<p>We studied the late-time acceleration scenarios using a quintessence field initially trapped in a metastable false vacuum state. The false vacuum has non-zero vacuum energy and can drive exponential expansion if not coupled with gravity. Upon decay of the false vacuum, the quintessence field is released and begins to evolve. We assumed conditions where the effective scalar potential gradient must satisfy <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(\nabla V_{\text {eff}} &gt; A\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">∇</mi> <msub> <mi>V</mi> <mtext>eff</mtext> </msub> <mo>&gt;</mo> <mi>A</mi> </mrow> </math></EquationSource> </InlineEquation>, characterised by a pressure term approximately <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="99" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta p / p &gt; \mathcal {O} (\hbar )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mi>p</mi> <mo stretchy="false">/</mo> <mi>p</mi> <mo>&gt;</mo> <mi mathvariant="script">O</mi> <mo stretchy="false">(</mo> <mi>ħ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> invoking the string swampland criteria. We then derived the effective potential of the scalar with an upper bound on the coupling constant <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda &lt; 0.6\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>&lt;</mo> <mn>0.6</mn> </mrow> </math></EquationSource> </InlineEquation>. Further analysis revealed that <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(V_{\text {eff}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mtext>eff</mtext> </msub> </math></EquationSource> </InlineEquation> shows a slow-roll behaviour for <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq5.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="119" /> </InlineMediaObject> <EquationSource Format="TEX">\(0.1&gt; \lambda &gt; -0.04\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0.1</mn> <mo>&gt;</mo> <mi>λ</mi> <mo>&gt;</mo> <mo>-</mo> <mn>0.04</mn> </mrow> </math></EquationSource> </InlineEquation> in the effective dark energy equation of state (EoS) <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="134" /> </InlineMediaObject> <EquationSource Format="TEX">\(-0.8&lt; w_0 &lt; -0.4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mn>0.8</mn> <mo>&lt;</mo> <msub> <mi>w</mi> <mn>0</mn> </msub> <mo>&lt;</mo> <mo>-</mo> <mn>0.4</mn> </mrow> </math></EquationSource> </InlineEquation>, stabilising at points between <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="104" /> </InlineMediaObject> <EquationSource Format="TEX">\(1&lt; A &lt; 2.718\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>A</mi> <mo>&lt;</mo> <mn>2.718</mn> </mrow> </math></EquationSource> </InlineEquation>. Our results suggest a stable scalar decoupled from its initial metastable state can indeed lead to a more stable Universe at later times. However, slight deviations in parameter orders can potentially violate the swampland criteria if <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12043_2025_2910_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(V_{\text {eff}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mtext>eff</mtext> </msub> </math></EquationSource> </InlineEquation> grows too rapidly. Since this is not something we expect, it opens up the possibility that the current dark energy configuration might be a result of a slowly varying scalar potential rather than being arbitrary.</p>

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Quintessence and false vacuum: Two sides of the same coin?

  • M V Pradosh Keshav,
  • Kenath Arun

摘要

We studied the late-time acceleration scenarios using a quintessence field initially trapped in a metastable false vacuum state. The false vacuum has non-zero vacuum energy and can drive exponential expansion if not coupled with gravity. Upon decay of the false vacuum, the quintessence field is released and begins to evolve. We assumed conditions where the effective scalar potential gradient must satisfy \(\nabla V_{\text {eff}} > A\) V eff > A , characterised by a pressure term approximately \(\Delta p / p > \mathcal {O} (\hbar )\) Δ p / p > O ( ħ ) invoking the string swampland criteria. We then derived the effective potential of the scalar with an upper bound on the coupling constant \(\lambda < 0.6\) λ < 0.6 . Further analysis revealed that \(V_{\text {eff}}\) V eff shows a slow-roll behaviour for \(0.1> \lambda > -0.04\) 0.1 > λ > - 0.04 in the effective dark energy equation of state (EoS) \(-0.8< w_0 < -0.4\) - 0.8 < w 0 < - 0.4 , stabilising at points between \(1< A < 2.718\) 1 < A < 2.718 . Our results suggest a stable scalar decoupled from its initial metastable state can indeed lead to a more stable Universe at later times. However, slight deviations in parameter orders can potentially violate the swampland criteria if \(V_{\text {eff}}\) V eff grows too rapidly. Since this is not something we expect, it opens up the possibility that the current dark energy configuration might be a result of a slowly varying scalar potential rather than being arbitrary.