989 resultados para Kinect simulink UDP C gesture UAV


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<p>Part I: The mobilities of photo-generated electrons and holes in orthorhombic sulfur are determined by drift mobility techniques. At room temperature electron mobilities between 0.4 cm<sup>2</sup>/V-sec and 4.8 cm<sup>2</sup>/V-sec and hole mobilities of about 5.0 cm<sup>2</sup>/V-sec are reported. The temperature dependence of the electron mobility is attributed to a level of traps whose effective depth is about 0.12 eV. This value is further supported by both the voltage dependence of the space-charge-limited, D.C. photocurrents and the photocurrent versus photon energy measurements.</p> <p>As the field is increased from 10 kV/cm to 30 kV/cm a second mechanism for electron transport becomes appreciable and eventually dominates. Evidence that this is due to impurity band conduction at an appreciably lower mobility (4.10<sup>-4</sup> cm<sup>2</sup>/V-sec) is presented. No low mobility hole current could be detected. When fields exceeding 30 kV/cm for electron transport and 35 kV/cm for hole transport are applied, avalanche phenomena are observed. The results obtained are consistent with recent energy gap studies in sulfur. </p> <p>The theory of the transport of photo-generated carriers is modified to include the case of appreciable thermos-regeneration from the traps in one transit time.</p> <p>Part II: An explicit formula for the electric field E necessary to accelerate an electron to a steady-state velocity v in a polarizable crystal at arbitrary temperature is determined via two methods utilizing Feynman Path Integrals. No approximation is made regarding the magnitude of the velocity or the strength of the field. However, the actual electron-lattice Coulombic interaction is approximated by a distribution of harmonic oscillator potentials. One may be able to find the best possible distribution of oscillators using a variational principle, but we have not been able to find the expected criterion. However, our result is relatively insensitive to the actual distribution of oscillators used, and our E-v relationship exhibits the physical behavior expected for the polaron. Threshold fields for ejecting the electron for the polaron state are calculated for several substances using numerical results for a simple oscillator distribution. </p>

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<p>Described in this thesis are measurements made of the thick-target neutron yield from the reaction <sup>13</sup>C(, n)<sup>16</sup>O. The yield was determined for laboratory bombarding energies between 0.475 and 0.700 MeV, using a stilbene crystal neutron detector and pulse-shape discrimination to eliminate gamma rays. Stellar temperatures between 2.5 and 4.5 x 10<sup>8</sup> <sup>o</sup>K are involved in this energy region. From the neutron yield was extracted the astrophysical cross-section factor S(E), which was found to fit a linear function: S(E) = [(5.48 1.77) + (12.05 3.91)E] x 10<sup>5</sup> MeV-barns, center-of-mass system. The stellar rate of the <sup>13</sup>C(, n)<sup>16</sup>O reaction if calculated, and discussed with reference to helium burning and neutron production in the core of a giant star. </p> <p>Results are also presented of measurements carried out on the reaction <sup>9</sup>Be(, n)<sup>12</sup>C, taken with a thin Be target. The bombarding energy-range covered was from 0.340 to 0.680 MeV, with excitation curves for the ground- and first excited-state neutrons being reported. Some angular distributions were also measured. Resonances were found at bombarding energies of E<sub>LAB</sub> = 0.520 MeV (E<sub>CM</sub> = 0.360 MeV, ~ 55 keV CM, = 3.79 eV CM) and E<sub>LAB</sub> = 0.600 MeV (E<sub>CM</sub> = 0.415 MeV, 4 keV CM, = 0.88 eV CM). The astrophysical rate of the <sup>9</sup>Be(, n)<sup>12</sup>C reaction due to these resonances is calculated. </p>

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Evidncias recentes sugerem que as doenas periodontais podem desempenhar um papel relevante na etiologia e patognese de doenas cardiovasculares e hipertenso arterial. A resposta inflamatria, com conseqente elevao de marcadores sistmicos como protena C-reativa, fibrinognio e interleucina-6, e a disfuno endotelial, podem ser os responsveis por essa associao. Alguns estudos tm relatado maiores nveis pressricos, maior massa ventricular esquerda e disfuno endotelial em pacientes com doenas periodontais. Ao mesmo tempo, estudos clnicos vm mostrando que a terapia periodontal pode levar reduo dos nveis plasmticos dos marcadores de inflamao e reduo do risco cardiovascular. O presente estudo teve como objetivo avaliar os efeitos da terapia periodontal no-cirrgica em 26 pacientes (idade mdia de 53.68.0 anos) hipertensos refratrios. Foram avaliados marcadores plasmticos de inflamao (protena C-reativa, fibrinognio e interleucina-6), presso arterial sistlica e diastlica, massa ventricular esquerda e rigidez arterial. A terapia periodontal foi eficaz na reduo da mdia de todos os marcadores de risco cardiovascular avaliados. Os nveis de protena C-reativa baixaram 0.7mg/dl 6 meses aps a terapia periodontal, os de IL-6, 1.6pg/dl e os de fibrinognio 55.3mg/dl (p<0.01). A presso arterial sistlica apresentou reduo mdia de 16.7mmHg e a diastlica de 9.6mmHg. A massa ventricular esquerda diminuiu em mdia 12.9g e a velocidade da onda de pulso, um marcador de rigidez arterial, e consequentemente de disfuno endotelial, apresentou reduo de seus valores mdios de 0.9m/s (p<0.01). Dessa forma, conclui-se que a terapia periodontal foi eficaz na reduo dos nveis de protena C-reativa, interleucina-6, fibrinognio, presso arterial, massa ventricular esquerda e rigidez arterial.

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The differential cross section for the reaction p <sup>+</sup>n was measured at 32 laboratory photon energies between 589 and 1269 MeV at the Caltech Synchrotron. At each energy, data have been obtained at typically fifteen <sup>+</sup> c.m. angles between 6 and 90. A magnetic spectrometer was used to detect the <sup>+</sup> photo-produced in a liquid hydrogen target. Two Cherenkov counters were used to reject the background of positrons and protons. The data clearly show the presence of a pole in the production amplitude due to the one pion exchange. Moravcsik fits to the 32 angular distributions, including data from another experiment, are presented. The extrapolation of these fits to the pole gives a value for the pion-nucleon coupling constant of 14.5 which is consistent with the accepted value. The second and third pion-nucleon resonances are evident as peaks in the total cross section and as changes in the shape of the angular distributions. At the third resonance there is evidence for both a D5/2 and an F5/2 amplitude. The absence of large variations in the 0 and 180 cross sections implies that the second and third resonances are mostly produced from an initial state with helicity 3/2.

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<p>The cross sections for the two antiproton-proton annihilation-in-flight modes,</p> <p>p + p <sup>+</sup> + <sup>-</sup></p> <p>p + p k<sup>+</sup> + k<sup>-</sup></p> <p>were measured for fifteen laboratory antiproton beam momenta ranging from 0.72 to 2.62 GeV/c. No magnets were used to determine the charges in the final state. As a result, the angular distributions were obtained in the form [d/d (<sub>C.M.</sub>) + d/d ( <sub>C.M.</sub>)] for 45 <sub>C.M.</sub> 135. </p> <p>A hodoscope-counter system was used to discriminate against events with final states having more than two particles and antiproton-proton elastic scattering events. One spark chamber was used to record the track of each of the two charged final particles. A total of about 40,000 pictures were taken. The events were analyzed by measuring the laboratory angle of the track in each chamber. The value of the square of the mass of the final particles was calculated for each event assuming the reaction</p> <p>p + p a pair of particles with equal masses.</p> <p>About 20,000 events were found to be either annihilation into <sup></sup>-pair or k <sup></sup>-pair events. The two different charged meson pair modes were also distinctly separated.</p> <p>The average differential cross section of p + p <sup>+</sup> + <sup>-</sup> varied from ~ 25 b/sr at antiproton beam momentum 0.72 GeV/c (total energy in center-of-mass system, s = 2.0 GeV) to ~ 2 b/sr at beam momentum 2.62 GeV/c (s = 2.64 GeV). The most striking feature in the angular distribution was a peak at <sub>C.M.</sub> = 90 (cos <sub>C.M.</sub> = 0) which increased with s and reached a maximum at s ~ 2.1 GeV (beam momentum ~ 1.1 GeV/c). Then it diminished and seemed to disappear completely at s ~ 2.5 GeV (beam momentum ~ 2.13 GeV/c). A valley in the angular distribution occurred at cos <sub>C.M.</sub> 0.4. The differential cross section then increased as cos <sub>C.M.</sub> approached 1.</p> <p>The average differential cross section for p + p k<sup>+</sup> + k<sup>-</sup> was about one third of that of the <sup></sup>-pair mode throughout the energy range of this experiment. At the lower energies, the angular distribution, unlike that of the <sup></sup>-pair mode, was quite isotropic. However, a peak at <sub>C.M.</sub> = 90 seemed to develop at s ~ 2.37 GeV (antiproton beam momentum ~ 1.82 GeV/c). No observable change was seen at that energy in the <sup></sup>-pair cross section.</p> <p>The possible connection of these features with the observed meson resonances at 2.2 GeV and 2.38 GeV, and its implications, were discussed. </p>

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En esta memoria se presenta una propuesta para desarrollar un proyecto de investigacin que permita establecer la eficacia de una estrategia original para evitar la entrada del virus de la hepatitis C (HCV) en las clulas hepticas. Se propone la utilizacin combinada de dos anticuerpos contra dos factores esenciales para la entrada HCV en las clulas hepticas, como son las molculas CD81 y SR-BI. La eficacia para reducir la capacidad infectiva del HCV de bloquear individualmente cada una de estas molculas ha sido previamente demostrada, as que en este proyecto proponemos que un uso combinado de molculas que bloqueen ambos receptores permitira avanzar en la bsqueda de vacunas que eviten eficazmente la infeccin del HCV.

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<p>Terphenyl diphosphines bearing pendant ethers were prepared to provide mechanistic insight into the mechanism of activation of aryl CO bonds with Group 9 and Group 10 transition metals. Chapters 2 and 3 of this dissertation describe the reactivity of compounds supported by the model phosphine and extension of this chemistry to heterogenous CO bond activation.</p> <p>Chapter 2 describes the synthesis and reactivity of aryl-methyl and aryl-aryl model systems. The metallation of these compounds with Ni, Pd, Pt, Co, Rh, and Ir is described. Intramolecular bond activation pathways are described. In the case of the aryl-methyl ether, aryl CO bond activation was observed only for Ni, Rh, and Ir.</p> <p>Chapter 3 outlines the reactivity of heterogenous Rh and Ir catalysts for aryl ether CO bond cleavage. Using Rh/C and an organometallic Ir precursor, aryl ethers were treated with H2 and heat to afford products of hydrogenolysis and hydrogenation. Conditions were modified to optimize the yield of hydrogenolysis product. Hydrogenation could not be fully suppressed in these systems.</p> <p>Appendix A describes initial investigations of bisphenoxyiminoquinoline dichromium compounds for selective C2H4 oligomerization to afford -olefins. The synthesis of monometallic and bimetallic Cr complexes is described. These compounds are compared to literature examples and found to be less active and non-selective for production of -olefins.</p> <p>Appendix B describes the coordination chemistry of terphenyl diphosphines, terphenyl bisphosphinophenols, and biphenyl phosphinophenols proligands with molybdenum, cobalt, and nickel. Since their synthesis, terphenyl diphosphine molybdenum compounds have been reported to be good catalysts for the dehydrogenation of ammonia borane. Biphenyl phosphinophenols are demonstrated provide both phosphine and arene donors to transition metals while maintaining a sterically accessible coordination sphere. Such ligands may be promising in the context of the activation of other small molecules.</p> <p>Appendix C contains relevant NMR spectra for the compounds presented in the preceding sections.</p>

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<p><u>I. The 3.7 Crystal Structure of Horse Heart Ferricytochrome C. </u></p> <p>The crystal structure of horse heart ferricytochrome c has been determined to a resolution of 3.7 using the multiple isomorphous replacement technique. Two isomorphous derivatives were used in the analysis, leading to a map with a mean figure of merit of 0.458. The quality of the resulting map was extremely high, even though the derivative data did not appear to be of high quality. </p> <p>Although it was impossible to fit the known amino acid sequence to the calculated structure in an unambiguous way, many important features of the molecule could still be determined from the 3.7 electron density map. Among these was the fact that cytochrome c contains little or no -helix. The polypeptide chain appears to be wound about the heme group in such a way as to form a loosely packed hydrophobic core in the molecule. </p> <p>The heme group is located in a cleft on the molecule with one edge exposed to the solvent. The fifth coordinating ligand is His 18 and the sixth coordinating ligand is probably neither His 26 nor His 33. </p> <p>The high resolution analysis of cytochrome c is now in progress and should be completed within the next year. </p> <p><u>II. The Application of the Karle-Hauptman Tangent Formula to Protein Phasing.</u> </p> <p>The Karle-Hauptman tangent formula has been shown to be applicable to the refinement of previously determined protein phases. Tests were made with both the cytochrome c data from Part I and a theoretical structure based on the myoglobin molecule. The refinement process was found to be highly dependent upon the manner in which the tangent formula was applied. Iterative procedures did not work well, at least at low resolution. </p> <p>The tangent formula worked very well in selecting the true phase from the two possible phase choices resulting from a single isomorphous replacement phase analysis. The only restriction on this application is that the heavy atoms form a non-centric cluster in the unit cell. </p> <p>Pages 156 through 284 in this Thesis consist of previously published papers relating to the above two sections. References to these papers can be found on page 155. </p>

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<p>Several new ligand platforms designed to support iron dinitrogen chemistry have been developed. First, we report Fe complexes of a tris(phosphino)alkyl (CP<sup>iPr</sup><sub>3</sub>) ligand featuring an axial carbon donor intended to conceptually model the interstitial carbide atom of the nitrogenase iron-molybdenum cofactor (FeMoco). It is established that in this scaffold, the iron center binds dinitrogen trans to the C<sub>alkyl</sub> anchor in three structurally characterized oxidation states. Fe-C<sub>alkyl</sub> lengthening is observed upon reduction, reflective of significant ionic character in the Fe-C<sub>alkyl</sub> interaction. The anionic (CP<sup>iPr</sup><sub>3</sub>)FeN<sub>2</sub><sup>-</sup> species can be functionalized by a silyl electrophile to generate (CP<sup>iPr</sup><sub>3</sub>)Fe-N<sub>2</sub>SiR<sub>3</sub>. This species also functions as a modest catalyst for the reduction of N<sub>2</sub> to NH<sub>3</sub>. Next, we introduce a new binucleating ligand scaffold that supports an Fe(-SAr)Fe diiron subunit that coordinates dinitrogen (N<sub>2</sub>-Fe(-SAr)Fe-N<sub>2</sub>) across at least three oxidation states (Fe<sup>II</sup>Fe<sup>II</sup>, Fe<sup>II</sup>Fe<sup>I</sup>, and Fe<sup>I</sup>Fe<sup>I</sup>). Despite the sulfur-rich coordination environment of iron in FeMoco, synthetic examples of transition metal model complexes that bind N<sub>2</sub> and also feature sulfur donor ligands remain scarce; these complexes thus represent an unusual series of low-valent diiron complexes featuring thiolate and dinitrogen ligands. The (N<sub>2</sub>-Fe(-SAr)Fe-N<sub>2</sub>) system undergoes reduction of the bound N<sub>2</sub> to produce NH<sub>3</sub> (~50% yield) and can efficiently catalyze the disproportionation of N<sub>2</sub>H<sub>4</sub> to NH<sub>3</sub> and N<sub>2</sub>. The present scaffold also supports dinitrogen binding concomitant with hydride as a co-ligand. Next, inspired by the importance of secondary-sphere interactions in many metalloenzymes, we present complexes of iron in two new ligand scaffolds ([SiP<sup>NMe</sup><sub>3</sub>] and [SiP<sup>iPr</sup><sub>2</sub>P<sup>NMe</sup>]) that incorporate hydrogen-bond acceptors (tertiary amines) which engage in interactions with nitrogenous substrates bound to the iron center (NH<sub>3</sub> and N<sub>2</sub>H<sub>4</sub>). Cation binding is also facilitated in anionic Fe(0)-N<sub>2</sub> complexes. While Fe-N<sub>2</sub> complexes of a related ligand ([SiP<sup>iPr</sup><sub>3</sub>]) lacking hydrogen-bond acceptors produce a substantial amount of ammonia when treated with acid and reductant, the presence of the pendant amines instead facilitates the formation of metal hydride species.</p> <p>Additionally, we present the development and mechanistic study of copper-mediated and copper-catalyzed photoinduced C-N bond forming reactions. Irradiation of a copper-amido complex, ((m-tol)<sub>3</sub>P)<sub>2</sub>Cu(carbazolide), in the presence of aryl halides furnishes N-phenylcarbazole under mild conditions. The mechanism likely proceeds via single-electron transfer from an excited state of the copper complex to the aryl halide, generating an aryl radical. An array of experimental data are consistent with a radical intermediate, including a cyclization/stereochemical investigation and a reactivity study, providing the first substantial experimental support for the viability of a radical pathway for Ullmann C-N bond formation. The copper complex can also be used as a precatalyst for Ullmann C-N couplings. We also disclose further study of catalytic C<sub>alkyl</sub>-N couplings using a CuI precatalyst, and discuss the likely role of [Cu(carbazolide)<sub>2</sub>]<sup>-</sup> and [Cu(carbazolide)<sub>3</sub>]<sup>-</sup> species as intermediates in these reactions.</p> <p>Finally, we report a series of four-coordinate, pseudotetrahedral P<sub>3</sub>Fe<sup>II</sup>-X complexes supported by tris(phosphine)borate ([PhBP<sub>3</sub>Fe<sup>R</sup>]<sup>-</sup>) and phosphiniminato X-type ligands (-N=PR'<sub>3</sub>) that in combination tune the spin-crossover behavior of the system. Low-coordinate transition metal complexes such as these that undergo reversible spin-crossover remain rare, and the spin equilibria of these systems have been studied in detail by a suite of spectroscopic techniques.</p>

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As hepatites crnicas por vrus so as mais frequentes, destacando-se os vrus das hepatites B (VHB) e C (VHC). O estudo anatomopatolgico da bipsia heptica considerado o padro ouro para avaliar com preciso a distoro arquitetural e o grau de fibrose do parnquima do fgado, importantes fatores prognsticos para os pacientes portadores de hepatites crnicas virais. Na avaliao histopatolgica atual, em adio aos relatos subjetivos das alteraes histolgicas, escores semiquantitativos que correlacionam achados morfolgicos com graus numricos so usados, tais como os reconhecidos escores de Ishak e METAVIR. Entretanto, em todos estes sistemas h a desvantagem da subjetividade do examinador e da incorporao de alteraes categricas, sem referncias s mudanas quantitativas do colgeno heptico. Tcnicas de anlise de imagens digitais (AID) que fornecem quantificao objetiva dos graus de fibrose em amostras histolgicas tm sido desenvolvidas. Todavia, o alto custo e dificuldade ao acesso das tecnologias descritas restringem seu uso a poucos centros especializados. Este estudo visa o desenvolvimento de uma tcnica de custo acessvel para a anlise de imagens digitais da fibrose heptica em hepatites crnicas virais. Foram estudadas 304 bipsias de pacientes com hepatite crnica por vrus B e C, obtidas atravs de agulhas Menghini. Todas as amostras tinham pelo menos 15 mm de comprimento ou cinco espaos-porta completos e foram coradas pelo mtodo Tricrmico de Masson. O estadiamento foi feito por um nico hepatopatologista experiente, sem o conhecimento dos dados clnicos dos pacientes. Os escores de Ishak e METAVIR foram aplicados. As imagens microscpicas foram digitalizadas. Os ndices de fibrose foram determinados de forma automatizada, em tcnica desenvolvida no programa Adobe Photoshop. Para o escore de Ishak, observamos os seguintes ndices de Fibrose (IF) mdios: 0,8% 0,0 (estgio 0), 2.4% 0,6 (estgio 1), 4,7% 1,6 (estgio 2), 7,4% 1,4 (estgio 3), 14,9% 3,7 (estgio 4), 23,4% 2,9 (estgio 5) e 34,5% 1,5 (estgio 6). Para a classificao METAVIR: 0,8% 0,1 (estgio F0), 3,8% 1,8 (estgio F1), 7,4% 1,4 (estgio F2), 20,4% 5,2 (estgio F3) e 34,5% 1,5 (estgio F4). Observamos uma excelente correlao entre os ndices de fibrose da AID e os escores de Ishak (r=0,94; p<0,001) e METAVIR (r=0,92; p<0,001). Em relao indicao de tratamento antiviral, foi observado IF mdio de 16,4%. Em relao ao diagnstico de cirrose, foi observado IF mdio de 26,9%, para o escore de Ishak, e 34,5% para a classificao METAVIR. A reprodutibilidade intra-observador foi excelente. Este novo mtodo de anlise de imagens digitais para a quantificao de fibrose heptica tem custo acessvel e foi desenvolvido com tecnologia que est disponvel em todo o mundo, permitindo identificar com preciso todos os estgios de fibrose, com excelente reprodutibilidade intra-observador.

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<p>The reaction K<sup>-</sup>pK<sup>-</sup><sup>+</sup>n has been studied for incident kaon momenta of 2.0 GeV/c. A sample of 19,881 events was obtained by a measurement of film taken as part of the K-63 experiment in the Berkeley 72 inch bubble chamber. </p> <p>Based upon our analysis, we have reached four conclusions. (1) The magnitude of the extrapolated K cross section differs by a factor of 2 from the P-wave unitarity prediction and the K<sup>+</sup>n results; this is probably due to absorptive effects. (2) Fits to the moments yield precise values for the K S-wave which agree with other recent statistically accurate experiments. (3) An anomalous peak is present in our backward K<sup>-</sup>p(+n) K<sup>-</sup> u-distribution. (4) We find a non-linear enhancement due to interference similiar to the one found by Bland et al. (Bland 1966).</p>

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<p>PART I</p> <p>The total cross-section for the reaction <sup>21</sup>Ne(, n)<sup>24</sup>Mg has been measured in the energy range 1.49 Mev E<sub>cm</sub> 2.6 Mev. The cross-section factor, S(O), for this reaction has been determined, by means of an optical model calculation, to be in the range 1.52 x 10<sup>12</sup> mb-Mev to 2.67 x 10<sup>12</sup> mb-Mev, for interaction radii in the range 5.0 fm to 6.6 fm. With S(O) 2 x 10<sup>12</sup> mb-Mev, the reaction <sup>21</sup>Ne(, n)<sup>24</sup>Mg can produce a large enough neutron flux to be a significant astrophysical source of neutrons.</p> <p>PART II</p> <p>The reaction<sup>12</sup>C(<sup>3</sup>He, p)<sup>14</sup>N has been studied over the energy range 12 Mev E<sub>lab</sub> 18 Mev. Angular distributions of the proton groups leading to the lowest seven levels in <sup>14</sup>N were obtained.</p> <p>Distorted wave calculations, based on two-nucleon transfer theory, were performed, and were found to be reliable for obtaining the value of the orbital angular momentum transferred. The present work shows that such calculations do not yield unambiguous values for the spectroscopic factors.</p>

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<p>A number of recent experiments have suggested the possibility of a highly inelastic resonance in K<sup>+</sup>p scattering. To study the inelastic K<sup>+</sup>p reactions, a 400 K exposure has been taken at the L.R.L. 25 inch bubble chamber. The data are spread over seven K<sup>+</sup> momenta between 1.37 and 2.17 GeV/c.</p> <p>Cross-sections have been measured for the reaction K<sup>+</sup>p pK+ which is dominated by the quasi-two body channels K and K*N. Both these channels are strongly peripheral, as at other momenta. The decay of the is in good agreement with the predictions of the rho-photon analogy of Stodolsky and Sakurai. The data on the K*p channel show evidence of both pseudo scalar and vector exchange.</p> <p>Cross-sections for the final state pK<sup>+</sup>+- shows a strong contribution from the quasi-two body channel K*. This reaction is also very peripheral even at threshold. The decay angular distributions indicate the reaction is dominated as at higher momenta by a pion exchange mechanism. The data are also in good agreement with the quark model predictions of Bialas and Zalewski for the K* and decay.</p>

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I. Ejercicios cortos de programacin: - Enunciados. - Soluciones propuestas. II. Ejercicios largos: - Componentes electrnicos. - Hbitos de consumo: bebidas. - Emisora de radio. - Gasolinera. - Tienda. - Central elctrica. - Ladrn Elca Comayor. - Cumbres de montaa. - Autopista. - Sala de juegos. - Farolas. - Pueblos de Guipzcoa. - Olimpiadas. - Ventas S.A. - Accidentes de circulacin. - Euskadi Irratia. - San Sebastin.

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I. Programazioko ariketa laburrak: - Enuntziatuak. - Soluzioen proposamenak. II. Ariketa luzeak: - Gailu elektronikoak. - Kontsumo ohiturak: edariak. - Irratsaioa. - Gasolindegia. - Denda. - Zentral elektrikoa. - Elca Comayor lapurra. - Medi igoerak. - Autopista. - Joko aretoa. - Farolak. - Herrien arteko distantziak. - Olinpiadak. - Ventas S.A. - Heriozko istripuak. - Euskadi Irratia. - San Sebastianak