ferrimagnetic structure of mn2co2c

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ii ABSTRACTS OF PAPERS TO APPEAR IN J. PHYS. CHEM. SOLIDS Vol.6, No.12 Fe 1~ phase has been carried out in the tempera- nearest neighbor sites of ~0. 035 eV accounts ture range 700- 1350°C using solid state electro- well for the experimentally observed quantities. chemical techniques. The results confirm the The configurational entropy is an appreciable presence of three wustite regions separated by fraction (~10% at 300° K) of the total entropy order - disorder transitions. Partial molar en- content. thalpies and entropies of solution of oxygen in. Fe1_~Oare reported. (Received 4 September 1968) (Received 29 April 1968) (Revised 18 September 1968) 7. OPTICAL CONDUCTWITY IN ALKALI METALS H. B~1ttner and E. Gerlach (Battelle- 5. MAGNETO-ACOUSTIC INVESTIGATION Institut e. V., Frankfurt am Main, OF THE FERMI SURFACE AND SPIN Germany) SPLITTING OF THE LANDAU LEVELS IN p-TYPE AND n-TYPE PbTe It is shown that the Mayer Naby peak in \V. Schllz (Philips Zentrallaboratorium the optical conductivity of alkali metals arises Hamburg, Hamburg 54, Vogt-Kollnstr.30) from transitions from the Fermi sea to the Brillouin zone boundaries. Quantum oscillations of the magneto- acoustic attenuation have been measured in p-type (Received 29 May 1968) and n-type samples of lead telluride. From the (Revised 14 August 1968) periods of these oscillations, measured as a function of the angle ~ between the direction of magnetic field and the [100] axis of the crystal, 8. STRUCTURAL AND MAGNETIC PRO- the shape of the Fermi surface has been investi- PERTIES OF NON-STOICHIOMETRIC gated as a function of the carrier concentration. PRASEO-DYMIUM MONOPHOSPHIDE A strong non-ellipsoidal behavior was observed Enrico Franceschi and Giorglo L. Olcese for both p-type and n-type material. Furthermore, (Istituto di Chimica fisica, Universita’ spin splitting of the Landau levels was measured. di Genova, Genova, Italy) The splitting was found to be around ~ the Landau- level spacing and decreases slightly with decrea- An investigation on the occurrence of non- sing carrier concentration. stoichiometry in solid praseodymium monophos- phide was carried out by evaluating the variation (Received 14 August 1968) of the lattice constant and density with the corn- (Revised 17 September 1968) position. A range of solid solution by vacancies in the phosphorus sub-lattice was found between the compositions corresponding to PrP and 6. ON THE THERMODYNAMIC PROPER- PrPO.B5 phases. Magnetic properties and their TIES OF THE SOLID ELECTROLYTE dependence on non-stoichiornetry were deter- RbAg4I5 mined in the temperature range 4.2°- 500°K: for H. Wiedersich and W.V. Johnston the quasi-stoichiometric phases there is no evi- (Science Center, North Americal Rock- dence of magnetic ordering and a superconducting well Corporation, Thousand Oaks, transition seems to occur below 7°K, while an California 91360, U. S. A.) antiferromagnetic coupling of praseodymium ions becomes possible when the interionic distances The non-random distribution of Ag~ions decrease by introduction of vacancies in the phos- on three crystallographically nonequivalent sets phorus sub-lattice. of tetrahedral sites in RbAg4I5 is a consequence of both site energy differences and mutual repul- (Received 5 August 1968) sion of silver ions on nearest neighbor sites. A (Revised 13 September 1968) method similar to the quasicheniical approxima- tion, used in the theory of order-disorder trans- formations, has been applied to obtain the con- 9. FERRIMAGNETIC STRUCTURE OF figurational entropy and excess specific heat Mn2Co2C associated with the disorder of the silver ions. N. S. Satya Murthy, R. J. Begum, C. S. Site energy differences of —~0. 027 and ‘~0. 042 eV Somanathan, B. S. Srinivasan and between the different types of silver sites and a M. R. L. N. Murthy (Bhabha Atomic Re- mutual repulsion energy between silver ions on Search Centre, Trombay, Bombay 74, India)

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ii ABSTRACTS OF PAPERSTO APPEAR IN J. PHYS. CHEM. SOLIDS Vol.6, No.12

Fe1~phasehasbeencarriedout in the tempera- nearestneighborsitesof ~0. 035 eV accountsture range700-1350°Cusingsolid stateelectro- well for the experimentallyobservedquantities.chemicaltechniques. The resultsconfirm the Theconfigurationalentropy is an appreciablepresenceof threewustiteregionsseparatedby fraction (~10%at 300°K) of the total entropyorder- disordertransitions. Partial molar en- content.thalpiesandentropiesof solutionof oxygen in.Fe1_~Oare reported. (Received4 September1968)

(Received29 April 1968)(Revised18 September1968) 7. OPTICAL CONDUCTWITY IN ALKALI

METALSH. B~1ttnerandE. Gerlach(Battelle-

5. MAGNETO-ACOUSTIC INVESTIGATION Institut e.V., FrankfurtamMain,OF THE FERMI SURFACE AND SPIN Germany)SPLITTING OF THE LANDAU LEVELSIN p-TYPE AND n-TYPE PbTe It is shownthat the Mayer Naby peakin\V. Schllz (Philips Zentrallaboratorium the optical conductivity of alkali metalsarisesHamburg, Hamburg54, Vogt-Kollnstr.30) from transitionsfrom the Fermi seato the

Brillouin zoneboundaries.Quantumoscillationsof the magneto-

acousticattenuationhavebeenmeasuredin p-type (Received29 May 1968)and n-type samplesof leadtelluride. Fromthe (Revised14 August 1968)periodsof theseoscillations, measuredas afunction of theangle ~ betweenthe direction ofmagneticfield andthe [100] axis of the crystal, 8. STRUCTURAL AND MAGNETIC PRO-the shapeof the Fermi surfacehasbeeninvesti- PERTIESOF NON-STOICHIOMETRICgatedasa function of the carrier concentration. PRASEO-DYMIUM MONOPHOSPHIDEA strongnon-ellipsoidalbehaviorwas observed Enrico FranceschiandGiorglo L. Olcesefor bothp-typeandn-type material. Furthermore, (Istituto di Chimicafisica, Universita’spin splitting of the Landaulevels wasmeasured. di Genova,Genova,Italy)The splitting wasfound to be around~ the Landau-level spacinganddecreasesslightly with decrea- An investigationon the occurrenceof non-sing carrier concentration. stoichiometryin solid praseodymiummonophos-

phide wascarriedout by evaluatingthe variation(Received14 August1968) of the lattice constantanddensitywith the corn-(Revised17 September1968) position. A rangeof solid solutionby vacancies

in thephosphorussub-latticewasfoundbetweenthe compositionscorrespondingto PrPand

6. ON THE THERMODYNAMIC PROPER- PrPO.B5 phases. MagneticpropertiesandtheirTIES OF THE SOLID ELECTROLYTE dependenceon non-stoichiornetryweredeter-RbAg4I5 mined in thetemperaturerange4.2°- 500°K:forH. Wiedersichand W.V. Johnston the quasi-stoichiometricphasesthere is no evi-(ScienceCenter, North Americal Rock- denceof magneticorderinganda superconductingwell Corporation,ThousandOaks, transitionseemsto occur below 7°K,while anCalifornia 91360, U. S.A.) antiferromagneticcouplingof praseodymiumions

becomespossiblewhenthe interionic distancesThenon-randomdistribution of Ag~ions decreaseby introductionof vacanciesin the phos-

on threecrystallographicallynonequivalentsets phorussub-lattice.of tetrahedralsites in RbAg4I5 is a consequenceof bothsiteenergydifferencesandmutualrepul- (Received5 August 1968)sion of silver ions on nearestneighborsites. A (Revised13 September1968)methodsimilar to the quasicheniicalapproxima-tion, usedin the theoryof order-disordertrans-formations, hasbeenappliedto obtainthe con- 9. FERRIMAGNETIC STRUCTURE OFfigurationalentropyandexcessspecific heat Mn2Co2Cassociatedwith the disorderof the silver ions. N. S. SatyaMurthy, R. J. Begum, C. S.Site energydifferencesof —~0.027 and ‘~0.042 eV Somanathan,B. S. Srinivasanandbetweenthe different typesof silver sitesanda M. R. L. N. Murthy (BhabhaAtomic Re-mutual repulsionenergybetweensilver ions on SearchCentre, Trombay, Bombay74,India)

Vol. 6, No. 12 ABSTRACTS OF PAPERSTO APPEAR IN J. PHYS. CHEM. SOLIDS

The carbideMn2Co2C hasbeenfound valuesfor the momentsare:4.0~Bfor the cor-

to be ferrimagneticwith aNéel temperatureof ner Mn atom, 3. 36 ~B for the facecentreMn535°C by meansof neutrondiffraction. It hasa and1.24 ~B for eachCo atom. The smaller mo-cubic unit cell with an Mn atom at the cubecar- mentsof the facecentreatomsarisefrom thenerandthe carbonatom at the bodycentre. The Influenceof thecarbonatom. Polarizedneutronsfacecentresitesare takenup by theother Mn and were usedto chooseastructurehavingcubicsyrn-the two Co atomsin a statisticalmanner. The metry overoneof tetragonalsymmetry.Mn momentsare alignedantiparallelto eachotherwhile the two Co momentsare parallelto (Received20 August1968)the cornerMn moment. Themostreasonable