A. Parisini, P. P. Lottici, C. Razzetti, R. Bacewicz
{"title":"Resonance Effects in the Raman Spectrum of CdGa2Se4","authors":"A. Parisini, P. P. Lottici, C. Razzetti, R. Bacewicz","doi":"10.1002/PSSB.2221340110","DOIUrl":"https://doi.org/10.1002/PSSB.2221340110","url":null,"abstract":"Resonance effects are observed in the Raman cross-section of the defect chalcopyrite CdGa2Se4. The results indicate a strong resonance of the highest frequency E(LO) sphalerite-like phonons in forbidden geometry, similar to the behaviour observed for zincblende-like crystals. The forbidden scattering may be described through a Prohlich intraband mechanism at the fundamental direct gap.Nous presentons les effets de la resonance sur la section efficace de la diffusion Raman de la chalcopyrite defectueuse CdGa2Se4. Les resultats montrent une forte resonance des phonons E(LO) les plus eleves en frequence dans une geometrie interdite. Cette resonance est comparable a celle observee dans les cristaux du type zinc-blende. La diffusion interdite peut ětre decrite par un processus d.'interaction de type Frohlich, avec I'energie fondamentale du gap direct.","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"29 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"89766472","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Capture of Majority Carriers by a Semiconductor Surface","authors":"R. A. Vardanyan, L. B. Khovakimyan","doi":"10.1002/PSSB.2221340138","DOIUrl":"https://doi.org/10.1002/PSSB.2221340138","url":null,"abstract":"The coefficient of majority carrier capture by a semiconductor surface is calculated in quasi-classical approximation. The carrier localization on the surface is accompanied by multiquantum fluctuational phonon emission. The temperature dependence of the capture coefficient is obtained. \u0000 \u0000 \u0000 \u0000[Russian Text Ignored].","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"35 8 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82802177","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Dislocation Core Models and Their Positron Annihilation Effects","authors":"J. Shen, C. Lung, K. L. Wang","doi":"10.1002/PSSB.2221340112","DOIUrl":"https://doi.org/10.1002/PSSB.2221340112","url":null,"abstract":"Positron annihilation parameters with three simplified dislocation core models are calculated. The positron annihilation effect at a dislocation line is mainly contributed by the dislocation core. The positron annihilation effects at pure dislocation lines are large enough to be measurable though they are much weaker than at vacancies. \u0000 \u0000 \u0000 \u0000Die Positronenannihilationsparameter werden mit drei vereinfachten Versetzungskernmodellen berechnet. Der Positronenannihilationseffekt an einer Versetzungslinie wird hauptsachlich durch den Versetzungskern beeinflust. Die Positronenannihilationseffekte an reinen Versetzungslinien sind gros genug, um mesbar zu sein, obgleich sie viel schwacher sind als die an Leerstellen.","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"30 3 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78622387","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"On the Influence of the Non-Locality of Exchange and Correlation on the Total Energy and on the Band Gap of Silicon","authors":"H. Wiesner, W. Cordts, J. Monecke","doi":"10.1002/PSSB.2221340164","DOIUrl":"https://doi.org/10.1002/PSSB.2221340164","url":null,"abstract":"","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"135 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"74691432","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"AC Transport in Short n+nn+ Layers","authors":"J. Sinkkonen, S. Eränen","doi":"10.1002/PSSB.2221340149","DOIUrl":"https://doi.org/10.1002/PSSB.2221340149","url":null,"abstract":"The admittance of n+nn+ semiconductor structures is studied by solving self-consistently the Poisson equation, the continuity equation, and the linearized Boltzmann equation in the relaxation time approximation for a spatially inhomogeneous electron system. Exact numerical results and an approximate, analytical solution are presented. In addition to the normal bulk admittance and the geometric capacitance of the central n region, the equivalent circuit of the structure consists of contact contributions, the magnitude of which depends on the length of the n region L. At low frequencies the effect of the contacts is to induce a conductance Gc, and a capacitance Cc, in parallel with Gc, in the equivalent circuit. On the other hand, above the plasma frequency of the n region the contact admittance vanishes because of the shunting of the capacitive elements. \u0000 \u0000 \u0000 \u0000Die Admittanz von n+nn+-Halbleiterstrukturen wird durch selbstkonsistentes Losen der Poisson- gleichung, der Kontinuitatsgleichung und der linearisierten Boltzmanngleichung in der Relaxationszeitnaherung fur ein raumlich inhomogenes Elektronensystem untersucht. Exakte numerische Ergebnisse und eine analytische Naherungslosung werden angegeben. Zusatzlich zur normalen Volumenadmittanz und der geometrischen Kapazitanz des zentralen n-Bereichs, besteht das Ersatzschaltbild aus Kontaktbeitragen, deren Grose von der Lange L des n-Bereichs abhangt. Bei niedrigen Frequenzen besteht der Einflus der Kontakte in der Induzierung eines Leitwerts Ge, und einer Kapazitanz Ce, parallel zu Ge, im Ersatzschaltbild. Andererseits verschwindet die Kontaktadmittanz oberhalb der Plasmafrequenz des n-Bereichs aufgrund der Uberbruckung der kapazitiven Elemente.","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"5 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"90153024","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Lattice Anharmonicity and Thermal Expansion of Alkali Metals","authors":"T. Soma, H. Kagaya","doi":"10.1002/PSSB.2221340151","DOIUrl":"https://doi.org/10.1002/PSSB.2221340151","url":null,"abstract":"","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"9 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84189853","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Z. Wilamowski, B. Oczkiewicz, P. Kacman, J. Blinowski
{"title":"Asymmetry of the EPR Absorption Line in CdF2 with Y","authors":"Z. Wilamowski, B. Oczkiewicz, P. Kacman, J. Blinowski","doi":"10.1002/PSSB.2221340137","DOIUrl":"https://doi.org/10.1002/PSSB.2221340137","url":null,"abstract":"An EPR absorption in CdF2:Y is investigated as a function of temperature. The shape of the observed derivative absorption line, which is symmetric at low T, becomes asymmetric at higher. The theoretical model of the line-asymmetrydependence on the sample dimensions and conductivity shows a non-monotonic behaviour of the line asymmetry ratio A/B in theregion where the skin depth is comparable to the sample thickness, in agreement with the experimental data. \u0000 \u0000 \u0000 \u0000Eine EPR-Absorption in CdF2:Y wird als Funktion der Temperatur untersucht. Die Form der beobachteten Ableitung der Absorptionslinie, die bei niedrigen T asymmetrisch ist, wird bei hoheren T symmetrisch. Das theoretische Model 1 der Abhangigkeit der Linienasymmetrie von den Probendimensionen und der Leitfahigkeit zeigt ein nichtmonotones Verhalten des Linienasymme-trieverhaltnisses A/B in dem Bereich, wo die Skintiefe vergleichbar mit der Probendicke ist, in Ubereinstimmung mit den experimentellen Werten.","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"417 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79468472","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"A Modified Bruggeman Theory of Optical Properties for Metal-Isolator Transitions","authors":"M. Arnold, P. Bussemer","doi":"10.1002/PSSB.2221340159","DOIUrl":"https://doi.org/10.1002/PSSB.2221340159","url":null,"abstract":"","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"22 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"89933245","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Renormalization Group Free Energy for an Ising Ferromagnet on a Simple Cubic Lattice","authors":"W. Reich, H. Cofta","doi":"10.1002/PSSB.2221340156","DOIUrl":"https://doi.org/10.1002/PSSB.2221340156","url":null,"abstract":"","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"52 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"88949595","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Bond Charges and Electronic Charge Transfer in Ternary Semiconductors","authors":"U. Pietsch","doi":"10.1002/PSSB.2221340104","DOIUrl":"https://doi.org/10.1002/PSSB.2221340104","url":null,"abstract":"By means of a simple molecule-theoretic model of “linear superposition of two-electron molecules” the bond charges between nearest neighbours and the effective charges of ions are calculated for ternary zinc-blende structure alloys as well as chalcopyrite semiconductors. Taking into account both, the charge transfer among the ions caused by the differences of electronegativities of atoms used and between the bonds created by the internal stress of the lattice a nearly unvaried averaged bond charge amount of the alloy is found, but rather dramatically changed local bond charge parameters in comparison with the respective values of binary compounds used. This fact should influence the noncentral force interaction in such semiconductors. \u0000 \u0000 \u0000 \u0000Mittels eines einfachen molekultheoretischen Modells der linearen Superposition von Zweielektronenmolekulen werden die Bindungsladungen zwischen nachsten Nachbarn und die effektiven Ladungen der Ionen fur ternare Festkorperlosungen mit Zinkblendestruktur und fur Chalkopyrit-Halbleiter berechnet. Der Ladungstransfer unter den lonen wird berucksichtigt, der durch die Differenz der atomaren Elektronegativitaten verursacht wird, und zwischen den Bindungen, der sich aus dem inneren Streszustand des Gitters erklart. Im Vergleich zu den Werten der entsprechenden binaren Verbindungen wird ein nahezu unveranderter mittlerer Bindungsladungsbetrag gefunden. Diese Tatsache sollte Einflus auf die Nichtzentralkraftwechselwirkung in solchen Halbleitern haben.","PeriodicalId":11113,"journal":{"name":"Day 1 Mon, March 21, 2022","volume":"65 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"1986-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"88297310","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}