1996
DOI: 10.1016/0040-6090(95)08072-4
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On the origin of blue luminescence arising from atmospheric impregnation of oxidized porous silicon

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Cited by 96 publications
(68 citation statements)
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“…Some researchers suggest that C-related defects are responsible for the blue PL characteristics [2,6] Others alternatively claim that the presence of OH groups adsorbed on the surface of porous silicon are associated with this type of output [7]. Although the physical origin of the blue PL band in porous Si has not been unambiguously clarified yet, it is quite likely that C-and/or OH-related surface defects play crucial role, either directly or indirectly, in exhibiting the blue PL band.…”
Section: Introductionmentioning
confidence: 99%
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“…Some researchers suggest that C-related defects are responsible for the blue PL characteristics [2,6] Others alternatively claim that the presence of OH groups adsorbed on the surface of porous silicon are associated with this type of output [7]. Although the physical origin of the blue PL band in porous Si has not been unambiguously clarified yet, it is quite likely that C-and/or OH-related surface defects play crucial role, either directly or indirectly, in exhibiting the blue PL band.…”
Section: Introductionmentioning
confidence: 99%
“…Blue photoluminescence (PL), which is characterized by single-exponential [1] or multi-exponential decay [2] on the order of nanoseconds, has been reported from a variety of porous silicon such as aged, chemically oxidized and thermally oxidized samples [3] Although there still exists an argument that the blue PL is explained by a quantum confined mechanism [4], the weight of evidence is in favor of a defect-related model [3,5]. Some researchers suggest that C-related defects are responsible for the blue PL characteristics [2,6] Others alternatively claim that the presence of OH groups adsorbed on the surface of porous silicon are associated with this type of output [7].…”
Section: Introductionmentioning
confidence: 99%
“…The F band luminescence, usually centered between 420 and 500 nm, decays on the nanosecond time scale. This can be observed on porous silicon samples aged in air or intentionally oxidized, and is thought to originate from structural defects in the silicon nanocrystal oxide shell, or from the luminescence of very small silicon nanocrystals [19,39,[69][70][71][72]. Other PL bands have been previously reported for porous silicon: the so-called UV band (centered around 350 nm), and the R band (ranging from 1100-1500 nm) [59].…”
Section: Optical Characterizationmentioning
confidence: 99%
“…23,41,45 Changes in the PL of nanocrystalline Si over time, presumably alongside alterations in the surface chemistry or size of the particles, have been reported consistently across the literature. 23,30,46 However, the promise of robust, inorganic fluorophores with size-dependent optical properties continues to motivate researchers to develop strategies to mitigate the changing PL energy and intensity. bandgap to occur, they must be coupled with phonons (i.e., lattice vibrations), which have enough momentum to elicit the transition.…”
Section: Technological Developments Leading To Photoluminescent Siliconmentioning
confidence: 99%
“…40,[43][44][45][46][47][48][49][50][51][52][53] For example, surface reconstructions, chemical impurities, lattice vacancies, dislocations, etc., can produce characteristic energy states (defect states)…”
Section: Effect Of Defects On Photoluminescence From Silicon Nanopartmentioning
confidence: 99%