Last edited by Teramar
Tuesday, October 13, 2020 | History

2 edition of Electron-phonon interactions and de Haas-van Alphen effect in dilute non-magnetic alloys found in the catalog.

Electron-phonon interactions and de Haas-van Alphen effect in dilute non-magnetic alloys

Narsingh Ramniwas Bharatiya

# Electron-phonon interactions and de Haas-van Alphen effect in dilute non-magnetic alloys

## by Narsingh Ramniwas Bharatiya

Published .
Written in English

Subjects:
• Free electron theory of metals.

• Edition Notes

The Physical Object ID Numbers Statement by Narsingh Ramniwas Bharatiya. Pagination 70 leaves, bound ; Number of Pages 70 Open Library OL14234233M

de Haas-van Alphen effect Demagnetization dynamics – Demagnetizing field, see Hyperfine field Dipolar interact , , Dipolar field DM interaction, see Dzyaloshinskii-Moria interaction Domain 21–23, –, , –; see also single domain Dzyaloshinskii-Moria interact Electrochemical control. Advanced Condensed Matter Physics Leonard M. Sander Department of Physics, The University of Michigan This book is intended as a textbook for a graduate course in condensed matter physics. It is based on many years’ experience in teaching in the Physics department at The University of Michigan. Further, an effect of spin-orbit.

With this volume of the Handbook on the Physics and Chemistry of Rare Earth Profs. JeanClaude Bünzli, Swiss Federal Institute of Technology, Lausanne, and Vitalij K. Pecharsky, Iowa State University, Ames have joined Prof. Karl A. Gschneidner, Jr., one of the founding editors of this series, as editors. Abstract book final. and further allows demonstrating the major role of the electron-phonon interaction in the superconducting mechanism (2, 3). Reference: [1]. Netherlands We report high magnetic field measurements of magnetic torque, thermoelectric power, magnetization, and the de Haas–van Alphen effect in CeIrIn5 across 28 T, where.

An Ultrasensitive Organic Semiconductor NO2 Sensor Based on Crystalline TIPS-Pentacene Films.. PubMed. Wang, Zi; Huang, Lizhen; Zhu, Xiaofei; Zhou, Xu; Chi, Lifeng. Organic semiconductor gas sensor is one of the promising candidates of room temperature operated gas sensors with high selectivity. However, for a long time the performance of organic semiconductor . BEGIN:VCALENDAR VERSION PRODID: //CERN//INDICO//EN BEGIN:VEVENT SUMMARY: From Re = to Re = \, with non-Newtonian and Newtonian liq uids DTSTART;VALUE=DATE.

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### Electron-phonon interactions and de Haas-van Alphen effect in dilute non-magnetic alloys by Narsingh Ramniwas Bharatiya Download PDF EPUB FB2

The de Haas–van Alphen effect at a quantum critical point Article in Energy 30(6) May with 35 Reads How we measure 'reads'. We report on measurements of the de Haas–van Alphen effect in the heavy electron metal CeCu 6 in the coherent state.

At least eight dHvA frequencies are observed with cyclotron masses as large as 80m 0. Compared with LaCu 6 the measured masses are greater by a factor of ≈ We find no evidence for the presence of ‘light’ carriers.

high magnetic field dependent diamagnetic shifts in al x ga 1-x as semiconductor alloys. jones, j. reno, s. crooker, k. bajaj and ; increase of quantum hall plateau widths due to electron-phonon interaction.

riess, t. duguet, p the de haas-van alphen effect in cemin 5 (where m = rh and co) d. hall, t. murphy, e. At p = MPa, the highest pressure of the present experiment, T c,sc is reduced from K to K to K upon increasing irradiation time from 50 h to h to h.

For non-magnetic alloys, the low temperature magnetoresistance behavior generally follows Kohler's rule. Schwerer and Silcox showed by a careful study of dilute Ni alloy samples that for a given series of alloys the ordinary magnetoresistance follows a Kohler's rule, but that the Kohler function varied considerably with the type of by:   Oscillations as a function of magnetic field in the magnetic susceptibility of Bi were observed by de Haas and van Alphen in Now known as the de Haas–van Alphen (dHvA) effect, the observation of such oscillations has evolved into one of the most powerful probes of the Fermi surface, but at the time there was no theory to understand Cited by: This banner text can have markup.

web; books; video; audio; software; images; Toggle navigation. Split Fermi Surfaces of the Spin–Orbit-Coupled Metal Cd 2 Re 2 O 7 Probed by de Haas–van Alphen Effect Yasuhito Matsubayashi, Kaori Sugii, Hishiro T.

Hirose, Daigorou Hirai, Shiori Sugiura, Taichi Terashima, Shinya Uji, Zenji Hiroi, Journal of Physical Society of Japan, 87, Samples of different age are in effect samples of slightly different materials: A non-magnetic pair-breaking action produces a residual density of electron states that increases with sample age.

It occurs preferentially in the electron band (one of two with different energy gaps) with the smaller gap, producing a change in the nature of the.

Uichiro Mizutani - Introduction to the Electron Theory of Metals () код для вставки. Calculated de Haas-van Alphen quantities of CeMIn 5 (M=Co, Rh, and Ir) compounds S.

Elgazzar, I. Opahle, R. Hayn, and P.M. Oppeneer Physical Review B 69, () Ultrafast demagnetization in Ni: Theory of magneto-optics for non-equilibrium electron distributions P.M.

Oppeneer and A. Liebsch Journal of Physis: Condensed Mat This talk will discuss recent transport and de Haas van Alphen studies of the archetypal heavy fermion systems $\rm CeRu_2Si_2$ [1] and $\rm YbRh_2Si_2$ [2], which are interpreted as showing that the f-electron disappears from the Fermi volume via two successive Lifshitz transitions: in the first transition a majority spin band sinks below the.

de Haas–van Alphen eﬀect Positron annihilation Electronic structure of magnetically dilute alloys Scattering of electrons in a magnetically dilute alloy – “partial wave method” non-magnetic metal, is described.

The resistivity–temperature curve for a‐uranium along the [] direction is shown in Fig. Many other physical properties of elemental uranium have been determined, such as elastic moduli, heat capacity, de Haas‐van Alphen measurements, transport properties and others.

8 Superconductors – Materials, Properties and Applications Theory of anti-proximity effect There are several theoretical models that could be used for the theoretical explanation of the magnetic field-induced or -enhanced superconductivity in nanowires, while some of which were proposed long before the anti-proximity effect was reported.

A Subj-class: Soft Condensed Matter; Statistical Mechanics \\ \\ Paper: cond-mat/ From: Arnd Hubsch >huebsch(at) Date: Tue, 18 May GMT (kb) Title: Computer aided perturbation theory by cumulants: dimerized and frustrated spin 1/2 chain Authors: S. Sykora, A. Huebsch, and K.W.

Becker Comments. The electronic structure of the transition ferromagnets has been studied in- tensively, and low temperature measurements such as the de Haas van Alphen effect in pure metal samples show that they have complex Fermi surfaces of much the same type as those of non-magnetic transition elements except that k 1' and k ~ states are not equivalent.

Afin de limiter votre attente si vous venez de l'extérieur du CEA, merci de contactez Sarah Mauduit en transmettant une copie de la pièce d'identité et en précisant date, lieu de naissance, nationalité, nom de jeune fille pour les femmes, statut et nom de l'employeur.

Grimvall - Thermophysical Properties of Materials ( North Holland).pdf код для вставки. Results of muon spin rotation (μ-SR) in the metallic intercalated C₆₀ compounds (AnC₆₀, where An are n alkali metal atoms) are presented.

Except for the case of K₁C₆₀, the metallic state of these systems is unstable at low temperature (to a superconducting transition in A₃C₆₀ and a magnetic metal insulator transition in A₁C₆₀)- In A₃C₆₀, the properties of the.

Matter Subj-class: Materials Science; Mesoscopic Systems and Quantum Hall Effect \\ \\ Paper: cond-mat/ From: Xi-Wen Guan >(at) Date: Mon, 4 Sep GMT (18kb) Title: Exact solution for the Bariev model with boundary fields Authors: A.

Foerster, X.-W. Guan, J. Links, I. Roditi and H.-Q. Zhou.0 scattering 1 theory 2 nuclear 3 magnetic 4 energy 5 effect 6 electron 7 absorption 8 resonance 9 structure 10 spectrum 11 decay 12 electrons 13 field 14 cross 15 crystals 16 effects 17 properties 18 neutrons 19 states 20 spectra 21 model 22 neutron 23 production 24 radiation 25 protons For example, transport measurements in magnetic fields [34, 35] show the difference between heavy fermion systems and dilute Kondo alloys.

Gutzwiller approach There have been attempts to explain the mass renormalization by using the Hubbard–Gutzwiller model [36–38].