PDF - Universiteit Twente
PDF - Universiteit Twente
PDF - Universiteit Twente
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Chapter 5. Extension Bergman distance<br />
where we used the triangle inequality for the norm of X in the last<br />
step. Since inequality (5.2) holds for all x0 ∈ X, we have<br />
d � e At , e Ct�2 ≤ � d � e At , e Bt � + d � e Bt , e Ct��2 .<br />
Hence the triangle inequality holds.<br />
The Bergman distance defines a metric. �<br />
5.1.2 Classes of cogenerators<br />
The Bergman distance on the Hilbert space X can be seen as a binary<br />
B<br />
relation on the set of cogenerators on X. We define Ad ∼ Ãd if the cogenerators<br />
A and à have a finite Bergman distance. that is if the following two<br />
equations hold.<br />
∞�<br />
k=1<br />
∞�<br />
k=1<br />
1<br />
k �(Ak d − Ãk d)x0� 2 < ∞,<br />
1<br />
k �(A∗k<br />
d − Ã∗k<br />
d )x0� 2 < ∞.<br />
These equations are the same as equations (4.5) and (4.6).<br />
Lemma 5.3 The binary relation B ∼ on the set of cogenerators on X, is an<br />
equivalence relation.<br />
Proof: We have to check the reflexivity, symmetry and transitivity of B ∼.<br />
B<br />
B<br />
The reflexivity, Ad ∼ Ad, and the symmetry, if Ad ∼ Ãd then Ãd<br />
B<br />
∼ Ad, are<br />
trivial. So it remains to show transitivity. Using the inequality<br />
the transitivity, if Ad<br />
∞�<br />
k=1<br />
1<br />
k �(Ak d − C k d )x0� 2 ≤<br />
= 2<br />
∞�<br />
k=1<br />
�x − z� 2 ≤ 2�x − y� 2 + 2�y − z� 2 ,<br />
B<br />
B<br />
B<br />
∼ Bd and Bd ∼ Cd then Ad ∼ Cd, is easy to see from<br />
∞�<br />
k=1<br />
1 � k<br />
2�(Ad − B<br />
k<br />
k d )x0� 2 + 2�(B k d − C k d )x0� 2�<br />
1<br />
k �(Ak d − B k d )x0� 2 + 2<br />
∞�<br />
k=1<br />
1<br />
k �(Bk d − C k d )x0� 2 < ∞.<br />
And the same holds for the adjoint operators Ãd, ˜ Bd, and ˜ Cd.<br />
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