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73 results on '"Miguel G. Echevarria"'

1. Factorization for J/ψ leptoproduction at small transverse momentum

Author

Miguel G. Echevarria, Samuel F. Romera, and Pieter Taels

Subjects
Factorization, Renormalization Group, Parton Distributions, Quarkonium, Effective Field Theories of QCD, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract Nonrelativistic Quantum Chromodynamics (NRQCD) breaks down in the region of low transverse momentum, where the transverse momentum of the produced quarkonium state is sensitive to multiple scattering with the incoming hadron and to soft gluon radiation. In this kinematic regime, the transverse-momentum-dependent (TMD) factorization framework is required, promoting the long-distance matrix elements (LDMEs) of NRQCD to the so-called TMD shape functions (TMDShFs), which encode both the soft gluon radiation and the formation of the heavy-quark bound state. In this work, we apply an effective-field theory approach (combining NRQCD and SCET) to the photon-gluon fusion process in inclusive J/ψ leptoproduction. We derive a factorization theorem for the cross section in terms of TMDShFs, compute these quantities at next-to-leading order, establish their evolution, and study their matching onto the corresponding LDMEs in the high-transverse-momentum region. Our results are particularly relevant to the Electron-Ion Collider, where J/ψ leptoproduction can be used to probe gluon transverse-momentum-dependent parton distribution functions (gluon TMDPDFs).

Published
2024
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2. Gluon TMD fragmentation function into quarkonium

Author

Miguel G. Echevarria, Samuel F. Romera, and Ignazio Scimemi

Subjects
Effective Field Theories of QCD, Higher-Order Perturbative Calculations, Quarkonium, Factorization, Renormalization Group, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We compute the gluon transverse-momentum-dependent fragmentation function (TMDFF) at next-to-leading order (NLO) into heavy quarkonium in the color-octet S 1 8 3 $$ {}^3{S}_1^{\left[8\right]} $$ channel, based on the NRQCD factorization approach. The spurious rapidity divergences are explicitly shown to cancel in a well-defined TMDFF, which incorporates the needed soft factor. We also compute the integrated gluon FF at NLO in the same S 1 8 3 $$ {}^3{S}_1^{\left[8\right]} $$ channel, and show that the matching coefficient of the TMDFF onto the FF at large transverse momentum is the expected one. These results are relevant to perform precise and sensible phenomenological studies of transverse-momentum spectra of quarkonium production, for which the production mechanism through fragmentation plays a relevant role, like in the future Electron-Ion Collider.

Published
2023
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3. GTMDs and the factorization of exclusive double Drell-Yan

Author

Miguel G. Echevarria, Patricia A. Gutierrez Garcia, and Ignazio Scimemi

Subjects
QCD, Factorization, Drell-Yan, Generalized transverse momentum dependent distributions (GTMDs), Light cone wave functions (LCWFs), Physics, QC1-999
Abstract

Different exclusive processes have been proposed to access the generalized transverse momentum dependent distributions (GTMDs) with no proof of factorization, which allows to rigorously define the GTMDs. Using Soft Collinear Effective Theory we derive for the first time the factorization of the differential cross section for the exclusive double Drell-Yan process πN→N′γ⁎γ⁎→N′(ℓ+ℓ−)(ℓ+ℓ−), for small transverse momenta of the photons in terms of a perturbatively calculable hard factor, GTMDs and light-cone wave functions (LCWFs). We find that the hard factor of the process can be obtained from single inclusive Drell-Yan production so that one can resum logarithms at high orders in QCD. We also discuss the evolution of the GTMDs and the LCWFs.

Published
2023
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4. Transverse momentum dependent distributions in dijet and heavy hadron pair production at EIC

Author

Rafael F. del Castillo, Miguel G. Echevarria, Yiannis Makris, and Ignazio Scimemi

Subjects
Jets, QCD Phenomenology, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We discuss the measurement of gluon transverse momentum distribution (TMD) in dijet and heavy hadron pair (HHP) production in semi-inclusive deep inelastic scattering. The factorization of these processes in position space shows the appearance of a specific new soft factor matrix element on top of angular and complex valued anomalous dimensions. We show in detail how these features can be treated consistently and we discuss a scale prescription for the evolution kernel of the dijet soft function. As a result we obtain phenomenological predictions for unpolarized and angular modulated cross-sections for the electron-ion collider (EIC) using current available information on unpolarized TMD.

Published
2022
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5. TMD factorization for dijet and heavy-meson pair in DIS

Author

Rafael F. del Castillo, Miguel G. Echevarria, Yiannis Makris, and Ignazio Scimemi

Subjects
Jets, QCD Phenomenology, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We study a transverse momentum dependent (TMD) factorization framework for the processes of dijet and heavy-meson pair production in deep-inelastic-scattering in an electron-proton collider, considering the measurement of the transverse momentum imbalance of the two hard probes in the Breit frame. For the factorization theorem we employ soft-collinear and boosted-heavy-quark effective field theories. The factorized cross-section for both processes is sensitive to gluon unpolarized and linearly polarized TMD distributions and requires the introduction of a new soft function. We calculate the new soft function here at one-loop, regulating rapidity divergences with the δ-regulator. In addition, using a factorization consistency relation and a universality argument regarding the heavy-quark jet function, we obtain the anomalous dimension of the new soft function at two and three loops.

Published
2021
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6. Global analysis of the Sivers functions at NLO+NNLL in QCD

Author

Miguel G. Echevarria, Zhong-Bo Kang, and John Terry

Subjects
QCD Phenomenology, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We perform global fit to the quark Sivers function within the transverse momentum dependent (TMD) factorization formalism in QCD. We simultaneously fit Sivers asymmetry data from Semi-Inclusive Deep Inelastic Scattering (SIDIS) at COMPASS, HERMES, and JLab, from Drell-Yan lepton pair production at COMPASS, and from W/Z boson at RHIC. This extraction is performed at next-to-leading order (NLO) and next-to-next-to leading logarithmic (NNLL) accuracy. We find excellent agreement between our extracted asymmetry and the experimental data for SIDIS and Drell-Yan lepton pair production, while tension arises when trying to describe the spin asymmetries of W/Z bosons at RHIC. We carefully assess the situation, and we study in details the impact of the RHIC data and their implications through different ways of performing the fit. In addition, we find that the quality of the description of W/Z vector boson asymmetry data could be strongly sensitive to the DGLAP evolution of Qiu-Sterman function, besides the usual TMD evolution. We present discussion on this and the implications for measurements of the transverse-spin asymmetries at the future Electron Ion Collider.

Published
2021
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7. Quarkonium TMD fragmentation functions in NRQCD

Author

Miguel G. Echevarria, Yiannis Makris, and Ignazio Scimemi

Subjects
Deep Inelastic Scattering (Phenomenology), QCD Phenomenology, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We study the transverse-momentum spectrum of quarkonium production from single light-parton fragmentation mechanism. In the case of semi-inclusive deep inelastic scattering, we observe that there are two possible initiating processes, namely photon-gluon fusion and light-quark fragmentation. For the second case we derive the factorization theorem, which involves a new hadronic quantity: the quarkonium transverse-momentum-dependent fragmentation functions in NRQCD. We calculate their matching onto the non-perturbative long distance matrix elements at the lowest order in the strong-coupling constant, O α s 2 $$ \mathcal{O}\left({\alpha}_s^2\right) $$ . Focusing on the case of the electron-ion collider, we make a comparative phenomenological study of the two production mechanisms and find the regions of the phase space where one is dominant over the other.

Published
2020
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8. Studies of gluon TMDs and their evolution using quarkonium-pair production at the LHC

Author

Florent Scarpa, Daniël Boer, Miguel G. Echevarria, Jean-Philippe Lansberg, Cristian Pisano, and Marc Schlegel

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract $$J/\psi $$ J/ψ - or $$\Upsilon $$ Υ -pair production at the LHC are promising processes to study the gluon transverse momentum distributions (TMDs) which remain very poorly known. In this article, we improve on previous results by including the TMD evolution in the computation of the observables such as the pair-transverse-momentum spectrum and asymmetries arising from the linear polarization of gluons inside unpolarized protons. We show that the azimuthal asymmetries generated by the gluon polarization are reduced compared to the tree level case but are still of measurable size (in the 5–10% range). Such asymmetries should be measurable in the available data sets of $$J/\psi $$ J/ψ pairs and in the future data sets of the high-luminosity LHC for $$\Upsilon $$ Υ pairs.

Published
2020
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9. Proper TMD factorization for quarkonia production: pp → η c, b as a study case

Author

Miguel G. Echevarria

Subjects
Effective Field Theories, Perturbative QCD, Renormalization Group, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract Quarkonia production in different high-energy processes has recently been proposed in order to probe gluon transverse-momentum-dependent parton distribution and fragmentation functions (TMDs in general). However, no proper factorization theorems have been derived for the discussed processes, but rather just ansatzs, whose main assumption is the factorization of the two soft mechanisms present in the process: soft-gluon radiation and the formation of the bound state. In this paper it is pointed out that, at low transverse momentum, these mechanisms are entangled and thus encoded in a new kind of non-perturbative hadronic quantities beyond the TMDs: the TMD shape functions. This is illustrated by deriving the factorization theorem for the process pp → η c, b at low transverse momentum.

Published
2019
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10. QCD×QED evolution of TMDs

Author

Alessandro Bacchetta and Miguel G. Echevarria

Subjects
Physics, QC1-999
Abstract

We consider for the first time the QED corrections to the evolution of (un)polarized quark and gluon transverse-momentum-dependent distribution and fragmentation functions (TMDs in general). By extending their operator definition to QCD×QED, we provide the mixed new anomalous dimensions up to O(αsα) and the pure QED ones up to O(α2). These new corrections are universal for all TMDs up to the flavor of the considered parton, i.e., the full flavor universality of TMD evolution found in pure QCD is broken in QCD×QED by the presence of the electric charge. In addition, we provide the leading-order QED corrections to the matching coefficients of the unpolarized quark TMD parton distribution function onto its integrated counterparts at O(αs0α).

Published
2019
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11. Matching factorization theorems with an inverse-error weighting

Author

Miguel G. Echevarria, Tomas Kasemets, Jean-Philippe Lansberg, Cristian Pisano, and Andrea Signori

Subjects
Physics, QC1-999
Abstract

We propose a new fast method to match factorization theorems applicable in different kinematical regions, such as the transverse-momentum-dependent and the collinear factorization theorems in Quantum Chromodynamics. At variance with well-known approaches relying on their simple addition and subsequent subtraction of double-counted contributions, ours simply builds on their weighting using the theory uncertainties deduced from the factorization theorems themselves. This allows us to estimate the unknown complete matched cross section from an inverse-error-weighted average. The method is simple and provides an evaluation of the theoretical uncertainty of the matched cross section associated with the uncertainties from the power corrections to the factorization theorems (additional uncertainties, such as the nonperturbative ones, should be added for a proper comparison with experimental data). Its usage is illustrated with several basic examples, such as Z boson, W boson, H0 boson and Drell–Yan lepton-pair production in hadronic collisions, and compared to the state-of-the-art Collins–Soper–Sterman subtraction scheme. It is also not limited to the transverse-momentum spectrum, and can straightforwardly be extended to match any (un)polarized cross section differential in other variables, including multi-differential measurements.

Published
2018
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13. Azimuthal asymmetries in unpolarized SIDIS and Drell-Yan processes: A case study towards TMD factorization at subleading twist

Author

Alessandro Bacchetta, Giuseppe Bozzi, Miguel G. Echevarria, Cristian Pisano, Alexei Prokudin, and Marco Radici

Subjects
Physics, QC1-999
Abstract

We consider the azimuthal distribution of the final observed hadron in semi-inclusive deep-inelastic scattering and the lepton pair in the Drell-Yan process. In particular, we focus on the cos⁡ϕ modulation of the unpolarized cross section and on its dependence upon transverse momentum. At low transverse momentum, for these observables we propose a factorized expression based on tree-level approach and conjecture that the same formula is valid in transverse-momentum dependent (TMD) factorization when written in terms of subtracted TMD parton distributions. Our formula correctly matches with the collinear factorization results at high transverse momentum, solves a long-standing problem and is a necessary step towards the extension of the TMD factorization theorems up to the subleading twist.

Published
2019
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14. Proper definition and evolution of generalized transverse momentum dependent distributions

Author

Miguel G. Echevarria, Ahmad Idilbi, Koichi Kanazawa, Cédric Lorcé, Andreas Metz, Barbara Pasquini, and Marc Schlegel

Subjects
Physics, QC1-999
Abstract

We consider one of the most fundamental sets of hadronic matrix elements, namely the generalized transverse momentum dependent distributions (GTMDs), and argue that their existing definitions lack proper evolution properties. By exploiting the similarity of GTMDs with the much better understood transverse momentum distributions, we argue that the existing definitions of GTMDs have to include an additional dependence on soft gluon radiation in order to render them properly defined. With this, we manage to obtain the evolution kernel of all (un)polarized quark and gluon GTMDs, which turns out to be spin independent. As a byproduct, all large logarithms can be resummed up to next-to-next-to-leading-logarithmic accuracy with the currently known perturbative ingredients.

Published
2016
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16. Illuminating the nucleon spin

Author

Miguel G. Echevarria

Subjects
High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), High Energy Physics::Lattice, Nuclear Theory, High Energy Physics::Phenomenology, FOS: Physical sciences, High Energy Physics::Experiment
Abstract

In this short note the QED extension of the nucleon spin sum rule is considered. To this end, the leading-order (LO) QED evolution kernels for the quark/gluon helicity and orbital-angular-momentum (OAM) distributions are calculated, as well as their lepton and photon analogue distributions introduced for the first time. The LO evolution kernels of the latter are also calculated, both in QCD and QED. Putting all together, the nucleon spin sum rule remains scale-invariant in QCD$\times$QED, as expected, which represents a check of the newly obtained results. This theoretical development will allow in the future the quantification of the contributions of lepton and photon distributions to the nucleon spin, and a more precise control over the uncertainties., Comment: v1: 6 pages

Published
2022
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17. Quarkonium TMD fragmentation functions in NRQCD

Author

Yiannis Makris, Miguel G. Echevarria, and Ignazio Scimemi

Subjects
Computer Science::Machine Learning, Nuclear and High Energy Physics, Particle physics, Física-Modelos matemáticos, Hadron, FOS: Physical sciences, Computer Science::Digital Libraries, 01 natural sciences, Statistics::Machine Learning, symbols.namesake, High Energy Physics - Phenomenology (hep-ph), Fragmentation (mass spectrometry), 0103 physical sciences, Física matemática, lcsh:Nuclear and particle physics. Atomic energy. Radioactivity, 010306 general physics, Nuclear Experiment, Deep Inelastic Scattering (Phenomenology), Physics, 010308 nuclear & particles physics, High Energy Physics::Phenomenology, Deep inelastic scattering, Quarkonium, QCD Phenomenology, High Energy Physics - Phenomenology, Distance matrix, Phase space, Weierstrass factorization theorem, Computer Science::Mathematical Software, symbols, lcsh:QC770-798, High Energy Physics::Experiment
Abstract

We study the transverse-momentum spectrum of quarkonium production from single light-parton fragmentation mechanism. In the case of semi-inclusive deep inelastic scattering, we observe that there are two possible initiating processes, namely photon-gluon fusion and light-quark fragmentation. For the second case we derive the factorization theorem, which involves a new hadronic quantity: the quarkonium transverse-momentum-dependent fragmentation functions in NRQCD. We calculate their matching onto the non-perturbative long distance matrix elements at the lowest order in the strong-coupling constant (${\mathcal O}(\alpha_s^2)$). Focusing on the case of the electron-ion collider, we make a comparative phenomenological study of the two production mechanisms and find the regions of the phase space where one is dominant over the other., Comment: v1: 21 pages, 5 figures. v2: matches version published in JHEP

Published
2020
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19. Prospects for quarkonium studies at the high-luminosity LHC

Author

Melih Arslan Ozcelik, Carlo Flore, Oleg Teryaev, Shohini Bhattacharya, L. Massacrier, Tomas Kasemets, Chris A. Flett, David D'Enterria, Cyrille Marquet, Riccardo Nagar, V. Kartvelishvili, Maxim Nefedov, Miguel G. Echevarria, R. McNulty, Charlotte Van Hulse, Luca Micheletti, Nodoka Yamanaka, Francesco Giovanni Celiberto, Pol Bernard Gossiaux, Hua-Sheng Shao, Thomas Mehen, M. Winn, Bertrand Ducloué, Amy Selvi Tee, Maria Vittoria Garzelli, Cvetan Valeriev Cheshkov, Yiannis Makris, Pieter Taels, Xiaojun Yao, Denys Yen Arrebato Villar, Matteo Rinaldi, Liupan An, Jibo He, Jonathan R. Gaunt, Cédric Mezrag, Darren Price, Florent Scarpa, Emilien Chapon, Kazuhiro Watanabe, Umberto D'Alesio, Jian-Wei Qiu, Yanxi Zhang, Ivan Vitev, Cesar Luiz Da Silva, Sangem Rajesh, Jean-Philippe Lansberg, Jaroslav Adam, Cristian Pisano, Biswarup Paul, E. G. Ferreiro, Maddie Smith, Laboratoire de physique subatomique et des technologies associées (SUBATECH), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-IMT Atlantique (IMT Atlantique), Institut Mines-Télécom [Paris] (IMT)-Institut Mines-Télécom [Paris] (IMT)-Nantes université - UFR des Sciences et des Techniques (Nantes univ - UFR ST), Nantes Université - pôle Sciences et technologie, Nantes Université (Nantes Univ)-Nantes Université (Nantes Univ)-Nantes Université - pôle Sciences et technologie, Nantes Université (Nantes Univ)-Nantes Université (Nantes Univ), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), ANR-20-CE31-0015,PrecisOnium,Promouvoir la précision des études de la production de quarkonia(2020), Université de Nantes - UFR des Sciences et des Techniques (UN UFR ST), Université de Nantes (UN)-Université de Nantes (UN)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-IMT Atlantique Bretagne-Pays de la Loire (IMT Atlantique), Institut Mines-Télécom [Paris] (IMT)-Institut Mines-Télécom [Paris] (IMT), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)

Subjects
J/psi(3100), heavy ion: scattering, generalized parton distribution, Nuclear Theory, Proton, nucleus nucleus, parton: distribution function, Parton, eta/c(3590), nucl-ex, transverse momentum dependence, Large Hadron Collider (LHC), 7. Clean energy, 01 natural sciences, High Energy Physics - Experiment, law.invention, Sivers function, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), law, High Luminosity, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], parton, Nuclear Experiment (nucl-ex), Quarkonium production, Nuclear Experiment, quark gluon: plasma, Physics, Large Hadron Collider, Luminosity (scattering theory), hep-ph, high, nucleus nucleus: scattering, Quarkonium, heavy ion, High Energy Physics - Phenomenology, CERN LHC Coll, Nuclear Physics - Theory, luminosity: high, eta/c(2980), Particle Physics - Experiment, quarkonium, Nuclear and High Energy Physics, Particle physics, p p: scattering, small-x, CERN Lab, nucl-th, [PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th], collective, FOS: Physical sciences, transverse momentum, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], Nuclear Theory (nucl-th), 0103 physical sciences, Nuclear Physics - Experiment, luminosity, 010306 general physics, Collider, p nucleus: scattering, quark gluon, plasma, Particle Physics - Phenomenology, 010308 nuclear & particles physics, hep-ex, High Energy Physics::Phenomenology, scattering, nucleus, gluon, Gluon, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], Quark–gluon plasma, High Energy Physics::Experiment, p nucleus, production
Abstract

Prospects for quarkonium-production studies accessible during the upcoming high-luminosity phases of the CERN Large Hadron Collider operation after 2021 are reviewed. Current experimental and theoretical open issues in the field are assessed together with the potential for future studies in quarkonium-related physics. This will be possible through the exploitation of the huge data samples to be collected in proton-proton, proton-nucleus and nucleus-nucleus collisions, both in the collider and fixed-target modes. Such investigations include, among others, those of: (i) J/psi and Upsilon produced in association with other hard particles; (ii) chi(c,b) and eta(c,b) down to small transverse momenta; (iii) the constraints brought in by quarkonia on gluon PDFs, nuclear PDFs, TMDs, GPDs and GTMDs, as well as on the low-x parton dynamics; (iv) the gluon Sivers effect in polarised-nucleon collisions; (v) the properties of the quark-gluon plasma produced in ultra-relativistic heavy-ion collisions and of collective partonic effects in general; and (vi) double and triple parton scatterings., Comment: Latex, 115 pages, 55 figures, 4 tables. v2: Review published in Progress in Particle and Nuclear Physics

Published
2022
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20. Heavy-flavour studies with a high-luminosity fixed-target experiment at the LHC

Author

C. Hadjidakis, J.P. Lansberg, Sarah Julie Porteboeuf, E. G. Ferreiro, Anthony Klein, Barbara Antonina Trzeciak, R. Haque, Aleksander Kusina, G. Cavoto, C. Quintans, A. Rakotozafindrabe, Patrick Robbe, Jakub Wagner, Zishuo Yang, W. Scandale, N.S. Topilskaya, C. VanHulse, Y. I. Makdisi, I. Schienbein, Alexey Kurepin, Laure Marie Massacrier, Miguel G. Echevarria, Nodoka Yamanaka, A. Zelenski, D. P. Kikola, J. Seixas, Florian Lyonnet, Stanley J. Brodsky, Hua-Sheng Shao, Ivana Hrivnacova, C. DaSilva, Antonio Uras, Cédric Lorcé, Andrea Signori, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Département de Physique Nucléaire (ex SPhN) (DPHN), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire de Lyon (IPNL), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne [2017-2020] (UCA [2017-2020])-Centre National de la Recherche Scientifique (CNRS), Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)

Subjects
p p: scattering, Particle physics, Physics::Instrumentation and Detectors, FOS: Physical sciences, quarkonium: production, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], nucl-ex, heavy quark: production, lead: beam, Nuclear Physics - Experiment, Rapidity, Nuclear Experiment (nucl-ex), Nuclear Experiment, p nucleus: scattering, quark gluon: plasma, Brookhaven RHIC Coll, Physics, Luminosity (scattering theory), Large Hadron Collider, nucleus: target, Quarkonium, Projection (relational algebra), CERN LHC Coll, gas: target, 13. Climate action, Quark–gluon plasma, Production (computer science), High Energy Physics::Experiment, Energy (signal processing)
Abstract

Extraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. pp, pd and pA collisions at $\sqrt{s}$ = 115 GeV and Pbp and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy. In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented., Hard Probes 2020 proceedings

Published
2021
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21. Global analysis of the Sivers functions at NLO+NNLL in QCD

Author

Zhong-Bo Kang, John Terry, and Miguel G. Echevarria

Subjects
Quark, Nuclear and High Energy Physics, Particle physics, Nuclear Theory, FOS: Physical sciences, 01 natural sciences, Vector boson, High Energy Physics - Experiment, Nuclear Theory (nucl-th), High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), 0103 physical sciences, lcsh:Nuclear and particle physics. Atomic energy. Radioactivity, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, Boson, Quantum chromodynamics, Physics, 010308 nuclear & particles physics, High Energy Physics::Phenomenology, Deep inelastic scattering, QCD Phenomenology, High Energy Physics - Phenomenology, Pair production, DGLAP, lcsh:QC770-798, High Energy Physics::Experiment, Lepton
Abstract

We perform global fit to the quark Sivers function within the transverse momentum dependent (TMD) factorization formalism in QCD. We simultaneously fit Sivers asymmetry data from Semi-Inclusive Deep Inelastic Scattering (SIDIS) at COMPASS, HERMES, and JLab, from Drell-Yan lepton pair production at COMPASS, and from $W/Z$ boson at RHIC. This extraction is performed at next-to-leading order (NLO) and next-to-next-to leading logarithmic (NNLL) accuracy. We find excellent agreement between our extracted asymmetry and the experimental data for SIDIS and Drell-Yan lepton pair production, while tension arises when trying to describe the spin asymmetries of $W/Z$ bosons at RHIC. We carefully assess the situation, and we study in details the impact of the RHIC data and their implications through different ways of performing the fit. In addition, we find that the quality of the description of $W/Z$ vector boson asymmetry data could be strongly sensitive to the DGLAP evolution of Qiu-Sterman function, besides the usual TMD evolution. We present discussion on this and the implications for measurements of the transverse-spin asymmetries at the future Electron Ion Collider., 48 pages, 21 figures

Published
2021

22. On the physics potential to study the gluon content of proton and deuteron at NICA SPD

Author

Maxim Nefedov, Vladimir Saleev, Marco Radici, A. Guskov, Jean-Philippe Lansberg, Alessandro Bacchetta, Miguel G. Echevarria, A. Rymbekova, K. F. Liu, Andrej Arbuzov, Oleg Teryaev, A. Karpishkov, Bernd A. Kniehl, Umberto D'Alesio, B. Parsamyan, Francesco Murgia, S. Kumano, M. Deka, N.Ya. Ivanov, A.V. Efremov, Francesco Giovanni Celiberto, Cristian Pisano, M. Butenschoen, A. Shipilova, Ya. Klopot, Qin-Tao Song, I. Denisenko, Aram Kotzinian, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), and Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)

Subjects
Proton, Nuclear Theory, gluon: helicity, 01 natural sciences, High Energy Physics - Experiment, law.invention, Sivers function, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), law, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Nuclear Experiment, transversity, Quantum chromodynamics, Physics, photon: production, Luminosity (scattering theory), Proton and deuteron spin structure, Helicity, 3. Good health, photon: direct production, High Energy Physics - Phenomenology, proposed experiment, Nucleon, spin: asymmetry, charmonium: production, Nuclear and High Energy Physics, Particle physics, p: polarized beam, polarization: longitudinal, FOS: Physical sciences, NICA, 0103 physical sciences, polarization: transverse, 010306 general physics, Spin (physics), Collider, deuteron: polarized beam, Dubna Lab, Polarized hadron collisions, 010308 nuclear & particles physics, nucleus, Spin asymmetries, nucleon: structure function, QCD, Gluon, TMD factorization, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], Gluon TMD PDFs, Physics::Accelerator Physics, High Energy Physics::Experiment, charm, experimental results
Abstract

The Spin Physics Detector (SPD) is a future multipurpose experiment foreseen to run at the NICA collider, which is currently under construction at the Joint Institute for Nuclear Research (JINR, Dubna, Russia). The physics program of the experiment is based on collisions of longitudinally and transversely polarized protons and deuterons at $\sqrt{s}$ up to 27 GeV and luminosity up to 10$^{32}$ cm$^{-2}$ s$^{-1}$. The SPD will operate as a universal facility for comprehensive study of unpolarized and polarized gluon content of the nucleon, using different complementary probes such as: charmonia, open charm, and prompt photon production processes. The aim of this work is to make a thorough review of the physics objectives that can potentially be addressed at the SPD, underlining related theoretical aspects and discussing relevant experimental results when available. Among different pertinent phenomena particular attention is drawn to the study of the gluon helicity, gluon Sivers and Boer-Mulders functions in the nucleon, as well as the gluon transversity distribution in the deuteron, via the measurement of specific single and double spin asymmetries., Comment: arXiv admin note: text overlap with arXiv:2102.00442

Published
2021
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23. Quantum Simulation of Light-Front Parton Correlators

Author

Enrique Rico, Miguel G. Echevarria, G. Schnell, and Iñigo L. Egusquiza

Subjects
Physics, High Energy Physics - Theory, Quantum Physics, Wilson loop, Condensed Matter - Mesoscale and Nanoscale Physics, High Energy Physics - Lattice (hep-lat), Hadron, FOS: Physical sciences, Quantum simulator, Parton, Quantum technology, symbols.namesake, Theoretical physics, High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), Quantum gate, High Energy Physics - Lattice, High Energy Physics - Theory (hep-th), Mesoscale and Nanoscale Physics (cond-mat.mes-hall), Weierstrass factorization theorem, symbols, Quantum algorithm, Quantum Physics (quant-ph)
Abstract

The physics of high-energy colliders relies on the knowledge of different non-perturbative parton correlators, such as parton distribution functions, that encode the information on universal hadron structure and are thus the main building blocks of any factorization theorem of the underlying process in such collision. These functions are given in terms of gauge-invariant light-front operators, they are non-local in both space and real time, and are thus intractable by standard lattice techniques due to the well-known sign problem. In this paper, we propose a quantum algorithm to perform a quantum simulation of these type of correlators, and illustrate it by considering a space-time Wilson loop. We discuss the implementation of the quantum algorithm in terms of quantum gates that are accessible within actual quantum technologies such as cold atoms setups, trapped ions or superconducting circuits., v2: minor changes, motivation improved, new figure added, accepted for publication in PRD; 13 pages, 5 figures. v1: 12 pages, 4 figures

Published
2020

24. Studies of gluon TMDs and their evolution using quarkonium-pair production at the LHC

Author

Daniël Boer, Miguel G. Echevarria, Cristian Pisano, Florent Scarpa, Jean-Philippe Lansberg, Marc Schlegel, Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Van Swinderen Institute for Particle Physics and G, and High-Energy Frontier

Subjects
Physics and Astronomy (miscellaneous), 01 natural sciences, High Energy Physics - Experiment, transverse momentum: momentum spectrum, COLLIDER, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), gluon: transverse momentum, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Nuclear Experiment, Physics, Large Hadron Collider, Linear polarization, Observable, Quarkonium, Polarization (waves), J-PSI, 3. Good health, High Energy Physics - Phenomenology, CERN LHC Coll, FACTORIZATION, HADRONIC PRODUCTION, Particle physics, COLLISIONS, angular distribution: asymmetry, Computation, FOS: Physical sciences, lcsh:Astrophysics, UPSILON, gluon: polarization, FIXED-TARGET EXPERIMENT, DOUBLE PARTON SCATTERINGS, lcsh:QB460-466, 0103 physical sciences, tree approximation, J/psi(3100): pair production, lcsh:Nuclear and particle physics. Atomic energy. Radioactivity, 010306 general physics, Engineering (miscellaneous), polarization: linear, 010308 nuclear & particles physics, High Energy Physics::Phenomenology, TRANSVERSE-MOMENTUM, Upsilon(9460): pair production, gluon: density, Gluon, J/PSI, Pair production, evolution equation, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], transverse momentum: factorization, lcsh:QC770-798, High Energy Physics::Experiment
Abstract

$J/\psi$- or $\Upsilon$-pair production at the LHC are promising processes to study the gluon transverse momentum distributions (TMDs) which remain very poorly known. In this article, we improve on previous results by including the TMD evolution in the computation of the observables such as the pair-transverse-momentum spectrum and asymmetries arising from the linear polarization of gluons inside unpolarized protons. We show that the azimuthal asymmetries generated by the gluon polarization are reduced compared to the tree level case but are still of measurable size (in the 5%-10% range). Such asymmetries should be measurable in the available data sets of $J/\psi$ pairs and in the future data sets of the high-luminosity LHC for $\Upsilon$ pairs., Comment: 16 pages, 6 figures

Published
2020
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25. Erratum to: QCD evolution of (un)polarized gluon TMDPDFs and the Higgs q T -distribution

Author

Cristian Pisano, Piet J. Mulders, Tomas Kasemets, and Miguel G. Echevarria

Subjects
Physics, Quantum chromodynamics, Nuclear and High Energy Physics, Particle physics, 010308 nuclear & particles physics, High Energy Physics::Lattice, High Energy Physics::Phenomenology, T distribution, Gauge (firearms), 01 natural sciences, Helicity, Physics::Geophysics, Gluon, 0103 physical sciences, Higgs boson, lcsh:QC770-798, High Energy Physics::Experiment, lcsh:Nuclear and particle physics. Atomic energy. Radioactivity, Invariant (mathematics), 010306 general physics, Gluon field
Abstract

The definition of the gauge invariant gluon field in eq. (2.4) in [1] should be divided by (Formula presented.) ∙ P: (Formula presented.) The matching coefficients of the gluon helicity in eq. (5.3) in [1] have been corrected, and they should read: (Formula presented.) Accordingly, figures 1 and 2 in the manuscript [1] should be replaced by figures 1 and 2 in this erratum.

Published
2017
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26. Studying the gluon TMDs with $J/\psi$- and $\Upsilon$-pair production at the LHC

Author

Daniël Boer, Marc Schlegel, Jean-Philippe Lansberg, Miguel G. Echevarria, Florent Scarpa, Cristian Pisano, Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and High-Energy Frontier

Subjects
Particle physics, Nuclear Theory, parton: distribution function, 02 engineering and technology, transverse momentum dependence, High Energy Physics - Experiment, 0202 electrical engineering, electronic engineering, information engineering, J/psi(3100): pair production, 0501 psychology and cognitive sciences, 050107 human factors, Physics, Large Hadron Collider, hep-ex, 05 social sciences, High Energy Physics::Phenomenology, 020207 software engineering, Observable, hep-ph, Upsilon(9460): pair production, gluon, Gluon, High Energy Physics - Phenomenology, Formalism (philosophy of mathematics), Pair production, CERN LHC Coll, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], High Energy Physics::Experiment
Abstract

We report on how $J/\psi$- and $\Upsilon$-pair production are promising processes to access the polarised and unpolarised gluon TMDs at the LHC. We present the formalism used, as well as resulting observables that could be extracted from data., Comment: 5 pages

Published
2019
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27. Azimuthal asymmetries in unpolarized SIDIS and Drell-Yan processes: a case study towards TMD factorization at subleading twist

Author

Alexei Prokudin, Marco Radici, Alessandro Bacchetta, Miguel G. Echevarria, Cristian Pisano, and Giuseppe Bozzi

Subjects
Physics, Nuclear and High Energy Physics, Particle physics, 010308 nuclear & particles physics, Hadron, High Energy Physics::Phenomenology, Drell–Yan process, FOS: Physical sciences, Observable, Parton, 16. Peace & justice, 01 natural sciences, lcsh:QC1-999, High Energy Physics - Phenomenology, Cross section (physics), High Energy Physics - Phenomenology (hep-ph), Factorization, 0103 physical sciences, High Energy Physics::Experiment, Twist, 010306 general physics, Nuclear Experiment, lcsh:Physics, Lepton
Abstract

We consider the azimuthal distribution of the final observed hadron in semi-inclusive deep-inelastic scattering and the lepton pair in the Drell-Yan process. In particular, we focus on the cos⁡ϕ modulation of the unpolarized cross section and on its dependence upon transverse momentum. At low transverse momentum, for these observables we propose a factorized expression based on tree-level approach and conjecture that the same formula is valid in transverse-momentum dependent (TMD) factorization when written in terms of subtracted TMD parton distributions. Our formula correctly matches with the collinear factorization results at high transverse momentum, solves a long-standing problem and is a necessary step towards the extension of the TMD factorization theorems up to the subleading twist.

Published
2019
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28. T-Odd Gluon TMDs Inside a Transversely Polarized Hadron

Author

Miguel G. Echevarria and (Astro)-Particles Physics

Subjects
Physics, Particle physics, 010308 nuclear & particles physics, Scattering, Hadron, 01 natural sciences, Atomic and Molecular Physics, and Optics, Gluon, Independent function, Quantum electrodynamics, 0103 physical sciences, Transverse momentum, Substructure, High Energy Physics::Experiment, SDG 7 - Affordable and Clean Energy, Limit (mathematics), Nuclear Experiment, 010306 general physics, Spin-½
Abstract

We consider the relevant gluon transverse momentum dependent distributions (TMDs) in the spin asymmetries generated by the scattering off transversely polarized hadrons. At large transverse momentum they can be expressed in terms of different collinear distributions, via perturbatively calculable Wilson coefficients. We calculate these coefficients at next-to-leading order, and show that when the small-x limit is taken only one independent function remains for dipole-type gluon TMDs: the so-called spin-dependent odderon. This universal origin for the spin asymmetries is of importance to better understand hadron substructure.

Published
2016
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29. QCD×QED evolution of TMDs

Author

Miguel G. Echevarria and Alessandro Bacchetta

Subjects
Quantum chromodynamics, Quark, Physics, Nuclear and High Energy Physics, Particle physics, 010308 nuclear & particles physics, High Energy Physics::Lattice, High Energy Physics::Phenomenology, Parton, 01 natural sciences, Electric charge, Computer Science::Digital Libraries, lcsh:QC1-999, Universality (dynamical systems), Gluon, Distribution function, 0103 physical sciences, High Energy Physics::Experiment, Physics::Atomic Physics, 010306 general physics, lcsh:Physics
Abstract

We consider for the first time the QED corrections to the evolution of (un)polarized quark and gluon transverse-momentum-dependent distribution and fragmentation functions (TMDs in general). By extending their operator definition to QCD×QED, we provide the mixed new anomalous dimensions up to O(αsα) and the pure QED ones up to O(α2). These new corrections are universal for all TMDs up to the flavor of the considered parton, i.e., the full flavor universality of TMD evolution found in pure QCD is broken in QCD×QED by the presence of the electric charge. In addition, we provide the leading-order QED corrections to the matching coefficients of the unpolarized quark TMD parton distribution function onto its integrated counterparts at O(αs0α).

Published
2018

30. Probing the high-$x$ content of the nuclei in the fixed-target mode at the LHC

Author

C. Quintans, I. Schienbein, Patrick Robbe, Cynthia Marie Hadjidakis, Z. Yang, W. Scandale, Aleksander Kusina, Elena G. Ferreiro, F. Donato, Nataliya Topilskaya, Hua-Sheng Shao, Jan Wagner, Y. I. Makdisi, Joao Seixas, Jean-Philippe Lansberg, Andry Malala Rakotozafindrabe, Cédric Lorcé, Alexander Kurepin, Antonio Uras, S. Porteboeuf, Laure Marie Massacrier, Andrea Signori, Ivana Hrivnacova, Anthony Klein, A. Zelenski, Nodoka Yamanaka, D. P. Kikola, Barbara Antonina Trzeciak, G. Cavoto, C. L. Da Silva, Miguel G. Echevarria, Florian Lyonnet, Stanley J. Brodsky, Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Leprince-Ringuet (LLR), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne (UCA)-Centre National de la Recherche Scientifique (CNRS), Département de Physique Nucléaire (ex SPhN) (DPHN), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de l'Accélérateur Linéaire (LAL), Institut de Physique Nucléaire de Lyon (IPNL), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)

Subjects
Drell-Yan process, Proton, Physics::Instrumentation and Detectors, Nuclear Theory, parton: distribution function, quarkonium: production, 7. Clean energy, 01 natural sciences, High Energy Physics - Experiment, hadronic interactions, quark: structure function, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), ALICE, beam extraction, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Charm (quantum number), Nuclear Experiment, 010303 astronomy & astrophysics, Physics, Large Hadron Collider, 05 social sciences, Detector, Drell–Yan process, hep-ph, p: beam, Quarkonium, hadronic collisions, fixed-target experiment at the LHC, High Energy Physics - Phenomenology, CERN LHC Coll, LHC, Particle Physics - Experiment, Quark, gluon: structure function, ion collisions, Particle physics, FOS: Physical sciences, 0502 economics and business, 0103 physical sciences, heavy quark, Particle Physics - Phenomenology, talk: Aix-Les-Bains 2018/10/01, hep-ex, nucleus: target, High Energy Physics::Phenomenology, LHC-B, Gluon, High Energy Physics::Experiment, charm, 050203 business & management, experimental results
Abstract

Using the LHCb and ALICE detectors in the fixed-target mode at the LHC offers unprecedented possibilities to study the quark, gluon and heavy-quark content of the proton and nuclei in the poorly known region of the high-momentum fractions. We review our projections for studies of Drell-Yan, charm, beauty and quarkonium production with both detector set-ups used with various nuclear targets and the LHC proton beams. Based on this, we show the expected improvement in the determination of the quark, charm and gluon proton and nuclear PDFs as well as discuss the implication for a better understanding of the cold-nuclear-matter effects in hard-probe production in proton-nucleus collisions., Comment: Proceedings of the Hard Probes 2018 conference

Published
2018
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31. A Fixed-Target Programme at the LHC: Physics Case and Projected Performances for Heavy-Ion, Hadron, Spin and Astroparticle Studies

Author

Laure Marie Massacrier, C. Hadjidakis, A. Zelenski, D. P. Kikola, J. Seixas, E.G. Ferreiro, Jakub Wagner, Zishuo Yang, Nataliya Topilskaya, W. Scandale, A. Klein, S. Porteboeuf Houssais, Cédric Lorcé, Patrick Robbe, Jean-Philippe Lansberg, Antonio Uras, C. L. Da Silva, Andrea Signori, Barbara Antonina Trzeciak, Miguel G. Echevarria, I. Hřivnáčová, G. Cavoto, F. Donato, Hua-Sheng Shao, Florian Lyonnet, Stanley J. Brodsky, Nodoka Yamanaka, A. B. Kurepin, C. Quintans, Ingo Schienbein, A. Rakotozafindrabe, A. Kusina, Y. I. Makdisi, Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Leprince-Ringuet (LLR), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne (UCA)-Centre National de la Recherche Scientifique (CNRS), Département de Physique Nucléaire (ex SPhN) (DPHN), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de l'Accélérateur Linéaire (LAL), Institut de Physique Nucléaire de Lyon (IPNL), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)

Subjects
heavy ion: scattering, Nuclear Theory, Physics::Instrumentation and Detectors, p nucleus: interaction, Hadron, heavy-ion physics, General Physics and Astronomy, parton: distribution function, beam transport, nucl-ex, hadron structure, fixed-target program for the Large Hadron Collider, 01 natural sciences, COMPASS, High Energy Physics - Experiment, Sivers function, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), ALICE, Compass, target: wire, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Nuclear Experiment (nucl-ex), Nuclear Experiment, bent crystal, gas: polarized target, Spin-½, Physics, Large Hadron Collider, Detector, hep-ph, collective phenomena, hadronization, nuclear physics, TMD physics, spin physics, astrophysics, Proton (rocket family), High Energy Physics - Phenomenology, CERN LHC Coll, Nuclear Physics - Theory, proposed experiment, Particle Physics - Experiment, performance, astroparticles, p p: scattering, nucl-th, [PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th], energy loss, FOS: Physical sciences, Context (language use), [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], gluon: polarization, Nuclear Theory (nucl-th), Nuclear physics, 0103 physical sciences, Nuclear Physics - Experiment, heavy ion physics, 010306 general physics, Particle Physics - Phenomenology, hep-ex, 010308 nuclear & particles physics, transverse momentum: dependence, nuclear matter: effect, nucleon: structure function, LHC-B, Beamline, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], Physics::Accelerator Physics, nucleon: spin, ion, quarkonium: hadroproduction, quark: polarization
Abstract

We review the context, the motivations and the expected performances of a comprehensive and ambitious fixed-target program using the multi-TeV proton and ion LHC beams. We also provide a detailed account of the different possible technical implementations ranging from an internal wire target to a full dedicated beam line extracted with a bent crystal. The possibilities offered by the use of the ALICE and LHCb detectors in the fixed-target mode are also reviewed., LaTeX, 115 pages. v2: version submitted to Physics Reports. A few figures added and some text improved. v3: accepted for publication in Physics Reports

Published
2018
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32. A fixed-target programme at the LHC for heavy-ion, hadron, spin and astroparticle physics: AFTER@LHC

Author

G. Cavoto, Y. I. Makdisi, Nodoka Yamanaka, A. Rakotozafindrabe, C. L. Da Silva, A. Zelenski, Barbara Antonina Trzeciak, Ingo Schienbein, Jakub Wagner, Zishuo Yang, D. P. Kikola, S. Porteboeuf, J. Seixas, Antonio Uras, Patrick Robbe, Andrea Signori, Miguel G. Echevarria, F. Donato, Nataliya Topilskaya, A. Kusina, Hua-Sheng Shao, A. Klein, Cédric Lorcé, Elena G. Ferreiro, W. Scandale, I. Hřivnáčová, C. Quintans, C. Hadjidakis, Alexey Kurepin, Florian Lyonnet, Stanley J. Brodsky, L. Massacrier, J.P. Lansberg, Laboratoire Leprince-Ringuet (LLR), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Centre de Physique Théorique [Palaiseau] (CPHT), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Département de Physique Nucléaire (ex SPhN) (DPHN), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de l'Accélérateur Linéaire (LAL), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire de Lyon (IPNL), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), AFTER@LHC study, Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne (UCA)-Centre National de la Recherche Scientifique (CNRS), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne [2017-2020] (UCA [2017-2020])-Centre National de la Recherche Scientifique (CNRS), and Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])

Subjects
heavy ion: scattering, Proton, bent crystals, channeling, beam extraction, large hadron collider, Physics::Instrumentation and Detectors, Hadron, quarkonium: production, 115 GeV-cms/nucleon, nucl-ex, spin, 01 natural sciences, 7. Clean energy, hadronic collisions, nuclear physics, fixed-target experiment at the LHC, spin physics, ALICE, lead: beam, Nuclear Experiment (nucl-ex), Nuclear Experiment, Physics, Large Hadron Collider, heavy ion, CERN LHC Coll, Nuclear and High Energy Physics, p p: scattering, Meson, 72 GeV-cms/nucleon, FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], meson, Nuclear physics, 0103 physical sciences, Nuclear Physics - Experiment, heavy quark, 010306 general physics, Spin (physics), p nucleus: scattering, Astroparticle physics, 010308 nuclear & particles physics, High Energy Physics::Phenomenology, LHC-B, Automatic Keywords, Heavy ion, High Energy Physics::Experiment, hadron
Abstract

Thanks to its multi-TeV LHC proton and lead beams, the LHC complex allows one to perform the most energetic fixed-target experiments ever and to study with high precision pp, pd and pA collisions at sqrt(s_NN) = 115 GeV and Pbp and PbA collisions at sqrt(s_NN) = 72 GeV. We present a selection of feasibility studies for the production of quarkonia, open heavy-flavor mesons as well as light-flavor hadrons in pA and PbA collisions using the LHCb and ALICE detectors in a fixed-target mode., Proceedings of the Quark Matter 2018 conference

Published
2018
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33. Quarkonium production to explore hadron 3D structure

Author

Miguel G. Echevarria

Subjects
Physics, Particle physics, Distribution function, Factorization, High Energy Physics::Phenomenology, Hadron, Effective field theory, Parton, Nuclear Experiment, Quarkonium, Gluon, Weighting
Abstract

We discuss how quarkonium production, in particular $\eta_c$ production in proton-proton collisions, can be used to access gluon transverse-momentum-dependent parton distribution functions (TMDPDFs). To do so, we apply the effective field theory machinery to factorize the process in terms of gluon TMDPDFs at low transverse momentum, and match this result with the collinear framework to obtain the full transverse-momentum spectrum. This matching is performed by applying the newly devised inverse-error weighting method, based on an estimation of the uncertainties coming from power corrections to construct a weighted average of both factorization theorems.

Published
2018
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34. Matching factorization theorems with an inverse-error weighting

Author

Jean-Philippe Lansberg, Miguel G. Echevarria, Cristian Pisano, Tomas Kasemets, Andrea Signori, Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Institut de Physique Nucléaire d'Orsay ( IPNO ), and Université Paris-Sud - Paris 11 ( UP11 ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Centre National de la Recherche Scientifique ( CNRS )

Subjects
Drell-Yan process, Nuclear and High Energy Physics, FOS: Physical sciences, Inverse, gauge boson: hadroproduction, 01 natural sciences, transverse momentum: momentum spectrum, Cross section (physics), High Energy Physics - Phenomenology (hep-ph), Factorization, factorization, Simple (abstract algebra), 0103 physical sciences, quantum chromodynamics, Applied mathematics, 010306 general physics, hadron hadron: interaction, Boson, Quantum chromodynamics, Physics, 010308 nuclear & particles physics, matching, deep-inelastic processes, factorization: collinear, High Energy Physics::Phenomenology, Quantum Chromodynamics, power corrections, Drell–Yan process, lcsh:QC1-999, Weighting, High Energy Physics - Phenomenology, kinematics, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], transverse momentum: factorization, [ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph], lcsh:Physics
Abstract

We propose a new fast method to match factorization theorems applicable in different kinematical regions, such as the transverse-momentum-dependent and the collinear factorization theorems in Quantum Chromodynamics. At variance with well-known approaches relying on their simple addition and subsequent subtraction of double-counted contributions, ours simply builds on their weighting using the theory uncertainties deduced from the factorization theorems themselves. This allows us to estimate the unknown complete matched cross section from an inverse-error-weighted average. The method is simple and provides an evaluation of the theoretical uncertainty of the matched cross section associated with the uncertainties from the power corrections to the factorization theorems (additional uncertainties, such as the nonperturbative ones, should be added for a proper comparison with experimental data). Its usage is illustrated with several basic examples, such as $Z$ boson, $W$ boson, $H^0$ boson and Drell-Yan lepton-pair production in hadronic collisions, and compared to the state-of-the-art Collins-Soper-Sterman subtraction scheme. It is also not limited to the transverse-momentum spectrum, and can straightforwardly be extended to match any (un)polarized cross section differential in other variables, including multi-differential measurements., Comment: 9 pages, 2 figures. v2: accepted for publication in PLB

Published
2018
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35. Ultra-peripheral-collision studies in the fixed-target mode with the proton and lead LHC beams

Author

Alexander Kurepin, Patrick Robbe, Y. I. Makdisi, Antonio Uras, Cédric Lorcé, I. Schienbein, Cynthia Marie Hadjidakis, Florian Lyonnet, Andrea Signori, Stanley J. Brodsky, Nataliya Topilskaya, A. Kusina, Z. Yang, W. Scandale, Ivana Hrivnacova, Laure Marie Massacrier, Nodoka Yamanaka, A. Zelenski, D. P. Kikola, Barbara Antonina Trzeciak, Andry Malala Rakotozafindrabe, S. Porteboeuf, Jean-Philippe Lansberg, Miguel G. Echevarria, G. Cavoto, Jan Wagner, C. Quintans, F. Donato, Hua-Sheng Shao, Joao Seixas, Anthony Klein, C. L. Da Silva, Elena G. Ferreiro, Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Leprince-Ringuet (LLR), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne [2017-2020] (UCA [2017-2020])-Centre National de la Recherche Scientifique (CNRS), Département de Physique Nucléaire (ex SPhN) (DPHN), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de l'Accélérateur Linéaire (LAL), Institut de Physique Nucléaire de Lyon (IPNL), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne (UCA)-Centre National de la Recherche Scientifique (CNRS), and Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])

Subjects
heavy ion: scattering, generalized parton distribution, Nuclear Theory, Proton, Physics::Instrumentation and Detectors, p nucleus: interaction, parton: distribution function, Parton, nucl-ex, High Energy Physics - Experiment, hadronic interactions, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), beam extraction, J/psi(3100): photoproduction, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Nuclear Experiment (nucl-ex), Nuclear Experiment, Physics, Large Hadron Collider, hep-ph, 3. Good health, High Energy Physics - Phenomenology, CERN LHC Coll, hydrogen: polarized target, Nuclear Physics - Theory, fixed-target experiment at the LHC, LHC, Particle Physics - Experiment, ion collisions, nucl-th, [PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th], FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], Measure (mathematics), Nuclear physics, Nuclear Theory (nucl-th), Nuclear Physics - Experiment, Particle Physics - Phenomenology, talk: Aix-Les-Bains 2018/10/01, lead, hep-ex, High Energy Physics::Phenomenology, Mode (statistics), gluon, Collision, Gluon, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], High Energy Physics::Experiment, experimental results
Abstract

We address the physics case related to the studies of ultra-peripheral pH, pPb, PbH, and PbPb collisions in the fixed-target mode at the LHC. In particular, we discuss how one can measure the gluon generalized parton distribution E_g(x,xi,t) in exclusive J/psi photoproduction with a transversely polarized hydrogen target., Comment: 6 pages, 3 figures, Proceedings of the International Conference on Hard & Electromagnetic Probes of High-Energy Nuclear Collisions (Hard Probes 2018), 30 September-5 October 2018, Aix-Les-Bains, France

Published
2018
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36. Physics perspectives with AFTER@LHC (A Fixed Target ExpeRiment at LHC)

Author

Ralf Ulrich, Nataliya Topilskaya, V. Chambert, B. Genolini, Z. Yang, Yang Gao, L. Massacrier, Florian Lyonnet, Stanley J. Brodsky, Nodoka Yamanaka, M. Anselmino, E. Steffens, Ulrik I. Uggerhøj, Cristian Pisano, A. Nass, Marc Schlegel, Ingo Schienbein, François Fleuret, Roberta Arnaldi, Jan Wagner, C. Hadjidakis, Cédric Lorcé, Miguel G. Echevarria, Patrick Robbe, J. Seixas, Barbara Antonina Trzeciak, J.P. Didelez, Antonio Uras, Andrea Signori, D. P. Kikola, I. Hřivnáčová, Anthony Klein, Lech Szymanowski, Hua-Sheng Shao, C. L. Da Silva, Elena G. Ferreiro, A. Kusina, Enrico Scomparin, Jean-Philippe Lansberg, Guillermo Martínez, A. B. Kurepin, Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Laboratoire Leprince-Ringuet (LLR), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre de Physique Théorique [Palaiseau] (CPHT), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Laboratoire de physique subatomique et des technologies associées (SUBATECH), Université de Nantes - UFR des Sciences et des Techniques (UN UFR ST), Université de Nantes (UN)-Université de Nantes (UN)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-IMT Atlantique Bretagne-Pays de la Loire (IMT Atlantique), Institut Mines-Télécom [Paris] (IMT)-Institut Mines-Télécom [Paris] (IMT), Laboratoire de l'Accélérateur Linéaire (LAL), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire de Lyon (IPNL), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Université de Nantes - Faculté des Sciences et des Techniques, Université de Nantes (UN)-Université de Nantes (UN)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-IMT Atlantique Bretagne-Pays de la Loire (IMT Atlantique), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire d'Orsay ( IPNO ), Université Paris-Sud - Paris 11 ( UP11 ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Centre National de la Recherche Scientifique ( CNRS ), Laboratoire Leprince-Ringuet ( LLR ), Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -École polytechnique ( X ) -Centre National de la Recherche Scientifique ( CNRS ), Centre de Physique Théorique [Palaiseau] ( CPHT ), École polytechnique ( X ) -Centre National de la Recherche Scientifique ( CNRS ), Laboratoire de physique subatomique et des technologies associées ( SUBATECH ), IMT Atlantique Bretagne-Pays de la Loire ( IMT Atlantique ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Centre National de la Recherche Scientifique ( CNRS ) -Université de Nantes ( UN ), Laboratoire de l'Accélérateur Linéaire ( LAL ), Laboratoire de Physique Subatomique et de Cosmologie ( LPSC ), Université Joseph Fourier - Grenoble 1 ( UJF ) -Institut polytechnique de Grenoble - Grenoble Institute of Technology ( Grenoble INP ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique ( CNRS ) -Université Grenoble Alpes ( UGA ), Laboratoire de Physique Théorique et Hautes Energies ( LPTHE ), Université Pierre et Marie Curie - Paris 6 ( UPMC ) -Centre National de la Recherche Scientifique ( CNRS ), Institut de Physique Nucléaire de Lyon ( IPNL ), Université Claude Bernard Lyon 1 ( UCBL ), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Centre National de la Recherche Scientifique ( CNRS ), Subatomic Physics, and Sub Subatomic Physics (SAP)

Subjects
Proton, 115 GeV-cms/nucleon, PROTON, nucl-ex, 7. Clean energy, 01 natural sciences, High Energy Physics - Experiment, High Energy Physics - Experiment (hep-ex), hadronic collisions, fixed-target experiment at the LHC, spin physics, 72 GeV-cms/nucleon115 GeV-cms/nucleon, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], [ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex], Nuclear Experiment (nucl-ex), Nuclear Experiment, n: spin, talk: Utrecht 2017/07/10, Brookhaven RHIC Coll, quark gluon: plasma, Physics, Large Hadron Collider, HELAC-ONIA, BEAMS, CERN LHC Coll, heavy quark: hadroproduction, proposed experiment, Particle Physics - Experiment, Particle physics, FEASIBILITY, QC1-999, 72 GeV-cms/nucleon, FOS: Physical sciences, Physics and Astronomy(all), MATRIX-ELEMENT, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], p: spin, [ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex], 0103 physical sciences, Neutron, Nuclear Physics - Experiment, 010306 general physics, HEAVY QUARKONIUM PHYSICS, Spins, 010308 nuclear & particles physics, hep-ex, High Energy Physics::Phenomenology, CERN SPS, GENERATOR, Quark–gluon plasma, High Energy Physics::Experiment
Abstract

AFTER@LHC is an ambitious fixed-target project in order to address open questions in the domain of proton and neutron spins, Quark Gluon Plasma and high-$x$ physics, at the highest energy ever reached in the fixed-target mode. Indeed, thanks to the highly energetic 7 TeV proton and 2.76 A.TeV lead LHC beams, center-of-mass energies as large as $\sqrt{s_{NN}}$ = 115 GeV in pp/pA and $\sqrt{s_{NN}}$ = 72 GeV in AA can be reached, corresponding to an uncharted energy domain between SPS and RHIC. We report two main ways of performing fixed-target collisions at the LHC, both allowing for the usage of one of the existing LHC experiments. In these proceedings, after discussing the projected luminosities considered for one year of data taking at the LHC, we will present a selection of projections for light and heavy-flavour production., Comment: Proceeding of SQM2017 conference

Published
2017
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38. Soft and collinear factorization and transverse momentum dependent parton distribution functions

Author

Ahmad Idilbi, Miguel G. Echevarria, and Ignazio Scimemi

Subjects
Physics, Nuclear and High Energy Physics, Particle physics, Differential equation, High Energy Physics::Phenomenology, Hadron, FOS: Physical sciences, Parton, Invariant (physics), High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), Distribution function, Factorization, High Energy Physics::Experiment, Rapidity, Nuclear Experiment, Lepton
Abstract

In this work we consider how a parton distribution function, with an explicit transverse momentum dependence can be properly defined in a regularization-scheme independent manner. We argue that by considering a factorized form of the transverse momentum dependent spectrum for the production of a heavy lepton pair in Drell-Yan reaction, one should first split the relevant soft function into two boost invariant contributions. When those soft contributions are added to the pure collinear contributions, well-defined hadronic matrix elements emerge, i.e., the transverse momentum dependent distributions. We also perform a comparison with Collins' definition., Comment: 9 pages, 3 figures. We modified the discussion about the equivalence between Collins (JCC) and Echevarria-Idilbi-Scimemi (EIS) definitions of TMDPDF. The results remain intact. Version to appear in Phys. Lett. B

Published
2013
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40. Proper definition and evolution of generalized transverse momentum dependent distributions

Author

Barbara Pasquini, Miguel G. Echevarria, Koichi Kanazawa, Marc Schlegel, Cédric Lorcé, Andreas Metz, Ahmad Idilbi, and (Astro)-Particles Physics

Subjects
Physics, Quark, Nuclear and High Energy Physics, Particle physics, Similarity (geometry), Logarithm, 010308 nuclear & particles physics, Hadron, High Energy Physics::Phenomenology, 01 natural sciences, lcsh:QC1-999, Gluon, Theoretical physics, Matrix (mathematics), Kernel (image processing), 0103 physical sciences, SDG 7 - Affordable and Clean Energy, 010306 general physics, lcsh:Physics, Spin-½
Abstract

We consider one of the most fundamental sets of hadronic matrix elements, namely the generalized transverse momentum dependent distributions (GTMDs), and argue that their existing definitions lack proper evolution properties. By exploiting the similarity of GTMDs with the much better understood transverse momentum distributions, we argue that the existing definitions of GTMDs have to include an additional dependence on soft gluon radiation in order to render them properly defined. With this, we manage to obtain the evolution kernel of all (un)polarized quark and gluon GTMDs, which turns out to be spin independent. As a byproduct, all large logarithms can be resummed up to next-to-next-to-leading-logarithmic accuracy with the currently known perturbative ingredients.

Published
2016
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41. Single-Transverse-Spin-Asymmetry studies with a fixed-target experiment using the LHC beams (AFTER@LHC)

Author

Cristian Pisano, Miguel G. Echevarria, Anthony Klein, A. Kusina, M. Anselmino, Enrico Scomparin, Jean-Philippe Lansberg, Cédric Lorcé, Cynthia Marie Hadjidakis, Ingo Schienbein, V. Chambert, B. Genolini, Z. Yang, C. L. Da Silva, François Fleuret, Elena G. Ferreiro, Ralf Ulrich, I. Hřivnáčová, Marc Schlegel, Laure Marie Massacrier, Hua-Sheng Shao, D. P. Kikola, E. Steffens, A. B. Kurepin, J.P. Didelez, Antonio Uras, A. Nass, Andrea Signori, Barbara Antonina Trzeciak, Nataliya Topilskaya, Patrick Robbe, Roberta Arnaldi, J. Seixas, Yang Gao, Florian Lyonnet, Stanley J. Brodsky, Ulrik I. Uggerhøj, Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Laboratoire Leprince-Ringuet (LLR), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut de Recherche pour le Développement (IRD), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), Laboratoire de l'Accélérateur Linéaire (LAL), Institut de Physique Nucléaire de Lyon (IPNL), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), ALICE, Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)

Subjects
Particle physics, Nuclear Theory, [PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th], media_common.quotation_subject, FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], 7. Clean energy, 01 natural sciences, Measure (mathematics), Asymmetry, High Energy Physics - Experiment, Nuclear Theory (nucl-th), Nuclear physics, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), 0103 physical sciences, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, media_common, Spin-½, Physics, Large Hadron Collider, 010308 nuclear & particles physics, High Energy Physics - Phenomenology, Transverse plane, Particle Physics - Experiment
Abstract

We discuss the potential of AFTER@LHC to measure single-transverse-spin asymmetries in open-charm and bottomonium production. With a HERMES-like hydrogen polarised target, such measurements over a year can reach precisions close to the per cent level. This is particularly remarkable since these analyses can probably not be carried out anywhere else, Comment: 8 pages, 3 figures, 1 table. LaTeX, uses PoS.cls (included). Contribution to the proceedings of the XXIV International Workshop on Deep-Inelastic Scattering and Related Subject - DIS 2016, 11-15 April 2016, DESY Hamburg, Germany

Published
2016

43. Physics case for a polarised target for AFTER@LHC

Author

Jean-Philippe Lansberg, Mauro Anselmino, Roberta Arnaldi, Stanley J. Brodsky, Valérie Chambert, Jean-Pierre Didelez, Miguel G. Echevarria, Elena Gonzalez Ferreiro, Frédéric Fleuret, Yuanning Gao, Bernard Genolini, Cynthia Hadjidakis, Ivana Hrivnacova, Daniel Kikola, A. Kurepin, Cedric Lorce, Laure Massacrier, Alexander Nass, Christian Pisano, Ingo Schienbein, Marc Schlegel, Enrico Scomparin, Joao SEIXAS, Andrea Signori, Erhard STEFFENS, Natalia Topilskaya, Barbara Trzeciak, Ulrik Uggerhoej, Antonio Uras, Ralf Matthias Ulrich, and Zhenwei Yang

Subjects
Physics, Spin physics, fixed-target experiment, LHC, hadron structure, Particle physics, Large Hadron Collider, Photon, Physics::Instrumentation and Detectors, High Energy Physics::Phenomenology, Measure (physics), Drell–Yan process, Jet (particle physics), Quarkonium, Gluon, Polarized target
Abstract

We review a number of ideas put forward in favour of the use of a polarised target along with the proposed idea of a fixed-target experiment using the LHC beams -- AFTER@LHC. A number of recent studies have shown that single transverse-spin asymmetries (STSAs) are large enough to be precisely measured in the region accessible with AFTER@LHC, in particular as regards the Drell-Yan process as well as single-pion, isolated-photon and jet production. AFTER@LHC with a polarised target would also be the ideal experimental set-up to measure the gluon Sivers effect via a number of original quarkonium STSA studies. We discuss first figures-of-merit based on simulations for AFTER@LHC with a polarised target.

Published
2016

44. Universal transverse momentum dependent soft function at NNLO

Author

Ignazio Scimemi, Miguel G. Echevarria, Aleksey Vladimirov, and (Astro)-Particles Physics

Subjects
High Energy Physics - Theory, Physics, Quark, Particle physics, Física-Modelos matemáticos, 010308 nuclear & particles physics, High Energy Physics::Phenomenology, Nuclear Theory, Drell–Yan process, FOS: Physical sciences, Deep inelastic scattering, 01 natural sciences, Gluon, Casimir effect, High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), High Energy Physics - Theory (hep-th), Regularization (physics), 0103 physical sciences, Física matemática, Rapidity, SDG 7 - Affordable and Clean Energy, Resummation, 010306 general physics
Abstract

All (un)polarized transverse momentum dependent functions (TMDs), both distribution and fragmentation functions, are defined with the same universal soft function, which cancels spurious rapidity divergences within an individual TMD and renders them well-defined hadronic quantities. Moreover, it is independent of the kinematics, whether it is Drell-Yan, deep inelastic scattering or $e^+e^-\rightarrow 2$ hadrons. In this paper we provide this soft function at next-to-next-to-leading order (NNLO), necessary for the calculation of all TMDs at the same order, and to perform the resummation of large logarithms at next-to-next-to-next-to-leading-logarithmic accuracy. From the results we obtain the $D$ function at NNLO, which governs the evolution of all TMDs. This work represents the first independent and direct calculation of this quantity. Given the all order relation through a Casimir scaling between the soft function relevant for gluon TMDs and the one for quark TMDs, we also obtain the first at NNLO. The used regularization method to deal with the rapidity divergences is discussed as well., Comment: 12 pages, 2 figures. v2: minor rewording, accepted for publication in PRD

Published
2016
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45. Transverse momentum dependent fragmentation function at next-to-next-to-leading order

Author

Miguel G. Echevarria, Aleksey Vladimirov, Ignazio Scimemi, and (Astro)-Particles Physics

Subjects
Physics, High energy, 010308 nuclear & particles physics, Soft function, Física, 01 natural sciences, Classical mechanics, Quantum electrodynamics, 0103 physical sciences, Transverse momentum, Fragmentation function, Rapidity, SDG 7 - Affordable and Clean Energy, Resummation, 010306 general physics, Spurious relationship
Abstract

We calculate the unpolarized transverse momentum dependent fragmentation function at next-to-next-to-leading order, evaluating separately the transverse momentum dependent (TMD) soft factor and the TMD collinear correlator. For the first time, the cancellation of spurious rapidity divergences in a properly defined individual TMD beyond the first nontrivial order is shown. This represents a strong check of the given TMD definition. We extract the matching coefficient necessary to perform the transverse momentum resummation at next-to-next-to-next-to-leading-logarithmic accuracy. The universal character of the soft function, which enters the definition of all (un)polarized TMD distribution/fragmentation functions, facilitates the future calculation of all the other TMDs and their coefficients at next-to-next-to-leading order, pushing forward the accuracy of theoretical predictions for the current and next generation of high energy colliders.

Published
2016
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46. DEFINITION AND EVOLUTION OF TRANSVERSE MOMENTUM DISTRIBUTIONS

Author

Ignazio Scimemi, Ahmad Idilbi, and Miguel G. Echevarria

Subjects
Physics, Particle physics, Logarithm, Soft function, High Energy Physics::Phenomenology, FOS: Physical sciences, Parton, Field (mathematics), High Energy Physics - Phenomenology, symbols.namesake, Theoretical physics, High Energy Physics - Phenomenology (hep-ph), Distribution function, Weierstrass factorization theorem, Transverse momentum, medicine, symbols, medicine.symptom, Confusion
Abstract

We consider the definition of unpolarized transverse-momentum-dependent parton distribution functions while staying on-the-light-cone. By imposing a requirement of identical treatment of two collinear sectors, our approach, compatible with a generic factorization theorem with the soft function included, is valid for all non-ultra-violet regulators (as it should), an issue which causes much confusion in the whole field. We explain how large logarithms can be resummed in a way which can be considered as an alternative to the use of Collins-Soper evolution equation. The evolution properties are also discussed and the gauge-invariance, in both classes of gauges, regular and singular, is emphasized., 15 pages. Proceedings of QCD Evolution Workshop, May 14-17 2012, JLAB

Published
2012
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47. Transverse Momentum Dependent (TMD) Parton Distribution Functions: Status and Prospects

Author

Emanuele R. Nocera, Federico Alberto Ceccopieri, Elena Petreska, Voica Radescu, Lech Szymanowski, Daniël Boer, S. Taheri Monfared, Krzysztof Kutak, Marco Radici, Cristian Pisano, Mariaelena Boglione, R. Placakyte, Hannes Jung, Patrick Connor, Gennady Lykasov, P. Van Mechelen, R. Boussarie, Francesco Hautmann, Igor Olegovich Cherednikov, Andrea Signori, Aleksandra Lelek, R. Angeles-Martinez, J. Grados Luyando, Miguel G. Echevarria, Alessandro Bacchetta, H. Van Haevermaet, G. Schnell, Alexey Vladimirov, Tomas Kasemets, J. D. Madrigal Martinez, Ian Balitsky, Ignazio Scimemi, Giancarlo Ferrera, F. F. Van der Veken, Jean-Philippe Lansberg, S. Wallon, Piet J. Mulders, (Astro)-Particles Physics, Theoretical Physics, High-Energy Frontier, Laboratoire de Physique Théorique d'Orsay [Orsay] (LPT), Université Paris-Sud - Paris 11 (UP11)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire d'Orsay (IPNO), and Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)

Subjects
HIGH-ENERGY FACTORIZATION, PROTON-PROTON COLLISIONS, density [parton], General Physics and Astronomy, momentum spectrum [transverse momentum], Parton, Jet (particle physics), transverse momentum dependence, mass [jet], DEEP-INELASTIC SCATTERING, High Energy Physics - Phenomenology (hep-ph), scattering [hadron], Resummation, Nuclear Experiment, Boson, Physics, Quantum chromodynamics, angular correlation, vector boson, hep-ph, transverse momentum [Higgs particle], High Energy Physics - Phenomenology, resummation, Higgs boson, Partículas, VECTOR-BOSON PRODUCTION, SINGLE-SPIN ASYMMETRIES, distribution function [parton], Phenomenology (particle physics), SMALL-X EVOLUTION, Particle physics, multiple production [jet], MONTE-CARLO GENERATOR, HEAVY FLAVOR PRODUCTION, heavy [boson], review, FOS: Physical sciences, transverse momentum [vector boson], transverse momentum, HARD-COLLINEAR COEFFICIENTS, Factorization, factorization, angular correlation [jet], production [vector boson], quantum chromodynamics, ddc:530, SDG 7 - Affordable and Clean Energy, High Energy Physics::Phenomenology, DIFFERENTIAL CROSS-SECTION, production [Higgs particle], [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], evolution equation, High Energy Physics::Experiment
Abstract

We provide a concise overview on transverse momentum dependent (TMD) parton distribution functions, their application to topical issues in high-energy physics phenomenology, and their theoretical connections with QCD resummation, evolution and factorization theorems. We illustrate the use of TMDs via examples of multi-scale problems in hadronic collisions. These include transverse momentum q_T spectra of Higgs and vector bosons for low q_T, and azimuthal correlations in the production of multiple jets associated with heavy bosons at large jet masses. We discuss computational tools for TMDs, and present an application of a new tool, TMDlib, to parton density fits and parameterizations., 20 pages

Published
2015
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48. Single spin asymmetries from a single Wilson loop

Author

Piet J. Mulders, Jian Zhou, Miguel G. Echevarria, Daniël Boer, High-Energy Frontier, and (Astro)-Particles Physics

Subjects
Particle physics, Wilson loop, Hadron, General Physics and Astronomy, FOS: Physical sciences, Expectation value, POLARIZED PROTON-BEAM, 01 natural sciences, Color-glass condensate, Momentum, High Energy Physics - Phenomenology (hep-ph), 0103 physical sciences, SDG 7 - Affordable and Clean Energy, 010306 general physics, Nuclear Experiment, Spin-½, Quantum chromodynamics, Physics, 010308 nuclear & particles physics, COLOR GLASS CONDENSATE, hep-ph, QCD, Gluon, High Energy Physics - Phenomenology, ODDERON, Quantum electrodynamics, ANALYZING POWER, APPROXIMATION
Abstract

We study the leading-power gluon transverse momentum dependent distributions (TMDs) of relevance to the study of asymmetries in the scattering off transversely polarized hadrons. Next-to-leading-order perturbative calculations of these TMDs show that at large transverse momentum they have common dynamical origins, but that in the limit of small longitudinal momentum fraction $x$ only one origin remains. We find that in this limit only the dipole-type gluon TMDs survive and become identical to each other. At small $x$ they are all given by the expectation value of a single Wilson loop inside the transversely polarized hadron, the so-called spin-dependent odderon. This universal origin of transverse spin asymmetries at small $x$ is of importance to current and future experimental studies, paving the way to a better understanding of the role of gluons in the three-dimensional structure of spin-polarized protons., 5 pages, 1 figure. Various changes to the text, additional references, conclusions unchanged, version accepted for publication in Physical Review Letters

Published
2015
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49. QCD evolution of (un)polarized gluon TMDPDFs and the Higgs qT -distribution

Author

Piet J. Mulders, Cristian Pisano, Miguel G. Echevarria, Tomas Kasemets, (Astro)-Particles Physics, and Theoretical Physics

Subjects
Nuclear and High Energy Physics, Particle physics, FOS: Physical sciences, Parton, 01 natural sciences, High Energy Physics - Experiment, Mathematics::Numerical Analysis, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), Mathematics::Probability, 0103 physical sciences, Resummation, Nuclear Experiment, 010306 general physics, Physics, Quantum chromodynamics, Large Hadron Collider, 010308 nuclear & particles physics, High Energy Physics::Phenomenology, Helicity, Gluon, Pseudoscalar, High Energy Physics - Phenomenology, Higgs boson, High Energy Physics::Experiment
Abstract

We provide the proper definition of all the leading-twist (un)polarized gluon transverse momentum dependent parton distribution functions (TMDPDFs), by considering the Higgs boson transverse momentum distribution in hadron-hadron collisions and deriving the factorization theorem in terms of them. We show that the evolution of all the (un)polarized gluon TMDPDFs is driven by a universal evolution kernel, which can be resummed up to next-to-next-to-leading-logarithmic accuracy. Considering the proper definition of gluon TMDPDFs, we perform an explicit next-to-leading-order calculation of the unpolarized ($f_1^g$), linearly polarized ($h_1^{\perp g}$) and helicity ($g_{1L}^g$) gluon TMDPDFs, and show that, as expected, they are free from rapidity divergences. As a byproduct, we obtain the Wilson coefficients of the refactorization of these TMDPDFs at large transverse momentum. In particular, the coefficient of $g_{1L}^g$, which has never been calculated before, constitutes a new and necessary ingredient for a reliable phenomenological extraction of this quantity, for instance at RHIC or the future AFTER@LHC or Electron-Ion Collider. The coefficients of $f_1^g$ and $h_1^{\perp g}$ have never been calculated in the present formalism, although they could be obtained by carefully collecting and recasting previous results in the new TMD formalism. We apply these results to analyze the contribution of linearly polarized gluons at different scales, relevant, for instance, for the inclusive production of the Higgs boson and the $C$-even pseudoscalar bottomonium state $\eta_{b}$. Applying our resummation scheme we finally provide predictions for the Higgs boson $q_T$-distribution at the LHC., Comment: 36 pages, 9 figures. v2: typos corrected, references added, discussion on resummation and analysis of theoretical uncertainties improved, JHEP version. v3: gluon helicity coefficient corrected, corresponding plots updated, typos fixed, references added. v4: typo fixed. v5: typos fixed

Published
2015
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50. Scale evolution of gluon TMDPDFs

Author

Miguel G. Echevarria, Tomas Kasemets, Cristian Pisano, Piet J. Mulders, and (Astro)-Particles Physics

Subjects
Physics, Particle physics, QC1-999, Hadron, High Energy Physics::Phenomenology, Parton, Gluon, Distribution function, Effective field theory, Higgs boson, Rapidity, High Energy Physics::Experiment, Resummation, Nuclear Experiment
Abstract

By applying the effective field theory machinery we factorize the transverse momentum spectrum of Higgs boson production, where the main hadronic quantities are the gluon transverse momentum dependent parton distribution functions (TMDPDFs). We properly define those quantities, showing explicitly, in the case of an unpolarized hadron, that they are free from rapidity divergences, and extract their evolution properties. It turns out that the evolution for all eight (un-)polarized leading-twist gluon TMDPDFs is driven by the same evolution kernel, for which we derive the necessary ingredients to obtain a resummation of large logarithms at next-tonext-to-leading-logarithmic accuracy. We make predictions for the contribution of linearly polarized gluons to the Higgs boson qT -spectrum.

Published
2015
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