<p>We consider the three-particle Schrödinger operator <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{a,b},\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>H</mi> <mrow> <mi>a</mi> <mo>,</mo> <mi>b</mi> </mrow> </msub> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(a,b&gt;0,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> associated with a system of three particles (two bosons with mass 1, interacting via zero-range pair potentials of strength <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(b&gt;0,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> and one arbitrary particle with mass <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(m&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, interacting with bosons via a zero-range potential of strength <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq5.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(a&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) on the three-dimensional lattice <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\( \mathbb {Z}^3.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="double-struck">Z</mi> </mrow> <mn>3</mn> </msup> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> We establish the exact number of the discrete eigenvalues of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{a,b}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mrow> <mi>a</mi> <mo>,</mo> <mi>b</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> below its essential spectrum in the cases when a boson interacts with the third particle strongly (that is <i>b</i> is fixed and <i>a</i> is large) and when two bosons strongly interact (that is for fixed <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1841_Article_IEq5.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(a&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and large <i>b</i>).</p>

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Bound states of strongly interacting three-body systems on a lattice

  • J. I. Abdullaev,
  • A. M. Khalkhuzhaev,
  • J.Kh. Boymurodov

摘要

We consider the three-particle Schrödinger operator \(H_{a,b},\) H a , b , \(a,b>0,\) a , b > 0 , associated with a system of three particles (two bosons with mass 1, interacting via zero-range pair potentials of strength \(b>0,\) b > 0 , and one arbitrary particle with mass \(m>0\) m > 0 , interacting with bosons via a zero-range potential of strength \(a>0\) a > 0 ) on the three-dimensional lattice \( \mathbb {Z}^3.\) Z 3 . We establish the exact number of the discrete eigenvalues of \(H_{a,b}\) H a , b below its essential spectrum in the cases when a boson interacts with the third particle strongly (that is b is fixed and a is large) and when two bosons strongly interact (that is for fixed \(a>0\) a > 0 and large b).