<p>We combine the Yang-Baxter (YB) and bi-Yang-Baxter (bi-YB) deformations with higher-spin auxiliary field deformations to construct multi-parameter families of integrable deformations of the principal chiral model on a Lie group <i>G</i> with semi-simple Lie algebra <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq1.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="fraktur">g</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathfrak{g} \)</EquationSource> </InlineEquation>. In the YB case, our construction produces one integrable deformation for each pair (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">R</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{R} \)</EquationSource> </InlineEquation><i>, E</i>), where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">R</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{R} \)</EquationSource> </InlineEquation> is an antisymmetric bilinear operator on <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq1.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="fraktur">g</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathfrak{g} \)</EquationSource> </InlineEquation> obeying the modified classical Yang-Baxter equation and <i>E</i> is a function of several variables. In the bi-YB case, the pair becomes a triplet (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">R</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{R} \)</EquationSource> </InlineEquation><i>,</i> <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq6.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <mi mathvariant="script">R</mi> <mo stretchy="true">~</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overset{\sim }{\mathcal{R}} \)</EquationSource> </InlineEquation><i>, E</i>), where <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq6.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <mi mathvariant="script">R</mi> <mo stretchy="true">~</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overset{\sim }{\mathcal{R}} \)</EquationSource> </InlineEquation> is another antisymmetric bilinear operator on <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26298_Article_IEq1.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="fraktur">g</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathfrak{g} \)</EquationSource> </InlineEquation> obeying the modified classical Yang-Baxter equation. We show that every model in these families is (weakly) classically integrable by exhibiting a Lax representation for their equations of motion.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Auxiliary field sigma models and Yang-Baxter deformations

  • Daniele Bielli,
  • Christian Ferko,
  • Liam Smith,
  • Gabriele Tartaglino-Mazzucchelli

摘要

We combine the Yang-Baxter (YB) and bi-Yang-Baxter (bi-YB) deformations with higher-spin auxiliary field deformations to construct multi-parameter families of integrable deformations of the principal chiral model on a Lie group G with semi-simple Lie algebra g \( \mathfrak{g} \) . In the YB case, our construction produces one integrable deformation for each pair ( R \( \mathcal{R} \) , E), where R \( \mathcal{R} \) is an antisymmetric bilinear operator on g \( \mathfrak{g} \) obeying the modified classical Yang-Baxter equation and E is a function of several variables. In the bi-YB case, the pair becomes a triplet ( R \( \mathcal{R} \) , R ~ \( \overset{\sim }{\mathcal{R}} \) , E), where R ~ \( \overset{\sim }{\mathcal{R}} \) is another antisymmetric bilinear operator on g \( \mathfrak{g} \) obeying the modified classical Yang-Baxter equation. We show that every model in these families is (weakly) classically integrable by exhibiting a Lax representation for their equations of motion.