<p>In this paper, we provide necessary and sufficient conditions on a triple of weights (<i>u</i>,&#xa0;<i>v</i>,&#xa0;<i>w</i>) so that the <i>t</i>-Haar multipliers <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq1.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(T^t_{w,\sigma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>T</mi> <mrow> <mi>w</mi> <mo>,</mo> <mi>σ</mi> </mrow> <mi>t</mi> </msubsup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, are uniformly (on the choice of signs <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sigma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>σ</mi> </math></EquationSource> </InlineEquation>) bounded from <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^2(u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> into <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^2(v)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. These dyadic operators have symbols <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq6.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="182" /> </InlineMediaObject> <EquationSource Format="TEX">\(s(x,I)=\sigma _I\,(w(x)/\langle w\rangle _I)^t\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>I</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>σ</mi> <mi>I</mi> </msub> <mspace width="0.166667em" /> <msup> <mrow> <mo stretchy="false">(</mo> <mi>w</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">/</mo> <msub> <mrow> <mo stretchy="false">⟨</mo> <mi>w</mi> <mo stretchy="false">⟩</mo> </mrow> <mi>I</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mi>t</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> which are functions of the space variable <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(x\in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> and the frequency variable <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(I\in \mathcal {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>I</mi> <mo>∈</mo> <mi mathvariant="script">D</mi> </mrow> </math></EquationSource> </InlineEquation>, making them dyadic analogues of pseudo-differential operators. Here <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq9.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">D</mi> </math></EquationSource> </InlineEquation> denotes the dyadic intervals, <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sigma _I=\pm 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>σ</mi> <mi>I</mi> </msub> <mo>=</mo> <mo>±</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq11.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\(\langle w\rangle _I\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">⟨</mo> <mi>w</mi> <mo stretchy="false">⟩</mo> </mrow> <mi>I</mi> </msub> </math></EquationSource> </InlineEquation> denotes the integral average of <i>w</i> on <i>I</i>. When <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq12.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(w\equiv 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>w</mi> <mo>≡</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> we have the martingale transform and our conditions recover the known two-weight necessary and sufficient conditions of Nazarov, Treil and Volberg. We also show how these conditions are simplified when <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq13.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(u=v\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <mi>v</mi> </mrow> </math></EquationSource> </InlineEquation>. In particular, the martingale one-weight and the <i>t</i>-Haar multiplier unsigned and unweighted (corresponding to <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq14.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sigma _I\equiv 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>σ</mi> <mi>I</mi> </msub> <mo>≡</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2011_Article_IEq15.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="73" /> </InlineMediaObject> <EquationSource Format="TEX">\(u=v\equiv 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <mi>v</mi> <mo>≡</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>) known results are recovered or improved. We also obtain necessary and sufficient testing conditions of Sawyer type for the two-weight boundedness of a single variable Haar multiplier similar to those known for the martingale transform.</p>

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Weighted Inequalities for t-Haar Multipliers

  • Daewon Chung,
  • Weiyan Huang,
  • Jean Carlo Moraes,
  • María Cristina Pereyra,
  • Brett D. Wick

摘要

In this paper, we provide necessary and sufficient conditions on a triple of weights (uvw) so that the t-Haar multipliers \(T^t_{w,\sigma }\) T w , σ t , \(t\in \mathbb {R}\) t R , are uniformly (on the choice of signs \(\sigma \) σ ) bounded from \(L^2(u)\) L 2 ( u ) into \(L^2(v)\) L 2 ( v ) . These dyadic operators have symbols \(s(x,I)=\sigma _I\,(w(x)/\langle w\rangle _I)^t\) s ( x , I ) = σ I ( w ( x ) / w I ) t which are functions of the space variable \(x\in \mathbb {R}\) x R and the frequency variable \(I\in \mathcal {D}\) I D , making them dyadic analogues of pseudo-differential operators. Here \(\mathcal {D}\) D denotes the dyadic intervals, \(\sigma _I=\pm 1\) σ I = ± 1 , and \(\langle w\rangle _I\) w I denotes the integral average of w on I. When \(w\equiv 1\) w 1 we have the martingale transform and our conditions recover the known two-weight necessary and sufficient conditions of Nazarov, Treil and Volberg. We also show how these conditions are simplified when \(u=v\) u = v . In particular, the martingale one-weight and the t-Haar multiplier unsigned and unweighted (corresponding to \(\sigma _I\equiv 1\) σ I 1 and \(u=v\equiv 1\) u = v 1 ) known results are recovered or improved. We also obtain necessary and sufficient testing conditions of Sawyer type for the two-weight boundedness of a single variable Haar multiplier similar to those known for the martingale transform.