Pali Buddhist Texts-explained to the Beginner. Rune. E. A. Johansson. Scandinavian Institute of Asian Studies Monograph Series No. 14 Curzon Press, London, Second edition, revised and enlarged, 1977 160 pp. £4.00.

Originally presented as the author's thesis (doctoral)--Universite catholique de Louvain, 1990.

The history of aesthetics, like the histories of other sciences, may be treated in a two-fold manner: as the history of the men who created the field of study, or as the history of the questions that have been raised and resolved in the course of its pursuit. The earlier History of Aesthetics (3 volumes, 1960-68, English-language edition 1970-74) by the author of the present book was a history of men, of writers and artists who in centuries past have spoken (...) up concerning beauty and art, form and crea tivity. The present book returns to the same subject, but treats it in a different way: as the history of aesthetic questions, concepts, theories. The matter of the two books, the previous and the present, is in part the same; but only in part: for the earlier book ended with the 17th century, while the present one brings the subject up to our own times. And from the 18th century to the 20th much happened in aesthetics; it was only in that period that aesthetics achieved recognition as a separate science, received a name of its own, and produced theories that early scholars and artists had never dreamed of. (shrink)

Problems connected with the questions of: being-nonbeing, existence, modes of existence and alike, belong to the basic and most important in metaphysics. The article discusses some answers to the aforementioned issues, as proposed by the ancient philosophers, St Thomas Aquinas, R. Ingarden and A.N. Whitehead. In the Appendix some remarks are made on Aristotle’s and S. Thomas’ theory of act and potency.

A fully quantum-mechanical description of the spontaneous emission from an excited two-level atom placed in front of a two-slit interferometer is given. Global modes of the electromagnetic field in a two slit system are derived within the Kirchhoff-Huygens diffraction approximation, serving as a base for the field quantization. The standard Fermi's golden rule, supplemented by a factor coming from the nontrivial mode structure caused by the presence of the two-slit interferometer, is used to show that interference results from the position-dependent (...) coupling between the atom and different field modes of the system. (shrink)