Bert Nickel

Dr. Bert Nickel


Research Focus & Metrics

Academic Career Length

30Years (1997-Present)

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

Representative Publications

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1 September 2015 in Nano Letters
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Journal Article
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JSJasmina A. Sichert
Jasmina A. Sichert
YTYu Tong
Yu Tong
NMNiklas Mutz
Niklas Mutz
MVMathias Vollmer
Mathias Vollmer
SFStefan Fischer
Stefan Fischer
JFJochen Feldmann
Jochen Feldmann

16 October 2004 in Chemistry of Materials
Verified
Journal Article
Closed access
RRRicardo Ruiz
Ricardo Ruiz
DCDevashish Choudhary
Devashish Choudhary
BNBert Nickel
Bert Nickel
TTTullio Toccoli
Tullio Toccoli
KCKee-Chul Chang
Kee-Chul Chang
GMGeorge Malliaras
George Malliaras

25 November 2003 in Journal of the American Chemical Society
Verified
Journal Article
Closed access
EHEric L. Hanson
Eric L. Hanson
JSJeffrey Schwartz
Jeffrey Schwartz
BNBert Nickel
Bert Nickel
NKNorbert Koch
Norbert Koch
MDMehmet Fatih Danisman
Mehmet Fatih Danisman

1 August 2007 in Journal of the American Chemical Society
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Journal Article
Closed access
SSStefan Schiefer
Stefan Schiefer
MHMartin Huth
Martin Huth
ADAlexander Dobrinevski
Alexander Dobrinevski
BNBert Nickel
Bert Nickel

10 April 2017 in Advanced Energy Materials
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Journal Article
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LPLakshminarayana Polavarapu
Lakshminarayana Polavarapu
BNBert Nickel
Bert Nickel
JFJochen Feldmann
Jochen Feldmann
AUAlexander S. Urban
Alexander S. Urban

12 March 2003 in Physical Review B
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Journal Article
Closed access
PDF file
RRRicardo Ruiz
Ricardo Ruiz
BNBert Nickel
Bert Nickel
NKNorbert Koch
Norbert Koch
LFLeonard C. Feldman
Leonard C. Feldman
RHRichard F. Haglund
Richard F. Haglund
GSGiacinto Scoles
Giacinto Scoles
We have compared the nucleation of pentacene on reduced and oxidized Si surfaces by a combination of x-ray reflectivity measurements and atomic force microscopy. For the reduced surface, the nucleation density is 0.007 μm−2. Second monolayer (ML) formation starts at a coverage of Θ=0.6 ML, and the first layer is completely closed at a total coverage of 2 ML. For the oxidized surface, the nucleation density is larger by a factor of 100 (0.7 μm−2). Second ML formation also starts at Θ=0.6 ML, but the first layer closes already at 1.1 ML coverage, indicating nearly ideal layer-by-layer growth. For both terminations, the electron density obtained for the closed first monolayer is only 75% of the bulk value, indicating a reduced mass packing efficiency of the layer. Second ML islands are aligned relative to each other on an area limited by the lateral size of first ML islands, which act as templates for epitaxial growth.