Beyond Collisions: Unlocking Nuclear Physics with a Fixed-Target Experiment

Author: Denis Avetisyan


A new study proposes a complementary fixed-target program at the future Electron-Ion Collider to broaden our understanding of nuclear matter and its fundamental properties.

Existing and proposed fixed-target experiments-including HADES, BM@N, AGS, STAR, NA49, NA61/SHINE, NA60, CBM, J-PARC, and SMOG-collectively map the <span class="katex-eq" data-katex-display="false">\sqrt{s_{NN}}</span> collision energy landscape, with the projected Electron-Ion Collider measurements extending this reach into previously unexplored regimes.
Existing and proposed fixed-target experiments-including HADES, BM@N, AGS, STAR, NA49, NA61/SHINE, NA60, CBM, J-PARC, and SMOG-collectively map the \sqrt{s_{NN}} collision energy landscape, with the projected Electron-Ion Collider measurements extending this reach into previously unexplored regimes.

This review details the physics opportunities offered by a fixed-target experiment at the EIC, including studies of cold nuclear matter, the QCD phase diagram, and nuclear structure with polarized beams and a broad energy range.

Despite significant progress in understanding the strong force, quantitative descriptions of cold nuclear matter and the quantum chromodynamics (QCD) phase diagram remain incomplete, particularly at intermediate energies. This paper, ‘Physics Opportunities with a Fixed-Target Program at the Electron-Ion Collider’, proposes a complementary experimental program leveraging a fixed-target setup at the future Electron-Ion Collider (EIC) to address these limitations. By providing high-luminosity, systematic measurements across a broad range of nuclear targets, this program would uniquely link proton-nucleus and nucleus-nucleus collisions, establishing crucial baselines and complementing collider measurements for probing the QCD critical point and refining models of space radiation. Will this fixed-target approach unlock a more complete and unified understanding of QCD matter across diverse energy scales and nuclear environments?


Deconstructing the Hadronic Landscape

The fundamental strong force, responsible for binding quarks into protons and neutrons, and subsequently these nucleons into atomic nuclei – collectively known as hadronic matter – presents a continuing puzzle for physicists. Unlike electromagnetism, the strong force increases with distance, confining quarks and making calculations exceedingly difficult. Understanding its behavior is crucial not only for unraveling the structure of ordinary matter but also for deciphering the conditions present in extreme astrophysical environments like neutron stars and the early universe. Current theoretical models often struggle to accurately predict the properties of hadronic matter under varying densities and temperatures, necessitating innovative experimental approaches and refined computational techniques to map out this complex landscape and fully characterize the interactions within the nucleus. \text{Hadronic Matter} = \{ \text{protons, neutrons, mesons, baryons} \}

The intricate dance of protons and neutrons within atomic nuclei, governed by the strong force, presents a formidable challenge to conventional theoretical approaches. While models built upon established quantum mechanics successfully describe many nuclear properties, they falter when pushed to extremes – such as the immense pressures and temperatures found in neutron stars or during heavy-ion collisions. These conditions dramatically alter the interactions between nucleons, introducing complex many-body effects and potentially breaking down the very notion of individual protons and neutrons. Current computational limitations, coupled with the inherent complexity of accurately modeling the strong force \sim 10^{38} times stronger than gravity, mean that predicting nuclear behavior under such stress remains a significant frontier in physics. Consequently, a deeper understanding necessitates innovative theoretical frameworks and experimental techniques capable of probing the nuances of nuclear interactions at these previously inaccessible regimes.

Investigating the behavior of matter at extremely low temperatures and high densities – the realm of cold nuclear matter – demands innovative experimental techniques. Traditional methods prove insufficient to fully characterize the subtle interplay of forces within nuclei under these conditions, necessitating the development of new probes capable of penetrating the nuclear core. Scientists are particularly interested in identifying the conditions under which this cold nuclear matter might transition into a Quark-Gluon\ Plasma, a state where quarks and gluons are no longer confined within hadrons. These advanced probes, including high-energy heavy-ion collisions and precision measurements of nuclear structure, aim to map the phase diagram of nuclear matter and reveal the fundamental properties of this exotic state, offering insights into the very building blocks of the universe and the forces that govern them.

A potential ePIC fixed-target configuration, leveraging the hpDIRC and central/forward tracking detectors, positions a point-like target at <span class="katex-eq" data-katex-display="false">z = -{3290}</span> mm to enable forward detector-based measurements.
A potential ePIC fixed-target configuration, leveraging the hpDIRC and central/forward tracking detectors, positions a point-like target at z = -{3290} mm to enable forward detector-based measurements.

The Electron-Ion Collider: A New Lens on Nuclear Structure

The Electron-Ion Collider (EIC) will employ two distinct experimental approaches to investigate nuclear structure: collider mode and fixed-target mode. In collider mode, a high-energy electron beam collides with a beam of ions, maximizing the center-of-mass energy \sqrt{s} available to probe the nucleus. Conversely, fixed-target mode directs the electron beam onto a stationary target, offering complementary access to kinematic regions and facilitating measurements at lower energies. This dual approach allows the EIC to cover a broad range of energy scales and provide a comprehensive understanding of nuclear dynamics, exploiting the advantages of each technique to map the internal structure of nuclei with high-energy electron beams.

Analysis of collision products at the EIC will reveal the three-dimensional structure of nucleons and nuclei, including the distributions of quarks and gluons. These investigations will probe the strong force, formally described by Quantum Chromodynamics (QCD), by examining how the fundamental constituents interact and contribute to observable properties like nucleon spin and hadron masses. Measurements of particle production, particularly at varying momentum transfer Q^2 and Bjorken-x, will allow for the determination of Parton Distribution Functions (PDFs) and Generalized Parton Distributions (GPDs), providing a comprehensive understanding of the nucleon’s internal dynamics and the origin of its properties. Furthermore, studying the correlations between produced particles will provide insight into the saturation phenomenon predicted by QCD, where the gluon density becomes very high at small values of x.

The Electron-Ion Collider (EIC) will utilize detectors such as the ePIC Detector and the Zero Degree Calorimeter to characterize particle production resulting from high-energy collisions. Precise measurements will focus on key kinematic variables including transverse momentum p_T, which indicates the momentum of a particle perpendicular to the beam axis, and pseudorapidity η, a proxy for the particle’s scattering angle. The ePIC Detector, a silicon-based tracking and particle identification system, will provide detailed information on charged particles over a broad momentum range and angular acceptance. Complementing this, the Zero Degree Calorimeter will measure energy deposited by particles scattered at very small angles, providing crucial information about the initial state and the dynamics of the strong interaction.

The proposed fixed-target program at the Electron-Ion Collider is designed to explore collision energies in the \sqrt{s_{NN}} regime of 7 to 23 GeV. This energy range is currently under-explored by existing experimental facilities, creating a gap in our understanding of nuclear structure and the strong force. By utilizing a fixed-target configuration, the EIC can access these lower collision energies complementary to the collider mode, allowing for detailed investigation of phenomena such as the emergence of the nucleon spin, the saturation of gluon densities at low x , and the behavior of the quark-gluon plasma at initial stages of heavy-ion collisions. These measurements will provide crucial constraints on theoretical models and improve our understanding of strong interaction dynamics.

Representative <span class="katex-eq" data-katex-display="false">\sqrt{s_{NN}}</span> nucleon-nucleon center-of-mass energies and estimated instantaneous luminosities for proton-gold and gold-gold collisions at the EIC, assuming a 1 mm gold foil and a 10 mA effective beam current, demonstrate the potential for high-luminosity fixed-target experiments.
Representative \sqrt{s_{NN}} nucleon-nucleon center-of-mass energies and estimated instantaneous luminosities for proton-gold and gold-gold collisions at the EIC, assuming a 1 mm gold foil and a 10 mA effective beam current, demonstrate the potential for high-luminosity fixed-target experiments.

Decoding Nuclear Modifications: A Signal Within the Noise

Nuclear modification patterns refer to alterations in particle production rates observed in heavy-ion collisions compared to proton-proton collisions. The Electron-Ion Collider (EIC) is designed to systematically map these modifications across a wide range of kinematic regions, including momentum and pseudorapidity. Deviations from expected production rates – such as suppression or enhancement of certain particles – indicate interactions between the produced particles and the surrounding nuclear medium. These effects are quantified by nuclear modification factors, ratios of heavy-ion to proton-proton production cross-sections, and provide insights into the density and dynamics of the nuclear environment. Detailed study of these modifications will reveal how the presence of nucleons alters the fragmentation and propagation of produced hadrons, offering a comprehensive understanding of the strong force in nuclear matter.

The Drell-Yan process, involving the collision of a nucleon with a positron to produce a lepton-antilepton pair, and the subsequent detection of heavy flavor particles such as J/Psi mesons, provide a means to map the distribution of quarks and gluons within the nucleus. These processes are sensitive to the Parton Distribution Functions (PDFs) of the nucleus, allowing for the determination of the spatial and momentum distribution of partons. Specifically, the production rate and transverse momentum distribution of leptons from the Drell-Yan process, and the J/Psi meson, are directly related to the density of quarks and gluons at a given fraction of the nucleon’s momentum. By analyzing these distributions in heavy ion collisions, or with different nuclear targets, modifications to the nuclear PDFs relative to free proton PDFs can be quantified, revealing insights into the complex many-body dynamics within the nucleus.

Disentangling initial and final state effects is critical for accurately interpreting particle production measurements in nuclear collisions. Initial state effects encompass phenomena occurring before the collision itself, such as the momentum distribution of partons within the colliding nuclei and the effects of multiple nucleon-nucleon interactions. Final state effects refer to interactions that occur after the primary collision, including hadronization, energy loss of produced particles as they traverse the nuclear medium, and subsequent particle decays. By carefully controlling experimental parameters and employing specific kinematic selections, the EIC aims to isolate and quantify each of these contributions, thereby revealing the fundamental dynamics of particle production within the complex nuclear environment. Accurate separation of these effects is essential for extracting precise measurements of nuclear parton distribution functions and understanding the mechanisms governing particle formation and propagation.

Precise determination of Nuclear Parton Distribution Functions (nPDFs) is essential for accurate modeling of nuclear structure and the interpretation of high-energy nuclear collisions. Unlike proton PDFs which are well-constrained by deep inelastic scattering and collider data, nPDFs suffer from limited experimental constraints and rely heavily on extrapolations from free nucleon PDFs and theoretical models. The Electron-Ion Collider (EIC) will provide the necessary data to systematically map nPDFs across a wide range of momentum fractions and Bjorken-x values, particularly at low-x and high-x regions where uncertainties are currently largest. Improved nPDFs will refine predictions for observables in heavy-ion collisions, such as the suppression of particle production, and provide insights into the emergence of collective behavior in nuclear matter. Furthermore, accurate nPDFs are critical for quantifying the modifications to parton distributions induced by nuclear effects like shadowing, saturation, and gluon recombination.

Simulations for the Electron-Ion Collider (EIC) indicate that measurements of particle production will be accessible up to a target momentum fraction, denoted as x_2, of 0.4. This accessibility is determined by the projected kinematic coverage of the EIC detectors and the expected range of momentum transfer during collisions. Reaching x_2 = 0.4 is significant as it allows probing a substantial portion of the nucleon’s momentum space, providing data crucial for mapping the distribution of quarks and gluons within the nucleus at intermediate to high momentum scales. The demonstrated accessibility at this value validates the EIC’s potential to constrain Nuclear Parton Distribution Functions (nPDFs) and refine theoretical models of nuclear structure with high precision.

Simulations of <span class="katex-eq" data-katex-display="false">p+p</span> collisions at <span class="katex-eq" data-katex-display="false">\sqrt{s}=19.4</span> GeV using the ePIC detector demonstrate the transverse momentum (<span class="katex-eq" data-katex-display="false">p_{T}</span>) distribution of charged pions as a function of pseudorapidity (η), utilizing a 1.7 T magnetic field and requiring at least four tracking hits.
Simulations of p+p collisions at \sqrt{s}=19.4 GeV using the ePIC detector demonstrate the transverse momentum (p_{T}) distribution of charged pions as a function of pseudorapidity (η), utilizing a 1.7 T magnetic field and requiring at least four tracking hits.

Mapping the QCD Phase Diagram: Probing the Extremes

The search for the QCD critical point represents a central goal of the upcoming Electron-Ion Collider (EIC) program, building upon the foundation laid by the Beam Energy Scan. Nuclear matter, under extreme temperatures and densities, isn’t simply a collection of individual protons and neutrons, but rather a fluid exhibiting a complex phase structure-transitioning between a state of confined quarks and gluons to one where these particles are deconfined. The EIC, by colliding electrons with heavy ions, aims to precisely map this phase diagram, identifying the conditions under which this transition occurs. Understanding the location of the QCD critical point-the endpoint of the transition between hadronic and quark-gluon plasma phases-requires probing the fluctuations in the system; these fluctuations are expected to be maximized at the critical point, acting as a unique signature. Through detailed measurements of particle production and correlations, the EIC promises to reveal the fundamental nature of this transition and the properties of matter under conditions not found anywhere else in the universe except in the cores of neutron stars and the very first moments after the Big Bang.

The search for the QCD critical point relies heavily on identifying subtle fluctuations in the density of nuclear matter, and researchers are employing statistical tools known as net-proton cumulants to achieve this. These cumulants aren’t simply averages; they quantify the correlations between protons and anti-protons, revealing how the number of protons fluctuates around its mean value. A key principle suggests that as a system approaches a critical point – a specific temperature and density where a phase transition occurs – these fluctuations should dramatically increase and exhibit characteristic scaling behavior. By meticulously measuring these cumulants across a range of collision energies at the EIC, scientists aim to detect these telltale signs of criticality, effectively mapping the boundary between the quark-gluon plasma and hadronic matter.

The study of nuclear matter under extreme conditions – temperatures and densities far exceeding those found in everyday life – offers crucial insights into some of the most fascinating and energetic phenomena in the universe. Investigations into the quark-gluon plasma, a state of matter theorized to have existed shortly after the Big Bang, directly inform models of neutron stars, incredibly dense remnants of collapsed stars. These stellar objects represent natural laboratories for probing the equation of state of matter at extreme densities, while collisions of heavy ions, recreated in terrestrial experiments, mimic the conditions present in both neutron star mergers and the early universe. By bridging the gap between these seemingly disparate realms, researchers gain a more complete understanding of the fundamental forces governing matter and its behavior under the most extreme conditions imaginable, potentially revealing new states of matter and deepening our knowledge of astrophysical processes.

Investigations at the Electron-Ion Collider extend beyond nuclear physics, offering crucial insights into the pervasive challenge of space radiation. Galactic cosmic rays, high-energy particles originating from outside our solar system, pose significant risks to astronauts and spacecraft components. The EIC’s detailed study of \text{Cosmic Ray Interactions} – how these particles collide with matter – coupled with an understanding of \text{Radiation Transport} , the mechanisms by which secondary particles are generated and propagate, will allow for more accurate modeling of the radiation environment in deep space. This improved understanding is critical for developing effective shielding strategies and mitigating the hazards posed by space radiation, ultimately enabling safer and more sustainable long-duration space exploration.

The future Electron-Ion Collider is projected to achieve exceptionally high collision rates, quantified by luminosity, to probe the fundamental structure of matter. Specifically, proton-gold (p+Au) collisions are anticipated to reach a luminosity exceeding 10^{36} \text{ cm}^{-2} \text{ s}^{-1}, while collisions involving gold nuclei (Au+Au) are expected to surpass 10^{38} \text{ cm}^{-2} \text{ s}^{-1}. These remarkably intense collision rates are crucial for creating a statistically significant number of events, allowing scientists to precisely measure rare phenomena and map the quantum chromodynamics phase diagram. The increased data volume facilitated by this luminosity will enable detailed studies of the strong force and the behavior of nuclear matter under extreme conditions, pushing the boundaries of current understanding in both nuclear physics and astrophysics.

The exploration of the QCD phase diagram at the future Electron-Ion Collider will benefit from an exceptionally broad kinematic reach, notably in the measurement of charged pions. Detectors are designed to reliably track these particles up to a pseudorapidity of η ~4, a significant extension beyond the capabilities of many current heavy-ion facilities. This expansive coverage is crucial for fully reconstructing the particle multiplicity distributions arising from nuclear collisions. By capturing pions over such a wide range of rapidities, researchers can obtain a more complete picture of the particle production mechanisms and better characterize the properties of the hot, dense matter created in these events. Such data will be instrumental in disentangling the signals of the QCD critical point and mapping the transition between phases of nuclear matter with unprecedented precision, while also improving the modeling of Cosmic Ray Interactions and Radiation Transport.

Simulations of <span class="katex-eq" data-katex-display="false">p+p</span> collisions at <span class="katex-eq" data-katex-display="false">\sqrt{s}=19.4</span> GeV using the ePIC detector demonstrate the transverse momentum (<span class="katex-eq" data-katex-display="false">p_{T}</span>) distribution of charged pions as a function of pseudorapidity (η), utilizing a 1.7 T magnetic field and requiring at least four tracking hits.
Simulations of p+p collisions at \sqrt{s}=19.4 GeV using the ePIC detector demonstrate the transverse momentum (p_{T}) distribution of charged pions as a function of pseudorapidity (η), utilizing a 1.7 T magnetic field and requiring at least four tracking hits.

The pursuit detailed within this study exemplifies a systematic dismantling of established observational boundaries. Much like probing the limits of known physics, the proposed fixed-target program at the EIC isn’t simply about confirming existing models; it’s about deliberately stressing them. This approach, pushing beyond collider measurements to investigate cold nuclear matter and map the QCD phase diagram, mirrors an ‘exploit of comprehension’. As Galileo Galilei observed, “You cannot teach a man anything; you can only help him discover it himself.” The researchers aren’t delivering answers, but creating the conditions for discovery by challenging conventional experimental frameworks and demanding a deeper understanding of nuclear structure.

Beyond the Collision

The proposition of a fixed-target program at the EIC isn’t merely additive; it’s a deliberate disruption. Collider experiments, by their nature, seek the spectacular – the rare, high-energy events that scream for attention. But reality often whispers in the mundane, in the subtle shifts of probability within seemingly uniform matter. This approach attempts to eavesdrop on those whispers, to systematically dismantle assumptions about nuclear structure and the conditions governing the QCD phase diagram. The real challenge lies not in building the experiment, but in confronting what it might not reveal – the limits of current theoretical frameworks, the inherent unpredictability of complex systems.

The stated goals – probing cold nuclear matter, mapping the QCD phase diagram – are, in a sense, misdirections. The true objective is to stress-test the Standard Model at the edges of its competence. To push beyond established parameters, and to force the development of new tools for interpretation. The breadth of energies and polarization possibilities offered by this fixed-target approach isn’t about answering existing questions, but about formulating better ones. It’s an invitation to discover the flaws in the current understanding.

Ultimately, the success of this endeavor won’t be measured in published results, but in the quality of the failures. Because it is in the anomalies, the unexpected null results, and the irreconcilable discrepancies that genuine progress resides. The task ahead isn’t to confirm what is known, but to systematically, elegantly, and relentlessly deconstruct it.


Original article: https://arxiv.org/pdf/2603.00265.pdf

Contact the author: https://www.linkedin.com/in/avetisyan/

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2026-03-03 21:53