<p>It is a classical result that, if <i>T</i> is a maximal symmetric operator in a Krein space <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathscr {H}=\mathscr {H}^+[\dotplus ]\mathscr {H}^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">H</mi> <mo>=</mo> <msup> <mi mathvariant="script">H</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">[</mo> <mo>∔</mo> <mo stretchy="false">]</mo> </mrow> <msup> <mi mathvariant="script">H</mi> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> with the domain <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathscr {D}_T\supset \mathscr {H}^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">D</mi> <mi>T</mi> </msub> <mo>⊃</mo> <msup> <mi mathvariant="script">H</mi> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>, then the imaginary part of its eigenvalue <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> from upper or lower half-plane is bounded by <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(|{{\,\textrm{Im}\,}}\lambda |\leqslant 2\Vert TP^-\Vert \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mrow> <mspace width="0.166667em" /> <mtext>Im</mtext> <mspace width="0.166667em" /> </mrow> <mi>λ</mi> <mo stretchy="false">|</mo> <mo>⩽</mo> <mn>2</mn> <mo stretchy="false">‖</mo> <mi>T</mi> </mrow> <msup> <mi>P</mi> <mo>-</mo> </msup> <mrow> <mo stretchy="false">‖</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We prove that in both half-planes <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(|{{\,\textrm{Im}\,}}\lambda |\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">|</mo> <mrow> <mspace width="0.166667em" /> <mtext>Im</mtext> <mspace width="0.166667em" /> </mrow> <mi>λ</mi> <mo stretchy="false">|</mo> </mrow> </math></EquationSource> </InlineEquation> never exceeds <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(t_0\Vert TP^-\Vert \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>t</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">‖</mo> <mi>T</mi> <msup> <mi>P</mi> <mo>-</mo> </msup> <mo stretchy="false">‖</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for some constant <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(t_0\approx 1.84\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>t</mi> <mn>0</mn> </msub> <mo>≈</mo> <mn>1.84</mn> </mrow> </math></EquationSource> </InlineEquation>. The result applies to a closed symmetric relation <i>T</i> and carries on a suitable, most notably dissipative, extension.</p>

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Location of non-real eigenvalues of a class of linear relations in a Krein space

  • Rytis Juršėnas

摘要

It is a classical result that, if T is a maximal symmetric operator in a Krein space \(\mathscr {H}=\mathscr {H}^+[\dotplus ]\mathscr {H}^-\) H = H + [ ] H - with the domain \(\mathscr {D}_T\supset \mathscr {H}^-\) D T H - , then the imaginary part of its eigenvalue \(\lambda \) λ from upper or lower half-plane is bounded by \(|{{\,\textrm{Im}\,}}\lambda |\leqslant 2\Vert TP^-\Vert \) | Im λ | 2 T P - . We prove that in both half-planes \(|{{\,\textrm{Im}\,}}\lambda |\) | Im λ | never exceeds \(t_0\Vert TP^-\Vert \) t 0 T P - for some constant \(t_0\approx 1.84\) t 0 1.84 . The result applies to a closed symmetric relation T and carries on a suitable, most notably dissipative, extension.