<p>We consider essential self-adjointness of strongly singular, homogeneous, polyharmonic operators of the form <Equation ID="Equ182"> <EquationSource Format="TEX">\( T_m = \left( (-\Delta )^m +c|x|^{-2\,m}\right) \big |_{C_0^{\infty }({\mathbb {R}}^n \backslash \{0\})}, \quad m \in {\mathbb {N}}, \; n \in {\mathbb {N}}, n\ge 2, \; c \in {\mathbb {R}}, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mi>T</mi> <mi>m</mi> </msub> <mo>=</mo> <mfenced close=")" open="("> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>m</mi> </msup> <mo>+</mo> <mi>c</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mn>2</mn> <mspace width="0.166667em" /> <mi>m</mi> </mrow> </msup> </mfenced> <msub> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">|</mo> </mrow> <mrow> <msubsup> <mi>C</mi> <mn>0</mn> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>,</mo> <mspace width="1em" /> <mi>m</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> <mo>,</mo> <mspace width="0.277778em" /> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> <mo>,</mo> <mi>n</mi> <mo>≥</mo> <mn>2</mn> <mo>,</mo> <mspace width="0.277778em" /> <mi>c</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> </mrow> </math></EquationSource> </Equation>in <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L^2({\mathbb {R}}^n; d^n x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>;</mo> <msup> <mi>d</mi> <mi>n</mi> </msup> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, with special emphasis on the biharmonic case <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(m=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> and the case <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(m=3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>=</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>. For instance, in the biharmonic case <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(m=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> we prove the sharp result <Equation ID="Equ183"> <EquationSource Format="TEX">\(\begin{aligned}&amp;T_2 \text { is essentially self-adjoint if and only if} \\&amp;\quad c\ge {\left\{ \begin{array}{ll} 3(n+2)(6-n) &amp; \text { for } 2\le n\le 5; \\ {\displaystyle -\frac{(n+4)n(n-4)(n-8)}{16}}&amp; \text {for } n\ge 6. \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <msub> <mi>T</mi> <mn>2</mn> </msub> <mspace width="0.333333em" /> <mtext>is essentially self-adjoint if and only if</mtext> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mi>c</mi> <mo>≥</mo> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mn>3</mn> <mo stretchy="false">(</mo> <mi>n</mi> <mo>+</mo> <mn>2</mn> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> <mn>6</mn> <mo>-</mo> <mi>n</mi> <mo stretchy="false">)</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>for</mtext> <mspace width="0.333333em" /> <mn>2</mn> <mo>≤</mo> <mi>n</mi> <mo>≤</mo> <mn>5</mn> <mo>;</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mo>-</mo> <mfrac> <mrow> <mo stretchy="false">(</mo> <mi>n</mi> <mo>+</mo> <mn>4</mn> <mo stretchy="false">)</mo> <mi>n</mi> <mo stretchy="false">(</mo> <mi>n</mi> <mo>-</mo> <mn>4</mn> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> <mi>n</mi> <mo>-</mo> <mn>8</mn> <mo stretchy="false">)</mo> </mrow> <mn>16</mn> </mfrac> </mrow> </mstyle> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>for</mtext> <mspace width="0.333333em" /> <mi>n</mi> <mo>≥</mo> <mn>6</mn> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>In particular, in the special (nonsingular) case <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(c=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\((-\Delta )^2\big |_{C_0^{\infty }({\mathbb {R}}^n \backslash \{0\})}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> <msub> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">|</mo> </mrow> <mrow> <msubsup> <mi>C</mi> <mn>0</mn> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> is essentially self-adjoint in <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(L^2({\mathbb {R}}^n; d^n x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>;</mo> <msup> <mi>d</mi> <mi>n</mi> </msup> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> if and only if <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(n \ge 8\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>8</mn> </mrow> </math></EquationSource> </InlineEquation>. Similarly, we derive the analogous sharp essential self-adjointness result for <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(T_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> (i.e., for <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(m=3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>=</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>) for all space dimensions <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(n \in {\mathbb {N}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(n \ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. Our methods generalize to homogenous polyharmonic differential operators; however, there are some nontrivial subtleties that arise. For example, the natural expectation that for <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(m, n \in {\mathbb {N}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(n \ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, there exist <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(c_{m,n} \in {\mathbb {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>c</mi> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> </mrow> </msub> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> such that <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\left( (-\Delta )^m +c|x|^{-2m}\right) \big |_{C_0^{\infty }({\mathbb {R}}^n \backslash \{0\})}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfenced close=")" open="("> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>m</mi> </msup> <mo>+</mo> <mi>c</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mn>2</mn> <mi>m</mi> </mrow> </msup> </mfenced> <msub> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">|</mo> </mrow> <mrow> <msubsup> <mi>C</mi> <mn>0</mn> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> is essentially self-adjoint in <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(L^2({\mathbb {R}}^n; d^n x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>;</mo> <msup> <mi>d</mi> <mi>n</mi> </msup> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> if and only if <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(c \ge c_{m,n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>≥</mo> <msub> <mi>c</mi> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, turns out to be false. Indeed, for <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(n=20\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>=</mo> <mn>20</mn> </mrow> </math></EquationSource> </InlineEquation>, we prove that the differential operator <Equation ID="Equ184"> <EquationSource Format="TEX">\( \left( (-\Delta )^5 +c|x|^{-10}\right) \big |_{C_0^{\infty }({\mathbb {R}}^{20} \backslash \{0\})}, \quad c \in {\mathbb {R}}, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mfenced close=")" open="("> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mn>5</mn> </msup> <mo>+</mo> <mi>c</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mn>10</mn> </mrow> </msup> </mfenced> <msub> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">|</mo> </mrow> <mrow> <msubsup> <mi>C</mi> <mn>0</mn> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>20</mn> </msup> <mo stretchy="true">\</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>,</mo> <mspace width="1em" /> <mi>c</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> </mrow> </math></EquationSource> </Equation>is essentially self-adjoint in <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(L^2\big ( {\mathbb {R}}^{20}; d^{20} x\big )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>20</mn> </msup> <mo>;</mo> <msup> <mi>d</mi> <mn>20</mn> </msup> <mi>x</mi> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> if and only if <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(c\in [0,\beta ]\cup [\gamma ,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>β</mi> <mo stretchy="false">]</mo> <mo>∪</mo> <mo stretchy="false">[</mo> <mi>γ</mi> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(\beta \approx 1.0436\times 10^{10}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>≈</mo> <mn>1.0436</mn> <mo>×</mo> <msup> <mn>10</mn> <mn>10</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(\gamma \approx 1.8324 \times 10^{10}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>≈</mo> <mn>1.8324</mn> <mo>×</mo> <msup> <mn>10</mn> <mn>10</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> are the two real roots of a particular quartic equation with integer coefficients (see Theorem <InternalRef RefID="FPar15">4.4</InternalRef>, eq.&#xa0;(<InternalRef RefID="Equ123">4.29</InternalRef>)).</p>

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Essential Self-Adjointness of Strongly Singular Homogeneous Polyharmonic Operators

  • Fritz Gesztesy,
  • Markus Hunziker

摘要

We consider essential self-adjointness of strongly singular, homogeneous, polyharmonic operators of the form \( T_m = \left( (-\Delta )^m +c|x|^{-2\,m}\right) \big |_{C_0^{\infty }({\mathbb {R}}^n \backslash \{0\})}, \quad m \in {\mathbb {N}}, \; n \in {\mathbb {N}}, n\ge 2, \; c \in {\mathbb {R}}, \) T m = ( - Δ ) m + c | x | - 2 m | C 0 ( R n \ { 0 } ) , m N , n N , n 2 , c R , in \(L^2({\mathbb {R}}^n; d^n x)\) L 2 ( R n ; d n x ) , with special emphasis on the biharmonic case \(m=2\) m = 2 and the case \(m=3\) m = 3 . For instance, in the biharmonic case \(m=2\) m = 2 we prove the sharp result \(\begin{aligned}&T_2 \text { is essentially self-adjoint if and only if} \\&\quad c\ge {\left\{ \begin{array}{ll} 3(n+2)(6-n) & \text { for } 2\le n\le 5; \\ {\displaystyle -\frac{(n+4)n(n-4)(n-8)}{16}}& \text {for } n\ge 6. \end{array}\right. } \end{aligned}\) T 2 is essentially self-adjoint if and only if c 3 ( n + 2 ) ( 6 - n ) for 2 n 5 ; - ( n + 4 ) n ( n - 4 ) ( n - 8 ) 16 for n 6 . In particular, in the special (nonsingular) case \(c=0\) c = 0 , \((-\Delta )^2\big |_{C_0^{\infty }({\mathbb {R}}^n \backslash \{0\})}\) ( - Δ ) 2 | C 0 ( R n \ { 0 } ) is essentially self-adjoint in \(L^2({\mathbb {R}}^n; d^n x)\) L 2 ( R n ; d n x ) if and only if \(n \ge 8\) n 8 . Similarly, we derive the analogous sharp essential self-adjointness result for \(T_3\) T 3 (i.e., for \(m=3\) m = 3 ) for all space dimensions \(n \in {\mathbb {N}}\) n N , \(n \ge 2\) n 2 . Our methods generalize to homogenous polyharmonic differential operators; however, there are some nontrivial subtleties that arise. For example, the natural expectation that for \(m, n \in {\mathbb {N}}\) m , n N , \(n \ge 2\) n 2 , there exist \(c_{m,n} \in {\mathbb {R}}\) c m , n R such that \(\left( (-\Delta )^m +c|x|^{-2m}\right) \big |_{C_0^{\infty }({\mathbb {R}}^n \backslash \{0\})}\) ( - Δ ) m + c | x | - 2 m | C 0 ( R n \ { 0 } ) is essentially self-adjoint in \(L^2({\mathbb {R}}^n; d^n x)\) L 2 ( R n ; d n x ) if and only if \(c \ge c_{m,n}\) c c m , n , turns out to be false. Indeed, for \(n=20\) n = 20 , we prove that the differential operator \( \left( (-\Delta )^5 +c|x|^{-10}\right) \big |_{C_0^{\infty }({\mathbb {R}}^{20} \backslash \{0\})}, \quad c \in {\mathbb {R}}, \) ( - Δ ) 5 + c | x | - 10 | C 0 ( R 20 \ { 0 } ) , c R , is essentially self-adjoint in \(L^2\big ( {\mathbb {R}}^{20}; d^{20} x\big )\) L 2 ( R 20 ; d 20 x ) if and only if \(c\in [0,\beta ]\cup [\gamma ,\infty )\) c [ 0 , β ] [ γ , ) , where \(\beta \approx 1.0436\times 10^{10}\) β 1.0436 × 10 10 , and \(\gamma \approx 1.8324 \times 10^{10}\) γ 1.8324 × 10 10 are the two real roots of a particular quartic equation with integer coefficients (see Theorem 4.4, eq. (4.29)).