Communication: Length-dependent thermopower of single-molecule junctions Free

As known, tailored nanostructures hold promise for enhanced efficiency of heat-to-electric energy conversion. Therefore, thermoelectric properties of tailored nanoscale systems including carbon-based nanostructures, quantum dots, and single-molecule junctions have been explored both theoretically and experimentally.^1–4 Numerous works were focused on the Seebeck effect which is directly responsible for the conversion of heat to electric energy. This effect occurs when a thermal gradient is applied across a system inducing a current of charge carriers. The Seebeck effect in nanoscale systems is measured by recording the voltage $ΔV$ which cancels the thermally induced current provided that the temperature difference $ΔT$ between two ends of the system is kept constant.^5,6 When $ΔT≪T(T$ being an average temperature characterizing the system), the system operates within the linear response regime, so $ΔV=−SΔT.$ The coefficient of proportionality which appears in this expression is commonly called thermopower.

Various properties of the thermopower of single-molecule systems were intensively studied including inelastic effects,^7–9 effects of molecular bridge geometry,^10,11 of Coulomb interactions between the electrons on the bridge,^12–15 of molecular vibrations,^16–18 and of quantum interference.¹⁹ In particular, it was demonstrated that both the thermopower and electron conductance of single-molecule junctions may depend on the molecular linker length. Length-dependent conductance and thermopower are usually observed in junctions where the molecular bridge is a chain-like structure consisting of several identical units (e.g., benzene rings).^{5,6,11,20–24} These molecular linkers provide a better opportunity to observe the relationship between the thermopower and the length of the linker. For other kinds of linkers, this relationship is less distinct due to the diversity of specific properties associated with different parts of the linker. In the most of the experiments concerning the issue, the thermopower appeared to be proportional to the molecular bridge length. However, this linear relationship between the thermopower and the bridge length is not a universal one. Recent experiments carried out on single-molecule junctions with gold electrodes and oligophenyl and alkane chain-like linkers showed a distinctly nonlinear length dependence of the thermopower.²³ The purpose of the present work is to theoretically analyze the possible origin of nonlinearities in the length dependence of thermopower. Also, we discuss specific features of the thermopower versus length profiles.

In the following analysis, we assume coherent electron tunnelling to be a predominant transport mechanism. At low temperatures, the thermopower and conductance through the junction may be computed from the electron transmission $τ(E)$ provided that the latter smoothly varies for $|E−EF|<kT(EF$ being the chemical potential of electrodes in the unbiased junction) and that the temperature difference between the electrodes $ΔT$ is much smaller than T. The corresponding approximations have the form²⁵ 

These approximations are commonly used to describe the conductance and thermopower dependences on the molecular length and geometry observed in experiments. To employ them, one needs to compute the electron transmission function through the considered molecular junction. Often, $τ(E)$ is obtained based on the electronic structure calculations carried out within the density functional theory (DFT) (see, e.g., Refs. 10, 20–23, and26). Nevertheless, the length-dependent electron transmission may be qualitatively analyzed using simplified Lorentzian and tight-binding models which were invented to explain specific experimental results.^20–23 

In this work, we simulate a chain-like linker in a single-molecule junction by a periodical chain including N identical sites. Each site is assigned a single on-site energy E_i and coupled to its nearest neighbors. For all sites except the terminal ones, the energies E_i are supposed to be equal $(Ei=E0, 2≤i≤N−1)$ whereas $E1=EN=ϵ.$ The terminal states are coupled to electrodes through imaginary self-energy terms $−iΓ/2$ which are supposed to be energy-independent. Also, we assume that the terminal states are coupled to their neighbors in the chain through the coupling parameter δ which may differ from the parameter β characterizing the coupling between the remaining sites. The terminal sites are separated out because they may play a significant part in the origin of nonlinearity in the length dependence of the thermopower in certain single-molecule junctions. This model is physically relevant for molecular bridges where $π−π$ dominates electron transport. Then, the parameter β characterizes the coupling between π orbitals.²⁷ 

Within the accepted model, $τ(E)=Γ24|G1N(E)|2$⁠, where G_1N is the corresponding matrix element of the retarded Green’s function for the chain,

and the Hamiltonian H is represented by $N×N$ matrix,

Using Eqs. (3) and (4), a close expression for $G1N(E)(N≥3)$ may be derived in the form consistent with previously reported results,^28,29

Here

and the determinant $ΔN(E,Γ)$ equals³⁰ 

Other determinants included into Eq. (6) are given by the expressions similar to Eq. (7) where $Γ=0.$ As follows from Eq. (7), $Δ0(E,0)=1$ and $Δ−1(E,0)=0.$ Also, in these expressions $α=E−ϵ,λ=E−E0$⁠, and $ζ=λ2−4β2,$ respectively.

Thermally induced charge carriers travel between electrodes using the highest occupied molecular orbital (HOMO) or the lowest unoccupied molecular orbital (LUMO) as transport channels. We remark that considering electron transport via HOMO, one should take into account that electron tunneling into a molecule causes an expansion in the eigenstates. As a result, other eigenstates besides HOMO may contribute to the transport even when it occurs at the HOMO resonant energy. However, it does not change the present results ((6) and (7)) which remain valid. When the energy values associated with HOMO/LUMO E_H,L noticeably differ from $EF(|EH,L−EF|≫β),$ one may put $β=0$ in the expression for $Δ∼N(EF).$ This results in the exponential decrease in electron conductance as a function of the molecule length typical for off-resonant tunnelling. Such electron conductance behaviour was observed in several experiments.^9,20,22,24 Presenting the conductance in the form $G(E)=A(E)exp[−η(E)N]$ and substituting this expression into Eq. (2), one obtains²¹ 

So, the exponential decrease in the electron conductance accompanying the increase in the molecular bridge length leads to a linear relationship between the thermopower and the bridge length often reported for single-molecule junctions with chain-like bridges.^9,20–22 Within the accepted model, this conclusion is illustrated in Fig. 1. The electron transmission curves plotted here are computed using Eqs. (5)–(7). Values of relevant parameters are chosen to describe the electron transport via HOMO. All peaks in the electron transmission function (including that one corresponding to HOMO) are located rather far away from E = E_F indicating an off-resonant tunneling. Accordingly, both S and $logG$ are linear functions of the number of sites N, as shown in Fig. 1 (right panel).

Nonlinear length dependences of the thermopower may appear when HOMO/LUMO is located near $EF(|EF−EH,L|<β)$⁠. It was suggested²³ that this may happen due to the effect of gateaway states representing the bonds between the terminal carbons in the bridge and electrodes. Within the accepted tight-binding model, these states are associated with

the terminal sites at the ends of the chain. Due to the presence of these states, the electron transmission profiles may be significantly affected. At certain values of energies $ϵ,E0$⁠, and coupling parameters $δ$ and $β,$ peaks associated with HOMO in the plots of $τ(E)$ versus E become broader than other resonance features, as shown in the left panels of Figs. 1 and 2. When these distorted HOMOs are located near E = E_F, the thermopower displays a nonlinear dependence on N presented in Fig. 2. We remark that the values of all relevant energies used in the computations of the electron conductance and thermopower displayed in this figure are the same as those used in Ref. 23, so the results for G(N) and S(N) at $3≤N≤6$ agree with the corresponding results presented in that work. One observes that nonlinear length dependence of the thermopower (and, to a smaller extent, of $logG$⁠) is noticeable while the bridge is rather short. For $N≥6,$ both S and $logG$ become linear functions of the bridge length. This happens because the effect of gateaway states on the electron transmission is fading away as the bridge lengthens and HOMO moves away from E = E_F.

As known, only HOMO/LUMO participates in thermally induced charge transport through a single-molecule junction provided that a temperature gradient applied across the system is sufficiently small. This gives grounds to disregard all molecular resonances except those corresponding to HOMO/LUMO, thus reducing the electron transmission to a single peak nearest to E = E_F. Lorentzian models were used to represent this peak in the computations of the junction thermopower in several works.^6,21,31 To describe the length-dependent thermopower, the coupling parameter between the bridge represented by a single orbital and the leads should be simulated by a length-dependent function. This function should be chosen in such a way that the peak associated with HOMO/LUMO would become sharper and narrower as the bridge length increases. Such models may predict nonlinear dependences of the junction thermopower on the bridge length. For example, the following model for the electron transmission:³¹ 

where $δN=δ0exp[−γN](δ0$ and γ being independent on energy and length) brings the expression for the thermopower which saturates for long molecular bridges approaching the limit

Within the tight-binding model adopted in the present work, one observes that the electron transmission function for the chain including an odd number of sites always shows a Lorentzian-like peak at E = E₀ (see Fig. 3). As the number of sites increases, the width of this peak shrinks although its height remains the same. Assuming that this peak is located slightly to the left from E = E_F and may serve as HOMO, we compute the molecular conductance and thermopower of the corresponding system using Eqs. (1) and (2). The results are presented in the right panel of Fig. 3. As shown in this figure, the thermopower may reach a maximum at a certain bridge length and then decrease as the bridge further extends. This is accompanied by a pronounced nonlinearity in the length dependence of $logG$⁠. This behavior of the thermopower originates from alterations in the transmission peak shape occurring as the number of sites in the bridge increases. At sufficiently small values of N, the slope of the curve $τ(E)$ at E = E_F grows as N enhances. However, at greater values of N, the slope significantly decreases causing the thermopower to decrease. We remark that the decrease in thermopower accompanying the extension of the molecular linker length was not reported so far, although some data experimentally obtained for alkane chains linking gold electrodes²³ may indicate that the thermopower of these molecular junctions could either saturate or decrease for longer chains.

In the present work, we have employed a tight-binding based model to describe a single-molecule junction with a chain-like bridge consisting of an arbitrary number of identical units. We used this model to qualitatively analyze the length-dependent thermopower of the considered system. The obtained results confirm that the character of thermopower dependences on the molecular length is determined by the location of HOMO/LUMO with respect to the chemical potential of electrodes and by the profile of the corresponding peak in the electron transmission function. It is shown that characteristics of terminal sites coupled to the electrodes may bring a nonlinear length dependence of the thermopower when the bridge is sufficiently short. This conclusion agrees with the results reported in Ref. 23. Also, it is predicted that under certain conditions the thermopower of a single-molecule junction may decrease as the molecule length increases. Since experiments on the thermopower of molecular junctions are often carried out at room temperature, finite-temperature effects may play a part in controlling the length dependences of the thermopower. They can affect it by giving rise to fluctuations in the molecular bridge geometry and to molecular vibrations.^6,7,32,33 The model employed in the present work may be generalized to include electron-vibron interactions following the way suggested in Ref. 34. It may be further improved by taking into consideration the energy shift which appears due to the real parts of self-energy terms describing the coupling of the molecular bridge to the leads. There are some grounds to conjecture that this energy shift may influence the thermopower behavior. Finally, the analysis could be extended to study the length-dependent thermoelectric properties of single-molecule junctions beyond linear in $ΔT$ regime. However, these studies are beyond the scope of the present work. Nevertheless, despite the simplicity of the adopted model, we believe that presented results may help in further understanding of the thermoelectric properties of single-molecule junctions.

The author thanks G. M. Zimbovsky for help with the manuscript. This work was supported by No. NSF-DMR-PREM 1523463.