Financial x-ray

An over view of the financial x-ray service. JL

EDTA溶胶凝胶法制备La_2Ni_(1-x)M_xO_4(M=Cu,Fe)稀土复合氧化物

本文以EDTA溶胶凝胶法合成K2NiF4型稀土复合氧化物La2Ni1-xMxO4(M=Cu,Fe),并对反应生成粉体分别进行SEM表征与XRD测试。结果表明,选取合适的制备工艺,可以形成La2Ni1-xMxO4(M=Cu,Fe)稀土复合氧化物材料;随着掺杂离子半径增大,生成材料晶格常数a增大同时,c减少,粉体颗粒粒径较大,同时少量杂相存在。

Análisis dieléctrico del compuesto La(1-x)Ca(x)MnO3 [x=0.2]

Lan honen helburua La1-x Cax MnO3 [x ~ 0.2] (perovskiten familiakoa) laginaren azterketan oinarritzen da. "High resolution dielectric analyzer" tresnari esker permitibitate dielektrikoa neurtuko da eta honen bitartez erresistentzia eta eroankortasun elektrikoa. Azterketa hau [10-2, 107] Hz maiztasun-tarte batean eta tenperatura desberdinetan (150K, 170K, 190K, 210K, 230K, 300K) burutuko da, ondoren materialak magnitude hauen bariazioekiko duen erantzuna aztertuz.

Dextran and protamine-based solid lipid nanoparticles as potential vectors for the treatment of X-linked juvenile retinoschisis

This is a copy of an article published in the Human gene therapy © 2012 copyright Mary Ann Liebert, Inc.; Human gene therapy is available online at: http://online.liebertpub.com.

Malcolm X y Steve Biko: la difícil recuperación de una identidad

Antonio Duplá Ansuategui, Piedad Frías Nogales e Iban Zaldúa (editores)

Small angle X-ray scattering of the colloidal crystal

The monodisperse polystyrene spheres are assembled into the colloidal crystal on the glass substrate by vertical deposition method, which is aimed at the so-called photonic crystal applications. The structural information of the bulk colloidal crystal is crucial for understanding the crystal growth mechanism and developing the various applications of colloidal crystal. Small-angle X-ray scattering (SAXS) technique was used to obtain the bulk structure of the colloidal crystal at Beamline 1W2A of BSRF. It is found that the SAXS pattern is sensitive to the relative orientation between the colloidal sample and the incident X-ray direction. The crystal lattice was well distinguished and determined by the SAXS data.

Angular distribution and conversion of multi-keV L-shell X-ray sources produced from nanosecond laser irradiated thick-foil targets

An experimental study on the angular distribution and conversion of multi-keV X-ray sources produced from 2 ns-duration 527nm laser irradiated thick-foil targets on Shenguang II laser facility (SG-II) is reported. The angular distributions measured in front of the targets can be fitted with the function of f(theta) = alpha+ (1- alpha)cos(beta) theta (theta is the viewing angle relative to the target normal), where alpha = 0.41 +/- 0.014, beta = 0.77 +/- 0.04 for Ti K-shell X-ray Sources (similar to 4.75 keV for Ti K-shell), and alpha = 0.085 +/- 0.06, beta = 0.59 +/- 0.07 for Ag/Pd/Mo L-shell X-ray Sources (2-2.8 keV for Mo L-shell, 2.8-3.5 keV for Pd L-shell, and 3-3.8 keV for Ag L-shell). The isotropy of the angular-distribution of L-shell emission is worse than that of the K-shell emission at larger viewing angle (>70 degrees), due to its larger optical depth (stronger self-absorption) in the cold plasma side lobe Surrounding the central emission region, and in the central hot plasma region (emission region). There is no observable difference in the angular distributions of the L-shell X-ray emission among Ag, Pd, and Mo. The conversion efficiency of Ag/Pd/Mo L-shell X-ray sources is higher than that of the Ti K-shell X-ray sources, but the gain relative to the K-shell emission is not as high as that by using short pulse lasers. The conversion efficiency of the L-shell X-ray sources decrease, with increasing atomic numbers (or X-ray photon energy), similar to the behavior of the K-shell X-ray Source.