“…Another approach is the use of a thermally grown silicon oxide layer or a combination of a thin thermal oxide film with a dielectric capping layer [9][10][11][12][13][14]. The literature provides some investigations of stack systems consisting of thermally or wet chemically grown or deposited oxide layers with different capping layers [8,[14][15][16]. So far, the role of the oxide layer thickness was not investigated in detail.…”
We investigate the role of a few nm thin thermal oxide films in PECVD passivation layer systems. Our results show that an intermediate thermal oxide layer located between the Si substrate and the PECVD layers has a strong impact on the interface properties. Capacitance-voltage measurements reveal that for Al 2O 3 and SiN X passivation layers, the oxide film lowers or suppresses the formation of fixed charges. Adjusting the oxide film thickness therefore permits the control of band bending and thus field effect passivation at the interface. For SiO X capping layers, a thermal oxide thickness of a few nm is sufficient to reduce the interface trap density, enabling surface recombination velocities as low as a few cm/s
“…Another approach is the use of a thermally grown silicon oxide layer or a combination of a thin thermal oxide film with a dielectric capping layer [9][10][11][12][13][14]. The literature provides some investigations of stack systems consisting of thermally or wet chemically grown or deposited oxide layers with different capping layers [8,[14][15][16]. So far, the role of the oxide layer thickness was not investigated in detail.…”
We investigate the role of a few nm thin thermal oxide films in PECVD passivation layer systems. Our results show that an intermediate thermal oxide layer located between the Si substrate and the PECVD layers has a strong impact on the interface properties. Capacitance-voltage measurements reveal that for Al 2O 3 and SiN X passivation layers, the oxide film lowers or suppresses the formation of fixed charges. Adjusting the oxide film thickness therefore permits the control of band bending and thus field effect passivation at the interface. For SiO X capping layers, a thermal oxide thickness of a few nm is sufficient to reduce the interface trap density, enabling surface recombination velocities as low as a few cm/s
“…Samples were cleaned in sulphuric acid mixture with hydrogen peroxide at 110°C for 10 min to oxidate and remove organic impurities on surface and also to dissolve metal ions from surface to solution. Then, samples were treated in hydrofluoric acid for 1 min at room temperature to remove silicon oxide which is 2 to 4 nm [4]. At last, samples were capped with PEALD Al 2 O 3 using Al(CH 3 ) 3 (TMA) and plasma O as reactants.…”
Plasma-enhanced atom layer deposition (PEALD) can deposit denser films than those prepared by thermal ALD. But the improvement on thickness uniformity and the decrease of defect density of the films deposited by PEALD need further research. A PEALD process from trimethyl-aluminum (TMA) and oxygen plasma was investigated to study the influence of the conditions with different plasma powers and deposition temperatures on uniformity and growth rate. The thickness and refractive index of films were measured by ellipsometry, and the passivation effect of alumina on n-type silicon before and after annealing was measured by microwave photoconductivity decay method. Also, the effects of deposition temperature and annealing temperature on effective minority carrier lifetime were investigated. Capacitance-voltage and conductance-voltage measurements were used to investigate the interface defect density of state (D it ) of Al 2 O 3 /Si. Finally, Al diffusion P + emitter on n-type silicon was passivated by PEALD Al 2 O 3 films. The conclusion is that the condition of lower substrate temperature accelerates the growth of films and that the condition of lower plasma power controls the films' uniformity. The annealing temperature is higher for samples prepared at lower substrate temperature in order to get the better surface passivation effects. Heavier doping concentration of Al increased passivation quality after annealing by the effective minority carrier lifetime up to 100 μs.
“…This would provide a means to combine a relatively straightforward and economically viable method of surface cleaning/conditioning with the formation of a very thin SiO 2 film and the passivation of the surface. 43,[46][47][48] In this article we extend previous work by carrying out a systematic investigation of the surface passivation induced by stacks of chemically grown SiO 2 films and PECVD a-SiN x :H and ALD Al 2 O 3 capping films. This is done for three different wet chemically grown SiO 2 films such that the passivation performance induced by the aSiN x :H and Al 2 O 3 films can be directly compared for differently prepared surfaces and for the two dielectric films.…”
mentioning
confidence: 97%
“…The most common conditioning process is H-termination of Si surfaces realized by hydrofluoric acid treatments (HF-dip). The surface passivation can be subsequently realized by depositing dielectric layers such as single-layer SiO 40,43,48 It should be noted that such an ultrathin SiO 2 film can also be present when passivating an H-terminated Si surface as a native and/or interfacial SiO 2 film can grow unintentionally when H-terminated Si surfaces are exposed to the ambient (for a significant amount of time) 2,49 or when oxides (such as Al 2 O 3 ) are deposited on the Si. 14,19,50,51 From recent studies it is known that an interfacial SiO 2 layer between the passivation material and the Si has a significant effect on the surface passivation of Al 2 O 3 and a-SiN x :H films as shown for thin ALD, PECVD and thermally grown SiO 2 interlayers.…”
mentioning
confidence: 99%
“…In these aspects, the results described in this article distinguish themselves from those in our previous publication. 43 Additionally, the Al 2 O 3 stacks were investigated by corona charging experiments to reveal the role of chemical passivation and field-effect passivation. This study was complemented by second harmonic generation analysis which also yields insight into the field-effect passivation.…”
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