8,581 research outputs found

    The Double-Dark Portal

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    In most models of the dark sector, dark matter is charged under some new symmetry to make it stable. We explore the possibility that not just dark matter, but also the force carrier connecting it to the visible sector is charged under this symmetry. This dark mediator then acts as a Double-Dark Portal. We realize this setup in the \emph{dark mediator Dark matter} model (dmDM), featuring a fermionic DM candidate Ο‡\chi with Yukawa couplings to light scalars Ο•i\phi_i. The scalars couple to SM quarks via the operator qΛ‰qΟ•iβˆ—Ο•j/Ξ›ij\bar q q \phi_i^* \phi_j/\Lambda_{ij}. This can lead to large direct detection signals via the 2β†’32\rightarrow3 process Ο‡Nβ†’Ο‡NΟ•\chi N \rightarrow \chi N \phi if one of the scalars has mass ≲10 \lesssim 10 keV. For dark matter Yukawa couplings yΟ‡βˆΌ10βˆ’3βˆ’10βˆ’2y_\chi \sim 10^{-3} - 10^{-2}, dmDM features a thermal relic dark matter candidate while also implementing the SIDM scenario for ameliorating inconsistencies between dwarf galaxy simulations and observations. We undertake the first systematic survey of constraints on light scalars coupled to the SM via the above operator. The strongest constraints are derived from a detailed examination of the light mediator's effects on stellar astrophysics. LHC experiments and cosmological considerations also yield important bounds. Observations of neutron star cooling exclude the minimal model with one dark mediator, but a scenario with two dark mediators remains viable and can give strong direct detection signals. We explore the direct detection consequences of this scenario and find that a heavy O(100)\mathcal{O}(100) GeV dmDM candidate fakes different O(10)\mathcal{O}(10) GeV WIMPs at different experiments. Large regions of dmDM parameter space are accessible above the irreducible neutrino background.Comment: 24 pages, 19 figures, + references and appendices, update the SIDM discussion and reference

    Spontaneous R-symmetry Breaking with Multiple Pseudomoduli

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    We examine generalized O'Raifeartaigh models that feature multiple tree-level flat directions and only contain fields with R-charges 0 or 2. We show that spontaneous R-breaking at up to one-loop order is impossible in such theories. Specifically, we prove that the R-symmetric origin of field space is always a local minimum of the one-loop Coleman-Weinberg potential, generalizing an earlier result for the case of a single flat direction. This result has consequences for phenomenology and helps elucidate the behavior of various models of dynamical SUSY breaking

    Quantifying the Morphologies and Dynamical Evolution of Galaxy Clusters. I. The Method

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    We describe and test a method to quantitatively classify clusters of galaxies according to their projected morphologies. This method will be subsequently used to place constraints on cosmological parameters (Ξ©\Omega and the power spectrum of primordial fluctuations on scales at or slightly smaller than that of clusters) and to test theories of cluster formation. We specifically address structure that is easily discernible in projection and dynamically important to the cluster. The method is derived from the two-dimensional multipole expansion of the projected gravitational potential and yields dimensionless {\it power ratios} as morphological statistics. If the projected mass profile is used to characterize the cluster morphology, the power ratios are directly related to the cluster potential. However, since detailed mass profiles currently exist for only a few clusters, we use the X-ray--emitting gas as an alternative tracer of cluster morphology. In this case, the relation of the power ratios to the potential is qualitatively preserved. We demonstrate the feasibility of the method by analyzing simulated observations of simple models of X-ray clusters using the instrument parameters of the ROSAT PSPC. For illustrative purposes, we apply the method to ROSAT PSPC images of A85, A514, A1750, and A2029. These clusters, which differ substantially in their X-ray morphologies, are easily distinguished by their respective power ratios. We discuss the suitability of this method to address the connection between cluster morphology and cosmology and to assess whether an individual cluster is sufficiently relaxed for analysis of its intrinsic shape using hydrostatic methods. Approximately 50 X-ray observations of Abell clusters with the PSPC will be amenable to morphological analysis using the method of this paper.Comment: To appear in ApJ October 20, 1995. 29 pages (7 figures missing), PostScrip

    Direct Detection with Dark Mediators

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    We introduce dark mediator Dark matter (dmDM) where the dark and visible sectors are connected by at least one light mediator Ο•\phi carrying the same dark charge that stabilizes DM. Ο•\phi is coupled to the Standard Model via an operator qΛ‰qΟ•Ο•βˆ—/Ξ›\bar q q \phi \phi^*/\Lambda, and to dark matter via a Yukawa coupling yχχc‾χϕy_\chi \overline{\chi^c}\chi \phi. Direct detection is realized as the 2β†’32\rightarrow3 process Ο‡Nβ†’Ο‡Λ‰NΟ•\chi N \rightarrow \bar \chi N \phi at tree-level for mϕ≲10Β keVm_\phi \lesssim 10 \ \mathrm{keV} and small Yukawa coupling, or alternatively as a loop-induced 2β†’22\rightarrow2 process Ο‡Nβ†’Ο‡N\chi N \rightarrow \chi N. We explore the direct-detection consequences of this scenario and find that a heavy O(100Β GeV)\mathcal{O}(100 \ \mathrm{GeV}) dmDM candidate fakes different O(10Β GeV)\mathcal{O}(10 \ \mathrm{GeV}) standard WIMPs in different experiments. Large portions of the dmDM parameter space are detectable above the irreducible neutrino background and not yet excluded by any bounds. Interestingly, for the mΟ•m_\phi range leading to novel direct detection phenomenology, dmDM is also a form of Self-Interacting Dark Matter (SIDM), which resolves inconsistencies between dwarf galaxy observations and numerical simulations.Comment: 9 pages, 8 figures + reference

    Critical Entanglement for the Half-Filled Extended Hubbard Model

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    We study the ground state of the one-dimensional extended Hubbard model at half-filling using the entanglement entropy calculated by Density Matrix Renormalization Group (DMRG) techniques. We apply a novel curve fitting and scaling method to accurately identify a 2nd2^{nd} order critical point as well as a Berezinskii-Kosterlitz-Thouless (BKT) critical point. Using open boundary conditions and medium-sized lattices with very small truncation errors, we are able to achieve similar accuracy to previous authors. We also report observations of finite-size and boundary effects that can be remedied with careful pinning.Comment: 10 pages, 12 figure

    Cosmological Signatures of a Mirror Twin Higgs

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    We explore the cosmological signatures associated with the twin baryons, electrons, photons and neutrinos in the Mirror Twin Higgs framework. We consider a scenario in which the twin baryons constitute a subcomponent of dark matter, and the contribution of the twin photon and neutrinos to dark radiation is suppressed due to late asymmetric reheating, but remains large enough to be detected in future cosmic microwave background (CMB) experiments. We show that this framework can lead to distinctive signals in large scale structure and in the cosmic microwave background. Baryon acoustic oscillations in the mirror sector prior to recombination lead to a suppression of structure on large scales, and leave a residual oscillatory pattern in the matter power spectrum. This pattern depends sensitively on the relative abundances and ionization energies of both twin hydrogen and helium, and is therefore characteristic of this class of models. Although both mirror photons and neutrinos constitute dark radiation in the early universe, their effects on the CMB are distinct. This is because prior to recombination the twin neutrinos free stream, while the twin photons are prevented from free streaming by scattering off twin electrons. In the Mirror Twin Higgs framework the relative contributions of these two species to the energy density in dark radiation is predicted, leading to testable effects in the CMB. These highly distinctive cosmological signatures may allow this class of models to be discovered, and distinguished from more general dark sectors.Comment: 30 pages, 6 figures; added new discussions and figures; references added; matches published versio
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