2006
DOI: 10.1063/1.2402239
|View full text |Cite
|
Sign up to set email alerts
|

Band gap energy determination by photoacoustic spectroscopy under continuous light excitation

Abstract: In this work the authors used the photoacoustic spectroscopy under continuous light excitation to determine the optical band gap of semiconductors. The experiments were performed in lead iodide PbI2 and hexagonal silicon carbide 4H-SiC samples. The nonradiative relaxation processes are discussed in terms of the generated signal. A mechanism to describe the signal increase/decrease under the continuous excitation is presented. The results showed that the method was useful to locate the band gap directly from th… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
12
0
1

Year Published

2010
2010
2020
2020

Publication Types

Select...
7
1

Relationship

1
7

Authors

Journals

citations
Cited by 19 publications
(13 citation statements)
references
References 23 publications
0
12
0
1
Order By: Relevance
“…(eV)Cryst. StructureMoS 2 1.370.121.870.040.501.251.19~1.3 * 1.87 34 2H polytypeMoSe 2 1.250.141.560.00.311.111.01~1.1 ** 1.56 34 MoTe 2 0.890.061.060.0270.170.830.80~0.8 * 1.15 25*** HfS 2 1.390.262.090.1310.701.031.001.96 44 NA1T polytypeHfSe 2 1.210.131.490.3800.281.080.961.19 44 NAWS 2 1.570.152.050.0270.481.421.30~1.3 ** 2.05 33 2H polytypeWSe 2 1.330.091.650.0200.321.241.16~1.3 ** 1.70 33 ReS 2 1.370.111.550.0490.181.261.201.52 36** 1.554 36** 3R polytypeReSe 2 1.180.061.310.0580.031.121.061.36 36** 1.387 36** SnS 2 2.360.23NANANA2.132.00~2.2 ** NA2H polytypeSnSe 2 1.240.10NANANA1.141.06NANAGaS2.870.372.920.3900.052.50<...>…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…(eV)Cryst. StructureMoS 2 1.370.121.870.040.501.251.19~1.3 * 1.87 34 2H polytypeMoSe 2 1.250.141.560.00.311.111.01~1.1 ** 1.56 34 MoTe 2 0.890.061.060.0270.170.830.80~0.8 * 1.15 25*** HfS 2 1.390.262.090.1310.701.031.001.96 44 NA1T polytypeHfSe 2 1.210.131.490.3800.281.080.961.19 44 NAWS 2 1.570.152.050.0270.481.421.30~1.3 ** 2.05 33 2H polytypeWSe 2 1.330.091.650.0200.321.241.16~1.3 ** 1.70 33 ReS 2 1.370.111.550.0490.181.261.201.52 36** 1.554 36** 3R polytypeReSe 2 1.180.061.310.0580.031.121.061.36 36** 1.387 36** SnS 2 2.360.23NANANA2.132.00~2.2 ** NA2H polytypeSnSe 2 1.240.10NANANA1.141.06NANAGaS2.870.372.920.3900.052.50<...>…”
Section: Resultsmentioning
confidence: 99%
“…PA spectroscopy can be used to determine the band gap as shown in refs 31,34,37 as well as the impurity and defect-related absorption 33,35 . Moreover, this technique can be used to study the surface and bulk nonradiative recombination 32 and the thermal diffusivity 36 .…”
Section: Introductionmentioning
confidence: 99%
“…7 In this letter, we analyze the PA-signal behavior of a nanostructured WO 3 film under continuous laser excitation, using an experimental procedure similar to that described in Ref. 12. The influence of the continuous excitation in the mechanisms responsible for the generation of the PA signal is discussed and adopted to determine the band-gap energy directly from the experimental optical absorption spectra.…”
mentioning
confidence: 99%
“…Additional details of experimental conditions are described in Ref. 12. The measurements were carried out in the following way: initially, the PA spectra were taken while the sample was excited only by the modulated light.…”
mentioning
confidence: 99%
“…A espectroscopia fotoacústica é usada extensivamente para determinar as propriedades ópticas dos materiais semicondutores pelo processo de transferência de energia que resulta na geração de calor. Recentemente foi proposto, através da EFA sobre condições contínuas de laser de excitação, uma maneira de fazer medidas diretas do valor de gap de energia dos semicondutores [47] . Geralmente o valor do gap de energia, para um semicondutor de gap direto, é assumido como o ponto inicial da absorção obtido a partir da curva do quadrado do coeficiente de absorção versus a energia do fóton (α 2 versus hν, como realizado para os filmes de PbI 2 ) ou usando o ponto inicial de absorção da curva do quadrado do coeficiente de absorção vezes a energia versus a energia, [(α hν) 2 versus hν], para semicondutores de gap indireto [46,47] .…”
Section: Caracterização óPticaunclassified