Kostenloser Versand
Bequem zahlen
Wir sind gerne für Sie daSince 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].
Produkteigenschaften
- Artikelnummer: 9783540414148
- Medium: Buch
- ISBN: 978-3-540-41414-8
- Verlag: Springer Berlin Heidelberg
- Erscheinungstermin: 12.12.2000
- Sprache(n): Englisch
- Auflage: 2000
- Serie: Lecture Notes in Mathematics
- Produktform: Kartoniert
- Gewicht: 201 g
- Seiten: 120
- Format (B x H x T): 155 x 235 x 8 mm
- Ausgabetyp: Kein, Unbekannt