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1.
According to the density functional theory we systematically study the electronic structure, the mechanical prop- erties and the intrinsic hardness of Si2N2O polymorphs using the first-principles method. The elastic constants of four Si2N2O structures are obtained using the stress-strain method. The mechanical moduli (bulk modulus, Young’s mod- ulus, and shear modulus) are evaluated using the Voigt-Reuss-Hill approach. It is found that the tetragonal Si2N2O exhibits a larger mechanical modulus than the other phases. Some empirical methods are used to calculate the Vickers hardnesses of the Si2N2O structures. We further estimate the Vickers hardnesses of the four Si2N2O crystal structures, suggesting all Si2N2O phases are not the superhard compounds. The results imply that the tetragonal Si2N2O is the hardest phase. The hardness of tetragonal Si2N2O is 31.52 GPa which is close to values of β-Si3N4 and γ-Si3N4.  相似文献   

2.
The structural stability, mechanical properties and thermodynamic parameters such as Debye temperature, minimum thermal conductivities of orthorhombic-A2N2O (A=C, Si and Ge) are calculated by first principles calculations based on density functional theory. The calculated lattice parameters, elastic constants of Si2N2O and Ge2N2O using PBEsol function are consisted with the experimental data and other calculated values. The full set elastic constants of the orthorhombic-A2N2O (A=C, Si and Ge) are calculated by stress–strain method. The mechanical moduli (bulk modulus, shear modulus and Young's modulus) are evaluated by the Voigt–Reuss–Hill approach. The orthorhombic-C2N2O exhibits larger mechanical moduli than the other two structures. The hardness of orthorhombic-A2N2O (A=C, Si and Ge) is evaluated according to the intrinsic hardness calculation theory of covalent crystal relying on Mulliken overlap population. The results indicate that the orthorhombic-C2N2O is a super hard material. Furthermore, the mechanical anisotropy, Debye temperature and minimum thermal conductivity of the orthorhombic-A2N2O (A=C, Si and Ge) have been estimated by empirical methods. The orthorhombic-Ge2N2O shows the lowest thermal conductivity, which may have useful applications as gas turbine engines and diesel engines.  相似文献   

3.
The addition of carbon nanotubes (CNT) in ceramic composites has stimulated a substantial interest due to their high mechanical, thermal and electrical properties. This approach used fluoride additives (AlF3 and MgF2) to prepare multi-walled carbon nanotubes/silicon nitride (MWCNT/Si3N4) composite densified at 1700 °C for 1 h by hot press (HP) sintering. The microstructural analyses of MWCNT/Si3N4 composites indicate that the fluoride additives have substantially improved densification and the transformation of α-Si3N4 to β-Si3N4. As observed, the mechanical properties, i.e. flexural strength, fracture toughness, Young's modulus and hardness of MWCNT/Si3N4 composites are improved with an increasing concentration of MWCNT. These results attributed to the highly dense composites, strong interfacial interaction and the pull-out mechanism of MWCNT and β-Si3N4. The maximum values of fracture toughness flexural strength, Young's modulus, and hardness were 12.76 ± 1.15 MPa.m0.5, 883 ±46 MPa, 260 ±9 GPa, and 26.4 ± 1.3 GPa, respectively. The improved mechanical properties also ascribed to the synergistic strengthening and toughening influence of MWCNT and β-Si3N4.  相似文献   

4.
The new P-43m-Si3P2 and P-43m-Si3As2 structures are predicted using the first-principles approach based density functional theory (DFT). The elastic constants, structural stability, phonon dispersion spectra, band structures, density of states, and optical properties of P-43m-Si3×2 (X=N, P and As) have been analyzed. The values of the elastic constants indicate that their structures are mechanically stable. Each elastic constant of the Si3N2 is greater than the corresponding elastic constants of Si3P2 and Si3As2. The Young's moduli, shear moduli, bulk moduli, Pugh ratios and Poisson's ratios of P-43m-Si3×2 are calculated at 0 GPa. Si3N2 has a larger Young's modulus, so it has higher hardness and good resistance to deformation. The bulk moduli of P-43m-Si3×2 are isotropic. The shear modulus of Si3As2 is anisotropic. The Pugh ratios of P-43m-Si3×2 are 0.50, 0.49 and 0.39, respectively. Their Poisson's ratios are 0.28, 0.29 and 0.33, respectively. The results show that they are brittle materials at zero pressure. The calculated phonon spectra confirm that they are dynamically stable. The calculated enthalpy of formation indicates their thermodynamic stability. The energy band gaps of P-43m-Si3×2 calculated by HSE06 hybrid function are 0.786, 0.955 and 0.343 eV, respectively. Si3N2 has a direct bandgap, Si3P2 and Si3As2 have indirect bandgaps. The dielectric functions, refractive indices, optical reflectance spectra, absorption coefficients, conductivities and loss functions of P-43m-Si3×2 are calculated. The calculated static dielectric constants of P-43m-Si3×2 are 5.207, 9.237 and 10.072, respectively. The maximum values of the loss functions of P-43m-Si3×2 are 6.408, 5.672 and 5.276 eV, respectively.  相似文献   

5.
The structural, mechanical properties and hardness of the new carbon-rich material C11N4 are studied by first-principles total energy calculations based on the density-functional theory. We use the empirical equations of state (EOS) to investigate the lattice properties and bulk modulus. It is found that the calculated lattice constants and bulk modulus are in good agreement with previous calculations. And the full set elastic constants are calculated using the stress-strain method. The Voigt-Reuss-Hill approximation is used to evaluate the mechanical moduli. The elastic constants show that the two phases of C11N4 are mechanically stable. The tetragonal-C11N4 (α-C11N4) exhibits larger mechanical moduli than the orthorhombic-C11N4 (β-C11N4). The mechanical anisotropy is calculated of several different anisotropic indexes and factors, such as universal anisotropic index (AU), the percent anisotropy (AG and AB) and shear anisotropic factors (A1, A2 and A3). Furthermore, the hardness of α-C11N4 and β-C11N4 are evaluated according to the intrinsic hardness calculation theory. α-C11N4 is predicted to be a superhard material with the Vickers hardness of 67.17 GPa, which is slightly higher than that of the cubic boron nitride. And the β-C11N4 is also a superhard material with the calculated Vickers hardness of 45.63 GPa. C11N4 can be considered as candidate superhard compounds.  相似文献   

6.
γ-Si3N4在高压下的电子结构和物理性质研究   总被引:2,自引:0,他引:2       下载免费PDF全文
采用基于密度泛函平面波赝势方法(PWP)和广义梯度近似(GGA-PW91),计算了不同压强下γ-Si3N4的电子结构、光学性质和力学性质.基于计算结果,分析讨论了γ-Si3N4各物理参数随外压力的变化规律.计算表明,γ-Si3N4是一种适合于在高压条件下工作的材料.  相似文献   

7.
乌晓燕  孔明  李戈扬  赵文济 《物理学报》2009,58(4):2654-2659
采用反应磁控溅射法制备了一系列具有不同Si3N4层厚度的AlN/Si3N4纳米多层膜,利用X射线衍射仪、高分辨透射电子显微镜和微力学探针表征了多层膜的微结构和力学性能.研究了Si3N4层在AlN/Si3N4纳米多层膜中的晶化现象及其对多层膜生长结构与力学性能的影响.结果表明,在六方纤锌矿结构的晶体AlN调制层的模板作用下,通常溅射条件下以非晶态存在的Si3N4层在其厚度小于约1nm时被强制晶化为结构与AlN相同的赝形晶体,AlN/Si3N4纳米多层膜形成共格外延生长的结构,相应地,多层膜产生硬度升高的超硬效应.Si3N4随层厚的进一步增加又转变为非晶态,多层膜的共格生长结构因而受到破坏,其硬度也随之降低.分析认为,AlN/Si3N4纳米多层膜超硬效应的产生与多层膜共格外延生长所形成的拉压交变应力场导致的两调制层模量差的增大有关. 关键词: 3N4纳米多层膜')" href="#">AlN/Si3N4纳米多层膜 外延生长 赝晶体 超硬效应  相似文献   

8.
β-Si3N4电子结构和光学性质的第一性原理研究   总被引:1,自引:0,他引:1       下载免费PDF全文
潘洪哲  徐明  祝文军  周海平 《物理学报》2006,55(7):3585-3589
采用基于密度泛函的平面波赝势方法(PWP)和广义梯度近似(GGA),计算了β相氮化硅(β-Si3N4)的电子结构和光学性质,得到的晶格常数、能带结构等均与实验结果较好符合.进一步还研究了β-Si3N4的光吸收系数以及禁带宽度随外压力的变化规律,为β-Si3N4材料在高压条件下的应用提供了理论参考. 关键词: β相氮化硅 电子结构 能带结构 光学性质  相似文献   

9.
The fracture toughness property (K1C) of Si3N4 and ZrO2 engineering ceramics was investigated by means of CO2 and a fibre laser surface treatment. Near surface modifications in the hardness were investigated by employing the Vickers indentation method. Crack lengths and the crack geometry were then measured by using the optical microscopy. A co-ordinate measuring machine was used to investigate the diamond indentations and to measure the lengths of the cracks. Thereafter, computational and analytical methods were employed to determine the K1C. An increase in the K1C of both ceramics was found by the CO2 and the fibre laser surface treatment in comparison to the as-received surfaces. The K1C of the CO2 laser radiated surface of the Si3N4 was over 3% higher in comparison to that of the fibre laser treated surface. This was by softening of the near surface layer of the Si3N4 which comprised of lowering of hardness, which in turn increased the crack resistance. The effects were not similar in ZrO2 ceramic to that of the Si3N4 as the fibre laser radiation in this case had produced an increase of 34% compared to that of the CO2 laser radiation. This occurred due to propagation of lower crack resulting from the Vickers indentation test during the fibre laser surface treatment which inherently affected the end K1C through an induced compressive stress layer. The K1C modification of the two ceramics treated by the CO2 and the fibre laser was also believed to be influenced by the different laser wavelength and its absorption co-efficient, the beam delivery system as well as the differences in the brightness of the two lasers used.  相似文献   

10.
研究了Si3N4层在ZrN/Si3N4纳米多层膜中的晶化现象及其对多层膜微结构与力学性能的影响. 一系列不同Si3N4层厚度的ZrN/Si3N4纳米多层膜通过反应磁控溅射法制备. 利用X射线衍射仪、高分辨透射电子显微镜和微力学探针表征了多层膜的微结构和力学性能. 结果表明,由于受到ZrN调制层晶体结构的模板作用,溅射条件下以非晶态存在的Si3N4层在其厚度小于0.9 nm时被强制晶化为NaCl结构的赝晶体,ZrN/Si3N4纳米多层膜形成共格外延生长的柱状晶,并相应地产生硬度升高的超硬效应. Si3N4随层厚的进一步增加又转变为非晶态,多层膜的共格生长结构因而受到破坏,其硬度也随之降低.  相似文献   

11.
The structural, elastic, and electronic properties of a series of icosahedral phases, such as boron subcarbides B12C3 and B13C2, subnitride B12N2, and suboxide B12O2, have been studied in the framework of the SCC-DFTB method. It has been found that the B12C2 and B13C2 phases manifest metal-like properties, while B12C3 and B12O2 are semiconductors. The estimates have shown that the insertion of 2p atoms (C, N, or O) into intericosahedral pores of elemental boron can cause both a decrease in its elastic modulus (an increase in the compressibility of B12N2) and a sharp increase in the modulus B (in subcarbides B12C3 and B12BCC). On the other hand, the insertion of 2p atoms into α-B12 will favor an increase in its hardness (suboxide B12O2 will have a maximum hardness).  相似文献   

12.
Porous Si3N4 ceramics with photoluminescence properties were prepared by pressureless sintering using α-Si3N4 powder as raw material and Eu2O3 as sintering additive. Chemical composition, phase formation, microstructure and photoluminescence properties of porous Si3N4 ceramics were studied by X-ray photoelectron spectroscopy (XPS), X-ray diffraction (XRD), scanning electron microscopy (SEM) and photoluminescence measurements (PL/PLE). The results show that single Eu2O3 additive promotes α→β transformation but not significant densification. A broad band emission center at 570 nm assigned to Eu2+ is observed, Eu3+ in Eu2O3 is (partially) converted to Eu2+ by reaction with Si3N4, which results in a lower β aspect ratio and β-content compared to the other Ln (Ln=lanthanide) oxide additives.  相似文献   

13.
HfC/Si3N4 nanomultilayers with various thicknesses of Si3N4 layer have been prepared by reactive magnetron sputtering. Microstructure and mechanical properties of the multilayers have been investigated. The results show that amorphous Si3N4 is forced to crystallize and grow coherently with HfC when the Si3N4 layer thickness is less than 0.95 nm, correspondingly the multilayers exhibit strong columnar structure and achieve a significantly enhanced hardness with the maximum of 38.2 GPa. Further increasing Si3N4 layer thickness leads to the formation of amorphous Si3N4, which blocks the coherent growth of multilayer, and thus the hardness of multilayer decreases quickly.  相似文献   

14.
In this work, the new ternary nitrides (CSi2N4 and SiC2N4) are designed by the substitution method. The structures, elastic properties, intrinsic hardness and Debye temperature of the new ternary nitrides (CSi2N4 and SiC2N4) are studied by first-principles calculations based on the density-functional theory. The elastic constants CijCij of these new ternary nitrides are obtained using the stress–strain method. Derived elastic constants, such as bulk modulus, shear modulus, Young's modulus, Poisson coefficient and brittle/ductile behavior are estimated using Voigt–Reuss–Hill theories. The results indicate that γ-CSi2N4, p-CSi2N4 and p-SiC2N4 are mechanically stable. Calculated B/GB/G values and Poisson's ratio for γ-CSi2N4, p-CSi2N4 and p-SiC2N4 indicate that these materials are brittle. The calculated anisotropy parameters indicate that γ-CSi2N4 shows weak anisotropy and p-SiC2N4 and p-CSi2N4 have larger anisotropy. Based on the microscopic hardness model, p-CSi2N4, p-SiC2N4 and γ-CSi2N4 should be viewed as superhard materials with some peculiar mechanical properties.  相似文献   

15.
Silicon nitride (Si3N4) and oxynitride (Si2N2O) were deposited by chemical vapor infiltration (CVI) through a novel route involving the in-situ thermal decomposition of Na2SiF6 in commercial nitrogen precursors containing impurity oxygen. In addition, the quantitative effect of processing time (30, 60, 90, 120 min), temperature (1000, 1100, 1200 and 1300 °C), nitrogen precursor (N2 or N2-5%NH3) and gas flow rate (46.5, 93, 120 and 240 cm3/min) on phase percentage and deposition rate of Si3N4 and Si2N2O was investigated. Analysis of variance shows that the parameter that most significantly impacts the total amount of deposited phase is the processing temperature, followed by processing time and nitrogen precursor. Regardless of the nitrogen precursor, at 1300 °C, Si3N4 and Si2N2O depositions follow an S-like and parabolic behavior, respectively. The incubation period shown by Si3N4 in N2-5%NH3 is associated to a decrease in the O2 partial pressure during Si2N2O formation while the rapid increase at long processing times is attributed to the enhanced effect of hydrogen. PACS 81.15.Gh; 81.05.Je; 81.15.-z; 81.05.Rm; 47.85.L-  相似文献   

16.
In this work, new ternary cubic spinel structures are designed by the substitutional method. The structures, elasticity properties, intrinsic hardness and Debye temperature of the cubic ternary spinel nitrides are studied by first principles based on the density-functional theory. The results show that γ-CSn2N4, γ-SiC2N4, γ-GeC2N4 and γ-SnC2N4 are not mechanically stable. The elastic constants Cij of these cubic spinel structures are obtained using the stress–strain method. Derived elastic constants, such as bulk modulus, shear modulus, Young's modulus, Poisson coefficient and brittle/ductile behaviour are estimated using Voigt–Reuss–Hill theories. The B/G value, the Poisson's ratio and anisotropic factor are calculated for eight ternary stable crystals. Based on the microscopic hardness model, we further estimate the Vickers hardness of all the stable crystals. From the calculated hardness of the stable group IVA ternary spinel nitrides by Gao's and Jiang's methods, it is observed that the stable group IVA ternary spinel nitrides are not superhard materials except for γ-CSi2N4. Furthermore, the Debye temperature for the eight stable crystals is also estimated.  相似文献   

17.
The crystal structures, band structures, elastic constants, hardness, and optical properties of pyrite-type dinitrides (CN2, SiN2, and GeN2) are obtained from the density functional theory using the plane-wave pseudopotential (PWP) method within the local density and generalized gradient approximations. The formation enthalpies for AN2 (A=C, Si, and Ge) compounds suggest the three structures that are stable. The calculated band structures show the indirect gaps (ΓR) in CN2, SiN2, and GeN2. The intrinsic hardnesses of AN2 (A=C, Si, and Ge ) compounds are calculated. Our results show that the cubic CN2 and SiN2 are superhard materials. Furthermore, we studied the optical properties such as the complex dielectric function and the electron energy loss spectra.  相似文献   

18.
Two new transition metal dinitrides, ReN2 and WN2, with the P4/mmm structure are investigated by the first-principles calculations. The computed shear moduli of 327 GPa for ReN2 and 334 GPa for WN2 exceed those of all transition metal dinitrides previously reported. The estimated theoretical hardness are 46.3 GPa for ReN2 and 47.9 GPa for WN2, respectively. The calculated high shear moduli and hardness indicate that they are potential ultrahard materials. It is important to note that the computed hardness of the weakest bond are 34.7 GPa (W-N) for WN2 and 33.1 GPa (Re-N) for ReN2, much higher than that of 21.1 GPa (Re-B) for ReB2, which suggests that tetragonal ReN2 and WN2 are probably harder than ReB2. The total and partial electron density of states and the electron localization function for ReN2 and WN2 are analyzed. We attribute the high bulk modulus, shear modulus, and hardness to a three-dimensional covalently bonded framework in tetragonal ReN2 and WN2. Our calculations show that tetragonal ReN2 is expected to be synthesized above 62.7 GPa and tetragonal WN2 may be hard to be synthesized.  相似文献   

19.
采用基于密度泛函理论的线性丸盒轨道原子球近似(LMTO-ASA)从头计算方法,研究了β-C3N4,β-Si3N4和β-Ge3N4的能带结构,得到了它们的能隙分别为:4.1751,5.1788和4.0279eV。对于β-C3N4,由于N的部分2p电子占据了非键轨道,禁带宽度较窄;对于β-Si3N4关键词:  相似文献   

20.
The mechanical properties of bulk and nanoscale TiO2 phases are examined with a view to assess the available bulk modulus and hardness data, and to understand the size-dependent behaviors. The bulk modulus values of thermodynamically stable bulk TiO2 phases show a general correlation with Ti-O coordination number. As with the cotunnite-structured (OII) phase, it is likely that the seven-coordinated OI and eight-coordinated fluorite forms of TiO2 are ultrahard substances. Of the nanoscale phases investigated thus far, nanocrystalline anatase displays the strongest size dependence of bulk modulus values, with possible stiffening behavior effected by incipient grain boundary amorphization under pressure. Nanocrystalline rutile and baddeleyite phases do not show appreciable size dependence in their compression behaviors.  相似文献   

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