<p>We present the first complete next-to-leading-order calculation of the impact factors for hadroproduction of the <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math display="inline"> <mmultiscripts> <msubsup> <mi>S</mi> <mn>0</mn> <mfenced close="]" open="["> <mn>1</mn> </mfenced> </msubsup> <mprescripts /> <none /> <mn>1</mn> </mmultiscripts> </math></EquationSource> <EquationSource Format="TEX">\( {}^1{S}_0^{\left[1\right]} \)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math display="inline"> <mmultiscripts> <msubsup> <mi>S</mi> <mn>0</mn> <mfenced close="]" open="["> <mn>8</mn> </mfenced> </msubsup> <mprescripts /> <none /> <mn>1</mn> </mmultiscripts> </math></EquationSource> <EquationSource Format="TEX">\( {}^1{S}_0^{\left[8\right]} \)</EquationSource> </InlineEquation>, and <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math display="inline"> <mmultiscripts> <msubsup> <mi>S</mi> <mn>1</mn> <mfenced close="]" open="["> <mn>8</mn> </mfenced> </msubsup> <mprescripts /> <none /> <mn>3</mn> </mmultiscripts> </math></EquationSource> <EquationSource Format="TEX">\( {}^3{S}_1^{\left[8\right]} \)</EquationSource> </InlineEquation> NRQCD states within the BFKL formalism. We complete the recent virtual-correction computation presented in JHEP 12 (2024) 129 by that of the real-emission contributions. We observe the cancellation of the soft divergences between these real- and virtual-emission contributions and we note that the surviving collinear singularities are compatible with factorisation up to one loop for a novel class of processes where BFKL resummation can be applied. Our work indeed represents the first complete NLO quarkonium impact factor in the BFKL framework and paves the way to first next-to-leading-logarithmic-precision studies for hadroproduction of forward-backward quarkonium associated production at hadron colliders.</p>

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Complete NLO BFKL impact factors for quarkonium hadroproduction in NRQCD: the case of \( ^1{S}_0^{\left[1\right]} \), \( ^1{S}_0^{\left[8\right]} \), and \( ^3{S}_1^{\left[8\right]} \) states

  • Michael Fucilla,
  • Jean-Philippe Lansberg,
  • Maxim Nefedov,
  • Lech Szymanowski,
  • Samuel Wallon

摘要

We present the first complete next-to-leading-order calculation of the impact factors for hadroproduction of the S 0 1 1 \( {}^1{S}_0^{\left[1\right]} \) , S 0 8 1 \( {}^1{S}_0^{\left[8\right]} \) , and S 1 8 3 \( {}^3{S}_1^{\left[8\right]} \) NRQCD states within the BFKL formalism. We complete the recent virtual-correction computation presented in JHEP 12 (2024) 129 by that of the real-emission contributions. We observe the cancellation of the soft divergences between these real- and virtual-emission contributions and we note that the surviving collinear singularities are compatible with factorisation up to one loop for a novel class of processes where BFKL resummation can be applied. Our work indeed represents the first complete NLO quarkonium impact factor in the BFKL framework and paves the way to first next-to-leading-logarithmic-precision studies for hadroproduction of forward-backward quarkonium associated production at hadron colliders.