National Centre for Nuclear Research
We study lepto- and hadroproduction of a heavy-quark pair in the ITMD factorization framework for dilute-dense collisions. Due to the presence of a nonzero quark mass and/or nonzero photon virtuality, new contributions appear compared to the cases of photo- and hadroproduction of dijets, for which the ITMD framework was originally derived. The extra terms are sensitive to gluons that are not fully linearly polarized. At small xx those gluons emerge only when saturation effects are taken into account, and in a proper way. As a result, in linear small-xx frameworks where gluon are fully linearly polarized, such contributions are absent. We show however that they are not always negligible, even for large gluon transverse momentum, due to the behavior of the off-shell hard factors.
We present ELENA (EvaLuator of tunnElliNg Actions), an open-source Python package designed to compute the full evolution of first-order phase transitions in the early Universe generated by particle physics models, taking into account several refinements that go beyond commonly assumed simplifications. The core of ELENA is based on a vectorized implementation of the tunnelling potential formalism, which allows for a fast computation of the finite-temperature tunnelling action. This, in turn, enables the sampling of the full range of temperatures where two phases coexist and the use of integral expressions that track the complete evolution of the transition, providing a comprehensive picture of it. In addition, ELENA provides all the tools to compute the resulting stochastic gravitational waves spectrum, allowing for the full chain of computations - from the Lagrangian parameter inputs to the final gravitational waves spectrum - in a fast and self-contained implementation.
While the James Webb Space Telescope (JWST) now allows identifying quiescent galaxies (QGs) out to early epochs, the photometric selection of quiescent galaxy candidates (QGCs) and the derivation of key physical quantities are highly sensitive to the assumed star-formation histories (SFHs). We aim to quantify how the inclusion of JWST/MIRI data and different SFH models impacts the selection and characterisation of QGCs. We test the robustness of the physical properties inferred from the spectral energy distribution (SED) fitting, such as M*, age, star formation rate (SFR), and AV, and study how they impact the quiescence criteria of the galaxies across cosmic time. We perform SED fitting for ~13000 galaxies at z<6 from the CEERS/MIRI fields with up to 20 optical-mid infrared (MIR) broadband coverage. We implement three SFH prescriptions: flexible delayed, NonParametric, and extended Regulator. For each model, we compare results obtained with and without MIRI photometry and dust emission models. We evaluate the impact of these configurations on the number of candidate QGCs, selected based on rest UVJ colours, sSFR and main-sequence offset, and on their key physical properties such as M*, AV, and stellar ages. The number of QGCs selected varies significantly with the choice of SFH from 171 to 224 out of 13000 galaxies, depending on the model. This number increases to 222-327 when MIRI data are used (up to ~45% more QGCs). This enhancement is driven by improved constraints on dust attenuation and M*. We find a strong correlation between AV and M*, with massive galaxies (M*~10^11 M\odot) being 1.5-4.2 times more attenuated in magnitude than low-mass systems (M*~10^9 M\odot), depending on SFH. Regardless of the SFH assumption, ~13% of QGCs exhibit significant attenuation (AV > 0.5) in support of recent JWST studies challenging the notion that quiescent galaxies are uniformly dust-free.
We present three rare and striking extragalactic radio sources discovered through visual inspection of low-frequency continuum maps from LoTSS DR2 and TGSS by the RAD@home citizen-science collaboratory. The first, RAD J131346.9+500320, is the first clear Odd Radio Circle (ORC) identified in LoTSS. At photometric zz \sim 0.94, it hosts a pair of intersecting rings of ~300 kpc diameter, embedded in diffuse emission extending over ~800 kpc, making it both the most distant and most powerful ORC reported to date. Its steep spectrum α54144=1.22±0.15\alpha_{54}^{144}=1.22\pm0.15) points to a relic synchrotron origin. The second object, RAD J122622.6+640622, is a ~865 kpc giant radio galaxy whose southern jet is abruptly deflected, inflating a ~100 kpc limb-brightened ring, while the northern jet terminates in a compact hotspot-like feature. The third, RAD J142004.0+621715 (~440 kpc), shows a comparable ring at the end of its northern filamentary jet, along with a secondary filament parallel to its southern jet. All three systems lie in 1014M\sim10^{14}M_\odot clusters or group-scale haloes, suggesting that environmental density gradients and possible jet-galaxy interactions play a central role in shaping these ring morphologies. These discoveries expand the zoo of extragalactic radio morphologies, highlight the diversity of pathways that can generate ring-like synchrotron structures, and demonstrate the continuing importance of human pattern recognition in identifying rare sources that escape current automated pipelines.
We investigate quantum entanglement in high-energy 222\to 2 scalar scattering, where the scalars are characterized by an internal flavor quantum number acting like a qubit. Working at the 1-loop order in perturbation theory, we build the final-state density matrix as a function of the scattering amplitudes connecting the initial to the outgoing state. In this construction, the unitarity of the SS-matrix is guaranteed at the required order by the optical theorem. We consider the post-scattering entanglement between the momentum and flavor degrees of freedom of the final-state particles, as well as the entanglement of the two-qubit flavor subsystem. In each case we identify the couplings of the scalar potential that can generate, destroy, or transfer entanglement between different bipartite subspaces of the Hilbert space.
This research from NCBJ clarifies the necessity of edge modes in classical gauge theories with boundaries by demonstrating they satisfy the degeneracy condition of the presymplectic form for field-independent gauge transformations. It also unifies the treatment of boundary-changing spacetime symmetries in both Yang-Mills theory and gravity using an extended phase space formalism, identifying the spacetime embedding map as a gravitational edge mode that resolves flux issues and ensures phase space degeneracy.
The evidence of a Stochastic Gravitational Wave Background (SGWB) in the nHz frequency range is posed to open a new window on the Universe. A preferred explanation relies on a supercooled first order phase transition at the 100 MeV - GeV scale. In this article, we address the feasibility going from the particle physics model to the production of the gravitational waves. We take a minimal approach for the dark sector model introducing the fewest ingredients required, namely a new U(1) gauge group and a dark scalar that dynamically breaks the symmetry. Supercooling poses challenges in the analysis that put under question the feasibility of this explanation: we address them, going beyond previous studies by carefully considering the effects of a vacuum domination phase and explicitly tracking the phase transition from its onset to its completion. We find that the proposed model can successfully give origin to the observed PTA SGWB signal. The strong supercooling imposes a correlation between the new gauge coupling and the scalar quartic one, leading to a significant hierarchy between the (heavier) gauge boson and the dark scalar. Ultimately, information on phase transitions from SGWB observations could provide a direct probe of the microphysics of the Early Universe and be used to guide future searches of dark sector in laboratories.
Gamma-Ray Bursts (GRBs), observed at high-z, are probes of the evolution of the Universe and can be used as cosmological tools. Thus, we need correlations with small dispersion among key parameters. To reduce such a dispersion, we mitigate gaps in light curves (LCs), including the plateau region, key to building the two-dimensional Dainotti relation between the end time of plateau emission (Ta) and its luminosity (La). We reconstruct LCs using nine models: Multi-Layer Perceptron (MLP), Bi-Mamba, Fourier Transform, Gaussian Process-Random Forest Hybrid (GP-RF), Bidirectional Long Short-Term Memory (Bi-LSTM), Conditional GAN (CGAN), SARIMAX-based Kalman filter, Kolmogorov-Arnold Networks (KANs), and Attention U-Net. These methods are compared to the Willingale model (W07) over a sample of 521 GRBs. MLP and Attention U-Net outperform other methods, with MLP reducing the plateau parameter uncertainties by 37.2% for log Ta, 38.0% for log Fa, and 41.2% for alpha (the post-plateau slope in the W07 model), achieving the lowest 5-fold cross-validation (CV) mean squared error (MSE) of 0.0275. Attention U-Net achieved the lowest uncertainty of parameters, a 37.9% reduction in log Ta, a 38.5% reduction in log Fa and a 41.4% reduction in alpha, but with a higher MSE of 0.134. Although Attention U-Net achieves the largest uncertainty reduction, the MLP attains the lowest test MSE while maintaining comparable uncertainty performance, making it the more reliable model. The other methods yield MSE values ranging from 0.0339 to 0.174. These improvements in parameter precision are needed to use GRBs as standard candles, investigate theoretical models, and predict GRB redshifts through machine learning.
We present a statistical study of spatially resolved chemical enrichment in 18 main-sequence galaxies at z=4z=4--6, observed with \jwst/NIRSpec IFU as part of the ALPINE-CRISTAL-\jwst\ survey. Performing an optimized reduction and calibration procedure, including local background subtraction, light-leakage masking, stripe removal, and astrometry refinement, we achieve robust emission-line mapping on kiloparsec scales. Although line-ratio distributions vary across galaxies in our sample, we generally find mild central enhancements in [O\,\textsc{iii}]/Hβ\beta, [O\,\textsc{ii}]/[O\,\textsc{iii}], [S\,\textsc{ii}]6732_{6732}/[S\,\textsc{ii}]6718_{6718}, Hα\alpha/Hβ\beta, and LHα/LUVL_{\rm H\alpha}/L_{\rm UV}, consistent with elevated electron density, dust obscuration, and bursty star formation accompanied by reduced metallicity and ionization parameter. These features point to inside-out growth fueled by recent inflows of pristine gas. Nevertheless, the median metallicity gradient is nearly flat over a few kpc scale, Δlog(O/H)=0.02±0.01\Delta \log({\rm O/H}) = 0.02 \pm 0.01 dex kpc1^{-1}, implying efficient chemical mixing through inflows, outflows, and mergers. From pixel-by-pixel stellar and emission-line characterizations, we further investigate the resolved Fundamental Metallicity Relation (rFMR). Metallicity is described by a fundamental plane with stellar mass and SFR surface densities, but with a stronger dependence on ΣSFR\Sigma_{\rm SFR} than seen in local galaxies. Our results indicate that the regulatory processes linking star formation, gas flows, and metal enrichment were already vigorous \sim1 Gyr after the Big Bang, producing the nearly flat metallicity gradient and a stronger coupling between star formation and metallicity than observed in evolved systems in the local universe.
In this Letter, we use the latest results from the Dark Energy Spectroscopic Instrument (DESI) survey to measure the Hubble constant. Baryon acoustic oscillation (BAO) observations released by the DESI survey, allow us to determine H0H_0 from the first principles. Our method is purely data-driven and relies on unanchored luminosity distances reconstructed from SN Ia data and H(z)H(z) reconstruction from cosmic chronometers. Thus it circumvents calibrations related to the value of the sound horizon size at the baryon drag epoch or intrinsic luminosity of SN Ia. We find H0=68.40.8+1.0 km s1 Mpc1H_0=68.4^{+1.0}_{-0.8}~{\rm km~s^{-1}~Mpc^{-1}} at 68% C.L., which provides the Hubble constant at an accuracy of 1.3% with minimal assumptions. Our assessments of this fundamental cosmological quantity using the BAO data spanning the redshift range z=0.512.33z=0.51-2.33 agree very well with Planck's results and TRGB results within 1σ1\sigma. This result is still in a 4.3σ4.3\sigma tension with the results of the Supernova H0 for the Equation of State (SH0ES).
We present morphological classifications of over 41,000 galaxies out to zphot2.5z_{\rm phot}\sim2.5 across six square degrees of the Euclid Deep Field North (EDFN) from the Hawaii Twenty Square Degree (H20) survey, a part of the wider Cosmic Dawn survey. Galaxy Zoo citizen scientists play a crucial role in the examination of large astronomical data sets through crowdsourced data mining of extragalactic imaging. This iteration, Galaxy Zoo: Cosmic Dawn (GZCD), saw tens of thousands of volunteers and the deep learning foundation model Zoobot collectively classify objects in ultra-deep multiband Hyper Suprime-Cam (HSC) imaging down to a depth of mHSCi=21.5m_{HSC-i} = 21.5. Here, we present the details and general analysis of this iteration, including the use of Zoobot in an active learning cycle to improve both model performance and volunteer experience, as well as the discovery of 51 new gravitational lenses in the EDFN. We also announce the public data release of the classifications for over 45,000 subjects, including more than 41,000 galaxies (median zphotz_{\rm phot} of 0.42±0.230.42\pm0.23), along with their associated image cutouts. This data set provides a valuable opportunity for follow-up imaging of objects in the EDFN as well as acting as a truth set for training deep learning models for application to ground-based surveys like that of the newly operational Vera C. Rubin Observatory.
The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from 39^{39}Ar beta decays and is suppressed using pulseshape discrimination (PSD). We use two types of PSD algorithm: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the charge of a single photoelectron, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulseshape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected.
Wuhan University of TechnologyWuhan UniversityChinese Academy of Sciences logoChinese Academy of SciencesCarnegie Mellon University logoCarnegie Mellon UniversityBudker Institute of Nuclear Physics SB RASSichuan UniversityGyeongsang National UniversityFudan University logoFudan UniversityUniversity of Science and Technology of China logoUniversity of Science and Technology of ChinaBeihang University logoBeihang UniversityShanghai Jiao Tong University logoShanghai Jiao Tong UniversityNanjing University logoNanjing UniversityHunan Normal UniversityGuangzhou UniversityCentral South UniversityNankai UniversityBeijing Jiaotong University logoBeijing Jiaotong UniversityPeking University logoPeking UniversityJoint Institute for Nuclear ResearchUniversity of Minnesota logoUniversity of MinnesotaSouth China Normal UniversitySouthwest UniversityAnhui UniversityPurdue University logoPurdue UniversityUppsala UniversityUniversity of LiverpoolGuangxi Normal UniversityJilin UniversityUniversity of SheffieldCentral China Normal UniversitySouthern University of Science and Technology logoSouthern University of Science and TechnologyShandong University logoShandong UniversityNovosibirsk State UniversityYunnan UniversityLanzhou UniversityNorthwest UniversityIndian Institute of Technology MadrasEast China Normal UniversityUniversity of South ChinaUniversity of JinanUniversity of Groningen logoUniversity of GroningenNanjing Normal UniversityYantai UniversityGuangxi UniversityGSI Helmholtzzentrum fuer Schwerionenforschung GmbHFuzhou UniversitySuranaree University of TechnologyINFN, Sezione di TorinoAkdeniz UniversityLinyi UniversityINFN, Laboratori Nazionali di FrascatiShandong Institute of Advanced TechnologyHenan Normal UniversityUniversit`a di TorinoNational Centre for Nuclear ResearchInstitute of Nuclear Physics, Polish Academy of SciencesUniversity of the PunjabShandong Normal UniversityYunnan Normal UniversityLiaoning Normal UniversityChina University of Geosciences (Wuhan)University of Science and Technology LiaoningHelmholtz-Institut MainzBeijing Institute of Petrochemical TechnologyP.N. Lebedev Physical Institute of the Russian Academy of SciencesLiaocheng UniversityJustus-Liebig-Universitaet GiessenUniversitaet Duisburg-EssenJohannes Gutenberg-Universitaet MainzShaanxi Key Laboratory of Quantum Information and Quantum Optoelectronic DevicesRuhr Universitaet BochumState Key Laboratory of Particle Detection and Electronics, USTCUniversità di FerraraINFN-Sezione di Ferrara
Based on the (2712.4±14.4)×106(2712.4\pm14.4)\times 10^{6} ψ(3686)\psi(3686) events collected with the BESIII detector, we present a high-precision study of the π+π\pi^+\pi^- mass spectrum in ψ(3686)π+πJ/ψ\psi(3686)\rightarrow\pi^{+}\pi^{-}J/\psi decays. A clear resonance-like structure is observed near the π+π\pi^+\pi^- mass threshold for the first time. A fit with a Breit-Wigner function yields a mass of 285.6±2.5 MeV/c2285.6\pm 2.5~{\rm MeV}/c^2 and a width of 16.3±0.9 MeV16.3\pm 0.9~{\rm MeV} with a statistical significance exceeding 10σ\sigma. To interpret the data, we incorporate final-state interactions (FSI) within two theoretical frameworks: chiral perturbation theory (ChPT) and QCD multipole expansion (QCDME). ChPT describes the spectrum above 0.3 GeV/c2c^2 but fails to reproduce the threshold enhancement. In contrast, the QCDME model, assuming the ψ(3686)\psi(3686) is an admixture of S- and D-wave charmonium, reproduces the data well. The pronounced dip near 0.3 GeV/c2c^2 offers new insight into the interplay between chiral dynamics and low-energy QCD.
CNRS logoCNRSUniversity of Amsterdam logoUniversity of AmsterdamNational Central UniversityNew York University logoNew York UniversityNikhefUniversity of MelbourneINFN logoINFNUniversity of WarsawJoint Institute for Nuclear ResearchUniversity of GranadaUniversity of GenoaSorbonne Université logoSorbonne UniversitéTechnical University of Munich logoTechnical University of MunichLeiden University logoLeiden UniversityUniversity of SheffieldUtrecht UniversityCadi Ayyad UniversityUniversity of JohannesburgINAFUnited Arab Emirates UniversityUniversity of South DakotaNCSR DemokritosLebedev Physical InstituteUniversity of ValenciaEberhard-Karls-Universität TübingenComenius UniversityGeorgian Technical UniversityUniversità di BariNational Centre for Nuclear ResearchWestern Sydney UniversityUniversitat Politécnica de ValénciaMohammed V UniversityInstitut de Physique des 2 Infinis de LyonUniversità di FirenzeUniversity of SalentoIFICUniversity of AthensUniversità degli Studi di Bari Aldo MoroPushchino Radio Astronomy ObservatoryLUPMLPC-CaenIFIN-HHChouaïb Doukkali UniversityInstitute of Experimental PhysicsTechnical University of KošiceUniversit di CataniaUniversité Sidi Mohamed Ben AbdellahRoyal Netherlands Institute for Sea ResearchUniversité Mohammed IerInstitut universitaire de technologie de Nantes* North–West UniversityUniversit degli Studi di FerraraUniversit de ParisUniversit Grenoble AlpesUniversit degli Studi di GenovaAix-Marseille Universit",Universit di SalernoUniversit Roma TreUniversit Paris CitUniversit La SapienzaUniversit de StrasbourgNantes UniversitUniversit di PadovaUniversit degli Studi di FirenzeUniversit degli Studi di Napoli Federico IIUniversit Di Bologna
Context: The detection of the highest energy neutrino observed to date by KM3NeT, with an estimated energy of 220 PeV, opens up new possibilities for the study and identification of the astrophysical sources responsible for a diffuse flux of such ultra-high-energy neutrinos, among which gamma-ray bursts are longstanding candidates. Aims: Based on the event KM3-230213A, we derive constraints on the baryon loading and density of the surrounding environment in models of blastwaves in long-duration gamma-ray bursts. Methods: We compute the diffuse flux from gamma-ray burst blastwaves, either expanding in a constant density interstellar medium or developing in a radially decreasing density of a wind-like environment surrounding the gamma-ray burst progenitor star, by taking into account the expected neutrino spectra and luminosity function. We use a Poisson likelihood method to constrain the blastwave model parameters by calculating the expected number of neutrino events within the 90% confidence level energy range of KM3-230213A and by using the joint exposure of KM3NeT/ARCA, IceCube and Pierre Auger. Results: We constrain the baryon loading to be {392,131,39,13}\leq \{392, 131, 39, 13\} at 90% confidence level, which is inversely proportional to a varying interstellar medium particle density of {1,3,10,30}\{1, 3, 10, 30\} cm3^{-3}. In the wind-like environment case, the baryon loading is {20,50,100}\leq \{20, 50, 100\} at 90% confidence level, which is proportional to the sixth power of a varying density parameter of {0.05,0.06,0.07}\{0.05, 0.06, 0.07\}.
We provide a systematic framework for solving the initial value problem for relativistic hydrodynamics formulated as a gradient expansion. Secular growth is handled by a suitable covariant resummation scheme, which reorganises the degrees of freedom at each order in the expansion while preserving the sum. Our scheme can be applied to any order in the gradient expansion; we provide the explicit formulation at first and second orders. When working to first order, we find that the BDNK equations of motion emerge as an intermediate step in a calculation performed in the Landau frame. We show that non-hydrodynamic modes appear only in such intermediate calculations and cancel when evaluating solutions to the required order. Our procedure does not introduce any other fields or require any additional initial data beyond those appearing in the theory of ideal fluids.
The production of light nuclei in relativistic heavy-ion collisions is well described by both the thermal model, where light nuclei are in equilibrium with hadrons of all species present in a fireball, and by the coalescence model, where light nuclei are formed due to final-state interactions after the fireball decays. We present and critically discuss the two models and further on we consider two proposals to falsify one of the models. The first proposal is to measure a yield of exotic nuclide 4Li^4{\rm Li} and compare it to that of 4He^4{\rm He}. The ratio of yields of the nuclides is quite different in the thermal and coalescence models. The second proposal is to measure a hadron-deuteron correlation function which carries information whether a deuteron is emitted from a fireball together with all other hadrons, as assumed in the thermal model, or a deuteron is formed only after nucleons are emitted, as in the coalescence model. The p ⁣ ⁣3Hep\! -\!^3{\rm He} correlation function is of interest in context of both proposals: it is needed to obtain the yield of 4Li^4{\rm Li} which decays into pp and 3He^3{\rm He}, but the correlation function can also tell us about an origin of 3He^3{\rm He}.
We clarify the connection between attractor solutions known from studies of Bjorken flow in conformal models of relativistic fluid dynamics and the more general description of attractors as submanifolds in phase space. We show how to determine sections of the attractor on slices of constant proper time, and point out that in conformal models one may choose a parametrisation of the extended phase space such that the intersection of the attractor with a slice of constant proper time is the same on all slices. In consequence, it is possibleto project these intersections and one finds that the result reproduces the attractor solution. This projection allows for an expressive picture of hydrodynamisation, but the attractor can be equally well described without taking advantage of this convenience. An immediate implication of these observations is that conformal symmetry does not play a significant role in the emergence of early-time attraction. We illustrate this by describing the hydrodynamic attractor in a simple model where conformal symmetry is broken by the equation of state. Our findings can be applied to studies of hydrodynamic attractors in more general situations, also beyond the context of quark-gluon plasma dynamics.
This research constructs an all-order transseries for a generating function in a U(1) symmetric, integrable quantum mechanical system using the complexified path integral and Lefschetz thimble method. It demonstrates that this transseries, which includes both perturbative and non-perturbative contributions, exactly matches the generating function obtained independently from the operator formalism.
The PRObabilistic Value-Added Bright Galaxy Survey (PROVABGS) catalog will provide measurements of galaxy properties, such as stellar mass (MM_*), star formation rate (SFR{\rm SFR}), stellar metallicity (ZMWZ_{\rm MW}), and stellar age (tage,MWt_{\rm age, MW}), for >10 million galaxies of the DESI Bright Galaxy Survey. Full posterior distributions of the galaxy properties will be inferred using state-of-the-art Bayesian spectral energy distribution (SED) modeling of DESI spectroscopy and Legacy Surveys photometry. In this work, we present the SED model, Bayesian inference framework, and methodology of PROVABGS. Furthermore, we apply the PROVABGS SED modeling on realistic synthetic DESI spectra and photometry, constructed using the L-GALAXIES semi-analytic model. We compare the inferred galaxy properties to the true galaxy properties of the simulation using a hierarchical Bayesian framework to quantify accuracy and precision. Overall, we accurately infer the true MM_*, SFR{\rm SFR}, ZMWZ_{\rm MW}, and tage,MWt_{\rm age, MW} of the simulated galaxies. However, the priors on galaxy properties induced by the SED model have a significant impact on the posteriors. They impose a {\rm SFR}{&gt;}10^{-1} M_\odot/{\rm yr} lower bound on SFR{\rm SFR}, a 0.3{\sim}0.3 dex bias on logZMW\log Z_{\rm MW} for galaxies with low spectral signal-to-noise, and t_{\rm age, MW} &lt; 8\,{\rm Gyr} upper bound on stellar age. This work also demonstrates that a joint analysis of spectra and photometry significantly improves the constraints on galaxy properties over photometry alone and is necessary to mitigate the impact of the priors. With the methodology presented and validated in this work, PROVABGS will maximize information extracted from DESI observations and provide a probabilistic value-added galaxy catalog that will extend current galaxy studies to new regimes and unlock cutting-edge probabilistic analyses.
The failure to calculate the vacuum energy is a central problem in theoretical physics. Presumably the problem arises from the insistent use of effective field theory reasoning in a context that is well beyond its intended scope. If one follows this path, one is led inevitably to statistical or anthropic reasoning for observations. It appears that a more palatable resolution of the vacuum energy problem requires some form of UV/IR feedback. In this paper we take the point of view that such feedback can be thought of as arising by defining a notion of quantum space-time. We reformulate the regularized computation of vacuum energy in such a way that it can be interpreted in terms of a sum over elementary phase space volumes, that we identify with a ground state degeneracy. This observation yields a precise notion of UV/IR feedback, while leaving a scale unfixed. Here we argue that holography can be thought to provide a key piece of information: we show that equating this microscopic ground state degeneracy with macroscopic gravitational entropy yields a prediction for the vacuum energy that can easily be consistent with observations. Essentially, the smallness of the vacuum energy is tied to the large size of the Universe. We discuss how within this scenario notions of effective field theory can go so wrong.
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