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1.
The exposure (in air) of As38S62 amorphous film was found to be accompanied (i) by significant structural changes in the film matrix (an increase of As-S bond density as indicated by IR spectroscopy), and (ii) by darkening of the film. No indications of photo-oxidation have been found. Exposure and subsequent annealing of the well-annealed film are accompanied by reversible changes of the As-S bond density, as indicated by the results of differential infrared spectroscopy. The dispersion of the refractive index of the virgin, annealed and exposed films can be described using the Wemple-DiDomenico (W-D) single-oscillator formula. Annealing- and exposure-induced changes of the parameters of the W-D formula follow the changes of both the optical gap and the As-S bond density. 相似文献
2.
Changes in the transmission, absorption edge and refractive coefficient in the UV-VIS and the transmission in the IR spectrum of thin As-Ge-S films after irradiation with an argon laser with =488 nm were studied. X-ray microanalysis showed that the composition of the films (with small variations) corresponded to that of the initial substances. Films with a defined concentration of the elements could also be deposited by evaporation of As2S3 and GeS2 from two sources. The optical properties of thin films prepared by thermal evaporation, flash evaporation and coevaporation from two crucibles have been compared. It was found that depending on the component content, both photodarkening and photobleaching coatings in a wide region of can be obtained in thin As-Ge-S films. The results have been explained from the viewpoint of the photostructural changes in chalcogenide layers. 相似文献
3.
Yoo IH Bae SH Koo H Kwon OJ Yoo J Kang S Park C 《Journal of nanoscience and nanotechnology》2012,12(4):3673-3676
Films of amorphous In(1-x)Sn(x)GaZnO(delta) (a-ISGZO) (x = 0.0-1.0) were pulsed laser deposited at a temperature range of room temperature to 300 degrees C, and in order to systematically investigate the effect of replacing In with Sn on the properties of amorphous In-Ga-Zn-O (a-IGZO), the electrical and optical properties were measured. The amount of Sn in the deposited film, which was determined by X-ray photoelectron spectroscopy, was very close to the composition of the targets used. Hall mobility and carrier concentration decreased, and resistivity increased as the amount of Sn in the film increased. It was observed that the increase of Sn concentration in films was accompanied by the decrease of oxygen vacancy concentration, which led to the decrease of carrier concentration. The electrical mobility was decreased as the amount of Sn increased, which can be attributed to the increased number of subgap states, which was determined by the UV/VNIS spectrophotometer. Optical transparencies of all samples were larger than 80% in the visible light range. Band gap values were also found to increase as the amount of Sn increased. 相似文献
4.
Neutral red (NR) is polycrystalline in powder form, it transforms to nanocrystallite phase upon thermal deposition. Gamma-ray irradiation with doses 1.25–6 KGy induced partial transformation of nanocrystallite phase to amorphous structure. The changes of optical constants with γ-ray doses were calculated using spectrophotometer measurements of transmittance and reflectance at normal incidence of light over spectral range 200–2500 nm. The complex refractive index of NR film is highly influenced by exposure to γ-ray irradiation, the onset and optical energy gaps decrease with increasing γ-ray doses, and Urbach tail increases linearly with increasing irradiation dose. The type of electronic transition, oscillator, and electric dipole strengths and dispersion parameters were determined before and after irradiation. The spectral behavior of dielectric constant with γ-ray doses was also estimated. 相似文献
5.
Thermally and optically induced irreversible changes in the optical gap and refractive index were studied for sulphur rich, nearly stoichiometric and sulphur poor Ge–As–S amorphous films prepared by thermal evaporation. For films studied the optical gap in the virgin state decreases from 2.559 (Ge0.121As0.172S0.707) to 1.632 eV (Ge0.254As0.294S0.452) and simultaneously the refractive index increases from 2.21 to 2.87, respectively. The most sensitive composition to illumination seems to be nearly stoichiometric film (Ge0.153As0.201S0.646), where the blue shift of the gap is observed close to 150 meV. Sulphur poor film (Ge0.254As0.294S0.452) was found insensitive to illumination. Highest thermally induced blue shift of the gap, close to 250 meV, we observed just for Ge0.254As0.294S0.452 film and for this film it was observed also nearly “giant” decrease in refractive index from 2.85 to 2.42. The behaviour of Ge0.254As0.294S0.452 film is qualitatively discussed using the concept of network rigidity (insensitivity to illumination) and assuming thermally induced changes in bonding arrangement (refractive index changes). 相似文献
6.
Metal-free 1,4,8,11,15,18,22,25-octahexylphthalocyanine was prepared directly by the cyclotetramerization of 3,6-dihexylphthalonitrile using lithium butoxide in butanol. Thin films of the material were deposited on glass substrates by the thermal evaporation technique. The structure of the films was found to be in the form, and showed a strong peak indicating preferential orientation. The surface morphology of the thin films was investigated by atomic force microscopy and showed that the molecules of 1,4,8,11,15,18,22,25-octahexylphthalocyanine grow in stacks of parallel rows. The spectrophotometric measurements of transmittance and reflectance were carried out in the wavelength range 190–3000 nm. The refractive index, n, and absorption index, k, were found to be independent of annealing at 373 K. The B band absorption occurred at 356 nm, and the Q band showed a doublet at 667 and 739 nm. Other optical parameters, such as absorption coefficient and optical dielectric constant ε, were determined. 相似文献
7.
《Optical Materials》2005,27(3):491-498
Thermally evaporated zinc phthalocyanine (ZnPc) films in the as deposited condition were identified to be as-amorphous. It undergoes structural transformation upon annealing up to 613 K. The optical properties and spectral behavior of as deposited and annealed thin films of ZnPc were studied using spectrophotometric measurements of the transmissivity and reflectivity at normal incidence of light in the wavelength range 200–2500 nm. The refractive index, n, and absorption index, k, were calculated and it was found that they are independent of film thickness in the thickness range 205–530 nm. Annealing at 613 K increases absorbance of films by 5–6 times in comparison with absorbance of as deposited ones and shifts peak positions of all bands towards low energy side of spectra except the peak position of N-band is shifted towards high energy side of spectra. The absorption spectra in the UV–VIS. region has been analyzed in terms of both molecular orbital and band theories. Indirect allowed transitions near the onset and fundamental absorption edges were observed. The energy at the onset was obtained and equals to 1.45 and 1.51 eV for as deposited and annealed films, respectively. The fundamental energy gap was obtained and equals to 2.94 and 2.88 eV for as deposited and annealed films, respectively. The absorption spectra shows four absorption bands. The oscillator strength, f, the electric dipole strength, q2, the molar extinction coefficient, ζmolar, were calculated for as deposited and annealed ZnPc thin films. 相似文献
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10.
Zhen Su Manwen Yao Fei Li Yong Peng Qian Feng Xi Yao 《Journal of Materials Science》2017,52(16):9314-9323
Dielectric Al2?x B x OY thin films were deposited onto Pt (100)/Ti/SiO2/Si substrates via sol–gel and spin-coating technology. The microstructural transition occurred at ~500 °C due to boron loading was confirmed by DSC and XRD. FTIR, 27Al MAS NMR and XPS measurements were employed to investigate the microstructural transition caused by different boron concentrations. The results revealed that Al–O–B bonds and [AlO4] tetrahedrons were produced resulting in the reinforcement of structure with relatively low boron concentrations. With the increase of boron concentration, [BO3] chains and new surfaces crossing over the internal structure gradually produced and disrupted the structural stability. Meanwhile, hydroxyl groups were accumulated in the internal structure owing to the hydrophilic property of boron. According to the reinforced structure with low boron concentrations, the current density decreased and the breakdown strength was enhanced. Typically, the current density was decreased two orders of magnitude at 100 MV m?1 and the breakdown strength of the 0.5 mol% B-doped alumina thin film was increased by 59% (from 293 to 465 MV m?1) in comparison with that of the undoped alumina thin film, whereas the dielectric properties gradually become poor due to the weak structure with the increase of boron concentration. Moreover, the dielectric constant increased owing to hydroxyl groups when the boron doping increased. This work may provide a general strategy for enhancing dielectric properties of the alumina thin film. 相似文献
11.
Changes in transmittance, refractive index, transmissivity in the infrared spectral region, and activation energy of the dissolution process were studied for thin films of the system As
x
S100–x
(28.6 x45) as they result from illumination and annealing at temperatures of T
g
. It is assumed that the irreversible changes occurring in the layers after treatment are accompanied by an increase in the concentration of As-S bonds. This leads to an increase in dissolution rate, a decrease in the activation energy of the process, and considerable changes in the absorption peaks at 370 and 310 cm–1 obtained by infrared spectroscopy. It is shown that the photo- and thermoinduced changes in as-deposited chalcogenide films follow identical courses. The results obtained are explained from the viewpoint of the structural changes occurring in chalcogenide films. 相似文献
12.
S. K. J. Al-Ani C. A. Hogarth S. W. D. B. Abeysuriya 《Journal of Materials Science》1985,20(7):2541-2548
Amorphous films of Ge-SiO have been co-evaporated and some of their optical properties are reported. The optical constants have been measured and estimated. At the high absorption end of the absorption edge, an equation due to non-direct transitions inK-space is found to match the optical absorption data. The variation of the optical band gapE
opt with film composition is reported. The infrared spectrum of a mixed layer is presented and a simple conclusion is drawn. 相似文献
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14.
Sang Yeol Lee Do Hyung Kim Bosul KimHyun Kwang Jung Dae Hwan Kim 《Thin solid films》2012,520(10):3796-3799
Thermally induced instability of amorphous Si-In-Zn-O (SIZO) with 1 wt.% silicon (Si) concentration and Ga-In-Zn-O (GIZO) with gallium (Ga) of 30 wt.% thin film transistors (TFTs) has been investigated, by comparing the density of states extracted from multi-frequency method. It was observed that the density of state of SIZO-TFT was lower than that of GIZO-TFT, in spite of low processing temperature of SIZO-TFT and thermally induced instability of SIZO- and GIZO-TFT was strongly related with the total trap density. We report that Si of only 1 wt.% in SIZO can improve thermal stability of threshold voltage of In-Zn-O based TFTs more effectively than Ga of 30 wt.% in GIZO. 相似文献
15.
Adil D Kanimozhi C Ukah N Paudel K Patil S Guha S 《ACS applied materials & interfaces》2011,3(5):1463-1471
Two donor-acceptor diketopyrrolopyrrole (DPP)-based copolymers (PDPP-BBT and TDPP-BBT) have been synthesized for their application in organic devices such as metal-insulator semiconductor (MIS) diodes and field-effect transistors (FETs). The semiconductor-dielectric interface was characterized by capacitance-voltage and conductance-voltage methods. These measurements yield an interface trap density of 4.2 × 10(12) eV?1 cm?2 in TDPP-BBT and 3.5 × 1012 eV?1 cm?2 in PDPP-BBT at the flat-band voltage. The FETs based on these spincoated DPP copolymers display p-channel behavior with hole mobilities of the order 10?3 cm2/(Vs). Light scattering studies from PDPP-BBT FETs show almost no change in the Raman spectrum after the devices are allowed to operate at a gate voltage, indicating that the FETs suffer minimal damage due to the metal-polymer contact or the application of an electric field. As a comparison Raman intensity profile from the channel-Au contact layer in pentacene FETs are presented, which show a distinct change before and after biasing. 相似文献
16.
Two series of glass and thin film specimens of BaO-TeO2 were prepared. The optical absorption edges and infrared absorption spectra were investigated. It was found that the fundamental absorption edge is a function of BaO content in both kinds of films and that the absorption is due to indirect electronic transitions. The values of optical gap for blown films were greater than those of thin evaporated films, but the widths of the band tails were greater for the evaporated thin films, which were expected to be more disordered than the thin blown glass films. 相似文献
17.
Hyeunseok Cheun Frank Galbrecht Benjamin Nehls Ullrich Scherf Michael J. Winokur 《Journal of Materials Science: Materials in Electronics》2009,20(Z1):498-504
The top and bottom interfaces of spin cast poly(di-n-octylfluorene) (PF8) and poly[bis(2-ethylhex-yl)fluorene] (PF2/6) films are investigated by optical absorption and emission
spectroscopy. In this study both the pure polyfluorene homopolymers and random copolymers comprised of linear di-n-octyl (F8) and the branched bis(2-ethylhexyl) (F2/6) units are used. PF2/6 is noted for forming a single conformationally
disordered helix whereas PF8 adopts a number of near-planar conformational isomers. PF2/6, PF8 and their copolymers form asymmetric
films in which the local structure at or near the top and bottom interfaces are distinctly different. This asymmetry is least
apparent in pure PF2/6 films but increases in F8 containing polymers. In polymers containing a large fraction of F2/6 monomers
the substrate-polymer side exhibits chains with slightly improved intrachain structural order and also increased green band
emission. The effects of thermal and solvent vapor annealing are also reported. 相似文献
18.
以酒石酸与柠檬酸钠为络合剂,采用化学水浴法(CBD)沉积ZnS薄膜.利用X射线衍射仪(XRD)、X射线能谱仪(EDAX)、扫描电镜(SEM)、紫外-可见分光光度计(UV-Vis)研究ZnS薄膜的结构、组成、形貌及光学性能,利用透射光谱计算ZnS薄膜的光学禁带宽度(Eg).结果表明:ZnS薄膜呈立方相晶体结构,经过300℃熟处理1h的ZnS薄膜原子比为Zn:S=1:0.85,表面均一致密,在可见光区的平均透射率达到80%,光学禁带宽度为3.74ev,适合作为太阳能电池过渡层. 相似文献
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