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Neal Weiner (NYU)11/06/2014, 09:00
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David Morrissey (TRIUMF)11/06/2014, 09:40New physics can be light relative to the electroweak scale provided it couples very weakly to the Standard Model. An attractive and well-motivated example of this is a new dark vector boson. In this talk I will cover the theory of dark vectors with an emphasis on kinetic mixing with the photon and mass mixing with the Z boson. I will also touch briefly on the experimental implications of...Go to contribution page
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11/06/2014, 10:20
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Charles Epstein (MIT)11/06/2014, 11:00The DarkLight experiment aims to search for a dark photon in the low mass region 10-100 MeV/c^2. By using the Jefferson Lab FEL’s high-intensity 100 MeV, 1 MW electron beam incident on a gaseous hydrogen target, the process ep -> ep,e+/e- will be studied. To search for a dark photon, full track reconstruction of the four-particle final state will be performed in order to observe a resonance on...Go to contribution page
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James Beacham (New York University)11/06/2014, 11:20APEX is a fixed target experiment in Experimental Hall A at Thomas Jefferson National Accelerator Facility (JLab) in Virginia, USA, that is designed to search for a new gauge boson (A') with sub-GeV mass and coupling to ordinary matter of g'/e ~ (1 - 10^-4). Electrons impinge upon a fixed target of high-Z material to produce an A' via a process analogous to photon bremsstrahlung. The A' then...Go to contribution page
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John A Jaros (SLAC National Accelerator Laboratory)11/06/2014, 11:40HPS is an new experiment at Jefferson Laboratory designed to look for hidden sector photons in the mass range 20 - 1000 MeV with couplings a'/a in the range 10-5 to 10-10. Presently under construction, HPS will be installed this fall in Hall B at JLab, commission thereafter, and take data in 2015. Heavy photons are identified as invariant mass bumps and as separated decay verticies. The...Go to contribution page
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Michael Distler (University Mainz, Germany)11/06/2014, 12:00The A1 collaboration at the Mainz Microtron has concluded a pilot study in 2011 and data taking periods in 2012/2013 to search for a dark photon. The focus of the experiment was on the mass range between 50-200 MeV where dark matter provides a possible explanation for the discrepancy in the anomalous magnetic moment of the muon (g-2). The analysis is finished and the final exclusion limits...Go to contribution page
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11/06/2014, 12:20
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11/06/2014, 12:30
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Brian Batell (University of Chicago)11/06/2014, 14:00
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Philip Schuster (Perimeter Institute)11/06/2014, 14:30
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Jeremy Mardon (Stanford)11/06/2014, 14:55
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11/06/2014, 15:20
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Prof. David Brown (University of Louisville)11/06/2014, 16:00Extensions to the Standard Model allow for new particles, including low-mass Higgs bosons and dark photons, that may bridge the Standard Model to the Dark Sector. We present recent results of searches for such particles in electron-positron annihilation with the BaBar Detector at the SLAC National Accelerator Laboratory. We also report briefly on a measurement of antideuteron production at...Go to contribution page
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Igal Jaegle (University of Hawaii at Manoa)11/06/2014, 16:20We will present a new Belle (preliminary) limit in the search for a dark photon, A, and a dark Higgs, h', with A and h' prompt, mh' > 2mA, 100 MeV < mA < 3.5 GeV and 200 MeV < mh' < 10.5 GeV. We will also discuss possible future contributions of Belle II to dark sector particle searches.Go to contribution page
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Elizabeth Worcester (BNL)11/06/2014, 16:40The dark photon couples to Standard Model particles via kinetic mixing, so it may be produced in SM processes and decay to SM particles. Experiments that are designed for precise measurements of meson decay and detection of rare meson decay have high-resolution detectors and large data samples, making them well suited to search for dark photons. I will describe limits on dark photons from...Go to contribution page
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Yorito Yamaguchi (University of Tokyo)11/06/2014, 17:00Several theoretical models introduce an additional U(1) gauge boson, a "dark photon" which mixes with ordinary QED photons with very small mixing strength. The dark photon is considered as one of the strongest candidates to describe some astrophysical anomalies as well as the 3sigma deviation of the experimental muon g-2 value from the Standard Model calculation. The dark photon as the cause...Go to contribution page
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Dr Hye-Sung Lee (College of William and Mary / Jefferson Lab)11/06/2014, 17:20
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Ze'ev Surujon (Stony Brook University)12/06/2014, 09:00Exotic Higgs decays may be our main window to new physics. They are common and often well-motivated in various new physics scenarios, partly due to the small natural width of the Higgs. Some exotic decay modes are cascades resulting in high multiplicity of the final state, and are therefore potentially spectacular. Still, they could easily be missed, partly due to triggering...Go to contribution page
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Aysen Tatarinov (Texas A&M University)12/06/2014, 09:30The results of searches for invisible decays of the Higgs boson in the vector boson fusion and associated ZH production modes, where Z decays to a pair of charged leptons or a bbbar quark pair, are presented. Searches performed using data collected in proton-proton collisions at center-of-mass energies of 7 TeV and 8 TeV by the CMS experiment at the LHC. With no excess of the observed data...Go to contribution page
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Stefano Giagu (Sapienza University of Rome)12/06/2014, 09:55The discovery of a Higgs-like particle in ATLAS and CMS at the Large Hadron Collider opened a rich and interesting range of opportunities for discovery of exotic decays, i.e. decays that involve new light states beyond the SM. A large class of simplified and complete models gives rise to peculiar patterns of exotic decays of the Higgs boson, patterns that the ATLAS experiment is exploring...Go to contribution page
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Kyoungchul Kong (University of Kansas)12/06/2014, 10:20We suggest top quark decays as a venue to search for light dark force carriers. The top quark is the heaviest particle in the standard model whose decays are relatively poorly measured, allowing sufficient room for exotic decay modes from new physics. A very light (GeV scale) dark gauge boson (Z') is a recently highlighted hypothetical particle that can address some astrophysical anomalies as...Go to contribution page
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Steven Schramm (University of Toronto)12/06/2014, 11:10Numerous independent astrophysical experiments have observed and measured the influence of the phenomenon named Dark Matter, but its nature is still unknown. If the assumption that Dark Matter is a particle which has a weak coupling to the Standard Model is valid, then collider searches have the ability to search for the production of this new Weakly Interacting Massive Particle (WIMP). Any...Go to contribution page
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Jordan Damgov (Texas Tech University)12/06/2014, 11:30
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Gordon Watts (University of Washington)12/06/2014, 11:50Hidden Valley models contain a hidden sector that communicates with the Standard Model via a scalar. The hidden sector phenomenology is unconstrained. It can be as complex or simple as desired, and prompt or long lived. In this case we explore the ATLAS program to search for long lived versions of the Hidden Valley model. The benchmark model is fairly simple, produces two hidden valley pions...Go to contribution page
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John Paul Chou (Rutgers University)12/06/2014, 12:10
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Fedor Ratnikov (Inst. für Exp. Kernphysik)12/06/2014, 14:00In this talk I will discuss Implications of CMS Run 1 SUSY searches for the SUSY neutralino as a WIMP Dark Matter candidateGo to contribution page
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Estel Perez Codina (TRIUMF)12/06/2014, 14:20Supersymmetry provides an excellent dark matter candidate. SUSY searches at ATLAS are sensitive to an extensive range of scenarios with either a neutralino or a gravitino as the lightest supersymmetric particle. In this talk I will present the latest results from analyses carried out using the Run 1 dataset collected by ATLAS at the LHC at 8 TeV center of mass energy.Go to contribution page
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James Philip Ilten (Massachusetts Institute of Technology)12/06/2014, 14:40LHCb, located on the LHC, is a fully instrumented forward detector with flexible triggers, low pileup, and excellent secondary vertex resolution which make it an ideal experiment to search for unique exotic signals. A review of current LHCb exotic particle searches is given. Searches for the anomalous decays of B-mesons and tau-leptons are presented, as well as direct searches through...Go to contribution page
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Taku Gunji (Center for Nuclear Study, the University of Tokyo)12/06/2014, 15:00ALICE is one of the largest experiments at the Large Hadron Collider at CERN and is designed to study the physics of strongly interacting matter at extreme high temperature and energy densities created in high-energy heavy ion collisions. ALICE has a good potential to search for a dark photon signal in pi0 and eta Dalitz decays, thanks to the excellent resolution of the tracking system and the...Go to contribution page
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12/06/2014, 15:20
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Kathryn Zurek (University of Michigan)12/06/2014, 16:00
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Dan Hooper (Fermilab)12/06/2014, 16:30Past studies have identified a spatially extended excess of ~1-3 GeV gamma rays from the region surrounding the Galactic Center, consistent with the emission expected from annihilating dark matter. Recent improvements in the analysis techniques have found this excess to be robust and highly statistically significant, with a spectrum, angular distribution, and overall normalization that is in...Go to contribution page
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Neelima Sehgal (Stony Brook University)12/06/2014, 17:00The Cosmic Microwave Background (CMB) is a remarkably powerful and clean probe of dark matter annihilation. I will review the constraints from existing CMB and low-redshift data, and discuss future prospects from current and upcoming CMB experiments such as Planck and Advanced ACTpol. Many simple models designed to explain various indirect detection anomalies can be decisively tested with...Go to contribution page
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12/06/2014, 17:20
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Sergei Dubovsky (New York University)13/06/2014, 09:00I will discuss electromagnetic signals of black hole superradiance in the presence of an axion coupled to a hidden QCD-like sector.Go to contribution page
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Benjamin Brubaker (Yale University)13/06/2014, 09:30The axion is a well-motivated cold dark matter candidate first postulated to explain the absence of CP violation in strong interactions. Dark matter axions may be detected via their resonant conversion into photons in a high-Q microwave cavity permeated by a strong magnetic field. The Axion Dark Matter eXperiment (ADMX) has used this technique to exclude axion models in the few μeV mass range....Go to contribution page
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Surjeet Rajendran (Stanford)13/06/2014, 09:55We propose an experiment to search for QCD axion and axion-like-particle (ALP) dark matter. Nuclei that are interacting with the background axion dark matter acquire time-varying CP-odd nuclear moments such as an electric dipole moment. In analogy with nuclear magnetic resonance, these moments cause precession of nuclear spins in a material sample in the presence of a background electric...Go to contribution page
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13/06/2014, 10:20
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Bryce Littlejohn (University Of Cincinnati)13/06/2014, 11:00The existence of sterile neutrinos has been presented as an explanation for many anomalous results in experimental astro-particle physics. This talk will discuss existing experimental indications for eV-scale sterile neutrinos, while surveying future prospects for resolving these hints at accelerator, reactor, and radioactive source neutrino experiments.Go to contribution page
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Kendrik Smith (Perimeter Institute)13/06/2014, 11:30
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Maxim Pospelov (University of Victoria)13/06/2014, 12:00
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