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Operator product expansion

We often write this in the so-called operator product expansion... [Pg.104]

For example, the energy momentum tensor T(z) = J2z n 2Ln = Y(lo,z) has the following operator product expansion ... [Pg.104]

The basic formula to take Fermi motion into account can be derived along lines very similar to those followed in the appendix to Chapter 16 [see eqn (16.9.19)]. The difference, of course, is that now V represents the momentum distribution of a nucleon in the nucleus. The following convolution formula emerges either using the techniques of the operator product expansion, or more simply, by considering the kinematics of Fig. 17.11 which shows a nucleus of atomic number A in a reference frame in which it is moving very fast with momentum P along OZ. A nucleon i inside the nucleus has -component of momentum pz = zP/A and a parton. [Pg.414]

Ferrara, S Gatto,R., Grillo.A.F. Conformal Algebra in Space-Time and Operator Product Expansion (Vol. 67)... [Pg.142]

In an alternative formulation of the Redfield theory, one expresses the density operator by expansion in a suitable operator basis set and formulates the equation of motion directly in terms of the expectation values of the operators (18,20,50). Consider a system of two nuclear spins with the spin quantum number of 1/2,1, and N, interacting with each other through the scalar J-coupling and dipolar interaction. In an isotropic liquid, the former interaction gives rise to J-split doublets, while the dipolar interaction acts as a relaxation mechanism. For the discussion of such a system, the appropriate sixteen-dimensional basis set can for example consist of the unit operator, E, the operators corresponding to the Cartesian components of the two spins, Ix, ly, Iz, Nx, Ny, Nz and the products of the components of I and the components of N (49). These sixteen operators span the Liouville space for our two-spin system. If we concentrate on the longitudinal relaxation (the relaxation connected to the distribution of populations), the Redfield theory predicts the relaxation to follow a set of three coupled differential equations ... [Pg.54]

This production expansion was made possible in no small degree by a sharp reduction in the cost of manufacture. From an original market price of 1.45 a pound in 1926, cellulose acetate dropped steadily to. 50 a pound in 1936, and further to. 30 in 1940. In addition to a lower cost as a result of the increasing quantity of production, these reductions in price were aided greatly by reductions in the cost of raw materials. Acetic acid became much cheaper during this period, and the cost of conversion of the acid to its anhydride was aided by improved process development. Recovery of acetic acid from aqueous solution also became cheaper with the adoption of extraction and azeotropic distillation processes, replacing the original recovery by evaporation of neutralized solutions. In addition, technical developments in the acetylation process increased the economy of plant unit operations. [Pg.322]

For a simple treatment of the (RS) perturbation expansions, it is often desirable to have just one wave operator 2, which is defined on the whole model space. This desire requests however that the distinction of internal and external excitations must apply for all determinants < ) e A4 in the same way [43]. This can be seen, for instance, from the second term (on the rhs) of the Bloch Eq. (16) which contains the operator product PVS2P. The projector P, standing left of this product, eliminates all contributions of the operator which leads out of the model space. For a single wave operator, acting on the whole model space, this projection must be the same for all determinants < ) e M. We therefore find that an unique dispartment of the excitations into internal and external ones is a necessary and sufficient condition. The importance of the proper choice of the model space and their classification has been discussed in detail by Lindgren [43]. [Pg.195]

An analogue representation applies independently also for the wave operator in every order n of fhe order-by-order expansion. Thaf is, if we are able fo bring the operator products on the rhs of fhe corresponding Bloch equafions (20)-(23) into normal form, we can identify the terms on the left- and right-hand side in order to express the amplitudes of the wave operator. For each order n, this finally... [Pg.199]

With this notation and the vacuum amplitudes (46), we can summarize the result of this section by saying that the wave operator as well as any effective operator and matrix element can be written always as perturbation expansion, independent of the particular shell structure of the system. More often than not, moreover, we shall be interested only in the vacuum amplitudes on the rhs of Eq. (46), i.e. only in the completely contracted terms of the operator product [(fl) Aeff(fl ) ], once it has been brought into its normal-order sequence. In fact, these are the... [Pg.200]

Evaluation of the operator products as they occur either on the rhs of fhe Bloch Eq. (23) or in fhe definifion of fhe effective operators (15) and (49). The aim of this step is to bring all the creation and annihilation operators (in each term of the expansions) into the extended normal-order form (50). The resulf is a sequence of normal-ordered operator ferms (briefly referred to as Feynman-Goldstone diagrams). [Pg.204]

Evaluates the operator product of oplistj x opKst2 x x opUst including all contractions where oplist,-can be either of type diagram or expansion. [Pg.209]

Very careful assessment of the demand for the product shall be made before planning to manufacture higher quantities by the plant and adding more products in the future. The product quality shall be continuously improved upon, and its usefulness for more applications shall be found out. Feedback shall be obtained from clients by regular meetings to get a hint whether the product may become obsolete due to better/cheaper products likely to enter the market. However, there shall be no compromise on safety, environmental pollution control, product quality, and efficiency of operations during expansion of capacity or while adding new products. [Pg.9]

As a result of this expansion, followed by a decoupling of four operator products (two magnon terms) in the Hartree-Fock approximation, and subsequent Fourier transformation, Lindgard and Danielsen (1975) deduce the full hamiltonian in the... [Pg.417]

An update of the existing operation, uranium extraction and the plans for the production expansion and upgrading beyond the 50,000tpa will be discussed. [Pg.269]

For the general case, we remark that the kinetic energy operator normally has the required form (23), but the potential energy operator often does not. It then may be fitted to the product form. A convenient, systematic, and efficient approach to obtain an optimal product representation is described in Refs. 6 and 19. We finally note that there are other methods which evaluate the Hamiltonian matrix elements efficiently without relying on a product expansion (23). Most notable here is the CDVR method of Manthe. ... [Pg.592]

The system is the combination or interrelation of hardware, software, people, and the operating environment. In system safety engineering, you must look at the system from cradle to grave. In other words, the system life cycle is the design, development, test, production, operation, maintenance, expansion, and retirement (or disposal) of the system. A nuclear power plant is one large system with operators, pressure subsystems, electrical and mechanical subsystems, structural containment, safety systems, etc. A far simpler example is a boy riding his bike. The bike, the boy, the street (with all its traffic conditions), the weather, the time of day, and even other children make up the system of boy on his bike. [Pg.22]

Production Expansions Binary Decision Variables Equations 3.33 and 3.34 ensure that a new production line t, proposed as a capacity expansion, is activated only when all the existing machines of similar technology t are operating. If at least one production line of type t is idle at a given plant, then no capacity expansion can be done. Note that these constraints can be relaxed if the analyst wants to evaluate the replacement of equipment. In such a case, new production lines could be opened even when the existing equipment is idle. [Pg.77]


See other pages where Operator product expansion is mentioned: [Pg.104]    [Pg.312]    [Pg.104]    [Pg.312]    [Pg.28]    [Pg.60]    [Pg.228]    [Pg.81]    [Pg.10]    [Pg.240]    [Pg.36]    [Pg.87]    [Pg.90]    [Pg.183]    [Pg.320]    [Pg.71]    [Pg.60]    [Pg.192]    [Pg.198]    [Pg.200]    [Pg.207]    [Pg.207]    [Pg.246]    [Pg.261]    [Pg.530]    [Pg.57]    [Pg.245]   
See also in sourсe #XX -- [ Pg.2 , Pg.135 , Pg.136 ]




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