Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Halbleiterphysik Mittwoch<br />
HL 29.9 Mi 17:15 H13<br />
Rashba spin precession of two-dimensional holes — •Michele<br />
Governale 1,2 , Marco G. Pala 3,2 , Jürgen König 4,2 , and Ulrich<br />
Zülicke 5,2 — 1 Scuola Normale Superiore, Pisa, Italy — 2 Institut für<br />
Theoretische Festkörperphysik, Universität Karlsruhe, Germany —<br />
3 Dipartimento di Ingegneria dell’Informazione, Università degli studi di<br />
Pisa, Italy — 4 Institut für Theoretische Physik III, Ruhr-Universität<br />
Bochum, Germany — 5 Institute of Fundamental Sciences, Massey<br />
University, New Zealand<br />
Spin-orbit coupling due to structural inversion asymmetry plays an<br />
important role in the field of phase-coherent spintronics.<br />
We present a study of spin precession due to Rashba spin splitting[1]<br />
of holes[2] in semiconductor quantum wells. Based on a simple analytical<br />
expression that we derive for the current modulation in a broad<br />
class of experimental situations of ferromagnet/nonmagnetic semiconductor/ferromagnet<br />
hybrid structures, we conclude that the Datta-Das<br />
spin transistor[3] (i) is feasible with holes and (ii) its functionality is not<br />
affected by integration over injection angles.<br />
The current modulation shows a universal oscillation period, irrespective<br />
of the different forms of the Rashba Hamiltonian for electrons and<br />
holes. The analytic formulas approximate extremely well exact numerical<br />
calculations of a more elaborate Kohn–Luttinger model.<br />
[1] E. I. Rashba, Fiz. Tverd. Tela (Leningrad) 2, 1224 (1960)<br />
[Sov. Phys. Solid State 2, 1109 (1960)].<br />
[2] R. Winkler, Phys. Rev. B 62, 4245 (2000).<br />
[3] S. Datta and B. Das, Appl. Phys. Lett. 56, 665, (1990).<br />
HL 29.10 Mi 17:30 H13<br />
ZnMnSe–Spinaligner on inverted GaAs/AlGaAs–2DEGs — •T.<br />
Leeb 1 , M. Döppe 1 , M. Reinwald 1 , H.-P. Tranitz 1 , D. Weiss 1 , W.<br />
Wegscheider 1 , P. Grabs 2 , G. Schmidt 2 , and L. Molenkamp 2 —<br />
1 Institut für Experimentalphysik, Universität Regensburg, D-93040 Regensburg,<br />
Germany — 2 Physikalisches Institut, Universität Würzburg,<br />
D-97074 Würzburg, Germany<br />
The optical detection of spin injection in ZnBeMnSe/GaAs/AlGaAs–<br />
semiconductor heterostructures represents a convincing, however, indirect<br />
result of voltage driven spin transfer across a semiconductor interface.<br />
In contrast, spin injection into a two dimensional electron gas<br />
(2DEG) has not yet been clearly proven in magnetotransport experiments.<br />
We have fabricated n-doped Zn1−x−yBexMnySe–spinaligner contacts<br />
on an inverted GaAs/AlGaAs–2DEG–structure which was applied<br />
to avoid barriers along the current path. The GaAs surface preparation<br />
and the conditions of the ZnMnSe growth initiation are crucial for achieving<br />
a low barrier electronic structure at the ZnMnSe/GaAs–interface. A<br />
strong Zeeman splitting in the conduction band of the Mn–doped II–VI<br />
semiconductor is observed in photoluminescence measurements at small<br />
external magnetic fields. This verifies the spin aligning capability of the<br />
ZnMnSe contact due to a strongly reduced transmission coefficient for<br />
HL 30 Photovoltaik II<br />
minority spin electrons. Magnetotransport measurements have been performed<br />
on a microstructured Hall contact geometry which was developed<br />
according to theoretical considerations concerning spin equilibration between<br />
quantum hall edge channels. This work is supported by DFG via<br />
SFB 348 and by BMBF 13N8282.<br />
HL 29.11 Mi 17:45 H13<br />
InAs-LEDs für Spininjektionsexperimente — •P. Grabs 1 ,<br />
I. Chado 1 , R. Fiederling 1 , A. Slobodskyy 1 , C. Gould 1 , G.<br />
Schmidt 1 , L. W. Molenkamp 1 , C. J. Meining 2 und B. D.<br />
McCombe 2 — 1 Physikalisches Institut, Experimentelle Physik 3,<br />
Universität Würzburg, Am Hubland, 97074 Würzburg — 2 University at<br />
Buffalo, The State University of New York, Buffalo, New York 14260<br />
InAs ist dank seiner hohen Elektronenbeweglichkeit und der starken<br />
Spin-Bahn-Kopplung ein interessantes Material für Spininjektionsexperimente.<br />
Mit Cd1−xMnxSe, einem verdünnten magnetischen Halbleiter<br />
(DMS), der gitterangepasst auf InAs gewachsen werden kann, steht ein<br />
passender Spinaligner zur Verfügung.<br />
Wir berichten über das MBE-Wachstum und die Charakterisierung<br />
von asymmetrischen LEDs mit einer p-Barriere aus AlSb1−xAsx, einem<br />
InAs-Quantentrog und Cd1−xMnxSe als n-Barriere und Spininjektor.<br />
Die zirkulare Polarisation des emittierten Lichts einer solchen LED kann<br />
als Maß für die Effizienz der Spininjektion dienen. Es werden Ergebnisse<br />
von Elektrolumineszenz- und Transportmessungen an den Strukturen<br />
gezeigt.<br />
Diese Arbeit wird unterstützt durch das DARPA SPINS Program.<br />
HL 29.12 Mi 18:00 H13<br />
Spin polarization due to Rashba spin-orbit and boundary<br />
scattering — •Kai Dittmer 1 , Jun-Ichiro Ohe 1,2 , and Bernhard<br />
Kramer 1 — 1 1. Institut für Theoretische Physik, Universität Hamburg<br />
— 2 Physics Department of Sophia University (Tokio)<br />
We calculate spin resolved transport properties of a three terminal [1]<br />
fork-shaped structure with spin-orbit coupling of the Rashba type. For<br />
the calculation of the conductance we apply the transfer matrix method<br />
for the Ando model of the Rashba hamiltonian in the ballistic regime. The<br />
conductance is computed as a function of the Fermi energy for different<br />
values of the spin-orbit coupling constant and for different geometrical<br />
structures and sizes of the model. We observe high polarization and transmission<br />
in the conductance in certain regions of the Fermi energy that<br />
can be explained by spin-orbit and boundary scattering [2]. The dependence<br />
of the spin polarization of the current in different regions of the<br />
sample and the corresponding probability density of the scattering states<br />
is investigated. The possibility of observing the effects in experiment is<br />
discussed.<br />
[1] Kiselev and Kim, Appl. Phys. Lett. 78, 775 (2001); J. Appl. Phys.<br />
94, 4001 (2003).<br />
[2] Chen et al., cond-mat/0308569<br />
Zeit: Mittwoch 15:15–16:45 Raum: H14<br />
HL 30.1 Mi 15:15 H14<br />
Photospannung bei Ladungsträgerinjektion von Farbstoffmolekülen<br />
in transparente Löcher- und Elektronenleiter — •B.<br />
Mahrov 1 , Th. Dittrich 2 , G. Boschloo 1 , L. Dloczik 2 und A.<br />
Hagfeldt 1 — 1 Department of Physical Chemistry, University of Uppsala,<br />
Box 579, 75123 Uppsala, Sweden — 2 Hahn-Meitner-Institut, SE2,<br />
Glienicker Str. 100, D-14109 Berlin, Germany<br />
Transiente und spektrale Photospannung (PV) wurde für Ladungsträgerinjektion<br />
von Farbstoffmolekülen (Ru(dcbpyH2)2(NCS)2) in transparente<br />
Löcher- (CuSCN, CuI, CuAlO2) und Elektronenleiter (TiO2,<br />
SnO2:F) untersucht. Das PV-Signal steigt innerhalb von 10 ns bis 10<br />
µs und die effektiven Lebensdauern variieren zwischen 100 ns und 1 ms<br />
je nach verwendetem Substrat und Mechanismus der Ladungstrennung.<br />
Die Injektionseffizienz ist für Löcher und Elektronen von der gleichen<br />
Größenordnung. Die Injektionsschwelle ist stark vom Substrat abhängig<br />
und liegt zwischen 1.2 und 1.9 eV.<br />
HL 30.2 Mi 15:30 H14<br />
Influence of Film Texture on Grain Boundary Activity in<br />
Cu(In,Ga)Se2 Films — •G. Hanna 1 , N. Ott 2 , H.P. Strunk 2 ,<br />
T. Glatzel 3 , S. Sadewasser 3 , U. Rau 1 , and J.H. Werner 1 —<br />
1 Institut für Physikalische Elektronik, Universität Stuttgart, Pfaffenwaldring<br />
47, 70569 Stuttgart — 2 Institut für Werkstoffwissenschaften<br />
VII, Universität Erlangen Nürnberg — 3 Hahn Meitner Institut, Berlin<br />
A preferred (220/204) crystallographic orientation (texture) of<br />
Cu(In,Ga)Se2 (CIGS) absorber layers is beneficial for the performance<br />
of finished CIGS solar cells as compared to (112) textured CIGS layers<br />
[1,2]. We study the laterally resolved electronic properties of CIGS thin<br />
films with different textures by means of Cathodoluminescence (CL)<br />
mapping, measured in a transmission electron microscope, and Kelvin<br />
Probe Force Microscopy (KPFM). The (220/204) textured samples have<br />
a very homogenous lateral CL-intensity whereas the (112) textured<br />
samples exhibit strong contrasts in the CL-signal. The line scans of the<br />
work function Φ across grain boundaries (GBs) measured with KPFM<br />
exhibit a dip of more than 300 meV across the GB at a (112)-textured<br />
sample while a (220/204) sample shows no comparable dip of Φ at the<br />
GB but rather small spikes. Both measurement methods show that<br />
the superior properties of CIGS solar cells with (220/204)-textured