The 41st annual IAP symposyum aims at providing an overview of research on cosmological inflation. This field is in full swing, with numerous emerging research themes, on theoretical, computational and observational grounds. Two main axes can be distinguished: precision physics, aiming to probe inflation on cosmological scales (with CMB and LSS observations), searching for fine effects such as primordial features and non-Gaussianities, effectively using inflation as a giant particle collider, and more generally as a laboratory for fundamental physics. The other axis concerns more exploratory physics: through the study of the stochastic gravitational-wave background and primordial black holes, gravitational-wave astronomy allows us to probe the late stage of the inflation, the physics of which is completely unknown.
The colloquium will bring together theoreticians, computational physicists and observers to review recent progress and open questions pertaining to the field, notably concerning the cosmological collider, cosmological bootstrap, non-perturbative formalisms, loop effects, open effective theories, constraints from the CMB and the Large-Scale Structure, field-level inference, gravitational-wave backgrounds, primordial black holes, simulations of inflation.
Invited speakers: Adam Andrews, Chiara Animali, Josu Aurrekoetxea, Mario Ballardini, Richard Bond, Matteo Braglia, Cliff Burgess, Angelo Caravano, Thomas Colas, Fabio Finelli, Jacopo Fumagalli, Juan Garcia-Bellido, Hayden Lee, Gonzalo Palma, Oliver Philcox, Shi Pi, Yuko Urakawa, Zhong-Zhi Xianyu, David Wands.
Registration: the number of on-site participants is limited to 130 due to the capacity of the amphitheatre. Participation in this event is thus moderated and instructions will be given to accepted participants for the payment of registration fees.
Talks and posters: the deadline for submission of an abstract for a contributed talk or a poster is September 28. Contributed talks last 15 mins including questions and are only for on-site participants. There will be a session of posters presentation.
Registration fees of 300 euros cover a welcome cocktail, coffee breaks and a dinner cruise on the Seine. Registration fees for online participants amount to 50 euros.
Conference dinner: we will have a dinner cruise on the Seine on Wednesday 3rd, from 8.15pm to 11pm, aboard the Capitaine Fracasse.
Any email about accommodation you could receive is a scam!
SOC: Silvia Galli, Guilhem Lavaux, Jérôme Martin, Lucas Pinol, Sébastien Renaux-Petel (chair), Vincent Vennin
LOC: Nathan Belrhali, Valérie Bona, Emily Diomat, Christophe Gobet, Jean Mouette, Ketia Musau, Arthur Poisson, Sébastien Renaux-Petel
Support: this operation was supported by the « action thématique » Cosmology-Galaxies (ATCG) of the CNRS/INSU PN Astro, the Initiative physique des infinis and the Fédération Recherche Interactions Fondamentales (FRIF).


The scalar spectral index, ns, plays a central role in testing inflationary models, with its precise value shaping theoretical and observational priorities. Recent analyses combining the latest cosmic microwave background (CMB) and baryon acoustic oscillation (BAO) data suggest a shift toward higher ns values compared to the Planck results. This comes with implications for inflation; previously preferred models appear to be now disfavoured by the data (>2 sigma). In this talk, I explore how this shift in ns arises due to differences between CMB and BAO data and caution against interpreting joint constraints in the context of inflation, until this emerging CMB-BAO tension is resolved.
We investigate a non-parametric Bayesian method for reconstructing the primordial power spectrum of scalar perturbations using temperature and polarisation data from the Planck, ACT, and SPT CMB experiments. We use the reconstructed scalar primordial power spectrum to derive several quantities related to inflationary dynamics, such as the effective scalar spectral index, slow-roll parameters for a slow and sudden variation of the background, and the speed of sound.
Primordial non-Gaussianity (PNG) represents a window into the nature of inflation, and large-scale structure (LSS) surveys can promisingly sharpen its constraints. To fully exploit this potential, cosmological simulations play a crucial role, allowing us to study the signatures and test the detectability of primordial features from LSS. I will present GENGARS, a framework to generate non-Gaussian initial conditions for N-body simulations from an arbitrary separable PNG shape. Building on the reduced-bispectrum-kernel formulation, we employ a Schwinger parameterization that improves efficiency by order of magnitudes, while preserving accuracy. I will outline the method and validation against 2LPT-PNG on the standard local, equilateral and orthogonal cases, emphasizing control of the induced large-scale primordial power spectrum correction, a critical requirement for accurate PNG simulations. I will then discuss how the same pipeline naturally accommodates non-standard templates, such as oscillatory PNG, and show their imprint on late-time statistics.
Detecting parity violation on cosmological scales would provide a striking clue to new physics. Large-scale structure offers the raw statistical power -- many three-dimensional modes -- to make such tests. However, for scalar observables, like galaxy clustering, the leading parity-sensitive observable is the trispectrum, whose high dimensionality makes the measurement and noise estimation challenging. We present two late-time parity-odd kurto spectra that compress the parity-odd scalar trispectrum into one-dimensional, power-spectrum-like observables. They are built by correlating (i) two appropriately weighted quadratic composite fields, or (ii) a linear and cubic composite field, constructed from dark matter (DM) or galaxy overdensity fields. We develop an FFTLog pipeline for efficient theoretical predictions of the two observables. We then validate the estimators for a specific parity-odd primordial template on perturbative DM field, and on DM and halo fields in full N-body \texttt{Quijote} simulations, with and without parity-odd initial conditions, in real and redshift space. For DM, the variance is dominated by the parity-even contribution -- i.e., the gravitationally induced parity-even trispectrum -- and is efficiently suppressed by phase-matched fiducial subtraction. For halos, discreteness-driven stochasticity dominates and is not appreciably reduced by subtraction; however, optimal weighting and halo-matter cross kurto spectra considerably mitigate this noise and enhance the signal. Using controlled down-sampling of the matter field, we empirically calibrate how the parity-even variance scales with number density and volume, and provide an illustrative forecast for the detectability of parity-odd kurto spectra in a Euclid-like spectroscopic galaxy survey.
Cosmological correlators and the associated wavefunction coefficients serve as a smoking gun towards the physics of inflation at high energy scales. In minimal setups of single-field inflation, wavefunction coefficients are purely real at tree-level due to unitarity, locality and scale invariance, leading to the so-called no-go theorems on parity violation. Such parity-violating correlators are therefore null tests of fundamental principles. Yet interestingly, there exists a twist of plot when quantum loops are involved. We show that such cosmological reality must be spontaneously broken by the renormalisation of UV divergences in de Sitter loops. More specifically, unitarity and analyticity dictate a universal imaginary part from the logarithmic running of the real part of the wavefunction coefficients. We then discuss the implications related to this universality.
In cosmology, correlation functions on a late-time boundary can arise from both field redefinitions and bulk interactions, which are usually believed to generate distinct results. In this letter, we propose a counterexample showcasing that correlators from local field redefinitions can be identical to the ones from bulk interactions. In particular, we consider a two-field model in de Sitter space, where the field space gets twisted by field redefinitions to yield a nontrivial reheating surface. We then exploit conformal symmetry to compute the three-point function, and show that the result takes the form of contact correlators with a total-energy singularity. Our finding suggests that in the effective field theory, a class of lower-dimensional operators, which were overlooked previously, may lead to nontrivial signals in cosmological correlators. As an illustration, we apply our result to cosmic inflation and derive a possibly leading signature of the Higgs in the primordial bispectrum.
Effective field theories in particle physics are usually designed for experiments where the initial state — the vacuum before a scattering event — is as clean and isolated as possible. Yet many physical systems, from condensed matter to cosmology, evolve in noisy and dissipative environments. Over the past decade, this recognition has driven progress at the interface between high-energy physics and condensed-matter. Motivated by these insights, I will present a framework for gravitational dynamics that combines General Relativity with the Schwinger–Keldysh formalism. I will show how symmetries, locality, and unitarity constrain dissipation and noise, and illustrate the approach by deriving the most general conservative and dissipative dynamics of scalar and tensor perturbations during single-clock inflation. I will conclude by discussing future prospects for dissipative dark sectors in the late universe.
We study quantum decoherence of curvature perturbations at superhorizon scales caused by the gravitational nonlinearities. We show that cubic gravitational couplings, constrained by the spatial diffeomorphism invariance, lead to infrared (IR) and ultraviolet (UV) divergences in the decoherence rate at one loop. These divergences arise from fluctuations of deep IR modes which look like a background mode for a local observer and violent zero-point fluctuations in the deep UV, respectively. We argue that these divergences are unobservable, as they vanish when considering proper observables. We consider correlators defined using the geodesic distance for IR divergences and time-averaged correlators for UV divergences. To account for these observer's perspectives, we propose to consider an effective quantum state, defined in terms of actual observables, as a more appropriate probe of the quantum coherence of the system measured by an observer. We then evaluate the finite decoherence rate induced by superhorizon environment during inflation and at late universe. This talk is based on the paper arXiv:2504.10472.
In order to shed light on the quantum to classical transition of the primordial perturbations in single field inflation, we investigate the decoherence and associated quantum corrections to the correlation functions of large-scale (superhorizon) scalar curvature perturbations. The latter are considered as an open quantum system which undergoes decoherence induced by a time-dependent environment of deep subhorizon tensorial modes (i.e. primordial gravitational waves) through the trilinear interactions predicted by General Relativity. We first prove that a time dependent subhorizon environment of gravitational waves can be relevant for decoherence during inflation, by considering derivativeless interactions, which, in our case, give the most important results. Our results show that important non-Markovian effects pop up, instead, when dealing with derivative interactions. When considering the interplay between derivativeless and derivative interactions, decoherence is slowed down. This underlines the importance of accounting for all the interactions in open quantum-system calculations in an inflationary setting. We finally compute the quantum corrections to cosmological correlation functions. We observe a resummation of the quantum corrections, which is a general property of quantum master equations.
Several major open problems in cosmology involve spacetime-filling media with unknown microphysics, and can only be probed through their gravitational effects. This observation motivates a systematic open-system approach, in which gravity evolves in the presence of a generic, unobservable environment. In this talk, I will present a general framework for open gravitational dynamics, based on the Schwinger-Keldysh path integral formalism. Applied to inflation, the framework recovers the Open Effective Field Theory of Inflation in the decoupling limit and naturally extends it to include gravitational interactions. These yield both conservative and dissipative corrections to graviton propagation. Remarkably, the leading gravitational birefringence is dissipative, while conservative birefringence only appears at higher derivative order — contrary to the electromagnetic case.
I will present an effective field theory (EFT) that captures the dominant late-time behavior of massless spectator fields in de Sitter space in the presence of heavy internal fields. As expected, when the mass of these internal fields is large, the leading term reproduces the infrared-divergent contributions to correlation functions obtained in the single-field description. Remarkably, even when the mass of the spectator field is below the Hubble scale, there still exists an EFT description organized in terms of leading local operators with subdominant nonlocal corrections. Crucially, this EFT describes a mixed rather than a pure state, and its four-point functions display logarithmically growing divergences at late times. In this regime, standard perturbation theory breaks down and must be reorganized. The resulting EFT is not obtained by integrating out heavy modes in the Wilsonian sense, but instead emerges from an explicit expansion of the time-evolution operator. The outcome is a local, Markovian, and generically non-unitary effective theory that resums the leading infrared behavior of the full theory to all orders. I will discuss its structure, diagrammatic interpretation, and implications for resumming loop corrections to inflationary correlators even when the heavy fields never go on shell.
A major CITA concentration is spatially concentrated primordial nonGaussianities (pinGs) from outlier trajectories (ponGs) which can arise generically during and after inflation from field-instabilities transverse to the inflaton flow. CMB and LSS lightcone Webskys we construct with pinGs can evade the stringent 2D perturbative single-nonG-template constraints from the ~10 e-folds probed by Planck+ACT. pinGs could play a role in the low-k CMB anomalies and have correlated localized B-modes sourced by anisotropic stress. pinGs would be more easily detected in 3D Large Scale Structure Surveys and could be hugely-big in the largely obscured 50 e-foldings from CMB/LSS scales to the end-of-inflation. We explore the generic nature of pinGs using pseudo-spectral lattice simulations applied to multi-field effective-potentials cast in an in-out state formulation. Though similar in spirit to the $mass^2 >0 $ cosmic collider program, the $mass^2 <0$ in (incomplete) phase transitions gives more dramatic observable phenomena, maybe even with entropic memories of domain wall and stringy structures in Cosmic Webskys. I will also relate this pinGy work to our popular stochastic-inflation framework.
I will summarize key results from a series of 4 papers in collaboration
with Dick Bond and Jonathan Braden: (1) Relating stochastic inflation to
the results of state-of-the-art lattice simulations, complete with
component separation of nonGaussianity; (2) Spatial localization of
primordial intermittent nonGaussianity (pinGs) and the statistics of
rare events; (3) The role of outlier trajectories (ponGs) in the
generation of pinGs; and (4) The graviational wave response and their
nonlinear correlation to an associated scalar nonGaussian signal, unlike
the classical zero-point fluctuation r case.
A set of 3+1 equations for stochastic inflation can be obtained in a gauge invariant manner, incorporating all scalar and tensorial perturbation degrees of freedom and without gradient expansion. We demonstrate a numerical implementation of the stochastic equations cast in the BSSN formulation of Numerical Relativity.
The QCD axion is a leading Dark-Matter candidate, typically studied in two cosmological scenarios: a 'post-inflationary' regime, in which axionic cosmic strings form after inflation, and a 'pre-inflationary' regime, in which the axion field is homogenized across the observable Universe and no strings are present. Here I explore a third possibility, in which the axion acquires large fluctuations during the visible part of inflation. This generates a non-standard cosmic-string network, which opens a new window for axion Dark Matter at large axion masses—potentially up to the astrophysical bounds near 0.01 eV, even within the most minimal QCD axion model.
Accurate predictions of correlators of the primordial curvature perturbation are
critical for connecting inflationary models to cosmological observations. Numer-
ical methods employing differential equations, such as the transport approach,
have been extensively used to compute the evolution of these correlators. In this
talk, I will present a novel numerical implementation of the transport formalism.
We use Multi-point propagators (MPPs), that link non-linearly evolved fields
to their values at some earlier time. This method recasts the direct evolution
of correlators into a system of differential equations for MPPs. We benchmark
the MPP approach against the established PyTransport code across a range
of models, and I will discuss the essential applications of the new method to
models than can lead to enhanced fluctuations on small scales.
We will review a proposal for which complex geometries should be included as saddle points in the semiclassical evaluation of gravitational path integrals, including a new efficient algorithm to detect violating saddles. Then we will turn to the application of constraining inflation via the Hartle-Hawking wave function.
The effective potential of a scalar field is a powerful tool in quantum field theory. Loosely speaking, it can be interpreted as the quantum corrected classical potential of the field, and in cosmology it is widely used to describe the evolution of the inflaton and other scalars during inflation and vacuum transition probabilities, among other things. However, for light scalar fields its standard definition has an infrared problem, which means that it is dominated by very long-wavelength fluctuations.
In this talk, I discuss an alternative definition, known as the constraint effective potential, dating back to 1980s. In Minkowski spacetime, the two definitions are equivalent, but in de Sitter spacetime they are not, and crucially the constraint effective potential does not suffer from the same infrared problem. I demonstrate this with an explicit one-loop calculation of the two effective potentials for a real scalar field in de Sitter in dimensional regularisation. I compare the resulting potentials and their physical interpretations, and in particular, I argue that the constraint effective potential is the correct one to use in certain common cosmological applications, for example stochastic inflation.
This work was carried out in collaboration with Lucas Vicente Garcia-Consuegra.
The primordial magnetic fields are generated during inflation by breaking the conformal invariance of the electromagnetic action through a coupling to the inflaton. Often, a parity violating term is also added to the action to generate helical magnetic fields. In this talk, I will first show that departures from slow roll inflation (as it occurs in scenarios involving a phase of ultra slow roll), which generate strong features in the scalar power spectrum, inevitably lead to sharp features in the power spectra of the electromagnetic fields and also suppress their strengths on large scales. Thereafter, I will illustrate that such challenges can be circumvented in two-field models of inflation to arrive at spectra of magnetic fields of the required strength and shape. Lastly, I will describe the evaluation of the three-point cross-correlation between the curvature perturbations and magnetic fields in slow roll and ultra slow roll inflation, and discuss the validity of the consistency relation in the squeezed limit.
Currently, the search for primordial gravitational waves is largely focused on detecting the parity-odd polarization pattern in the Cosmic Microwave Background - the B-modes. Accurately interpreting B-mode measurements depends heavily on understanding their production mechanisms. A particularly compelling scenario involves gravitational wave generation through the interaction of axion with gauge fields during inflation. I will present recent advances in axion inflation with non-Abelian gauge fields, focusing on the signatures in the primordial gravitational wave background and their correlation with primordial magnetic fields. I will conclude with a discussion of how the Schwinger effect at the end of inflation can nearly exclude axion magnetogenesis as a viable scenario.
With high precision data about to be released by large scale cosmological surveys, the development of higher order perturbative descriptions of cosmological observables is becoming increasingly important.
The so-called Geodesic Light-Cone (GLC) coordinates are a physically motivated set of coordinates accounting for the fact that light-rays propagate on the past light-cone of an observer. They are a powerful tool to study both the primordial universe and the late-time one. In particular, regarding the latter, they allow for fully non-linear expressions for light-like cosmological observables.
In this talk, I will first review how these coordinates are defined. Then, I will show how a cosmological perturbation theory up to the second order can be built on top of a background light-cone geometry. Within this new perturbative framework and adopting a fully gauge invariant approach, higher order formulae for cosmological observables can be computed. I will focus on the observed redshift, the angular distance-redshift relation and the redshift drift. In particular, by means of the GLC gauge fixing, IR divergences arising in first and second order formulae can be eliminated in a totally model independent way. Moreover, with this formalism one can obtain compact expressions for general relativistic effects, which play a crucial role in the study of Large Scale Structures as emergent features of primordial inflationary fluctuations.
We study stochastic gravitational waves (GW) sourced by a Higgs-like spectator field via the modulated reheating mechanism. The spectator is non-minimally coupled to spacetime curvature, while the inflaton decays via shift-symmetric, dimension-five operators into fermions or vectors. The curvature perturbations generated by the spectator in the de Sitter vacuum are blue-tilted and strongly non-Gaussian. They must be suppressed on scales probed by CMB anisotropies but can grow large on sub-Mpc scales, generating observationally testable stochastic GWs. Within this framework, we find that for Standard Model values of the gauge and Yukawa couplings the GWs signal remains unobservably small. A detectable signal within the reach of future experiments would require moving to a non-perturbative regime of the couplings.
The early period of accelerated expansion, known as inflation, in its minimal form, is driven by a scalar field (inflaton) and it takes place when this scalar field slowly rolls down a potential well. However, the origin of this scalar field and the correct form of the scalar potential remains an open question in cosmology. I will present a string theory motivated model where the inflaton is connected to the geometry of the internal space -- the overall volume of it drives the inflation. In particular, I will present a construction where the overall volume modulus (scalar field) is dynamically stabilized to an exponentially large value only via perturbative corrections, also known as perturbative large volume scenario (LVS). In this framework, the robustness of the single-field inflationary model is checked against possible sub-leading corrections. Next, I will focus on the global embedding of the fibre inflation in perturbative LVS and show how our constructions pose less challenge in realizing a successful period of inflation. Finally, I will finish my talk by emphasizing how perturbative LVS can as well accommodate a viable three-field model of inflation with non-trivial late time physics.
The stochastic approach to inflation aims to describe the non-perturbative evolution of long-wavelength modes of quantum fields during inflation as a classical stochastic theory. After highlighting how such an approach is non-Markovian by construction, I will explore the connection between stochastic approach and standard cosmological perturbation theory, showing that non-Markovian effects are crucial to study inflationary perturbations beyond the squeezed limit.
The primordial gravitational-wave background (PGWB), if detected, would provide key information about the inflationary period, complementary to scalar perturbations. Typical calculations of the PGWB decouple tensor and scalar perturbations; however, for non-standard models of inflation such as ultra-slow-roll, tensors and scalars can interact strongly to produce large non-Gaussian signatures in late-time correlators. We use the numerical relativity code GRChombo/GRTeclyn to predict the shape of these correlators by evolving a stochastic gravitational-wave background according to the fully-relativistic Einstein’s equations during slow-roll inflation. We briefly present our validation study, where we recovered the Mukhanov-Sasaki solution across two orders of magnitude in Fourier space, and outline the correction we make to the phase of our initial conditions, which allows us to make a mode-by-mode recovery of the linear solution. We then present recent work on the recovery of second-order gravitational waves from similar simulations.
We present a novel realization of Dirac leptogenesis based on the post-inflationary reheating phase of the early universe. An asymmetry generated within the scalar sector via CP-violating and out-of-equilibrium inflaton decays is transferred to chiral neutrinos through Yukawa interactions and then to baryons via electroweak sphalerons. We describe in detail a minimal realization of this mechanism that naturally accommodates small neutrino Yukawa couplings and results in contributions to the effective number of relativistic species, $N_{\rm eff}$, testable in upcoming cosmological observations.
The examination of parity symmetry in gravity is attracting growing attention. Previous studies have suggested that a non-minimal coupling between a dual 2-form field and gravity generates chiral gravitational waves. In this study, we construct a ghost-free Lagrangian density containing all dimension-four operators composed of the 2-form field, its dual field, and the curvature tensor. To make it applicable to cosmology, we consider a triplet of 2-form fields in a manner similar to cosmological models with mutually orthogonal vector fields. Then, we examine the tensor perturbations. We conclude that dual 2-form fields, other than those included in the potential, can be absorbed into a redefinition of the 2-form fields. Moreover, even if the action contains no non-minimal coupling, the dual field in the potential can generate chiral gravitational waves.
Parity-violation in the primordial universe leaves tell-tale trails in many cosmological observables. Chirality in cosmological gravitational wave background is one of the smoking gun signatures of parity violation. Induction of chirality becomes non-trivial in the simple and inevitable background of scalar-induced gravitational waves (SIGW). In this talk, I shall discuss the chirality imparted to SIGW by the parity-odd component of the primordial four-point correlation, the trispectrum. The degree of chirality in SIGW allows us to impose an independent limit on the strength of the parity-odd trispectrum and compare against observational bounds. Over certain scales, we find SIGW directly quantify parity-violation in primordial non-Gaussianity, unobscured by the Gaussian contribution. Our results call for the treatment of chiral gravitational waves and parity-odd trispectrum as complementary predictions of parity-violating theories of the early universe.
We consider a stochastic spectator scalar field coupled to fermion via the Yukawa interaction, in the inflationary de Sitter background. We consider the fermion to be massless, and take the one loop effective potential found earlier by using the exact fermion propagator in de Sitter spacetime. We take the potential for the spectator scalar to be quintessence-like, $V(\phi)=\alpha |\phi|^p$ ($\alpha \ensuremath{>} 0,\ p\ensuremath{>} 4$), so that the total effective potential is generically bounded from below for all values of the parameters and couplings, and a late time equilibrium state is allowed. Using next the stochastic spectral expansion method, we numerically investigate the two point correlation function, as well as the density fluctuations corresponding to the spectator field, with respect to the three parameters of the total effective potential, $\alpha,\ p$ and the Yukawa coupling, $g$. In particular, we find that the power spectrum and the spectral index corresponds to blue tilt with increasing $g$. The three point correlation function and non-Gaussianity corresponding to the density fluctuation has also been investigated. The increasing Yukawa coupling is shown to flatten the peak of the shape function in the squeezed limit. Also in this limit, the increase in the same is shown to increase the local non-Gaussianity parameter.
The Universe is currently in a phase of accelerated expansion, a fact that was experimentally proven in the late 1990s. Cosmological models involving scalar fields allow the description of this accelerated expansion regime in the Cosmos and present themselves as a promising alternative in the study of the inflationary eras, especially the actual one which is driven by the dark energy. In this work we use the $f(R, T) - \Lambda(\phi)$ gravity to find different cosmological scenarios for our Universe. We also introduce a new path to derive analytic cosmological models which may have a non-trivial mapping between $f$ and $T$. We show that the analytic cosmological models obtained with this approach are compatible with a good description of the radiation era. In addition, we investigated the inflationary scenario and obtained a good agreement for the scalar spectral index $n_s$. Concerning the tensor-to-scalar ratio $r$, we found promising scenarios compatible with current CMB data.
We assess the potential of the J-PAS survey to constrain the primordial power spectrum using a non-parametric Bayesian reconstruction method. Simulated spectra are generated with a localized oscillatory feature, motivated by non-standard inflation, and analyzed in the range k ∈ [0.02,0.2] h Mpc^-1, where J-PAS is most sensitive and non-linearities remain subdominant. The primordial spectrum is reconstructed via linear interpolation across N knots in the log(k)–log(P_R(k)) plane, jointly sampled with cosmological parameters {H_0, Ω_b h^2, Ω_c h^2} using PolyChord. Feature detection is quantified using both the Bayes factor and a hypothesis test. We examine the recovery of the injected feature under different J-PAS configurations—redshift binning, tracer type, survey area, and filter strategy—and find that amplitudes as small as 2% can be detected when combining tracers and redshift bins.
As ongoing work, we are applying this reconstruction framework to existing large-scale structure data from BOSS and eBOSS, providing the first validation on real data and setting competitive constraints on potential primordial features.
In this talk, we extend the stochastic formalism to Loop Quantum Cosmology (LQC) to study how quantum fluctuations affect the dynamics of a scalar field with an exponential potential. Building on previous results in the classical collapse case, where stochastic effects can destabilise pressureless collapse, we now explore their role near the LQC bounce. This approach provides a framework to investigate the quantum-to-classical transition beyond inflationary settings.
Primordial gravitational waves (PGWs) generated during inflation exhibit a steep growth in the spectral energy density (SED) at small scales. In this talk, we will discuss the behavior of the SED at high frequencies in the light of adiabatic regularization. For an instantaneous inflation-radiation transition, the regularized spectrum remains nearly scale invariant at small scales. We will show that, introducing smoother transitions of the effective potential, leads to power-law suppression, or even exponential suppression of the SED at small scales. These results highlight that the spectrum of PGWs at high frequency is highly sensitive to the dynamics of the inflation-radiation transition.
Higher-order correlation functions, such as the bispectrum and trispectrum, encode the non-Gaussian statistics of primordial fluctuations during inflation and serve as powerful probes of the underlying inflationary microphysics. In this work, we compute the inflationary trispectrum of primordial gauge fields arising from scalar and tensor exchanges in models with spectator U(1) gauge fields kinetically coupled to the inflaton. Using the in-in formalism, we obtain exact analytical expressions for the full trispectrum of both electric and magnetic fields and analyse their contributions in some interesting momentum configurations. For scalar exchange, we find that the equilateral trispectrum grows with exchange momentum and peaks in the flattened limit, while in the counter-collinear limit, the associated non-linearity parameter scales quadratically with that of the cross-bispectrum of magnetic fields and curvature perturbations, thereby establishing a hierarchical relation between different correlation functions. In contrast, tensor exchange induces a richer angular dependence, with the trispectrum exhibiting characteristic modulations tied to the relative orientation of the momentum quadrilateral and tensor polarisations. The detection of such angular signatures in future high-precision observations would offer a unique probe of tensor-mediated interactions in the early universe.
The non-linear dynamics inherent in the axial coupling between massless gauge fields and a pseudo-scalar during inflation have been thoroughly investigated, and some features of the strong backreaction regime can be captured using simple analytical expressions for the interaction terms. In this talk, I will show some preliminary work on the extension of the mechanism to the case of massive gauge fields, which are expected from thermalisation or from a Stückelberg mechanism. I will present analytical formulas for the comoving energy density of gauge fields and for the helicity. An estimation of the enhancement in the power spectrum of the scalar perturbations in the gauge-induced slow-roll phase will also be provided.'
Out-of-equilibrium quantum fields play an important part in early universe phenomena such as inflation and reheating. Two particle irreducible -formalism (2PI-formalism) offers a way to track the nonlinear evolution of the fields, but solving the resulting system is very numerically demanding. In this talk I will present a method of reducing the 2PI equations of motion of a scalar field into a set of quantum Boltzmann equations. Focusing on gravitational dark matter production during reheating, I go through select applications of the formalism as well touch on some of the challenges in its implementation.
The gauge dependence of second-order tensor perturbations has long been a challenge in the study of scalar-induced gravitational waves. Using a fully general setup, we systematically derive observables associated with these perturbations before fixing gauge. Our analysis shows that, when gravitational waves arise purely as second-order effects, the physically measurable quantities coincide precisely with the transverse-traceless (TT) components of the metric perturbation in the Newtonian gauge. This result provides a clear and gauge-independent interpretation of second-order gravitational wave signals and facilitates their connection to upcoming observations.
In the context of axion inflation coupled with SU(2) gauge fields, commonly called chromo-natural inflation, the gauge fields' interaction with the axion acts as an extra friction term. Aside from making inflation last more e-folds of evolution, this friction also sources the scalar and tensor sectors for the perturbations, generating a particular gravitational wave signal along with curvature perturbations. On the chromo-natural evolution, this axion-gauge interaction generates a strong backreaction from the gauge tensor sector to the background evolution. This build-up to a strong backreaction regime which is independent of the potential and almost unavoidable (unless there is severe fine-tuning of the system's parameters). The effect of this backreaction leads to a particular evolution of the gauge VEV, which passes through a period of large curvature perturbations generation to reach a recently described, well-defined, new attractor evolution. In this work, we studied the most general scenarios, which show compatibility between the CMB constraints and the evolution from a weak to a strong backreaction regime. Additionally, we consider a pure natural potential for our numerical solver of the system. We also examine the gravitational wave signal (both direct and scalar-induced) and the PBH production generated due to this particular inflationary evolution.
The question of geodesic completeness of cosmological spacetimes has recently received renewed scrutiny. A particularly interesting result is the observation that the well-known Borde-Guth-Vilenkin (BGV) theorem may misdiagnose geodesically complete cosmologies. We propose a simple amendment to the BGV theorem which addresses such loopholes while retaining much of its generality. We give straightforward proofs of some recently offered conjectures concerning (generalized) Friedmann-Lemaître-Robertson-Walker spacetimes: geodesic completeness implies (i) the existence of a bounce, loitering phase or an emergent cosmology, and (ii) a phase of accelerated expansion with strictly increasing Hubble rate. Our results are purely kinematic and do not assume general relativity or energy conditions.
During inflation, quantum vacuum fluctuations are stretched beyond the Hubble radius, modifying the large-scale dynamics of the Universe. While their backreaction is negligible in the perturbative regime, it can become important in scenarios leading to primordial black hole (PBH) formation, where large density fluctuations are generated. The combination of stochastic inflation and the 𝛿N formalism provides an efficient framework to track these large fluctuations non-perturbatively. After reviewing the emergence of heavy non-Gaussian tails in the curvature perturbation distribution, I will show how large fluctuations are spatially correlated by computing real-space correlation functions within the stochastic-𝛿N approach. This can be used to characterise the spatial distribution of PBHs, revealing a universal clustering profile at their formation.
I will then introduce a novel framework that implements stochastic inflation on stochastic trees, modelling inflationary expansion as a branching process. Notably, stochastic trees do not operate on a fixed background, instead new spacetime units dynamically emerge as the trees unfold, naturally incorporating metric fluctuations. The tree structure naturally encodes the statistics of curvature perturbations and other cosmological fields, providing a direct tool to study PBH formation. Within this picture, PBHs emerge at unbalanced nodes of the tree, and their mass function can be derived while automatically accounting for the “cloud-in-cloud” effect. Finally, I will discuss ongoing work on extracting compaction-function criteria for PBH formation and probing type I and type II perturbations directly from the stochastic tree population.
We have investigated primordial black holes formation within a model of the early Universe dominated by a massless scalar field, developing a numerical spherically symmetric code dedicated to this problem. Imposing initial conditions on super horizon scales using the gradient expansion approach, we show that a massless scalar filed is equivalent to a perfect fluid, where the pressure is equal to the total energy density, only in the regime of cosmological expansion, while during the gravitational collapse space-like gradients arises and the comoving slicing is failing. For this reason, moving to a constant mean curvature slicing, we follow entirely the numerical evolution of cosmological perturbations, also during the gravitational collapse, computing the threshold for primordial black hole formation, and the corresponding mass distribution described by critical collapse.
Stochastic inflation is a method for computing super-Hubble perturbations beyond the small-perturbation limit. I show how to obtain the radial profile of the curvature perturbations in a random patch of space using this method. The profiles turn out to be spiky, far from the smooth mean profiles often considered in the literature. Based on extensive numerical simulations, I discuss the profiles' structure and its implications for the formation of primordial black holes.
The inflationary diffusion of scalar fields with discrete symmetries can generate a gas of closed domain walls after inflation, which later collapse into primordial black holes (PBHs) upon horizon re-entry. This mechanism predicts a distinctive, nearly flat PBH mass distribution, avoiding some issues of critical collapse. We show that QCD axion models with decay constants near the inflationary Hubble scale (f_a \sim 10^8 GeV) can produce PBHs making up ∼1% of dark matter, consistent with CMB isocurvature bounds.
The Hawking evaporation of primordial black holes (PBHs) induces local reheating of the Universe, generating transient hot spots that persist over their evaporation timescale. Within this framework, we develop a method to compute the decay rate of metastable vacua in cosmological settings, circumventing conceptual issues associated with the Hartle–Hawking and Unruh vacua. Applying our approach to the electroweak vacuum instability, we derive constraints on the PBH abundance from the condition that if the electroweak vacuum is metastable, then a large population of evaporating PBHs is ruled out.
We compare two setups incorporating new massive spinning degrees of freedom during inflation within the framework of the effective field theory of inflation (EFToI). Even though they differ on which symmetries are linearly realised, since they couple to the inflaton, it is possible they yield same signatures on cosmological correlators. We will see that their signatures are the same at bispectrum, but not higher-point correlators. There will also be a portion dedicated to the Feynman rules when calculating the correlators in these setups involving non-dynamical modes.
Understanding the microscopic origin of primordial fluctuations remains a central challenge in inflationary cosmology. In this talk, I will explore a scenario where curvature perturbations interact with a strongly coupled, gapless sector known as unparticles. This setup allows for analytic control of cosmological correlators and reveals novel bispectrum shapes with distinctive phenomenological signatures. If time permits, I will also comment on possible model realizations and gapped scenarios.
Using perturbation theory, we compute the one-point probability density function for primordial fluctuations valid to first order in the potential. We examine under which conditions our solution respects the Fokker-Planck equation encountered within the stochastic approach. We identify discrepancies and elucidate their origins, allowing us to shed light on the status of the stochastic formalism.
Light, polynomially self-interacting scalars in de Sitter notoriously generate infrared (IR) divergences: on superhorizon scales, their fluctuations grow so large that perturbation theory breaks down. We address this problem using non-perturbative techniques from stochastic inflation, by encoding the superhorizon dynamics in a probability distribution involving composite operators of the light scalar. We find that these composites behave as late-time conformal primaries, with their position-space four-point function collapsing to a strikingly simple power law. We conjecture a new physical picture: light interacting scalars in de Sitter effectively hadronize on superhorizon scales, producing a tower of composite states. We then explore whether this emergent spectrum can be captured within a weakly coupled effective field theory, which would amount to recasting the stochastic scalar IR-dynamics in terms of new, effective degrees of freedom.
In the stochastic $\delta N$ formalism, the statistics of the primordial density perturbations can be mapped to the first-passage distribution of a stochastic process. In this talk, I will present a general framework to evaluate the rare-event tail of this distribution, based on an instanton approximation to a path integral representation of the transition probability. I will show how this stochastic description can be derived from a more fundamental formulation via the Schwinger-Keldysh path integral, where integrating out short-wavelength modes yields an influence functional that encodes the noise statistics underlying the stochastic approach. Finally, I will apply this method to a number of cases, highlighting its connections with, and advantages over, the existing methodologies.
In this work we provide the missing link between two approaches aimed at characterizing the effect of long perturbation modes in Inflation. We consider the Inflationary Fossils' approach (arXiv:1203.0302 and related works) that characterizes the power-spectrum of the inflaton field in presence of other long and non dynamical fossil fields, and a technique, appeared in arXiv:2103.09244, that computes, beyond perturbation theory, the power-spectrum of a scalar field in presence of a large fluctuation of a second field. We clarify a few points on the applicability of the non-perturbative technique. We prove in five distinct cases that the non-perturbative approach, once expanded to first order in the coupling, matches the perturbative result following the Fossils' approach. We believe that this non-perturbative technique extends to all orders the Fossils' approach, resumming infinitely many diagrams of standard in-in perturbation theory.
Primordial Gravitational Waves (PGWs) are a key prediction of inflation, with ongoing efforts to detect them through CMB polarization patterns and direct interferometric searches. In this talk, I will present a novel approach to probing PGWs through their impact on Large-Scale Structure (LSS). While PGWs are often assumed to have a negligible effect on structure formation, our study shows that they can source second-order scalar perturbations. These "tensor-induced scalar modes" emerge upon horizon entry, modifying the matter density contrast and leaving distinct imprints on the matter power spectrum. This mechanism also introduces an intrinsic source of non-Gaussianity in the density field, providing a unique observational signature. I will discuss how different PGW power spectra shape this imprint and evaluate its detectability in future galaxy surveys like Euclid and SKA.
Spectator fields which provide additional tensor degrees of freedom, on top of the standard metric tensor perturbations, can produce significant amounts of gravitational waves (GWs). Employing the effective field theory approach for spin-2 fields, we find a universal prediction that linear mixing between the metric and extra tensor modes inevitably induces oscillatory features in the GW spectrum. Moreover, parity-violating operators in the spin-2 sector can imprint chiral signatures on the resulting GW background. These results provide a model-independent characterization of the key signatures and observational implications of such scenarios which can be detected with future GW detectors.
The separate universe approach (SUA) is a powerful tool offering us a simple way to compute cosmic inhomogeneities at large scales including their non-linear evolution. It consists in describing the universe as a collection of independent patches which are taken to be homogeneous and isotropic. The assumptions one has to do to apply the SUA and its simplifications need to be checked, notably in multifield models of inflation. In this talk I will present the validity conditions of the SUA in non-linear sigma models by matching it to a complete cosmological perturbation theory computation taken to large scales. In particular I will dive into the subtleties of gauge fixing procedures and how they compare in both schemes.
Observations of the cosmic microwave background (CMB) lend strong evidence for the paradigm of cosmic inflation, but the specific form of the inflaton potential remains unknown. Under certain conditions, the oscillating inflaton condensate filling the Universe after inflation can fragment and form interesting non-linear structures known as oscillons. These long-lived soliton-like field configurations can dominate the Universe for several e-folds of expansion, leading to an early matter-dominated phase preceding the standard radiation era.
In this talk, I will show how the rapid decay of the oscillons leads to an enhanced production of induced gravitational waves (GWs), whose energy density can saturate the observational bound on the effective number of relativistic species. We leverage this bound to constrain the inflaton mass, cubic, and quartic self-coupling in generic models that admit oscillon formation, providing novel and complementary constraints in regions of parameter space that are inaccessible with CMB observations alone.