.I. 51-3-12/24 TITLE: Optics of magnetic crystals. II. Binormals and biradials. Optical.surfaces. (Optika magnitnykh kristallov. II. Binormali i Biradiali. Opticheskiye Poverkhnosti). PERIODICAL:"Optika i Spektroskopiya" (Optics and Spectroscopy), 1957, Vol.2, No-3, PP. 361-370 ~U.S.S.R.) ABSTRACT: Continuation of the author's paper in "Optika i Spektroskopiya", Vol.1, p.926, 1956. Theoretical electro- magnetic calculations give directions of binormals in a general type of magnetic crystal. It is found that, in general, transparent magnetic crystals (just like non- magnetic ones) have two binormals. A principle of duality, i.e. parallelism of the systems of equations, is established for normals and rays in infinite magnetic crystals. Binormal and biradial surfaces are found to be, in general, different. The limiting values of the refractive indices are obtained. The optical normal surface and its cross-sections are derived and shown in figures. There are Card 1/1 5 figures; 3 references (2 Slavic); a mathematical appendix (matrices and tensors). SUBMITTED: June 2 1956 ASSOCIATION: Physics ana Mathematics Institute,Ac.Se. of Byelorussian .-SSR (Institut Fiziki i Matematiki Ak.Nauk BSSR). , AUTHORt Fedorov, F.I. 51-4-17/25 TITLE:,6_pMT5q ZI-Magnetic crystals. III Uni-axial and uni-refringent magnetic crystals. (Optika magnit~Wkh kristallov. III Odi~ow~We 1i odnoprelom1,yayushch!34,f magd,~nve kristally). PERIODICAL: "Ontika i-Spektroskoviyall (uptics and Spectroscopy) ~ .. .-1957, Vol.2, No.4s PP-514-Y23 (U.S.S.R.) ABSTRACT: This purely theoretical paper is the continuation of the author's papers in Optika i Spektroskopiya, Vol.1, p.926, 1956 and Vol.2, P-361, 1957. The electromagnetic'theory of ~wave propagation is applied here to particular cases of magneto-anisotropic media. Uni-axial magnetic crystals, de7 fined as those which possess a unique axis along which both normal velocities are identical) are considered. Optical sur- faces are derived and illustrated for these crystals. It is established that, in general, in uni-axial magnetic crystals; (a) binormals do not coincide with biradials; (b) ray velocity along a biradial is not equal to normal velocity along a binormal. It is shown, in principle, that there also exists a group of anisotropic magnetic crystals for which birefrin- gence is absent (they are called uni-refringent). In other words in such crystals light velocity depends ondirection Card 1/2 but has only one value for each direction. Linear polarization AUTHOR: Fedorov, F.I. 51-5-10/26 TITIR: Optics of the Absorbing Crystals. (Optika pogloshchayu- shchikh kristallov) I. General Relationships. (I. Obshchlye sootnosheniya) PERIODICAL: Optika i Spektroskopiya, 1957 Vol.2 No-5 ppe &6 - 6L (USAR). ABSTRACT: The fundamentals of the optical theory of the absorbing crystals were given by'Voigt and DrIlde at the end of the last and beginning of the current centuries. Their theory, however, is not absolutely general since it has limitations due to using a special system of co-ordinates, the -so-called"principal a:kes" of the complex tensor of dielectric permittivity. this theory is also very complicated and leaves certain important questions un-answered. In the current paper (which is to be followed by further parts), a fully-general theory of the optical proper- ties of the absorbing crystals is developed on a new invariant basis and this now theory is free of many limitations of the Voigt and Drdde theory. .Starting from Maxwell's electro-magnetic equations, general relationships are put forward for propagdion of plane, in particular, non-uniform,waves in the-absorbing crystals. A Card 1/2 general equation for normals in an invariant form is obtained. Optics of the Absorbing Crystals. 51-5-10/26 The conditions for linear and circular polarisation of waves are discussed* The directions of the wave-field vectors are determined for a given vector of refraction-Theh?aRe5 is ent- irely mathbmatlOal-TheTe` "0' 8:, -references 9 . or. w c are Slavic. ASSOCIATION: Institute of Physics and Mathematics of the Ac-Sc. Belorussi'an SSR. (Institut Fiziki i Matematiki AN BSSR) SUBMITTED: July 6, 1956. AVAILABLE: Library of Congress uard 2/2 AUTHORs Fedorov.. 51-6-13/26 TITLE: Optics of Absorbing Crystals. II. Crystals of Middle Syngonies. (Optika pogloshchayushchikh kristallov II.. Kristally arednikh singoniy.) PERIODICAL: Optika i Spektroakopiya, 1957, Vol.11, Vr.6, ppe 776-780. (USSR) ABSTRACT., A theoretical paper. Optical properties in an Invariant form are discussed for absorbing crystals of trigonal, tetragonal and hexagonal syngonies. General equations are obtained for the refractive Vector and for field vectors of the orcHnary and extra- ordinary waves. Both uniform and non-uniform waves are treated. The conditions for linear and circular polarisation of waves are given. In uniaxial absorbing crystals for uniform waves polarisation properties are obtained similar to those of transpareAt uniaxial crystals. It is found that absence of double refraction occurs in absorbing uniaxial crystals not just fbr a single direction of the incident of wave, as in trans- Card 1/2 parent uniaxial crystals, but for a range of directions. 61-6-13/26 optics of Absorbing Crystals. Il. Crystals of Middle Syngonies. r There are 4 references, all of which are Slavic. ASSOCIATIONs Institute of Physics and Mathematics) Academy of Sciences of the Byelorussian SSR. (Institut fiziki i matematiki AN BSSR) SUBMITTEDs July 6, 1956. AVAILA.BLEs Library of Congress. Card 2/2 - 1 ~~ I I %F I I ~w %I / j . -A- , I%- . SUPRUNEM , D.A.; NEWSHEVICH, I.G. History, of development of physicomathematleal White Russia. Vestsi AN BSSR Ser. fiz.-takh. 157. (White Rusaia--Physica) (White Russia--Mathematics) sciences In nav. no-3:17-20 (MIRA 11:1) Light reflection and refraction laws In a vector form. Uch.zap. BOU no.32:169-lV. 1 57. (MIRA M12) (Light) PHM I BOOK Z-21A.-UATION 663 OYtIkA anizotropufth are& (Optics of Antootropic Media) Minsk,, Izd-vo AN BBSR" 190. 379 p. 2pOOO copies printed. Zdat Stepswvj, B. L# Prof.; Ed, of Publishing House: Barmichey, V, Tech. Ed.; Als"androvich., Xh. PURPOSE: This book in intended for the use of students and specialists in the field of optics with special emphasis on aniacytropic media, COVERACIN: Thin book is a presentation of the phenomenological electromagnetic theory of light propagation in homogeneous, mainly sainotropiczedla. It also covers the theory of reflection and refraction of 11*tt on the surface of these media, The first three chapters contain well known resulteg but many of them are obtained by methods different from the ones employed in available vorks in theoretical optics. Along the same lines chapters 1., 11,, and 311 present a series of.new results concerning pol6rization., heterogeneous waves, total reflection, etc. The majority of results presented in chapters IV., V, sn& VI are said, to be original. Pertinent mathematical relations are found in paragraph 4 of chapter I., and paragraphs 16 and 20 of chapter 133. Card 116 Optics -of--Arxisotropie-Media----------o"0'3 Sow are also found throuatout chapters V and VI, Recognition is given to Professor Z.,I. Stepanoy for,his invaluable advice and observations and to Be Ve Bokutf for his help in reading the manuscripts and getting the book ready foi the printers. There are 210 references, 72 of Aich are Soviet, .104 Clemmt 25 English., 8 French imd 1 Svedish. TAZX OF CONTENTS: Fare rd 3 Cho Io Plane.Electromagmetic Waves 7 lo. Mamalfs equations and boundary conditions, The Law of Conservation of Znerg-. 7 2, Plane electromagnetic wav a 14 3, Polarization 23 4. Invariant form of relationships characterizing polarization 33 3* Addition of vaves with different polarization 46 6* Reflection and refroation of plane vayes 56 Card 2/6 (Ypties.of Anisotropic Media 66,4 Ch, II. Isotropic Media 62 7. Continuous plane waves in isotropic dielectrics 62 8. Heterogeneous plane waves in an isotropic dielectric 68 9. General solutions of Maxwell's equations for heterogeneous plane waves 78 10. Plans wav a in isotropic conducting media 03 3.1, Plane wave on the boundary of two isotropic media. Freenel's fbr=Llas 91 12. Light intensity and polwization in reflection and refraction 103 13, Total reflection 3-12 14, Total reflection at arbitrary polarization of incident waves. Reflection f conducting media 3.19 ch, III, Propagation of Plane Waves in TraMwent Normagnetie Crystals 129 15. Tensors of dielectric and sagnstie penetrability 129 3.6. Certain data fron linear algebra 135 17. Plans vaves in a nonmagnetie anisotropic dielectric. Equation of normals 141 18, Analysis of plane ways vectors in a crystal 145 19, Density and, flow of energy* Principle of reciprocity 151. 20, Invariant representations for tbree-dimansional. real synntrical, tensors 157 Card 3A Optics of Anisatropic Media 663 21* UnlWal crystals 263 22. Biwdal crystals 167 23. Optical surfaces 171 Ch. IV. Reflection and Refraction of Ught in Transparent Nomiagnetic crystals 24o Introduction 174 25. Oeneral statement of the problem 17 26, Reflection and refraction in unimdal crystals 179 27. Rotation of the plans of polarization in reflection, Angle of total polarization 1W 28. Reflection and transmission coefficients, Total reflection from uniWal crystals. 203 29., Buie vectors of reflection and refraction waves 209 30. BiWal crystals 221 31. Methods of determining optical parameters of transparent crystals 234 32a Determining paramters of unimdal crystals 237 33. Determining parameters of biwdel crystals 248 34, Small angles of incidence nethod applicable to biaxial crystals 259 Card 4/6 Optics of Aninotropic Media Cho Ve Propagation of LiSbt in Magnetic -Anisotropie Media 35o Buie equations for magnetic crystals 263 36o Equation of nozmls 265 3T. Flow of energy and the first principle of reciprocity 272 38. Binornals and birsdials 276 39. Uniazial magnstia crystals. Optical classification of savetie crystals 284 40. Invariant representations for tensors of uniwdal magnetic crystals 290 Cho VI, Absorbent Normwoetit Crystals 41. Introduction 300 42. General relationships 309 43, Absorbent crystals of average syngony 316 44, Absorbent crystals of poor syngony 320 45o General classification of absorbent 4;,,.-yatals according to optical properties, 330 46o Reflection of light from absorbent crystals of average ewwny and deteminatlon of their optical parameters 344 47. General rules for the reflection of 31&tt from crystals 350 48. Determining optical parameters of absorbent crystals of poor syngony according to reflection of ligbt 355 Card 5/6 0 Optics of Anizatrople Media 663 . Supplement to Chapter VI. 365 Bibliography 3T3 AVAILABIZ: Library of Congress Card 616 MKIM" 10-15-58 rSDINI?(%v Reflection and refraction of light In biaxlal crystals. Inzh.-fis.zhur. no,1:41-52 Ja 158. (MIRA 11:7) I.Institut fiziki i mtematiki AN BSSR, g.Minuk. (Crystallography) FEDOROV, Compogition of parameters of a rotation grrAip. Dokl.Ali BSSR 2 no.10:408-IPIP H 158. (HIRA, 12:8) (Gronpa. Theory of) AUTHOR: Fedorax.-YE.-I. SOV/r/0-3-1-8/26 TITIS: ---Invarialit Methods in the Optics of Transparent Non- magnetic Vrystals (Invariantnyye metody v optike prozrachnykh nemagnitnykh kristallov) PERIODICAL: Kristallografiya, 1958, Vol 3, Nr 1$ pp 49 - 56 (USSR) ABSTRACT: According to the electromagnetic theory of light, the optical properties of non-magnetic crystals are determined by the symmetric dielectric constant tonsor, e . Usually a special system of co-ordinates is used in the case of such crystals.so that this tensor assumes a diagonal form. However, in spite of the fact that it is widely used, this method is neither unique nor the best for solution. of problems in the optics of anisotropic media. Invariant vector-tensor methods which do not employ any special co-ord1nate systems have considerable advantages. The author has shown in Refs 1 and 2 that the latter methods may be used to develop a general theory of the optical properties of media having an arbitrary magnetic ahisotropy and absorption anisotropy. A particu- larly useful simplification of the theory is obtained Cardl/3 by the use of special invariant dyadic representations SOV/70-3-1-8/26 Invariant Methods in the Optics of Transparent Non-magnetic Crystals for 3-dimenaional tensors. The present work is concerned with the application of the methods developed in Ref 3 by the present author to some of the main problems in the optics of transparent non-magnetic crystals. The second section of the present paper (Section 1, is an introduction) is concerned with the definition of a "canonical" represen- tation of a tensor. Such a representation is defined by Zq (3). Section 3 treats uniaxial crystals. The "canonical" tensor representation is applied to ddrive -the usual properties of plane, monochromatic waves N - 1) in tri- tetra- and hexagonal crystals. Section 4 deals with bi1xial crystals and again the "canonical" represen- tation formalism is applied and among other things it is shown that the biradials of the crystal coincide with the axes of the dielectric constant tensor, or the binormals of a non-magnetie transparent crystal ire the axes of the inverse dielectric constant tensor e- . The final section deals with optical surfaces and it is shown that invariant methods may lead to the usual results in a much simpler way. In general, even in the case of the simpler Card2/3 problems in the optics of anisotropic media, there is no SOV/70-3-1-8/26 Invariant Methods in the Cptios of Transparent Non-magnetic Crystalb necessity to use any special system of axes since t!~e invariant approach is both more general and simpler. There are 5 Soviet references, 1 of which is a translation from German. ASSOCIATION: Institut fiziki i matematiki AN BSSR (Institute of Physics and Mathematics, Ac.Sc. Belorussian SSR) SUMITTED: Janua37 15, 1957 Card 3/3 AUTHOR: Fedorov, F.I. TITLE: On Certain e Light from Crystals yakh pri otrazhenii PERIODICAL: Kristallografija, 70-3-3-11/36 Regularities in the Reflection of (0 nekotorykh obshchikh zakonomernost- sveta ot kristallov) 1958, Vol 3, fir 3, PP 322 - 324 (USSR). ABSTRACT: It has been theoretically established that on the reflection of light from a crystal of any type (transparent, absorbing, magnetic, etc .) for every given di-ection of the wave normal of the incident wave, there exists a unique pair of mutually perpendicular directions of polarisation of the incident wave, to which correspond two mutually perpendicular directions of polarisation of the reflected wave. For these polarisation conditions, the coefficients of reflection assume the maximum and minimum values. It is assumed that the relations between D and E and B and H are linear. The results follow dire7ctly fro! an analysis oCMaxwell's equations. The reflected wave has a magnetic vector HI connected with the magnetic vector of the incident wave F by HI = R H (R being a matrix). R+ is the Hermitian-conjugate to R .The reflected energy is H'kH' and the coefficient of reflection Cardl/4-- 70-3-3-11/36 On Certain General Regularities in the Reflection of Light from Crystals 2 2 2 r / /E/ /H'/ HIR+RH = HI"TH where T-R+R = T+ is the Hermitian self-conjugate matrix. If / 2 is made 1 then r = HXTH - The task is to find the extrema of the Hermitian quadratic form r(H) = HATH with the supplementary condition H'*H=l . As is known the vectors H corresponding to the extrema correspond to vectors of the matrix T of the Hermitiali form. As these vectors H and HI are each determined by two complex components in corresponding phaseplanes, the matrix T then has two rows and two columns and consequently the two corresponding vectors Hl and H2 are determined by the conditions TH `~rlHi and TH2=r where r and r2 1, 2H2 1 denote the corresponding special values of the matrix T. From this it is deduced that HjJ~ ' = r 'H~ 2Hl'OH2 = 0 The following conclusions are drawn: 1) For l' ht falling from an isctropic medium (non- conductinIg5 onto an arbitrary medium for a given direction Card2/4 of the wave normal of the incident wave, there exists one 70--3-3-11/36 On Certain General Regularities in the Reflection of Light from Crystals and only one pair of magnetic ve,,-tors H1and H2 connected by HwA,"H' 2=O, which correspond to a pair of vectors for the reflected wave Hiani % which are connected by Hjm~' = 0 . 2) These vectors are eigen ve~.,toors of the Hermitian matrix T. 3~ They correspond to extrema of the reflection coefficient. 4 For the usual case of reflection from a transparent medium T and H, and H 2 are real. 5) If H, and H2 are non-linear then the maximm mi3ection will be obtained for elliptically polarised incident waves. 6~ For total reflection R 'must be a unitary matrix. 7 For reflection from isotropic media H1and H2' are linear and together with Hi and H~ , the incident ray and its perpendicular lie in a plane. Ca-rd3/4 There are 6 references, 3 of which we Soviet and 3 German. 70-7 11/36 ,On Certain General Regularities in the Reflectic from Crystals ,ASSOCIATION: Institut fiziki i matematiki AN BSSR .(Institute of Physics and Mathematics, AS BSW SUBMITTED: October 30, 1957 Card 4/4 SOV/r/0-3-5-9/24 AUTHORS: Goncharenko, A.M. and Fedorov, F.I. TITIS: The Surfaces of Refraction an ion in Absorbing Crystals (Poverkhnosti refraktsii i absorbtaii pogloshchayushchikh kristallov) PERIODICAL: Kristallografiya, 1958, Vol 3, Nr 51 PP 58?-592 (USSR) ABSTRACT: A theoretical ans sis is made of some of the properties of the surfaces representing the refractive index and absorption in absorbing crystals. Only the propagation of uniform waves is considered where wave and amplitude normals are parallel. The refractive index surface is defined by a radius vector R, of length proportional to the r.i. n, for the wave normal direction n - Hence, El - nl n and n. is the real part of the r.i.2 n - n, -in2, n2 being the absorption coefficient. The absorption surface is defined by E2 = n2 n . The task is to describe these two surfaces as functions of the wave normal n . The coeffici-ents in the expression: Card 1/3 SOV/70-3-5-9/24 The Surfaces of Refraction and Absorption in Absorbing Crystals 2 1/2 13~,2 nmn] 2 - a + b fne 11 [ne"I + Z-j have to be found. The parameters come from the reciprocal complex tensor for the dielectric susceptibility: v-1-1 - a + b(01.0" + 0".cl) . A graphical method for finding the directions of the extrema, in principal sections of both the r.i. and the absorption surfaces is explained. Zxplicit values for the parameters in the above equation are given in terms of thq real and imaginary parts of the r.i. andthe directions are given. There are 2 figures and 4 references, 3 of which are Soviet and 1 German. Card 2/3 SOV/70-3-5-9/24 The Surfaces of Refraction and Absorption in Absorbing Crystals ASSOCIATION: Institut fiziki i matematiki AN BSSR (Institute of Physics and Mathemtics of the Ac,Sc. Belorussian SSR) SIMMITTBD; March 17, 1958 Card 3/3 AJThO1W: .51-A -1-20/26 Fadorov, F. 1. and Tomillchik, L. 1.i. xial the Optical properit;ies of Bia. On ~the ' ~naorY~ of I Elaonctic Crystals, (K teorii opticheskilul --voys'uv dvuosiiylch magnitnykh kristallov.) Optiltu i Spelctroskopiya, 1958, Vol. IV, IxTr. 1, pp. 109-112. (USSR) Er. 1. Fodorov (Refs. 1-4) developed a theory of the optical prope rties of ma~;netic crystals in an in~,rariaat form. From this theory lie deduces the m-An lavis of propaGation of liE;ht in magnetic crystals of all synL,,onies. In the case of biaxial crystals the problem was complicated by the presence of two nop--- commutins tensors c and ~L. The theory can be considerablZr simplified by usine a special "canonical" dyadic representation of tensors. In Ref.5 such a representation of the symmetric tenser c mas applied to the case of transparent non-mab-notic cry~~,tals. In PI~RIUDNAI.b: A 13 62 RA G T Card 1/2 1 - A -3. - 2 021-6 a rT-, r; t i c On tho 'cory of tile Optic 1 P--op xtiez ol Biaxial L the case of maLrgietic biaxial crystals, the optical properties depend greatly on the non-syuunetric tensor ~. = V.-lp -A canonical dyadic repro sentation for t'he latter tonsor was obtained in Ref.6. The present (oatirely thoorotical) paper gives the main optical relationships for transparent magnetic biaydal crystals. There aiy-. 6 reforen,ces, all of which are Russian. ASSO%JJ1.k2IO1T; Belorussian 0-itate University imeni V.I. I-enin. (&-lorusskly .-Osudarstvennyy universitet im. V.I. Lenina. ) SL1M1-.OZjD-- April 17, 1957. AVAIIAB14;: Library of Congress. Card 2/2 1. Hognetic crystals-Biaxial-Optical properties 51-1- 4 -3-13/30 AUTHORS: Sotakiy, B.A., and ~dorov, F-L& TITIA,j: Molecular Theory of Reflection and Refraction of Light. I. LiOat Incident from Vacuum on-to an Isotropic Medium. (K molelollyaln-loy teori-i otrazheni a i prelomieniya ly sNeta. 1. Padeniye S--reta iz zakirina na izotropnuyu sredu . ) EBRIODICAL: Optika i Spektroskopiya, 1956, Vol-IV, Ur-3, PP. 365-372 (USSR). ABSTRACT: Molecular theoi-j of propagation and no-fraction of light in it-otropic Laedia was developed by Eviald, Esmarch, Oseen, Landblad and othera This theory Is based an the followixiE; as-amptions. Under the action of an electromagnetic wave, inoident frou vacuuLt onto the aesdium, moleculaz dipoles are ex-,it-ed into a state of degr-i:erate vibrationo-, and emit 6econdary waves. Both the incident und secondary waves obey 111amjelllc equations for --,,a,.~uucj. -SUporpositior', cT all the z-Eicondary waves and of the 14'ricident, wave the xefracted gaVe 4nsdde the, and 1-he ::,~~,flected wave outsLde it. This mr.-Iccular t1aeory hac a number Card 113 of fallits of , !1- 4 .3-13/30 J Molecular Thoory of Rof I rj,.t L olrt an d 14).Crar;l, ioc- r, f IA~~it . L . formulae for the L;enerai case of obligae incAdence are obtained, only in approximate form by using, tile method of Oseen and Lundblad (Ref.10--12). In none of the papers on the molecular theory of reflection and refraction is the case of total reflei:~tion of light dealt with. The present paper is an attempt to develop a more complete and exact -molecular theory of reflection and refraction, including in particular the case of total reflection. All the main relationships (such as the relationship between the refractive index and polarizability the quenching theoi-j of Oseen, Fresnel's formulae~ are obtained exac;tly and in a comparatively simple way. The present authors also generalize Oseen's theory to tile case of non-horAogeneous waves. The paper is entirely theoretical. There are 2 figures and 21 references, of which- 14 are German, 4 Soviet, 2 English and I a translation of Born's "Optics" into Rl-ssian. ASSODIAIMIT; Belorussian State University (Belorzsskiy Card 2/3 gosudarstvennyy uni:versitet.) 51.- 4 -3-13130 Molecular Theox-j of Reflection and Refraction of Light. T. SUBLITTED: May 4, 1957. - ~ 1. Light-Reflection-Theory 2. Light-ROTaction-Theary 3. Ligh+,-P"Pipticm-Thavry Card 3/3 5 Oil5l -.-1 -1 - 10/19 AUTHORSs Sotskiy, BA. and Fodorov, F.I. TITLE t On the Molecular Theory of Reflection and Refra-z-Lllon of Light- ~K moloicalyarnoy toorii otrazheniya I prolomleniya svota) II. Light Incident on the Boundary Between an Isotroplu, Medium and Vacuum or Another Isotropic Medium. Total Refle-Aicin. (II. Padeniye eveta. na granitau izotropnoy sred a valmunitga III a druGoy itotropnoy srodoy. Polnoye otrazheniye~ PERIODIGALs Optika I Spektroalcopiya, 1958, Vol 5, Hr 1, pp 57-C5 (USSR) ABSTROT; In the preceding part of this work (Ref 1) the authcrs considered the came of an Infinite plane monochromatic electronugnotic wave incident from vacuum on to an isotropic medium. The present paper gives the molecular theory of reflection and refraction of light at the boundary of two media, of which the first consists of molecular dipole& and the second is vacuum or consists of dipoles of another typo. The molecular theory of total refleetvion is givea. Card 1/2 It is found that, under certain conditions, the vacim vavo -which SOV161-5-1-10,1,19 On the Molecular Theory of Reflection and Refraction of Light - II - Light Incident on the Boundary Between an Isotropic Medium and Vacuum or Another Isotropic Medium. Total Reflection. appears as the result of superposition of primary waves produced by vibrations of dipoles, may be damped in spite of the fact that the dipole vibrations are undamped. This Is the converse of the =so discussed in Part I (Rof 1) where a damped dipolo wave produced an undamped vacwam viave. There are 3 figures and 5 referen.-as, 2 of rhich are Soviet, 1 translation of a Western work into Ruasian, 1 German and 1 English. ASSOGIATIONs Belorusskiy gasudarstvannyy universitet ( Belorussian State University) SUELITTED Attgast 15, 1957 Card 2/2 1. Light - Reflection 2. Light - Refraction 3. Light - 1461scular theory ii C, R Fadorov, F 3 011/51 -5-3 -17/ 21 TITLY.t Optics of Absorbing Crystals. (Optika pogloshcha,~ushchikh kristallov). III. Crystals of Lower Syngonies. Optical Axes kIII- Kristally nizshikh singoniy. Opticheskiya oul). FERIODICALs OptikM i Spektrookopiya, 1958, Vol 5, Nr 3, pp 322-3,',3 kUSSH) AM TRAC T s In eariier parts (Refs 1,2) the autJ-.or established an invariant form of general relationanips for propagation or plane monocnromatic waves in absorbing crystals and discussed the case of crys+Als of medium r,yr.:,0nio5- ',"he prajent pupar deals with the optical properties of cryatals of lower syngonles using a canonical lLvariaut reprasenzUtioa of the reciprocal complex tensor of partaitdvity. Gan,3ral expressions are obrAined for polarization of plane viuvos in crystals of loNer syngonioa with canplex. rafractiva indices for uniform vmves. A Card 1/2 SOV/51-5-3-17/21 Optics- of Absorbing Crystalu. III. Urystald of Lo.-;er :;~mgoniaj- Optical A7.3a. 0 - general expression Is found for the apocial 31rections -,ihich have a aingle value of tha rafractive indeam. The puper is antir3ly theoretical. There are 2 figuras, 1 appendix and 19 references, 14 of whicn are Soviet, into Ru3sia:a. iWSO~XLTIONsInqtltut fizIkI j lzato:aAtiki, XT B3JR (Instituts of Piysics and Mathawatics, Academy of Sciences of th, Belorussian SSR) ~;UBIJTTEDi October 28, 1957' 1. Crystals--Optical properties 2. Cryutals--Theory AUTHOR s Fedorov, F.I. TITLE optics of Absorbing Crystals (Optika pogloshchayushchikh kristallov). IV. Classification (IV. Klass Ifilcatsiya) PMUODICAL i Optika I Spektroskoplya, 1958, Vol 5, Nr 4, pp 450-461 (USSR) LBSTR&CT% The author discusses all possible types of absorbing crystals of lower apganies, frota the point of view of the number and nature of the optical axes. It is shown that isotropic optical axes may be present in such crystals. In contrast. to transparent crystals the cptical properties of absorbing crystals of rhowbic, monoclinic and triclinic syngonies differ essentially between each syngony. The -total nnber of various types of absorbing crystals roaches 16, instead of 3 according to' Voigt--Drudeve theory. Octaplate classification 0~ absorbing i~on-active non-magnetic crystals according to their -SOV/51-5-4-14/Zl Optics of Absorbing Crystals. IV, Classification. optical pioperties is given. The.paper is entirely theoretioal. Thera are 9 references, 7 of which are Soviet and 2 German. ASSOCIATION tInstitut I itiki I matematik:i, AN SSSR (Institute of Physics and Mathematti s . Academy of Science of the U.S.S.R.) SUEMMD% October 21 , 1957. 1. Crysta3s--Optieal properties 2. Crystals--Classification Card 2/2 3. Crystal3--Theory AUTHORS s Tomillchi1c, L.M. and Fedorov, F.I* SOV/51-5--t-15/21 TITLE. Optics of Absorbing gnetic Grystals. (Optiks. pogloshchayushchikh magnitnykh kristallov). I. Polarization of Uniform Plane T(Aves (I. Folyarizatsiya odnorodnykh plookikh voin). MRIODICAL; Optilm i Spektrookoplya, 1958, Vol 5, Wr 4, pp 462-468 (USSR) ABSTRACT. Applicution of invariant methods (Refs 1-8) simplifies considerably the theory of the optical properties of absorbing crystals. Such a theory is, however, incomplete without allowing for the magnetic properties of crystals. Although 1A transparent bodies the magnetic susceptibility is negligibly small, it may reach conparatively large values in absorbing crystals. Thus crystalline hydrates of organic and inorganic salts of rare earths and of metals of the iron group (Fe, Ni, Go) are strongly param gnatic (ILdiffers frou 1 in the third decimal place) and exhibit strong magnetic anisotropy (20% of the absolute value of magnetic susceptibility). There are also Many organic and inorganic diamagnetic crystals in uhichii differs from I only in the fourth or even sixth decimal place but vhich are nevertheless strongly anisotroplo, e.g. graphite. In such substances the magnetic susceptibility and its anisotropy are of the same order as the Card 1/2 anisotropy of the permittivity tensor F_. The authors deal 'with 'Optics of Absorbing Magnetic crystals. I. Polarization of Uniform Plane Waves. polarization of plane uniform electromagnetic waves propagated in a non-active medium-with an arbitrary anisotropy of the dielectric, magnetic and conducting properties. The discussion is given in a general invariant form. The folloning results are obtained. (1) The most general case of polarization in absorbing orystals is elliptical polarization and the polarization ellipses of the transversefield vectors D! and B are pot similar and are not Lautually orthogonal. (2) Elliptically polarized vqves v4th similar and Identically distributed ellipses of transverse vectors of induction are propagated along optical axes. (3) circular polarization to possible only for maves propagated along optical axes, and then only in crystals %hose parameters obey an additioMl.special relationship involving the permittivity and parmeability vectors. (4) Linear polarization of one of the transverse vectors produces linear polarization of the Ga rd 2/2 other vector. The paper is entirely theoretical. There are 15 references 8 of which are Soviet, 5 Englishand 2 translations, AS-30CLITIONsBalorusakly gosudaretvannyy universitat im. V.I.Lenina (1~rolorussian State University Dneni V.I. Lenin) 1. Crystals-Magnetic factors SUBLUTTSDs October 29, 1957 2. Electromagnetic waves-Polorization ME MTHORS s Torall'ohik, L.M. and Fodorov, F.I. SOV151-5-5-15123 TITLE: Optics of Absorbing YLagnetic Crystals. (Optillca pogloshchayushchikh magnitnykh lcristallov). II. Field Vectors for Plane 7.,Tavos. Refractive Indices and Optical Axes. (11. Vaktory polya ploskikh voln. Polmuitali prolomleniya I opticheskiye osi) PSUWICAL: Optika i Spektrookoplya, 1958, Vol 5, Yr 5. r-p 601-605, (USSR~' I A,~ TRU T In Part I (Rat 1) it was shown that the difforance between the equations for plans electromagnetic waves in absorbing r4arnotic crystals and the corresponding equations for transparent vagnetic crystals can be reduced to replacement of the real permittivity tensorE by a complex tensor el . Following Refs 2, 3 it is concluded that optical properties of abaorbin6,uagnetic crystals should be determined primarily by the tensor Ir = (FIJ-1 I'll The I I tensor Is in general couplex and asymmetric, bat it may be made symetrical using the real sy=otric permeability Card 1/2 SOV151-5-5-15123 Optics of Absorbing Magnetic Crystals. II. Field Vectors for Plane 1aves Refractive Indices and Optical Axe&. tensor p- Using a canonical dyad representation for the tensor the authors obtained general Invariant expressions which give complex refractive indices and polarization of plans uniform monachromtic -waves, as wall as the directions of optical axes. The paper Is entirely theoretical. There are 8 Soviet references. SUBLaTTED: December 3, 1957, 1. Magnetic crystals--Optical properties 2. Electromagnetic waves Card 2/2 --Analysis 24 (5) AUTHOR: TITLE: PERIODICAL: ABSTRACT: Card 1/2 Fedorov, F. I. SOV/56-35-2-25/60 Projective Operators in the Theory of Elementary Particles (Proyektivnyye operatory v teorii elementarnykh chastits) Zhurnal eksperimentallnoy i teoreticheskoy fizikip 1958, vol 359 Nr 2, pp 493-500 (USSR) By means of the minimal polynomials of the matrices of the relativistic wave-equation and the apin-matrices projective matrices are written down; dyadee are concerned here by means of which every possible particle-state can be described in the case of any spin. The physical fundamental quantities (energy-momentum, current-charge, transition probability) can be represented immediately by means of these projective operatorsp viz. in an invariant manner (independent of the manner of representation). The calculation of various effects for particlea with spin can be reduced to the evaluation of the traces of definite combinations of matrices. In application of the method described the general conditions for the definiteness of energy and charge for Projeotivo Operators in the Theory of SOV/56-35-2-25/60 Elementary particles particles of the same mass are derived. Furthermorep a derivation of the commutation relations for particles with any spin is given. It is shown that the two formulae a V f (2)),Zpk 2k m A -'� "2k' 2k 1 "2k' 2k (x/X22po can be used also for the purpose of dealing with all sorts of other problems in which the spin of particles plays an important part. There are 9 references, 8 of which are Soviet. ASSOCIATION: Institut fiziki i matematiki Akademii nauk Belorueskoy SSR (Institute of Physics and MathematiesiAS Belorussian SSR) SUBMITTED: March 269 1958 Card 2/2 "? Y. V 00 6,%V/58-59-7-16463 Translation from: Referativnyy Zhurnal Fizika, 1959, Nr 7, p 257 (USSR) AUTHOR: Fedorov, F.I. % X TITLE: Reflection and Refraction of Li&h Iin Transparent Uniaxial Crystal PERIODICAL: Uch. -zap. Belorussk.-un-t. 1958, Nr 41, pp 219 - 230 ABSTRACT: Using the invariance method, the author solved 'the problem of the reflection and refraction of light in unbounded transparent uniaxial crystals in the case of arbitrary orientation of the optical axis, division plane, and plane of incidence. The resulting formulae for detem.ining the amplitudes of the waves reflected and refracted on a uniaxial crystal have the same value as the Fresnel formulae for Iso- tropic media. The following particular cases are examined: a) the optical axis is parallel to the division plane, b) the optical axis is perpendicular to the division plane, c) the optical axis Is ar- bitrarily oriented relative to the division plane but parall *el to the plane of incidence, and d) the normal incidence of light. Card 1/1 B.V. Bokut' TOMILICHIII, L.M.-,-F=R()V, F.I. Optical characteristics of absorptive magnetic crystals with average and rhombic eyngony. Trudy Inst.fis.i mt. All BSSR no.3:142-151 159. OURIL 13:4) (Crystals--Optical properties) MOROZ, L. G. ; rAWROV, F. L Wave functions of an electromagnetic field in a vacuna. Trudy Inst.fiz.1 mat.AV BSSR no.1:154-166 '59. (KRA 13:4) (Wave mechanics) (Blectromagnatic waves) SOV/70-4-4-6/34 AUTHORS: Tomillchik, L.M. and Fedorov, F TITLE: Magnetic Anisotropy as a Metric Property of Space PERIODICAL: Kristallografiya, 1959, Vol 4, Nr 4, pp 498-504 (USSR) ABSTRACT: It is shown that the theory of the optical properties of homogeneous magnetic crystals can be derived from the corresponding theory for non-magnetic crystals by intro- ducing a metric, the metric tensor g being determined by the magnetic permeability tensor ji . A covariant tensor A in denoted by A and a contravariant tensor by 2: . (0-1 = I . g converts from a space with an orthogonal Euclidean metric to a space with some other metric. In Maxwellts equations E Is a covarlant vector and B a contravariant pseudovector. As V = 1/81T (ED + 1W) is scalar, 5 is a contravariant vector and R a covariant pseudovector. The refraction m Is a covarlant vector. In this notation these quantities are denoted by Cardl/3 0 SOV/70-4-2-6/34 Magnetic Anisotropy an a Metric Property of pace The dielectric and magnelic iermeabilities are doubly contravariant.tonsors III * A marks a pseudo- vector. For non-magnetic crystalsw Maxwell's equations and the equation for a plane wave take the form: I R Lis B, a For a magnetic crystal: A 4 n A ITY 0 L*6j These quantities are.transformed by the metric tensor as: A A r-.,t t% - k R [;Kj I B H I k~MEJ ~7g ~ 0 \[Tg~ The sets of equations for the two cases can be made to Card2/3 coincide if SOV/-78-4-4-6/34 Magnetic Anisotropy as a Metric Property of pace IL -T IL or and IL 0. This statement is poved and two examples are given. There are 9 Soviet references. ASSOCIATION: Institut -f&:bik:L i mat*matikI AN BSSR (Inditute of Physics and Mathematics of the Ac.Sc., Byelorussian SSR) SUBMITTED: March 22, 1959 Card 3/3 I SOV/51-ti-1-14/30 AUM-10R. Fedorov, F.I. - .11~ TI7L,E.- Tha,~ry -,f the Opft~-%2 A:-ti-r-Ity of Cryytala. (K t,3orii optichaskoy a"Ivr.o.M. &iutall-c7). I -, 11-ka Law -~Jr Conzarvation of Bnergy and Opti~sl A,Aivity Temqcrz (I. Zakaa soUiraneniya energii i tenzory akt1,,tc!xtt) PERIODICAL: Optik-a 1 5pAtraF.L,.*riya, 11c.-1 E. Nr 1, p? 83-03 (USSR) ABSTRACT; Thio raprat sri-7as a tntory of t4i,~ optical activity of cryetalu in an invarl-&-it fv= .vhirh -is ln4apendvat of zoordinatox. Starting from the assumption of Jzdapsndenco of the electric and m9gneti,~, in4m,.-tion vosctorx D anl A of -che gradienta of the corresponding flold4 t:ia autbor applien the law d r-=zarvatiot of energy to obtain the baf:i-! ralatlounhip of B-arnIc moleralar theory of the opticaily a,itlve -.!rystrilc. It was found thitt the 'rector of the energy flow density in the optically aA1-T6 media ditforis from the u,3,--al Umov--Foynting vector P Thir rector 1,T nc, given by 'S 0 P + ^41 / ulti where it. pare transposezef third-rank teasors d., 15, called electric and ma~paetl~ ft;,~ttvlty tanaorc. The author obtains invariant expressions Card 1/2 4/aO Theory of the Optical Aebirity of Oryai,.Alu 4_,ii of Conservation of~ Energy and Optical Activity Tensors. for the activity tonsort cL and 19 of all classes of the optically active crystals. Of the 32 z1asses of crystals the activtty tensors become zero for all cantrai. and plamaxial classes (there are 11 of them) which possoss Inversicn o~metry. Also both inversion classes of hexagonal syngony (with sixth-order Inversion axis) and the planar class of -.ubic ayugony have zero activity tonsor4. Only the remaining classes of crystal symetry may exhibit optical activity. The paper is entirely theoretical. There are 10 references, 7 of which are Sooit, 1 French, I Gaman and I translation. SUBMITTED: March 15, 19SP Card 2/2 AUTHOR: Fedorov, F.I. SOV/51-6-3-15/28 TITLE: On the Theory of Optical Activity of Crystals. 11 Crystals of Cubic Syngony and Planar Classes of Middle Syngoniea (K teorii opticheskoy aktivnosti kristallov. II Krialally kubicheskoy aingonii i planallnykh klassov srednikh aingonly) PERIODICAL: Optika i Spektroakopi-ya, 1959, Vol 6, Nr 3, pp 377-383 (USBR) ABS~TRACT: The author showed that Maxwell's equations together with constitutive equations far plane waves in optically active media have.the following form; - cng ], (1) CIA 1, (2) + + (4) where m A is the refraction vector, k /0 is the wave number in vacuum and ~cc, 0 are the electric and Card 1/3 magnetic activity tensors respectively. Using EqB.(I)-(4) SOV/61-6-3-10/28 On the Theory of Optical Activity of Crystals. II Crystals of Oubie Syngony and Planar Classes-of Middle Syngoniea the author studied propagation of light in anisotropio media with the highest symmetry, i.e. in crystals of cubic syngony and planar classes of middle syngonies. As in the preceding paper (Ref.1), invariant treatment was employed. The author found that in planar classes of middle syngoniea there is no rotation of the plans of polarization on propagation of light along the optical axes. Neverthelesaproperties of such crystals differ essentially from properties of optically inactive crystals, since the light reflected at such crystals is elliptically polarized. The author points out that optically active .substances do not necessarily exhibit the property of rotation of the plane of polarisation. He proposes that a medium should be called optically active if its constitutive equations have the form -0 4 -J, D = eB + (0CVj' E]J' B = JAH + [,6q, HI (45) Card 2/3 F-,03~ :~- plane waves these equations have the form given by sov/51-6-3-15/28 On the Theory of Optical Activity of Crystals. II Crystals Of Cubic Syngony and Planar Classes of Middle Syngonies Eq.( 3) -Eq.( 4) with, & and P not equal to zero. From this definition it follows that a medium which rotates the plans of polariaation for one or more directions of propa- gation of light is necessarily an optically active medium, ,.but, in general, the reverse is not true. The paper is entirely theoretical. There are 8 references, of which 6 are Soviet, I translation from German into Russian and 1 German. SUBMITTED: February 15, 1958 Card 3/3 24(4), 24(2) SO'1/51-6-4-21/29 AUTHORS t Bokut', B.V. and Fedorov, Fa. TI TIZ: On the Theory of the Optical Activity of Crystals. (K toorii oDticheskoy aktivnooti kristallov). III. 'the General Equation of Normals (III. Obshcheye uravneniyo normaley)" FERIODICALs Optika i Spektroskoplya, 1959, Vol 6. Nr 4, pp 537-541 (USSR) ABSTRACTt In the earlier part3 of this work (Refs 1, 2) the author developed an invariant phenomenological theory on the optical activity of crystals of all types of sy=etry. The present paper deals with the general ec,pation. of normals for the optically active crystals when magnetic effects are allowed for. 'rho theory shows that three types of waves are possible in the optically active crystals, and the phase velocity of the tbird Tave should be very small ccmpared with the velocity of light. The paper is entirely theoretical. There are 6 references. 5 of which are Soviet and 1 translation from German into Russian. SUMffTTZD,- March 15, 1958 ca rd 1/1 SO'1/51-7-4-20/32 AUTHORSs Bokat', B.V. and Fedorov, F.I. ------------ TITMz Propagation of Light in Absorbing Magnetic Active Isotropic Media and Cubic Crystals FMODICALs Optika I spektroskopiya, 1969, Vol 7, Wr %, pp 558-561 (USSR) AM TROT s The authors discuss propagation of plane electromagnetic waves in an optically isotropic medium, possessing optical absorption, optical activity and magnetic properties.. It in shown that when the magnetic tems of the optical activity are taken into account, circular dichroism should occur. The paper is entirely theoretical. There are 8 references, 6 of which are Soviet and 2 translations. SUBMITTFjD: March 23, 1959 Ca-rd 1/1 LOBKO, S.I.; ;$ Spin 1/2 - 312 particle In a homogeneous magnetic field, Dokl.AM BSSR 4 no. 5:194-198 My 160. (HIRA 13:10) 1. Beloruashy gosudaretvanVy univereitat im. Y.I.Imnina. (Particles (Unclear physics))