On Spectral Theory for Singular Hamiltonians under Left-definiteness Conditions by Albert Schneider, Univ Dortmund AEB350, 3:15pm Tuesday, March 26, 1996 Abstract On an arbitrary interval I = {a; b} of the real line the Hamiltonian system +- -+ +- -+ +- -+ | 0 I | | D D | | E 0 | | m | | 11 12 | | 11 | (1) | | y' + | | y = r | | y |-I 0 | | D D | | 0 0 | | m | | 12 22 | | | +- -+ +- --+ +- -+ is considered under the assumptions: 1. D (x), D (x), D (x), E (x) are locally integrable on I 11 12 22 11 2. D (x), D (x), E (x) are hermitian for x in I, a.e. 11 22 11 3. D (x), -D (x) are positive-definite for x in I, a.e. 11 22 4. If y is solution of (1) for r=0 and the usual Hilbert space inner product on I equals zero, 11 22 then y = 0, and it will be shown, how selfadjoint operators can be generated by the system (1) and suitable boundary conditions in a Hilbert space setting, defined by the left side of the systems (1) and the boundary conditions. One of the main points is, that the spectral theory for these operators is developed without using a growth-condition of the form -s D (x) <= E (x) <= s D (x), s > 0 11 11 11 for x in I, a.e., which was originally introduced by H. Weyl in 1910 in connection with the Sturm-Liouville equation and which has been assumed until today in all investigations looking for expansion theorems. As one result and application we get a proof of Weyl's expansion theorem without the growth-condition now after 80 years. Requests for preprints and reprints to: schneider@math.uni-dortmund.de This source can be found at http://www.math.utah.edu/research/