<p>Potentials in cosmological inflation often involve scalars with trans-Planckian ranges. As a result, towers of states become massless and their presence pushes the fundamental scale not to coincide with <i>M</i><sub>P</sub> but rather with the <i>species scale</i>, Λ. This scale transforms as an automorphic form of the theory’s duality symmetries. We propose that the inflaton potential should be 1) an automorphic invariant form, non-singular over all moduli space, 2) depending only on Λ and its field derivatives, and 3) approaching constant values in the region of large moduli VEVs to ensure a long period of inflation. These conditions lead to the proposal <i>V</i> ~ <i>λ</i>(<i>ϕ, ϕ</i><sup>*</sup>), with <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25915_Article_IEq1.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="169" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi>λ</mi> <mo>=</mo> <msup> <mi>G</mi> <mrow> <mi>i</mi> <mover accent="true"> <mi>j</mi> <mo stretchy="true">¯</mo> </mover> </mrow> </msup> <mfenced close=")" open="("> <mrow> <msub> <mi>∂</mi> <mi>i</mi> </msub> <mi mathvariant="normal">Λ</mi> </mrow> </mfenced> <mfenced close=")" open="("> <mrow> <msub> <mi>∂</mi> <mover accent="true"> <mi>j</mi> <mo stretchy="true">¯</mo> </mover> </msub> <mi mathvariant="normal">Λ</mi> </mrow> </mfenced> <mo>/</mo> <msup> <mi mathvariant="normal">Λ</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">\( \lambda ={G}^{i\overline{j}}\left({\partial}_i\Lambda \right)\left({\partial}_{\overline{j}}\Lambda \right)/{\Lambda}^2 \)</EquationSource> </InlineEquation>, determining the ‘species scale convex hull’. For a single elliptic complex modulus with SL(2<i>, Z</i>) symmetry, this results in an inflaton potential <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25915_Article_IEq2.gif" Format="GIF" Height="38" Rendition="HTML" Resolution="72" Type="Linedraw" Width="154" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi>V</mi> <mo>≃</mo> <msup> <mfenced close=")" open="("> <mrow> <mo>Im</mo> <mi>τ</mi> </mrow> </mfenced> <mn>2</mn> </msup> <msup> <mfenced close="|" open="|"> <msub> <mover accent="true"> <mi>G</mi> <mo stretchy="true">~</mo> </mover> <mn>2</mn> </msub> </mfenced> <mn>2</mn> </msup> <mo>/</mo> <msup> <mi>N</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">\( V\simeq {\left(\operatorname{Im}\tau \right)}^2{\left|{\overset{\sim }{G}}_2\right|}^2/{N}^2 \)</EquationSource> </InlineEquation>, with <i>N</i> ≃ − log(Im<i>τ</i>|<i>η</i>(<i>τ</i>)|<sup>4</sup>), where <i>η</i> is the Dedekind function and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25915_Article_IEq3.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msub> <mover accent="true"> <mi>G</mi> <mo stretchy="true">~</mo> </mover> <mn>2</mn> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {\overset{\sim }{G}}_2 \)</EquationSource> </InlineEquation> the Eisenstein modular form of weight 2. Surprisingly, this potential at large modulus VEV resembles that of the Starobinsky model. We compute inflationary parameters yielding results similar to Starobinsky’s, but extended to modular invariant expressions. Interestingly, the number of e-folds is proportional to the number of species in the tower, <i>N</i><sub><i>e</i></sub> ≃ <i>N</i>, and <i>ϵ</i> ≃ Λ<sup>4</sup> at large moduli VEV, suggesting that the tower of states plays an important role in the inflation process.</p>

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Modular invariant Starobinsky inflation and the Species Scale

  • Gonzalo F. Casas,
  • Luis E. Ibáñez

摘要

Potentials in cosmological inflation often involve scalars with trans-Planckian ranges. As a result, towers of states become massless and their presence pushes the fundamental scale not to coincide with MP but rather with the species scale, Λ. This scale transforms as an automorphic form of the theory’s duality symmetries. We propose that the inflaton potential should be 1) an automorphic invariant form, non-singular over all moduli space, 2) depending only on Λ and its field derivatives, and 3) approaching constant values in the region of large moduli VEVs to ensure a long period of inflation. These conditions lead to the proposal V ~ λ(ϕ, ϕ*), with λ = G i j ¯ i Λ j ¯ Λ / Λ 2 \( \lambda ={G}^{i\overline{j}}\left({\partial}_i\Lambda \right)\left({\partial}_{\overline{j}}\Lambda \right)/{\Lambda}^2 \) , determining the ‘species scale convex hull’. For a single elliptic complex modulus with SL(2, Z) symmetry, this results in an inflaton potential V Im τ 2 G ~ 2 2 / N 2 \( V\simeq {\left(\operatorname{Im}\tau \right)}^2{\left|{\overset{\sim }{G}}_2\right|}^2/{N}^2 \) , with N ≃ − log(Imτ|η(τ)|4), where η is the Dedekind function and G ~ 2 \( {\overset{\sim }{G}}_2 \) the Eisenstein modular form of weight 2. Surprisingly, this potential at large modulus VEV resembles that of the Starobinsky model. We compute inflationary parameters yielding results similar to Starobinsky’s, but extended to modular invariant expressions. Interestingly, the number of e-folds is proportional to the number of species in the tower, NeN, and ϵ ≃ Λ4 at large moduli VEV, suggesting that the tower of states plays an important role in the inflation process.