Quantum Yield Investigation of Ag−BaO Thin Film

Abstract

Ag-BaO thin films have been fabricated by evaporating silver into BaO semiconductor thin film in ultrahigh vacuum and the quantum yield distribution in the visible region between 1.5 and 3.7 eV has been measured. The quantum yield spectra have a peak when the energy of the incident light is 2.5 eV. The direct transitions and surface plasmon resonance of silver nanoparticles appear to be very important in determining the shape of quantum yield spectra. The explanation for the small discrepancy between the experimental result and the theoretical data is given.

Highly transparent and conductive electrodes enabled by scalable printing-and-sintering of silver nanowires

“…One is to pattern Ag NWs in deterministic shapes and sizes. A variety of techniques have been utilized to pattern the Ag NWs, such as photolithography [14,20], shadow masking [21,22], ultraviolet ozone surface treatment [23,24], and dry transfer process [25]. However, these techniques either require multiple processing steps or suffer from limited patterning size that also limits the patterning efficiency.…”

Hydration of Arylacetylenes Promoted by the Photothermal ­Effect of Gold Nanoparticles

“…For example, Joshi reported the successful hydration of the arylacetylenes at high temperature and high pressure, 9 and Wang achieved similar approaches in the presence of H 2 SO 4 at 80 °C. 10 Moreover, various metal species had been applied in such process as the catalysts, 11 such as Bi(NO 3 ) 3 ·5H 2 O, 12 (Ph 3 P)AuCH 3 , 13 Au(I)(NHC), 14 AgSbF 6 , 15 PdCl 2 , 16 and FeCl 3 . 17 Typically, the functionalized gold (Au) nanomaterials, Au-SH@SO 3 H-SBA-15 2 and Au-HS@SO 3 H-PMO(Et), 18 had also been reported as efficient catalysts for the hydration of the alkynes.…”

Кремниевые Светодиоды С Люминесценцией (113) Дефектов

“…Предположение о взаимосвязи (113) дефектов, сформированных в процессе двухступенчатого длительного отжига кремния, выращенного методом Чохральского, и линии излучения на длине волны 1.37 мкм было высказано в работе [7]. Исследования образцов, имплантированных ионами Si + с последующим отжигом в инертной атмосфере [8][9][10], или имплантированных ионами О + с последующим отжигом в хлорсодержащей атмосфере [11][12][13], методами высокоразрешающей электронной микроскопии и фотолюминесценции подтвердили, что линия 1.37 мкм принадлежит (113) дефекту. Также было показано, что фотолюминесценция наблюдается и при температурах выше азотной (> 77 K) [7,9,13].…”