Piezophototronics

Piezo-phototronic effect is a three-way coupling effect of piezoelectric, semiconductor and photonic properties in non-central symmetric semiconductor materials, using the piezoelectric potential (piezopotential) that is generated by applying a strain to a semiconductor with piezoelectricity to control the carrier generation, transport, separation and/or recombination at metal–semiconductor junction or p–n junction for improving the performance of optoelectronic devices, such as photodetector,[1] solar cell[2] and light-emitting diode.[3] Prof. Zhong Lin Wang at Georgia Institute of Technology proposed the fundamental principle of this effect in 2010.[4][5]

Mechanism
Energy band diagrams for a p-n junction (a) with the absence of piezo-charges, and (b, c) with the presence of positive and negative piezo-charges at the junction, respectively. The red solid lines are the band diagrams with considering the piezopotential. Holes are trapped at the interface due to the piezopotential modified energy band, which will enhance the electron-hole recombination efficiency.
Schematic diagram showing the three-way coupling among piezoelectricity, photoexcitation and semiconductor properties.

When a p-type semiconductor and a n-type semiconductor form a junction, the holes in the p-type side and the electrons in the n-type side tend to redistribute around the interface area to balance the local electric field, which results in a charge depletion layer. The diffusion and recombination of the electrons and holes in the junction region is closely related to the optoelectronic properties of the device, which is greatly affected by the local electric field distribution. The existence of the piezo-charges at the interface introduces three effects: a shift in local electronic band structure due to the introduced local potential, a tilt of the electronic band structure over the junction region for the polarization existing in the piezoelectric semiconductor, and a change in the charge depletion layer due to the redistribution of the local charge carriers to balance the local piezo-charges. The positive piezoelectric charges at the junction lower the energy band and the negative piezoelectric charges raise the energy band in n-type semiconductor region near the junction region. A modification in the local band by piezopotential may be effective for trapping charges so that the electron-hole recombination rate can be largely enhanced, which is very beneficial for improving the efficiency of a light-emitting diode. Furthermore, the inclined band tends to change the mobility of the carriers moving toward the junction. The materials for piezo-phototronics should have three basic properties: piezoelectricity, semiconductor property, and photon excitation property [5]. Typical materials are the wurtzite structures, such as ZnO, GaN and InN. the three-way coupling among piezoelectricity, photoexcitation and semiconductor properties, which is the basis of piezotronics (piezoelectricity-semiconductor coupling), piezophotonics (piezoelectric-photon excitation coupling), optoelectronics, and piezo-phototronics piezoelectricity-semiconductor-photoexcitation). The core of these coupling relies on the piezopotential created by the piezoelectric materials.

Experimental realization

Van der Waals heterostructures based on graphene and transition metal dichalcogenides (TMD) are promising for the realization of piezophototronic effect.[6] It has been shown that the photo-response of graphene/MoS2 junction can be tuned by means of tensile stress manifesting piezophototronic effect in TMD devices.[6]

References
  1. Yang, Qing; Guo, Xin; Wang, Wenhui; Zhang, Yan; Xu, Sheng; Lien, Der Hsien; Wang, Zhong Lin (4 October 2010). "Enhancing Sensitivity of a Single ZnO Micro-/Nanowire Photodetector by Piezo-phototronic Effect" (PDF). ACS Nano. American Chemical Society (ACS). 4 (10): 6285–6291. doi:10.1021/nn1022878. ISSN 1936-0851. PMID 20919691.
  2. Yang, Ya; Guo, Wenxi; Zhang, Yan; Ding, Yong; Wang, Xue; Wang, Zhong Lin (9 November 2011). "Piezotronic Effect on the Output Voltage of P3HT/ZnO Micro/Nanowire Heterojunction Solar Cells" (PDF). Nano Letters. American Chemical Society (ACS). 11 (11): 4812–4817. Bibcode:2011NanoL..11.4812Y. doi:10.1021/nl202648p. ISSN 1530-6984. PMID 21961812.
  3. Yang, Qing; Wang, Wenhui; Xu, Sheng; Wang, Zhong Lin (14 September 2011). "Enhancing Light Emission of ZnO Microwire-Based Diodes by Piezo-Phototronic Effect" (PDF). Nano Letters. American Chemical Society (ACS). 11 (9): 4012–4017. Bibcode:2011NanoL..11.4012Y. doi:10.1021/nl202619d. ISSN 1530-6984. PMID 21823605.
  4. Hu, Youfan; Chang, Yanling; Fei, Peng; Snyder, Robert L.; Wang, Zhong Lin (15 January 2010). "Designing the Electric Transport Characteristics of ZnO Micro/Nanowire Devices by Coupling Piezoelectric and Photoexcitation Effects" (PDF). ACS Nano. American Chemical Society (ACS). 4 (2): 1234–1240. doi:10.1021/nn901805g. ISSN 1936-0851. PMID 20078071.
  5. Wang, Zhong Lin (2010). "Piezopotential gated nanowire devices: Piezotronics and piezo-phototronics" (PDF). Nano Today. Elsevier BV. 5 (6): 540–552. doi:10.1016/j.nantod.2010.10.008. ISSN 1748-0132.
  6. Javadi, Mohammad; Darbari, Sara; Abdi, Yaser; Ghasemi, Fooad (2016-05-29). "Realization of a Piezophototronic Device Based on Reduced Graphene Oxide/MoS2 Heterostructure". IEEE Electron Device Letters. 37 (5): 677–680. doi:10.1109/LED.2016.2547993. ISSN 1558-0563.
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