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1.
Time-resolved mass spectrometric data show that the concentration of di- and trisilane, which are formed from monosilane under discharge conditions typical for the deposition of high electronic quality amorphous silicon, correlate with the measured deposition rate of a-Si. The data can be quantitatively and self-consistently described by a simple set of consecutive reactions:
  1. SiH4 →-SiH2 + H2
  2. SiH2 + SiH4 → Si2H6
  3. SiH2 + Si2H6 → Si3H8
  4. Si n H2(n + 1)n ·a-Si:H+(n+1)H2,n=2,3
The only fitting parameter necessary for an excellent fit of the measured data over a wide range of experimental parameters is the value of the reactive sticking coefficient .for the decomposition of di- and trisilane (reaction 3). The resultant value agrees well with the published data of other authors and with those calculated from the measured deposition rate and Si2H6, concentration. We did not find and physically meaningful way to lit the measured data with the various “SiH3 models” proposed by other authors who assumed that the dominant species responsiblefor the deposition of a-Si: H is the SiH3, radical. For this and some additional reasons mentioned in the present paper. the SiH3 model is in disagreement with available experimental data.  相似文献   

2.
Gas‐phase reactions of SiHx with Si2Hy (x = 1,2,3,4; y = 6,5,4,3) species, respectively, which may coexist under chemical vapor deposition (CVD) conditions, have been investigated by means of ab initio molecular orbital and statistical theory calculations. Potential energy surface (PES) predicted at the CCSD(T)/CBS//B3LYP/6–311++G(3df,2p) level shows that these reactions take place primarily via trisilany radicals, n‐Si3H7 and i‐Si3H7. For example, SiH2 can associate with Si2H5 producing n‐H2SiSiH2SiH3 exothermically by 55.8 kcal/mol; SiH3 can undergo addition to H2SiSiH2 to produce n‐Si3H7 or associate with H3SiSiH barrierlessly forming i‐Si3H7; whereas SiH can insert into one of the Si─H bonds of Si2H6 to give excited n‐Si3H7. Similarly, H2SiSiH and SiSiH3 can undergo insertion reactions with SiH4 producing n /i‐Si3H7 intermediates, respectively, to be followed by fragmentation to various smaller species. These processes are fully depicted in the complete PES. The predicted heats of formation of various species agree well with available thermochemical data. The rate constants and product branching ratios for the low‐energy channel products have been calculated for the temperature range 300–1000 K by variational RRKM (Rice–Ramsperger–Kassel–Macus) theory with Eckart tunneling corrections. The results may be employed for realistic kinetic modeling of the plasma‐enhanced chemical vapor deposition growth of a‐Si:H thin films under practical conditions.  相似文献   

3.
Gas phase ion—molecule reactions occurring in GeH4/SiH4 systems under different partial pressures and their mechanisms have been investigated by ion trap mass spectrometry (ITMS). SiH+n (n=0–3) and GeH+n (n = 0–3) are the main ionic species at zero reaction time when the GeH4: SiH4 ratio is in the range 1:1 to 1:12. Self-condensation sequences are observed at increasing reaction times. Moreover, formation of ions containing GeSi bonds, such as GeSiH+n (in = 2–5) and GeSi2H+n (n = 4, 5), occurs by reactions of Si2H+n (n = 2–5) and Si3H+n (n = 4, 5) with GeH4. At longer reaction times, further substitution of silicon with germanium in GeSiH+n (n = 2–5) ions has been observed, to give Ge2H+n (n = 2–5).  相似文献   

4.
Two-photon ionization mass spectra are obtained for NH3H2O binary clusters both with a nozzle beam and an ArF excimer laser. The detected major ions are H+(NH3)n(H2O)m(1 <m + n < 9). The results suggest that ammonia molecules constitute an inner shell which is surrounted by water molecules.  相似文献   

5.
Zusammenfassung Die Darstellung von Si2H5J sowie von Si2H4J2 (SiH3–SiHJ2+SiH2J–SiH2J), Si3H7J (SiH3–SiH2–SiH2J+SiH3–SiHJ–SiH3) und Si3H6J2 (Isomerengemisch) durch Umsetzung der entsprechenden Silane mit elementarem Jod (ohne Verwendung eines Lösungsmittels) wird mitgeteilt. Durch katalytische Mengen Alkohol wird die Reaktion von Jod mit Silanen beschleunigt, gleichzeitig jedoch die Spaltung der Si–Si-Bindung gefördert.
Preparation of disilanyl iodide and trisilanyl iodide
The preparation of Si2H5J as well as Si2H4J2 (SiH3–SiHJ2+SiH2J–SiH2J), Si3H7J (SiH3–SiH2–SiH2J+SiH3–SiHJ–SiH3) and Si3H6J2 (isomeric mixture) by reaction of the corresponding silanes with elementary iodine without using a solvent is communicated. The reaction of iodine with silanes is accelerated by catalysings amounts of alcohol. At the same time, however, the cleavage of the Si–Si-bond is stimulated.


Mit 3 Abbildungen

19. Mitt.:F. Fehér, D. Schinkitz undH. Strack, Z. anorg. allgem. Chem.385, 202 (1971).

B. Mostert, Dissertation Univ. Köln 1961.

A. G. Wronka, Dissertation Univ. Köln 1961.

G. Betzen, Dissertation Univ. Köln 1967,G. Betzen, Diplomarbeit Univ. Köln 1963.  相似文献   

6.
Ditopic complex formation of silene H2SiCH2 with bidentate ligands Me2NCH2SiHnF3-n (n = 0-3) was studied at the MP4(SDQ(T)6-311G(d,p))//MP2/6-31G(d,p) levels of theory. The AIM and ELF analyses have shown that π-bonding in the silenic Si1C moiety in the relatively weak (H2Si1CH2)·(Me2NCH2Si2HnF3-n) (n = 2, 3) ditopic complexes is partially preserved.  相似文献   

7.
The problem of the prediction of the valence IPs for silanes is considered. It is shown that the data on the silicon band structure combined with the photoelectron spectra of SiH4, and Si2H6 permit to obtain the parameter scale, which includes all the nearest neighbour, second neighbour and the main third neighbour interaction parameters. Using the derived parameter scale the vertical ionization potentials of Si3H8, SiH(SiH3)3, Si(SiH3)4, the infinite polysilane valence band structure and the inner a 1g level for disilane are calculated. All the calculated levels are located above ? 20 eV and are expected to be measurable by the He (I) photoelectron spectroscopy.  相似文献   

8.
The electronic structure of a series of phenylsilanes Ph4?n SiH n (n = 0?C3) is studied by X-ray emission spectroscopy and quantum chemical calculations by the density functional theory method. Based on the calculations theoretical X-ray emission SiK??1 spectra of phenylsilanes Ph4?n SiH n (n = 0?C4) are constructed and their energy structure and shape turn out to be well consistent with experiment. The distribution of the electron density of states with different symmetry of Si, C, H atoms are also constructed. An analysis of the obtained X-ray fluorescent SiK??1 spectra and the distribution of the electron density of states in Ph4Si and Ph3SiH compounds shows that their energy structure is mainly determined by a system of the energy levels of phenyl ligands weakly perturbed by interactions with valence AOs of silicon. In the energy structure of MOs of the PhSiH3 compound, energy orbitals related to t 2 and a 1 levels of tetrahedral SiH4 are mainly presented.  相似文献   

9.
Zusammenfassung Von den Jodderivaten der Silane SiH4, Si2H6 und Si3H8 werden Dichte, Dampfdruck und Molrefraktion sowie die entsprechenden Atom- und Bindungsinkremente mitgeteilt. Die Ramanspektren von SiH3J, Si2H5J und Si3H7J werden aufgenommen und zugeordnet.
Spectroscopic and other physical investigations of silanyl iodides
Density, vapour pressure and molecular refraction as well as the corresponding atom increments and bond increments of the iodine derivatives of the silanes SiH4, Si2H6 and Si3H8 are communicated. The Raman spectra of SiH3J, Si2H5J and Si3H7J are recorded and assigned.


XX. Mitt.:F. Fehér, B. Mostert, A. G. Wronka undG. Betzen, Mh. Chem.103, 959 (1972).

A. G. Wronka, Dissertation Univ. Köln 1961.

B. Mostert, Dissertation Univ. Köln 1961.  相似文献   

10.
The interaction between S2 molecule and SiHx (x=1, 2, 3) in porous silicon is investigated using the B3LYP method of density functional theory with the lanl2dz basis set. The model of porous silicon doped with CH3,Si-O-Si and OH species is built. By analyzing the binding energy and electronic transfer, we conclude that the interaction of S2 molecule with SiHx (x=1, 2, 3) is much stronger than the interaction of S2 molecule with CH3 and OH, as S2 molecule is located in different sites of the model. Using the transition state theory, we study the Si2H6+S2→H3SiH2SiS+HS reaction, and the reaction energy barrier is 50.2 kJ/mol, which indicates that the reaction is easy to occur.  相似文献   

11.
Mass spectrometry has been used to assess plasma composition during a low-energy plasma-enhanced chemical vapor deposition (LEPECVD) process using argon-silane-hydrogen (Ar-SiH4-H2) gas mixtures with input flows of 50 sccm Ar, 2–20 sccm SiH4 and 0–50 sccm H2 at total pressures of 1–4 Pa. Energy-integrated ion densities, residual gas analysis and threshold ionization mass spectrometry have been used to characterize the transition from amorphous (a-Si) to nano-crystalline silicon (nc-Si) deposition at constant LEPECVD operating parameters. While relative ion densities have a marked decrease with H2 input, the densities of SiHx (x < 4) radicals show evolution trends depending on the SiH4 and H2 input. For conditions leading to nc-Si growth a turning point is reached above which SiH is the main radical. Observed SiHx density trends with H2 input are explained based on kinetic reaction rates calculated from previously obtained Langmuir probe data.  相似文献   

12.
Tunneling spectra of Al2O3/—SiHx, MgO/—SiHx, Al2O3/—SiDx, and Al2O3/—SiHx + NCS? are reported. Analysis of the vibrational spectra observed from isotopic substitution of the barriers obtained by deposition of a thin film of SiO onto alumina and magnesia indicate that the supported species is —SiH. The Al2O3/—SiH barrier can be used as a support for studying inorganic ions by IETS.  相似文献   

13.
For plasma enhanced and catalytic chemical vapor deposition (PECVD and Cat‐CVD) processes using small silanes as precursors, disilanyl radical (Si2H5) is a potential reactive intermediate involved in various chemical reactions. For modeling and optimization of homogeneous a‐Si:H film growth on large‐area substrates, we have investigated the kinetics and mechanisms for the thermal decomposition of Si2H5 producing smaller silicon hydrides including SiH, SiH2, SiH3, and Si2H4, and the related reverse reactions involving these species by using ab initio molecular‐orbital calculations. The results show that the lowest energy path is the production of SiH + SiH4 that proceeds via a transition state with a barrier of 33.4 kcal/mol relative to Si2H5. Additionally, the dissociation energies for breaking the Si? Si and H? SiH2 bonds were predicted to be 53.4 and 61.4 kcal/mol, respectively. To validate the predicted enthalpies of reaction, we have evaluated the enthalpies of formation for SiH, SiH2, HSiSiH2, and Si2H4(C2h) at 0 K by using the isodesmic reactions, such as 2HSiSiH2 + 1C2H61Si2H6 + 2HCCH2 and 1Si2H4(C2h) + 1C2H61Si2H6 + 1C2H4. The results of SiH (87.2 kcal/mol), SiH2 (64.9 kcal/mol), HSiSiH2 (98.0 kcal/mol), and Si2H4 (68.9 kcal/mol) agree reasonably well previous published data. Furthermore, the rate constants for the decomposition of Si2H5 and the related bimolecular reverse reactions have been predicted and tabulated for different T, P‐conditions with variational Rice–Ramsperger–Kassel–Marcus (RRKM) theory by solving the master equation. The result indicates that the formation of SiH + SiH4 product pair is most favored in the decomposition as well as in the bimolecular reactions of SiH2 + SiH3, HSiSiH2 + H2, and Si2H4(C2h) + H under T, P‐conditions typically used in PECVD and Cat‐CVD. © 2013 Wiley Periodicals, Inc.  相似文献   

14.
Hydrogen molybdenum bronzes HxMoO3 (~0.3 < x < 2.0) have been investigated with elastic and inelastic neutron scattering. Neutron diffraction studies of orthorhombic D0.36MoO3 show that deuterium is incorporated as -OD without any major structural change to the MoO3 layer lattice. The inelastic neutron scattering spectra of HxMoO3 phases confirm that, for H0.34MoO3, H is present as -OH, but, for the monoclinic phases H0.93MoO3, H1.68MoO3 and H2.0MoO3, only peaks associated with -OH2 groups are found.  相似文献   

15.
This paper reports on a mass spectrometric study of the neutral and ionic species in a low-pressure rf discharge sustained in a C2H4-SiH4 mixture diluted in helium. It is shown that C2H4 is readily decomposed into C2H 2 * and C2H3. The formation of secondary products such as C4H2, C4H4, and C4H6 is observed and confirms the presence of C2H2 in the discharge. Methylsilane (CH3SiH3) and ethylsilane (C2H5SiH3) are also synthesized in this discharge. It is also observed that the major ions C2H 4 + , C3H 5 + , SiH 3 + , Si2H 4 + , SiCH 3 + , SiC2H 3 + , and SiC2H 7 + are not representative of the direct ionization of neutral species. Their formation is thus interpreted on the basis of ion-molecule reactions.  相似文献   

16.
A complete vibrational study of xerogels of vanadium oxide corresponding to the formula V2O5 · nH2O with n = 1.6, 1.2, 0.6, 0.4, and 0.3, was performed. Raman and infrared spectra of powder and oriented films of the samples have been recorded at 100 and 300 K. It has been possible to verify the existence of two different structures. For n = 0.3, V2O5 layers are connected as in the crystal through VOV bonds, each water molecule trapped into cavities being linked by its two hydrogen atoms to the oxygen lattice, the interlayer distance (b parameter) should be close to that of the crystal. For n = 0.6, the V2O5 layers are not connected as in the crystal through the long VO bonds, but the vanadium atoms are coordinated to H2O molecule by VOH2 bonds. For 0.6 < n < 1.4 three kinds of water molecules are likely present. Finally, it is shown that the conclusions are consistent with the literature structural models proposed from diffraction methods.  相似文献   

17.
Ab initio molecular orbital calculations using an extended Gaussian basis set have been performed on C2H4, CH2SiH2 and Si2H4. The species CH2 and SiH2 have also been examined. Geometries were partially optimized and the energy difference between the planar singlet and orthogonal or twist triplet geometries of Si2H4 was studied in order to provide a measure of the strength of the Si-Si bond in this molecule. Mulliken population analyses were carried out on CH2CH2 and SiH2SiH2, to further study the nature of the Si-Si double bond in comparison with the C—C double bond.  相似文献   

18.
The substitution reactions of H2SiLiF (A) with SiH3XH n?1 (X = F, Cl, Br, O, N; n = 1, 1, 1, 2, 3) have been studied using DFT and ab initio methods. The results indicate that the substitution reactions of A with SiH3XH n?1 proceed via two reaction paths, I and II. The following conclusions emerge from this work. (i) The substitutions of A with SiH3XH n?1 are nucleophilic reactions and occur in a concerted manner. Path I is more favorable than path II. The substitution barriers of A with SiH3XH n?1 for path I decrease with the increase of the atomic number of X for the same period systems, whereas the barriers increase with the increase of the atomic number of X for the same family systems. (ii) The substitution products are H2SiFSiH3 and LiXH n?1. If the H atoms in SiH3 of SiH3XH n–1 are substituted by different atoms or groups, silanes H2SiFSiH3 obtained via paths I and II would be enantiomers. (iii) All the substitution reactions of A with SiH3XH n?1 are exothermic.  相似文献   

19.
Differences between SiH+5 and CH+5 are more significant than the similarities. The proton affinity of SiH4 exceeds than of CH4 by ≈25 kcal/mol. but the heat of hydrogenation of SiH+3 is smaller than that of CH+3 by nearly the same amount. Like CH+5 the C5 structures of SiH+5 are preferred, but SiH+5 is best regarded as a weaker SiH+3—H2 complex. D3h, C2v, and C4v forms are much higher in energy and SiH+5 should not undergo hydrogen scrambling (pseudorotation) readily, as does CH+5 The neutral BH5 is only weakly bound toward loss H2, and the D3h. C2v, and C4v forms are also high in energy. The contral-atom electronegativities, C+ > B > Si+, control this behavior. The electronegativities also determine the ability to bear positive charges. Thermodynamically. SiH+5 and SiH+3 are more stable than CH+5 and CH+3, respectively; hydride transfer occurs from SiH4 to CH+3 and proton transfer from CH+5 to SiH4.  相似文献   

20.
Formation of Organosilicon Compounds. 111. The Hydrogenation of Si-chlorinated, C-spiro-linked 2,4-Disilacyclobutanes with LiAlH4 or iBu2AlH. The Access to Si8C3H20 The hydrogenation of Si-chlorinated, C-spiro-linked 2,4-disilacyclobutanes containing C(SiCl3)2 terminal groups with LiAlH4 in Et2O proceeds under complete cleavage of the fourmembered rings and under elimination of one SiH3 group. Such, Si8C3Cl20 4 forms (H3Si)2CH? SiH2? CH(SiH3)? SiH2? CH(SiH3)2 4 α, and even Si8C3H20 4a with LiAlH4 forms 4 α. The hydrogenation of related compounds containing however CH(SiCl3) terminal groups similarly proceeds under ring cleavage but no SiH3 groups are eliminated. Such, (Cl3Si)CH(SiCl2)2CH(SiCl3) 41 forms (H3Si)2CH? SiH2? CH2(SiH3) 41 α. However, in reactions with iBu2AlH in pentane neither the disilacyclobutane rings are cleaved nor are SiH3 groups eliminated. Only by this method Si8C3H20 is accessible from 4 , Si6C2H16 3a from Si6C2Cl16 3 and Si4C2H12 41a from 41 . C(SiCl3)4 cleanly produces C(SiH3)4. Based on the knowledge about the different properties of LiAlH4 and iBu2AlH in hydrogenation reactions of disilacyclo-butanes it was possible to elucidate the composition and the structures of the hydrogenated derivatives of the product mixture from the reaction of MeCl2Si? CCl2? SiCl3 with Si(Cu) [1] and to trace them back to the initially formed Si chlorinated disilacyclobutanes Si6C2Cl15Me 34 , Si6C2Cl14Me2 35 , Si8C3Cl19Me 36 and Si8C3Cl18Me2 37 . Compound 4a forms colourless crystals of space group P1 with a = 799.7(6), b = 1263.6(12), c = 1758.7(14) pm, α = 103.33(7)°, β = 95.28(6)°, γ = 105.57(7)° and Z = 4.  相似文献   

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