Andriy Lotnyk

Prof. Andriy Lotnyk

1. Leibniz Institute of Surface Engineering (IOM), Leipzig, Germany
+1
orcid

Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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10 October 2011 in Physical Chemistry Chemical Physics
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HBHenrik Buschmann
Henrik Buschmann
JDJanis Dölle
Janis Dölle
SBStefan Berendts
Stefan Berendts
AKAlexander Kuhn
Alexander Kuhn
PBPatrick Bottke
Patrick Bottke
JJJürgen Janek
Jürgen Janek
The solid lithium-ion electrolyte “Li7La3Zr2O12” (LLZO) with a garnet-type structure has been prepared in the cubic and tetragonal modification following conventional ceramic syntheses routes. Without aluminium doping tetragonal LLZO was obtained, which shows a two orders of magnitude lower room temperature conductivity than the cubic modification. Small concentrations of Al in the order of 1 wt% were sufficient to stabilize the cubic phase, which is known as a fast lithium-ion conductor. The structure and ion dynamics of Al-doped cubic LLZO were studied by impedance spectroscopy, dc conductivity measurements, 6Li and 7Li NMR, XRD, neutron powder diffraction, and TEM precession electron diffraction. From the results we conclude that aluminium is incorporated in the garnet lattice on the tetrahedral 24dLi site, thus stabilizing the cubic LLZO modification. Simulations based on diffraction data show that even at the low temperature of 4 K the Li ions are blurred over various crystallographic sites. This strong Li ion disorder in cubic Al-stabilized LLZO contributes to the high conductivity observed. The Li jump rates and the activation energy probed by NMR are in very good agreement with the transport parameters obtained from electrical conductivity measurements. The activation energy Ea characterizing long-range ion transport in the Al-stabilized cubic LLZO amounts to 0.34 eV. Total electric conductivities determined by ac impedance and a four point dc technique also agree very well and range from 1 × 10−4 Scm−1 to 4 × 10−4 Scm−1 depending on the Al content of the samples. The room temperature conductivity of Al-free tetragonal LLZO is about two orders of magnitude lower (2 × 10−6 Scm−1, Ea = 0.49 eV activation energy). The electronic partial conductivity of cubic LLZO was measured using the Hebb–Wagner polarization technique. The electronic transference number te − is of the order of 10−7. Thus, cubic LLZO is an almost exclusive lithium ion conductor at ambient temperature.

12 June 2012 in Advanced Materials
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MMMatthias Mecklenburg
Matthias Mecklenburg
ASArnim Schuchardt
Arnim Schuchardt
Yogendra MishraYogendra Mishra
Yogendra Mishra
SKSören Kaps
Sören Kaps
RARainer Adelung
Rainer Adelung
KSKarl Schulte
Karl Schulte

15 June 2008 in Nature Nanotechnology
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WLWoo Lee
Woo Lee
HHHee Han
Hee Han
Andriy LotnykAndriy Lotnyk
Andriy Lotnyk
MSMarkus Andreas Schubert
Markus Andreas Schubert
SSStephan Senz
Stephan Senz
UGUlrich Gösele
Ulrich Gösele

18 September 2019 in Nanoscale Advances
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Andriy LotnykAndriy Lotnyk
Andriy Lotnyk
MBMario Behrens
Mario Behrens
BRBernd Rauschenbach
Bernd Rauschenbach
The paper reviews materials science aspects of chalcogenide-based phase change thin films relevant for non-volatile memory applications.

20 March 2013 in ACS Nano
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PHPascal Hartmann
Pascal Hartmann
Torsten BrezesinskiTorsten Brezesinski
Torsten Brezesinski
JSJoachim Sann
Joachim Sann
Andriy LotnykAndriy Lotnyk
Andriy Lotnyk
JEJens-Peter Eufinger
Jens-Peter Eufinger
JJJürgen Janek
Jürgen Janek

1 February 2016 in Acta Materialia
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Journal Article
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Andriy LotnykAndriy Lotnyk
Andriy Lotnyk
SBSabine Bernütz
Sabine Bernütz
XSXinxing Sun
Xinxing Sun
URUlrich Ross
Ulrich Ross
MEMartin Ehrhardt
Martin Ehrhardt
BRBernd Rauschenbach
Bernd Rauschenbach