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In fact let — -~->Z^Z2>^. Then taking into consideration Remark 1 and the fact that /j given to (1) by (2. 7) and (2.8) equals — 4 ' (3.1) and (3. 2) are satisfied by R = —~-, where Ci is sufficiently large constant depending only on Z3. On the other hand, we can show the following fact which is more precise than Lemma 5. There exist an "extension operator" 0i which maps £^2(.ft) to and some constant C2 depending only on Z3 such that for any

Corrections to: ``Finiteness of the number of discrete eigenvalues of the Schrödinger operator for a three particle system''