Cinzia Cepek

Dr. Cinzia Cepek


Research Focus & Metrics

Academic Career Length

32Years (1995-Present)

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

Representative Publications

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24 February 2007 in Nano Letters
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Journal Article
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SHStephan Hofmann
Stephan Hofmann
RSRenu Sharma
Renu Sharma
CDCaterina Ducati
Caterina Ducati
GDGaohui Du
Gaohui Du
Cecilia MatteviCecilia Mattevi
Cecilia Mattevi
JRJohn Robertson
John Robertson

22 July 2008 in The Journal of Physical Chemistry C
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Journal Article
Closed access
Cecilia MatteviCecilia Mattevi
Cecilia Mattevi
CWChristoph Tobias Wirth
Christoph Tobias Wirth
SHStephan Hofmann
Stephan Hofmann
RBRaoul Blume
Raoul Blume
MCMirco Cantoro
Mirco Cantoro
JRJohn Robertson
John Robertson

8 August 2013 in ACS Nano
Verified
Journal Article
Closed access
LPLaerte L. Patera
Laerte L. Patera
CACristina Africh
Cristina Africh
RWRobert S. Weatherup
Robert S. Weatherup
RBRaoul Blume
Raoul Blume
SBSunil Bhardwaj
Sunil Bhardwaj
CCCinzia Cepek
Cinzia Cepek

16 June 2005 in Advanced Materials
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Journal Article
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EBE. Barborini
E. Barborini
ACA. M. Conti
A. M. Conti
IKI. Kholmanov
I. Kholmanov
PPP. Piseri
P. Piseri
APAlessandro Podestà
Alessandro Podestà
MSM. Sancrotti
M. Sancrotti

15 March 1996 in Physical Review B
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Journal Article
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CCCinzia Cepek
Cinzia Cepek
AGAndrea Goldoni
Andrea Goldoni
SMS. Modesti
S. Modesti
The interaction between C60 and the Pt(111) surface has been studied by high-resolution electron-energy-loss spectroscopy, photoemission and Auger spectroscopy, and low-energy electron diffraction from 100 to 1150 K. C60 forms strong covalent bonds with Pt with very small charge transfer (<0.8 electrons/molecule from C60 to the substrate), has a low surface mobility, and decomposes at about 1050 K, leaving a multidomain graphitic surface layer. C60 decomposes also on Ni(110) at about 760 K, forming a carbidic carbon layer, which transforms into graphitic carbon at higher temperatures. Both surfaces act as a catalyst for the fragmentation process. © 1996 The American Physical Society.

6 May 2014 in Journal of Applied Physics
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Journal Article
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MIM. Ishfaq
M. Ishfaq
MKM. Rizwan Khan
M. Rizwan Khan
MBM. F. Bhopal
M. F. Bhopal
FNF. Nasim
F. Nasim
AAA. Ali
A. Ali
CCCinzia Cepek
Cinzia Cepek
In this paper, we report the effect of 1.5 MeV proton beam irradiation dose on the structural and electrical properties of TiO2 thin films deposited on n–Si substrates. The formation and transformation of different TiO2 phases in the irradiated thin films were characterized by X-ray diffraction and X-ray photoelectron spectroscopy (XPS). X-ray diffraction measurements revealed that the as grown film was rich in Ti5O9 phase and then converted to mixed phases of TiO2 (rutile and anatase) after exposure with radiation doses up to 5 × 1014 cm−2. The XPS results revealed the formation of oxygen vacancy (negative) traps in the exposed TiO2 films, which showed strong dependence on the dose. The C-V measurements showed that proton radiations also damaged the Si substrate and created deep level defects in the substrate, which caused a shift of 0.26 ± 0.01 V in the flat band voltage (VFB). I–V measurements showed that the ideality factor increased and the rectification ratio dropped with the increase in the radiation dose. The present study showed the stability of TiO2/Si interface and TiO2 film as an oxide layer against proton radiations.