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51.
By the use of complete orthonormal sets of -exponential-type orbitals, where ( = 1, 0, –1, –2,...) the multicenter electronic attraction (EA), electric field (EF) and electric field gradient (EFG) integrals of nonscreened and Yukawa-like screened Coulomb potentials are expressed through the two-center overlap integrals with the same screening constants and the auxiliary functions introduced in our previous paper (I.I. Guseinov, J. Phys. B, 3 (1970) 1399). The recurrence relations for auxiliary functions are useful for the calculation of multicenter EA, EF and EFG integrals for arbitrary integer and noninteger values of principal quantum numbers, screening constants, and location of slater-type orbitals. The convergence of the series is tested by calculating concrete cases.  相似文献   
52.
Orbital relaxation (OR) amounts to variation of the orbital exponents in hydrogen molecules and ions relative to the exponents of the isolated atom; it is represented as the sum of the one- and two-center contributions depending on the effective atomic charge and on the presence of other atoms in the molecule. The procedure for isolating the contributions of the exponent includes treatment of the OR of hydrogen in a special set of neutral and charged atoms and molecules with certain multiplicities of their electronic states. Within the framework of the spin-unrestricted Hartree-Fock method, we found and discussed the optimal values of the exponents of the basis orbitals of hydrogen atoms and molecules using the minimal split valence-shell basis set, the basis set that includes the polarization function, and the expanded set of grouped natural orbitals. A simple energy model is suggested for OR. Expressions are derived for evaluating the exponents of the relaxed orbitals in hydrogen-containing systems.Original Russian Text Copyright © 2004 by A. I. Ermakov, A. E. Merkulov, A. A. Svechnikova, and V. V. Belousov__________Translated from Zhurnal Strukturnoi Khimii, Vol. 45, No. 6, pp. 973–978, November–December, 2004.  相似文献   
53.
The complete symmetrization with respect to x, p x,... of the operators associated with dynamical properties can sometimes lead to results different from those obtained by the conventional quantum formalism based on the rule op (A 2)=(op A)2. For example, angular momentum operators M z 2 and M 2 are modified by the additive constants 2/2 and 3 2/2 respectively (M 20 for electron in the ground state of H atom, rotator never at rest, but spectra unchanged); the average quadratic dispersion of energy is different from zero. These results can be interpreted by assuming that the system is never strictly isolated but communicates with the other systems of the universe by means of electromagnetic interactions. Quantum mechanics would give only average values over a sufficiently long time and would exhibit a quasi-ergodic character. Examples supporting this possibility are given, in particular that of arsines for which quantum forecasts correspond to average values over one year.Dedicated to Professor J. Koutecký on the occasion of his 65th birthday  相似文献   
54.
Interaction of quantum system S a described by the generalised × eigenvalue equation A| s =E s S a | s (s=1,...,) with quantum system S b described by the generalised n×n eigenvalue equation B| i = i S b | i (i=1,...,n) is considered. With the system S a is associated -dimensional space X a and with the system S b is associated an n-dimensional space X n b that is orthogonal to X a . Combined system S is described by the generalised (+n)×(+n) eigenvalue equation [A+B+V]| k = k [S a +S b +P]| k (k=1,...,n+) where operators V and P represent interaction between those two systems. All operators are Hermitian, while operators S a ,S b and S=S a +S b +P are, in addition, positive definite. It is shown that each eigenvalue k i of the combined system is the eigenvalue of the × eigenvalue equation . Operator in this equation is expressed in terms of the eigenvalues i of the system S b and in terms of matrix elements s |V| i and s |P| i where vectors | s form a base in X a . Eigenstate | k a of this equation is the projection of the eigenstate | k of the combined system on the space X a . Projection | k b of | k on the space X n b is given by | k b =( k S b B)–1(V k P})| k a where ( k S b B)–1 is inverse of ( k S b B) in X n b . Hence, if the solution to the system S b is known, one can obtain all eigenvalues k i } and all the corresponding eigenstates | k of the combined system as a solution of the above × eigenvalue equation that refers to the system S a alone. Slightly more complicated expressions are obtained for the eigenvalues k i } and the corresponding eigenstates, provided such eigenvalues and eigenstates exist.  相似文献   
55.
Synthesis and Structure of Silver(II) Tetrafluoroaurate(III) Ag[AuF4]2 Intensive green single crystals of Ag[AuF4]2 can be obtained by heating up micro crystalline Ag[AuF4]2 in autoclaves (p(F2) ~ 200 bar, T ~ 400°C, t ~ 14 d). It crystallizes monoclinic, space group P21/n ? C; (No. 14) with a = 522.3(1), b = 1101.3(3), c = 550.5(2) pm, β = 94.98(3), Z = 2 and is isotypic with Pd[AuF4]2.  相似文献   
56.
梁文龙 《山西科技》2005,(4):83-83,91
鄂尔多斯盆地北部(简称鄂北)工区钻井技术已配套成龙,优选的井身结构经济效益明显;3KP钾基聚合物钻井液、TG无固相完井液可保证井内安全;低密度水泥浆技术已成功应用。  相似文献   
57.
采用线性组合算符及幺正变换方法研究了量子阱中强、弱耦合束缚光学极化子的性质.导出了量子阱中束缚光学极化子的基态能量与库仑束缚势、电子-LO声子的耦合强度和阱宽的变化关系.通过数值计算结果表明:基态能量因电子-LO声子的耦合强度和库仑束缚势的不同而不同,它随电子-LO声子的耦合强度和库仑束缚势的增大而增大,当电子-LO声子的耦合强度和库仑束缚势取某一定值时随阱宽的增大而增大.  相似文献   
58.
经典的多用户检测技术,其求解最优解的时间复杂度为0(2n),这是一个NP难解问题.在Pauli算子的基础上建立量子多用户信道模型,给出利用Grover算法的多用户检测解决方法.该算法的时间复杂度为O(√2n),并且当2n足够大时,其错误的概率趋近于0.  相似文献   
59.
OO技术用类来描述具有相同特征的一组对象,以继承作为共享机制,支持单一继承和多重继承.在面向对象的程序设计中,多继承使用频繁,但容易出现二性义问题.继承机制提供了规范化的结构体系和具有自然意义的重用方法,实现了代码和对象域的共享,从而使应用程序更容易维护、更新和升级.  相似文献   
60.
半个世纪以来,人们普遍接受了建立在广义相对论基础上的大爆炸学说,后来又确立了大爆炸早期的暴涨阶段,对于在这个标准模型中存在的疑难,人们试图从宇宙的创生期,应运量子理论来找出答案,文章尝试着从这个探索过程中,理清量子宇宙学的形成、内涵及影响,并期望能为以后的研究理清一个思路。  相似文献   
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