<p>The main objective of this paper is to extend certain fundamental inequalities from a single function to a family of orthonormal systems. In the first part of the paper, we consider a non-negative, self-adjoint operator <i>L</i> on <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L^2(X,\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\((X,\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is a measure space. Under the assumption that the kernel <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(K_{it}(x,y)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>K</mi> <mrow> <mi mathvariant="italic">it</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> of the Schrödinger propagator <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(e^{itL}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mi mathvariant="italic">itL</mi> </mrow> </msup> </math></EquationSource> </InlineEquation> satisfies a uniform <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>∞</mi> </msup> </math></EquationSource> </InlineEquation>-decay estimate of the form <Equation ID="Equ58"> <EquationSource Format="TEX">\(\begin{aligned} \sup _{x,y\in X}|K_{it}(x,y)|\lesssim |t|^{-\frac{n}{2}},\,|t|&lt;T_0, {\text { for some }}n\ge 1, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <munder> <mo movablelimits="true">sup</mo> <mrow> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>∈</mo> <mi>X</mi> </mrow> </munder> <mrow> <mo stretchy="false">|</mo> </mrow> <msub> <mi>K</mi> <mrow> <mi mathvariant="italic">it</mi> </mrow> </msub> <msup> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> <mo>≲</mo> <mo stretchy="false">|</mo> <mi>t</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mfrac> <mi>n</mi> <mn>2</mn> </mfrac> </mrow> </msup> <mo>,</mo> <mspace width="0.166667em" /> <mrow> <mo stretchy="false">|</mo> <mi>t</mi> <mo stretchy="false">|</mo> </mrow> <mo>&lt;</mo> <msub> <mi>T</mi> <mn>0</mn> </msub> <mo>,</mo> <mrow> <mspace width="0.333333em" /> <mtext>for some</mtext> <mspace width="0.333333em" /> </mrow> <mi>n</mi> <mo>≥</mo> <mn>1</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(T_0\in (0,+\infty ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>T</mi> <mn>0</mn> </msub> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mo>+</mo> <mi>∞</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, we establish Strichartz estimates for the Schrödinger propagator <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(e^{itL}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mi mathvariant="italic">itL</mi> </mrow> </msup> </math></EquationSource> </InlineEquation> and using a duality principle argument by Frank-Sabin [<CitationRef CitationID="CR11">11</CitationRef>], we extend it for a system of infinitely many fermions on <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(L^2(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We also obtain orthonormal Strichartz estimates for a class of dispersive semigroup <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(U(t)=e^{it\phi (L)}\psi (\sqrt{L}),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>U</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi>e</mi> <mrow> <mi>i</mi> <mi>t</mi> <mi>ϕ</mi> <mo stretchy="false">(</mo> <mi>L</mi> <mo stretchy="false">)</mo> </mrow> </msup> <mi>ψ</mi> <mrow> <mo stretchy="false">(</mo> <msqrt> <mi>L</mi> </msqrt> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> where <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\phi : \mathbb {R}^+\rightarrow \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϕ</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> </msup> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> is a smooth function and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\psi \in C_c^\infty ([\frac{1}{2},2])\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ψ</mi> <mo>∈</mo> <msubsup> <mi>C</mi> <mi>c</mi> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mrow> <mo stretchy="false">[</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo>,</mo> <mn>2</mn> <mo stretchy="false">]</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. As an application of these orthonormal versions of Strichartz estimates, we prove the well-posedness for the Hartree equation in the Schatten spaces. In the next part of the paper, we obtain some new orthonormal Strichartz estimates, which extend prior work of Kenig-Ponce-Vega [<CitationRef CitationID="CR22">22</CitationRef>] for single functions. Using those orthonormal versions of Kenig-Ponce-Vega result, we prove the orthonormal restriction theorem for the Fourier transform on some particular noncompact hypersurface of the form <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(S=\{(\xi , \phi (\xi )): \xi \in \mathbb {R}\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <mo>=</mo> <mo stretchy="false">{</mo> <mo stretchy="false">(</mo> <mi>ξ</mi> <mo>,</mo> <mi>ϕ</mi> <mo stretchy="false">(</mo> <mi>ξ</mi> <mo stretchy="false">)</mo> <mo stretchy="false">)</mo> <mo>:</mo> <mi>ξ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> satisfies certain growth condition.</p>

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Orthonormal Strichartz inequalities and their applications on abstract measure spaces

  • Guoxia Feng,
  • Shyam Swarup Mondal,
  • Manli Song,
  • Huoxiong Wu

摘要

The main objective of this paper is to extend certain fundamental inequalities from a single function to a family of orthonormal systems. In the first part of the paper, we consider a non-negative, self-adjoint operator L on \(L^2(X,\mu )\) L 2 ( X , μ ) , where \((X,\mu )\) ( X , μ ) is a measure space. Under the assumption that the kernel \(K_{it}(x,y)\) K it ( x , y ) of the Schrödinger propagator \(e^{itL}\) e itL satisfies a uniform \(L^\infty \) L -decay estimate of the form \(\begin{aligned} \sup _{x,y\in X}|K_{it}(x,y)|\lesssim |t|^{-\frac{n}{2}},\,|t|<T_0, {\text { for some }}n\ge 1, \end{aligned}\) sup x , y X | K it ( x , y ) | | t | - n 2 , | t | < T 0 , for some n 1 , where \(T_0\in (0,+\infty ]\) T 0 ( 0 , + ] , we establish Strichartz estimates for the Schrödinger propagator \(e^{itL}\) e itL and using a duality principle argument by Frank-Sabin [11], we extend it for a system of infinitely many fermions on \(L^2(X)\) L 2 ( X ) . We also obtain orthonormal Strichartz estimates for a class of dispersive semigroup \(U(t)=e^{it\phi (L)}\psi (\sqrt{L}),\) U ( t ) = e i t ϕ ( L ) ψ ( L ) , where \(\phi : \mathbb {R}^+\rightarrow \mathbb {R}\) ϕ : R + R is a smooth function and \(\psi \in C_c^\infty ([\frac{1}{2},2])\) ψ C c ( [ 1 2 , 2 ] ) . As an application of these orthonormal versions of Strichartz estimates, we prove the well-posedness for the Hartree equation in the Schatten spaces. In the next part of the paper, we obtain some new orthonormal Strichartz estimates, which extend prior work of Kenig-Ponce-Vega [22] for single functions. Using those orthonormal versions of Kenig-Ponce-Vega result, we prove the orthonormal restriction theorem for the Fourier transform on some particular noncompact hypersurface of the form \(S=\{(\xi , \phi (\xi )): \xi \in \mathbb {R}\}\) S = { ( ξ , ϕ ( ξ ) ) : ξ R } , where \(\phi \) ϕ satisfies certain growth condition.