2018
DOI: 10.1002/adma.201804945
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Ultrasensitive 2D Bi2O2Se Phototransistors on Silicon Substrates

Abstract: 2D materials have shown great potential for high-performance electronic devices, thanks to their dangling-bond-free surface and atomic thickness which bring merits of high carrier mobility, efficient channel current regulation, and higher degree of vertical integration. [1][2][3][4][5] Many 2D semiconducting materials have shown outstanding phototransistor performance, such as MoS 2 , [6][7][8] WSe 2 , [9,10] GaTe, [11,12] and SnSe 2 , [13][14][15] because of their suitable energy bandgap and high mobility.

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Cited by 210 publications
(227 citation statements)
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References 44 publications
(104 reference statements)
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“…Under UV illumination (405 nm) with increasing power density from 6.7 to 866.8 μW cm −2 , I light is markedly enhanced and the corresponding photocurrent ( I ph = I light − I dark ) was instantly generated and gradually increased from 5.2 to 111 nA ( V G =10 V, Figure b), and the maximum P value (photocurrent on/off ratio) was estimated to be 353 (light intensity: 866.8 μW cm −2 , V G =20 V). The I ph value can be expressed by a simple law ( I ph ∝ P 0.61 ) from the log–log plot of I ph dependence on the light intensity and exhibits a sublinear response, which can be ascribed to the process involved in the trap states induced by the defects or charge impurities present in the TMCA microrod and the semiconductor/dielectric interface (Figure d) . In addition, the threshold voltage shift (Δ V th , towards more positive values) also exhibits an approximately linear relationship as a function of the power density, and the maximum Δ V th is up to 73 V (Figure e), which is derived from filling of the trap sites by the photogenerated carriers, which causes injection and accumulation of additional holes in the active layer .…”
Section: Resultsmentioning
confidence: 99%
“…Under UV illumination (405 nm) with increasing power density from 6.7 to 866.8 μW cm −2 , I light is markedly enhanced and the corresponding photocurrent ( I ph = I light − I dark ) was instantly generated and gradually increased from 5.2 to 111 nA ( V G =10 V, Figure b), and the maximum P value (photocurrent on/off ratio) was estimated to be 353 (light intensity: 866.8 μW cm −2 , V G =20 V). The I ph value can be expressed by a simple law ( I ph ∝ P 0.61 ) from the log–log plot of I ph dependence on the light intensity and exhibits a sublinear response, which can be ascribed to the process involved in the trap states induced by the defects or charge impurities present in the TMCA microrod and the semiconductor/dielectric interface (Figure d) . In addition, the threshold voltage shift (Δ V th , towards more positive values) also exhibits an approximately linear relationship as a function of the power density, and the maximum Δ V th is up to 73 V (Figure e), which is derived from filling of the trap sites by the photogenerated carriers, which causes injection and accumulation of additional holes in the active layer .…”
Section: Resultsmentioning
confidence: 99%
“…Figure c depicts the measured photocurrent of the In 2 S 3 /graphene/Si PD as a function of 405 nm light intensity at a fixed V ds = −2 V. The photocurrent can be expressed by a simple power law I ph ∝ P 0.18 for weak light and I ph ∝ P 0.02 for strong light. Here, the nonunity of exponent can be associated with the complex process of electron–hole excitation, trapping, and recombination within the In 2 S 3 /graphene/Si heterojunction …”
Section: Resultsmentioning
confidence: 99%
“…Very lately, a new star ternary material Bi 2 O 2 Se joins into the 2D family . Bi 2 O 2 Se possesses high Hall mobility (29 000 cm 2 V −1 s −1 at 1.9 K and 450 cm 2 V −1 s −1 at room temperature) and appropriate bandgap of 0.8 eV, which pave the way for high sensitivity and fast response IR photodetection.…”
Section: Individual 2d Metal Chalcogenides For Ir Photodetectionmentioning
confidence: 99%