Open Access

Electronic Properties of a New All-Inorganic Perovskite TlPbI3 Simulated by the First Principles

Nanoscale Research Letters201712:232

https://doi.org/10.1186/s11671-017-2015-y

Received: 28 February 2017

Accepted: 20 March 2017

Published: 29 March 2017

Abstract

All-inorganic perovskites have been recognized as promising photovoltaic materials. We simulated the perovskite material of TlPbI3 using ab initio electronic structure calculations. The band gap of 1.33 eV is extremely close to the theoretical optimum value. Compared TlPbI3 with CsPbI3, the total energy (−3980 eV) of the former is much lower than the latter. The partial density of states (PDOS) of TlPbI3 shows that a strong bond exists between Tl and I, resulting in the lower total energy and more stable existence than CsPbI3.

Keywords

All-inorganic perovskite TlPbI3 CsPbI3 First principles

Background

Hybrid organic–inorganic halide perovskites ABX3 (A is an organic cation, B is Pb or Sn, and X is a halide) have been widely used as solar cells and attracted enormous interest due to the low-cost and simple solution process for extensive production in the field of photovoltaic (PV) applications. The rapid rise of hybrid organic–inorganic perovskite solar cells has seen photoelectric conversion efficiencies rise from 3.8% [1] to 21.1% [2] in less than 6 years, although the fact that the perovskite absorber layers are subject to degradation because of heat and humidity. To overcome these issues, numerous investigations on enhancing the efficiency [3, 4] and long-term stability [5, 6] have been performed for years [712], and now, the perovskite with all-inorganic structure is a primary focus [13]. For solar cells, an appropriate band gap will give a satisfactory efficiency. And the band gap should be narrow enough to absorb a broad solar spectrum from near infrared to visible light. The open-circuit voltage Voc is always lower than the band gap energy because thermodynamic detailed balance requires the cell to be in equilibrium with its environment, which indicates that there is spontaneous light emission from the cell. Considering the two factors, the cubic cesium lead iodide (CsPbI3) is a promising candidate for PV devices. Reference [14] reported the maximum efficiency occurs for a semiconductor with a band gap of 1.34 eV and is 33.7%.

The outer electron configuration of the thallium atom is [Xe]4f145d106s26p1, which has two valence states of +1 and +3, +1 valence compounds are more stable than +3 [15]. In this paper, we simulated the perovskite material of TlPbI3 with a band gap of 1.33 eV using ab initio electronic structure calculations based on the Density Functional Theory (DFT), and the band gap is extremely closer to the theoretical optimum value than CsPbI3 (Figs. 1 and 2). Compared TlPbI3 with CsPbI3, the total energy (−3980 eV) of the former is much lower than the latter. The partial density of states (PDOS) of TlPbI3 shows that a strong bond exists between Tl and I, resulting in the lower total energy and more stable existence than CsPbI3. Besides, we calculated the carrier concentration and found both the two materials indicate similar carrier concentration ranged from −20 to 50 °C.
Fig. 1

ab The band structure and density of states of TlPbI3

Fig. 2

abThe band structure and density of states of CsPbI3

Methods

We employed ab initio electronic structure calculations with DFT and the generalized gradient approximation (GGA) [16] put forward by Perdew–Burke–Ernzerhof (PBE) [17]. We used plane-wave basis sets and pseudopotentials. Kohn and Hohenberg [18] suggested that the real density of electrons would lead to a quite tiny functional value. Thus, Shan and Kohn optimized and put forward the density functional theory again, namely Kohn–Sham equations (KS equation) [19]:
$$ \left[-\frac{1}{2}{\nabla}^2+{\nu}_{\mathrm{ext}}\left(\overrightarrow{r}\right)+{\nu}_{\mathrm{H}}\left(\overrightarrow{r}\right)+{\nu}_{\mathrm{xc}}\left(\overrightarrow{r}\right)\right]{\varphi}_i={\varepsilon}_i{\varphi}_i $$
(1)
Formula (1) represents the motion of the electrons in the molecular system. Where, \( {\nu}_{\mathrm{ext}}\left(\overrightarrow{r}\right)=-{\displaystyle \sum_{\alpha =1}^{\mathrm{N}}\frac{Z_{\alpha}}{\left|\overrightarrow{r}-\overrightarrow{r_{\alpha}}\right|}} \) is the interaction between electrons and atoms, namely external potential. \( {\nu}_{\mathrm{H}}\left(\overrightarrow{r}\right)={\displaystyle \int \frac{\rho \left({\overrightarrow{r}}^l\right)}{\left|\overrightarrow{r}-{\overrightarrow{r}}^l\right|} d{\overrightarrow{r}}^l} \) stands for the interaction potential between electrons. \( {\nu}_{\mathrm{xc}}\left(\overrightarrow{r}\right) \) is the functional differential of exchange-correlation energy. E xc. \( {\nu}_{\mathrm{xc}}\left(\overrightarrow{r}\right)=\frac{\delta {E}_{\mathrm{xc}}\left[\rho \left(\overrightarrow{r}\right)\right]}{\delta \rho \left(\overrightarrow{r}\right)} \) represents the exchange-correlation potential. The effective potential \( {v}_{\mathsf{eff}}={v}_{\mathrm{xtf}}+{v}_H+{v}_{\mathrm{xc}} \) is mainly determined by electron density, which can be obtained by KS equation. Obviously, the equation can be solved by self-consistent field equations (SCF) if we know the exchange-correlation energy E xc. After obtaining the self-consistent convergence charge density ρ 0, the ground-state energy of the system can be expressed as [20]:
$$ {E}_0={\displaystyle \sum_{i=1}^N{\varepsilon}_i}-\frac{1}{2}{\displaystyle \int {\displaystyle \int \frac{\rho_0\left(\overrightarrow{r}\right){\rho}_0\left({\overrightarrow{r}}^l\right)}{\left|\overrightarrow{r}-{\overrightarrow{r}}^l\right|} d\overrightarrow{r} d{\overrightarrow{r}}^l}}-{\displaystyle \int {v}_{\mathrm{xc}}\left(\overrightarrow{r}\right){\rho}_0\left(\overrightarrow{r}\right) d\overrightarrow{r}+{E}_{\mathrm{xc}}\left[{\rho}_0\left(\overrightarrow{r}\right)\right]} $$
(2)
ε i is the eigenvalue of Eq (1):
$$ {\varepsilon}_i=\left\langle {\varphi}_i\left|-\frac{1}{2}{\nabla}^2+{v}_{\mathsf{eff}}\right|{\varphi}_i\right\rangle $$
(3)

In theory, the KS equation derived from DFT should be accurate [21]. But in the specific case, as E xc is a function associated with the single electron density \( \rho \left(\overrightarrow{r}\right) \), it is necessary to find a function that can replace the single electron density. We can solve a set of φ i by taking v xc into the KS equation. Then a new v xc can be calculated with this φ i . Finally, we submit it into KS equation and solve. Repeat the iteration until a certain accuracy. The key problem is to find the appropriate exchange correlation energy E xc. In the case of different calculation methods of exchange correlation energy E xc, a series of DFT models have been reported [22]. The GGA method is more accurate because it has been combined with inhomogeneous electron gas to obtain \( {E}_x^{B88} \), \( {E}_x^{\mathrm{LYP}} \) and other parameters [23].

To calculate out carrier concentration, we must know the effective mass of electron, expressed by the following formula [18].
$$ {m}_e^{*}={\hslash}^2{\left[\frac{d^2 E}{d{ k}^2}\right]}^{-1} $$
(4)
As expressed in formula (4), effective mass of holes and electrons can be obtained by calculating the two derivatives of valence-band maximum and conduction-band bottom. Finally, the carrier concentration is obtained as follows:
$$ {n}_i=\left(2.510\times {10}^{19}\right){\left(\frac{m_n^{*}}{m_0}\cdot \frac{m_p^{*}}{m_0}\right)}^{\frac{3}{4}}{\left(\frac{T}{300}\right)}^{\frac{3}{2}}{e}^{\frac{-{E}_g}{2 T}} $$
(5)
\( \frac{m_n^{*}}{m_0} \) is the effective mass of electron, obtained by:
$$ \frac{m_n^{*}}{m_0}=\frac{{\left(\frac{6.626\times {10}^{-34}}{a\times {10}^{-10}}\right)}^2}{X_0\times 1.6\times {10}^{-19}\times 9.109\times {10}^{-31}} $$
(6)

of which, X 0 is the two derivatives of conduction-band bottom. a is the lattice constant. Instead of conduction-band bottom by valance-band maximum, the formula (6) is often applied to solve the effective mass of hole \( \frac{m_p^{*}}{m_0} \) [24].

The Brillouin zone was sampled with a 2 × 2 × 2 k-point set and built by 2 × 2 × 2 supercell. The simulated models using 6s24f145d10 and 5s24d105p6 as valence electrons for Tl and Cs, respectively, are carried out. Firstly, we use the ultrasoft pseudopotentials to optimize the Pm3m structures of both TlPbI3 and CsPbI3. Then, we calculate the equilibrium volume and proper values of the lattice constants. After optimizing the crystalline structure, we calculate the total energy, band structure, density of states, and carrier concentration for two kinds of materials in the last.

Results and Discussion

Optimizing the geometry of TlPbI3 and CsPbI3, we have simulated that the lattice constants are 6.2621 Å and 6.3225 Å, respectively. The bond distances and bond angels calculated are presented in Table 1.
Table 1

The bond distances and bond angels of TlPbI3 and CsPbI3

 

X = Tl

X = Cs

X-Pb

5.423 Å

5.475 Å

X-I

4.428 Å

4.471 Å

Pb-I

3.131 Å

3.161 Å

X-Pb-I

54.736I

54.736I

The total energies of TlPbI3 and CsPbI3 are −3979.94 − 3154.36 eV independently. The lower total energy means the better stability. Thus, a conclusion that TlPbI3 has better stability than CsPbI3 is summarized theoretically.

The band gap of both semiconductors are calculated out 1.763 and 1.331 eV, respectively. The absorption spectrum of CsPbI3 measured by the experiment (Fig. 3a) shows the optical band gap is 1.73 eV, which is close to the simulated value. And the absorption decreases above the wavelength of ~716 nm. The outcomes further indicate that the model we simulated are correct. Both of their Fermi levels are extremely close to the valence-band maximum, meaning that they are p-type semiconductors. The band gap of TlPbI3 is quite close to the perfect semiconductor reported in reference [14]. If we can fabricate the solar cells with this material, a high efficiency will be obtained. However, the devices based on TlPbI3 are limited to simulate because of the toxicity.
Fig. 3

a is the absorption spectrum of CsPbI3 measured by experiment. b is the structures of valence-band maximum and conduction-band minimum of TlPbI3 and CsPbI3

Here, we select the valence-band maximum and conduction-band minimum for further analysis. As shown in Fig. 3b, the curvature of energy band in TlPbI3 is less than that in CsPbI3. The conduction band of TlPbI3 is relatively smooth and conducive to receive electron from valence band, enhancing the existence of carries.

According to the molecular orbital theory [25], the corresponding to the bond or anti-bond orbitals are formed by the more gentle part of the band curve. As shown in Figs. 1 and 2, if the peak of DOS curve is quite sharp, the corresponding energy-band curve is smooth; if the peak of DOS curve is relatively flat, the energy-band curve is relatively curved. So it can be deduced that the molecular orbitals are consistent with the peaks of the DOS graph. The peak height in the PDOS diagram (shown in Fig. 4) reflects the number of electrons contributing to this peak. If the PDOS of two different atoms has the resonance peaks in the range of same energy, it means the two atoms have already bonded. However, it cannot be determined that whether the band or anti-band are formed by analyzing the PDOS without further experiments. When the existence of resonance peaks are caused by the interaction of several atoms, we cannot distinguish that the bonds are formed by the two specific atoms. The conclusion does not affect our analysis.
Fig. 4

ac are the partial density of states (PDOS) in CsPbI3. df are the partial density of states (PDOS) in TlPbI3

As illustrated in Fig. 4a–c, the conduction-band minimum of CsPbI3 is mainly composed by 6p state of Pb, and the valence-band maximum is contributed by 5p states of I. In Fig. 4d–f, the bottom of the conduction band of TlPbI3 is mainly composed by both 6p states of Tl and 6p states of Pb, and the top of the valence band is contributed by 5p states of I. As presented in Fig. 4d–f, Tl and I have a strong resonance peaks between −12 and −10 eV, resulting in a deep level state. It also explains why TlPbI3 is more stable than CsPbI3.

Finally, carrier concentration are calculated by formulas (5) and (6). The relationship between temperature and carrier concentrations of both TlPbI3 and CsPbI3 is shown in Fig. 5. The carrier concentration of TlPbI3 is slightly less than that of CsPbI3 because the electronegativity of Tl (2.04) atom is larger than that of Cs (0.79) atom [26]. A larger electronegativity leads to a larger ionic bond component and stronger polarity, enhancing the attraction between electrons.
Fig. 5

The relationship between temperature and carrier concentration

Conclusions

We simulated the perovskite material of TlPbI3 with a band gap of 1.33 eV using ab initio electronic structure calculations and the band gap is extremely close to the theoretical optimum value. Compared TlPbI3 with CsPbI3, the total energy (−3980 eV) of the former is much lower than the latter. The partial density of states (PDOS) of TlPbI3 shows that a strong bond exists between Tl and I, resulting in the lower total energy and more stable than CsPbI3. Besides, we calculated the carrier concentration and found both the two materials have similar carrier concentration ranged from −20 to 50 °C.

Declarations

Acknowledgements

This work was supported by the National Natural Science Foundation of China under grant nos. 61421002, 61574029, and 61371046. This work was also partially supported by the University of Kentucky.

Authors’ Contributions

ZL designed and carried out the simulations. ZL and TZ participated in the work to analyze the data and prepared the manuscript initially. YW, CW, PZ, HS, ZC, and SL gave equipment support. All authors read and approved the final manuscript.

Competing Interests

The authors declare that they have no competing interests.

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Authors’ Affiliations

(1)
State Key Laboratory of Electronic Thin Films and Integrated Devices, School of Optoelectronic Information, University of Electronic Science and Technology of China (UESTC)
(2)
Department of Electrical & Computer Engineering and Center for Nanoscale Science and Engineering, University of Kentucky

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