Melih A. Ozcelik

ORCID: 0000-0002-8312-7116
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About
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Research Areas
  • Particle physics theoretical and experimental studies
  • Quantum Chromodynamics and Particle Interactions
  • High-Energy Particle Collisions Research
  • Particle Accelerators and Free-Electron Lasers
  • Quantum, superfluid, helium dynamics
  • Particle Detector Development and Performance
  • Nuclear physics research studies
  • Cold Atom Physics and Bose-Einstein Condensates

Laboratoire de Physique des 2 Infinis Irène Joliot-Curie
2021-2025

Université Paris-Saclay
2022-2024

Centre National de la Recherche Scientifique
2022-2024

Institut National de Physique Nucléaire et de Physique des Particules
2019

Institut de Physique
2019

Abstract We cure the perturbative instability of total-inclusive-photoproduction cross sections vector S -wave quarkonia observed at high photon-proton-collision energies ( $$\sqrt{s_{\gamma p}}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:msub> <mml:mi>s</mml:mi> <mml:mrow> <mml:mi>γ</mml:mi> <mml:mi>p</mml:mi> </mml:mrow> </mml:msub> </mml:msqrt> </mml:math> ) in Next-to-Leading Order (NLO) Collinear-Factorisation (CF) computations. This is achieved using...

10.1140/epjc/s10052-024-12588-x article EN cc-by The European Physical Journal C 2024-04-03

A bstract We compute, in the framework of renormalon calculus, $$ \mathcal{O}\left({\Lambda}_{\textrm{QCD}}\right) <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:msub> <mml:mi>Λ</mml:mi> <mml:mi>QCD</mml:mi> </mml:msub> </mml:mfenced> </mml:math> corrections to production t\overline{t} <mml:mi>t</mml:mi> <mml:mover> <mml:mo>¯</mml:mo> </mml:mover> pairs hadron collisions under assumption that q\overline{q}\to <mml:mi>q</mml:mi>...

10.1007/jhep01(2024)074 article EN cc-by Journal of High Energy Physics 2024-01-15

We revisit inclusive J/psi and Upsilon photoproduction at lepton-hadron colliders, namely in the limit when exchanged photon is quasi real. Our computation includes next-to-leading-order (NLO) alpha_s corrections to leading-order contributions v. Similarly case of NLO charmonium-hadroproduction processes, resulting cross sections obtained MS-bar factorisation scheme are sometimes found be negative. show that scale-fixing criteria which we derived a previous study eta(c) production...

10.1016/j.physletb.2022.137556 article EN cc-by Physics Letters B 2022-11-09

Abstract We address the unphysical energy dependence of quarkonium-hadroproduction cross sections at Next-to-Leading Order (NLO) in $$\alpha _s$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mi>s</mml:mi> </mml:msub> </mml:math> which we attribute to an over-subtraction factorisation collinear singularities inside PDFs $$\overline{\text {MS}}$$ <mml:mover> <mml:mtext>MS</mml:mtext> <mml:mo>¯</mml:mo> </mml:mover> scheme. Such over- or...

10.1140/epjc/s10052-021-09258-7 article EN cc-by The European Physical Journal C 2021-06-01

A bstract We present the analytic expressions for two-loop form factors production or decay of pseudo-scalar quarkonia, in a scheme where quarks are produced at threshold. consider amplitude process $$ \gamma \leftrightarrow {}^1{S}_0^{\left[1\right]} <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>γγ</mml:mi> <mml:mo>↔</mml:mo> <mml:mmultiscripts> <mml:msubsup> <mml:mi>S</mml:mi> <mml:mn>0</mml:mn> <mml:mfenced> <mml:mn>1</mml:mn> </mml:mfenced> </mml:msubsup>...

10.1007/jhep02(2023)250 article EN cc-by Journal of High Energy Physics 2023-02-27

A bstract The energy dependence of the total hadroproduction cross section pseudoscalar quarkonia is computed via matching Next-to-Leading Order (NLO) Collinear-Factorisation (CF) results with resummed higher-order corrections, proportional to $$ {\alpha}_s^n{\ln}^{n-1} <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>α</mml:mi> <mml:mi>s</mml:mi> <mml:mi>n</mml:mi> </mml:msubsup> <mml:msup> <mml:mo>ln</mml:mo> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn>...

10.1007/jhep05(2022)083 article EN cc-by Journal of High Energy Physics 2022-05-13

A bstract We use an abelian model to study linear power corrections which arise from infrared renormalons and affect event shapes in e + − annihilation into hadrons. While previous studies explored the two-jet region, this paper we focus on three-jet is most relevant one for determination of strong coupling constant. show that a broad class shape variables, can be written factorised form, involves analytically-calculable function, characterises changes variable when soft parton emitted,...

10.1007/jhep12(2022)062 article EN cc-by Journal of High Energy Physics 2022-12-12

A bstract We compute the master integrals relevant for two-loop corrections to pseudo-scalar quarkonium and leptonium production decay. present both analytic high-precision numerical results. The expressions are given in terms of multiple polylogarithms (MPLs), elliptic (eMPLs) iterated Eisenstein series. As an application our results, we obtain first time expression amplitude para-positronium decay two photons at loops.

10.1007/jhep09(2022)194 article EN cc-by Journal of High Energy Physics 2022-09-22

We discuss the linear power corrections to electroweak production of top quarks at LHC using renormalon calculus. show how such non-perturbative can be obtained Low-Burnett-Kroll theorem, which provides first subleading term expansion real-emission amplitudes around soft limit. demonstrate that there are no total cross sections arbitrary processes a single type provided these expressed in terms short-distance quark mass. also derive universal formula for generic observables involve top-quark...

10.1007/jhep05(2023)153 article EN cc-by Journal of High Energy Physics 2023-05-18

We explore how the positivity of $P_T$-integrated $\eta_c$-hadroproduction cross-section computed at NLO in $\alpha_s$ can set up constraints on $x$-dependence gluon PDFs low scales.

10.22323/1.352.0159 preprint EN cc-by-nc-nd Proceedings of XXVII International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS2019) 2019-07-24

The energy dependence of the total hadroproduction cross section pseudo-scalar quarkonia is computed via matching Next-to-Leading Order (NLO) Collinear-Factorisation (CF) results with resummed higher-order corrections, proportional to $\alpha_s^{n}\ln^{n-1}(1/z)$, CF hard-scattering coefficient, where $z=M^2/\hat{s}$ $M$ and $\hat{s}$ being quarkonium mass partonic center-of-mass squared. resummation performed using High-Energy Factorisation (HEF) in Doubly-Logarithmic (DL) approximation,...

10.1007/jhep05(2022)083 preprint EN arXiv (Cornell University) 2021-12-13

We consider top quark production and decay in the narrow width approximation study if polarisation effects, that manifest themselves correlations of angular distributions particles from decays final state jets sub-process, are affected by linear power corrections. find that, general, answer to this question is affirmative. also discuss how these non-perturbative corrections affect observables used single at LHC. Finally, we point out generic kinematic leptons corrections, which may have...

10.1007/jhep11(2024)112 article EN cc-by Journal of High Energy Physics 2024-11-19

We discuss the linear power corrections to electroweak production of top quarks at LHC using renormalon calculus. show how such non-perturbative can be obtained Low-Burnett-Kroll theorem, which provides first subleading term expansion real-emission amplitudes around soft limit. demonstrate that there are no total cross sections arbitrary processes a single type provided these expressed in terms short-distance quark mass. also derive universal formula for generic observables involve top-quark...

10.48550/arxiv.2302.02729 preprint EN other-oa arXiv (Cornell University) 2023-01-01

We cure the perturbative instability of total-inclusive-photoproduction cross sections vector $S$-wave quarkonia observed at high photon-proton-collision energies ($\sqrt{s_{\gamma p}}$) in Next-to-Leading Order (NLO) Collinear-Factorisation (CF) computations. This is achieved using High-Energy Factorisation (HEF) Doubly-Logarithmic Approximation (DLA), which a subset Leading-Logarithmic (LLA) HEF resums higher-order QCD corrections proportional to $\alpha_s^n \ln^{n-1} (\hat{s}/M^2)$ Regge...

10.48550/arxiv.2306.02425 preprint EN cc-by arXiv (Cornell University) 2023-01-01

We compute, in the framework of renormalon calculus, ${\cal O}(\Lambda_{\rm QCD})$ corrections to production $t\bar{t}$ pairs hadron collisions under assumption that $q \bar q \to t t$ is dominant partonic channel. This not applicable top quark pair at LHC but it valid for Tevatron where protons and anti-protons were studied. show linear power correction total $t cross section vanishes provided one uses a short-distance scheme mass. also derive relatively simple formulas kinematic...

10.48550/arxiv.2308.05526 preprint EN other-oa arXiv (Cornell University) 2023-01-01

We explore how the positivity of P_T-integrated eta_c-hadroproduction cross-section computed at NLO in alpha_s can set up constraints on x-dependence gluon PDFs low scales.

10.48550/arxiv.1907.01400 preprint EN other-oa arXiv (Cornell University) 2019-01-01

We use an abelian model to study linear power corrections which arise from infrared renormalons and affect event shapes in $e^+e^-$ annihilation into hadrons. While previous studies explored the two-jet region, this paper we focus on three-jet is most relevant one for determination of strong coupling constant. show that a broad class shape variables, can be written factorised form, involves analytically-calculable function, characterises changes variable when soft parton emitted, constant...

10.48550/arxiv.2204.02247 preprint EN other-oa arXiv (Cornell University) 2022-01-01

We present the analytic expressions for two-loop form factors production or decay of pseudo-scalar quarkonia, in a scheme where quarks are produced at threshold. consider amplitude process $γγ\leftrightarrow {^1S_0^{[1]}}$, that was previously known only numerically, as well processes $gg \leftrightarrow $γg {^1S_0^{[8]}}$ and {^1S_0^{[8]}}$, which have not been computed before. The corrections to {^1S_0^{[1]}}$ last missing ingredients full NNLO calculation $η_Q$ hadro-production. discuss...

10.48550/arxiv.2211.08838 preprint EN other-oa arXiv (Cornell University) 2022-01-01

We revisit inclusive J/psi and Upsilon photoproduction at lepton-hadron colliders, namely in the limit when exchanged photon is quasi real. Our computation includes next-to-leading-order (NLO) alpha_s corrections to leading-order contributions v. Similarly case of NLO charmonium-hadroproduction processes, resulting cross sections obtained MS-bar factorisation scheme are sometimes found be negative. show that scale-fixing criteria which we derived a previous study eta(c) production...

10.48550/arxiv.2112.05060 preprint EN other-oa arXiv (Cornell University) 2021-01-01
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