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Showing papers in "Physical Review D in 2021"


Journal ArticleDOI
Shadab Alam1, Marie Aubert, Santiago Avila2, Christophe Balland3, Julian E. Bautista4, Matthew A. Bershady5, Matthew A. Bershady6, Dmitry Bizyaev7, Dmitry Bizyaev8, Michael R. Blanton9, Adam S. Bolton10, Jo Bovy11, Jonathan Brinkmann8, Joel R. Brownstein10, Etienne Burtin12, Solène Chabanier12, Michael J. Chapman13, Peter Doohyun Choi14, Chia-Hsun Chuang15, Johan Comparat16, M. C. Cousinou, Andrei Cuceu17, Kyle S. Dawson10, Sylvain de la Torre, Arnaud de Mattia12, Victoria de Sainte Agathe3, Hélion du Mas des Bourboux10, Stephanie Escoffier, Thomas Etourneau12, James Farr17, Andreu Font-Ribera17, Peter M. Frinchaboy18, S. Fromenteau19, Héctor Gil-Marín20, Jean Marc Le Goff12, Alma X. Gonzalez-Morales21, Alma X. Gonzalez-Morales22, Violeta Gonzalez-Perez23, Violeta Gonzalez-Perez4, Kathleen Grabowski8, Julien Guy24, Adam J. Hawken, Jiamin Hou16, Hui Kong25, James C. Parker8, Mark A. Klaene8, Jean-Paul Kneib26, Sicheng Lin9, Daniel Long8, Brad W. Lyke27, Axel de la Macorra19, Paul Martini25, Karen L. Masters28, Faizan G. Mohammad13, Jeongin Moon14, Eva Maria Mueller29, Andrea Muñoz-Gutiérrez19, Adam D. Myers27, Seshadri Nadathur4, Richard Neveux12, Jeffrey A. Newman30, P. Noterdaeme3, Audrey Oravetz8, Daniel Oravetz8, Nathalie Palanque-Delabrouille12, Kaike Pan8, Romain Paviot, Will J. Percival31, Will J. Percival13, Ignasi Pérez-Ràfols3, Patrick Petitjean3, Matthew M. Pieri, Abhishek Prakash32, Anand Raichoor26, Corentin Ravoux12, Mehdi Rezaie33, J. Rich12, Ashley J. Ross25, Graziano Rossi14, Rossana Ruggeri4, Rossana Ruggeri34, V. Ruhlmann-Kleider12, Ariel G. Sánchez16, F. Javier Sánchez35, José R. Sánchez-Gallego36, Conor Sayres36, Donald P. Schneider, Hee-Jong Seo33, Arman Shafieloo37, Anže Slosar38, Alex Smith12, Julianna Stermer3, Amélie Tamone26, Jeremy L. Tinker9, Rita Tojeiro39, Mariana Vargas-Magaña19, Andrei Variu26, Yuting Wang, Benjamin A. Weaver, Anne-Marie Weijmans39, C. Yeche12, Pauline Zarrouk12, Pauline Zarrouk40, Cheng Zhao26, Gong-Bo Zhao, Zheng Zheng10 
TL;DR: In this article, the authors present the cosmological implications from final measurements of clustering using galaxies, quasars, and Lyα forests from the completed SDSS lineage of experiments in large-scale structure.
Abstract: We present the cosmological implications from final measurements of clustering using galaxies, quasars, and Lyα forests from the completed Sloan Digital Sky Survey (SDSS) lineage of experiments in large-scale structure. These experiments, composed of data from SDSS, SDSS-II, BOSS, and eBOSS, offer independent measurements of baryon acoustic oscillation (BAO) measurements of angular-diameter distances and Hubble distances relative to the sound horizon, rd, from eight different samples and six measurements of the growth rate parameter, fσ8, from redshift-space distortions (RSD). This composite sample is the most constraining of its kind and allows us to perform a comprehensive assessment of the cosmological model after two decades of dedicated spectroscopic observation. We show that the BAO data alone are able to rule out dark-energy-free models at more than eight standard deviations in an extension to the flat, ΛCDM model that allows for curvature. When combined with Planck Cosmic Microwave Background (CMB) measurements of temperature and polarization, under the same model, the BAO data provide nearly an order of magnitude improvement on curvature constraints relative to primary CMB constraints alone. Independent of distance measurements, the SDSS RSD data complement weak lensing measurements from the Dark Energy Survey (DES) in demonstrating a preference for a flat ΛCDM cosmological model when combined with Planck measurements. The combined BAO and RSD measurements indicate σ8=0.85±0.03, implying a growth rate that is consistent with predictions from Planck temperature and polarization data and with General Relativity. When combining the results of SDSS BAO and RSD, Planck, Pantheon Type Ia supernovae (SNe Ia), and DES weak lensing and clustering measurements, all multiple-parameter extensions remain consistent with a ΛCDM model. Regardless of cosmological model, the precision on each of the three parameters, ωΛ, H0, and σ8, remains at roughly 1%, showing changes of less than 0.6% in the central values between models. In a model that allows for free curvature and a time-evolving equation of state for dark energy, the combined samples produce a constraint ωk=-0.0022±0.0022. The dark energy constraints lead to w0=-0.909±0.081 and wa=-0.49-0.30+0.35, corresponding to an equation of state of wp=-1.018±0.032 at a pivot redshift zp=0.29 and a Dark Energy Task Force Figure of Merit of 94. The inverse distance ladder measurement under this model yields H0=68.18±0.79 km s-1 Mpc-1, remaining in tension with several direct determination methods; the BAO data allow Hubble constant estimates that are robust against the assumption of the cosmological model. In addition, the BAO data allow estimates of H0 that are independent of the CMB data, with similar central values and precision under a ΛCDM model. Our most constraining combination of data gives the upper limit on the sum of neutrino masses at mν<0.115 eV (95% confidence). Finally, we consider the improvements in cosmology constraints over the last decade by comparing our results to a sample representative of the period 2000-2010. We compute the relative gain across the five dimensions spanned by w, ωk, mν, H0, and σ8 and find that the SDSS BAO and RSD data reduce the total posterior volume by a factor of 40 relative to the previous generation. Adding again the Planck, DES, and Pantheon SN Ia samples leads to an overall contraction in the five-dimensional posterior volume of 3 orders of magnitude.

575 citations


Journal ArticleDOI
TL;DR: In this article, the authors evaluate the consistency of the LIGO-Virgo data with predictions from the theory and find no evidence for new physics beyond general relativity, for black hole mimickers, or for any unaccounted systematics.
Abstract: Gravitational waves enable tests of general relativity in the highly dynamical and strong-field regime. Using events detected by LIGO-Virgo up to 1 October 2019, we evaluate the consistency of the data with predictions from the theory. We first establish that residuals from the best-fit waveform are consistent with detector noise, and that the low- and high-frequency parts of the signals are in agreement. We then consider parametrized modifications to the waveform by varying post-Newtonian and phenomenological coefficients, improving past constraints by factors of ∼2; we also find consistency with Kerr black holes when we specifically target signatures of the spin-induced quadrupole moment. Looking for gravitational-wave dispersion, we tighten constraints on Lorentz-violating coefficients by a factor of ∼2.6 and bound the mass of the graviton to mg≤1.76×10-23 eV/c2 with 90% credibility. We also analyze the properties of the merger remnants by measuring ringdown frequencies and damping times, constraining fractional deviations away from the Kerr frequency to δf^220=0.03-0.35+0.38 for the fundamental quadrupolar mode, and δf^221=0.04-0.32+0.27 for the first overtone; additionally, we find no evidence for postmerger echoes. Finally, we determine that our data are consistent with tensorial polarizations through a template-independent method. When possible, we assess the validity of general relativity based on collections of events analyzed jointly. We find no evidence for new physics beyond general relativity, for black hole mimickers, or for any unaccounted systematics.

368 citations


Journal ArticleDOI
TL;DR: In this article, the parton distribution functions (PDFs) from the CTEQ-TEA collaboration were obtained using a wide variety of high-precision Large Hadron Collider (LHC) data, in addition to the combined HERA I+II deep-inelastic scattering dataset, along with the datasets present in the CT14 global QCD analysis.
Abstract: We present the new parton distribution functions (PDFs) from the CTEQ-TEA collaboration, obtained using a wide variety of high-precision Large Hadron Collider (LHC) data, in addition to the combined HERA I+II deep-inelastic scattering dataset, along with the datasets present in the CT14 global QCD analysis. New LHC measurements in single-inclusive jet production with the full rapidity coverage, as well as production of Drell-Yan pairs, top-quark pairs, and high-pT Z bosons, are included to achieve the greatest sensitivity to the PDFs. The parton distributions are determined at next-to-leading order and next-to-next-to-leading order, with each of these PDFs accompanied by error sets determined using the Hessian method. Fast PDF survey techniques, based on the Hessian representation and the Lagrange multiplier method, are used to quantify the preference of each data set to quantities such as αs(mZ), and the gluon and strange quark distributions. We designate the main resulting PDF set as CT18. The ATLAS 7 TeV precision W/Z data are not included in CT18, due to their tension with other datasets in the global fit. Alternate PDF sets are generated including the ATLAS precision 7 TeV W/Z data (CT18A), a new scale choice for low-x DIS data (CT18X), or all of the above with a slightly higher choice for the charm mass (CT18Z). Theoretical calculations of standard candle cross sections at the LHC (such as the gg fusion Higgs boson cross section) are presented.

335 citations


Journal ArticleDOI
TL;DR: The curvature parameter tension between Planck 2018, cosmic microwave background (CMB) lensing, and baryon acoustic oscillation (BAO) data is measured using the suspiciousness statistic to be $2.5--3\ensuremath{\sigma}$ as discussed by the authors.
Abstract: The curvature parameter tension between Planck 2018, cosmic microwave background (CMB) lensing, and baryon acoustic oscillation (BAO) data is measured using the suspiciousness statistic to be $2.5--3\ensuremath{\sigma}$. Conclusions regarding the spatial curvature of the Universe which stem from the combination of these data should therefore be viewed with suspicion. Without CMB lensing or BAO, Planck 2018 has a moderate preference for closed universes, with Bayesian betting odds of over $50\ensuremath{\mathbin:}1$ against a flat universe and over $2000\ensuremath{\mathbin:}1$ against an open universe.

206 citations


Journal ArticleDOI
TL;DR: In this article, the authors revisited the analysis of the HESE sample with an additional 4.5 years of data, newer glacial ice models, and improved systematics treatment.
Abstract: The IceCube Neutrino Observatory has established the existence of a high-energy all-sky neutrino flux of astrophysical origin. This discovery was made using events interacting within a fiducial region of the detector surrounded by an active veto and with reconstructed energy above 60 TeV, commonly known as the high-energy starting event sample, or HESE. We revisit the analysis of the HESE sample with an additional 4.5 years of data, newer glacial ice models, and improved systematics treatment. This paper describes the sample in detail, reports on the latest astrophysical neutrino flux measurements, and presents a source search for astrophysical neutrinos. We give the compatibility of these observations with specific isotropic flux models proposed in the literature as well as generic power-law-like scenarios. Assuming $ u_e: u_\mu: u_\tau=1:1:1$, and an equal flux of neutrinos and antineutrinos, we find that the astrophysical neutrino spectrum is compatible with an unbroken power law, with a preferred spectral index of ${2.87}^{+0.20}_{-0.19}$ for the $68.3\%$ confidence interval.

195 citations


Journal ArticleDOI
Richard J. Abbott1, T. D. Abbott2, Sheelu Abraham3, Fausto Acernese4  +1678 moreInstitutions (193)
TL;DR: In this article, the authors report results of a search for an isotropic gravitational-wave background (GWB) using data from Advanced LIGO's and Advanced Virgo's third observing run (O3) combined with upper limits from the earlier O1 and O2 runs.
Abstract: We report results of a search for an isotropic gravitational-wave background (GWB) using data from Advanced LIGO’s and Advanced Virgo’s third observing run (O3) combined with upper limits from the earlier O1 and O2 runs. Unlike in previous observing runs in the advanced detector era, we include Virgo in the search for the GWB. The results of the search are consistent with uncorrelated noise, and therefore we place upper limits on the strength of the GWB. We find that the dimensionless energy density Ω GW ≤ 5.8 × 10 − 9 at the 95% credible level for a flat (frequency-independent) GWB, using a prior which is uniform in the log of the strength of the GWB, with 99% of the sensitivity coming from the band 20–76.6 Hz; Ω GW ( f ) ≤ 3.4 × 10 − 9 at 25 Hz for a power-law GWB with a spectral index of 2 / 3 (consistent with expectations for compact binary coalescences), in the band 20–90.6 Hz; and Ω GW ( f ) ≤ 3.9 × 10 − 10 at 25 Hz for a spectral index of 3, in the band 20–291.6 Hz. These upper limits improve over our previous results by a factor of 6.0 for a flat GWB, 8.8 for a spectral index of 2 / 3 , and 13.1 for a spectral index of 3. We also search for a GWB arising from scalar and vector modes, which are predicted by alternative theories of gravity; we do not find evidence of these, and place upper limits on the strength of GWBs with these polarizations. We demonstrate that there is no evidence of correlated noise of magnetic origin by performing a Bayesian analysis that allows for the presence of both a GWB and an effective magnetic background arising from geophysical Schumann resonances. We compare our upper limits to a fiducial model for the GWB from the merger of compact binaries, updating the model to use the most recent data-driven population inference from the systems detected during O3a. Finally, we combine our results with observations of individual mergers and show that, at design sensitivity, this joint approach may yield stronger constraints on the merger rate of binary black holes at z ≳ 2 than can be achieved with individually resolved mergers alone.

146 citations


Journal ArticleDOI
TL;DR: The MiniBooNE experiment at Fermilab reported a total excess of 638.0±132.8 electron-like events (4.8σ) from a data sample corresponding to 18.75×1020 protons-on-target in neutrino mode, which is a 46% increase in the data sample with respect to previously published results.
Abstract: The MiniBooNE experiment at Fermilab reports a total excess of 638.0±132.8 electron-like events (4.8σ) from a data sample corresponding to 18.75×1020 protons-on-target in neutrino mode, which is a 46% increase in the data sample with respect to previously published results, and 11.27 × 1020 protons-on-target in antineutrino mode. The additional statistics allow several studies to address questions on the source of the excess. First, we provide two-dimensional plots in visible energy and cosine of the angle of the outgoing lepton, which can provide valuable input to models for the event excess. Second, we test whether the excess may arise from photons that enter the detector from external events or photons exiting the detector from π0 decays in two model independent ways. Beam timing information shows that almost all of the excess is in time with neutrinos that interact in the detector. The radius distribution shows that the excess is distributed throughout the volume, while tighter cuts on the fiducal volume increase the significance of the excess. We conclude that models of the event excess based on entering and exiting photons are disfavored.

135 citations


Journal ArticleDOI
T. Albahri1, A. Anastasi, Alexey Anisenkov2, Alexey Anisenkov3  +195 moreInstitutions (40)
TL;DR: The Muon g-2 Experiment at Fermi National Accelerator Laboratory (FNAL) has measured the muon anomalous precession frequency to an uncertainty of 434 parts per billion (ppb), statistical, and 56 ppb, systematic, with data collected in four storage ring configurations during its first physics run in 2018.
Abstract: The Muon g-2 Experiment at Fermi National Accelerator Laboratory (FNAL) has measured the muon anomalous precession frequency $\omega_a$ to an uncertainty of 434 parts per billion (ppb), statistical, and 56 ppb, systematic, with data collected in four storage ring configurations during its first physics run in 2018. When combined with a precision measurement of the magnetic field of the experiment's muon storage ring, the precession frequency measurement determines a muon magnetic anomaly of $a_{\mu}({\rm FNAL}) = 116\,592\,040(54) \times 10^{-11}$ (0.46 ppm). This article describes the multiple techniques employed in the reconstruction, analysis and fitting of the data to measure the precession frequency. It also presents the averaging of the results from the eleven separate determinations of \omega_a, and the systematic uncertainties on the result.

129 citations


Journal ArticleDOI
TL;DR: In this paper, a precessing extension of imrphenomxphm is presented, which incorporates multipoles beyond the dominant quadrupole in the pre-cessing frame, which is referred to as ''twisting up'' the nonprecessing waveforms.
Abstract: We present imrphenomxphm, a phenomenological frequency-domain model for the gravitational-wave signal emitted by quasicircular precessing binary black holes, which incorporates multipoles beyond the dominant quadrupole in the precessing frame. The model is a precessing extension of imrphenomxhm, [C. Garc\'{\i}a-Quir\'os et al., Phys. Rev. D 102, 064002 (2020)] based on approximate maps between aligned-spin waveform modes in the coprecessing frame and precessing waveform modes in the inertial frame, which is commonly referred to as ``twisting up'' the nonprecessing waveforms. imrphenomxphm includes imrphenomxp as a special case, the restriction to the dominant quadrupole contribution in the coprecessing frame. We implement two alternative mappings, one based on a single-spin post-Newtonian approximation, as used in imrphenompv2 [M. Hannam et al., Phys. Rev. Lett. 113, 151101 (2014).], and one based on the double-spin multiple scale analysis approach of [K. Chatziioannou et al., Phys. Rev. D 95, 104004 (2017).]. We include a detailed discussion of conventions used in the description of precessing binaries and of all choices made in constructing the model. The computational cost of imrphenomxphm is further reduced by extending the interpolation technique of [C. Garc\'{\i}a-Quir\'os et al., Classical Quant. Grav. 38, 015006 (2021).] to the Euler angles. The accuracy, speed, robustness, and modularity of the imrphenomx family will make these models productive tools for gravitational wave astronomy in the current era of greatly increased number and diversity of detected events.

129 citations


Journal ArticleDOI
TL;DR: In this article, the authors present a complete list of the dimension-eight operator basis in the standard model effective field theory using group theoretic techniques in a systematic and automated way, and decompose operators into the ones with definite permutation symmetries among flavor indices to deal with subtlety from repeated fields.
Abstract: We present a complete list of the dimension-eight operator basis in the standard model effective field theory using group theoretic techniques in a systematic and automated way. We adopt a new form of operators in terms of the irreducible representations of the Lorentz group and identify the Lorentz structures as states in a $SU(N)$ group. In this way, redundancy from equations of motion is absent and that from integration by part is treated using the fact that the independent Lorentz basis forms an invariant subspace of the $SU(N)$ group. We also decompose operators into the ones with definite permutation symmetries among flavor indices to deal with subtlety from repeated fields. For the first time to our knowledge, we provide the explicit form of independent flavor-specified operators in a systematic way. Our algorithm can easily be applied to higher-dimensional standard model effective field theory and other effective field theories, making these studies more approachable.

128 citations


Journal ArticleDOI
TL;DR: Gruzinov et al. as discussed by the authors performed a detailed analysis of the rich dynamics of spin-0 superradiance with self-interactions, and the resulting observational signatures, and explored multiple distinct regimes of parameter space introduced by a nonzero self interaction, including the simultaneous population of two or more bound levels.
Abstract: Black hole superradiance is a powerful probe of light, weakly coupled hidden sector particles. Many candidate particles, such as axions, generically have self-interactions that can influence the evolution of the superradiant instability. As pointed out in [A. Gruzinov, arXiv:1604.06422.] in the context of a toy model, much of the existing literature on spin-0 superradiance does not take into account the most important self-interaction-induced processes. These processes lead to energy exchange between quasi-bound levels and particle emission to infinity; for large self-couplings, superradiant growth is saturated at a quasi-equilibrium configuration of reduced level occupation numbers. In this paper, we perform a detailed analysis of the rich dynamics of spin-0 superradiance with self-interactions, and the resulting observational signatures. We focus on quartic self-interactions, which dominate the evolution for most models of interest. We explore multiple distinct regimes of parameter space introduced by a nonzero self-interaction, including the simultaneous population of two or more bound levels; at large coupling, we confirm the basic picture of quasiequilibrium saturation and provide evidence that the ``bosenova'' collapse does not occur in most of the astrophysical parameter space. Compared to gravitational superradiance, we find that gravitational wave ``annihilation'' signals and black hole spin-down are parametrically suppressed with increasing interactions, while new gravitational wave ``transition'' signals can take place for moderate interactions. The novel phenomenon of scalar wave emission is less suppressed at large couplings, and if the particle has Standard Model interactions, then coherent, monochromatic axion wave signals from black hole superradiance may be detectable in proposed axion dark matter experiments.

Journal ArticleDOI
TL;DR: The cosmological standard model has recently come under pressure from measurements of the Hubble constant, and theoretically from the swampland conjecture that emphasizes consistency with quantum gravity as discussed by the authors.
Abstract: The cosmological standard model ($\mathrm{\ensuremath{\Lambda}}$CDM) has recently come under pressure from measurements of the Hubble constant ${H}_{0}$, and theoretically from the swampland conjecture that emphasizes consistency with quantum gravity. The authors sweep through the typical class of string theory motivated dark-energy models, (coupled) quintessence with a clever expansion in low redshift and show that these models worsen the ${H}_{0}$ tension, but they also point to a gateway that might be tested with future $21c\phantom{\rule{0}{0ex}}m$ observations.

Journal ArticleDOI
TL;DR: In this paper, the impact of early dark energy (EDE) on galaxy clustering using BOSS galaxy power spectra, analyzed using the effective field theory (EFT) of large-scale structure (LSS), and anisotropies of the cosmic microwave background (CMB) from Planck.
Abstract: We revisit the impact of early dark energy (EDE) on galaxy clustering using BOSS galaxy power spectra, analyzed using the effective field theory (EFT) of large-scale structure (LSS), and anisotropies of the cosmic microwave background (CMB) from Planck. Recent studies found that these data place stringent constraints on the maximum abundance of EDE allowed in the Universe. We argue here that their conclusions are a consequence of their choice of priors on the EDE parameter space, rather than any disagreement between the data and the model. For example, when considering EFT-LSS, CMB, and high-redshift supernovae data we find the EDE and $\Lambda$CDM models can provide statistically indistinguishable fits ($\Delta \chi^2 = 0.12$) with a relatively large value for the maximum fraction of energy density in the EDE ($f_{\rm ede} = 0.09$) and Hubble constant ($H_0 = 71$ km/s/Mpc) in the EDE model. Moreover, we demonstrate that the constraining power added from the inclusion of EFT-LSS traces to the potential tension between the power-spectrum amplitudes $A_s$ derived from BOSS and from Planck that arises even within the context of $\Lambda$CDM. Until this is better understood, caution should be used when interpreting EFT-BOSS+Planck constraints to models beyond $\Lambda$CDM. These findings suggest that EDE still provides a potential resolution to the Hubble tension and that it is worthwhile to test the predictions of EDE with future data-sets and further study its theoretical possibilities.

Journal ArticleDOI
TL;DR: In this paper, a first order phase transition is considered, allowing in a minimal model a reduction of the tension to 2.5 ϵ ϵ −2.5 ε.
Abstract: The authors discuss in detail a popular scenario to alleviate the current Hubble tension (different measurements of the expansion rate of the Universe show a 4.4 $\ensuremath{\sigma}$ discrepancy), namely ``early dark energy''. Hereby a false vacuum early on acts as an additional repulsive force (dark energy) but decays quickly enough to remain consistent with numerous other observational data. Contrary to the usual approach, a first order phase transition is considered, allowing in a minimal model a reduction of the tension to 2.5 $\ensuremath{\sigma}$.

Journal ArticleDOI
TL;DR: The authors constrain primordial black hole formation models within a hierarchical Bayesian inference framework based on deep learning techniques, finding best-fit values for distinctive features of these models, including the PBH initial mass function, the fraction of PBHs in dark matter, and the accretion efficiency.
Abstract: Primordial black holes (PBHs) might be formed in the early Universe and could comprise at least a fraction of the dark matter. Using the recently released GWTC-2 dataset from the third observing run of the LIGO-Virgo Collaboration, we investigate whether current observations are compatible with the hypothesis that all black hole mergers detected so far are of primordial origin. We constrain PBH formation models within a hierarchical Bayesian inference framework based on deep learning techniques, finding best-fit values for distinctive features of these models, including the PBH initial mass function, the fraction of PBHs in dark matter, and the accretion efficiency. The presence of several spinning binaries in the GWTC-2 dataset favors a scenario in which PBHs accrete and spin up. Our results indicate that PBHs may comprise only a fraction smaller than 0.3% of the total dark matter, and that the predicted PBH abundance is still compatible with other constraints.

Journal ArticleDOI
TL;DR: In this article, it was shown that both JT gravity and a simplified version of CGHS admit a regime where the contribution of connected replica wormholes to the free energy is larger than that of disconnected topologies.
Abstract: Euclidean wormholes---geometries which connect disconnected boundaries---present a challenge to a standard quantum mechanical interpretation of the theory. One potential resolution is that the gravitational path integral computes the ensemble average of many theories. The connected topologies contribute to the simplest possible observable: the free energy, which is computed using a replica trick. This is distinct from the replica trick used to compute entanglement entropies and appears in the computation of any extensive quantity. We argue that both JT gravity and a simplified version of CGHS admit a regime where the contribution of connected replica wormholes to the free energy is larger than that of disconnected topologies. In both theories we find evidence of replica symmetry breaking, which is reminiscent of the behavior of certain spin glasses. We discuss possible insights about ensemble averaging in gravity from this perspective.

Journal ArticleDOI
TL;DR: In this article, the authors considered the power-law form of the cosmological model and analyzed its behavior at both the background and perturbation level, finding that the effective evolution of the model is the same as that of the CDM model for any value of n −1.
Abstract: The present work studies one of Einstein's alternative formulations based on the nonmetricity scalar $Q$ generalized as $f(Q)$ theory. More specifically, we consider the power-law form of $f(Q)$ gravity, i.e., $f(Q)=Q+\ensuremath{\alpha}{Q}^{n}$. Here, we analyze the behavior of the cosmological model at the background and perturbation level. Using the dynamical system analysis, at the background level, we find the effective evolution of the model is the same as that of the $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ for $|n|l1$. Interestingly, the geometric component of the theory solely determined the late-time acceleration of the Universe. We also examine the integrability of the model by employing the method of singularity analysis. In particular, we find the conditions under which field equations pass the Painlev\'e test and hence possess the Painlev\'e property. While the equations pass the Painlev\'e test in the presence of dust for any value of $n$, the test is valid after the addition of radiation fluid only for $nl1$. Finally, at the perturbation level, the behavior of matter growth index signifies a deviation of the model from the $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ even for $|n|l1$.

Journal ArticleDOI
TL;DR: In this article, a flow-based sampling algorithm for lattice gauge theories that is gauge invariant by construction is presented. But this algorithm is restricted to two dimensions and cannot be used to sample distributions of single SU(N) variables.
Abstract: We develop a flow-based sampling algorithm for $\mathrm{SU}(N)$ lattice gauge theories that is gauge invariant by construction. Our key contribution is constructing a class of flows on an $\mathrm{SU}(N)$ variable [or on a $\mathrm{U}(N)$ variable by a simple alternative] that respects matrix conjugation symmetry. We apply this technique to sample distributions of single $\mathrm{SU}(N)$ variables and to construct flow-based samplers for SU(2) and SU(3) lattice gauge theory in two dimensions.

Journal ArticleDOI
TL;DR: In this article, the relativistic scattering of unequal-mass scalar particles through graviton exchange in the small-angle high-energy regime was considered and the self-consistency of expansion around the eikonal limit was shown, up to the next-to-leading power correction of the light particle energy.
Abstract: We consider the relativistic scattering of unequal-mass scalar particles through graviton exchange in the small-angle high-energy regime. We show the self-consistency of expansion around the eikonal limit and compute the scattering amplitude up to the next-to-leading power correction of the light particle energy, including gravitational effects of the same order. The first power correction is suppressed by a single power of the ratio of momentum transfer to the energy of the light particle in the rest frame of the heavy particle, independent of the heavy particle mass. We find that only gravitational corrections contribute to the exponentiated phase in impact parameter space in four dimensions. For large enough heavy-particle mass, the saddle point for the impact parameter is modified compared to the leading order by a multiple of the Schwarzschild radius determined by the mass of the heavy particle, independent of the energy of the light particle.

Journal ArticleDOI
TL;DR: In this paper, it was shown that rotating black holes do not experience any tidal deformation when they are perturbed by a weak and adiabatic gravitational field, and the dissipative part of the black hole's tidal response is nonvanishing due to the absorptive nature of the event horizon.
Abstract: We show that rotating black holes do not experience any tidal deformation when they are perturbed by a weak and adiabatic gravitational field. The tidal deformability of an object is quantified by the so-called ``Love numbers,'' which describe the object's linear response to its external tidal field. In this work, we compute the Love numbers of Kerr black holes and find that they vanish identically. We also compute the dissipative part of the black hole's tidal response, which is nonvanishing due to the absorptive nature of the event horizon. Our results hold for arbitrary values of black hole spin, for both the electric-type and magnetic-type perturbations, and to all orders in the multipole expansion of the tidal field. The boundary conditions at the event horizon and at asymptotic infinity are incorporated in our study, as they are crucial for understanding the way in which these tidal effects are mapped onto gravitational-wave observables. In closing, we address the ambiguity issue of Love numbers in general relativity, which we argue is resolved when those boundary conditions are taken into account. Our findings provide essential inputs for current efforts to probe the nature of compact objects through the gravitational waves emitted by binary systems.

Journal ArticleDOI
TL;DR: In this paper, the problem of time in quantum gravity calls for a relational solution, and the trinity of relational quantum dynamics is defined, which consists of three faces of the same dynamics: relational observables in the clock-neutral picture of Dirac quantization, Page and Wootters' (PW) Schrodinger picture formalism, and relational Heisenberg picture obtained via symmetry reduction.
Abstract: The problem of time in quantum gravity calls for a relational solution. Using quantum reduction maps, we establish a previously unknown equivalence between three approaches to relational quantum dynamics: (1) relational observables in the clock-neutral picture of Dirac quantization, (2) Page and Wootters' (PW) Schr\"odinger picture formalism, and (3) the relational Heisenberg picture obtained via symmetry reduction. Constituting three faces of the same dynamics, we call this equivalence the trinity. In the process, we develop a quantization procedure for relational Dirac observables using covariant positive operator-valued measures which encompass nonideal clocks and resolve the nonmonotonicity issue of realistic quantum clocks reported by Unruh and Wald. The quantum reduction maps reveal this procedure as the quantum analog of gauge-invariantly extending gauge-fixed quantities. We establish algebraic properties of these relational observables. We extend a recent ``clock-neutral'' approach to changing temporal reference frames, transforming relational observables and states, and demonstrate a clock dependent temporal nonlocality effect. We show that Kucha\ifmmode \check{r}\else \v{r}\fi{}'s criticism, alleging that the conditional probabilities of the PW formalism violate the constraint, is incorrect. They are a quantum analog of a gauge-fixed description of a gauge-invariant quantity and equivalent to the manifestly gauge-invariant evaluation of relational observables in the physical inner product. The trinity furthermore resolves a previously reported normalization ambiguity and clarifies the role of entanglement in the PW formalism. The trinity finally permits us to resolve Kucha\ifmmode \check{r}\else \v{r}\fi{}'s criticism that the PW formalism yields wrong propagators by showing how conditional probabilities of relational observables give the correct transition probabilities. Unlike previous proposals, our resolution does not invoke approximations, ideal clocks or ancilla systems, is manifestly gauge invariant, and easily extends to an arbitrary number of conditionings.

Journal ArticleDOI
TL;DR: In this article, the authors studied chiral algebras associated with Argyres-Douglas theories engineered from M5 branes and obtained the Schur index of these theories by computing the vacua character of the corresponding chiral algebra.
Abstract: We study chiral algebras associated with Argyres-Douglas theories engineered from M5 branes. For the theory engineered using 6D (2,0) type $J$ theory on a sphere with a single irregular singularity (without mass parameter), its chiral algebra is the minimal model of W algebra of $J$ type. For the theory engineered using an irregular singularity and a regular full singularity, its chiral algebra is the affine Kac-Moody algebra of $J$ type. We can obtain the Schur index of these theories by computing the vacua character of the corresponding chiral algebra.

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TL;DR: In this paper, the authors show that the need for sizable hadronic contributions and correlations among them decays in light of the recent measurements from the LHCb experiment, showing that new data strengthen the need to have sizable correlated contributions and correlation among them.
Abstract: We perform an analysis within the Standard Model of ${B}^{0,+}\ensuremath{\rightarrow}{K}^{*0,+}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ decays in light of the recent measurements from the LHCb experiment, showing that new data strengthen the need for sizable hadronic contributions and correlations among them. We then extend our analysis to new physics via the Standard Model effective theory, and carry out a state-of-the-art fit of available $b\ensuremath{\rightarrow}s{\ensuremath{\ell}}^{+}{\ensuremath{\ell}}^{\ensuremath{-}}$ data, including possible hadronic contributions. We find the case of a fully left-handed operator standing out as the simplest scenario with a significance of almost $6\ensuremath{\sigma}$.

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TL;DR: In this article, the authors show that a TeV-scale future muon collider will discover all possible singlet model solutions to the Muon anomaly, and that such a machine would either discover new particles associated with high-scale electroweak model solutions, or empirically prove that nature is fine-tuned, both of which would have profound consequences for fundamental physics.
Abstract: The longstanding muon $g\ensuremath{-}2$ anomaly may indicate the existence of new particles that couple to muons, which could either be light $(\ensuremath{\lesssim}\mathrm{GeV})$ and weakly coupled, or heavy $(\ensuremath{\gg}100\text{ }\text{ }\mathrm{GeV})$ with large couplings. If light new states are responsible, upcoming intensity frontier experiments will discover further evidence of new physics. However, if heavy particles are responsible, many candidates are beyond the reach of existing colliders. We show that, if the $(g\ensuremath{-}2{)}_{\ensuremath{\mu}}$ anomaly is confirmed and no explanation is found at low-energy experiments, a high-energy muon collider program is guaranteed to make fundamental discoveries about our Universe. New physics scenarios that account for the anomaly can be classified as either ``singlet'' or ``electroweak'' (EW) models, involving only EW singlets or new EW-charged states respectively. We argue that a TeV-scale future muon collider will discover all possible singlet model solutions to the anomaly. If this does not yield a discovery, the next step would be a $\mathcal{O}(10\text{ }\text{ }\mathrm{TeV})$ muon collider. Such a machine would either discover new particles associated with high-scale EW model solutions to the anomaly, or empirically prove that nature is fine-tuned, both of which would have profound consequences for fundamental physics.

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D. Dutcher, L. Balkenhol, P. A. R. Ade, Z. Ahmed, Ethan Anderes, Adam Anderson, M. Archipley, Jessica Avva, K. Aylor, Peter S. Barry, RB Thakur, Karim Benabed1, Andreas Bender, Bradford Benson, Federico Bianchini, Lindsey Bleem, François R. Bouchet1, Lincoln Bryant, Karen Byrum, John E. Carlstrom, Faustin Carter, Thomas Cecil, C. L. Chang, P. Chaubal, Gang Chen, H-M. Cho, T.-L. Chou, J. F. Cliche, T. M. Crawford, A. Cukierman, C. Daley, T. de Haan, E. V. Denison, K. Dibert, Junjia Ding, M. A. Dobbs, W. B. Everett, Chang Feng, K. R. Ferguson, A. Foster, J. Fu, Silvia Galli1, A. E. Gambrel, Robert Gardner, Neil Goeckner-Wald, R. Gualtieri, S. Guns, Nikhel Gupta, R. Guyser, N. W. Halverson, A. H. Harke-Hosemann, N. L. Harrington, Jason W. Henning, Gene C. Hilton, E. Hivon1, G. P. Holder, W. L. Holzapfel, J. C. Hood, D. Howe, N. Huang, Kent D. Irwin, Oliver Jeong, M. Jonas, Anthony P. Jones, Trupti Khaire, Lloyd Knox, A. M. Kofman, M. Korman, Donna Kubik, S. E. Kuhlmann, C. L. Kuo, A. T. Lee, E. M. Leitch, A. Lowitz, C. Lu, S. S. Meyer, Daniel Michalik, M. Millea, Joshua Montgomery, Andrew Nadolski, T. Natoli, H. Nguyen, G. I. Noble, Novosad, Y. Omori, S. Padin, Z. Pan, P. Paschos, John E. Pearson, C. M. Posada, K. Prabhu, W. Quan, Srinivasan Raghunathan, Alexandra S. Rahlin, Christian L. Reichardt, D. Riebel, B. Riedel, M. Rouble, J. E. Ruhl, J. T. Sayre, E. Schiappucci, Erik Shirokoff, Graeme Smecher, J. A. Sobrin, A. A. Stark, J. Stephen, K. T. Story, A. Suzuki, K. L. Thompson, B. Thorne, C. Tucker, C. Umilta, L. R. Vale, K. Vanderlinde, J. D. Vieira, Gensheng Wang, Nathan Whitehorn, W. L. K. Wu, Yefremenko, K. W. Yoon, Young 
TL;DR: In this paper, the authors used the SPT-3G data collected by the South Pole Telescope to obtain binned values of the polarization power spectrum and temperature-E$-mode cross-power spectrum of the cosmic microwave background.
Abstract: We present measurements of the $E$-mode ($EE$) polarization power spectrum and temperature-$E$-mode ($TE$) cross-power spectrum of the cosmic microwave background using data collected by SPT-3G, the latest instrument installed on the South Pole Telescope. This analysis uses observations of a 1500 deg$^2$ region at 95, 150, and 220 GHz taken over a four month period in 2018. We report binned values of the $EE$ and $TE$ power spectra over the angular multipole range $300 \le \ell < 3000$, using the multifrequency data to construct six semi-independent estimates of each power spectrum and their minimum-variance combination. These measurements improve upon the previous results of SPTpol across the multipole ranges $300 \le \ell \le 1400$ for $EE$ and $300 \le \ell \le 1700$ for $TE$, resulting in constraints on cosmological parameters comparable to those from other current leading ground-based experiments. We find that the SPT-3G dataset is well-fit by a $\Lambda$CDM cosmological model with parameter constraints consistent with those from Planck and SPTpol data. From SPT-3G data alone, we find $H_0 = 68.8 \pm 1.5 \mathrm{km\,s^{-1}\,Mpc^{-1}}$ and $\sigma_8 = 0.789 \pm 0.016$, with a gravitational lensing amplitude consistent with the $\Lambda$CDM prediction ($A_L = 0.98 \pm 0.12$). We combine the SPT-3G and the Planck datasets and obtain joint constraints on the $\Lambda$CDM model. The volume of the 68% confidence region in six-dimensional $\Lambda$CDM parameter space is reduced by a factor of 1.5 compared to Planck-only constraints, with only slight shifts in central values. We note that the results presented here are obtained from data collected during just half of a typical observing season with only part of the focal plane operable, and that the active detector count has since nearly doubled for observations made with SPT-3G after 2018.

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TL;DR: In this paper, the authors exploit the clustering scale of the gravitational wave sources with galaxies of a known redshift to infer the expansion history from redshift unknown Gravitational wave sources.
Abstract: Gravitational waves can provide an accurate measurement of the luminosity distance to the source but cannot provide the source redshift unless the degeneracy between mass and redshift can be broken. This makes it essential to infer the redshift of the source independently to measure the expansion history of the Universe. We show that by exploiting the clustering scale of the gravitational wave sources with galaxies of a known redshift, we can infer the expansion history from redshift unknown gravitational wave sources. By using gravitational wave sources of unknown redshift that are detectable from the network of gravitational wave detectors with Advanced LIGO design sensitivity, we will be able to obtain accurate and precise measurements of the local Hubble constant, the expansion history of the Universe, and the gravitational wave bias parameter, which captures the distribution of gravitational wave sources with respect to the redshift tracer distribution. While we showcase its application to low redshift gravitational waves, this technique will be applicable also to the high redshift gravitational wave sources detectable from Laser Interferometer Space Antenna (LISA), Cosmic Explorer (CE), and Einstein Telescope (ET). Moreover, this method will also be applicable to samples of supernovae and fast radio bursts with unknown or photometric redshifts.

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TL;DR: In this article, the authors consider a Kerr black hole embedded in a weak and slowly varying, but otherwise arbitrary, multipolar tidal environment and compute the linear response of the black hole to the tidal field.
Abstract: The open question of whether a Kerr black hole can become tidally deformed or not has profound implications for fundamental physics and gravitational-wave astronomy. We consider a Kerr black hole embedded in a weak and slowly varying, but otherwise arbitrary, multipolar tidal environment. By solving the static Teukolsky equation for the gauge-invariant Weyl scalar ${\ensuremath{\psi}}_{0}$ and by reconstructing the corresponding metric perturbation in an ingoing radiation gauge, for a general harmonic index $\ensuremath{\ell}$, we compute the linear response of a Kerr black hole to the tidal field. This linear response vanishes identically for a Schwarzschild black hole and for an axisymmetric perturbation of a spinning black hole. For a nonaxisymmetric perturbation of a spinning black hole, however, the linear response does not vanish, and it contributes to the Geroch-Hansen multipole moments of the perturbed Kerr geometry. As an application, we compute explicitly the rotational black hole tidal Love numbers that couple the induced quadrupole moments to the quadrupolar tidal fields, to linear order in the black hole spin, and we introduce the corresponding notion of a tidal Love tensor. Finally, we show that those induced quadrupole moments are closely related to the well-known physical phenomenon of tidal torquing of a spinning body interacting with a tidal gravitational environment.

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TL;DR: In this article, the authors revisited the possibilities of accommodating the experimental indications of the lepton flavor universality violation in $b$-hadron decays in the minimal scenarios in which the Standard Model is extended by the presence of a single leptoquark state.
Abstract: We revisit the possibilities of accommodating the experimental indications of the lepton flavor universality violation in $b$-hadron decays in the minimal scenarios in which the Standard Model is extended by the presence of a single $\mathcal{O}(1\text{ }\text{ }\mathrm{TeV})$ leptoquark state. To do so we combine the most recent low energy flavor physics constraints, including ${R}_{{K}^{(*)}}^{\mathrm{exp}}$ and ${R}_{{D}^{(*)}}^{\mathrm{exp}}$, and combine them with the bounds on the leptoquark masses and their couplings to quarks and leptons as inferred from the direct searches at the LHC and the studies of the large ${p}_{T}$ tails of the $pp\ensuremath{\rightarrow}\ensuremath{\ell}\ensuremath{\ell}$ differential cross section. We find that none of the scalar leptoquarks of ${m}_{\mathrm{LQ}}\ensuremath{\simeq}1\textdiv{}2\text{ }\text{ }\mathrm{TeV}$ can accommodate the $B$-anomalies alone. Only the vector leptoquark, known as ${U}_{1}$, can provide a viable solution which, in the minimal setup, provides an interesting prediction, i.e., a lower bound to the lepton flavor violating $b\ensuremath{\rightarrow}s{\ensuremath{\mu}}^{\ifmmode\pm\else\textpm\fi{}}{\ensuremath{\tau}}^{\ensuremath{\mp}}$ decay modes, such as $\mathcal{B}(B\ensuremath{\rightarrow}K\ensuremath{\mu}\ensuremath{\tau})\ensuremath{\gtrsim}0.7\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}$.

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TL;DR: In this article, a simple prescription based on the results of numerical simulations was provided to compute the threshold for primordial black hole formation, taking into account both the nonlinearities between the Gaussian curvature perturbation and the density contrast, which increase the value of the threshold by about a factor two with respect to the one computed on superhorizon scales.
Abstract: Primordial black holes could have been formed in the early universe from nonlinear cosmological perturbations reentering the cosmological horizon when the Universe was still radiation dominated. Starting from the shape of the power spectrum on superhorizon scales, we provide a simple prescription, based on the results of numerical simulations, to compute the threshold ${\ensuremath{\delta}}_{c}$ for primordial black hole formation. Our procedure takes into account both the nonlinearities between the Gaussian curvature perturbation and the density contrast and, for the first time in the literature, the nonlinear effects arising at horizon crossing, which increase the value of the threshold by about a factor two with respect to the one computed on superhorizon scales.

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TL;DR: In this paper, the authors provide a theoretical model of gravity in which it is possible to describe in a unified way inflation, an early and a late dark energy era, in the presence of a light axion particle which plays the role of the dark matter component of the universe.
Abstract: We provide a theoretical model of $F(R)$ gravity in which it is possible to describe in a unified way inflation, an early and a late dark energy era, in the presence of a light axion particle which plays the role of the dark matter component of the Universe. Particularly, the early time phenomenology is dominated by an ${R}^{2}$ term, while the presence of the other terms $f(R)$ ensure the occurrence of the early and late-time dark energy eras. The inflationary phenomenology is compatible with the Planck 2018 data for inflation, while the late-time dark energy era is compatible with the Planck 2018 constraints on the cosmological parameters. Also, the model exhibits an early dark energy era, at $z\ensuremath{\sim}2.5$ approximately, followed by a deceleration era, which starts at approximately $z\ensuremath{\sim}1.5$, which in turn is followed by a late-time dark energy era for redshifts $z\ensuremath{\sim}0.5$, which lasts for approximately 5 billion years up to present time. A notable feature of our model is that the dark energy era is free from dark energy oscillations, at least in the redshift interval $z=[0,10]$. In addition, we also discuss several features related to observational data at $z\ensuremath{\sim}2.34$, at which redshift intricate observational data exist in the literature. Moreover, the numerical code for the dark energy phenomenology, written in python3, is presented in the end of the article. Finally, the model has another interesting characteristic, a sudden jump of the value of the Hubble rate in the redshift interval $z\ensuremath{\sim}[2,2.6]$ where its value suddenly increases and then decreases until $z\ensuremath{\sim}0$.