Kamuran kara koç

Dr. Kamuran kara koç

orcid

Research Focus & Metrics

Academic Career Length

18Years (2009-Present)

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

Representative Publications

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14 March 2014 in Discover Nano
Verified
Journal Article
Open access
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FSFahrettin Sarcan
Fahrettin Sarcan
ÖDÖmer Dönmez
Ömer Dönmez
KKKamuran kara koç
Kamuran kara koç
AEAyşe Erol
Ayşe Erol
EAElif Akalın
Elif Akalın
CFChantal Fontaine
Chantal Fontaine
Bulk GaAs1 - x Bi x /GaAs alloys with various bismuth compositions are studied using power- and temperature-dependent photoluminescence (PL), Raman scattering, and atomic force microscopy (AFM). PL measurements exhibit that the bandgap of the alloy decreases with increasing bismuth composition. Moreover, PL peak energy and PL characteristic are found to be excitation intensity dependent. The PL signal is detectable below 150 K at low excitation intensities, but quenches at higher temperatures. As excitation intensity is increased, PL can be observable at room temperature and PL peak energy blueshifts. The quenching temperature of the PL signal tends to shift to higher temperatures with increasing bismuth composition, giving rise to an increase in Bi-related localization energy of disorders. The composition dependence of the PL is also found to be power dependent, changing from about 63 to 87 meV/Bi% as excitation intensity is increased. In addition, S-shaped temperature dependence at low excitation intensities is observed, a well-known signature of localized levels above valence band. Applying Varshni’s law to the temperature dependence of the PL peak energy, the concentration dependence of Debye temperature (β) and thermal expansion coefficient (α) are determined. AFM observations show that bismuth islands are randomly distributed on the surface and the diameter of the islands tends to increase with increasing bismuth composition. Raman scattering spectra show that incorporation of Bi into GaAs causes a new feature at around 185 cm-1 with slightly increasing Raman intensity as the Bi concentration increases. A broad feature located between 210 and 250 cm-1 is also observed and its intensity increases with increasing Bi content. Furthermore, the forbidden transverse optical (TO) mode becomes more pronounced for the samples with higher bismuth composition, which can be attributed to the effect of Bi-induced disorders on crystal symmetry. PACS 78.55Cr 78.55-m 78.20-e 78.30-j

18 July 2011 in ACS Nano
Verified
Journal Article
Open access
SMStefan Müllegger
Stefan Müllegger
WSWolfgang Schöfberger
Wolfgang Schöfberger
MRMohammad Rashidi
Mohammad Rashidi
TLThomas Lengauer
Thomas Lengauer
FKFlorian Klappenberger
Florian Klappenberger
RKReinhold Koch
Reinhold Koch
Supporting functional molecules on crystal facets is an established technique in nanotechnology. To preserve the original activity of ionic metallorganic agents on a supporting template, conservation of the charge and oxidation state of the active center is indispensable. We present a model system of a metallorganic agent that, indeed, fulfills this design criterion on a technologically relevant metal support with potential impact on Au(III)-porphyrin-functionalized nanoparticles for an improved anticancer-drug delivery. Employing scanning tunneling microscopy and -spectroscopy in combination with photoemission spectroscopy, we clarify at the single-molecule level the underlying mechanisms of this exceptional adsorption mode. It is based on the balance between a high-energy oxidation state and an electrostatic screening-response of the surface (image charge). Modeling with first principles methods reveals submolecular details of the metal–ligand bonding interaction and completes the study by providing an illustrative electrostatic model relevant for ionic metalorganic agent molecules, in general.

1 April 2013 in Applied Surface Science
Verified
Journal Article
Closed access
NEN.H. Erdogan
N.H. Erdogan
KKKamuran kara koç
Kamuran kara koç
HOH. Ozdamar
H. Ozdamar
RER. Esen
R. Esen
HKHamide Kavak
Hamide Kavak

15 March 2014 in Journal of Materials Science: Materials in Electronics
Verified
Journal Article
Closed access
PDF file
DTDeniz Kadir Takci
Deniz Kadir Takci
ETEbru Şenadım Tüzemen
Ebru Şenadım Tüzemen
KKKamuran kara koç
Kamuran kara koç
SYSadi Yilmaz
Sadi Yilmaz
RERamazan Esen
Ramazan Esen
OBOzge Baglayan
Ozge Baglayan

1 November 2014 in Applied Surface Science
Verified
Journal Article
Closed access
ETEbru Şenadım Tüzemen
Ebru Şenadım Tüzemen
KKKamuran kara koç
Kamuran kara koç
SESezai Elagoz
Sezai Elagoz
DTDeniz Kadir Takci
Deniz Kadir Takci
IAIsmail Altuntas
Ismail Altuntas
RERamazan Esen
Ramazan Esen

1 January 2022 in Physica Scripta
Verified
Journal Article
Closed access
ÜDÜmit Doğan
Ümit Doğan
FSfahrettin sarcan
fahrettin sarcan
KKKamuran kara koç
Kamuran kara koç
FKFurkan Kuruoğlu
Furkan Kuruoğlu
AEAyşe Erol
Ayşe Erol
In this paper, the effects of annealing temperature on the performance of a ZnO thin film-based Metal-Semiconductor-Metal (MSM) type ultraviolet (UV) photodetector is reported. ZnO thin films were grown on a glass substrate using the Pulsed Filtered Cathodic Vacuum Arc Deposition (PFCVAD) technique at room temperature and after the deposition process the samples were annealed at 400, 450 and 550 °C in air condition to investigate the annealing effect on the structural, electrical, and optical properties of the photodetector. ZnO thin films which have grains in nanometer range has an increasing in the diameter of grains from 10.5 to 18.3 nm as a function of annealing temperature results in a red shift in the cut-off wavelength of the photodetector from 3.25 eV (381 nm) to 3.23 eV (383 nm). It is demonstrated that the sensitivity and the speed (rise/fall times) of the ZnO thin film based MSM photodetectors enhances with increasing post growth annealing temperature of ZnO thin film due to the increase in the absorption coefficient and the decrease of the total area of the grain boundaries due to the larger grain sizes formation in ZnO thin films with increasing thermal annealing temperature.