<p>For a Banach lattice <i>X</i>, its lattice Schäffer constant is defined by <Equation ID="Equ14"> <EquationSource Format="TEX">\(\begin{aligned} \lambda ^+(X)=\inf \{\max \{\Vert x+y\Vert ,\Vert x-y\Vert \}\,:\,\Vert x\Vert =\Vert y\Vert =1,x,y\ge \textbf{0}\}. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msup> <mi>λ</mi> <mo>+</mo> </msup> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mo movablelimits="true">inf</mo> <mo stretchy="false">{</mo> <mo movablelimits="true">max</mo> <mo stretchy="false">{</mo> <mo stretchy="false">‖</mo> <mi>x</mi> <mo>+</mo> <mi>y</mi> <mo stretchy="false">‖</mo> <mo>,</mo> <mo stretchy="false">‖</mo> <mi>x</mi> <mo>-</mo> <mi>y</mi> <mo stretchy="false">‖</mo> <mo stretchy="false">}</mo> <mspace width="0.166667em" /> <mo>:</mo> <mspace width="0.166667em" /> <mo stretchy="false">‖</mo> <mi>x</mi> <mo stretchy="false">‖</mo> <mo>=</mo> <mo stretchy="false">‖</mo> <mi>y</mi> <mo stretchy="false">‖</mo> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>≥</mo> <mn mathvariant="bold">0</mn> <mo stretchy="false">}</mo> <mo>.</mo> </mrow> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>In this paper, we investigate this constant, as well as the companion parameter <Equation ID="Equ15"> <EquationSource Format="TEX">\(\begin{aligned} \beta (X)=\inf \{\Vert x\vee y\Vert \,:\, \Vert x\Vert =\Vert y\Vert =1, x,y\ge \textbf{0} \hbox { and } x\wedge y=\textbf{0}\}. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>β</mi> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mo movablelimits="true">inf</mo> <mo stretchy="false">{</mo> <mo stretchy="false">‖</mo> <mi>x</mi> <mo>∨</mo> <mi>y</mi> <mo stretchy="false">‖</mo> <mspace width="0.166667em" /> <mo>:</mo> <mspace width="0.166667em" /> <mo stretchy="false">‖</mo> <mi>x</mi> <mo stretchy="false">‖</mo> <mo>=</mo> <mo stretchy="false">‖</mo> <mi>y</mi> <mo stretchy="false">‖</mo> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>≥</mo> <mn mathvariant="bold">0</mn> <mspace width="0.333333em" /> <mtext>and</mtext> <mspace width="0.333333em" /> <mi>x</mi> <mo>∧</mo> <mi>y</mi> <mo>=</mo> <mn mathvariant="bold">0</mn> <mo stretchy="false">}</mo> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>Our main results fall into two groups. (1) We link the behavior of the parameters <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\lambda ^+\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>λ</mi> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\beta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> </InlineEquation> to the global properties of the lattice <i>X</i>. For instance, we prove that (i) if <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda ^+(X)&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>λ</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, then the Banach lattice <i>X</i> is a KB-space, and moreover, <i>X</i> is <i>q</i>-concave for some <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(q\in (1,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>; (ii) <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\lambda ^+(X)=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>λ</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> if and only if <i>X</i> contains lattice-almost isometric copies of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\ell _\infty ^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>ℓ</mi> <mi>∞</mi> <mn>2</mn> </msubsup> </math></EquationSource> </InlineEquation>; (iii) that <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\lambda ^+(X)=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>λ</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> if and only if <i>X</i> is an abstract <i>L</i>-space; and (iv) if X is a Banach lattice with <i>p</i>-convexity constant 1, then <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\lambda ^+(X)=2^{1/p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>λ</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mn>2</mn> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mi>p</mi> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> if and only if <i>X</i> is an abstract <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(L_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-space. (2) We establish inequalities relating <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\lambda ^+(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>λ</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to the characteristics of monotonicity, <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\varepsilon _{0,m}(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ε</mi> <mrow> <mn>0</mn> <mo>,</mo> <mi>m</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\tilde{\varepsilon }_{0,m}(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mover accent="true"> <mi>ε</mi> <mo stretchy="false">~</mo> </mover> <mrow> <mn>0</mn> <mo>,</mo> <mi>m</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Along the way, we compute <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\lambda ^+(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>λ</mi> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\beta (X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> for various Banach lattices <i>X</i>.</p>

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The lattice Schäffer constant

  • Michael A. Rincón-Villamizar,
  • Timur Oikhberg

摘要

For a Banach lattice X, its lattice Schäffer constant is defined by \(\begin{aligned} \lambda ^+(X)=\inf \{\max \{\Vert x+y\Vert ,\Vert x-y\Vert \}\,:\,\Vert x\Vert =\Vert y\Vert =1,x,y\ge \textbf{0}\}. \end{aligned}\) λ + ( X ) = inf { max { x + y , x - y } : x = y = 1 , x , y 0 } . In this paper, we investigate this constant, as well as the companion parameter \(\begin{aligned} \beta (X)=\inf \{\Vert x\vee y\Vert \,:\, \Vert x\Vert =\Vert y\Vert =1, x,y\ge \textbf{0} \hbox { and } x\wedge y=\textbf{0}\}. \end{aligned}\) β ( X ) = inf { x y : x = y = 1 , x , y 0 and x y = 0 } . Our main results fall into two groups. (1) We link the behavior of the parameters \(\lambda ^+\) λ + and \(\beta \) β to the global properties of the lattice X. For instance, we prove that (i) if \(\lambda ^+(X)>1\) λ + ( X ) > 1 , then the Banach lattice X is a KB-space, and moreover, X is q-concave for some \(q\in (1,\infty )\) q ( 1 , ) ; (ii) \(\lambda ^+(X)=1\) λ + ( X ) = 1 if and only if X contains lattice-almost isometric copies of \(\ell _\infty ^2\) 2 ; (iii) that \(\lambda ^+(X)=2\) λ + ( X ) = 2 if and only if X is an abstract L-space; and (iv) if X is a Banach lattice with p-convexity constant 1, then \(\lambda ^+(X)=2^{1/p}\) λ + ( X ) = 2 1 / p if and only if X is an abstract \(L_p\) L p -space. (2) We establish inequalities relating \(\lambda ^+(X)\) λ + ( X ) to the characteristics of monotonicity, \(\varepsilon _{0,m}(X)\) ε 0 , m ( X ) and \(\tilde{\varepsilon }_{0,m}(X)\) ε ~ 0 , m ( X ) . Along the way, we compute \(\lambda ^+(X)\) λ + ( X ) and \(\beta (X)\) β ( X ) for various Banach lattices X.