Measurement of the average transverse momentum of forward prompt charged particles in $pp$ and pPb collisions at sNN=5.02TeV
Using LHCb data from $pp$ and pPb collisions at sNN=5.02TeV, this study presents the first measurements of the average transverse momentum of forward prompt charged particles, revealing a decreasing trend with pseudorapidity that supports collective behavior and aligns with hydrodynamic calculations while contradicting saturation models.
Original authors: LHCb collaboration, R. Aaij, M. Abdelfatah, A. S. W. Abdelmotteleb, C. Abellan Beteta, F. Abudinén, T. Ackernley, A. A. Adefisoye, B. Adeva, M. Adinolfi, P. Adlarson, C. Agapopoulou, C. A. Aidala, S. Akar, K. Akiba, P. Albicocco, J. Albrecht, R. Aleksiejunas, F. Alessio, P. Alvarez Cartelle, S. Amato, J. L. Amey, Y. Amhis, L. An, L. Anderlini, M. Andersson, P. Andreola, M. Andreotti, S. Andres Estrada, A. Anelli, D. Ao, C. Arata, F. Archilli, Z. Areg, M. Argenton, S. Arguedas Cuendis, L. Arnone, M. Artuso, E. Aslanides, R. Ataíde Da Silva, M. Atzeni, B. Audurier, J. A. Authier, D. Bacher, I. Bachiller Perea, S. Bachmann, M. Bachmayer, J. J. Back, Z. B. Bai, V. Balagura, A. Balboni, W. Baldini, Z. Baldwin, L. Balzani, H. Bao, J. Baptista de Souza Leite, C. Barbero Pretel, M. Barbetti, I. R. Barbosa, R. J. Barlow, M. Barnyakov, S. Baron, S. Barsuk, W. Barter, J. Bartz, S. Bashir, B. Batsukh, P. B. Battista, A. Bavarchee, A. Bay, A. Beck, M. Becker, F. Bedeschi, I. B. Bediaga, N. A. Behling, S. Belin, A. Bellavista, I. Belov, I. Belyaev, G. Bencivenni, E. Ben-Haim, J. L. M. Berkey, R. Bernet, A. Bertolin, F. Betti, J. Bex, O. Bezshyyko, S. Bhattacharya, M. S. Bieker, N. V. Biesuz, A. Biolchini, M. Birch, F. C. R. Bishop, A. Bitadze, A. Bizzeti, T. Blake, F. Blanc, J. E. Blank, S. Blusk, J. A. Boelhauve, O. Boente Garcia, T. Boettcher, A. Bohare, C. Bolognani, R. Bolzonella, R. B. Bonacci, A. Bordelius, F. Borgato, S. Borghi, M. Borsato, J. T. Borsuk, E. Bottalico, S. A. Bouchiba, M. Bovill, T. J. V. Bowcock, A. Boyer, C. Bozzi, J. D. Brandenburg, A. Brea Rodriguez, N. Breer, C. Breitfeld, J. Brodzicka, J. Brown, D. Brundu, E. Buchanan, M. Burgos Marcos, C. Burr, C. Buti, J. S. Butter, J. Buytaert, W. Byczynski, S. Cadeddu, H. Cai, Y. Cai, A. Caillet, R. Calabrese, L. Calefice, M. Calvi, M. Calvo Gomez, P. Camargo Magalhaes, J. I. Cambon Bouzas, P. Campana, A. C. Campos, A. F. Campoverde Quezada, Y. Cao, S. Capelli, M. Caporale, L. Capriotti, R. Caravaca-Mora, A. Carbone, L. Carcedo Salgado, R. Cardinale, A. Cardini, P. Carniti, L. Carus, A. Casais Vidal, R. Caspary, G. Casse, M. Cattaneo, G. Cavallero, V. Cavallini, S. Celani, I. Celestino, S. Cesare, A. J. Chadwick, I. Chahrour, M. Charles, Ph. Charpentier, E. Chatzianagnostou, R. Cheaib, M. Chefdeville, C. Chen, J. Chen, S. Chen, Z. Chen, A. Chen Hu, M. Cherif, S. Chernyshenko, X. Chiotopoulos, G. Chizhik, V. Chobanova, M. Chrzaszcz, V. Chulikov, P. Ciambrone, X. Cid Vidal, P. Cifra, P. E. L. Clarke, M. Clemencic, H. V. Cliff, J. Closier, C. Cocha Toapaxi, V. Coco, J. Cogan, E. Cogneras, L. Cojocariu, S. Collaviti, P. Collins, T. Colombo, M. Colonna, A. Comerma-Montells, L. Congedo, J. Connaughton, A. Contu, N. Cooke, G. Cordova, C. Coronel, I. Corredoira, A. Correia, G. Corti, G. C. Costantino, J. Cottee Meldrum, B. Couturier, D. C. Craik, N. Crepet, M. Cruz Torres, M. Cubero Campos, E. Curras Rivera, R. Currie, C. L. Da Silva, X. Dai, J. Dalseno, C. D'Ambrosio, G. 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Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). ✨ This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer
Imagine the universe as a giant, cosmic kitchen. For decades, physicists have been trying to figure out what happens when you smash ingredients together at speeds close to the speed of light. Usually, they use massive "ovens" called particle colliders to smash heavy atoms (like lead) into each other. When these heavy atoms collide, they melt into a super-hot, super-dense soup called a quark-gluon plasma. This soup behaves like a near-perfect fluid, flowing and swirling together in a coordinated dance known as "collective behavior." It's like dropping a drop of milk into a cup of coffee and watching it swirl in a perfect, organized pattern rather than just splashing randomly.
But here's the mystery: scientists started seeing this same organized "swirling" dance even when they smashed tiny ingredients together, like single protons (the building blocks of atoms) or a proton against a lead atom. These are much smaller collisions, and according to old theories, they should be too small to create a fluid soup. It's like seeing a perfect swirl in a single drop of coffee. This has sparked a huge debate. One group of scientists thinks this is actually a tiny drop of the same fluid soup. Another group thinks it's something else entirely, like a "Color Glass Condensate"—a state where the tiny particles inside the proton are so packed together they act like a frozen, saturated sponge. To solve this, we need to look at how the particles fly out of the collision. If they are flowing like a fluid, they should move in a specific way depending on where you look. If they are just a saturated sponge, they should move differently.
This paper from the LHCb collaboration at CERN takes a fresh look at this puzzle by measuring the "average push" (transverse momentum) of particles flying out of these tiny collisions. They didn't just look at the particles; they looked at how many particles were created in each crash and where they were flying. They found that in collisions with a lot of particles (high multiplicity), the particles fly out in a way that strongly suggests they are flowing like a fluid. The data matches the predictions of complex fluid simulations perfectly. However, the data does not match the predictions of the "saturated sponge" models, especially when there are many particles involved.
The researchers used the LHCb detector, which is like a high-speed camera positioned to the side of the collision point, to catch particles flying out at a forward angle. They analyzed data from collisions at an energy of 5.02 TeV. They measured the average transverse momentum (how hard the particles are kicked sideways) for different numbers of particles produced. They discovered that as you look further out toward the "edges" of the collision (higher pseudorapidity), the average kick gets weaker. This drop-off is much more noticeable when a lot of particles are created.
The results are a strong hint that the "fluid soup" theory is the right one for these small systems. The authors state that their measurements are reproduced by state-of-the-art hydrodynamic calculations (the fluid models). In contrast, they explicitly note that the saturation models (the "saturated sponge" or Color Glass Condensate ideas) are not compatible with their data. While the models can describe the data qualitatively in some low-particle cases, they fail to explain the trend when many particles are produced. The paper concludes that this specific behavior—where the particle push decreases as you look further forward, especially in crowded collisions—is a signature of collective fluid behavior, providing a unique view into how matter behaves even in the smallest collision systems.
Technical Summary: Measurement of the average transverse momentum of forward prompt charged particles in pp and pPb collisions at sNN=5.02 TeV
Problem and Motivation
The characterization of collective behavior in high-energy particle collisions remains a central challenge in nuclear physics. While signatures of collectivity, such as azimuthal anisotropies and radial flow, are well-established in large nucleus-nucleus systems interpreted as quark-gluon plasma (QGP), their emergence in smaller systems (proton-proton and proton-lead) is less understood. Two primary theoretical frameworks compete to explain these phenomena: the hydrodynamic expansion of a dense medium and the Color Glass Condensate (CGC) model, which attributes correlations to initial-state gluon saturation.
A critical observable proposed to distinguish between these mechanisms is the average transverse momentum (⟨pT⟩) of charged particles. Previous measurements in large systems have shown ⟨pT⟩ increases with event multiplicity. However, the dependence of ⟨pT⟩ on pseudorapidity (η) in small collision systems, particularly in the forward region where small Bjorken-x dynamics dominate, had not been measured. The LHCb experiment, with its forward geometry, is uniquely positioned to probe this kinematic region to test whether collective behavior persists and how it evolves with rapidity.
Methodology
This analysis utilizes data recorded by the LHCb experiment at a nucleon-nucleon centre-of-mass energy of sNN=5.02 TeV. The dataset includes:
- pPb collisions: Acquired in 2013 with integrated luminosities of 42.7±1.0μb−1 (pPb) and 38.7±1.0μb−1 (Pbp).
- pp collisions: Acquired in 2015 with an integrated luminosity of 3.49±0.07nb−1.
The analysis focuses on prompt charged particles, defined as hadrons and leptons with a mean lifetime τ>0.3×10−10 s, produced directly or from short-lived decays. The measurement covers the transverse momentum range 0.5<pT<8.0 GeV/c and the laboratory pseudorapidity range 2.0<ηLab<4.8.
Key methodological steps include:
- Event Selection: Events are selected using minimum-bias triggers (for pPb) or unbiased triggers (for pp), requiring a single reconstructed primary vertex (PV).
- Track Reconstruction and Background Suppression: Candidates must have hits in the Vertex Locator (VELO) and tracking stations. Backgrounds from fake tracks, secondary particles (from detector material or weak decays), and clone tracks are suppressed using neural-network classifiers (ghost probability), track-fit quality, and impact parameter requirements.
- Efficiency and Purity Corrections: Reconstruction and selection efficiencies are determined using simulation (Epos-lhc for pPb, Pythia for pp) and validated with data-driven tag-and-probe methods using J/ψ→μ+μ− decays. Particle composition corrections are applied to account for discrepancies in simulation.
- Unfolding: A Bayesian unfolding procedure is employed to correct for bin migration in the multiplicity distribution.
- Observable Definition: The average transverse momentum is calculated as a function of the prompt charged particle yield (Nchacc) and pseudorapidity (η).
Key Contributions
This paper presents the first measurement of the average transverse momentum of forward prompt charged particles in pp and pPb/Pbp collisions as a function of both collision multiplicity and pseudorapidity. It extends the study of collectivity to the forward rapidity region, a domain previously unexplored for this specific observable in small systems.
Results
- Multiplicity Dependence: The measured ⟨pT⟩ increases with event multiplicity for all three collision systems (pp, pPb, and Pbp). This trend is consistent with observations in larger collision systems by the ALICE collaboration.
- Pseudorapidity Dependence: A decreasing trend of ⟨pT⟩ with increasing pseudorapidity is observed. This splitting is more pronounced in high-multiplicity events, while low-multiplicity events show convergence across η intervals.
- Comparison with Models:
- Hydrodynamics: State-of-the-art (3+1D) hydrodynamic calculations from the JETSCAPE collaboration reproduce the data qualitatively, capturing the decreasing trend in ⟨pT⟩ at forward rapidities.
- CGC Models: Saturation models (specifically rcBK, GBW, and BUW) fail to reproduce the data. While the rcBK model qualitatively describes low-multiplicity pp data, the GBW model incorrectly predicts an increase in ⟨pT⟩ with η. Generally, CGC models do not describe the observed pseudorapidity trend, particularly at high multiplicities.
- Multiplicity Distributions: The measured multiplicity distributions are qualitatively described by Epos-lhc (for pPb) and Pythia (for pp), though Epos-lhc overestimates the data in the high-multiplicity region for Pbp collisions.
Significance
The paper claims that these measurements provide a unique view of collective effects in small collision systems using an observable not previously measured in this kinematic regime. The observation of a decreasing ⟨pT⟩ with pseudorapidity, which strengthens with multiplicity, is consistent with the expectations of collective behavior (hydrodynamic expansion). The inability of current CGC-based models to reproduce the pseudorapidity trend, especially at high multiplicities, suggests that initial-state saturation effects alone may be insufficient to describe the dynamics in these forward regions, lending support to the hydrodynamic interpretation of collectivity even in small systems.
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