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Strain Effect on Thermoelectric Performance of InSe Monolayer
Nanoscale Research Letters volume 14, Article number: 287 (2019)
Abstract
Strain engineering is a practical method to tune and improve the physical characteristics and properties of twodimensional materials, due to their large stretchability. Tensile strain dependence of electronic, phonon, and thermoelectric properties of InSe monolayer are systematically studied. We demonstrate that the lattice thermal conductivity can be effectively modulated by applying tensile strain. Tensile strain can enhance anharmonic phonon scattering, giving rise to the enhanced phonon scattering rate, reduced phonon group velocity and heat capacity, and therefore lattice thermal conductivity decreases from 25.9 to 13.1 W/mK when the strain of 6% is applied. The enhanced figure of merit indicates that tensile strain is an effective way to improve the thermoelectric performance of InSe monolayer.
Introduction
Twodimensional (2D) semiconductor materials have been drawing the attention of researcher to explore their fascinating properties and useful application since the discovery of graphene. Especially, the family of twodimensional metalchalcogenide has been found to show great potential in nanoelectronics and nanophotonics due to their extraordinary electronic, optical, and mechanical properties [1,2,3,4]. Recently, indium selenide (InSe), a IIIVI group layered metalchalcogenide compound, is of great interest both experimentally and theoretically. The atomic layer of InSe has been reported to successfully synthesized via physical [5,6,7,8,9,10] and chemical methods [11,12,13,14], and the applications of InSe nanosheet on sensors [15], optoelectronics, and photodetectors have been explored. Srinivasa et al. reported the fabrication of fewlayer InSe photodetectors with high responsivity and a broad spectral detection from the visible to nearinfrared region [6]. Bandurin et al. found a highquality twodimensional electron gas in fewlayer InSe with the carrier mobilities of 10^{3} and 10^{4} cm^{2}/Vs at room and liquidhelium temperatures [16]. Wei et al. discovered backgated multilayer InSe FETs exhibit ultrahigh carrier mobility up to 1055 cm^{2}/Vs at room temperatures due to suppressed carrier scattering from the dielectric substrate [5].
2D InSe has a rather unusual band structure, which is the combination of a flat band at the top of the valence band and parabolic band at the bottom of the conduction band, thus exhibiting high thermoelectric characteristics [17]. Particularly, thermoelectric performance can be described by the nondimensionalized figure of merit, ZT, defined as ZT = S^{2}Tσ/(Κ_{e} + Κ_{l}), where S is the Seebeck efficient, T is the absolute temperature, σ is the electrical conductivity, and Κ_{e} and the Κ_{l} are the thermal conductivity with the contributions from electronic carriers and lattice, respectively. The lattice thermal conductivity K_{l} relevant to phonon transport property plays an important role to determine the thermoelectric performance. The previous reported K_{l} of InSe monolayer is much lower than that of graphene, while it was 10 times as much as that of SnSe sheet [18, 19].
The high level of electron mobility and low thermal conductivity is beneficial to the thermoelectric performance. Besides, monolayer InSe exhibits superior mechanical flexibility, and the electronic properties can be continuously modulated by moderate strain in a wide range [20,21,22]. It has been demonstrated that the thermoelectric power factor of monolayer InSe can be significantly enhanced through band convergence under a compressive strain [23]. For thermoelectric materials, tensile strain can also induce a variation of band structure and thermal transport properties. However, the dependence of thermal transport properties on the strain is unpredictable, closely related to the particular material and crystal structure. In this paper, the present work is performed on the biaxial tensile strain effect for the thermoelectric performance of InSe monolayer by firstprinciples calculations, including electronic and phonon transport properties. Due to the increased anharmonic scattering, the positive effect of tensile strain on the thermoelectric performance of InSe monolayer is determined.
Methodology
The calculation of the structural and electronic properties for InSe monolayer are performed based on density functional theory (DFT) as implemented in the Vienna ab initio simulation package (VASP) [24,25,26]. We chose the projectoraugmented wave method with the local density approximation (LDA) [27,28,29] for the exchangecorrelation functional. And 12 Å vacuum along the zaxis is used to avoid the interaction between periodic images of slabs. The 21 × 21 × 1 and 31 × 31 × 1 MonkhorstPack kmeshes were used during structural relaxation and electronic structure calculations for the unit cell. The energy cutoff of the plane wave basis was set to be 500 eV. The convergence criterion for a total energy was set as 10^{−4} eV, and all the atomic positions and lattice structures were fully relaxed with a force tolerance of 10^{−3} eV/Å.
The thermoelectric transport properties can be obtained within the constant relaxation time approximation by the Boltzmann theory as implemented in BoltzTraP program [30, 31]. Within this approximation, the electronic transport coefficients can be given by
where Ω is the volume of the unit cell, f_{μ} is the FermiDirac distribution function, and α and β are tensor indices. The transport distribution function ∑_{αβ}(ε) is given by
where N_{0} indicates the number of q points sampled, i is the band index, v is the group velocity of carriers, and τ is the relaxation time.
The ShengBTE package [32] is employed to solve the phonon Boltzmann transport equation and determine the lattice thermal and other relevant parameters. A 5 × 5 × 1 supercell is used to calculate the harmonic interatomic force constants by using densityfunctional perturbation theory (DFPT) calculation [33]. And the finitedifference method is used to calculate anharmonic interatomic force constants with a 4 × 4 × 1 supercell [34]. Phonon spectrum was calculated by using the Phonopy program [35].
Result and Discussion
Monolayer InSe is a quadruple atomic sheet with SeInInSe covalently bonding in one layer. From a top view, the monolayer exhibits a honeycomb lattice, and every Se atom is bonded with other three In atoms, as shown in Fig. 1a. On the basis of the minimization of the total energy, the lattice parameters of this crystal are calculated to be a_{0} = 3.95 Å. In this paper, we employ the biaxial strain on monolayer InSe maintaining the crystal symmetry by changing its lattices as δ = (a−a_{0})/a_{0} × 100%, where a and a_{0} are the lattice constant of monolayer InSe with strain and without strain, respectively. When the biaxial tensile strain is imposed on the monolayer InSe, the bond length d_{InSe} monotonically increase with the increase of strain, and this lead to the increasing bond angle of InSeIn (see Fig. 1b).
InSe monolayer exhibits an indirect semiconductor with the bandgap of 1.67 eV, where the conduction band minimum (CBM) exists on the Г point, and valence band maximum (VBM) sites on between Г and K point, as shown in Fig. 2a. The valence band of InSe monolayer exhibits a Mexican hat dispersion, which can be also found in many twodimensional materials [36,37,38,39]. The band structure modification in response to tensile strain was investigated in Fig. 2, and the three conduction band extrema are denoted by the symbols I, II, and III respectively. Under a tensile strain, the lowestenergy conduction band is sensitive to strain and shifts downwards, while valence band almost remain constant, giving rise to the reduction of the bandgap. Without strain, there are minute differences between the second and third conduction band minimum, and the band valleys are tending to convergence. However, with the increase of tensile strain, the energy difference gradually increases. We also compared the bandgaps under different strains with related theoretical and experimental results as detailed in Additional file 1: Table S2.
Effect of Tensile Strain on Thermoelectric Transport Coefficients
On the basis of the calculated electronic structure, we perform thermoelectric transport coefficient calculations by the semiclassical Boltzmann theory. With respect to scattering time τ, Seebeck coefficient S, and electrical conductivity σ can be calculated. Figure 3a shows the calculated Seebeck coefficient as a function of the Fermi level. For simplicity, the band structure is often assumed to remain unchanged from doping at finite temperatures [40, 41], and doping effect on thermoelectric transport coefficient can be obtained by the variation of the position of Fermi level. A negative ε_{f} indicates ptype doping by moving the Fermi level into the valence band, and the positive Seebeck coefficient can be obtained. Similarly, a positive ε_{f} gave a negative Seebeck coefficient. We can find the obtained result without strain is very close to the previous report [17], and the maximum of Seebeck coefficient decreases with increasing tensile strain, which is related to the change of the bandgap [42].
To calculate the electrical conductivity σ, relaxation time τ is required because the output is σ/τ in BoltzTraP code. Herein, τ is determined by
where μ is carrier mobility and m* is the effective mass. In the deformation potential theory, the carrier mobility in 2D materials can be calculated by [43, 44]
Here, e is the electron charge, ℏ is the Planck constant, and k_{B} is Boltzmann constant. C represents the elastic modulus and can be calculated by C = (∂^{2}E/∂δ^{2})/S_{0}, where E, δ, and S_{0} are the total energy, the applied strain, and the area at equilibrium for the 2D system, respectively. E_{1} is deformation potential constant shown as E_{1} = ΔE_{edge}/Δδ, where ΔE_{edge} is the energy change of band edges. m_{d} is average effective mass derived from \( {m}_d=\sqrt{m_x^{\ast }{m}_y^{\ast }} \). In order to calculate the mobility, a rectangular x × y supercell is adopted as shown in Fig. 1a. The obtained value of C along x (y) direction is 60.43 N/m (53.68 N/m), which is obtained by fitting the curve of energystrain relationship, as shown in Additional file 1: Figure S1. The calculated deformation potential E_{1} is 6.13 eV (6.14 eV) for electron along x (y) direction, and 3.45 eV (3.33 eV) for hole along x (y) direction. The calculated results of effective mass, carrier mobility, and relaxation time for monolayer InSe under different strain are summarized in Table 1. We can find that little difference along with different directions, and the carrier effective mass and mobility is general isotropic. Therefore, we use the average value of x and y directions to evaluate the thermoelectric performance later. The hole effective masses are enhanced by the applied strain while the effective masses for electron remains almost unchanged. With the calculated relaxation time, the electrical conductivity can be obtained at a given chemical potential in Fig. 3b. It can be seen that electrical conductivity σ increase with increasing the tensile strain in a heavy ptype doped system due to the enhancement of hole mobility, whereas σ remains relatively low at low doping level. Moreover, the trend of electronic thermal conductivity keeps with the electrical conductivity through the WiedemannFranz law: K_{e} = LσT in Fig. 3c, where L is the Lorenz number. Power factor can be obtained by PF = S^{2}σ /τ, which determines how much electricity can be generated. Considering the comprehensive trend of Seebeck coefficient and electrical conductivity, tensile strain slightly reduces the power factor, as observed in Fig. 3d.
Effect of Tensile Strain on Κ _{l}
In metals, electrons are responsible for heat carriers, while in semiconductors and dielectric solids where the doping and temperature are not very high, lattice vibrations will be the main reason for energy transport [45]. Lattice thermal conductivity is a very important parameter for thermoelectric application. From the theoretical point of view and as a simple approximation, the lattice thermal conductivity Κ_{l} can be expressed as follows [46,47,48]:
where C_{λ}, v_{λ}, and V are specific heat contribution, phonon group velocity, and crystal volume, respectively. τ_{λ} is the relaxation time of mode λ, which can be estimated using the Matthiessen rule [49]:
where \( \frac{1}{\tau_{\uplambda}^b} \)is the boundary scattering rate, \( \frac{1}{\tau_{\uplambda}^{\mathrm{iso}}} \)is the isotropic impurity scattering rate, and \( \kern0.1em \frac{1}{\tau_{\uplambda}^{3\mathrm{ph}}} \) is the threephonon scattering rate.
Figure 4a presents Κ_{l} variation of monolayer InSe with temperature under different strain. The lattice thermal conductivity in the strainfree case is 25.9 W/mK at room temperature, which is comparable with the previous report [19]. When the applied strain is increased to 6%, the lattice thermal conductivity decreased to 13.1 W/mK, which confirms that strain engineering is a very efficient method to modify the lattice thermal conductivity. We plot the corresponding phonon dispersion curve of InSe monolayer for different strains in Fig. 4c, to determine the origin of the reduction on lattice thermal conductivity. It contains 12 phonon modes as monolayer InSe has a fouratom unit cell. There is no negative frequency in phonon spectra, confirming that InSe monolayer is thermally stable. Three branches starting from 0 in the low energy region of the phonon dispersion curve are zaxis acoustic (ZA), longitudinal acoustic (LA), and transverse acoustic (TA), respectively, and the others are optical modes. With the increase of tensile strain, the quadratic nature of the ZA mode changes into almost a straight line in the lowenergy region. The downward trend in the frequency of optical modes can be observed under tensile strain, because tensile strain weakens the bonds and then leads to lower frequencies. We also discuss the contribution of each phonon branch towards Κ_{l} for the unstrained and 6% strain monolayer InSe in Fig. 4b. For the strainfree condition, the ZA mode contributes significantly to carrying heat, and when 6% tensile strain is applied to monolayer InSe, the relative contribution of ZA mode is decreased from 58 to 38%. As the tensile strain increases, ZA mode becomes harder, leading to a decreased contribution to Κ_{l}.
Next, a detailed analysis of phonon group velocity variation induced by tensile strain is presented to understand the phonon transport properties. For inplane acoustic modes, phonon group velocities are decreased at the strain of 6%, as shown in Fig. 5a, b. Combined with the enhanced contribution of LA and TA, decreased phonon group velocity plays a vital role in the reduction of Κ_{l}. The change of phonon group velocities originates from straininduced structure variation: when tensile strain is turned on, the bond distance increase and bonding strength decrease, leading to the lower phonon frequency and group velocity. Considering that three acoustic phonon branches contribute mostly to Κ_{l}, the increased phonon group velocities of optical branches have limited effect.
The threephonon scattering rate of monolayer InSe without and with 6% strain as a function of frequency is depicted in Fig. 5d. It can be observed that threephonon scattering rate of 6% strained monolayer InSe in the lower frequency region is significantly larger than that of the unstrained case, which indicates that the increase of strain gives rise to stronger threephonon scattering. The enhanced threephonon scattering is mostly responsible for the reduced lattice thermal conductivity, which is also consistent with previous conclusion [19]. A similar trend of phonon scattering rate with the increased tensile strain has been observed in ZrS_{2} and 2H MoTe_{2} monolayer [50, 51]. We also analyzed the effect of biaxial tensile strain on phonon heat capacity (C_{ph}), as presented in Fig. 5c. With the increase of tensile strain, the phonon heat capacity of InSe monolayer is monotonously decreased. For the 6% strained system, the phonon heat capacity is reduced to 6.2 × 10^{5} J/Km^{3}. Because of the linearization and stiffening of the ZA mode, the phonon density of states is decreased, leading to the reduced phonon heat capacity. The Gruneisen parameters provide information about the anharmonicity of a system and can be obtained from the anharmonic interatomic force constants (IFCs) [32, 52]. Figure 5c displays the calculated Gruneisen parameters under different strains. The increased Gruneisen parameter induced by the tensile strain means stronger anharmonicity, leading to lower thermal conductivity [18].
With all the thermoelectric transport properties available, the figure of merit, ZT, can be obtained. The applied tensile strain has a different effect on these transport properties, and the improvement of the thermoelectric performance of InSe monolayer necessitates a complicated balance between these parameters S, σ, and κ. Figure 6 displays the calculated figure of merit with different strain as a function of chemical potential at 300 K, and it is obvious that the variation of ZT value under different strains strongly depends on the chemical potential and ZT maximum value can be effectively enhanced with the increase of strain. Without strain, the InSe monolayer has a peak ZT value of 0.36 at room temperature, which is close to that of silicene (0.36), germanene (0.41), and singlelayer MoS_{2} (0.58) [53, 54], and lower than that of 2D monochalcogenides (1.29~2.63 at 700 K) [55]. Considering the high carrier mobility and superior mechanical flexibility, strained InSe monolayer is also a promising potential material for thermoelectric application. When tensile strain is applied, the weakened interatomic bond induces stronger anharmonicity. The increased phonon scattering rate, decreased phonon group velocity and phonon heat capacity together resulted in reduced lattice thermal conductivity, leading to an enhanced figure of merit. Previous theoretical calculations demonstrated that InSe monolayer can sustain a tensile strain over 20%, which is much larger than our predicted strains [20]. In the experiment, applying a strain on 2D materials are mostly through their interaction with substrates, which can be induced from heating [56], the lattice mismatch between epitaxial thin films [57], or bending of the 2D material on substrate [58, 59]. Actually, it is experimentally more common to apply uniaxial strain instead of biaxial strain. Based on the previous reports [20], a uniaxial strain may exhibit similar improvement on the thermoelectric properties of monolayer InSe.
Conclusion
In conclusion, we systematically investigate the possible impact of biaxial tensile strain on the electronic, thermoelectric, and phonon transport properties for InSe monolayer by firstprinciples calculations. The bandgap decreases as the increase of tensile strain, leading to the reduced Seebeck coefficient. The tensile strain also induced stronger anharmonic scattering, and the reduction of lattice thermal conductivity could be attributed to the resulting increased phonon scattering rate, decreased phonon group velocity, and phonon heat capacity. The reduction of lattice thermal conductivity outweighs that of the Seebeck coefficient, thus bringing about an enhanced performance with the increase of tensile strain.
Availability of Data and Materials
The datasets generated and/or analyzed during the current study are available from the corresponding author on request.
Abbreviations
 2D:

Two dimensional
 CBM:

Conduction band minimum
 τ :

Relaxation time
 C _{ph} :

Phonon heat capacity
 FET:

Fieldeffect transistor
 LA:

Longitudinal acoustic phonon dispersion
 PF:

Power factor
 S :

Seebeck coefficient
 TA:

Transverse acoustic phonon dispersion
 VBM:

Valence band maximum
 ZA:

zaxis acoustic phonon dispersion
 ZT:

Figure of merit
 ε _{f} :

Fermi level
 Κ _{e} :

The thermal conductivity with the contributions from electronic carriers
 Κ _{l} :

The thermal conductivity with the contributions from lattice
 σ :

Electrical conductivity
References
 1.
Schwarz S et al (2014) Twodimensional metalchalcogenide films in tunable optical microcavities. Nano Letters 14(12):7003–7008
 2.
Hu Y et al (2015) GeSe monolayer semiconductor with tunable direct band gap and small carrier effective mass. Applied Physics Letters 91(12):161404–161377
 3.
Gomes LC, Carvalho A (2015) Phosphorene analogues: isoelectronic twodimensional groupIV monochalcogenides with orthorhombic structure. Physics 92
 4.
Wu L et al (2018) Stanene nanomeshes as anode materials for Naion batteries. Journal of Materials Chemistry A 6(17):7933–7941
 5.
Feng W et al (2014) Back gated multilayer InSe transistors with enhanced carrier mobilities via the suppression of carrier scattering from a dielectric interface. Advanced Materials 26(38):6587–6593
 6.
Tamalampudi SR et al (2014) High performance and bendable fewlayered InSe photodetectors with broad spectral response. Nano letters 14(5):2800–2806
 7.
Beardsley R et al (2016) Nanomechanical probing of the layer/substrate interface of an exfoliated InSe sheet on sapphire. Scientific reports 6:26970
 8.
BrotonsGisbert M et al (2016) Nanotexturing to enhance photoluminescent response of atomically thin indium selenide with highly tunable band gap. Nano letters 16(5):3221–3229
 9.
Mudd GW et al (2013) Tuning the bandgap of exfoliated InSe nanosheets by quantum confinement. Advanced Materials 25(40):5714–5718
 10.
Wu L et al (2018) Firstprinciples characterization of twodimensional (CH_{3}(CH_{2})_{3}NH_{3})_{2}(CH_{3}NH_{3})_{n−1}Ge_{n}I_{3n+1} perovskite. Journal of Materials Chemistry A 6(47):24389–24396
 11.
Lei S et al (2014) Evolution of the electronic band structure and efficient photodetection in atomic layers of InSe. ACS nano 8(2):1263–1272
 12.
Lin S et al (2019) Roomtemperature production of silvernanofiber film for largearea, transparent and flexible surface electromagnetic interference shielding. npj Flexible Electronics 3(1):6
 13.
Bi K et al (2019) Experimental demonstration of ultralargescale terahertz alldielectric metamaterials. Photonics Research 7(4):457–463
 14.
He X et al (2019) Facile loading mesoporous Co_{3}O_{4} on nitrogen doped carbon matrix as an enhanced oxygen electrode catalyst. Materials Letters
 15.
Brus V et al (2015) 2D nanocomposite photoconductive sensors fully dry drawn on regular paper. Nanotechnology 26(25):255501
 16.
Bandurin DA et al (2017) High electron mobility, quantum Hall effect and anomalous optical response in atomically thin InSe. Nature nanotechnology 12(3):223
 17.
Hung NT, Nugraha AR, Saito R (2017) Twodimensional InSe as a potential thermoelectric material. Applied Physics Letters 111(9):092107
 18.
Wang FQ et al (2015) Thermoelectric properties of singlelayered SnSe sheet. Nanoscale 7(38):15962–15970
 19.
Nissimagoudar AS et al (2017) Thermal transport in monolayer InSe. Journal of Physics: Condensed Matter 29(33):335702
 20.
Hu T, Zhou J, Dong J (2017) Strain induced new phase and indirectdirect band gap transition of monolayer InSe. Physical Chemistry Chemical Physics 19(32):21722–21728
 21.
Khoa DQ et al (2019) Modulation of electronic properties of monolayer InSe through strain and external electric field. Chemical Physics 516:213–217
 22.
Song C et al (2018) Largely tunable band structures of fewlayer InSe by uniaxial strain. ACS applied materials & interfaces 10(4):3994–4000
 23.
Nguyen TH et al (2019) Thermoelectric performance of monolayer InSe improved by convergence of multivalley bands. Journal of Applied Physics 125(8):082502
 24.
Kresse G, Furthmüller J (1996) Efficient iterative schemes for ab initio totalenergy calculations using a planewave basis set. Physical review B 54(16):11169
 25.
Wang Q et al (2019) Electronic and interface properties in graphene oxide/hydrogenpassivated Ge heterostructure. physica status solidi (RRL)Rapid Research Letters 13(2):1800461
 26.
Zhang J et al (2019) Electronic and luminescence characteristics of interstitial Bi^{0} atom in bismuthdoped silica optical fiber. Journal of Luminescence 207:346–350
 27.
Perdew JP, Zunger A (1981) Selfinteraction correction to densityfunctional approximations for manyelectron systems. Physical Review B 23(10):5048
 28.
Lin S et al (2017) Rolltoroll production of transparent silvernanofibernetwork electrodes for flexible electrochromic smart windows. Advanced Materials 29(41):1703238
 29.
Bi K et al (2019) Wideband slotcoupled dielectric resonatorbased filter. Journal of Alloys and Compounds 785:1264–1269
 30.
Madsen GK, Singh DJ (2006) BoltzTraP. A code for calculating bandstructure dependent quantities. Computer Physics Communications 175(1):67–71
 31.
Xu H et al (2018) Switchable complementary diamondringshaped metasurface for radome application. IEEE Antennas and Wireless Propagation Letters 17(12):2494–2497
 32.
Li W et al (2014) ShengBTE: A solver of the Boltzmann transport equation for phonons. Computer Physics Communications 185(6):1747–1758
 33.
Baroni S et al (2001) Phonons and related crystal properties from densityfunctional perturbation theory. Reviews of Modern Physics 73(2):515
 34.
Li W et al (2012) Thermal conductivity of bulk and nanowire Mg_{2}Si_{x}Sn_{1−x} alloys from first principles. Physical Review B 86(17):174307
 35.
Togo A, Tanaka I (2015) First principles phonon calculations in materials science. Scripta Materialia 108:1–5
 36.
Wickramaratne D, Zahid F, Lake RK (2015) Electronic and thermoelectric properties of van der Waals materials with ringshaped valence bands. Journal of Applied Physics 118(7):075101
 37.
Zahid F, Lake R (2010) Thermoelectric properties of Bi_{2}Te_{3} atomic quintuple thin films. Applied Physics Letters 97(21):212102
 38.
Saeed Y, Singh N, Schwingenschlögl U (2014) thickness and strain effects on the thermoelectric transport in nanostructured Bi_{2}Se_{3}. Applied Physics Letters 104(3):033105
 39.
Lin S et al (2019) Direct spraycoating of highly robust and transparent Ag nanowires for energy saving windows. Nano Energy 62:111–116
 40.
Scheidemantel T et al (2003) Transport coefficients from firstprinciples calculations. Physical Review B 68(12):125210
 41.
Wang Y et al (2018) Firstprinciples thermodynamic theory of Seebeck coefficients. Physical Review B 98(22):224101
 42.
Goldsmid H, Sharp J (1999) Estimation of the thermal band gap of a semiconductor from Seebeck measurements. Journal of electronic materials 28(7):869–872
 43.
Xi J et al (2012) Firstprinciples prediction of charge mobility in carbon and organic nanomaterials. Nanoscale 4(15):4348–4369
 44.
Lv H et al (2014) Enhanced thermoelectric performance of phosphorene by straininduced band convergence. Physical Review B 90(8):085433
 45.
Kim W (2015) Strategies for engineering phonon transport in thermoelectrics. Journal of Materials Chemistry C 3(40):10336–10348
 46.
Transport, M.E., CL Tien, A. Majumdar and FM Gerner. 1998, Taylor & Francis.
 47.
Chen, G., Nanoscale energy transport and conversion: a parallel treatment of electrons, molecules, phonons, and photons. 2005. Oxford University Press
 48.
Kittel C, McEuen P (1996) Introduction to solid state physics. Wiley
 49.
Srivastava GP (1990) The physics of phonons. CRC press
 50.
Lv H et al (2016) Straininduced enhancement in the thermoelectric performance of a ZrS_{2} monolayer. Journal of Materials Chemistry C 4(20):4538–4545
 51.
Shafique A, Shin YH (2017) Strain engineering of phonon thermal transport properties in monolayer 2HMoTe_{2}. Physical Chemistry Chemical Physics 19(47):32072–32078
 52.
Wang X et al (2019) Recent advances in the functional 2D photonic and optoelectronic devices. Advanced Optical Materials 7(3):1801274
 53.
Yang K et al (2014) Thermoelectric properties of atomically thin silicene and germanene nanostructures. Physical Review B 89(12):125403
 54.
Huang W, Da H, Liang G (2013) Thermoelectric performance of MX_{2} (M= Mo, W; X= S, Se) monolayers. Journal of Applied Physics 113(10):104304
 55.
Shafique A, Shin YH (2017) Thermoelectric and phonon transport properties of twodimensional IV–VI compounds. Scientific reports 7(1):506
 56.
Huang S et al (2019) Straintunable van der Waals interactions in fewlayer black phosphorus. Nature communications 10(1):2447
 57.
Gao G, Jin S, Wu W (2007) Latticemismatchstrain induced inhomogeneities in epitaxial La_{0.7}Ca_{0.3}MnO_{3} films. Applied physics letters 90(1):012509
 58.
Li Y et al (2018) Ultrasensitive tunability of the direct bandgap of 2D InSe flakes via strain engineering. 2D Materials 5(2):021002
 59.
Song C et al (2019) Drastic enhancement of the Raman intensity in fewlayer InSe by uniaxial strain. Physical Review B 99(19):195414
 60.
Ding Ym et al (2017) Enhancement of hole mobility in InSe monolayer via an InSe and black phosphorus heterostructure. Nanoscale 9(38):14682–14689
 61.
Sun Y et al (2018) InSe: a twodimensional material with strong interlayer coupling. Nanoscale 10(17):7991–7998
 62.
Errandonea D et al (2006) Highpressure electrical transport measurements on ptype GaSe and InSe. High Pressure Research 26(4):513–516
Acknowledgements
We thank the computational support from the Beijing Computational Science Research Center (CSRC). We also thank Prof. Pengfei Guan for his fruitful discussion.
Funding
This work was supported by the National Key Research and Development Program of China (no. 2017YFB0405100), the National Natural Science Foundation (61675032), and the Open Program of State Key Laboratory of Functional Materials for Informatics.
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QW and LW carried out the firstprinciples calculations and prepared the manuscript. LH, TZ, and SL discussed and analyzed the calculation results. PL supervised the manuscript. All authors read and approved the final manuscript.
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Additional file 1:
Table S2. Calculated bandgaps of InSe monolayer under different tensile strain. For sake of comparison, some previous theoretical and experimental (optical bandgap) results without strain are also listed. Figure S1. (a) The 2D elastic constant is obtained by parabola fitting total energystrain relationship along x and y directions of monolayer InSe. (b) The band edge positions of conduction band and valence band with respect to the applied strain along x and y directions. Dotted line represents the linear fit, which defines deformation potential constant (DOCX 66 kb)
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Wang, Q., Han, L., Wu, L. et al. Strain Effect on Thermoelectric Performance of InSe Monolayer. Nanoscale Res Lett 14, 287 (2019). https://doi.org/10.1186/s1167101931139
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Keywords
 Twodimensional materials
 Thermoelectric
 Strain engineering