Conservation concluding remarks

Move 3, the last and most important move of the abstract (and often the longest), highlights the principal Endings of the work. Three examples are considered (P12-P14). Only the most essential or representative data are reported, including numerical values, when appropriate. (Note that numerical data should include units and standard errors or deviations. Do not omit units or error terms to conserve space.) Move 3 may also inform readers about the contents of the full article. For example, P12 informs readers that acute toxicity information for three pesticides is presented in the text. Move 3 sometimes ends with a concluding remark. In P12 and P13, the data themselves end the abstract and no summative remarks are made in P14, the authors add a concluding remark. 

We continue with Kenney s commentary on the favorable economics of energy conservation, but also on the Institutional barriers that limit its wider applicability, and close the Chapter with some concluding remarks. 

Finally, Section 2.6, after some concluding remarks, proposes some ideas for future work that particularly concern the high-temperature oxidation of intermetallic compounds that are not considered in the present overview. Contrary to the case of pure metals or disordered solid solutions, vacancies in intermetallic compounds cannot be considered as non-conservative species. Indeed, their equilibrium molar fraction depends not only on temperature and stress state but also on the local chemical composition, which corresponds to a situation drastically different from that of a pure metal or a disordered solid solutions. 

Many problems appear to be ripe for a more quantitative discussion. What is the error involved in the introduction of unstable states as asymptotic states in the frame of the 5-matrix theory 16 What is the role of dissipation in mass symmetry breaking What is the consequence of the new definition of physical states for conservation theorems and invariance properties We hope to report soon about these problems. We would like, however, to conclude this report with some general remarks about the relation between field description and particles. The full dynamical description, as given by the density matrix, involves both p0 and the correlations pv. However, the particle description is expressed in terms of p (see Eq. (50)). Now p has only as many elements as p0. Therefore the... 

---