<p>Let <i>L</i> be a field of positive characteristic <i>p</i> with a fixed algebraic closure <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\overline{L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mi>L</mi> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation>, and let <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\alpha _1,\alpha _2,\beta \in L\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo>,</mo> <mi>β</mi> <mo>∈</mo> <mi>L</mi> </mrow> </math></EquationSource> </InlineEquation>. For an integer <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(d\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, we consider the family of polynomials <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(f_{\lambda }(z):= z^d+\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>f</mi> <mi>λ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo>:</mo> <mo>=</mo> <msup> <mi>z</mi> <mi>d</mi> </msup> <mo>+</mo> <mi>λ</mi> </mrow> </math></EquationSource> </InlineEquation>, parameterized by <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\lambda \in \overline{L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mover> <mi>L</mi> <mo>¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation>. Define <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(C(\alpha _1,\alpha _2;\beta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mo stretchy="false">(</mo> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo>;</mo> <mi>β</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> to be the set of all <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\lambda \in \overline{L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mover> <mi>L</mi> <mo>¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> for which there exist <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(m,n\in {\mathbb {N}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation> such that <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(f_{\lambda }^m(\alpha _1)=f_{\lambda }^n(\alpha _2)=\beta \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>f</mi> <mrow> <mi>λ</mi> </mrow> <mi>m</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msubsup> <mi>f</mi> <mrow> <mi>λ</mi> </mrow> <mi>n</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>β</mi> </mrow> </math></EquationSource> </InlineEquation>. In other words, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(C(\alpha _1,\alpha _2;\beta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mo stretchy="false">(</mo> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo>;</mo> <mi>β</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> consists of all <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\lambda \in \overline{L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mover> <mi>L</mi> <mo>¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> with the property that the orbit of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\alpha _1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>α</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> collides with the orbit of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\alpha _2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>α</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> under the same polynomial <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(f_{\lambda }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>f</mi> <mi>λ</mi> </msub> </math></EquationSource> </InlineEquation> precisely at the point <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\beta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> </InlineEquation>. Assuming <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\alpha _1,\alpha _2,\beta \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo>,</mo> <mi>β</mi> </mrow> </math></EquationSource> </InlineEquation> are not all contained in a finite subfield of <i>L</i>, we provide explicit necessary and sufficient conditions under which <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(C(\alpha _1,\alpha _2;\beta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mo stretchy="false">(</mo> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo>;</mo> <mi>β</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is infinite. We also discuss the remaining case where <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\alpha _1,\alpha _2,\beta \in \overline{\mathbb {F}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo>,</mo> <mi>β</mi> <mo>∈</mo> <msub> <mover> <mi mathvariant="double-struck">F</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> and provide ample computational data that suggest a somewhat surprising conjecture. Our problem fits into a long series of questions in the area of unlikely intersections in arithmetic dynamics, which have been primarily studied over fields of characteristic 0. Working in characteristic <i>p</i> adds significant difficulties, but also reveals the subtlety of our problem, especially when some of the points lie in a finite field or when <i>d</i> is a power of <i>p</i>.</p>

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Collision of orbits for families of polynomials defined over fields of positive characteristic

  • Shamil Asgarli,
  • Dragos Ghioca

摘要

Let L be a field of positive characteristic p with a fixed algebraic closure \(\overline{L}\) L ¯ , and let \(\alpha _1,\alpha _2,\beta \in L\) α 1 , α 2 , β L . For an integer \(d\ge 2\) d 2 , we consider the family of polynomials \(f_{\lambda }(z):= z^d+\lambda \) f λ ( z ) : = z d + λ , parameterized by \(\lambda \in \overline{L}\) λ L ¯ . Define \(C(\alpha _1,\alpha _2;\beta )\) C ( α 1 , α 2 ; β ) to be the set of all \(\lambda \in \overline{L}\) λ L ¯ for which there exist \(m,n\in {\mathbb {N}}\) m , n N such that \(f_{\lambda }^m(\alpha _1)=f_{\lambda }^n(\alpha _2)=\beta \) f λ m ( α 1 ) = f λ n ( α 2 ) = β . In other words, \(C(\alpha _1,\alpha _2;\beta )\) C ( α 1 , α 2 ; β ) consists of all \(\lambda \in \overline{L}\) λ L ¯ with the property that the orbit of \(\alpha _1\) α 1 collides with the orbit of \(\alpha _2\) α 2 under the same polynomial \(f_{\lambda }\) f λ precisely at the point \(\beta \) β . Assuming \(\alpha _1,\alpha _2,\beta \) α 1 , α 2 , β are not all contained in a finite subfield of L, we provide explicit necessary and sufficient conditions under which \(C(\alpha _1,\alpha _2;\beta )\) C ( α 1 , α 2 ; β ) is infinite. We also discuss the remaining case where \(\alpha _1,\alpha _2,\beta \in \overline{\mathbb {F}}_p\) α 1 , α 2 , β F ¯ p and provide ample computational data that suggest a somewhat surprising conjecture. Our problem fits into a long series of questions in the area of unlikely intersections in arithmetic dynamics, which have been primarily studied over fields of characteristic 0. Working in characteristic p adds significant difficulties, but also reveals the subtlety of our problem, especially when some of the points lie in a finite field or when d is a power of p.