Mostrando 41 - 60 Resultados de 247 Para Buscar 'antimasón~', tiempo de consulta: 3.91s Limitar resultados
  1. 41
    “…The submicron fibers were obtained from an optimized electroblowing synthesis that resulted in elastic and uniform fibers with a tetragonal structure and high length-to-diameter ratio. In antimonate (Sb(v)) adsorption experiments, the higher calcination temperature (350 °C) of the fibers did not seem to decrease the Sb(v) adsorption capacity excessively since the high theoretical adsorption capacities were 113 mg g(−1) and 58 mg g(−1) for the aggregate and fibers, respectively. …”
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    “…SVR strains proliferate using antimonate [Sb(V)] as an electron acceptor, providing insights into the antimony reduction mechanism.…”
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  6. 46
    “…Trirutile zinc antimonate (ZnSb(2)O(6)) nano-cubes/cuboids have been fabricated by a sol–gel spin-coating method using polyethylene glycol (PEG) as the structure-directing agent. …”
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  7. 47
    “…Herein, cobalt antimonate (CoSb(2)O(6)) nanospheres were fabricated via the sol–gel spin-coating process and employed as a functional liquefied petroleum gas (LPG) sensor at room temperature (25 °C). …”
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  8. 48
    “…Here, we establish a novel route toward powerful and easy-to-use SXR sources by presenting a compact experiment in which nonlinear pulse self-compression to the few-cycle regime is combined with phase-matched high-order harmonic generation in a single, helium-filled antiresonant hollow-core fibre. This enables the first 100 kHz-class repetition rate, table-top soft X-ray source that delivers an application-relevant flux of 2.8 × 10(6) photon s(−1) eV(−1) around 300 eV. …”
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  15. 55
    por Paryev, E.Ya.
    Publicado 2022
    “…We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of <math altimg="si1.svg"><mi>J</mi><mo stretchy="false">/</mo><mi>ψ</mi></math> mesons off protons as well as off carbon and tungsten target nuclei at near-threshold incident antikaon energies by considering these elementary production channels as well as by assuming the spin-parity assignment of the hidden-charm resonance <math altimg="si4.svg"><msub><mrow><mi>P</mi></mrow><mrow><mi>c</mi><mi>s</mi></mrow></msub><msup><mrow><mo stretchy="false">(</mo><mn>4459</mn><mo stretchy="false">)</mo></mrow><mrow><mn>0</mn></mrow></msup></math> with strangeness as <math altimg="si5.svg"><msup><mrow><mi>J</mi></mrow><mrow><mi>P</mi></mrow></msup><mo linebreak="goodbreak" linebreakstyle="after">=</mo><msup><mrow><mo stretchy="false">(</mo><mn>3</mn><mo stretchy="false">/</mo><mn>2</mn><mo stretchy="false">)</mo></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">−</mo></mrow></msup></math> within six different scenarios for the branching ratio <math altimg="si6.svg"><mi>B</mi><mi>r</mi><mo stretchy="false">[</mo><msub><mrow><mi>P</mi></mrow><mrow><mi>c</mi><mi>s</mi></mrow></msub><msup><mrow><mo stretchy="false">(</mo><mn>4459</mn><mo stretchy="false">)</mo></mrow><mrow><mn>0</mn></mrow></msup><mo stretchy="false">→</mo><mi>J</mi><mo stretchy="false">/</mo><mi>ψ</mi><mi mathvariant="normal">Λ</mi><mo stretchy="false">]</mo></math> of the decay <math altimg="si7.svg"><msub><mrow><mi>P</mi></mrow><mrow><mi>c</mi><mi>s</mi></mrow></msub><msup><mrow><mo stretchy="false">(</mo><mn>4459</mn><mo stretchy="false">)</mo></mrow><mrow><mn>0</mn></mrow></msup><mo stretchy="false">→</mo><mi>J</mi><mo stretchy="false">/</mo><mi>ψ</mi><mi mathvariant="normal">Λ</mi></math>. …”
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    por Paniagua Navarro, Antonio
    Publicado 2004
    Materias: “…Animacón por computadora.…”
    Libro
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