1951
Flexible heterostructures based on metal phthalocyanines thin films obtained by MAPLE
Socol, M; Preda, N; Rasoga, O; Breazu, C; Stavarache, I; Stanculescu, F; Socol, G; Gherendi, F; Grumezescu, V; Popescu-Pelin, G; Girtan, M; Stefan, N
JUN 30 2016, APPLIED SURFACE SCIENCE, 374, 410
DOI: 10.1016/j.apsusc.2015.10.166
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Heterostructures based on zinc phthalocyanine (ZnPc), magnesium phthalocyanine (MgPc) and 5,10,15,20-tetra(4-pyrydil)21H,23H-porphine (TPyP) were deposited on ITO flexible substrates by Matrix Assisted Pulsed Laser Evaporation (MAPLE) technique. Organic heterostructures containing (TPyP/ZnPc(MgPc)) stacked or (ZnPc(MgPc):TPyP) mixed layers were characterized by X-ray diffraction-XRD, photoluminescence-PL, UV-vis and FTIR spectroscopy. No chemical decomposition of the initial materials was observed. The investigated structures present a large spectral absorption in the visible range making them suitable for organic photovoltaics applications (OPV). Scanning electron microscopy-SEM and atomic force microscopy-AFM revealed morphologies typical for the films prepared by MAPLE. The current-voltage characteristics of the investigated structures, measured in dark and under light, present an improvement in the current value (similar to 3 order of magnitude larger) for the structure based on the mixed layer (Al/MgPc:TPyP/ITO) in comparison with the stacked layer (Al/MgPc//TPyP/ITO). A photogeneration process was evidenced in the case of structures Al/ZnPc:TPyP/ITO with mixed layers. (C) 2015 Elsevier B.V. All rights reserved.
1952
Multi-stage pulsed laser deposition of aluminum nitride at different temperatures
Duta, L; Stan, GE; Stroescu, H; Gartner, M; Anastasescu, M; Fogarassy, Z; Mihailescu, N; Szekeres, A; Bakalova, S; Mihailescu, IN
JUN 30 2016, APPLIED SURFACE SCIENCE, 374, 150
DOI: 10.1016/j.apsusc.2015.10.093
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We report on multi-stage pulsed laser deposition of aluminum nitride (AlN) on Si (100) wafers, at different temperatures. The first stage of deposition was carried out at 800 degrees C, the optimum temperature for AlN crystallization. In the second stage, the deposition was conducted at lower temperatures (room temperature, 350 degrees C or 450 degrees C), in ambient Nitrogen, at 0.1 Pa. The synthesized structures were analyzed by grazing incidence X-ray diffraction (GIXRD), transmission electron microscopy (TEM), atomic force microscopy and spectroscopic ellipsometry (SE). GIXRD measurements indicated that the two-stage deposited AlN samples exhibited a randomly oriented wurtzite structure with nanosized crystallites. The peaks were shifted to larger angles, indicative for smaller inter-planar distances. Remarkably, TEM images demonstrated that the high-temperature AlN "seed" layers (800 degrees C) promoted the growth of poly-crystalline AlN structures at lower deposition temperatures. When increasing the deposition temperature, the surface roughness of the samples exhibited values in the range of 0.4-2.3 nm. SE analyses showed structures which yield band gap values within the range of 4.0-5.7 eV. A correlation between the results of single and multi-stage AlN depositions was observed. (C) 2015 Elsevier B.V. All rights reserved.
1953
Role of the dithiolate backbone on the passivation of p-GaAs(111)B surface
Preda, L; Anastasescu, M; Dobrescu, G; Negrila, C; Lazarescu, V
JUN 15 2016, JOURNAL OF ELECTROANALYTICAL CHEMISTRY, 771, 63
DOI: 10.1016/j.jelechem.2016.03.046
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Effects of the self-assembled layers of biphenyl 4,4'-dithiol (BPDT) and 1,8-octanedithiol (ODT) on the chemical and electronic properties of p-doped GaAs (111)-As terminated substrate, (p-GaAs(111)B), were investigated in order to evidence whether the hydrocarbon moiety plays a role in tailoring the semiconductor surface properties. The electrochemical properties of the BPDT and ODT coated p-GaAs(111)B substrates were studied by Electrochemical Impedance Spectroscopy (EIS). The structural and chemical changes caused by the dithiolate layers formed on p-GaAs(111)B substrates were monitored by Atomic Force Microscopy (AFM) and X-ray Photoelectron Spectroscopy (XPS) investigations, respectively. The XPS data showed that BPDT and ODT bind to pGaAs(111)B via the thiol group. The ODT layer provides better protection against the further oxidation in air of p-GaAs(111)B substrate compared to the BPDT layer. The EIS investigations are in good agreement with XPS results, pointing to better insulating properties of the ODT layer compared to the BPDT layer in the electron transfer at the electrode/solution interface. The results evidenced that backbone plays an important role in tailoring the properties of p-GaAs(111)B substrate. (C) 2016 Elsevier B.V. All rights reserved.
1954
Assessment of structural, optical and conduction properties of ZnO thin films in the presence of acceptor impurities (vol 28, 224008, 2016)
Plugaru, R; Plugaru, N
JUN 8 2016, JOURNAL OF PHYSICS-CONDENSED MATTER, 28
DOI: 10.1088/0953-8984/28/18/189601
1955
Assessment of structural, optical and conduction properties of ZnO thin films in the presence of acceptor impurities
Plugaru, R; Plugaru, N
JUN 8 2016, JOURNAL OF PHYSICS-CONDENSED MATTER, 28
DOI: 10.1088/0953-8984/28/22/224008
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The structural, optical and electrical conduction properties of (Li/Cu,N):ZnO codoped thin films synthesized by the sol-gel method were investigated by field emission scanning electron microscopy (FESEM), x-ray diffraction (XRD), transmission and absorption, photoluminescence (PL) and I-V measurements in order to bring evidence of the formation of acceptor centers by dual-acceptor codoping processes. The (Li 3%, N 5%): ZnO films consist of crystallites with average size of 15 nm, show 95% transmission in the visible region, and an optical band gap of 3.22 eV. The PL spectra show emission maxima at 3.21 and 2.96 eV which are related to the emission of acceptor centers and the presence of defects, respectively. Li occupies interstitial sites and may form Lii-N(O) defect complexes that act as acceptor centers. The (Cu 3%, N 5%): ZnO films consist of crystallites with average size of 12 nm, and exhibit 90% transmission in the visible region. The PL spectra reveal band edge emission at 3.23 eV and defect related emission at 2.74 eV. In the (Cu, N) codoped films, copper substitutes zinc and adopts mainly the Cu1+ state. A possible defect complex involving Cu and N determines the transition from n-to p-type conductivity. These findings are in agreement with results of electronic structure calculations at the GGA-PBE level.
1956
Exciton-phonon interaction in CdS of different morphological forms manifested as stimulated Raman scattering
Baibarac, M; Nila, A; Baltog, I
JUN 1 2016, OPTICAL MATERIALS EXPRESS, 6, 1895
DOI: 10.1364/OME.6.001881
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Raman studies performed on different morphologies of CdS samples indicate an exciton-phonon interaction (EPI) that manifests at low temperatures by different enhancements in intensity of the Raman spectra in the Stokes and anti-Stokes branches. This effect, interpreted as stimulated Raman effect, is conditioned on the appearance and strength by the degree of overlap of the excitation laser light with the excitonic photoluminescence band. EPI is greatest in samples characterized by high light diffusing power, which means a long path of light into the sample and a great overlapping of the two optical fields, i.e., the pump laser and excitonic light. (C) 2016 Optical Society of America
1957
Correlation between strain and defects in Bi implanted Si
Palade, C; Lepadatu, AM; Slav, A; Ciurea, ML; Lazanu, S
JUN 2016, JOURNAL OF PHYSICS AND CHEMISTRY OF SOLIDS, 93, 32
DOI: 10.1016/j.jpcs.2016.02.005
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The strain in Si containing group-V impurities is a topical subject of study due to its potential applications in quantum computing. In this paper we study Bi-209 implanted Si concerning the correlation between the strain produced by stopped Bi ions and trapping characteristics of the defects resulted from implantation. The depths distributions of stopped ions and primary defects are simulated and the distributions of permanent defects are modelled for Si implanted with low fluence Bi-209 ions of 28 MeV kinetic energy. For comparison, these depths distributions were similarly calculated for I-127 ions with the same fluence and energy, implanted in Si. The results are compared with each other and correlated with the characteristics of traps in these systems, previously obtained. We demonstrate that the intensity of the strain field is the most important factor in changing of trap parameters, while the superposition between the region with strain and the region where defects are located is a second order effect. (C) 2016 Elsevier Ltd. All rights reserved.
1958
Intrinsic pyroelectric properties of thick, coarse grained Ba1-xSrxTiO3 ceramics
Ianculescu, A; Pintilie, I; Vasilescu, CA; Botea, M; Iuga, A; Melinescu, A; Dragan, N; Pintilie, L
JUN 2016, CERAMICS INTERNATIONAL, 42, 10348
DOI: 10.1016/j.ceramint.2016.03.152
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The intrinsic pyroelectric properties of thick, coarse grained Ba1-xSrxTiO3 (BST) ceramics were studied in relation with Sr content. The intrinsic values of the pyroelectric coefficient were determined directly from the frequency dependence of the measured pyroelectric signal by adapting the formalism developed for thin films deposited on thick substrates to thick and non-uniformly heated ceramics with uniform composition. Ceramic pellets, of about 1 mm thickness, with relative density of 89-95% were prepared using powder synthesized by the sol gel method. It was found that the intrinsic pyroelectric properties are enhanced by increasing the Sr content, while other features (e.g. tetragonality, grain size, polarization, transition temperature) decrease. The best intrinsic pyroelectric properties were obtained for 30% Sr content. The present results open the possibility to use large and thick BST ceramic pellets for manufacturing detectors useful for monitoring high power lasers. (C) 2016 Elsevier Ltd and Techna Group S.r.l. All rights reserved.
1959
Up-conversion luminescence of BaCl2:Er3+ nanocrystals embedded in oxychloride nano-glass ceramic
Secu, M; Secu, CE
JUN 2016, JOURNAL OF THE EUROPEAN CERAMIC SOCIETY, 36, 1703
DOI: 10.1016/j.jeurceramsoc.2016.01.016
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A novel glassy nanocomposite containing Er3+-doped BaCl2 nanocrystals of about tens of nm embedded in a silicate matrix has been prepared by using sol-gel route followed by controlled crystallization of the xerogel. Under 810 nm laser light pumping it shows green ((H-2(11/2), S-4(3/2)) -> I-4(15/2)) and red (F-4(9/2) -> I-4(15/2)) up-conversion luminescences ascribed by a two-photon processes. The luminescence signal recorded in the oxychloride nano-glass ceramic is only about 10% compared to the NaYF4:Er3+ (18%). In the nano glass ceramic there are effective non-radiative decay channels, most probably related to hydroxyl ions and surface defects acting as centers for the non-radiatively energy dissipation. (C) 2016 Elsevier Ltd. All rights reserved.
1960
Al2O3-cBN composites sintered by SPS and HPHT methods
Klimczyk, P; Cura, ME; Vlaicu, AM; Mercioniu, I; Wyzga, P; Jaworska, L; Hannula, SP
JUN 2016, JOURNAL OF THE EUROPEAN CERAMIC SOCIETY, 36, 1789
DOI: 10.1016/j.jeurceramsoc.2016.01.027
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Spark Plasma Sintering (SPS) and High Pressure-High Temperature (HPHT) methods were chosen in order to study the behaviour of metastable cubic boron nitride (cBN) during sintering of Al2O3 + 30 vol.% cBN composites at low and high pressure. Relatively low sintering temperatures were used to avoid the undesired reverse transformation of cBN to hexagonal, graphite-like form. The microstructure, and phase composition as well as physical and mechanical properties of the resulting Al2O3-cBN composites were investigated. In the ball-on-disc tests, the coefficient of friction and the specific wear rate of the sintered samples were determined by rotating the sample against a stationary alumina ball. The best composites obtained by SPS (at 1300 degrees C/75 MPa) had slightly lower density, Young's modulus and hardness than those obtained by HPHT but their wear resistance was much better. Formation of hBN was suppressed up to 1300 degrees C during SPS consolidation at the pressure of 75 MPa. (C) 2016 Elsevier Ltd. All rights reserved.