Eitner Ulrich (12 results)

Paperback. Condition: Very Good. Slender softback in very good condition. From the collection of a London Professor of Mathematics, (ret'd.). Light shelfwear only, including tanning to pageblock, this leading into page edges. Within, pages are tightly bound, content unmarked. CN.

Condition: New.

Condition: New. In.

Condition: New. pp. 128.

Paperback. Condition: Brand New. 1st edition. 120 pages. French language. 9.75x6.75x0.25 inches. In Stock.

Condition: New.

Taschenbuch. Condition: Neu. Druck auf Anfrage Neuware - Printed after ordering - Since the time of surfaces -+ in differential Gauss, parametrized (x, y) P(x, y) have been described a frame attached to the moving geometry through TI(x, y) surface. One introduces the Gauss- which linear dif- Weingarten equations are , ferential equations = U = TIX T1, VT', !PY (1. for the and their condition frame, compatibility - = V + [U, V] 0, UY (1.2) which the Gauss-Codazzi For surfaces in three-dim- represents equations . a sional Euclidean the frame T1 lies in the usually or space, group SO(3) SU(2). On the other a of a non-linear in the form hand, representation equation (1.2) is the of the of of starting point theory integrable equations (theory solitons), which in mathematical in the 1960's appeared physics [NMPZ, AbS, CD, FT, More the differential for the coefficients of AbC]. exactly, partial equation (1.2) the matrices U and V is considered to be if these matrices can be integrable , extended to U V non-trivially a one-parameter family (x, y, A), (x, y, A) satisfying - = + U(A)y V(A). [U(A), V(A)] 0, (1-3) so that the differential is and original partial equation preserved.' . Usually U(A) V are rational functions of the which is called the (A) parameter A, spectral param- In soliton the eter is called the Lax . theory, representation (1.3) representation the Zakharov-Shabat or representation [ZS].

Pas de couverture. Condition: Neuf. Edition originale. Kiepenheuer & Witsch, Köln, 2003, 12,5 x 19 cm, 317 p., broché. Texte sur le Sujet en allemand avec les contributions de Dokoupil, Distel, Diederichsen, Drechsler, Eitner, Glaser, Goetz, Heyder, Kippenberger, Lobeck, Lottmann, Morshäuser, Padeluun, Schwebel, Stingl, Waffender, Winkels sous la direction de Peter Glaser.

Fischerhude, Verl. Atelier im Bauernhaus, 2011, 184 pag., (fold.) (full-page) coloured illustrations, hardcover with dustjacket, quarto. = Stamp on first free endpaper. Else a fine copy.

Condition: New. Print on Demand pp. 128 Illus.

Taschenbuch. Condition: Neu. This item is printed on demand - it takes 3-4 days longer - Neuware -Since the time of surfaces -+ in differential Gauss, parametrized (x, y) P(x, y) have been described a frame attached to the moving geometry through TI(x, y) surface. One introduces the Gauss- which linear dif- Weingarten equations are , ferential equations = U = TIX T1, VT', !PY (1. for the and their condition frame, compatibility - = V + [U, V] 0, UY (1.2) which the Gauss-Codazzi For surfaces in three-dim- represents equations . a sional Euclidean the frame T1 lies in the usually or space, group SO(3) SU(2). On the other a of a non-linear in the form hand, representation equation (1.2) is the of the of of starting point theory integrable equations (theory solitons), which in mathematical in the 1960's appeared physics [NMPZ, AbS, CD, FT, More the differential for the coefficients of AbC]. exactly, partial equation (1.2) the matrices U and V is considered to be if these matrices can be integrable , extended to U V non-trivially a one-parameter family (x, y, A), (x, y, A) satisfying - = + U(A)y V(A). [U(A), V(A)] 0, (1-3) so that the differential is and original partial equation preserved.' . Usually U(A) V are rational functions of the which is called the (A) parameter A, spectral param- In soliton the eter is called the Lax . theory, representation (1.3) representation the Zakharov-Shabat or representation [ZS]. 128 pp. Englisch.

Condition: New. PRINT ON DEMAND pp. 128.