The successful exfoliation of atomically-thin bismuth telluride (Bi2Te3) quintuple layer (QL) attracts tremendous research interest in this strongly anharmonic quasi-two-dimensional material. The thermal transport properties of this material are not well understood, especially the mode-wise properties and when it is coupled with a substrate. In this work, we have performed molecular dynamics simulations and normal mode analysis to study the mode-resolved thermal transport in freestanding and supported Bi2Te3 QL. The detailed mode-wise phonon properties are calculated and the accumulated thermal conductivities with respect to phonon mean free path (MFP) are constructed. It is shown that 60% of the thermal transport is contributed by phonons with MFP longer than 20 nm. Coupling with a-SiO2 substrate leads to about 60% reduction of thermal conductivity. Through varying the interfacial coupling strength and the atomic mass of substrate, we also find that phonon in Bi2Te3 QL is more strongly scattered by interfacial potential and its transport process is less affected by the dynamics of substrate. Our study provides an in-depth understanding of heat transport in Bi2Te3 QL and is helpful in further tailoring its thermal property through nanostructuring.
Bismuth telluride as one of the best room temperature thermoelectric materials has attracted significant attention recently1,2,3,4,5. The performance of thermoelectric materials is characterized by its figure of merit
where S, σ, T, κe and κl are the Seebeck coefficient, electrical conductivity, absolute temperature, electrical thermal conductivity and lattice thermal conductivity, respectively. One effective approach to enhance ZT is to reduce the lattice thermal conductivity of a thermoelectric material1,2,3. Significant progress has been made in the last decade to decrease the lattice thermal conductivity of Bi2Te3-based materials. For example, in nanostructured bismuth antimony telluride bulk alloy, a peak ZT of 1.4 can be achieved at 100 °C1. The ZT value of p-type Bi2Te3/Sb2Te3 superlattice was reported to be as high as 2.4 at room temperature, which is mainly due to the controlled transport of phonons and electrons in the superlattices2. Comparing to nanostructured bulk materials, low dimensional materials have large surface-to-volume ratios and size effects, which could be utilized to further enhance the ZT value6,7,8. A few quintuple layers (QLs) Bi2Te3 recently attracted great interest on its thermoelectric property due to its quasi-two-dimensional (2D) structure9. For example, Zhang et al. studied the electron and phonon transport properties in Bi2Te3 QL and found that the ZT value can be optimized to as high as 2.2 at 800 K10. Qiu and Ruan investigated the thermal transport in few-QLs Bi2Te3 thin films using molecular dynamics (MD) simulations11. They found that the thermal conductivity of Bi2Te3 QL first decreases and then increases with the number of QLs, which is attributed to the interplay between Umklapp scattering and boundary scattering11. It is also shown that the thermal conductivity of QLs can be reduced by introducing nanopores11. More recently, Park et al. calculated the thermal conductivity of Bi2Te3 thin films by solving the Boltzmann transport equation under the relaxation time approximation12. They extended the Klemens-Callaway’s model to incorporate the phonon scattering process due to the van der Waals force at the interface of adjacent Bi2Te3 QLs and could correctly reproduce the anisotropic heat transport of Bi2Te312. While these studies provided a better understanding of electronic and thermal transport properties in Bi2Te3 QL, detailed information about mode-resolved phonon transport properties and its contribution to thermal conductivity is still missing. Such information is crucial for a better understanding of thermal transport and tailoring the thermal conductivity13,14.
On the other hand, in the experimental characterization of thermal properties, the 2D Bi2Te3 QLs could be supported on a substrate15,16. More generally, the coupling with another material (typically unavoidable) could affect the thermal transport of low-dimensional materials5,17. There have been quite a few studies focusing on the thermal transport of low-dimensional materials when it is weakly bonded to another material (typically to a substrate)18,19,20,21. It is generally believed that the properties of low dimensional materials are very sensitive to the presence of substrate18,19,20,21. For example, Ong et al. studied the substrate effects on thermal transport in graphene and found that coupling to the substrate can reduce the thermal conductivity of graphene by an order of magnitude, but further increasing the coupling strength will enhance the thermal transport, due to the coupling of flexural acoustic phonons with substrate Rayleigh waves19. Qiu and Ruan performed a phonon spectral analysis to study the effect of silicon dioxide substrate on graphene22. They found that the presence of silicon dioxide substrate can reduce the phonon relaxation times (RTs) on all phonon branches22. There are also some studies showing that the thermal conductivity of could be enhanced due to the coupling with another material. For example, Zhang et al. studied the effect of substrate on heat transport in two-dimensional (2D) silicene and found that depending on the different crystal types of silicon carbide substrate, the thermal conductivity of 2D silicene could be either enhanced or suppressed23. Guo et al. investigated thermal transport in two coupled Fermi-Pasta-Ulam chains. The results show that in certain regions the coupling to another chain can increase the thermal conductivity of the chain20. They believe that the enhancement of thermal conductivity is due to the reduction of anharmonic phonon scattering, which is induced by the shift of the phonon band to the low wave vector20. Bi2Te3 QL is different from those materials in previous studies, because it has strong anharmonicity and extremely low thermal conductivity. The detailed effects of substrate on its thermal transport remain unclear and a systematic investigation is highly desirable.
In this work, we adopt MD based methods to study the phonon transport in 2D Bi2Te3 QL. Thermal conductivities of freestanding and supported Bi2Te3 QL are first calculated through non-equilibrium molecular dynamics (NEMD) and Green-Kubo methods. Then the normal mode analysis (NMA) method is employed to obtain the mode-resolved phonon transport properties in Bi2Te3 QL. The structure of Bi2Te3 QL coupled with an a-SiO2 substrate is also investigated to explore the substrate effects. Accumulated thermal conductivities with respect to MFP for both freestanding and supported Bi2Te3 are constructed to quantify the contribution of different phonon modes to thermal conductivity. We also investigated the effect of coupling strength and the atomic mass of substrate on the heat transfer in Bi2Te3 QL.
Molecular dynamics simulations
In this work, MD based methods are adopted to study the thermal transport properties of Bi2Te3 QL. LAMMPS package is used to carry out all the MD simulations24. It should be noted that there are also some recent works using the first-principles methods to study the thermal properties in Bi2Te310,25. Although first-principles simulation can extract more accurate force constants, it is still difficult to incorporate higher order anharmonicity26,27. The large computational cost also made it is difficult to be applied to study a Bi2Te3 QL or the effect of the external perturbation from a substrate.
The atomic structure of Bi2Te3 QL is shown in Fig. 1(a). It contains five atomic layers with a sequence of Te1-Bi-Te2-Bi-Te1. Each layer has a hexagonal crystal structure with lattice constant a = 4.369 Å. The thickness of the QL is 10.14 Å, which is one-third of lattice constant of bulk Bi2Te3 along the cross-plane direction. A two-body Morse-type potential developed by Qiu et al. is used to model the interaction between atoms in Bi2Te3 QL28. An a-SiO2 substrate is used to study the effect of substrate on heat transport in Bi2Te3 QL. We choose a-SiO2 for its widely used in experiments15. A Tersoff-type potential parameterized by Munetoh et al.29 is used to model the interaction between Si and O atoms. To generate the a-SiO2, we first heat the β-cristobalite to 6000 K using a Langevin thermostat and maintain that temperature for 10 ps. Then the system is slowly quenched to 300 K at a rate of 1012 K/s30. The a-SiO2 substrate is 2 nm thick, which should be thick enough to eliminate the size effect based on the previous studies22,31,32. Because of the van der Waals nature of interaction between the Bi2Te3 QL and substrate, a Lennard-Jones (LJ) potential is adopted to describe the interaction, which has the form of
where εij is the potential well depth, σij is the distance at which the potential energy reaches zero and rij is the separation between atoms i and j. In this study, the parameters are obtained based on the universal force model33, which gives εBi-Si = 17.9 meV, σBi-Si = 3.9 Å, εBi-O = 7.6 meV, σBi-O = 3.5 Å, εTe-Si = 17.3 meV, σTe-Si = 3.9 Å, εTe-O = 6.7 meV and σTe-O = 3.5 Å. The cutoff distance for LJ potential is set to be 10 Å.
We use both NEMD and Green-Kubo methods to calculate the thermal conductivity of freestanding Bi2Te3 QL and use NEMD to calculate the thermal conductivity of supported Bi2Te3 QL. The schematic of the simulation domain used in NEMD is shown in Fig. 1(b,c). The outermost regions are static regions in which the atoms are fixed during the NEMD process. Next to the fixed regions are the hot and cold thermal reservoirs. Periodic boundary condition is applied to all three directions, while a vacuum layer of 5 nm is used in z direction (cross plane direction) to model the freestanding situation. The width (y direction) of the simulation domain is set to be 6 nm after convergence tests. It is well known that NEMD methods suffer from the finite size effect in predicting the thermal conductivity. In order to eliminate this effect, we vary the domain size along the x direction and use the extrapolation method to obtain the thermal conductivity. In freestanding cases, we vary the length from 16 to 80 nm. For the supported cases, due to the large computational costs, the maximum length along the heat flux direction is 40 nm. A time step of 2 fs is used the simulations of freestanding Bi2Te3 QL. Due to the existence high of frequency vibration modes in a-SiO2 substrate, we use a time step of 0.25 fs for supported Bi2Te3 QL. The system is first equilibrated in an NVT ensemble at 300 K for 0.5 ns and then switched to NPT ensemble to release the internal stress for 1 ns. After that atoms at two ends are fixed and the temperature of two reservoirs are maintained at 320 K and 280 K respectively through the velocity rescaling method34. After obtaining the steady state temperature gradient and heat flux across the system, Fourier’s law is applied to calculate the thermal conductivity.
For the Green-Kubo method, the thermal conductivity is obtained from the autocorrelation of the heat current vector. Equilibrium molecular dynamic (EMD) simulations are carried out to calculate heat current vectors. The simulation domain used for EMD simulations is 5.6 × 5.2 nm2 in the x and y direction (containing 910 atoms), while in z direction a length of 10 nm is used to model the freestanding structure. According to the previous MD study on Bi2Te3 QL11, our simulation domain size is large enough to obtain converged thermal conductivity. We first run the pre-equilibrium procedures similar to the NEMD simulation to make sure the system reaches equilibrium state. After that the system is switched to an NVE ensemble for 2 ns and the heat current data is recorded every 10 fs. These heat current data are then used to calculate the heat current autocorrelation function (HCACF). Fifteen independent simulations (different in initial velocities) are used to explore the phase space and make sure our results are true ensemble average30,35. Here a direct integral method is used to integrate the HCACF and to obtain the thermal conductivity. It should be noted that in some previous works, a low-pass filter is used to remove the optical component in the HCACF and the exponential fitting method is used to extract the final thermal conductivity28,36. To make a comparison, we used the directed integral method to integrate the HCACF with and without a low-pass filter (the cutoff frequency is 0.5 THz) and found they yield similar results.
Normal mode analysis
While NEMD and Green-Kubo method can provide an overall thermal conductivity, no information at the phonon level can be obtained. In order to obtain better insights about heat transport in Bi2Te3 QL, a mode-wise analysis is necessary. In normal mode analysis (NMA), the trajectories of each atom are projected onto the normal modes and the amplitude of each normal mode can be written as37,38
where Q(k, ν, t) denotes the amplitude of a normal-mode with wave vector k and polarization ν at time t, N is the number of unit cells in the simulation domain, m is the mass, r is the equilibrium position of an atom, e(k, ν) is the mode eigenvector and u is the displacement. The subscript j denotes the j-th atom in a unit cell, l denotes the l-th unit cell and the superscript *denotes the complex conjugate.
When the lattice is purely harmonic, the normal-mode amplitudes will be periodic functions of time. The anharmonic forces cause the damping of the normal-mode. If the anharmonic effect is small, the normal-mode amplitudes can be written as39
where ω0(k, ν) is the unperturbed harmonic frequency of this mode, Δ(k, ν) is the frequency shift and Γ(k, ν) is the linewidth. The phonon spectral linewidth Γ(k, ν) and the phonon relaxation time τ(k, ν) have the following relationship
In order to obtain the phonon relaxation time, we apply a Fourier transform to the time derivative of each normal-mode and express the spectral energy density (SED) of this mode as:
where denotes the Fourier transform, (k, ν, t) is the time derivative of Q(k, ν, t), ω(k, ν) is the anharmonic phonon frequency (equals to ω0(k, ν) + Δ(k, ν) from Equation (4)) and Φ(k, ν,ω) is the SED of this mode and can be expressed as a Lorentzian function. The phonon frequency and relaxation time are obtained by fitting the SED plot with a Lorentzian function. The location of peak gives the phonon frequency and the inverse of full width at half maximum 2Γ is the phonon relaxation time τ.
Similar to previous studies, we make the isotropic approximation for the first Brillouin zone32,40. A simulation domain of 13.1 × 6.1 nm2 in the x and y direction is used in our study. It should be noted that available k points are depending on the size of simulation domain41, so there are 21 k points available along the Γ to K direction in our simulations. The lattice dynamics program GULP is used to calculate the eigenvectors42. The atomic positions and velocities are recorded at a 10 fs interval during an NVE process at 300 K. A trajectory of 20 ns is used in the NMA to extract the phonon frequencies and relaxation times. We also apply the NMA to bulk Bi2Te3. In bulk Bi2Te3 the lattice constant along the cross-plane direction is 30.42 Å, which contains three QLs. Periodic boundary condition is used in the cross-plane direction to model the bulk situation. All the other simulation details are similar to that used for Bi2Te3 QL.
Results and Discussions
Thermal conductivity of freestanding and supported Bi2Te3 QL
Thermal conductivity values of freestanding and supported Bi2Te3 QL at different lengths calculated from the NEMD method are shown in Fig. 2. These data points were extrapolated with a linear function to obtain the thermal conductivity at infinite length43, which are 2.2 ± 0.2 W/mK and 0.91 ± 0.08 W/mK for freestanding and supported cases, respectively. For the freestanding case, there seems to be an onset of a convergence of the thermal conductivity at the point when L = 80 nm (1/L = 0.0125 nm−1). Adopting linear fitting may overestimate the thermal conductivity. Therefore, we also tried to extrapolate thermal conductivity using a quadratic fitting and it yields 2.1 W/mK. The Green-Kubo method was also used to calculate the in-plane thermal conductivity of freestanding Bi2Te3 QL for comparison. To obtain the thermal conductivity, one can either fit the HCACF with exponential function, or directly integrate the HCACF. In a previous work by Qiu and Ruan28, the former approach was adopted and a low-pass filter was used to remove the high frequency oscillation. In our simulation the direct integration method is used. From Fig. 3, one can see that whether removing the high frequency oscillation components of the HCACF does not obviously affect the final thermal conductivity value. The result is 1.8 ± 0.1 W/mK, which is consistent with our NEMD result and agrees well with the work by Qiu and Ruan (1.7 ± 0.4 W/mK)11. To compare with experiment, Teweldebrhan et al.15 measured the thermal conductivity of stacked few QLs and found that the thermal conductivity is about 1.1 W/mK, which is slightly lower than our simulation results.
Supporting on an a-SiO2 substrate leads to a ∼60% reduction in thermal conductivity based on our NEMD simulation results. Such a magnitude of reduction is smaller compared to some other 2D materials that supported on the same substrate. For example, Ong et al. found that the thermal conductivity of graphene is reduced by an order of magnitude once supported on an a-SiO2 substrate19. Wang et al. also reported a 78% reduction in thermal conductivity of silicene supported on a-SiO2 substrate32. Comparing to these monolayer 2D materials, the substrate has less effect on the thermal conductivity of Bi2Te3 QL. This is likely due to the five-layer structure of Bi2Te3 QL: only the lowest layer is strongly coupled with the substrate while the other layers are relatively weakly coupled. In another work that studies the supported multilayer graphene, it was also found that the substrate suppression of the thermal conductivity is less prominent in multilayer graphene44.
Mode-wise phonon properties in Bi2Te3 QL
In order to gain a better understanding of thermal conductivity reduction in the supported Bi2Te3 QL, we perform the NMA to the freestanding and supported QL. The SED spectra of freestanding and supported QL are firstly calculated for comparison. In order to obtain a better resolution in the SED figures, a larger simulation domain (131 × 6.1 nm2 in the x and y direction) was adopted so that 201 k-points can be extracted along Γ to K direction. The total simulation time is reduced to 2 ns. The phonon SEDs at points along the Γ to K direction of freestanding and supported Bi2Te3 QL are shown in Fig. 4(a,b). The SED spectra of supported Bi2Te3 with a stronger coupling strength (5 times of the original one) are also shown in Fig. 4(c). The magnitude of the SED is represented by different colors, as shown in Fig. 4. The location of local maximum in the SED spectra gives the frequency of a normal mode (or phonon mode) while the broadening of the local maximum gives the phonon linewidth. Therefore, the local peaks in SED spectra give the phonon dispersion curve and the span of the peaks represents the phonon RTs.
A major difference between the supported and freestanding QL is the zone center flexural modes. For supported case, the flexural mode near the zone center is flattened and significantly broadened. A similar flattening of ZA-mode was also reported in a previous study of few layer graphene supported on a-SiO2 substrate45,46. From their studies, the coupling to the substrate has twofold effects on the supported graphene45,46. First, the dispersion of the flexural mode upward shifted from the origin. Second, the flexural mode will become linearized due to the hybridization with the surface Rayleigh mode45,46. For the supported Bi2Te3 QL, the flexural mode indeed shifted upward but the linearization is not clearly observed. The dispersion curve in supported Bi2Te3 QL became blurred comparing to the freestanding QL, which indicates a relatively shorter phonon RTs in the supported case. From Fig. 4(c) it can be seen that the dispersion curve became further blurred with the increasing of coupling strength. This indicates that the substrate could introduce additional phonon scattering and the scattering strength increases with the increasing of coupling strength.
To quantitatively evaluate the effect of substrate on supported Bi2Te3 QL, we calculate the phonon RTs by fitting the SED spectra with a Lorentz function as described in Eq. (6). The results are shown in Fig. 5. Phonon RTs along Γ to K point in bulk Bi2Te3 are also shown for comparison. It can be seen that the RTs in freestanding Bi2Te3 QL can be as long as 200 ps in the low frequency region. Supporting on a substrate leads to a reduction in RTs within the frequency range. The reduction of RTs is especially strong for flexural modes, which are marked by stars in Fig. 5. The average RTs of flexural modes in freestanding QL is 46 ps, while in the supported case the average RTs is reduced to 8.5 ps. It is also reported in graphene that the flexural modes are more sensitive to the presence of substrate19,22. We believe there are two major reasons for the strong reduction of ZA mode RTs. First, the potential field from the substrate can break the selection rule for ZA phonon scattering, so that a three phonon process involving odd number of ZA modes could occur in the supported QL. This gives a larger scattering rate of ZA modes47. Second, the ZA modes in QL will hybridize with the substrate Rayleigh mode, which leads to an enhanced scattering rate between the ZA mode and the substrate mode46.
Thermal conductivity analysis
After obtaining the spectral phonon properties from the NMA and making the assumption that the first Brillouin zone is isotropic, we can express the thermal conductivity as32,40
where κx is the thermal conductivity in x direction, δ is the thickness of Bi2Te3 QL, ν represents different polarization, cph(kx, ν) is the phonon specific heat of phonon mode (kx, ν), vg,x(kx, ν) is the phonon group velocity in x direction calculated from harmonic lattice dynamics and τ(kx, ν) is the phonon relaxation time.
The overall thermal conductivities of freestanding and supported Bi2Te3 QL predicted by NMA are 2.1 and 1.0 W/mK, which agree relativity well with that calculated from NEMD and Green-Kubo method. From the NMA calculation, the substrate leads to a ~50% reduction in thermal conductivity, which is also similar to the NEMD results.
We further build the accumulated thermal conductivity with respect to MFP, which can be expressed as
where λ* is the cutoff MFP, cλ(λ) is the volumetric heat capacity per unit MFP and the sum is over all polarizations. The phonon MFP λ and relaxation time τ has the relationship λ = vgτ. In practice, we used a discrete summation over phonon modes with MFP less than λ* to calculate the integral in Eq. (8). The accumulated thermal conductivities are shown in Fig. 6. Comparing the accumulated thermal conductivity of freestanding and supported Bi2Te3 QL, it can be seen that the reduction in thermal conductivity of supported QL is mainly due to the suppression of long MFP phonon modes. Below 20 nm, the accumulated thermal conductivity of freestanding and supported Bi2Te3 QL are almost the same, while the thermal conductivity contributed by phonon with MFPs larger than 20 nm is 1.2 W/mK in freestanding Bi2Te3 QL and 0.2 W/mK in supported Bi2Te3 QL. We can also see that half of the heat in freestanding Bi2Te3 QL is carried by phonons with MFPs larger than 52.4 nm, while in supported QL this value is reduced to 24.2 nm. The accumulated thermal conductivity as a function of MFP for bulk Bi2Te3 is also shown in Fig. 6 for comparison. It has been previously demonstrated by EMD simulations that Bi2Te3 QL has a larger thermal conductivity than bulk Bi2Te311. From the accumulated thermal conductivity function, it can be seen that such an enhancement is mainly contributed by the phonons with MFPs longer than 25 nm (phonon modes near zone center) in Bi2Te3 QL.
The thermal conductivity contributed from different branches, namely out-of-plane (ZA), longitudinal acoustic (LA), transverse acoustic (TA) and optical branches are also analyzed and the results are shown in Fig. 7. For freestanding Bi2Te3 QL, the ZA branch contributes most of the thermal conductivity (37%) and the contribution from all three acoustic branches (ZA, TA and LA branch) is 88%. The contribution from optical branch is very small. It should be noted that the large contribution from ZA mode to the heat transfer is not unusual for 2D materials. For materials with reflectional symmetry in the xy plane (e.g. graphene), due to the unique selection rule for phonon scattering, the ZA modes tend to scatter less with other phonon modes47. Placing on the substrate will suppress the thermal conductivity of all branches, while the suppression in ZA branch is the most significant. From the relaxation times in Fig. 5, it can be seen that this is mainly due to the largely reduced in relaxation time of ZA modes.
Effect of substrate atomic mass and interaction strength
When a 2D material is coupled with another material, for example, supported by a substrate, the detailed interaction and adhesion energy may be quite different, depending on the material types, the interfacial geometry and the surface polarity of substrate48,49. It is also reported that the thermal conductivity of supported materials could be quite different depending on the coupling strength and mass ratio to the substrate20. In fact this feature could be utilized to tune the thermal conductivity of supported materials20,23. To explore the effects of different substrate, we generalize our substrate to a virtual one with different atomic masses and coupling strengths with the supported QL. The NMA in combination with Eq. (7) is used to calculate the thermal conductivity of supported Bi2Te3 QL on different virtual substrates. The coupling strength is tuned by scaling the potential depth ε in the LJ potential for all atom-pairs between the substrate and the QL. The results are shown as the inset of Fig. 8. We can see that increasing the coupling strength tends to further reduce the thermal conductivity of Bi2Te3 QL. Doubling the interaction strength could reduce the thermal conductivity to 0.63 W/mK. Further increasing the coupling strength leads to a further reduction in thermal conductivity. It should be noted that in the case of 10 times the coupling strength, the adhesion energy between substrate and QL becomes 0.91 J/m2, while the adhesion energy between the atomic layers in QL is 9.8 J/m2. In this case the QL and the substrate are relatively strongly coupled and it can be inferred from Fig. 4 that the zone center flexural branch is flattened due to the existence of substrate. This means that the phonon frequencies and eigenvectors of the supported QL are changed due to the perturbation from the substrate. In such case, whether the eigenvectors for the freestanding QL are applicable for the perturbed system remains unclear50,51. To demonstrate the applicability of the unperturbed eigenvectors to the perturbed system, we check the SED profiles of zone center flexural modes with the 10 times coupling strength and plot a typical spectrum (flexural mode with wavevector k = (1/15, 0, 0) × 2π/a) in Fig. 9. We can clearly see a single peak in the SED profile with no significant disruption, indicating that the eigenvectors of the freestanding QL are robust enough to resolve the phonon modes in the supported QL. This further confirms the accuracy of our NMA calculation on the RTs and thermal conductivity for the supported case.
We also scale the atomic mass of all atoms in the substrate by a factor (mass ratio) to explore the effects of substrate atomic mass on the thermal transport in supported materials. The relationship between thermal conductivity and atomic mass ratio of substrate is shown in Fig. 8. We can see that with the increasing of the atomic mass, thermal conductivity of supported Bi2Te3 QL does not change much, except for the cases when the mass ratio is 1000 or when the atoms fixed. When the atomic mass is 1000, the substrate becomes almost immovable and the direct scattering process between phonon in Bi2Te3 QL and phonons in substrate is largely suppressed45. The presence of substrate can affect the thermal transport in supported materials from two different aspects: the static potential at the interface introduced by the substrate and the dynamics of the substrate itself 52. These two effects can be decoupled through comparing the thermal conductivity of QL under different environment: freestanding, supported and supported on a substrate with fixed atoms. For the case of substrate with fixed atoms, the reduction of thermal conductivity is mainly due to the static potential at the interface. From Fig. 8, it can be seen that this effect leads to a 40% reduction in thermal conductivity. Allowing the atoms in the substrate to move will introduce additional scattering with substrate phonons, which leads to an additional 13% reduction in thermal conductivity.
To summarize, we have systematically investigated the mode-resolved phonon transport properties of freestanding and supported Bi2Te3 QL by the MD-based NMA methods. The thermal conductivities of freestanding and supported Bi2Te3 QL are predicted to be 2.1 and 1.0 W/mK, respectively. These values are consistent with the predictions from NEMD and Green-Kubo methods. It is shown that the phonon RTs in the Bi2Te3 QL range from 1 to 200 ps. Some low frequency phonons have evidently larger relaxation time than that in the bulk Bi2Te3, which are responsible for the larger thermal conductivity of the QL comparing to bulk phase. The accumulated thermal conductivity is also constructed, which shows that about 60% of the heat is carried by phonons with MFP longer than 20 nm in the QL. The low thermal conductivity of supported QL is mainly attributed to the reduced phonon RTs of all the frequency range and most significantly for ZA phonon modes. By further varying the coupling strength with substrate and the atomic mass of substrate, we conclude that interfacial scattering is the dominating factor that leads to a reduction of about 40% of the thermal conductivity of Bi2Te3 QL. Further increasing the coupling strength can significantly suppress the thermal conductivity in Bi2Te3 QL. Scattering with the substrate phonons can reduce the thermal conductivity by about 13%. Moderate variation of the atomic mass of the substrate has a relatively small effect on the thermal conductivity of the supported QL.
How to cite this article: Shao, C. and Bao, H. Thermal transport in bismuth telluride quintuple layer: mode-resolved phonon properties and substrate effects. Sci. Rep. 6, 27492; doi: 10.1038/srep27492 (2016).
Poudel, B. et al. High-thermoelectric performance of nanostructured bismuth antimony telluride bulk alloys. Science 320, 634–638 (2008).
Venkatasubramanian, R., Siivola, E., Colpitts, T. & O’quinn, B. Thin-film thermoelectric devices with high room-temperature figures of merit. Nature 413, 597–602 (2001).
Tang, X. et al. Preparation and thermoelectric transport properties of high-performance p-type Bi2Te3 with layered nanostructure. Appl. Phys. Lett. 90, 012102 (2007).
Zhao, X. B. et al. Bismuth telluride nanotubes and the effects on the thermoelectric properties of nanotube-containing nanocomposites. Appl. Phys. Lett. 86, 062111 (2005).
Cao, Y. Q., Zhao, X. B., Zhu, T. J., Zhang, X. B. & Tu, J. P. Syntheses and thermoelectric properties of Bi2Te2∕Sb2Te3 bulk nanocomposites with laminated nanostructure. Appl. Phys. Lett. 92, 143106 (2008).
Hicks, L. D. & Dresselhaus, M. S. Thermoelectric figure of merit of a one-dimensional conductor. Phys. Rev. B 47, 16631 (1993).
Balandin, A. & Wang, K. L. Significant decrease of the lattice thermal conductivity due to phonon confinement in a free-standing semiconductor quantum well. Phys. Rev. B 58, 1544 (1998).
Dresselhaus, M. S. et al. New directions for low-dimensional thermoelectric materials. Adv. Mater. 19, 1043–1053 (2007).
Teweldebrhan, D., Goyal, V., Rahman, M. & Balandin, A. A. Atomically-thin crystalline films and ribbons of bismuth telluride. Appl. Phys. Lett. 96, 053107 (2010).
Zhang, J. et al. Enhanced thermoelectric performance of a quintuple layer of Bi2Te3 . J. Appl. Phys. 116, 023706 (2014).
Qiu, B. & Ruan, X. Thermal conductivity prediction and analysis of few-quintuple Bi2Te3 thin films: A molecular dynamics study. Appl. Phys. Lett. 97, 183107 (2010).
Park, K. H., Mohamed, M., Aksamija, Z. & Ravaioli, U. Phonon scattering due to van der Waals forces in the lattice thermal conductivity of Bi2Te3 thin films. J. Appl. Phys. 117, 015103 (2015).
Pernot, G. et al. Precise control of thermal conductivity at the nanoscale through individual phonon-scattering barriers. Nature Mater. 9, 491–495 (2010).
Hu, Y., Zeng, L., Minnich, A. J., Dresselhaus, M. S. & Chen, G. Spectral mapping of thermal conductivity through nanoscale ballistic transport. Nature Nanotech. 10, 701–706 (2015).
Teweldebrhan, D., Goyal, V. & Balandin, A. A. Exfoliation and characterization of bismuth telluride atomic quintuples and quasi-two-dimensional crystals. Nano Lett. 10, 1209–1218 (2010).
Jia, L., Ma, W. & Zhang, X. Ultrafast carrier dynamics in polycrystalline bismuth telluride nanofilm. Appl. Phys. Lett. 104, 241911 (2014).
Liao, Q., Liu, Z., Liu, W., Deng, C. & Yang, N. Extremely high thermal conductivity of aligned carbon nanotube-polyethylene composites. Sci. Rep. 5, 16543 (2015).
Seol, J. H. et al. Two-dimensional phonon transport in supported graphene. Science 328, 213–216 (2010).
Ong, Z.-Y. & Pop, E. Effect of substrate modes on thermal transport in supported graphene. Phys. Rev. B 84, 075471 (2011).
Guo, Z.-X., Zhang, D. & Gong, X.-G. Manipulating thermal conductivity through substrate coupling. Phys. Rev. B 84, 075470 (2011).
Yue, Y., Zhang, J., Tang, X., Xu, S. & Wang, X. Thermal transport across atomic-layer material interfaces. Nanotechnol. Rev. 4, 533 (2015).
Qiu, B. & Ruan, X. Reduction of spectral phonon relaxation times from suspended to supported graphene. Appl. Phys. Lett. 100, 193101 (2012).
Zhang, X., Bao, H. & Hu, M. Bilateral substrate effect on the thermal conductivity of two-dimensional silicon. Nanoscale 7, 6014–6022 (2015).
Plimpton, S. Fast parallel algorithms for short-range molecular dynamics. J. Comput. Phys. 117, 1 (1995).
Hellman, O. & Broido, D. A. Phonon thermal transport in Bi2Te3 from first principles. Phys. Rev. B 90, 134309 (2014).
Feng, T. & Ruan, X. Prediction of spectral phonon mean free path and thermal conductivity with applications to thermoelectrics and thermal management: a review. J. Nanomater. 2014, e206370 (2014).
Xie, H., Hu, M. & Bao, H. Thermal conductivity of silicene from first-principles. Appl. Phys. Lett. 104, 131906 (2014).
Qiu, B. & Ruan, X. Molecular dynamics simulations of lattice thermal conductivity of bismuth telluride using two-body interatomic potentials. Phys. Rev. B 80, 165203 (2009).
Munetoh, S., Motooka, T., Moriguchi, K. & Shintani, A. Interatomic potential for Si–O systems using Tersoff parameterization. Comput. Mater. Sci. 39, 334 (2007).
Shao, C. & Bao, H. A molecular dynamics investigation of heat transfer across a disordered thin film. Int. J. Heat Mass Transfer 85, 33–40 (2015).
Ong, Z.-Y. & Pop, E. Molecular dynamics simulation of thermal boundary conductance between carbon nanotubes and SiO2 . Phys. Rev. B 81, 155408 (2010).
Wang, Z., Feng, T. & Ruan, X. Thermal conductivity and spectral phonon properties of freestanding and supported silicene. J. Appl. Phys. 117, 084317 (2015).
Rappé, A. K., Casewit, C. J., Colwell, K. S., Goddard Iii, W. A. & Skiff, W. M. UFF, a full periodic table force field for molecular mechanics and molecular dynamics simulations. J. Am. Chem. Soc. 114, 10024–10035 (1992).
Bao, H., Shao, C., Luo, S. & Hu, M. Enhancement of interfacial thermal transport by carbon nanotube-graphene junction. J. Appl. Phys. 115, 053524 (2014).
McGaughey, A. Predicting phonon properties from equilibrium molecular dynamics simulations. Ann. Rev. Heat Transfer 17, 49–87 (2014).
Huang, B.-L. & Kaviany, M. Ab initio and molecular dynamics predictions for electron and phonon transport in bismuth telluride. Phys. Rev. B 77, 125209 (2008).
Dove, M. T. Introduction to lattice dynamics. 93–94 (Cambridge university press, 1993).
Bao, H., Qiu, B., Zhang, Y. & Ruan, X. A first-principles molecular dynamics approach for predicting optical phonon lifetimes and far-infrared reflectance of polar materials. J. Quant. Spectrosc. Radiat. Transfer 113, 1683–1688 (2012).
Ladd, A. J. C., Moran, B. & Hoover, W. G. Lattice thermal conductivity: A comparison of molecular dynamics and anharmonic lattice dynamics. Phys. Rev. B 34, 5058–5064 (1986).
Wang, Y., Qiu, B., McGaughey, A. J., Ruan, X. & Xu, X. Mode-wise thermal conductivity of bismuth telluride. J. Heat Transfer 135, 091102 (2013).
Qiu, B., Bao, H., Zhang, G., Wu, Y. & Ruan, X. Molecular dynamics simulations of lattice thermal conductivity and spectral phonon mean free path of PbTe: Bulk and nanostructures. Comput. Mater. Sci. 53, 278–285 (2012).
Gale, J. D. GULP : A computer program for the symmetry-adapted simulation of solids. J. Chem. Soc., Faraday Trans. 93, 629–637 (1997).
Sellan, D. P., Landry, E. S. & Turney, J. E. Size effects in molecular dynamics thermal conductivity predictions. Phys. Rev. B 81, 214305 (2010).
Chen, J., Zhang, G. & Li, B. Substrate coupling suppresses size dependence of thermal conductivity in supported graphene. Nanoscale 5, 532–536 (2013).
Ni, Y., Kosevich, Y. A., Xiong, S., Chalopin, Y. & Volz, S. Substrate-induced cross-plane thermal propagative modes in few-layer graphene. Phys. Rev. B 89, 205413 (2014).
Amorim, B. & Guinea, F. Flexural mode of graphene on a substrate. Phys. Rev. B 88, 115418 (2013).
Lindsay, L., Broido, D. A. & Mingo, N. Flexural phonons and thermal transport in graphene. Phys. Rev. B 82, 115427 (2010).
Kang, Y.-J., Kang, J. & Chang, K. J. Electronic structure of graphene and doping effect on SiO2 . Phys. Rev. B 78, 115404 (2008).
Sachs, B., Wehling, T. O., Katsnelson, M. I. & Lichtenstein, A. I. Adhesion and electronic structure of graphene on hexagonal boron nitride substrates. Phys. Rev. B 84, 195414 (2011).
Huberman, S., Larkin, J., McGaughey, A. & Amon, C. Disruption of superlattice phonons by interfacial mixing. Phys. Rev. B 88, 155311 (2013).
Feng, T., Qiu, B. & Ruan, X. Anharmonicity and necessity of phonon eigenvectors in the phonon normal mode analysis. J. Appl. Phys. 117, 195102 (2015).
Ong, Z.-Y., Pop, E. & Shiomi, J. Reduction of phonon lifetimes and thermal conductivity of a carbon nanotube on amorphous silica. Phys. Rev. B 84, 165418 (2011).
This work is supported by the National Natural Science Foundation of China (No. 51306111) and Shanghai Municipal Natural Science Foundation (No. 13ZR1456000). The computational support from Center for High Performance Computing at Shanghai Jiao Tong University (π) is also gratefully appreciated. C.S. would like to thank Dr. Bo Qiu for sharing the NMA code and Tianli Feng for fruitful discussions.
The authors declare no competing financial interests.
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Shao, C., Bao, H. Thermal transport in bismuth telluride quintuple layer: mode-resolved phonon properties and substrate effects. Sci Rep 6, 27492 (2016). https://doi.org/10.1038/srep27492
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