<p>Pluto’s argument of perihelion is known to librate around <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10569_2025_10249_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(90^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>90</mn> <mo>∘</mo> </msup> </math></EquationSource> </InlineEquation>. This libration is related to the secular phenomenon known as the von Zeipel–Lidov–Kozai (vZLK) oscillation. In this work, we make a quantitative assessment of the influence of Neptune’s mean motion resonance and of the other giant planets’ secular perturbations on the libration of Pluto’s argument of perihelion. Here, a parameter <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10569_2025_10249_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="138" /> </InlineMediaObject> <EquationSource Format="TEX">\(k^2 = (1-e^2) \cos ^2 I\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>k</mi> <mn>2</mn> </msup> <mo>=</mo> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <msup> <mi>e</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> <msup> <mo>cos</mo> <mn>2</mn> </msup> <mi>I</mi> </mrow> </math></EquationSource> </InlineEquation> is the key where <i>e</i> is eccentricity and <i>I</i> is inclination. When <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10569_2025_10249_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(k^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>k</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> of a Pluto-like object is larger than a certain critical value, libration of its argument of perihelion would not occur. The secular effect of other disturbing planets (Jupiter, Saturn, Uranus) plays a significant role in determining the critical <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10569_2025_10249_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(k^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>k</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>. The nonzero oscillation amplitude of the critical resonant argument also plays a role, although not a dominant one.</p>

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Libration of Pluto’s argument of perihelion and the role of the major planets

  • Takashi Ito,
  • Renu Malhotra

摘要

Pluto’s argument of perihelion is known to librate around \(90^\circ \) 90 . This libration is related to the secular phenomenon known as the von Zeipel–Lidov–Kozai (vZLK) oscillation. In this work, we make a quantitative assessment of the influence of Neptune’s mean motion resonance and of the other giant planets’ secular perturbations on the libration of Pluto’s argument of perihelion. Here, a parameter \(k^2 = (1-e^2) \cos ^2 I\) k 2 = ( 1 - e 2 ) cos 2 I is the key where e is eccentricity and I is inclination. When \(k^2\) k 2 of a Pluto-like object is larger than a certain critical value, libration of its argument of perihelion would not occur. The secular effect of other disturbing planets (Jupiter, Saturn, Uranus) plays a significant role in determining the critical \(k^2\) k 2 . The nonzero oscillation amplitude of the critical resonant argument also plays a role, although not a dominant one.