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Normal ordering

Certain base adducts of borane, such as triethylamine borane [1722-26-5] (C2H )2N BH, dimethyl sulfide borane [13292-87-OJ, (CH2)2S BH, and tetrahydrofuran borane [14044-65-6] C HgO BH, are more easily and safely handled than B2H and are commercially available. These compounds find wide use as reducing agents and in hydroboration reactions (57). A wide variety of borane reducing agents and hydroborating agents is available from Aldrich Chemical Co., Milwaukee, Wisconsin. Base displacement reactions can be used to convert one adduct to another. The relative stabiUties of BH adducts as a function of Group 15 and 16 donor atoms are P > N and S > O. This order has sparked controversy because the trend opposes the normal order estabUshed by BF. In the case of anionic nucleophiles, base displacement leads to ionic hydroborate adducts (eqs. 20,21). [Pg.236]

In order to illustrate the type of questions which can be addressed within such an idealized lattice model, we show a histogram of the normalized order parameters M = Si/N and Q = being the system... [Pg.658]

To return to a more historical development the mercuric acetate oxidation of substituted piperidines (77) should be discussed next. This study established that the normal order of hydrogen removal from the aW-carbon is tertiary —C—H > secondary —C—H > primary —C—H, an observation mentioned earlier in this section. The effect of substitution variations in the piperidine series can be summarized as follow s l-mcthyl-2,6-dialkyl and 1-methyl-2,2,6-trialkyl piperidines, as model systems, are oxidized to the corresponding enamines the 1,2-dialkyl and l-methyl-2,5-dialkyl piperidines are oxidized preferentially at the tertiary a-carbon the 1-methyl-2,3-dialkyl piperidines gave not only the enamines formed by oxidation at the tertiary a-carbon but also hydroxylated enamines as found for 1-methyl-decahydroquinoline (48) (62) l-methyl-2,2,6,6-tctraalkyl piperidines and piperidine are resistant to oxidation by aqueous mercuric acetate and... [Pg.71]

The component can be represented over the initial I) and intermediate J) states of the system defined by Wn, which is a normal-ordered Hamiltonian with respect to the I) state ... [Pg.158]

This index is divided into two parts. Part 1 gives the names of compounds as used in these volumes as well as general terms for classes of compounds, types of reactions, synthetic applications, special apparatus, and unfamiliar methods. The complete names of all specific compounds are given in normal order as written in the text (e.g., ethyl cyano-acetate appears under ethyl). Some entries are common names and others are systematic Chemical Abstracts names, whichever was used in the text. [Pg.245]

Figure 1.133. The normal order in other epithermal gold deposits in Japan (Nagayama, 1993a). Figure 1.133. The normal order in other epithermal gold deposits in Japan (Nagayama, 1993a).
Fig. 1. Possible positions of electronic energy levels associated with hydrogen in a semiconductor. (a) normal order (acceptor above donor), allowing possible predominance of any of the charge states H+, H°, H. (b) negative-U order (donor above acceptor), H+ or H always predominant. Fig. 1. Possible positions of electronic energy levels associated with hydrogen in a semiconductor. (a) normal order (acceptor above donor), allowing possible predominance of any of the charge states H+, H°, H. (b) negative-U order (donor above acceptor), H+ or H always predominant.
It can be seen from display 51 and Figure 16 that pure through-bond interaction (B = 0) places the symmetric orbital (p on top of the antisymmetric orbital through-space interaction ( /i > 0), the energy gap 3 — 2 between cross-over occurs when the parameters obey the condition... [Pg.219]

We teach our students that the infinite zero-point energy that arises when a free relativistic scalar (or Dirac-) field theory is canonically quantized can be subtracted (discarded) by a suitable redefinition of the energy-origin in other words, by normal ordering. However, the energy-origin can be re-defined only once, and only in homogenous space (i.e. without boundary conditions) and... [Pg.232]

Observe that the command "Default order" is marked, which means that the program is working on a normal order of priority, i.e. the one set into the program. Consequently disconnections will be activated in the order in which they appear in the previous figure. [Pg.461]

Consider the exponential of (f)a z). This does not make sense yet since we have an inhnite sum in coefficients of the z-expansion. In order to remedy the difficulty, we need to introduce so-called normal ordering, which defines an order on operators a n), e" s. [Pg.106]

Remark 9.28. Our normal ordering is slightly different from that in [20]. Ours satisfies ihh l = ih hl. [Pg.106]

We can always write G in normal order of aj, oi. Therefore G can be written as a superposition of the monomials with m,n>Q integers. Hence, we will... [Pg.143]

Here frs and (ri-l tM> are, respectively, elements of one-electron Dirac-Fock and antisymmetrized two-electron Coulomb-Breit interaction matrices over Dirac four-component spinors. The effect of the projection operators is now taken over by the normal ordering, denoted by the curly braces in (15), which requires annihilation operators to be moved to the right of creation operators as if all anticommutation relations vanish. The Fermi level is set at the top of the highest occupied positive-energy state, and the negative-energy states are ignored. [Pg.164]

This is an analogue of the classical moments-generating functional discussed by Kubo [39]. Upon expanding the exponential as a power series, the operator J f acts to place each term in so-called normal order, in which all creation operators are to the left of all annihilahon operators j/. By virtue of this ordering (and only by virtue of this ordering). [Pg.269]

GENERALIZED NORMAL ORDERING, IRREDUCIBLE BRILLOUIN CONDITIONS, AND CONTRACTED SCHRODINGER EQUATIONS... [Pg.293]

C. Normal Ordering with Respect to Arbitrary Reference Eunction... [Pg.293]

Formulating conditions for the energy to be stationary with respect to variations of the wavefunction P in this generalized normal ordering, one is led to the irreducible Brillouin conditions and irreducible contracted Schrodinger equations, which are conditions on the one-particle density matrix and the fe-particle cumulants k, and which differ from their traditional counterparts (even after reconstruction [4]) in being strictly separable (size consistent) and describable in terms of connected diagrams only. [Pg.294]


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See also in sourсe #XX -- [ Pg.55 , Pg.60 ]

See also in sourсe #XX -- [ Pg.244 ]

See also in sourсe #XX -- [ Pg.61 ]




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