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Tiefe Temperaturen Montag<br />

Höchst, Europhysics Letters 60 (2002) 615<br />

[2] R. Manzke, R. Müller, C. Janowitz, M. Schneider, A. Krapf, H. Dwelk,<br />

Phys. Rev. B 63 (2001) R 100504<br />

TT 8.47 Mo 14:30 Poster A<br />

Superconductivity and weak electron-phonon coupling in transition<br />

metal diborides — •H. Rosner 1 , S.-L. Drechsler 2 , G.<br />

Fuchs 2 , K.-H. Müller 2 , G. Behr 2 , H. Eschrig 2 , R. Heid 3 , E.<br />

Forzani 4 , K. Winzer 4 , Y. Naidyuk 5 , and O. Otani 6 — 1 Max Planck<br />

Institut für Chemische Physik fester Stoffe — 2 Institut für Festkörper und<br />

Werkstoffforschung Dresden — 3 FZ Karlsruhe — 4 Universität Göttingen<br />

— 5 NAS Kharkiv, Ukraine — 6 NIMS Tsukuba, Japan<br />

After the surprising discovery of superconductivity at 40K in MgB2 an<br />

intense search for other superconducting diborides was started. Several<br />

contradicting reports about the superconductivity in TB2 (T = transition<br />

metal) have been published so far, and the discussion is not settled<br />

yet. Combining extensive electronic structure and model calculations<br />

with various experiments (specific heat, resistivity, susceptibility,<br />

de-Haas-van-Alphen oscillations, point contacts) we investigate the electronic<br />

structure and the electron-phonon coupling λ in various TB2 with<br />

focus on ZrB2. Based on our calculations, we provide a clear microscopic<br />

picture for the rather weak electron-phonon coupling in these systems<br />

and the absence of conventional superconductivity in agreement with<br />

the empirically determined values from thermodynamic and transport<br />

measurements. Open problems are briefly discussed.<br />

TT 8.48 Mo 14:30 Poster A<br />

”Supraleitende” und ”magnetische” Energiebänder bestimmter<br />

Symmetrie als Voraussetzung für Supraleitung bzw. Magnetismus<br />

— •Ekkehard Krüger — Kraussweg 5, 70597 Stuttgart<br />

Beobachtungen an den Bandstrukturen der elementaren Metalle lassen<br />

vermuten, dass zur Bildung stabiler Cooper-Paare sowie stabiler magnetischer<br />

Strukturen gewisse Symmetriebedingungen im Leitungsband eines<br />

Metalles erfüllt sein müssen, die sich im Rahmen der Gruppentheorie optimal<br />

lokalisierter Wannier-Funktionen behandeln lassen. Zur Erklärung<br />

der Beobachtungen wird ein nichtadiabatisches Modell atomartiger Leitungselektronen<br />

vorgeschlagen.<br />

TT 8.49 Mo 14:30 Poster A<br />

Budd-Vannimenus theorem for superconductors — P. Lipavsk´y<br />

1 , •K. Morawetz 2,3 , Jan Koláček 1 , J.J. Mares 1 , E.H.<br />

Brandt 3 , and M. Schreiber 2 — 1 Institute of Physics, Academy of<br />

Sciences, Cukrovarnická 10, 16258 Praha 6, Czech Republic — 2 Istitute<br />

of Physics, Chemnitz University of Technology, 09107 Chemnitz,<br />

Germany — 3 Max-Planck-Institute for the Physics of Complex Systems,<br />

Nöthnitzer Str. 38, 01187 Dresden, Germany<br />

The Budd-Vannimenus theorem is generalized to apply to superconductors<br />

in the Meissner state. This identity links the surface value of the<br />

electrostatic potential to the free energy in the bulk which allows one<br />

to evaluate the observed potential without the explicit solution of the<br />

charge profile at the surface.<br />

[1] P. Lipavsk´y, K. Morawetz, J. Koláček, J. J. Mareˇs, E. H. Brandt, M.<br />

Schreiber, Phys. Rev. B in press (2003), cond-mat/0311166<br />

[2] P. Lipavsk´y, K. Morawetz, J. Koláček, J. J. Mareˇs, E. H. Brandt, M.<br />

Schreiber, Phys. Rev. B submitted, cond-mat/0311167<br />

TT 8.50 Mo 14:30 Poster A<br />

Pressure and Doping Dependence of the Super Exchange of<br />

2D-Cuprates — •Helge Rosner 1 , Ulrike Nitzsche 2 , and Stefan-<br />

Ludwig Drechsler 2 — 1 Max-Planck-Institute for Chemical Physics of<br />

Solids, Noethnitzer Str. 40, D-01187 Dresden, Germany — 2 Leibniz Institute<br />

for Solid State and Materials Research Dresden, P.O.B. 270016,<br />

01171 Dresden, Germany<br />

The dependence of superconducting Tc from the exchange integrals J<br />

is investigated within many models devoted to HTSC. However, most of<br />

these models ignore the dependence of the exchange integrals on both<br />

the lattice parameters and the doping level because of lacking reliable<br />

data. Here we present a systematic study for the two-dimensional model<br />

compound CaCuO2. Based on LDA and LDA+U band structure calculations<br />

and subsequently derived tight-binding models we calculate<br />

the magnitude of the most relevant exchange integrals and their dependence<br />

on doping and uniaxial pressure. We compare the results of<br />

total energy calculations with those of various tight-binding models (oneband<br />

and multi-band approaches) and the parameters obtained by microscopic<br />

models analyzing the experimental data for the superconducting<br />

HgBaCuO-family.<br />

TT 8.51 Mo 14:30 Poster A<br />

Crystal growth, perfection and selected physical properties<br />

of RENi2B2C (RE=Y, Tb, Ho) — •Dmitri Souptel 1 , Günter<br />

Behr 1 , Wolfgang Löser 1 , Günter Fuchs 1 , Konstantin<br />

Nenkov 1 , and Andreas Kreyssig 2 — 1 IFW Dresden, Helmholtzstr.<br />

20, 01171 Dresden — 2 IAPD, TU Dresden, 01062 Dresden<br />

Single crystals of HoNi2B2C, YNi2B2C and TbNi2B2C intermetallic<br />

compounds have been grown by a floating zone technique with optical<br />

heating. Crystals are crack free, without traces of 2nd phases and single<br />

crystalline in the volumes of 6 mm in diameter and 25-40 mm in length.<br />

YNi2B2C shows superconducting transition temperature Tc=15.5 K<br />

with the width ∆Tc=0.1-0.2 K and RRR=35-39. HoNi2B2C single crystals<br />

exhibit a variety of physical properties. For the first time, macroscopic<br />

single crystalline samples with zero-field re-entrant superconductivity<br />

were prepared. Origins of variations of superconducting properties<br />

have been related to composition, lattice parameters and local resistance<br />

ratio measurements of crystal sections. The results corroborate the existence<br />

of a finite homogeneity range of the HoNi2B2C intermetallic compound.<br />

TT 8.52 Mo 14:30 Poster A<br />

Tieftemperaturverhalten von CeNi2B2C — •Dmitrij Bogdanov,<br />

Klaus Winzer und Eugenio Forzani — I. Physikalisches Institut,<br />

Universität Göttingen, Tammannstr. 1, 37077 Göttingen<br />

Die bisher vorliegenden Untersuchungen an CeNi2B2C lassen die Frage<br />

nach dem Grundzustand des Systems bei tiefen Temperaturen offen.<br />

Die Möglichkeit eines supraleitenden Grundzustandes bei T = 0,1 K [1]<br />

konnte bisher nicht bestätigt werden. Für die Charakterisierung des Systems<br />

wurden sowohl polykristalline Proben als auch Einkristalle hergestellt,<br />

deren Phasenreinheit und Qualität durch Röntgendiffraktometrie<br />

und Messungen des Restwiderstandsverhältnisses bestimmt wurden. Die<br />

Temperatur- und Magnetfeldabhängigkeit des spezifischen Widerstandes<br />

und der magnetischen Suszeptibilität wurden für Temperaturen bis 40<br />

mK bestimmt. Mit einem SQUID-System wurden zusätzlich Messungen<br />

des magnetischen Moments und der Suszeptibilität bis 1,8 K durchgeführt.<br />

Der elektrische Widerstand zeigt im Temperaturbereich um 2<br />

K einen stufenförmigen Verlauf, der auf eine geringe Aufspaltung des<br />

Kristallfeld-Grundzustandes hindeutet. Bei tiefen Temperaturen wird ein<br />

sehr steiler Anstieg der paramagnetischen Suszeptibilität mit einem Maximum<br />

bei T = 100 mK beobachtet, das als Signatur einer magnetischen<br />

Ordnung gedeutet wird. Messungen des spezifischen Widerstandes zeigen<br />

keinerlei Anzeichen für das Auftreten von Supraleitung.<br />

[1] M. El Massalami et al., Physica C 304 , 184 (1998)<br />

TT 8.53 Mo 14:30 Poster A<br />

The effect of noble-gas preplating on quench-condensed hydrogen<br />

films — •Stefan Tibus, Jürgen Klier, and Paul Leiderer<br />

— Universität Konstanz, Universitätsstraße 10, 78464 Konstanz<br />

Triple-point dewetting of H2 on e.g. Au is a well-known phenomenon<br />

and prevents the forming of a thick (i.e. more than a few monolayers)<br />

solid equilibrium film on such surfaces. It was theoretically shown that<br />

a modification of the substrate-adsorbate interaction by means of preplating<br />

should lead to complete wetting and thus to a thick solid film at<br />

saturated vapor pressure (provided that the substrate surface is ideally<br />

smooth). Ne and Ar were found to be appropriate candidates as intermediate<br />

layers, but investigations found no significant change in the film<br />

thickness upon preplating, which was attributed to the roughness of the<br />

substrate.<br />

However, preliminary experiments with quench-condensed hydrogen<br />

showed an effect of the preplating on the film’s structure. This is to be<br />

investigated in more detail by means of a new experimental setup allowing<br />

for both surface-plasmon microscopy (at a higher resolution than<br />

before) as well as surface-plasmon spectroscopy.<br />

TT 8.54 Mo 14:30 Poster A<br />

Josephson coupling in Nb/Al 2 O3/Cu 1 Ni1−x/Nb tunnel junctions<br />

— •Martin Weides 1 , Edward Goldobin 2 , Reinhold Kleiner 2 ,<br />

and Hermann Kohlstedt 1 — 1 Institut für Festkörperforschung,<br />

Forschungszentrum Jülich, D-52425 Jülich — 2 Physikalisches Institut-<br />

Experimentalphysik II, Universität Tübingen, D-72076 Tübingen<br />

The realization of qubits for quantum computation attracts considerable<br />

interest. One of the approaches is to use π Josephson junctions (JJs)<br />

which can be realized as hybrids of superconducting (S) tunnel junction

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