<p>We investigate three-body recombination of helium and hydrogen atoms at cold collision energies, adopting the hyperspherical adiabatic formulation. By taking into account non-rotating (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(J=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>J</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) and rotating (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(J&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>J</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) states, we calculate the rates for the recombination processes <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(^4\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>4</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>He+<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(^4\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>4</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>He+X<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\rightarrow ^4\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mo stretchy="false">→</mo> <mn>4</mn> </msup> </math></EquationSource> </InlineEquation>He<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>+X (X=<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(^1\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>1</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>H, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>2</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>H, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(^3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>3</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>H and <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(^3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>3</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>He), up to 0.1 Kelvin. In addition, we compute the collision induced dissociation rates for the same three-body systems.</p>

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Three-Body Recombination of Cold Helium and Hydrogen Atoms

  • Hiroya Suno

摘要

We investigate three-body recombination of helium and hydrogen atoms at cold collision energies, adopting the hyperspherical adiabatic formulation. By taking into account non-rotating ( \(J=0\) J = 0 ) and rotating ( \(J>0\) J > 0 ) states, we calculate the rates for the recombination processes \(^4\) 4 He+ \(^4\) 4 He+X \(\rightarrow ^4\) 4 He \(_2\) 2 +X (X= \(^1\) 1 H, \(^2\) 2 H, \(^3\) 3 H and \(^3\) 3 He), up to 0.1 Kelvin. In addition, we compute the collision induced dissociation rates for the same three-body systems.