1,721,012 research outputs found

    Challenging the Cosmological Constant

    No full text
    Kaloper, Nemanja. (2012). Challenging the Cosmological Constant. Retrieved from the University Digital Conservancy, https://hdl.handle.net/11299/129785

    Anisotropies in nonthermal distortions of cosmic light from photon-axion conversion

    No full text
    Ultralight axions which couple sufficiently strongly to photons can leave imprints on the sky at diverse frequencies by mixing with cosmic light in the presence of background magnetic fields. We explore such direction dependent grey-body distortions of the cosmic microwave background spectrum, enhanced by resonant conditions in the intergalactic medium plasma. We also find that if such axions are produced in the early Universe and represent a subdominant dark radiation component today, they could convert into x-rays in supervoids and brighten them at x-ray frequencies

    Quantum Field Theory of Interacting Dark Matter/Dark Energy: Dark Monodromies

    No full text
    We discuss how to formulate a quantum field theory of dark energy interacting with dark matter. We show that the proposals based on the assumption that dark matter is made up of heavy particles with masses which are very sensitive to the value of dark energy are strongly constrained. Quintessence-generated long range forces and radiative stability of the quintessence potential require that such dark matter and dark energy are completely decoupled. However, if dark energy and a fraction of dark matter are very light axions, they can have significant mixings which are radiatively stable and perfectly consistent with quantum field theory. Such models can naturally occur in multi-axion realizations of monodromies. The mixings yield interesting signatures which are observable and are within current cosmological limits but could be constrained further by future observations.We discuss how to formulate a quantum field theory of dark energy interacting with dark matter. We show that the proposals based on the assumption that dark matter is made up of heavy particles with masses which are very sensitive to the value of dark energy are strongly constrained. Quintessence-generated long-range forces and radiative stability of the quintessence potential require that such dark matter and dark energy are completely decoupled. However, if dark energy and a fraction of dark matter are very light axions, they can have significant mixings which are radiatively stable and perfectly consistent with quantum field theory. Such models can naturally occur in multi-axion realizations of monodromies. The mixings yield interesting signatures which are observable and are within current cosmological limits but could be constrained further by future observations.We discuss how to formulate a quantum field theory of dark energy interacting with dark matter. We show that the proposals based on the assumption that dark matter is made up of heavy particles with masses which are very sensitive to the value of dark energy are strongly constrained. Quintessence-generated long range forces and radiative stability of the quintessence potential require that such dark matter and dark energy are completely decoupled. However, if dark energy and a fraction of dark matter are very light axions, they can have significant mixings which are radiatively stable and perfectly consistent with quantum field theory. Such models can naturally occur in multi-axion realizations of monodromies. The mixings yield interesting signatures which are observable and are within current cosmological limits but could be constrained further by future observations

    Power-law Inflation Satisfies Penrose's Weyl Curvature Hypothesis

    Full text link
    Based on entropy considerations and the arrow of time Penrose argued that the universe must have started in a special initial singularity with vanishing Weyl curvature. This is often interpreted to be at odds with inflation. Here we argue just the opposite, that Penrose's persuasions are in fact consistent with inflation. Using the example of power law inflation, we show that inflation begins with a past null singularity, where Weyl tensor vanishes when the metric is initially exactly conformally flat. This initial state precisely obeys Penrose's conditions. The initial null singularity breaks TT-reversal spontaneously and picks the arrow of time. It can be regulated and interpreted as a creation of a universe from nothing, initially fitting in a bubble of Planckian size when it materializes. Penrose's initial conditions are favored by the initial O(4)O(4) symmetry of the bubble, selected by extremality of the regulated Euclidean action. The predicted observables are marginally in tension with the data, but they can fit if small corrections to power law inflation kick in during the last 60 efolds.Comment: 19 pages LaTeX, 5 figures png format; v2: added comments, discussion and references; published versio

    Monodromy inflation at strong coupling: 4π4\pi in the sky

    No full text
    We present a simple effective field theory formulation of a general family of single-field flux monodromy models for which strong coupling effects at large field values can flatten the potential and activate higher-derivative operators. Both of these effects can suppress the tensor amplitude. These models are radiatively and nonperturbatively stable and can sustain ≳60 e folds of inflation. The dynamics combines features of both large-field chaotic inflation and k inflation. Reducing the tensor-scalar ratio below the observational bound r≲0.1 while keeping the scalar spectral index ns within experimental bounds either yields equilateral non-Gaussianity fNLeq≃O(1), close to the current observational bounds, or gives very small r.We present a simple effective field theory formulation of a general family of single field flux monodromy models for which strong coupling effects at large field values can flatten the potential and activate operators with higher powers of derivatives. These models are radiatively and non-perturbatively stable and can easily sustain \ga 60 efolds of inflation. The dynamics combines features of both large field chaotic inflation and kk-inflation, both of which can suppress the tensor amplitude. Reducing the tensor-scalar ratio below the observational bound r0.1r \lesssim 0.1 while keeping the scalar spectral index nsn_s within experimental bounds either yields equilateral nongaussianity fNLeqO(1)f_{NL}^{eq} \simeq {\cal O}(1), close to the current observational bounds, or ultimately gives very small rr

    Super-GZK photons from photon–axion mixing

    No full text
    We show that photons with energies above the GZK cutoff can reach us from very distant sources if they mix with light axions in extragalactic magnetic fields. The effect which enables this is the conversion of photons into axions, which are sufficiently weakly coupled to travel large distances unimpeded. These axions then convert back into high energy photons close to the Earth. We show that photon-axion mixing facilitates the survival of super-GZK photons most efficiently with a photon-axion coupling scale M ≳ 1011 GeV, which is in the same range as the scale for the photon-axion mixing explanation for the dimming of supernovae without cosmic acceleration. We discuss possible observational consequences of this effect

    Very Hairy Inflation

    Full text link
    We revisit the rollercoaster cosmology based on multiple stages of monodromy inflation. Working within the framework of effective flux monodromy field theory, we include the full range of strong coupling corrections to the inflaton sector. We find that flattened potentials Vϕp+V \sim \phi^p + \ldots with p1/2p \lesssim 1/2, limited to N2540 N \lesssim 25 - 40 efolds in the first stage of inflation, continue to fit the CMB. They yield 0.96ns0.970.96 \lesssim n_s \lesssim 0.97, and produce relic gravity waves with 0.006r0.0350.006 \lesssim r \lesssim 0.035, in full agreement with the most recent bounds from BICEP/{\it Keck}. The nonlinear derivative corrections generated by strong dynamics in EFT also lead to equilateral non-Gaussianity fNLeqO(1)O(10)f_{NL}^{eq} \simeq {\cal O}(1) - {\cal O}(10), close to the current observational bounds. Finally, in multi-stage rollercoaster, an inflaton-hidden sector U(1)U(1) coupling can produce a tachyonic chiral vector background, which converts rapidly into tensors during the short interruption by matter domination. The produced stochastic gravity waves are chiral, and so they may be clearly identifiable by gravity wave instruments like LISA, Big Bang Observatory, Einstein Telescope, NANOgrav or SKA, depending on the precise model realization. We also point out that the current attempts to resolve the H0H_0 tension using early dark energy generically raise nsn_s. This may significantly alter the impact of BICEP/{\it Keck} data on models of inflation.Comment: 25+1 pages LaTeX, 8 figures. v2: Minor changes, references added, published in PR

    An Etude on Global Vacuum Energy Sequester

    Full text link
    Recently two of the authors proposed a mechanism of vacuum energy sequester as a means of protecting the observable cosmological constant from quantum radiative corrections. The original proposal was based on using global Lagrange multipliers, but later a local formulation was provided. Subsequently other interesting claims of a different non-local approach to the cosmological constant problem were made, based again on global Lagrange multipliers. We examine some of these proposals and find their mutual relationship. We explain that the proposals which do not treat the cosmological constant counterterm as a dynamical variable require fine tunings to have acceptable solutions. Furthermore, the counterterm often needs to be retuned at every order in the loop expansion to cancel the radiative corrections to the cosmological constant, just like in standard GR. These observations are an important reminder of just how the proposal of vacuum energy sequester avoids such problems

    de Sitter Space Decay and Cosmological Constant Relaxation in Unimodular Gravity with Charged Membranes

    No full text
    General covariant unimodular gravity frameworks, based on the Henneaux-Teitelboim formulation, are, in disguise, precisely 44-form field theories corrected with higher dimension operators. In the presence of charged tensional membranes, any de Sitter space in all such theories is unstable and decays. If the fluxes sourced by membranes are mutually incommensurate, de Sitter geometries comprise a very refined discretuum of states. Whenever the 44-form sector is dominated by terms linear in flux the almost-Minkowski space is the unique long-time attractor. As a result, a tiny cosmological constant is natural in all such frameworks, without appealing to anthropic reasoning.Comment: 28 pages, 5 figures; v2: Final version as published in PRD: title changed in journal, added discussion, added labels in a figure, extra reference
    corecore