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Q condition

Oxidation of ketones R—C—R1——>-no reaction II Mild q conditions Ketone... [Pg.244]

As an instructive example, we consider the primal SDP formulation in detail. First, we show that the variational minimization of a two-particle system can be trivially formulated as a primal SDP problem. Next, we show how we constrain the eigenvalues of the 1-RDM between zero and one, and finally, how we set the SDP constraints to satisfy P and Q conditions simultaneously. [Pg.106]

Restrictions on 1-RDM P condition Q condition G condition Tl condition T2 condition... [Pg.109]

In Table V we check the A-representability of the CSE 2-RDMs through three well-known positivity conditions, the D-, the Q-, and the G-conditions [4, 5, 63], The D- and the Q-conditions are given in Eqs. (86) and (87), while the G-condition states that the following matrix (known as the G-matrix)... [Pg.196]

Although a formal solution of the A-representability problem for the 2-RDM and 2-HRDM (and higher-order matrices) was reported [1], this solution is not feasible, at least in a practical sense [90], Hence, in the case of the 2-RDM and 2-HRDM, only a set of necessary A-representability conditions is known. Thus these latter matrices must be Hermitian, Positive semidefinite (D- and Q-conditions [16, 17, 91]), and antisymmetric under permutation of indices within a given row/column. These second-order matrices must contract into the first-order ones according to the following relations ... [Pg.209]

Considering that Q has the same block structure as D, one obtains analogously that if one takes A < (1 — n )(l — tip), and the R x R block of is positive, the Q-condition is fulfilled. Consequently, the D-condition is more restrictive than the Q-condition between orbitals with ONs close to zero, whereas for A elements between orbitals with ONs close to one, the Q-condition is predominant. [Pg.411]

Electronic structure computations would be greatly simplified by the finding of practical NOFs. One may attempt to approximate the unknown off-diagonal elements of A considering the sum rule (89) and analytic constraints (101) imposed by the D-, G-, and Q-conditions. However, it is not evident how to approach A, for p q, in terms of the ONs. Due to this fact, let s rewrite the energy term, which involves A, as... [Pg.415]

These constraints are the P condition, Q condition, and G condition, respectively... [Pg.467]

A second clue arises when one realizes that among the entire set of (Q, Q) conditions, only the simplest condition,... [Pg.469]

Column, glass, 1.2 m x 4 mm. Wash column and glass wool plugs with 5% (v/v) dichlorodimethyl silane in toluene (in a hood) before packing with 1 g Apiezon L/ 20 g 80 to 100 mesh Gas Chrom Q. Condition for 3 days at 200 °C at 10 mL Nj/min or until a steady baseline is obtained. Order of elution CSj, BHA, BHT, di-BHA. This column will separate the 2 and 3 isomers of BHA. [Pg.593]

Figure 6.11 Computed trajectories through a linear quadrupole mass filter for ions of mIz (a) 100, (b) 99 and (c) 101. In all cases the top trajectory is for the xz plane and the other for the yz plane. All trajectories were calculated for the same initial conditions (ion energy and point and angle of entry) under a, q) conditions chosen such that ions of miz 100 are close to the apex value (0.701,0.2353) within the stability range (Figure 6.15(b)) and are thus transmitted as shown in (a). However, the scan-line slope f scan = 2U/Vo was Set so that the corresponding a, q) values for miz 99 and 101 lie outside this intersected stability region at the instantaneous values of U and Vq that led to stable trajectories for the m z 100 ions, and are thus not transmitted but are lost on the quadrupole rod as shown in (b) and (c). (Recall that the z-direction is the main axis of the quadrupole, i.e., the horizontal direction in this sketch). Reproduced from Campana, Int. J. Mass Spectrom. Ion Phys. (1980) 33, 101, copyright (1980), with permission of Elsevier. Figure 6.11 Computed trajectories through a linear quadrupole mass filter for ions of mIz (a) 100, (b) 99 and (c) 101. In all cases the top trajectory is for the xz plane and the other for the yz plane. All trajectories were calculated for the same initial conditions (ion energy and point and angle of entry) under a, q) conditions chosen such that ions of miz 100 are close to the apex value (0.701,0.2353) within the stability range (Figure 6.15(b)) and are thus transmitted as shown in (a). However, the scan-line slope f scan = 2U/Vo was Set so that the corresponding a, q) values for miz 99 and 101 lie outside this intersected stability region at the instantaneous values of U and Vq that led to stable trajectories for the m z 100 ions, and are thus not transmitted but are lost on the quadrupole rod as shown in (b) and (c). (Recall that the z-direction is the main axis of the quadrupole, i.e., the horizontal direction in this sketch). Reproduced from Campana, Int. J. Mass Spectrom. Ion Phys. (1980) 33, 101, copyright (1980), with permission of Elsevier.
Then we have the critical conditionally stable case. In this case, we must impose the following boundary conditions p + q q k) conditions at t = 0, and m-p-q conditions at t = 1. [Pg.80]

This stresses that the measured cell potential E depends on the difference between equilibrium conditions and the given Q conditions. Other relations of use in thermodynamic calculations relate these to the standard free energy change ... [Pg.208]

Different expansion factor models for correcting data obtained in good solvents to Q conditions, or neglecting of such correction altogether [4]... [Pg.129]

KEY Q Resistant Q Not Recommended Limned Resistance Q Conditional. Test Required Q Not Tested TYPE mortar R S N-- FUR... [Pg.404]


See other pages where Q condition is mentioned: [Pg.107]    [Pg.108]    [Pg.126]    [Pg.151]    [Pg.189]    [Pg.209]    [Pg.215]    [Pg.238]    [Pg.242]    [Pg.396]    [Pg.467]    [Pg.468]    [Pg.107]    [Pg.269]    [Pg.359]    [Pg.20]    [Pg.593]    [Pg.529]    [Pg.265]    [Pg.255]    [Pg.239]    [Pg.217]   


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Q, distillation feed condition

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