these

In this way, $D$ yields operators $D^+$ and $D^-$. These are formal adjoints of each other.

The best known of these is the Knaster continuum.

One of these lies in the union of the other two.

We refer to these as homogeneous Sobolev spaces.

Each of these three integrals is finite.

We begin by constructing a function $f$ which has these prescribed zeros.



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