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Hector Villarrubia-Rojo

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3works
6topics
3close collaborators

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3 publications

preprint2026arXiv

Testing General Relativity Through Gravitational Wave Classification: A Convolutional Neural Network Framework

We present a machine learning framework for testing general relativity (GR) with gravitational wave signals from binary black hole mergers. Using the source parameters of 173 BBH events from the GWTC catalog as a realistic astrophysical population, we generate simulated GR waveforms and construct beyond GR (BGR) waveforms by applying controlled phase deformations. We introduce a response function formalism that provides a systematic framework for quantifying how any observable responds to modifications of GR. We train convolutional neural networks (CNNs) on two input representations: whitened waveforms and a response function type observable derived from the waveform mismatch, which isolates the effect of phase deviations from the bulk signal. Using response functions as the CNN input improves the classification sensitivity by a factor of approximately 33 compared to whitened waveforms, demonstrating that the choice of observable representation is as important as the classifier architecture. We study the fundamental limits of this classification through Bayes optimal error analysis, averaging methods that reveal coherent patterns hidden in noise, and a comparison between CNN accuracy and a single feature classifier as a proxy for human performance. At all deformation scales, the CNN outperforms the best single feature approach. We extend the framework to physically motivated theories using the parameterized post Einsteinian (ppE) formalism and apply it to massive gravity, where the classifier detects deviations for graviton masses of order mg∼10−23  eV/c2m_g \sim 10^{-23}\;\mathrm{eV}/c^2 with aLIGO design sensitivity.

preprint2022arXiv

Can late-time extensions solve the H0H_0 and σ8σ_8 tensions?

We analyze the properties that any late-time modification of the ΛΛCDM expansion history must have in order to consistently solve both the H0H_0 and the σ8σ_8 tensions. Taking a model-independent approach, we obtain a set of necessary conditions that can be applied to generic late-time extensions. Our results are fully analytical and merely based on the assumptions that the deviations from the ΛΛCDM background remain small. For the concrete case of a dark energy fluid with equation of state w(z)w(z), we derive the following general requirements: (i) Solving the H0H_0 tension demands w(z)<−1w(z)<-1 at some zz (ii) Solving both the H0H_0 and σ8σ_8 tensions requires w(z)w(z) to cross the phantom divide. Finally, we also allow for small deviations on the effective gravitational constant. In this case, our method is still able to constrain the functional form of these deviations.

preprint2022arXiv

Simultaneously solving the H0H_0 and σ8σ_8 tensions with late dark energy

In a model independent approach, we derive generic conditions that any late time modification of the ΛΛCDM expansion history must satisfy in order to consistently solve both the H0H_0 and the σ8σ_8 tensions. Our results are fully analytical and the method is merely based on the assumption that the late-time deviations from ΛΛCDM remain small. For the concrete case of a dark energy fluid with deviations encoded in the expansion history and the gravitational coupling constant, we present necessary conditions on its equation of state. Solving both the H0H_0 and σ8σ_8 tensions requires that w(z)w(z) must cross the phantom divide if Geff=GG_\text{eff}=G. On the other hand, for Geff=G+δG(z)G_\text{eff}=G+δG(z) and w(z)≤−1w(z)\leq -1, it is required that δG(z)G<α(z)δH(z)H(z)<0\displaystyle \frac{δG(z)}{G}<α(z)\frac{δH(z)}{H(z)}<0 at some redshift zz.

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