178 research outputs found

    Who wants to conserve remaining forest fragments in the Manompana Corridor?

    Get PDF
    Contiguous forests in Madagascar are continuously converted into forest fragments due to deforestation, and dispersed into landscape mosaics dominated by agriculture. These fragments are of increasing importance for biodiversity conservation as well as for the well being of rural inhabitants, providing a high diversity of timber and non- timber forest products. An increasing number of international projects are therefore trying to preserve remaining forests and to transfer the management of these forests to local communities. However, it is not known how important the preservation of forest fragments is to local people. We therefore explore the importance of forest fragments as a source of cash income to different groups separated by wealth level and access to forest resources. A multi-method research approach was taken, based on score application exercises as well as interviews with individual households and focus groups. Our study site was located at the east coast of Madagascar in the Manompana corridor. Results show that some groups are significantly more interested in the preservation of forest fragments than others. Interest is significantly related to the wealth of local inhabitants as well as to the walking distance between villages and forest resources. Nevertheless, interest in resource preservation does not depend on how important fragments are to local people, but rather on the awareness about resource scarcity.  RĂ©sumĂ© En raison d’une forte dĂ©forestation sur la cĂŽte est de Madagascar, de nombreux massifs forestiers d’un seul tenant et de vastes Ă©cosystĂšmes interconnectĂ©s ont Ă©tĂ© dĂ©truits, laissant des fragments de forĂȘts qui s’intĂšgrent dans une mosaĂŻque paysagĂšre dominĂ©e par l’agriculture. Ces fragments gagnent en importance. Ils jouent un rĂŽle de premier plan dans les rĂ©seaux de biodiversitĂ© en assurant un certain niveau de connectivitĂ©. Mais les fragments sont essentiels au bien - ĂȘtre de la population locale, fournissant produits et services pour la consommation quotidienne ou donnant accĂšs Ă  un revenu monĂ©taire. Sur un plan global, aussi bien les organisations de protection de la nature que les milieux scientifiques essayent d’endiguer la dĂ©forestation. Depuis les annĂ©es 1996 la politique nationale Ă  Madagascar a gĂ©nĂ©rĂ© lois et processus visant Ă  transfĂ©rer la gestion des ressources forestiĂšres de l’Etat aux communautĂ©s locales. Cependant, il n’a pas Ă©tĂ© possible, jusqu’à ce jour, d’attĂ©nuer l’ampleur de la destruction et de la fragmentation des forĂȘts pluviales de l’üle. Plus encore, Ă  l’heure actuelle la perception de l’importance des fragments de forĂȘts n’est pas connue par la population. Un projet de recherche a Ă©tĂ© lancĂ© pour contribuer Ă  combler cette lacune, dans le corridor de Manompana, sur la cĂŽte. Les buts de ce projet Ă©taient (i) d’explorer l’importance des fragments de forĂȘts pour les revenus monĂ©taires de la population locale et (ii) d’analyser la perception de l’importance des fragments de forĂȘts par la population locale. Les recherches se sont dĂ©roulĂ©es dans quatre villages situĂ©s Ă  des distances diffĂ©rentes du grand massif forestier. La population locale a Ă©tĂ© rĂ©partie en diffĂ©rentes catĂ©gories de niveau de vie et en fonction de la distance Ă  parcourir entre les villages et la forĂȘt. Cette approche a permis d’étudier le rĂŽle de la forĂȘt quant aux revenus monĂ©taires des diffĂ©rents groupes de la population. Nous avons Ă©galement cherchĂ© Ă  Ă©tablir un lien entre l’ampleur des revenus monĂ©taires et un intĂ©rĂȘt Ă  conserver les fragments de forĂȘts qui subsistent. Nos mĂ©thodes de recherche font recours Ă  des exercices de « scoring », Ă  des discussions avec des groupes ciblĂ©s et Ă  des enquĂȘtes de mĂ©nages. Il ressort des analyses que certains groupes ont un intĂ©rĂȘt Ă  conserver les fragments forestiers. Cet intĂ©rĂȘt est significativement liĂ©, d’une part, au niveau de vie de la population, d’autre part, Ă  la distance entre le village et le massif forestier. Cependant, l’intĂ©rĂȘt Ă  conserver les fragments de forĂȘts est plus fortement liĂ© Ă  la conscience de la finitude des ressources forestiĂšres qu’au montant des revenus monĂ©taires que la population peut tirer des produits forestiers.

    On the Corrections to Dashen's Theorem

    Full text link
    The electromagnetic corrections to the masses of the pseudoscalar mesons π\pi and KK are considered. We calculate in chiral perturbation theory the contributions which arise from resonances within a photon loop at order O(e2mq)O(e^2 m_q). Within this approach we find rather moderate deviations to Dashen's theorem.Comment: 14 pages, sligthly enlarged version; a numerical error is corrected and the embedding of the figures is improved. The complete paper, including figures, is also available via anonymous ftp at ftp://www-ttp.physik.uni-karlsruhe.de/ , or via www at http://www-ttp.physik.uni-karlsruhe.de/cgi-bin/preprints/; to be published in Phys.Rev.

    Boltzmann Equations for Spin and Charge Relaxations in Superconductors

    Full text link
    In a superconductor coupled with a ferromagnetic metal, spin and charge imbalances can be induced by injecting spin-polarized electron current from the ferromagnetic metal. We theoretically study a nonequilibrium distribution of quasiparticles in the presence of spin and charge imbalances. We show that four distribution functions are needed to characterize such a nonequilibrium situation, and derive a set of linearized Boltzmann equations for them by extending the argument by Schmid and Sch\"{o}n based on the quasiclassical Green's function method. Using the Boltzmann equations, we analyze the spin imbalance in a thin superconducting wire weakly coupled with a ferromagnetic electrode. The spin imbalance induces a shift ÎŽÎŒ\delta\mu (−ΎΌ- \delta \mu) of the chemical potential for up-spin (down-spin) quasiparticles. We discuss how ÎŽÎŒ\delta \mu is relaxed by spin-orbit impurity scattering.Comment: 16 pages, 2 figure

    Sequential vector and axial-vector meson exchange and chiral loops in radiative phi decay

    Get PDF
    We study the radiative ϕ\phi decay into π0π0Îł\pi^0 \pi^0 \gamma and π0ηγ\pi^0 \eta \gamma taking into account mechanisms in which there are two sequential vector-vector-pseudoscalar or axial-vector--vector--pseudoscalar steps followed by the coupling of a vector meson to the photon, considering the final state interaction of the two mesons. There are other mechanisms in which two kaons are produced through the same sequential mechanisms or from ϕ\phi decay into two kaons and then undergo final state interaction leading to the final pair of pions or π0η\pi^0 \eta, this latter mechanism being the leading one. The results of the parameter free theory, together with the theoretical uncertainties, are compared with the latest experimental results of KLOE at Frascati.Comment: 28 pages, 20 figure

    Shape modeling technique KOALA validated by ESA Rosetta at (21) Lutetia

    Full text link
    We present a comparison of our results from ground-based observations of asteroid (21) Lutetia with imaging data acquired during the flyby of the asteroid by the ESA Rosetta mission. This flyby provided a unique opportunity to evaluate and calibrate our method of determination of size, 3-D shape, and spin of an asteroid from ground-based observations. We present our 3-D shape-modeling technique KOALA which is based on multi-dataset inversion. We compare the results we obtained with KOALA, prior to the flyby, on asteroid (21) Lutetia with the high-spatial resolution images of the asteroid taken with the OSIRIS camera on-board the ESA Rosetta spacecraft, during its encounter with Lutetia. The spin axis determined with KOALA was found to be accurate to within two degrees, while the KOALA diameter determinations were within 2% of the Rosetta-derived values. The 3-D shape of the KOALA model is also confirmed by the spectacular visual agreement between both 3-D shape models (KOALA pre- and OSIRIS post-flyby). We found a typical deviation of only 2 km at local scales between the profiles from KOALA predictions and OSIRIS images, resulting in a volume uncertainty provided by KOALA better than 10%. Radiometric techniques for the interpretation of thermal infrared data also benefit greatly from the KOALA shape model: the absolute size and geometric albedo can be derived with high accuracy, and thermal properties, for example the thermal inertia, can be determined unambiguously. We consider this to be a validation of the KOALA method. Because space exploration will remain limited to only a few objects, KOALA stands as a powerful technique to study a much larger set of small bodies using Earth-based observations.Comment: 15 pages, 8 figures, 2 tables, accepted for publication in P&S

    Non-Perturbative Study of the Light Pseudoscalar Masses in Chiral Dynamics

    Get PDF
    We perform a non-perturbative chiral study of the masses of the lightest pseudoscalar mesons. In the calculation of the self-energies we employ the S-wave meson-meson amplitudes taken from Unitary Chiral Perturbation Theory (UCHPT) that include the lightest nonet of scalar resonances. Values for the bare masses of pions and kaons are obtained, as well as an estimate of the mass of the \eta_8. The former are found to dominate the physical pseudoscalar masses. We then match to the self-energies from Chiral Perturbation Theory (CHPT) to O(p^4), and a robust relation between several O(p^4) CHPT counterterms is obtained. We also resum higher orders from our calculated self-energies. By taking into account values determined from previous chiral phenomenological studies of m_s/\hat{m} and 3L_7+L^r_8, we determine a tighter region of favoured values for the O(p^4) CHPT counterterms 2L^r_6-L^r_4 and 2L^r_8-L^r_5. This determination perfectly overlaps with the recent determinations to O(p^6) in CHPT. We warn about a likely reduction in the value of m_s/\hat{m} by higher loop diagrams and that this is not systematically accounted for by present lattice extrapolations. We also provide a favoured interval of values for m_s/\hat{m} and 3L_7+L^r_8.Comment: 26 pages, 9 figures. Original new material is included. Major rewriting when comparing with lattice QC

    The Electromagnetic Mass Differences of Pions and Kaons

    Get PDF
    We use the Cottingham method to calculate the pion and kaon electromagnetic mass differences with as few model dependent inputs as possible. The constraints of chiral symmetry at low energy, QCD at high energy and experimental data in between are used in the dispersion relation. We find excellent agreement with experiment for the pion mass difference. The kaon mass difference exhibits a strong violation of the lowest order prediction of Dashen's theorem, in qualitative agreement with several other recent calculations.Comment: 40 pages, Latex, needs axodraw. and psfig. macros, 4 figure

    Hadronic light-by-light scattering contribution to the muon g-2: an effective field theory approach

    Get PDF
    The hadronic light-by-light contribution to a_{mu}, the anomalous magnetic moment of the muon, is discussed from the point of view of an effective low-energy theory. As an application, the coefficient of the leading logarithm arising from the two-loop graphs involving two anomalous vertices is computed, and found to be positive. This corresponds to a positive sign for the pion-pole contribution to the hadronic light-by-light correction to a_{mu}, and to a sizeable reduction of the discrepancy between the present experimental value of a_{mu} and its theoretical counterpart in the standard model.Comment: 4 pages, 1 figure. v2: published versio

    Isospin Breaking and ω\omega->ππ\pi\pi Decay

    Full text link
    We study ω→π+π−\omega\to\pi^+\pi^- decay up to including all orders of the chiral expansion and one-loop level of mesons in formlism of chiral constituent quark model. This G-parity forbidden decay is caused by mu≠mdm_u\neq m_d and electromagnetic interaction of mesons. We illustrate that in the formlism both nonresonant contact interaction and ρ\rho resonance exchange contribute to this process, and the contribution from ρ\rho resonance exchange is dominant. We obtain that transition matrix element is =[−(3956±280)−(1697±130)i]=[-(3956\pm 280)-(1697\pm 130)i]MeV2^2, and isospin breaking parameter is md−mu=3.9±0.22m_d-m_u=3.9\pm 0.22MeV at energy scale Ό∌mω\mu\sim m_\omega.Comment: Revtex file, 16 pages, four eps figur
    • 

    corecore