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1.
The formation and migration mechanisms of three different point defects (mono-vacancy, anti-site defect and interstitial atom) in B2-type MoTa alloy have been investigated by combining molecular dynamics (MD) simulation with modified analytic embedded-atom method (MAEAM). From minimization of the formation energy, we find that the anti-site defects MoTa and TaMo are easier to form than Mo and Ta mono-vacancies, while Mo and Ta interstitial atoms are difficult to form in the alloy. In six migration mechanisms of Mo and Ta mono-vacancies, one nearest-neighbor jump (1NNJ) is the most favorable due to its lowest activation and migration energies, but it will cause a disorder in the alloy. One next-nearest-neighbor jump (1NNNJ) and one third-nearest-neighbor jump (1TNNJ) can maintain the ordered property of the alloy but require higher activation and migration energies, so the 1NNNJ and 1TNNJ should be replaced by straight [1 0 0] six nearest-neighbor cyclic jumps (S[1 0 0]6NNCJ) or bent [1 0 0] six nearest-neighbor cyclic jumps (B[1 0 0]6NNCJ) and [1 1 0] six nearest-neighbor cyclic jumps ([1 1 0]6NNCJ), respectively. Although the migrations of Mo and Ta interstitial atoms need much lower energy than Mo and Ta mono-vacancies, they are not main migration mechanisms due to difficult to form in the alloy. 相似文献
2.
We present preliminary results on the structure of nano-sized particles (clusters of solute atoms or Guinier-Preston-Bagaryatsky (GPB) zones) in aluminum alloys. Hindering the motion of dislocations, these GPB zones (precipitates) are responsible for the strength of AlCuMg-alloys - used e.g. as AA2024 - for the outer shell plates in aircraft industry. We will discuss the role of quenched-in vacancies for the formation and growth of the precipitates. Using positron annihilation (Doppler broadening together with the recently developed tool of high-momentum analysis (HMA)) and X-ray absorption spectroscopy measurements, we are able to characterize the local atomic environment in the vicinity of vacancies and selected elements (Cu) forming the precipitates. The interpretation will be based on a comparison to numerical calculations of positron lifetimes and momentum distributions as well as simulated X-ray absorption spectra. Often reliable numerical calculations of experimental quantities are possible only if relaxed atomic positions - calculated employing an ab-initio code like SIESTA - are used as input. 相似文献
3.
Heavily trivalent ions doped into PbWO4 will exert a distinct influence on the scintillation performance and the conductivity of the crystal. In the light of the doping mechanism, the microstructure of the heavily La3+ doped and undoped PbWO4 crystals was studied using extended X‐ray absorption fine structure (EXAFS) and X‐ray Photoelectron Spectroscopy (XPS). When heavily doped, La3+ may substitute the W sites as well as the Pb2+ sites for self‐compensation by forming La dimers or La small aggregates, which results in a significant decrease in the light yield. Another charge compensator, the interstitial oxygen ion, was also observed and is discussed in this paper. 相似文献
4.
Internal friction behaviors of B2 Fe–Al alloys were examined to understand the correlation between the anelasticity and thermal vacancies. Three internal friction peaks were found in the rapidly cooled specimens at around 210 °C (P1), 410 °C (P2) and 520 °C (P3), respectively, while in the slowly cooled specimens, the P1 peak was significantly decreased and the P2 peak was decomposed into two peaks (P2L and P2H). All the internal friction peaks showed relaxational nature and they shifted toward high temperature with increasing frequency. It is suggested that the P1 peak originates from the reorientation of the divacancies composed of Fe vacancies and the nearest‐neighboring Al vacancies, the P2L peak from the dissociation and diffusion of the interstitial carbon atoms from the carbon‐vacancy complexes and the P2H peak from the reorientation of the triple defects. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
5.
The electronic structures of different types of PbWO4 (PWO) crystal have been studied within the framework of the fully relativistic self‐consistent Dirac–Slater theory, using a numerically discrete variational (DV‐Xα) method. In the calculation, the lattice relaxation of sheelite‐like PWO (Pb7.5W8O32) is considered. The densities of states and joint densities of states for sheelite and sheelite‐like PWO clusters are obtained. The calculated results indicate that the electronic structures of sheelite and sheelite‐like PWO clusters embedded in themselves are very similar. However, when the sheelite and sheelite‐like PWO clusters are embedded in each other the electronic structures change significantly; for example, peaks for density of states become undistinguishable, and some states even become forbidden. The calculated results show that stolzite‐type PWO may be the most stable structure and the physical properties of the PWO crystal are sensitive to its structure. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
6.
A novel nano‐porous oxide 12CaO·7Al2O3 (C12A7) can host a large concentration of interstitial ions, which are present in high concentrations of the order of 1021 cm–3. We use ab initio calculations and an embedded cluster approach to investigate the effect of the interstitial ions on the optical absorption of C12A7. It is demonstrated that the position of the absorption edge can shift in the range of at least 1.5 eV depending on the chemical composition of different interstitial ions. This property of C12A7 can be used for fabrication of materials with tuneable band gaps on the basis of the same lattice host. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
7.
The alloys of the Cu2CdSnSe4–Cu2MnSnSe4 system were investigated using the X‐ray powder method that showed the continuous solubility of the original system components at 670 K. The refinement of the crystal structures of Cu2MnSnSe4 (space group (SG) I&4macr;2m, a = 0.57362(4) nm, c = 1.14007(7) nm, c/a = 1.9875, RI = 0.0531, RP = 0.1186) and of the solid solution of Cu2Cd0.5Mn0.5SnSe4 composition (SG I&4macr;2m, a = 0.57935(2) nm, c = 1.14036(5) nm, c/a = 1.9683, RI = 0.0455, RP = 0.0902) was performed. It was established that Cd mixes statistically with Mn in its crystallographic position. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
8.
V. P. Sachanyuk A. O. Fedorchuk I. D. Olekseyuk O. V. Parasyuk 《physica status solidi b》2007,244(4):1288-1295
The compounds Cu2MnZrS4 and Cu2MnZrSe4 were obtained by solid‐state synthesis method. It was established using an XRD powder method that they crystallize in the hexagonal structural type (space group P3m1) with unit cell parameters a = 0.37427(2) nm, c = 0.61004(3) nm (Cu2MnZrS4); a = 0.39085(2) nm, c = 0.63709(3) nm (Cu2MnZrSe4). Atomic parameters were calculated using the anisotropic approximation (RI = 0.0523 and RI = 0.0473 for Cu2MnZrS4 and Cu2MnZrSe4, respectively). (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
9.
A.N. Kravtsova I.E. Stekhin A.V. Soldatov X. Liu M.E. Fleet 《physica status solidi b》2002,234(2):R4-R5
10.
M. Agundez D. Ruiz S. Van Petegem J. De Baerdemaeker K. W. Chou D. Segers Y. Houbaert 《physica status solidi (a)》2005,202(9):1751-1757
Positron annihilation lifetime and coincidence Doppler broadening measurements have been performed on ultra low carbon steel and Fe–Si alloys with different Si contents (from 3.32 up to 11.1 wt%) in the annealed state and after a deformation of 5% thickness reduction. It was seen that above 5.6 wt% Si the nature of the defects trapping the positron changes. This coincides with the concentration for the onset of long range D03 ordering in the Fe–Si alloys changing the nature of the dislocation structure. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
11.
Absorption, excitation in vacuum ultraviolet region, emission and decay of emission of alkaline‐earth crystals (CaF2, SrF2, BaF2) doped by different concentrations of YF3 or LaF3 were studied. New emission bands in the region 3–6 eV and excitation bands just below exciton edges were observed. Unempirical Hartree–Fock and density functional calculations of alkaline‐earth crystal clusters containing Y or La impurity were performed. We concluded that observed optical bands belong to transitions between interstitial fluorine and trivalent metal parts of pairs Me3+–F–i. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
12.
T. G. Berger A. Leineweber E. J. Mittemeijer P. Fischer 《physica status solidi (a)》2004,201(7):1484-1492
The mean square atomic displacement parameter of Pd in the fcc interstitial solid solution PdBy, 〈uPd2(y)〉, was determined for atomic ratios of y = 0.050, 0.100, and 0.184 using neutron powder diffraction data obtained at 15 K and 300 K. The values determined are significantly larger than those determined for pure Pd, 〈uPd2(0)〉, at the same temperatures. Assuming that the dynamic (thermal) contribution to 〈uPd2(y)〉 equals 〈uPd2(0)〉, the static mean square atomic displacement parameter 〈uPd2(y)〉st = 〈uPd2(y)〉 – 〈uPd2(0)〉 was obtained as 0.0020(1) Å2 to 0.0027(1) Å2. 〈uPd2(y)〉st showed no systematic variation with y or the sample temperature. This contrasts with an expected y(1 – y) concentration dependence for 〈uPd2(y)〉st. Comparison of 〈uPd2(y)〉st with values for the static mean square displacements of the metal atoms in different defect‐NaCl type transition metal nitrides and carbides indicates that the current values for Pd in PdBy are exceptionally small. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
13.
Czochralski‐grown dislocation‐free silicon crystals of 50 and 80 mm in diameter have been extensively studied by techniques of transmission electron microscopy and preferential etching. Crystals were grown at various growth rates, followed by subsequent processing (thermal treatment, ion implantation). The physical nature (positive/negative sign of silicon lattice imperfection) of grown‐in microdefects inside and within the OSF ring was determined. It was found that background oxygen and carbon impurities mostly affect the formation mechanism of grown‐in microdefects. It was shown that crystals might grow in interstitial and interstitial–vacancy regimes. The transformation scheme of the grown‐in microdefects in the course of subsequent processing is clarified. (© 2003 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
14.
S. A. Ahmad Razia Ramzan 《中国物理快报》2007,24(9):2631-2634
The interaction between small vacancy clusters and twin boundaries in copper is studied by using many-body potential developed by Ackland et aL for fcc metals. The interaction energies of single-, di- and tri-vacancy clusters with (111) and (112) twin boundaries are computed using well established simulation techniques. For (111) twins the vacancy clusters are highly repelled when they are on the adjacent planes, and are attracted when they are away from the boundary. In the case of (112) twins, vacancy clusters are more attracted to the boundary when they are near the boundary as compared to away from it. Vacancy clusters on both the sides of the boundary are also investigated, and it is observed that the clusters energetically prefer to lie on the off-mirror sites as compared to the mirror position across the twin. 相似文献
15.
M. Ellouze M.S. Ben Kraiem A. Cheikh‐Rouhou Ph. l'Hritier 《physica status solidi (a)》2002,189(3):865-869
The crystallographic and magnetic properties of Sm2Fe14—xCoxMn3 with x = 0, 1, 2, and 3 have been investigated using X‐ray diffraction and magnetic measurements. The Sm2Fe14—xCoxMn3 samples crystallised in the rhombohedral Th2Zn17 structure. The unit cell volume decreases with increasing Co concentration. The Curie temperature as well as the saturation magnetisation increases with increasing cobalt contents. The Curie temperature of Sm2Fe11Co3Mn3 is about 470 K and the saturation magnetisation is about 160 emu/g. All the samples exhibit an easy direction of magnetization along the c‐axis. 相似文献
16.
Local structure around Mn atoms in (MnS)2x (CuInS2)1–x alloys for x ≤ 0.09 has been determined using near‐edge and extended X‐ray absorption fine structure (XANES and EXAFS) measured at the Mn K‐edge. We found that for the Mn concentration up to 9 at% Mn atoms substitute preferentially for indium in the chalcopyrite lattice. The Mn–S bond length is 2.43 ± 0.015 Å, and is about 2% shorter than the In–S bond length. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
17.
C. Paduani J. Schaf A. I. C. Persiano M. T. Raposo J. D. Ardisson A. Y. Takeuchi 《physica status solidi b》2009,246(6):1362-1365
In this work we report the observation of weak ferromagnetism in the hexagonal C14 Laves phase (s.g. P63/mmc) of the (Fe1–x Nix)2Nb system, which has been reported as nonmagnetic in the literature. A larger unit cell volume is observed as compared to Fe2Nb. From low‐temperature magnetization measurements it is found that the Ni substitution for Fe indeed leads to the onset of a weak ferromagnetic ordering in the C14 Laves phase of this pseudobinary system. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
18.
It is shown that the equations for the concentrations of atomic defects in B2 compounds obtained by the established grand‐canonical approach are equivalent to the master equations derived recently by Ren and Otsuka within the framework of the empirical nearest‐neighbour pair interaction model. Because the grand‐canonical approach is not bound to any specific calculational method for the determination of the defect energetics, these master equations are valid beyond the pair interaction model originally used for their derivation. 相似文献
19.
M. Heidari Saani M. A. Vesaghi K. Esfarjani A. Shafiekhani 《physica status solidi b》2006,243(6):1269-1275
Many‐electron calculations based on a generalized Hubbard Hamiltonian for electronic states of the diamond vacancies are reported. The model does not use the configuration interaction (CI) method and proper tetrahedral symmetry and spin properties of the defect are included in the Hamiltonian. Atomic orbital bases are introduced for the Hamiltonian calculation. Excited states of both neutral and negatively charged vacancies in diamond are calculated. The calculated values for the experimentally observed first dipole transition energies of the vacancies in diamond, GR1 and ND1 bands, are in good agreement with experiment. To obtain these results, we used a semi‐empirical Hamiltonian parameter. The position of the low‐lying 3T 1 state was found to be 260 meV above the ground state, which is consistent with experimental expectations. In addition to the energy spectrum, the model gives all eigenfunctions of the vacancies, which have not been calculated before. This model has high potential for further applications in point defects of diamond and other semiconductors. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
20.
The electronic structures of CaWO4 crystals with interstitial oxygen atoms are studied within the framework of the fully relativistic self‐consistent Dirac–Slater theory, using a numerically discrete variation (DV‐Xα) method. It is concluded by the calculation that interstitial oxygen atoms combine with two formal lattice oxygen ions forming oxygen molecular ions, which exhibits donor energy level locating in the forbidden bands. The optical transition energy is 3.85 eV, which correspond to the 324 nm absorption bands. It is predicted that the 324 nm absorption bands originate from the interstitial oxygen in CaWO4 crystals. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献