K.P. Korona
University of Warsaw
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Featured researches published by K.P. Korona.
Solid State Communications | 1996
K. Pakuła; A. Wysmołek; K.P. Korona; J. M. Baranowski; R. Stępniewski; I. Grzegory; M. Bockowski; J. Jun; Stanisław Krukowski; Miroslaw Wroblewski; Sylwester Porowski
Abstract In this work we report results of photoluminescence (PL) and reflectivity measurements in the exciton region of GaN homoepitaxial layers grown by metalorganic chemical vapour deposition on GaN substrates. At low temperature (4.2K), very narrow (FWHM = 1.0meV) PL lines related to excitons bound to neutral acceptor (3.4666eV) and neutral donor (3.4719eV) were observed. The energies of free excitons from reflectivity and PL measurements were found to be: E A = 3.4780eV, E B = 3.4835eV and E C = 3.502eV.
Applied Physics Letters | 1996
K.P. Korona; A. Wysmol; ek; K. Pakul; R. Ste̢pniewski; J. M. Baranowski; I. Grzegory; ucznik; Miroslaw Wroblewski; Sylwester Porowski
Reflection measurements in the exciton region of GaN homoepitaxial layers grown by metalorganic chemical vapor deposition (MOCVD) on GaN single crystals are reported. At low temperature (4.2 K) three free exciton lines have been found with energies; EA=3.4776 eV, EB=3.4827 eV, and EC=3.502 eV. The spin‐orbit parameter Δso=19.7±1.5 meV and the crystal field parameter Δcr=9.3±0.3 meV have been obtained. From temperature dependence of exciton spectra the energy gap dependence has been found: E(T)=E(0)−λ/[exp(β/T)−1] (λ=0.121 eV, β=316 K).
Physical Review B | 2006
J. Suffczyński; T. Kazimierczuk; M. Goryca; B. Piechal; A. Trajnerowicz; K. Kowalik; P. Kossacki; A. Golnik; K.P. Korona; M. Nawrocki; J. A. Gaj; G. Karczewski
Systematic measurements of auto- and cross-correlations of photons emitted from individual
Semiconductor Science and Technology | 2007
E. Przeździecka; E. Kamińska; K.P. Korona; E. Dynowska; W. Dobrowolski; R. Jakieła; Ł. Kłopotowski; J. Kossut
\mathrm{Cd}\mathrm{Te}∕\mathrm{Zn}\mathrm{Te}
Journal of Applied Physics | 2009
K.P. Korona; Aneta Drabińska; Piotr Caban; W. Strupiński
quantum dots under pulsed excitation were used to elucidate nonresonant excitation mechanisms in this self-assembled system. Memory effects extending over a few excitation pulses have been detected in agreement with previous reports and quantitatively described by a rate equation model, fitting a complete set of correlation and PL intensity results. The important role of single carrier trapping in the quantum dot was established. An explanation was suggested for the unusually wide antibunching dip observed previously in
MRS Proceedings | 1996
J. M. Baranowski; Z. Liliental-Weber; K.P. Korona; K. Pakuła; R. Stępniewski; A. Wysmołek; I. Grzegory; G. Nowak; S. Porowski; B. Monemar; Peder Bergman
X\text{\ensuremath{-}}X
Applied Physics Letters | 1996
C. Jagadish; H.H. Tan; A. Krotkus; Saulius Marcinkevicius; K.P. Korona; M. Kamińska
autocorrelation experiments on quantum dots under cw excitation.
Physica Status Solidi B-basic Solid State Physics | 1998
R. Stępniewski; A. Wysmołek; M. Potemski; J. Lusakowski; K.P. Korona; K. Pakuła; J. M. Baranowski; G. Martinez; P. Wyder; I. Grzegory; S. Porowski
ZnO doped with N and/or As layers was fabricated by thermal oxidation of ZnTe films grown by MBE on different substrates. Hall effect measurements demonstrated p-type conductivity with a hole concentration of ~5 × 1019 cm−3 for ZnO:As and ZnO:As:N on GaAs substrates and ~6 × 1017 cm−3 for ZnO:N on ZnTe substrates. The concentration of N and As atoms in ZnO is estimated to be ~1020 cm−3. This suggested that simple substitutional N atoms form acceptor impurities with a smaller efficiency than an As-related complex, probably AsZn–2VZn. In particular, we were able to distinguish between nitrogen and arsenic acceptor-related luminescence. Optical studies showed meaningful differences of the PL features in samples with different acceptors, grown on different substrates.
Solid State Communications | 1998
Irina Buyanova; J.P. Bergman; B. Monemar; Hiroshi Amano; Isamu Akasaki; A. Wysmołek; P Lomiak; J. M. Baranowski; K. Pakuła; R. Stępniewski; K.P. Korona; I. Grzegory; M. Bockowski; Sylwester Porowski
We present the optical and the electrical properties of GaN/AlGaN structures that can be used as tunable ultraviolet photodetectors. The photosensitivity spectrum of the structures can be tuned in the range 3.5–3.85 eV by external voltage. The photosensitivity of the sample in the 3.5 eV spectral range increases about 500 times when the reverse bias changes from −2 to −6 V. The effect can be explained by changes in the electric field in the GaN/AlGaN structure. The field is generated by the internal electric polarization and the external bias. We present also a numerical modeling of the electric field, the potential profiles, and the current flow in such structures. Our modeling shows that at low bias a two-dimensional (2D)-electron gas at the AlGaN/GaN interface screens the electric field generated by spontaneous polarization. The lack of the field stops transport of photoexcited holes. The holes that are accumulated on the interface causes fast electron recombination and reduces photocurrent. The extern...
Nanotechnology | 2014
Jolanta Borysiuk; Z. R. Zytkiewicz; M. Sobanska; A. Wierzbicka; K. Klosek; K.P. Korona; P.S. Perkowska; A. Reszka
The review of structural and optical properties of homoepitaxial layers grown by MOVCD on single crystals GaN substrates is presented. The TEM technique is used to characterise the structural properties of epi-layers. It is found that the structural properties of GaN homoepitaxial layers are determined by the polarity of the substrate surface on which the growth takes place. It is shown that threading dislocations are present only in the layers grown on the [0001] “smooth” surface. On the other hand the layers grown on the [0001] “rough” surface are free from vertical defects. The characteristic feature of the growth on the “rough” surface are pinholes. The optical properties of homoepitaxial layers are predominantly determined by the growth polarity as well. It is shown also that the reflectivity measurement is the most precise way to determine the exciton energies and that emissions due to free excitons are strongly affected by polariton effects.