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41por Lönnrot, Satu, Suorsa, Valtteri, Paajanen, Johanna, Hatanpää, Timo, Ritala, Mikko, Koivula, Risto“…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. …”
Publicado 2019
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44por Ahmad, A, Sheikh, S, Shah, T, Reddy, MS, Prasad, BSV, Verma, KK, Chandrakant, BB, Paithankar, M, Kale, P, Solanki, RV, Patel, R, Barkate, H, Ahmad, I“…Thus, endoxifen has been shown as a promising novel antimanic or mood stabilizing agent.…”
Publicado 2016
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45por Warashina, Tomoro, Yamamura, Shigeki, Suzuki, Haruo, Amachi, Seigo, Arakawa, Kazuharu“…SVR strains proliferate using antimonate [Sb(V)] as an electron acceptor, providing insights into the antimony reduction mechanism.…”
Publicado 2021
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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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47por Singh, Satyendra, Singh, Archana, Singh, Ajendra, Rathore, Sanjeev, Yadav, B. C., Tandon, Poonam“…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). …”
Publicado 2020
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48por Gebhardt, M., Heuermann, T., Klas, R., Liu, C., Kirsche, A., Lenski, M., Wang, Z., Gaida, C., Antonio-Lopez, J. E., Schülzgen, A., Amezcua-Correa, R., Rothhardt, J., Limpert, J.“…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. …”
Publicado 2021
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50por Morales-Bautista, Jacob, Guillén-Bonilla, Héctor, Guillén-Bonilla, Alex, Rodríguez-Betancourtt, Verónica-María, Ramírez-Ortega, Jorge Alberto, Guillén-Bonilla, José Trinidad“…The crystalline phase obtained at 800 °C of trirutile-type nickel antimonate was confirmed with powder X-ray diffraction. …”
Publicado 2023
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52por Aderholz, Michael, Deutschmann, Martin, Rumpf, K, Speth, R, Steinberg, R, Klugow, J, Lanius, Karl, Nowak, S, Pose, D, Schller, H, Cocconi, Vanna T, Ely, R P, Hausen, J, Kellner, Gottfried, Kittel, E W, Lindblom, K P C, Morrison, Douglas Robert Ogston, Paler, Kenneth, Tøfte, Harald, Dallman, David Peter, Dornan, Peter J, Losty, Michael J, Buschbeck, Brigitte, Markytan, Manfred, Otter, Gerd, Porth, Paul, Schmid, PEnlace del recurso
Publicado 1969
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54por Antimanon, Sompot, Anantayanon, Jutamas, Wannawilai, Siwaporn, Khongto, Bhimabol, Laoteng, KobkulEnlace del recurso
Publicado 2020
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55por Paryev, E.Ya.“…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>. …”
Publicado 2022
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57por Mougharbel, Ali S., Ahmedi, Sihana, Bhattacharya, Saurav, Rajan, Ananthu, Kortz, UlrichEnlace del recurso
Publicado 2021
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