Next Article in Journal
All–Inorganic Perovskite Quantum Dot–Based Blue Light–Emitting Diodes: Recent Advances and Strategies
Previous Article in Journal
Solid-State Synthesis of Cobalt/NCS Electrocatalyst for Oxygen Reduction Reaction in Dual Chamber Microbial Fuel Cells
 
 
Search for Articles:
Title / Keyword
Author / Affiliation / Email
Journal
Article Type
 
 
Advanced Search
 
Section
Special Issue
Volume
Issue
Number
Page
 
Journals
Nanomaterials
Volume 12
Issue 24
10.3390/nano12244370
nanomaterials-logo
Submit to this Journal Review for this Journal Propose a Special Issue
► Article Menu

Article Menu

share Share announcement Help format_quote Cite question_answer Discuss in SciProfiles thumb_up
...
Endorse textsms
...
Comment
first_page
settings
Order Article Reprints
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Acoustically Stimulated Charge Transport in Graphene Film

by
Dmitry Roshchupkin
1,*,
Oleg Kononenko
1,
Rashid Fakhrtdinov
1,
Evgenii Emelin
1 and
Alexander Sergeev
2
1
Institute of Microelectronics Technology and High Purity Materials Russian Academy of Sciences, 142432 Chernogolovka, Russia
2
Federal State Institution, Scientific Research Institute for System Analysis of the Russian Academy of Sciences, 117218 Moscow, Russia
*
Author to whom correspondence should be addressed.
Nanomaterials 2022, 12(24), 4370; https://doi.org/10.3390/nano12244370
Submission received: 21 November 2022 / Revised: 6 December 2022 / Accepted: 6 December 2022 / Published: 7 December 2022
(This article belongs to the Topic Application of Graphene-Based Materials)
Browse Figures
Review Reports Versions Notes

Abstract

:
The process of acoustically stimulated charge transport in the graphene film on the surface of the Y Z − cut of a LiNbO3 crystal was investigated. It was found that the dependence of the current in the graphene film on the frequency of the surface acoustic wave (SAW) excitation repeats the amplitude-frequency response of the SAW delay time line. It is shown that increasing the SAW amplitude leads to an increase in the current in the graphene film, and the current in the graphene film depends linearly on the amplitude of the high-frequency input signal supplied to the interdigital transducer (IDT, in dB). It is demonstrated that at a positive bias potential on the graphene film, the SAW propagation allows to change the direction of the current in the graphene film by changing the amplitude of the SAW. It is also shown that in the frequency range of the amplitude-frequency response of the SAW delay time line, the current in the graphene film can vary from positive to negative values depending on the frequency. The capability to control the SAW excitation frequency or the SAW amplitude makes it possible to control the value and direction of the current in the graphene film. The SAW propagation lets to collect and transport the photo-stimulated charges in the graphene film on the crystal surface.

1. Introduction

Modern acoustoelectronics is based on the use of surface and bulk acoustic waves for the transmission and processing of information in a real time mode [1]. Also, acoustoelectronic devices are actively used as physical quantity sensors, the principle of operation of which is based on the change of resonance excitation frequencies of acoustic waves in specific physical conditions (pressure, acceleration, temperature, humidity, etc.) [2,3,4,5,6].
Recently, the development of gas sensor acoustoelectronic devices is associated with the use of 1D (ZnO and AlN nanorods) and 2D crystals (graphene and graphene oxide) [7,8,9,10]. One-dimensional and 2D crystals on the surface of piezoelectric crystals act as adsorbents, which leads either to a change in the electrical properties of 1D and 2D crystals or to a change in their mass, which ultimately leads to a change in the velocity and excitation frequency of surface and bulk acoustic waves in crystals.
An interesting proposal is to use the surface acoustic waves in solar energy for acoustically stimulated transport of charge carriers generated in semiconductor structures under the influence of light [11,12,13,14]. In the future, the use of SAW in solar cells can increase the efficiency of cells up to 90% [14]. SAWs propagating in piezoelectric crystals (including GaN and GaAs crystals) have opposite potential values in the acoustic wave minima and maxima due to the piezoelectric effect. Electrons and holes generated in the semiconductor structure under the influence of sunlight are distributed, respectively, between the minima and maxima of the SAW. The charges are then carried by the SAW to the solar cell output at the velocity of an acoustic wave. The use of SAW in solar cells can increase the charge collection area in the semiconductor structure and increase the efficiency of solar cells. Perspectives in solar energy are also associated with the use of graphene [15,16], which can be used as transparent electrodes, and in which electron-hole pairs can also be generated under the influence of light. Moreover, the graphene film is a good medium for SAW propagation. A number of studies have demonstrated the possibility of charge transport by the surface acoustic wave in graphene [17,18,19], as well as the possibility of controlling the acoustic wave under the application of an electric potential to the graphene film [20]. In [21], the possibility of fabrication of the interdigital transducer (IDT) from graphene for SAW excitation was demonstrated. Here, the interest in the application of graphene is due to its association with its practically zero mass and the absence of influence on the SAW propagation. In [22], using the Talbot effect, the SAW propagation process was visualized and the dependence of the current in the graphene film on the SAW amplitude was studied. Also, the process of acoustically stimulated charge transport in the graphene film was visualized by scanning electron microscopy and the induced current method [23]. A number of studies have demonstrated the transport of charges generated by sunlight in the graphene film with the help of the SAW [24,25].
The purpose of these investigations is to study the process of the SAW propagation in the graphene film on the surface of a LiNbO3 ferroelectric crystal depending on the SAW amplitude and the bias potential on the graphene film. The process of charge transport in a graphene film under the conditions of generation of electron-hole pairs under the action of optical radiation is also studied.

2. Fabrication of Graphene/LiNbO3 SAW Delay Time Line

The Y Z − cut of a LiNbO3 crystal was used to study the process of the SAW propagation in the graphene film. This crystal cut has large values of piezoelectric moduli and a large value of the electromechanical coupling coefficient. The process of SAW propagation in the Y Z − cut of a LiNbO3 crystal is characterized by the autocollimation of the acoustic beam. The velocity of SAW propagation in the Y Z − cut of the LiNbO3 crystal is V = 3420 m/s. The well-known value of the SAW velocity in the Y Z − cut of a LiNbO3 crystal is V = 3488 m/s, but the actual value of the velocity depends on the particular crystal and can vary. The substrate size was 8 × 16 × 1 mm3. The substrate surface has been polished. The substrate roughness does not exceed 3 Å at the damaged layer thickness of 24 Å.
A SAW delay time line consisting of two identical interdigital transducers (IDTs) was fabricated on the surface of the Y Z − cut of a LiNbO3 crystal. The IDTs (input and output) were fabricated by photolithography and consisted of 25 pairs of Al electrodes. The period of the IDT electrodes was 15 μm, which corresponds to the SAW wavelength Λ = 30 μm. The aperture of the IDT was W = 50 × Λ = 1500 µm.
Figure 1 shows an optical micrograph of the SAW delay time line. A graphene film was formed on the substrate surface between two IDTs by a transfer method. Figure 2 shows the Raman spectra of the graphene film transferred to the surface of the Y Z − cut of a LiNbO3 crystal. In the left part of the spectrum, strong peaks of the LiNbO3 crystal are visible. The inset shows a zoomed-in part of the spectrum, in which the peaks of graphene (G, 2D, D+D”, 2D’) are visible. The spectrum demonstrates features characteristic of single-layer graphene, namely, a symmetric 2D peak with a full width at half-maximum FWHM = 28 cm−1 and intensity ratio I2D/IG = 2.1 [26,27]. In the inset of Figure 2, the peaks related to the Raman spectrum from the LiNbO3 substrate are marked by asterisks.
To study the acoustically stimulated charge transport on the graphene surface, four gold electrodes were fabricated (Figure 1). The distance between the electrodes was 800 µm. The two central electrodes were used to measure the current I in the graphene film; the distance between them was 800 µm. The two outermost electrodes were used to apply the bias potential U and the distance between them was 2400 µm.

3. Investigation of SAW Propagation in Graphene Film by Scanning Electron Microscopy Method

Usually, to study the operation of acoustoelectronic devices (in our case the SAW delay time line), the amplitude-frequency characteristics are measured, which compare the electrical signals at the input and output interdigital transducers. Figure 3 shows the amplitude-frequency response S21 (acoustic wave transmission coefficient from input IDT to output IDT) of the SAW delay time line. The figure clearly shows that the resonance excitation frequency of the SAW is f 0 = 114.5 MHz, and the dependence of the amplitude-frequency response itself has the form of a sin x / x function. Unfortunately, the amplitude-frequency response does not provide information about the real SAW propagation on the surface of the piezoelectric substrate.
To study the process of the SAW propagation on the surface of a piezoelectric substrate with graphene, a scanning electron microscopy method was used to visualize the SAW in real time [28,29,30]. The process of the SAW propagation in the SAW delay time line was investigated using a JEOL JSM840 SEM at an electron probe current of 1 nA and an accelerating voltage of 1 kV. The use of higher accelerating voltages of electrons leads to the formation of negative charges on the surface of the piezoelectric substrate and distortion of the formed image. The SAW image is formed in the mode of recording of low-energy secondary electrons with energy of ~1 eV, which are sensitive to the piezoelectric potential that accompanies the SAW propagation on the surface of the piezoelectric substrate.
Figure 4 shows the SEM microphotographs of SAW propagation in the SAW delay time line, the surface of which in the central part is covered by a film of single-layer graphene. Figure 4a shows the SEM microphotograph of the traveling SAW excited by the input IDT at the resonant excitation frequency of f 0 = 114.5 MHz. In an acoustic beam at the output of the IDT, the Fresnel diffraction pattern can be observed that is associated with the SAW diffraction at the IDT aperture (analogous to the diffraction of optical radiation on a slit). The structure of the acoustic wave field of SAW in the graphene film is observed much weaker compared to the free surface of the crystal. Figure 4b shows a SAW image in the graphene film and at the output from the graphene film. The decrease of the SAW contrast in the graphene film is due to the fact that the graphene film has a small conductivity and acts as an equipotential surface, which screens the piezoelectric potential of the traveling SAW in the crystal. Since the resistance of the graphene film is several kΩ, the SAW image can be observed on the surface of the graphene film.

4. Investigation of Acoustically Stimulated Charge Transport in Graphene Film

To study the process of charge transport in the graphene film by the surface acoustic wave, the scheme shown in Figure 1 was applied. Two central Au electrodes were used to measure the current in the graphene film under the conditions of the SAW propagation. The two outermost Au electrodes were used to apply a bias voltage U to the graphene film. The bias voltage was varied in the range of U = − 80   to   80 mV. The studies were carried out in the frequency range of f = 95   to   135 MHz, which corresponds to the frequency range of the amplitude-frequency response in Figure 3.
Figure 5 shows the dependences of the current in the graphene film as a function of the amplitude of the input signal on the IDT. The amplitude of the input signal on the IDT was varied from 0 to 20 V. The current in the graphene film was measured in the frequency range of f = 95 ÷ 135 MHz. The structure of the frequency dependence of the current in the graphene film is similar to the structure of the amplitude-frequency response and has the form of a sin x / x function. Small oscillations on the current-frequency dependences (Figure 5) and on the amplitude-frequency response of the SAW delay time line (Figure 3) are determined by the electrode’s structure of the interdigital transducer (number of electrodes pairs). The dependences of the current on frequency clearly show that with an increase in the SAW amplitude, the current in the graphene film increases. At a negative bias U = − 80 mV (Figure 5a) in the graphene film, a current is already observed between two gold electrodes in the absence of the SAW propagation, and SAW excitation leads to an increase in the current between the electrodes. At zero bias U = 0 mV (Figure 5b) the current in the graphene film is zero and begins to increase with increasing amplitude of the input signal on the IDT. With a positive bias U = 80 mV (Figure 5c) in the absence of SAW, the current between the electrodes has the opposite direction with respect to the current in Figure 5a. In this case, SAW propagation leads to a decrease in current; at certain amplitudes of the input signal at the IDT, the current becomes equal to zero, since the charge transport due to the positive bias U = 80 mV is compensated by the charge transport by the surface acoustic wave in the opposite direction. A further increase in the amplitude of the SAW, by increasing the amplitude of the input signal on the IDT, leads to an increase in current in the opposite direction with respect to the initial current direction. That is, in this case, with a positive bias U = 80 mV at the SAW resonance excitation frequency of f 0 = 114.5 MHz the SAW propagation in the Y Z − cut of a LiNbO3 crystal allows to change the direction of charge transport in the graphene film. In Figure 5a,b at a negative and zero bias potential, the current has a constant direction in the frequency range of f = 95 ÷ 135 MHz, while at a positive bias potential U = 80 mV (Figure 5c), the current direction in the graphene film depends on the SAW excitation frequency and the SAW amplitude. Therefore, in this case, by varying the SAW excitation frequency within the amplitude-frequency response, it is possible to change the direction of the current in the graphene film.
Figure 6 shows the dependences of the current in the graphene film on the amplitude of the input signal at the IDT (dB), measured at the bias potentials U = − 80 ,   0 ,   80 mV and the SAW resonance excitation frequency of f 0 = 114.5 . The dependence of the current in the graphene film on the amplitude of the input signal at the IDT in dB has a linear character. At a bias potential of U = 80 mV and in the absence of SAW propagation, the current in the graphene film is I = 100 nA. Excitation of the SAW leads to the beginning of the charge transport process in the graphene film in the opposite direction. When the input signal amplitude at the IDT is 7 dB, the charge transport process is compensated and the current in the graphene film becomes equal to zero. A further increase in the SAW amplitude by increasing the amplitude of the high-frequency input signal at the IDT leads to an increase in current in the opposite direction. At the amplitude of the input signal at the IDT 100 dB, the current in the graphene film is I = − 1470 nA. Thus, it has been demonstrated that the SAW allows the charge transport in the graphene film, and this process depends on the amplitude of the SAW on the surface of the substrate. An increase in the SAW amplitude leads to an increase in the current in the graphene film.
Hence, it is possible to use the surface acoustic waves to control the direction and magnitude of the current in a graphene film by changing the SAW amplitude or changing the SAW excitation frequency.

5. Transport of Photo-Stimulated Charges in a Graphene Film by Surface Acoustic Waves

Acoustically stimulated charge transport is of interest for the development of solar cells, where using of the surface acoustic waves allows collecting charges from large surfaces [11,12,13,14]. Figure 7 shows a diagram of a simulated experiment to study the transport of photo-stimulated charges by the surface acoustic wave. A laser with a wavelength of 532 nm and a power of 5 mW was used as a light source. The size of the laser beam spot on the surface of the Y Z − cut of a LiNbO3 crystal covered by the graphene film was 1 mm in diameter, which is less than the aperture of the IDT W = 1500 μm.
Charge carriers are generated under the influence of laser radiation in the near-surface area of the LiNbO3 crystal. The use of graphene as a conductive medium makes it possible to move the photo-stimulated charges by surface acoustic wave.
The bias potential of U = − 80 mV was used for the investigation of the transport of photo-stimulated charges. The SAW excitation frequency was f 0 = 114.5 MHz at an input high-frequency signal power of 100 dB. Illumination of the crystal surface by the laser radiation allows increasing the value of current I in the graphene film between the two central gold electrodes (Figure 1 and Figure 7).
Figure 8 shows the dependences of the current in the graphene film under the on/off switching of illumination of the Y Z − cut of a LiNbO3 crystal surface in the absence and under the excitation of the surface acoustic waves. In the absence of the surface acoustic waves, the current in the graphene film at the bias potential of U = − 80 mV was I = − 100 nA. Illumination of the Y Z − cut of a LiNbO3 crystal with a graphene film leads to an increase in the current in the graphene film to I = − 170 nA. The propagation of surface acoustic waves in the LiNbO3 crystal leads to a significant increase in the current in the graphene film. Thus, in the absence of illumination, the current value in the graphene film is I = − 1800 nA. Illumination of the crystal surface leads to a significant increase in the current in the graphene film up to I = − 2850 nA. Figure 8 shows the current modulation under conditions of on/off switching of illumination of the crystal surface by the laser radiation source. Thus, the acquisition and transport of charge carriers in the graphene film by the surface acoustic wave was demonstrated.
In the future, this approach allows increasing efficiency of the solar cells by increasing the collection of charge carriers with the use of surface acoustic waves.

6. Conclusions

The process of acoustically stimulated charge transport in the graphene film on the surface of the Y Z − cut of a LiNbO3 crystal was investigated. It is shown that the frequency dependence of the current in the graphene film repeats the amplitude-frequency response of the SAW delay time line. It is demonstrated that the increase of the SAW amplitude (the increase of the input signal amplitude on the IDT) leads to an increase in the current in the graphene film. The dependence of the current in the graphene film depends linearly on the amplitude of the input signal on the IDT in dB.
At a positive bias potential U = 80 mV on the graphene film, the propagation of the SAW can change the direction of the current in the graphene film due to a change in the SAW amplitude. At the certain amplitude of the SAW (the amplitude of the input signal on the IDT is 3.5 dB), the current in the graphene film becomes equal to zero. It should also be noted that in the frequency range of the amplitude-frequency response, the current in the graphene film can vary from positive to negative values depending on the frequency. Thus, the possibility of controlling the value and direction of the current in the graphene film by changing the frequency of the SAW excitation or changing the amplitude of the SAW has been demonstrated.
The possibility of the transport of the photo-stimulated charges by the surface acoustic wave, i.e., the charges generated by the optical radiation in the ferroelectric substrate of the Y Z − cut of a LiNbO3 crystal, has been demonstrated. The SAW propagation allows the collecting of the photo-stimulated charges and transferring them in the graphene film on the substrate surface. This method of charge collection and transfer will significantly improve the efficiency of solar cells in the future.

Author Contributions

Conceptualization, D.R. and O.K.; SAW design, A.S.; fabrication of graphene film, E.E.; investigations, D.R., O.K., R.F.; writing—original draft preparation, D.R. and O.K. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by Ministry of Science and Higher Education of the Russian Federation (grant number 075-15-2020-791).

Data Availability Statement

All relevant data presented in the article are stored according to institutional requirements and as such are not available online. However, all data used in this manuscript can be made available upon request to the authors.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Campbell, C. Surface Acoustic Wave Devices and Their Signal Processing Applications; Academic Press: San Diego, CA, USA, 1989; pp. 1–470. [Google Scholar]
  2. Priya, R.B.; Venkatesan, T.; Pandiyarajan, G.; Pandya, H.M. A short review of SAW sensors. J. Environ. Nanotechnol. 2015, 4, 15–22. [Google Scholar]
  3. Liu, J.; Wang, W.; Li, S.; Liu, M.; He, S. Advances in SAW Gas Sensors Based on the Condensate-Adsorption Effect. Sensors 2011, 11, 11871–11884. [Google Scholar] [CrossRef]
  4. Wingqvist, G.; Yantchev, V.; Katardjiev, I. Mass sensitivity of multilayer thin film resonant BAW sensors. Sens. Actuators A 2008, 148, 88–95. [Google Scholar] [CrossRef]
  5. Leong, A.; Seeneevassen, S.; Saha, T.; Swamy, V.; Ramakrishnan, N. Low hysteresis relative humidity sensing characteristics of graphene oxide–gold nanocomposite coated langasite crystal microbalance, Surf. Interfaces 2021, 23, 100964. [Google Scholar]
  6. Sahaa, T.; Guo, N.; Ramakrishnan, N. A novel langasite crystal microbalance instrumentation for UV sensing application. Sens. Actuators A 2016, 252, 16–25. [Google Scholar] [CrossRef]
  7. Chen, C.; Jin, J. Surface Acoustic Wave Vapor Sensor with Graphene Interdigital Transducer for TNT Detection. Sens. Imaging 2020, 21, 24. [Google Scholar] [CrossRef]
  8. Varghesea, S.S.; Lonkar, S.; Singh, K.K.; Swaminathan, S.; Abdala, A. Recent advances in graphene based gas sensors. Sens. Actuators B 2015, 218, 160–183. [Google Scholar] [CrossRef]
  9. Lupana, O.; Ursaki, V.V.; Chai, G.; Chowa, L.; Emelchenkoe, G.A.; Tiginyanug, I.M.; Gruzintsev, A.N.; Redkin, A.N. Selective hydrogen gas nanosensor using individual ZnO nanowire with fast response at room temperature. Sens. Actuators B 2010, 144, 56–66. [Google Scholar] [CrossRef]
  10. Roshchupkin, D.; Redkin, A.; Emelin, E.; Sakharov, S. Ultraviolet Radiation Sensor Based on ZnO Nanorods/La3Ga5SiO14 Microbalance. Sensors 2021, 21, 4170. [Google Scholar] [CrossRef]
  11. Rocke, C.; Zimmermann, S.; Wixforth, A.; Kptthaus, J.P.; Böhm, G.; Weimann, G. Acoustically Driven Storage of Light in a Quantum Well. Phys. Rev. Lett. 1997, 78, 4099. [Google Scholar] [CrossRef] [Green Version]
  12. Batista, P.D.; Hey, R.; Santos, P.V. Efficient electrical detection of ambipolar acoustic transport in GaAs. Appl. Phys. Lett. 2008, 92, 262108. [Google Scholar] [CrossRef]
  13. Jiao, S.J.; Batista, P.D.; Biermann, K.; Hey, R.; Santos, P.V. Electrical detection of ambipolar acoustic carrier transport by surface acoustic waves. J. Appl. Phys. 2009, 106, 053708. [Google Scholar] [CrossRef]
  14. Yakovenko, V.M. Novel method for photovoltaic energy conversion using surface acoustic waves in piezoelectric semiconductors. Phys. B 2012, 407, 1969–1972. [Google Scholar]
  15. Novoselov, K.S.; Geim, A.K.; Morozov, S.V.; Jiang, D.; Katsnelson, M.I.; Grigorieva, I.V.; Dubonos, S.V.; Firsov, A.A. Two-dimensional gas of massless Dirac fermions in graphene. Nature 2005, 438, 197. [Google Scholar] [CrossRef] [Green Version]
  16. Katsnelson, M.I.; Novoselov, K.S. Graphene: New Bridge between Condensed Matter Physics and Quantum Electrodynamics. Solid State Commun. 2007, 143, 3–13. [Google Scholar] [CrossRef] [Green Version]
  17. Miseikis, V.; Cunningham, J.E.; Saeed, K.; O’Rorke, R.; Davies, A.G. Acoustically induced current flow in graphene. Appl. Phys. Lett. 2012, 100, 133105. [Google Scholar] [CrossRef]
  18. Poole, T.; Nash, G.R. Acoustoelectric Current in Graphene Nanoribbons. Sci. Rep. 2017, 7, 1767. [Google Scholar] [CrossRef] [Green Version]
  19. Santos, P.V.; Schumann, T.; Oliveira Jr., M.H.; Lopes, J.M.J.; Riechert, H. Acousto-electric transport in epitaxial monolayer graphene on SiC. Appl. Phys. Lett. 2013, 102, 221907. [Google Scholar] [CrossRef] [Green Version]
  20. Insepov, Z.; Emelin, E.; Kononenko, O.; Roshchupkin, D.V.; Tnyshtykbayev, K.B.; Baigarin, K.A. Surface acoustic wave amplification by direct current-voltage supplied to graphene film. Appl. Phys. Lett. 2015, 106, 023505. [Google Scholar] [CrossRef] [Green Version]
  21. Mayorov, A.S.; Hunter, N.; Muchenje, W.; Wood, C.D.; Rosamond, M.; Linfield, E.H.; Davies, A.G.; Cunningham, J.E. Surface acoustic wave generation and detection using graphene interdigitated transducers on lithium niobate. Appl. Phys. Lett. 2014, 104, 083509. [Google Scholar] [CrossRef]
  22. Roshchupkin, D.; Ortega, L.; Zizak, I.; Plotitcyna, O.; Matveev, V.; Kononenko, O.; Emelin, E.; Erko, A.; Tynyshtykbayev, K.; Irzhak, D.; et al. Surface acoustic wave propagation in graphene film. J. Appl. Phys. 2015, 118, 104901. [Google Scholar] [CrossRef]
  23. Emelin, E.; Cho, H.D.; Insepov, Z.; Lee, J.C.; Kang, T.W.; Panin, G.; Roshchupkin, D.; Tynyshtykbayev, K. SEM imaging of acoustically stimulated charge transport in solids. Appl. Phys. Lett. 2017, 110, 264103. [Google Scholar] [CrossRef]
  24. Poole, T.; Nash, G.R. Acoustoelectric photoresponse of graphene nanoribbons. J. Phys. D Appl. Phys. 2018, 51, 154001. [Google Scholar] [CrossRef]
  25. Kononenko, O.V.; Emelin, E.V.; Matveev, V.N.; Roshchupkin, D.V. Photoresponse in Multilayer Graphene during the Passage of a Surface Acoustic Wave. Tech. Phys. Lett. 2020, 46, 220–223. [Google Scholar] [CrossRef]
  26. Ferrari, A.C.; Basko, D.M. Raman spectroscopy as a versatile tool for studying the properties of graphene. Nat. Nanotechnol. 2013, 8, 235–246. [Google Scholar] [CrossRef] [Green Version]
  27. Ferrari, A.C.; Meyer, J.C.; Scardaci, V.; Casiraghi, C.; Lazzeri, M.; Mauri, F.; Piscanec, S.; Jiang, D.; Novoselov, K.S.; Roth, S.; et al. Raman spectrum of graphene and graphene layers. Phys. Rev. Lett. 2006, 97, 187401. [Google Scholar] [CrossRef] [Green Version]
  28. Eberharter, G.; Feuerbaum, H.P. Scanning-elctron-microscope observations of propagating acoustic waves in surface acoustic wave devices. Appl. Phys. Lett. 1980, 37, 698. [Google Scholar] [CrossRef]
  29. Roshchupkin, D.V.; Brunel, M. Scanning electron microscopy observation of surface acoustic wave propagation in the LiNbO3 crystals with regular domain structures. IEEE Trans. Ultrason. Ferroelectr. Freq. Control 1994, 41, 512–517. [Google Scholar] [CrossRef]
  30. Roshchupkin, D.; Emelin, E.; Plotitcina, O.; Mololkin, A.; Telminov, O. Scanning Electron Microscopy Investigation of Surface Acoustic Wave Propagation in a 41° YX-Cut of a LiNbO3 Crystal/Si Layered Structure. Crystals 2021, 11, 1082. [Google Scholar] [CrossRef]
Nanomaterials 12 04370 g001 550
Figure 1. Optical image of the SAW delay time line with graphene.
Figure 1. Optical image of the SAW delay time line with graphene.
Nanomaterials 12 04370 g001
Nanomaterials 12 04370 g002 550
Figure 2. The representative Raman spectra of the graphene film transferred to the LiNbO3 substrate. Insert: zoomed-in spectrum showing graphene Raman peaks.
Figure 2. The representative Raman spectra of the graphene film transferred to the LiNbO3 substrate. Insert: zoomed-in spectrum showing graphene Raman peaks.
Nanomaterials 12 04370 g002
Nanomaterials 12 04370 g003 550
Figure 3. Electrical characterization S21 of the SAW delay time line.
Figure 3. Electrical characterization S21 of the SAW delay time line.
Nanomaterials 12 04370 g003
Nanomaterials 12 04370 g004 550
Figure 4. SAW propagation in the Y Z − cut of a LiNbO3 crystal covered by graphene film: (a) SAW excitation by interdigital transducer, (b) SAW propagation in the graphene film and on the free crystal surface. Λ = 30 µm, f 0 = 114.5 MHz, V = 3435 m/s.
Figure 4. SAW propagation in the Y Z − cut of a LiNbO3 crystal covered by graphene film: (a) SAW excitation by interdigital transducer, (b) SAW propagation in the graphene film and on the free crystal surface. Λ = 30 µm, f 0 = 114.5 MHz, V = 3435 m/s.
Nanomaterials 12 04370 g004
Nanomaterials 12 04370 g005 550
Figure 5. Dependences of the current in the graphene film on the bias potential U and the amplitude of the input signal supplied to the IDT (1÷100 dB): (a) U = − 80 mV, (b) U = 0 mV, (c) U = − 80 mV.
Figure 5. Dependences of the current in the graphene film on the bias potential U and the amplitude of the input signal supplied to the IDT (1÷100 dB): (a) U = − 80 mV, (b) U = 0 mV, (c) U = − 80 mV.
Nanomaterials 12 04370 g005
Nanomaterials 12 04370 g006 550
Figure 6. Dependences of current in graphene film versus amplitude of the input signal supplied to IDT (in dB). Y Z − cut of a LiNbO3 crystal, Λ = 30 µm, f 0 = 114.5 MHz, V = 3420 m/s.
Figure 6. Dependences of current in graphene film versus amplitude of the input signal supplied to IDT (in dB). Y Z − cut of a LiNbO3 crystal, Λ = 30 µm, f 0 = 114.5 MHz, V = 3420 m/s.
Nanomaterials 12 04370 g006
Nanomaterials 12 04370 g007 550
Figure 7. Scheme of a photo-stimulated charge transport in a graphene film by a surface acoustic wave.
Figure 7. Scheme of a photo-stimulated charge transport in a graphene film by a surface acoustic wave.
Nanomaterials 12 04370 g007
Nanomaterials 12 04370 g008 550
Figure 8. Dependences of acoustically stimulated photocurrent in graphene film on the on/off switching of the surface acoustic wave.
Figure 8. Dependences of acoustically stimulated photocurrent in graphene film on the on/off switching of the surface acoustic wave.
Nanomaterials 12 04370 g008
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Roshchupkin, D.; Kononenko, O.; Fakhrtdinov, R.; Emelin, E.; Sergeev, A. Acoustically Stimulated Charge Transport in Graphene Film. Nanomaterials 2022, 12, 4370. https://doi.org/10.3390/nano12244370

AMA Style

Roshchupkin D, Kononenko O, Fakhrtdinov R, Emelin E, Sergeev A. Acoustically Stimulated Charge Transport in Graphene Film. Nanomaterials. 2022; 12(24):4370. https://doi.org/10.3390/nano12244370

Chicago/Turabian Style

Roshchupkin, Dmitry, Oleg Kononenko, Rashid Fakhrtdinov, Evgenii Emelin, and Alexander Sergeev. 2022. "Acoustically Stimulated Charge Transport in Graphene Film" Nanomaterials 12, no. 24: 4370. https://doi.org/10.3390/nano12244370

APA Style

Roshchupkin, D., Kononenko, O., Fakhrtdinov, R., Emelin, E., & Sergeev, A. (2022). Acoustically Stimulated Charge Transport in Graphene Film. Nanomaterials, 12(24), 4370. https://doi.org/10.3390/nano12244370

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop