共查询到19条相似文献,搜索用时 0 毫秒
1.
Xiaofeng Guo Tingyu Liu Min Song Jigang Yin Haiyan Zhang Xi’en Wang 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2009,267(7):1093-1096
The electronic structures of perfect crystals of barium molybdate (BaMoO4) and of crystals containing F and F+ color centers are studied within the framework of the fully relativistic self-consistent Dirac-Slater theory by using the numerically discrete variational (DV-Xα) method. The calculated results suggest that the donor energy level of the F center as well as F+ center is located within the band gap. The respective optical transition energies are 1.86 eV and 2.105 eV corresponding to the wavelength of the absorption band of 668 nm and 590 nm. It is therefore suggested that these bands are originate from the F and F+ centers in the crystal. 相似文献
2.
Jigang Yin Tingyu Liu Xiaofeng Guo Min Song Xien Wang Haiyan Zhang 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2009,267(1):74-78
The positions of the interstitial oxygen atoms in LiYF4 crystal are simulated by computer technologies. It is found that the total energy of cluster is low when interstitial oxygen atoms exist around the Li+ ion. Basing on the computer results, the electronic structures of perfect LiYF4 and the LiYF4 containing interstitial oxygen atoms with the lattice structure optimized are studied within the framework of the density functional theory. By analyzing the calculated results it can be concluded that an interstitial oxygen atom could combine with formal lattice fluorine ions forming molecular ions, which cause the 260 nm absorption band. 相似文献
3.
Hailing Qiao Qiren Zhang Xiuwen Zhou 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2009,267(15):2467-2470
The most likely substituting positions of impurity oxygen ions in LiBaF3 crystals are studied using the general utility lattice program (GULP). The calculated results indicate that the main defect model is [] in the O:LiBaF3 crystal. The electronic structures of the LiBaF3 crystal with the defect [] are calculated using the DV-Xα method. It can be concluded from the electronic structures that the LiBaF3 crystal with the defect [] will exhibit a 217-280 nm absorption band and the impurity oxygen will decrease core-valence luminescence yield. 相似文献
4.
Zexu Shao Tingyu Liu Jianyu Chen 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2008,266(5):797-801
A computer simulation has been performed to study the intrinsic defects in CaWO4. The inter-atomic interaction potentials are empirically fitted to the known crystal properties. The results reveal that the predominant intrinsic defects existed in the crystal should be oxygen Frenkel-type. Calculated formation energies of electronic defects suggest that the hole is easier to be trapped by oxygen ion than by calcium ion, and oxygen would prior to occupy the oxygen vacancy during the annihilation under oxidation atmosphere. An analysis of activation energy shows that oxygen vacancy migration is movable ionic defects in CaWO4. 相似文献
5.
We have investigated the behavior of He in UO2, using the projector-augmented-wave (PAW) method and the generalized gradient approximation (GGA) based on the density functional theory. Total energy calculations with atomic relaxation included have been performed in a 96-atom large supercell. We have found that He has a strong tendency to form a cluster in vicinity of an octahedral interstitial site (OIS) in the UO2 matrix. In addition, the strain energy produced by a He-cluster was found to be sufficient to create point defects of the host atoms in UO2. Our study suggests that He-clusters and He-induced point defects play an important role for the local mechanical properties of UO2. 相似文献
6.
B. Canut A. Ayari M. Lemiti S. Ramos 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2009,267(6):917-920
Silicon nitride layers of 140 nm thickness were deposited on silicon wafers by low pressure chemical vapour deposition (LPCVD) and irradiated at GANIL with Pb ions of 110 MeV up to a maximum fluence of 4 × 1013 cm−2. As shown in a previous work these irradiation conditions, characterized by a predominant electronic slowing-down (Se = 19.3 keV nm−1), lead to damage creation and formation of etchable tracks in Si3N4. In the present study we investigated other radiation-induced effects like out of plane swelling and refractive index decrease. From profilometry, step heights as large as 50 nm were measured for samples irradiated at the highest fluences (>1013 cm−2). From optical spectroscopy, the minimum reflectivity of the target is shifted towards the high wavelengths at increasing fluences. These results evidence a concomitant decrease of density and refractive index in irradiated Si3N4. Additional measurements, performed by ellipsometry, are in full agreement with this interpretation. 相似文献
7.
Fang Cheng Qiren Zhang Hailin Qiao Xiuwen Zhou 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2010,268(15):2403-2407
The experiments indicate that the perfect KMgF3 crystal has no absorption in the visible range, however the electron irradiation induces a complex absorption spectrum. The absorption spectra can be decomposed by five Gaussian bands peaking at 2.5 eV (488 nm), 3.4 eV (359 nm), 4.2 eV (295 nm), 4.6 eV (270 nm) and 5.2 eV (239 nm), respectively. The purpose of this paper is to seek the origins of the absorption bands. The electronic structures and absorption spectra either for the perfect KMgF3 or for KMgF3: with electrical neutrality have been studied by using density functional theory code CASTEP with the lattice structure optimized. The calculation results predicate that KMgF3: also exhibits five absorption bands caused by the existence of the fluorine ion vacancy and the five absorption bands well coincide with the experimental results. It is believable that the five absorption bands are related to in KMgF3 crystal produced by the electron irradiation. 相似文献
8.
We have performed ab initio total energy calculations to investigate the behavior of helium and its diffusion properties in uranium dioxide (UO2). Our investigations are based on the density functional theory within the generalized gradient approximation (GGA). The trapping behavior of He in UO2 has been modeled with a supercell containing 96-atoms as well as uranium and oxygen vacancy trapping sites. The calculated incorporation energies show that for He a uranium vacancy is more stable than an oxygen vacancy or an octahedral interstitial site (OIS). Interstitial site hopping is found to be the rate-determining mechanism of the He diffusion process and the corresponding migration energy is computed as 2.79 eV at 0 K (with the spin-orbit coupling (SOC) included), and as 2.09 eV by using the thermally expanded lattice parameter of UO2 at 1200 K, which is relatively close to the experimental value of 2.0 eV. The lattice expansion coefficient of He-induced swelling of UO2 is calculated as 9 × 10−2. For two He atoms, we have found that they form a dumbbell configuration if they are close enough to each other, and that the lattice expansion induced by a dumbbell is larger than by two distant interstitial He atoms. The clustering tendency of He has been studied for small clusters of up to six He atoms. We find that He strongly tends to cluster in the vicinity of an OIS, and that the collective action of the He atoms is sufficient to spontaneously create additional point defects around the He cluster in the UO2 lattice. 相似文献
9.
G. Kuri D. Gavillet D. Novikov 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2008,266(8):1216-1223
The present work is devoted to investigate the local atomic environment (of Zr, Y and O) as well as surface modifications associated with excess helium in the cubic phase of (1 0 0)-oriented Zr0.8Y0.2O1.9 single crystal substrates. Commercially available oxide crystals have been implanted at various fluences in the range 0.15-2.0 × 1016 He-atoms/cm2 using a 2.74 MeV He+ ion beam passing through a 8.0 μm Al foil. The microstructure and surface morphology of the irradiated surface are examined using atomic force microscopy (AFM). The local atomic environments of Zr, Y and O in the implanted layer are studied using synchrotron radiation and by extended X-ray absorption fine structure (EXAFS) measured at glancing angles to probe the implanted layer. From AFM studies it was observed that the surface roughness increases as fluence increases and above a critical fluence stage, small blister-like structures originating from helium bubbles are scattered on the irradiated surface. The radial distribution functions (RDFs), derived from EXAFS data at the Zr K-edge, have been found to evolve continuously as a function of ion fluence describing the atomic scale structural modifications in YSZ by helium implantation. From the pristine data, long range order (beyond the first- and second-shell) is apparent in the RDF spectrum. It shows several nearest neighbour peaks at about 2.1, 3.6, 4.3 and 5.4 Å. In the implanted specimens, all these peaks are greatly reduced in magnitude and their average positions are changed, typical of damaged material. A simple model taking into account only the existence of lattice vacancies has been used for the interpretation of measured EXAFS spectra. 相似文献
10.
11.
Wen Deng Li Yue Wei Zhang Xu-xin Cheng Yan-yan Zhu Yu-yang Huang 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2009,267(18):3094-3096
Two-detector coincidence system and mono-energetic slow positron beam has been applied to measure the Doppler broadening spectra for single crystals of SiO2, SiO2 films with different thickness thermally grown on single crystal of Cz-Si, and single crystal of Si without oxide film. Oxygen is recognized as a peak at about 11.85 × 10−3m0c on the ratio curves. The S parameters decrease with the increase of positron implantation energy for the single crystal of SiO2 and Si without oxide film. However, for the thermally grown SiO2-Si sample, the S parameters in near surface of the sample increase with positron implantation energy. It is due to the formation of silicon oxide at the surface, which lead to lower S value. S and W parameters vary with positron implantation depth indicate that the SiO2-Si system consist of a surface layer, a SiO2 layer, a SiO2-Si interface layer and a semi-infinite Si substrate. 相似文献
12.
The influence of grain boundaries on the primary damage state created by a recoil nucleus in UO2 matrix is studied here by molecular dynamics simulations. This study is divided in two steps: (1) the study of the structural properties of several symmetrical tilt boundaries for different misorientation angles ranging from 12.7° to 61.9°; and (2) the study of displacement cascades near these grain boundaries. For all the grain boundaries studied, the structure around the interface up to about 2 nm presents a perturbed but stable fluorite lattice. The type of defect at the interface depends directly on the value of the misorientation angles. For the small angles (12.7° and 16.3°) the interface defects correspond to edge dislocations. For higher misorientation angles, a gap of about 0.3 nm exists between the two halves of the bicrystal. This gap is composed of Schottky defects involving numerous vacancies along the interface. About 10 keV displacement cascades were initiated with an uranium projectile close to the interface. In all the cases, numerous point defects are created in the grain boundary core, and the mobility of these defects increases. However, cascade morphologies depend strongly on the grain boundary structure. For grain boundaries with edge dislocations, the evolution of the displacement cascades is similar to those carried out in monocrystals. On the other hand, cascades initiated in grain boundaries with vacancy layer defects present an asymmetry on the number of displaced atoms and the number of point defects created. 相似文献
13.
Yuxiang Chen Ying Ma Yichun Zhou 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2009,267(18):3090-3093
In order to study the radiation effects in BaTiO3 ferroelectric crystal, a previously developed shell model is modified. The modifications include adding the ZBL universal potentials at short distances and distance-dependent spring constants for core-shell interactions. The phase transition sequences in BaTiO3 were correctly reproduced using molecular dynamics simulations with this modified shell model. Also, the calculated Frenkel pair formation energies agree well with results obtained by first principles calculations, which suggests that this model is suitable for the simulation of the radiation effects in BaTiO3. The dependence of polarization on the number of oxygen vacancies was also studied. 相似文献
14.
Intragranular bubbles grow in the nuclear fuel by diffusion and precipitation of fission gases, mainly xenon; and are ultimately destroyed, under irradiation, by fission fragments. This article will attempt to determine the in-pile bubble distributions taking into account the evolution of the concentration profile around a bubble during its growth and the destruction process by fission fragments. From these distributions a relation between the bubble mean radius and the diffusion coefficient of xenon can be established, allowing the determination, from experimental measurements of intragranular bubble sizes, of the in-pile Xe diffusion coefficient in UO2. The estimated activation energy (0.9 eV) is about one order of magnitude lower than the widely used value of 3.9 eV determined from out-of-pile experiments. This effect can be attributed to the presence of point defects created by the irradiation. 相似文献
15.
Sanju Rani N.K. Puri M.C. Bhatnagar 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2008,266(9):1987-1992
Swift heavy ion irradiation has been successfully used to modify the structural, optical, and gas sensing properties of SnO2 thin films. The SnO2 thin films prepared by sol-gel process were irradiated with 75 MeV Ni+ beam at fluences ranging from 1 × 1011 ion/cm2 to 3 × 1013 ion/cm2. Structural characterization with glancing angle X-ray diffraction shows an enhancement of crystallinity and systematic change of stress in the SnO2 lattice up to a threshold value of 1 × 1013 ions/cm2, but decrease in crystallinity at highest fluence of 3 × 1013 ions/cm2. Microstructure investigation of the irradiated films by transmission electron microscopy supports the XRD observations. Optical properties studied by absorption and PL spectroscopies reveal a red shift of the band gap from 3.75 eV to 3.1 eV, and a broad yellow luminescence, respectively, with increase in ion fluence. Gas response of the irradiated SnO2 films shows increase of resistance on exposure to ammonia (NH3), indicating p-type conductivity resulting from ion irradiation. 相似文献
16.
Gujie Qian A. Guerra Yuan Shuanglong Guorong Chen 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2007,262(2):276-280
Irradiation resistance of as-studied scintillating glass samples were tested under the 60Co γ-ray radiation at doses between 60 and 700 Gy. Photoluminescence properties of glasses with and without cerium ions were investigated to show the effect of cerium (III) on the luminescence of ZnO. Ultraviolet and visible optical transmittance spectra were compared before and after irradiation treatment. The so-called radiation-induced absorption coefficient (RIAC) was introduced to compare more effectively the radiation damage on glass samples. The much reduced transmittance change and decreased RIAC value in UV-Vis region indicate that the density of electron centers and hole centers caused by radiation decreased, which helps to confirm that the reduction and oxidation reaction of cerium ions took place in radiation process. From RIAC curves, it can be seen that TiO2 enhances the irradiation resistance of sample in UV region. However, high TiO2 content has negative effect on visible transmittance of glasses after the higher dose irradiation (700 Gy). 相似文献
17.
A. Upadhyay R. Rai 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2008,266(11):2594-2598
KNaSO4:Tb3+ phosphors were synthesized by melt technique with different concentration of Tb3+ ions and MgSO4:Dy3+ phosphor is prepared by solid state diffusion method. Lyoluminescence and photoluminescence characterization of KNaSO4:Tb and MgSO4:Dy3+ phosphors are reported in this paper. Only one sharp peak is observed in the lyoluminescence (LL) glow curve and KNaSO4:Tb(0.05 mol%) phosphor shows maximum efficiency. The LL intensity increases linearly with gamma ray dose. LL emission occurs in the blue and yellow region of the spectrum. Photoluminescence (PL) characterization of KNaSO4:Tb(0.05 mol%) phosphor shows PL emission at 486 and 546 nm. These PL emissions from KNaSO4:Tb3+ are due to 5D4 → 7F6 and 5D4 → 7F5 transitions of Tb3+ ion respectively. Lyoluminescence of MgSO4:Dy3+ phosphor shows the high sensitivity to γ-ray exposure and LL emission observed at 486 and 572 nm in the blue and yellow emission of the spectrum is due to Dy3+ ion. Experimental results obtained in the present investigation show that KNaSO4:Tb3+ and MgSO4:Dy3+ phosphors are suitable as a lyoluminescence dosimetry phosphor for ionizing radiations. 相似文献
18.
A. Tataro?lu ?. Alt?ndal M.H. Bölükdemir G. Tan?r 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2007,264(1):73-78
The Au/SiO2/n-Si (MOS) structures were exposed to beta-ray irradiation to a total dose of 30 kGy at room temperature. Irradiation effect on dielectric properties of MOS structures were investigated using capacitance−voltage (C−V) and conductance−voltage (G/ω−V) characteristics. The C−V and G/ω−V measurements carried out in the frequency range from 1 kHz to 10 MHz and at various radiation doses, while the dc voltage was swept from positive bias to negative bias for MOS structures. The dielectric constant (ε′), dielectric loss (ε″), loss factor (tan δ) and ac electrical conductivity (σac) were calculated from the C−V and G/ω−V measurements and plotted as a function of frequency at various radiation doses. A decrease in the ε′ and ε″ were observed when the irradiation dose increased. The decrease in the ε′ and ε″ of irradiated MOS structures in magnitude is explained on the basis of Maxwell−Wagner interfacial polarization. Also, the σac is found to decrease with increasing radiation dose. In addition, the values of the tan δ decrease with increasing radiation dose and give a peak. From the experimental results, it is confirmed that the peak of loss tangent is due to the interaction between majority carriers and interface states which induced by radiation. 相似文献
19.
Ram Prakash R.J. Choudhary D.M. Phase 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2008,266(8):1242-1246
Thin films of Fe3O4 have been deposited on single crystal MgO(1 0 0) and Si(1 0 0) substrates using pulsed laser deposition. Films grown on MgO substrate are epitaxial with c-axis orientation whereas, films on Si substrate are highly 〈1 1 1〉 oriented. Film thicknesses are 150 nm. These films have been irradiated with 200 MeV Ag ions. We study the effect of the irradiation on structural and electrical transport properties of these films. The fluence value of irradiation has been varied in the range of 5 × 1010 ions/cm2 to 1 × 1012 ions/cm2. We compare the irradiation induced modifications on various physical properties between the c-axis oriented epitaxial film and non epitaxial but 〈1 1 1〉 oriented film. The pristine film on Si substrate shows Verwey transition (TV) close to 125 K, which is higher than generally observed in single crystals (121 K). After the irradiation with the 5 × 1010 ions/cm2 fluence value, TV shifts to 122 K, closer to the single crystal value. However, with the higher fluence (1 × 1012 ions/cm2) irradiation, TV again shifts to 125 K. 相似文献