State lists

All state lists are divided into three sections  

The control section is a storage for information which is relevant only as long as an entity is open. This section will not survive when the list is closed. Essential items in this section are the enclosing entity and its state. Also the name which was used on the neutral file to identify the entity is part of this section. 

The directory section contains a directory of all named entities received within the open entity from the neutral file. The directory contains the names as given on the file together with references to the entities after the storage in the open entity. 

The value section will store the result of actions which have been carried out to define the open entity. Upon closure of an open entity the value will become one entry in the enclosing entity list. When the open world is closed, its value is copied into the receiving CAD system data base (either on the world level or on an assembly level depending on the directives to the post-processor). 

TYPE STATE = ( ASSEMBLY OPEN, B REP OPEN, COMPOUND B REP OPEN, 

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Provides the means to recalculate end state values after modifying event failure data and/or cutsets. After choosing End State from the menu, the End State List appears listing all end states in... 

Table 21.2 lists some of the more important hydrogen compounds of the nonmetals. (Those of carbon are discussed in Chapter 22.) The physical states listed are those observed at 25°C and 1 atm. The remainder of this section is devoted to a discussion of the chemical properties of the compounds shown in boldface in die table. 

The symmetries of the lowest excited states listed in Table 1 are nothing but the symmetries to which the most soft second-order bond distortions belong. It is seen that the types of symmetry reduction predicted using the symmetry rule are in complete agreement with those obtained on the basis of the dynamic theory. 

In addition to the organized and loose networks that generally fund their own activities, there are a number of states that sponsor terrorism. This is of particular concern with regards to weapons of mass destruction, because the numerous resources that can be brought to bear in state development of CBRN weapons can in turn be transferred to terrorists. Disincentives do exist to prevent this proliferation. As of October 2004, the United States lists six countries as state sponsors of terrorism Cuba, Iran, Libya, North Korea, Sudan, and Syria. Of these, five are pursuing WMD to one degree or another. Libya repudiated its WMD program as discussed below. 

Phenol is listed on the Food and Drug Administration s EAFUS (Everything Added to Foods in the United States) List (FDA 1998a), and is approved as a component of food packaging materials (FDA 1998b, 1998c, 1998d). 

Listed pesticides (formulated, manufacturing-use, and off-specification) are regulated as hazardous wastes under the RCRA if they are discarded rather than used for their intended purposes. State listings are often more extensive. Both onsite and offsite disposal options are regulated under the RCRA. Onsite facilities that generate more than 1 kg/month of acutely hazardous wastes in the RCRA E List or 1000 kg/month of any waste as defined in 40 CFR 261.31, 261.32, or 261.33 will require an RCRA hazardous waste permit for treatment or for storage for more than 90 days. Offsite disposal must be handled by an RCRA-permitted facility. 

Which leading causes of death in the United States, listed in table 10.1, can be linked with certainty to products of the CPI Which causes can be linked plausibly to the CPI How would you estimate the drop in annual death rate if the CPI ceased to exist, and is this a large percentage change ... 

Similarly, we can obtain the tunneling matrix elements for all the tip states listed in Table 3.1. Table 3.2 is a summary of the results. 

Rankine-Hugoniot equations 181-87 (Equations of state which include among others the following Jones Miller, Lennard-Jones Devonshire, Halford-Kistiakowsky-Wilson, Joffe its modification by Su Chang, Taylor, Kihara Hikita, Travers, Cook, Kistiakowsky-Wilson-Brinkley and Polytropic equations) 194 (Landau-Stanyukovich and Hirschfelder et al equations of state 11) J.F. Roth, Explosiv-stoffe 1958, 50 (Abel sche Zustandsgleichung fur die Detonation) 12) Cook (1958), 37 (General equation of state) 62-3 [Halford-Kistiakowsky-W ilson-Brinkley equation of state, (listed as K-H-W-B equation of state)] ... 

By adding the values of 2J + 1 for the ten Russell-Saunders states listed above we see that there are in fact 36 states based upon the configuration 2p3p and that application of a magnetic field gives rise to 36 energy levels. 

Label all vessels to indicate what they contain. An unlabeled bottle left and forgotten in a refrigerator or cabinet presents an expensive disposal problem, because the contents must be analyzed before they can be legally discarded. National Fire Protection Association labels shown in Figure 2-2 identify hazards associated with chemical reagents. A Material Safety Data Sheet provided with each chemical sold in the United States lists hazards and safety precautions for that chemical. It gives first aid procedures and instructions for handling spills. 

We can now obtain the result we desire. We can immediately make a unique assignment of multiplicities to the states listed in the lower part of our chart by noting that there is only one yAK state and two yBR states. These must therefore be assigned to the Ag and two Bg states arising from thus establishing that the TXg state is a spin triplet and, hence, that the >4,, Eg. and T2k states are all spin singlets. 

List the standard conditions used in your state. List the standard conditions used in this book. Convert a pressure of 10 atmospheres (absolute) to psia. 

Efficient methods of selection of admixed configurations in this approach are described in [12]. The computer code for generating the reduced configuration state list is presented in [13]. A special diagonalisation method is developed to reduce the orders of matrices to be diagonalised [14]. A more detailed overview of the methods considered may be found in [15]. All these improvements considerably speed up the calculations and widen the domains of applicability of the methods developed. 

P. Bogdanovich, A. Momkauskaite, A program for generating configuration state lists in many-electron atoms, Comput. Phys. Commun., 157, 217-225 (2004). 

The selection rules have to be fulfilled for the transition from the ls2s22p6 2Se initial state to the possible final states. Thus, the final state contains one of the final ionic states listed in Table 3.2 and the wavefunction for the emitted Auger electron in its partial wave expansion (see equ. (7.28b)). Due to the selection rules, only a few t values from the partial wave expansion contribute. In the present case there is only one possibility which will be characterized by si. Therefore, one... 

Figure 3.8 Tanabe-Sugano energy level diagram for a 3d6 ion in an octahedral crystal field. Note that some of the highest energy triplet and singlet crystal field states listed in table 3.3 are not shown in the diagram.

Ohrimenco, G.M. (1978) A hydraulic press. Registered in the State list of the inventions of USSR, N° 641711 on September 14, 1978 with priority from December 9, 1974. (mss)... 

The spin-orbit coupling therefore removes the degeneracy of the so-called fine-structure states listed above. For example, simply by substituting the appropriate values of J, L and S, the three fine-structure components arising from the L = 1, S= 1 configuration are calculated to have the following first-order spin orbit energies ... 

Diagonalisation of the Stark matrices enables us to plot the Stark energies, given values of B and /M), and the results are shown in figure 8.27 for the first three rotational levels, J = 0, 1 and 2. The parameter X is defined by A.2 = iJ E jB. In figure 8.28 we show plots of the effective electric moment of the molecule in the different J, M states listed in figure 8.27. With the aid of both diagrams, we are able to understand the principles of electric state selection, and the electric resonance transitions. 

The case (b) eigenkets for the three electronic states listed above and their parities may be written as follows. 

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