270 research outputs found

    Environmental Justice and Regional Political Ecology converge in the other California

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    This article illuminates the value of the concept of the region in political ecology and environmental justice studies by presenting three arguments about the role of regions in environmental justice social movements engaged in climate change mitigation in California's San Joaquin Valley. First, regional planning agencies and environmental justice advocates are engaged in conflicts over not only the content of regional climate change plans, but the very definitions of region and the authority used to put these regional visions into action. Second, regional organizing provides environmental justice movements with new opportunities to address regional economic patterns and to negotiate with regional planning agencies, both of which influence local manifestations of environmental injustice. Third, regional strategies raise significant dilemmas for these movements as they try to sustain engagement across extensive spatial territories and engage with a broad set of policy and economic protagonists. Together, this analysis demonstrates that a dynamic approach to regions, regionalism, and regionalization can assist political ecology and environmental justice scholars in their common aim of understanding the co-production of social and environmental inequity and collective action to change it. Key Words: Environmental justice, regional political ecology, climate change mitigation, regional planning, rural community developmen

    Cumulative Environmental Vulnerability and Environmental Justice in California’s San Joaquin Valley

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    The identification of “environmental justice (EJ) communities” is an increasingly common element in environmental planning, policy, and regulation. As a result, the choice of methods to define and identify these communities is a critical and often contentious process. This contentiousness is, in turn, a factor of the lack of a commonly accepted method, the concern among many EJ advocates and some regulators that existing frameworks are inadequate, and ultimately, the significant consequences of such designations for both public policy and community residents. With the aim of assisting regulators and advocates to more strategically focus their efforts, the authors developed a Cumulative Environmental Vulnerability Assessment (CEVA). This CEVA is composed of a Cumulative Environmental Hazard Index and a Social Vulnerability Index, with a Health Index as a reference. Applying CEVA produces spatial analysis that identifies the places that are subject to both the highest concentrations of cumulative environmental hazards and the fewest social, economic and political resources to prevent, mitigate, or adapt to these conditions. We recommended that these areas receive special consideration in permitting, monitoring, and enforcement actions, as well as investments in public participation, capacity building, and community economic development

    Weak Coupling Phase from Decays of Charged B Mesons to πK\pi K and ππ\pi\pi

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    The theory of CPCP violation based on phases in weak couplings in the Cabibbo-Kobayashi-Maskawa (CKM) matrix requires the phase γArg Vub\gamma \equiv {\rm Arg~} V^*_{ub} (in a standard convention) to be nonzero. A measurement of γ\gamma is proposed based on charged BB meson decay rates to π+K0\pi^+ K^0, π0K+\pi^0 K^+, π+π0\pi^+ \pi^0, and the charge-conjugate states. The corresponding branching ratios are expected to be of the order of 10510^{-5}. (submitted to Physical Review Letters)Comment: LaTeX, 8 pages, 2 figures (not included, available upon request), TECHNION-PH-94-7, EFI-94-14, UdeM-LPN-TH-94-19

    An E6_6 interpretation of an e+eγγE ⁣ ⁣ ⁣/Te^+ e^- \gamma \gamma E\!\!\!/_T event

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    The lowest-dimensional representation of the group E6_6 contains both the standard quarks and leptons and a set of exotic quarks and leptons whose decays can involve a series of chains ending in radiative decay of one light neutrino species to another. An example is given based on the decomposition E6_6 \to SU(2)I×_I \times SU(6), where SU(2)I_I is an ``inert'' subgroup whose gauge bosons WI(±)W_I^{(\pm)} and ZIZ_I are all electromagnetically neutral, while SU(6) contains the conventional SU(5) grand-unified group. The possibility is explored that such a chain is responsible for an event observed by the Collider Detector at Fermilab (CDF) involving the production in proton-antiproton collisions at Ec.m.=1.8E_{\rm c.m.} = 1.8 TeV of an electron-positron pair, two photons, and missing energy (e+eγγE ⁣ ⁣ ⁣/Te^+ e^- \gamma \gamma E \!\!\!/_T).Comment: 14 pages, latex, no figures. Revised version submitted to PR

    Forward-Backward Asymmetries in Hadronically Produced Lepton Pairs

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    It has now become possible to observe appreciable numbers of hadronically produced lepton pairs in mass ranges where the contributions of the photon and Z0Z^0 are comparable. Consequently, in the reaction ppˉ++p \bar p \to \ell^- \ell^+ + \ldots, substantial forward-backward asymmetries can be seen. These asymmetries provide a test of the electroweak theory in a new regime of energies, and can serve as diagnostics for any new neutral vector bosons coupling both to quarks and to charged lepton pairs.Comment: 11 pages, latex, 4 uuencoded figures sent separately, Fig. 2 revise

    Atomic Parity Violation and Precision Electroweak Physics - An Updated Analysis

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    A new analysis of parity violation in atomic cesium has led to the improved value of the weak charge, QW(Cs)=72.06±0.46Q_W({\rm Cs}) = -72.06 \pm 0.46. The implications of this result for constraining the Peskin-Takeuchi parameters S and T and for guiding searches for new Z bosons are discussed.Comment: 8 pages, LaTeX, 3 figures, Submitted to Physical Review D. Updated experimental inputs and references; clarification of notatio

    Charmless BPPB \to PP decays using flavor SU(3) symmetry

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    The decays of BB mesons to a pair of charmless pseudoscalar (PP) mesons are analyzed within a framework of flavor SU(3). Symmetry breaking is taken into account in tree (TT) amplitudes through ratios of decay constants; exact SU(3) is assumed elsewhere. Acceptable fits to BππB \to \pi \pi and BKπB \to K \pi branching ratios and CP asymmetries are obtained with tree, color-suppressed (CC), penguin (PP), and electroweak penguin (PEWP_{EW}) amplitudes. Crucial additional terms for describing processes involving η\eta and η\eta' include a large flavor-singlet penguin amplitude (SS) as proposed earlier and a penguin amplitude PtuP_{tu} associated with intermediate tt and uu quarks. For the B+π+ηB^+ \to \pi^+ \eta' mode a term StuS_{tu} associated with intermediate tt and uu quarks also may be needed. Values of the weak phase γ\gamma are obtained consistent with an earlier analysis of BVPB \to VP decays, where VV denotes a vector meson, and with other analyses of CKM parameters.Comment: 26 pages, 1 figure. To be submitted to Phys. Rev. D. Reference update

    How generic is cosmic string formation in SUSY GUTs

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    We study cosmic string formation within supersymmetric grand unified theories. We consider gauge groups having a rank between 4 and 8. We examine all possible spontaneous symmetry breaking patterns from the GUT down to the standard model gauge group. Assuming standard hybrid inflation, we select all the models which can solve the GUT monopole problem, lead to baryogenesis after inflation and are consistent with proton lifetime measurements. We conclude that in all acceptable spontaneous symmetry breaking schemes, cosmic string formation is unavoidable. The strings which form at the end of inflation have a mass which is proportional to the inflationary scale. Sometimes, a second network of strings form at a lower scale. Models based on gauge groups which have rank greater than 6 can lead to more than one inflationary era; they all end by cosmic string formation.Comment: 31 pages, Latex, submitted to PR

    New Physics Contributions to The B -> phi K_S Decay

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    Recent measurements of the time-dependent CP asymmetry of the B -> phi K_S decay give results whose central values differ from standard model expectations. It is shown how such data can be used to identify new physics contributions in a model-independent manner. In general, a sizeable new amplitude with nontrivial weak and strong phases would be required to explain current data. Improvement in the quality of data will allow one to form a more definite conclusion.Comment: 17 pages, 7 figures; some references added; analysis updated in light of recent BaBar data announced at Moriond conferenc
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