<p>In this article we characterize the existence of ring solutions to the <i>n</i>-body problem on <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathbb {S}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>, parametrized by the circumradius <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(a \in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. For configurations with identical masses <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(m_j= m, j=1, \ldots , n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>m</mi> <mi>j</mi> </msub> <mo>=</mo> <mi>m</mi> <mo>,</mo> <mi>j</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mi>n</mi> </mrow> </math></EquationSource> </InlineEquation>, we show that when <i>n</i> is even, there exists a single bifurcation value associated with <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\omega ^2/m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ω</mi> <mn>2</mn> </msup> <mo stretchy="false">/</mo> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation> (where <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ω</mi> </math></EquationSource> </InlineEquation> is the angular velocity), for which there may exist zero, one, or two admissible values of <i>a</i> for which ring solutions exist, while for odd <i>n</i>, there are two bifurcation values of <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\omega ^2/m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ω</mi> <mn>2</mn> </msup> <mo stretchy="false">/</mo> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation>, leading again to zero, one, or two possible values of <i>a</i> for which ring solutions exist. On the other hand, we prove that if <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\frac{n}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mfrac> <mi>n</mi> <mn>2</mn> </mfrac> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\frac{n-1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mfrac> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> <mn>2</mn> </mfrac> </math></EquationSource> </InlineEquation> is even, then there exists a value of the circumradius <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(a_* \in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mi>a</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> such that the ring solution admits non-identical masses. In this case, we also provide an explicit parameterization of the corresponding mass distribution. Important differences with the Newtonian case are found.</p>

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On the Existence of Ring Solutions in the N-Body Problem on \(\mathbb {S}^2\)

  • Jaime Andrade,
  • Claudio Vidal

摘要

In this article we characterize the existence of ring solutions to the n-body problem on \(\mathbb {S}^2\) S 2 , parametrized by the circumradius \(a \in (0,1)\) a ( 0 , 1 ) . For configurations with identical masses \(m_j= m, j=1, \ldots , n\) m j = m , j = 1 , , n , we show that when n is even, there exists a single bifurcation value associated with \(\omega ^2/m\) ω 2 / m (where \(\omega \) ω is the angular velocity), for which there may exist zero, one, or two admissible values of a for which ring solutions exist, while for odd n, there are two bifurcation values of \(\omega ^2/m\) ω 2 / m , leading again to zero, one, or two possible values of a for which ring solutions exist. On the other hand, we prove that if \(\frac{n}{2}\) n 2 or \(\frac{n-1}{2}\) n - 1 2 is even, then there exists a value of the circumradius \(a_* \in (0,1)\) a ( 0 , 1 ) such that the ring solution admits non-identical masses. In this case, we also provide an explicit parameterization of the corresponding mass distribution. Important differences with the Newtonian case are found.