Efficiently photo-charging lithium-ion battery by perovskite solar cell

Abstract

Electric vehicles using lithium-ion battery pack(s) for propulsion have recently attracted a great deal of interest. The large-scale practical application of battery electric vehicles may not be realized unless lithium-ion batteries with self-charging suppliers will be developed. Solar cells offer an attractive option for directly photo-charging lithium-ion batteries. Here we demonstrate the use of perovskite solar cell packs with four single CH₃ NH₃ PbI₃ based solar cells connected in series for directly photo-charging lithium-ion batteries assembled with a LiFePO₄ cathode and a Li₄ Ti₅ O₁₂ anode. Our device shows a high overall photo-electric conversion and storage efficiency of 7.80% and excellent cycling stability, which outperforms other reported lithium-ion batteries, lithium-air batteries, flow batteries and super-capacitors integrated with a photo-charging component. The newly developed self-chargeable units based on integrated perovskite solar cells and lithium-ion batteries hold promise for various potential applications.

ARTICLE

Received 20 May 2015 | Accepted 17 Jul 2015 | Published 27 Aug 2015

Electric vehicles using lithium-ion battery pack(s) for propulsion have recently attracted a great deal of interest. The large-scale practical application of battery electric vehicles may not be realized unless lithium-ion batteries with self-charging suppliers will be developed. Solar cells offer an attractive option for directly photo-charging lithium-ion batteries. Here we demonstrate the use of perovskite solar cell packs with four single CH3NH3PbI3 based solar cells connected in series for directly photo-charging lithium-ion batteries assembled with a

LiFePO4 cathode and a Li4Ti5O12 anode. Our device shows a high overall photo-electric conversion and storage efciency of 7.80% and excellent cycling stability, which outperforms other reported lithium-ion batteries, lithiumair batteries, ow batteries and super-capacitors integrated with a photo-charging component. The newly developed self-chargeable units based on integrated perovskite solar cells and lithium-ion batteries hold promise for various potential applications.

DOI: 10.1038/ncomms9103 OPEN

Efciently photo-charging lithium-ion battery by perovskite solar cell

Jiantie Xu1,*, Yonghua Chen1,* & Liming Dai1

1 Center of Advanced Science and Engineering for Carbon (Case4Carbon), Department of Macromolecular Science and Engineering, Case Western Reserve University, Cleveland, Ohio 44106, USA. * These authors contributed equally to this work. Correspondence and requests for materials should be addressed toL.D. (email: mailto:[email protected]

Web End [email protected] ).

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The importance of developing new types of energy conversion and storage systems is evident by the ever-increasing human reliance on energy-based

appliances, the rapidly diminishing fossil fuels and the continuously growing environmental concerns. The global energy consumption by automobiles, along with the associated greenhouse-gas emission, has been accelerating at an alarming rate due to the rapid increase in world population and economic expansion worldwide. Unlike traditional vehicles relying heavily on the fossil fuels, electric vehicles or plug-in hybrid electric vehicles hold great promise to solve current energy and environmental challenges. With recent advance in the development of eco-friendly rechargeable lithium-ion batteries (LIBs) of higher power and energy densities1, battery electric vehicles (BEVs) using LIB pack(s) for propulsion have attracted a great deal of interest2. Of particular interest, Tesla has recently demonstrated the use of a battery pack consisting of 7,000 cylindrical LIB cells (each with 18 mm in diameter 65 mm in

length) connected in series and parallel to power electric vehicles (http://www.cadex.com/en/batteries/safety-of-lithium-ion-batteries

Web End =http://www.cadex.com/en/batteries/safety-of-lithium-ion- http://www.cadex.com/en/batteries/safety-of-lithium-ion-batteries

Web End =batteries ), opening a new era of transportation with BEVs3. Although the excellent electrochemical performance of LIBs, including their high specic capacity, power and energy density, and rate capability, could ensure a long cruise duration, short charging time and low total cost of a BEV, implementing the BEV technology in our daily life is still a big challenge as it requires a cross-country network of BEV-charging stations. This will not only cause inexibilities to travel plans but also inevitably increase the total cost of the BEV technology. Therefore, the large-scale practical application of BEVs cannot be realized unless LIBs with self-charging suppliers will be achieved.

The solar cell technology that can generate electricity from the sunlight4,5, could offer a viable approach to self-charging of LIBs wherever needed. With the free and abundant sunlight that provides about 10,000 times more energy to the Earth than we consume, solar cells can ensure sustainable access to electrical power for charging LIBs anywhere around the world with no air pollution, hazardous waste or noise, and they requires little upkeep. If solar cells can be used for directly photo-charging LIBs, therefore, the BEV technology could be marketed for large-scale applications even without the presence of a cross-country network of charging stations. Although conceptually promising, photo-charging of batteries, including LIBs, with solar cells has been much less discussed than photo-charging super-capacitors and is far from practical so far (Supplementary Table 1)623. This is because all the limited number of the photo-charging LIB devices reported to date exhibited a very low overall photo-electric storage-conversion efciency and poor cycling stability (Supplementary Table 1).

One of the critical issues needs to be addressed for efcient photo-charging of LIBs is to enhance the usually low current density and power-conversion efciency associated with most current solar cells, particularly polymer solar cells. In this regard, the recent availability of high-performance perovskite solar cells (PSCs)5,2431 could not only facilitate the development of highly efcient (up to B20%) and low cost solar cells for practical applications but also allow for the integration of PSCs into various energy systems. Herein, we report the rst use of PSC packs with four single CH3NH3PbI3 PSCs connected in series for directly photo-charging LIBs assembled with a LiFePO4 cathode and a Li4Ti5O12 anode. The fabricated PSCLIB units were shown to possess a high overall photo-electric conversion and storage efciency of 7.80% and excellent cycling stabilityoutperformed all other reported LIBs, lithiumair batteries, ow batteries and super-capacitors integrated with a photo-charging component. This work clearly indicates that the PSCLIB units developed in

this study hold great promise for potential applications as self-chargeable batteries to power the BEVs and various portable electronics.

ResultsWorking mechanism of a PSCsLIB unit. Figure 1 schematically shows the fabricated system for photo-charging a LIB by PSCs connected in series. As shown in Fig. 1, the photogenerated free holes and electrons within the PSCs ow into the cathode and anode of the LIB, respectively. This current ow from the PSC to the close circuited LIB (top, Fig. 1) leads to charging the LIB through oxidative extraction of lithium ions from the cathode (for example, olive structure LiFePO4), followed by reductive insertion onto the anode (for example, spinel structure Li4Ti5O12). The energy (charge) stored during the charging process can be released to external loading (bottom, Fig. 1) by turning S1 off and S2 on, which is accompanied by a simultaneous back ow of lithium ions from the anode to cathode.

Fabrication and performance of PSCs. To construct the PSCsLIB system shown in Fig. 1, we rst fabricated PSCs with a device structure of ITO (indium tin oxide)/poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) (40 nm)/ CH3NH3PbI3 (perovskite) (375 nm)/[6,6]-phenyl-C61-butyric acid methyl ester (PC61BM) (100 nm)/Ca (20 nm)/Al (100 nm). Supplementary Fig. 1 schematically shows structures of the perovskite material and solar cell device while their characterization and fabrication details can be found in Supplementary Note 1 and Supplementary Methods. The CH3NH3PbI3 perovskite layer was prepared according to our previously reported layer-by-layer process29. Briey, we rst thermally evaporated a thin (125 nm) layer of lead iodide (PbI2) onto a PEDOT:PSS layer pre-coated on an ITO/glass substrate (Supplementary Fig. 1). Subsequently, we dipped the PbI2 into a solution of CH3NH3I in 2-propanol (10 mg ml 1) to transfer it into a layer of CH3NH3PbI3 perovskite.

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Figure 1 | Photo-charging a LIB by PSCs. Schematic diagram of the fabricated system of PSCLIB.

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Similarly, a second PbI2 layer (125 nm) was thermally evaporated onto the newly formed CH3NH3PbI3 perovskite lm, followed by dipping into the CH3NH3I solution to form the second layer of CH3NH3PbI3 perovskite intimately contacted with the underlying pre-formed CH3NH3PbI3 perovskite layer. The above process was repeated three times to form an interface-free uniform CH3NH3PbI3 perovskite layer of a desirable total thickness for outstanding photovoltaic performance required for photo-charging LIBs. The individual layer thickness of PbI2 was optimized at 125 nm as a thinner layer PbI2 (o125 nm) cannot ensure pinhole free, whereas a thicker PbI2 (4125 nm) cannot be totally transformed into CH3NH3PbI3 perovskite (Supplementary Fig. 2a). A typical scanning electron microscopy image for the resultant CH3NH3PbI3 perovskite lm is given in Supplementary

Fig. 2b, which shows a uniform, pinhole-free morphology. Supplementary Fig. 2c shows a typical X-ray diffraction pattern with peaks at 13.68, 24.01, 28.04 and 42.80 characteristic of the (110), (202), (220) and (330) diffractions, respectively, from the tetragonal CH3NH3PbI3 perovskite, indicating a complete transformation of the three-layered PbI2 with a total thickness of 375 nm into the CH3NH3PbI3 perovskite lm. Further evidence for the complete conversion of the PbI2 layer into the CH3NH3PbI3 perovskite lm came from the optical absorption spectrum given in Supplementary Fig. 2d, which shows a broad band with an onset

at 770 nm characteristic of the CH3NH3PbI3 perovskite. The chemical composition of the CH3NH3PbI3 perovskite lm was measured by X-ray photoelectron spectroscopy (XPS). Supplementary Fig. 3a shows an XPS survey spectrum while Supplementary Fig. 3be reproduce the high-resolution XPS spectra of C 1s, I 3d, Pb 4f and N 1s, respectively. Numerical data from the XPS measurements are listed in Supplementary Table 2. As expected, the atomic ratio of I/Pb was found to be 2.85, which is close to the stoichiometric value of 3.

Before the system integration, we have further investigated the PSC performance. Figure 2a,b show typical current densityvoltage (JV) characteristics for a single PSC and four of them connected in series, respectively. For the single PSC, a short-circuit photocurrent density of 22.85 mA cm 2, open-circuit voltage of0.96 V, ll factor of 0.71 and power-conversion efciency (PCE; Z1,

Method calculation 1) of 15.67% were obtained. The short-circuit current density matched well with the current density of21.93 mA cm 2 calculated from the incident photon-to-current efciency (IPCE) spectrum (Supplementary Fig. 4). To ensure a sufciently high operating voltage for directly photo-charging LIBs, we then fabricated a PSC pack by connecting four single cells in series (top, Fig. 1). The detailed Jc, Voc, FF and Z1 of these four single cells were shown in Supplementary Figs 5a and 6. As a result, we obtained a short-circuit photocurrent density of

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Figure 2 | Performance of PSCs and LIBs. (a) JV curve for single PSC. (b) A typical JV curve for the connected PSCs unit with four single PSCs connected in series. (c) Rate capabilities of LFPOLi, LTOLi and LFPOLTO cells measured at various C-rates (1 C 170 mA g 1) in the voltage ranges of 2.54.0,

1.03.0 and 1.02.6 V, respectively. (df) Typical chargedischarge curves of (d) LFPOLi, (e) LTOLi and (f) LFPOLTO cells.

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4.82 mA cm 2 (per the total area of four PSCs), open-circuit voltage of 3.84 V, ll factor of 0.68 and PCE of 12.65% for the connected PSC unit (Fig. 2b). While the connected PSC unit exhibited sufciently good performance with a high open-circuit voltage (3.84 V) for photo-charging LIBs, its long-term operation stability was tested, along with the corresponding single cells, to be superb even up to 720 h (in Ar atmosphere).

Fabrication and electrochemical performance of LIBs. Owing to their high energy density, excellent thermal and chemical stability, long cycling life and superior safety, LiFePO4 (LFPO)

and Li4Ti5O12 (LTO) have been widely regarded as promising cathode and anode materials, respectively, for the next generation of high-energy LIBs attractive for BEVs1,32,33. In this regard, we have fabricated a full LIB cell based on LiFePO41M LiFP6 in ethylene carbonate/dimethyl carbonate/diethyl carbonate (v/v/v: 1:1:1)Li4Ti5O12 with a working voltage range of 1.02.6 V (Methods). The structure and morphology of the LFPO and LTO electrodes were conrmed by X-ray diffraction measurements (Supplementary Fig. 7a,b) and scanning electron microscopy images (Supplementary Fig. 7c,d). The electrochemical performance of a LFPOLi or LTOLi half cell (lithium foil as a counter and reference electrode) and a full cell of LFPOLTO (with a LFPO/LTO mass ratio of B1.1) was given in Fig. 2cf.

Specically, Fig. 2c shows the rate capability of the LFPO and LTO electrodes with respect to a full LFPOLTO cell at the same C-rates. As can be seen, the LFPO and LTO electrodes exhibited

initial charge/discharge capacities of 159.1/152.5 and 152.8/ 158.6 mAh g 1 at 0.2 C (1 C 170 mA g 1), and 151.2/150.1

and 139.4/147.5 mAh g 1 at 0.5 C, respectively. Figure 2d,e show typical chargedischarge proles for the LFPOLi and LTOLi half cells, respectively, at various C-rates, showing the at voltage proles without signicant over-potential at the C-rate r0.5 C.

Similar at dischargecharge proles were observed for the LFPOLTO cell. As shown in Fig. 2c,f, the LFPOLTO cell exhibited a good cycling stability over a wide range of C-rates from 0.2 to 2 C with average charge/discharge capacities of 145.3/144.3 mAh g 1 at 0.2 C and 135.7/

135.1 mAh g 1 at 0.5 C.

Performance of PSCsLIB device. Having carried out systematic performance evaluations for both the PSCs and LFPO/LTO-based LIBs, we used the PSC unit with four single PSCs connected in series to directly photo-charge a LFPOLTO LIB at an current density of 0.5 C (0.085 mA g 1, 1 C 170 mA g 1), which

matches well with the photogenerated current density from the PSC unit over the voltage range of 2.02.5 V(4.614.52 mA cm 2 and 0.0870.085 mA g 1, Fig. 2b). Figure 3a shows photo-charge (blue lines) and galvanostatic discharge (black lines) curves of a LIB repeatedly photo-charged by the connected PSC unit (PSCsLIB) for 10 cycles at 0.5 C between 1.0 and 2.6 V. To compare with the photo-charging, we also performed galvanostatic chargedischarge of the same LIB cell, using an automatic battery tester system (Land, China) as

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Figure 3 | Performance of fabricated PSCsLIB and PS-LIB. (a) Voltagetime (Vt) curves of the PSCsLIB device (blue and black lines at the 1st10th cycles: charged at 0.5 C using PSC and galvanostatically discharged at 0.5 C using power supply. Red and black lines at the 11th15th cycles: both galvanostatically charged and discharged at 0.5 C using power supply). (b) JV curves, (c) Voc and Jc, (d) ll factor (FF) and solar-to-electric PCE (Z1) of the connected PSCs before and after various cycles. (e) Discharge capacity (Note, a slight variation was observed for the discharge duration at different cycle numbers), (f) overall photo-electric conversion efciency of the PSCsLIB device (Z2) and (g) energy storage (conversion) efciency (Z3) of LIB, as a function of the cycle number.

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power supply (PS) after the completion of the 10 photo-charge/ galvanostatic discharge cycles (PS-LIB, red lines in Fig. 3a). As shown in Fig. 3a, the PSCsLIB and PS-LIB cells showed almost identical very stable dischargecharge curves over all the cycles, indicating excellent capabilities of the PSCs for photo-charging LIBs. Even after continued illumination under AM1.5G for 17.8 h over 10 repeated photo-charge and galvanostatic discharge cycles (Supplementary Fig. 8), the connected PSC unit showed only slight changes in all the photovoltaic characteristics, including Jc,

Voc and FF, with a small decrease in PCE (Z1) from 12.65 to11.16% (Fig. 3bd, Supplementary Table 3), corresponding to an average of 0.15% per cycle decay in Z1. The above observed operation stability was also conrmed by the high Z1 retention (B93%) obtained for single (Supplementary Fig. 9ac) and connected PSCs out of the photo-charging system (Fig. 1, Supplementary Fig. 9df) even after 720 h testing in an Ar-lled glove box without any encapsulation protection. As seen in Fig. 3e (blue dots), the fabricated PSCsLIB cell delivered an initial reversible capacity of 140.4 mAh g 1 while maintained a reversible capacity of 111.6 mAh g 1 after 10 photo-charge and galvanostatic discharge cycles (that is, 79.49% initial capacity,

B2.05% decay per cycle). This was followed by a highly reversible capacity of 111.1 mAh g 1 during the PS-LIB process up to the 15th galvanostatic chargedischarge cycle (Fig. 3e, red dots).

In comparison, the galvanostatic chargedischarge cycles measured for fresh LFPOLi, LTOLi and LFPOLTO cells at0.5 C in the voltage ranges of 2.54.0, 1.03.0 and 1.02.6 V, respectively, for 30 cycles, using the automatic battery tester system as power supply (that is, PS), were given in Fig. 4. As expected, the fresh LFPOLTO cell (Fig. 4a) using PS showed the similar chargedischarge Vt curves to that of (PSCs and PS)-LIB (Fig. 3a). As shown in Fig. 4b, the fresh cell delivered the initial, 11th, 15th and 30th reversible capacities of 141.6, 117.5, 115.5 and 115.2 mAh g 1, corresponding to an average capacity decay of1.70% at the 10th cycle, 1.85% at the 15th cycle and 1.88% at the 30th cycle, during the galvanostatic charge and discharge cycles. As shown in Fig. 4b, the cycling stability of LFPOLTO cell was signicantly improved after initial few cycles due to the enhanced compatibility between the electrode and electrolyte. Along with the almost identical electrochemical behaviour (Fig. 4a), the close discharge capacity and average capacity decay observed for both

the PS-LIB and PSCsLIB indicate, once again, the excellent photo-charging capability of the PSCs and high cycling stability of the LFPOLTO LIBs.

To gain insights into the power-conversion and storage efciencies, we calculated the overall photo-electric conversion efciency of the fabricated PSCsLIB system (Z2) by dividing the discharge energy of the LFPLTO cell shown in Fig. 1 by the illumination energy (Method calculation 2). Figure 3f (blue dots) shows a rather stable Z2 for the PSCsLIB system during the 10 photo-charge and galvanostatic discharge cycles at 0.5 C, with a maximum Z2 of 7.36% and an average Z2 of 6.97%

(Supplementary Table 4). Owing to a low potential polarization between the charge and discharge voltage plateaus at lower C-rates (cf. Fig. 2f), the PSCsLIB exhibited an increased Z2 with decreasing C-rate: 7.80% at 0.1 C, 7.35% at 0.25 C, 6.87% at 0.5 C,6.47% at 0.75 C and 6.11% at 1 C (Supplementary Table 5). To our best knowledge, the overall 7.80% photo-electric conversion efciency (Z2) for the PSCsLIB unit outperformed all other reported LIBs7, lithiumair batteries20, ow batteries11,14 and super-capacitors10,19,23 integrated with a photo-charging component, such as a solar cell (Supplementary Table 1). Furthermore, the energy storage efciency (Z3) of the LIB in the PSCsLIB was calculated by Z2/Z1 (that is, Method calculation 3, blue dots in Fig. 3g) to beB60% while Z3 for the LIB in the PSLIB was calculated to be B66% (Method calculation 4, red dots in Fig. 3g). The single fresh LFPOLTO LIB showed a Z3 of

B71% and an average Coulombic efciency of B99.5% (Fig. 4c). Clearly, therefore, the newly developed PSCsLIB system possesses the highest Z1, Z2 and Z3 among all reported photo-chargeable energy devices, including batteries and capacitors (Supplementary Table 1), holding great promise as a self-chargable power supplier for BEVs and many other optoelectronic systems.

DiscussionAs can be seen from above, the solar cell technology offers a viable option to self-charge LIBs for potentially marketing the BEV technology for large-scale applications. However, all the photo-charging LIB devices reported to date exhibited a very low overall photo-electric storage-conversion efciency and poor

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Figure 4 | Cycling performance of the LTO, LFPO and LFPOLTO. (a) Vt curves of a fresh LFPOLTO cell measured at 0.5 C in the voltage range of1.02.6 V for 15 cycles. (b) Cycling performance of LTO, LFPO and LFPOLTO cells measured at 0.5 C in the voltage ranges of 1.03.0, 2.54.0 and 1.02.6 V, respectively, for 30 cycles. (c) Conversion efciency (Z3) and Coulombic efciency of LFPOLTO for 30 cycles.

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cycling stability (Supplementary Table 1). We have, for the rst time, demonstrated the use of PSC packs for directly photo-charging LIBs. The solar cell pack with four single CH3NH3PbI3

PSCs connected in series showed an outstanding solar-to-electric PCE of 12.65% (15.67% for the single cell), while the full LIB cell assembled with the LiFePO4 cathode and Li4Ti5O12 anode exhibited a high specic capacity and rate capability. The fabricated PSCsLIB units were demonstrated to possess a high photo-electric conversion and storage efciency of 7.80% and excellent cycling stability under continued illumination with AM1.5G for 17.8 h. For practical applications, repeatable and reliable fabrication of the PSCsLIB units with good performance is another important issue needs to be addressed. Supplementary Figs 5b, 6 and 10 show a good repeatability for reliable fabrication of PSCs and integration of the resultant PSCs units for efcient photo-charging LIBs. In addition, an excellent discharge rate capability at various discharge rates was observed for the LFPOLTO cell in the PSCsLIB system (Supplementary Fig. 11). Both the photo-charged PSCsLIB and the PS-LIB cells, gavanostatically charged and discharged at 0.5 C, exhibited a similar rate capability from 0.1 to 1 C (Supplementary Fig. 12), further indicating a highly stable PSCsLIB system. To our best knowledge, the newly developed PSCsLIB units outperformed all other reported LIBs, lithiumair batteries, ow batteries and super-capacitors integrated with a photo-charging component (Supplementary Table 1). These excellent results clearly indicate that the PSCsLIB developed in this study hold great promise for potential applications as self-chargeable batteries to power the BEVs and various portable electronics.

Methods

Materila preparation. The commercial LiFePO4 cathode and Li4Ti5O12 anode materials were purchased from the MTI Corporation (USA). The PEDOT:PSS, PbI2 and PC61BM were purchased from Clevious, Sigma Aldrich and Nano-C, respectively. CH3NH3I was synthesized according to the reported procedures31.

PSCsLIB device assemble. The cathode (anode) was fabricated by blending LiFePO4, LFPO (Li4Ti5O12, LTO) with acetylene black carbon and polyvinylidene diuoride at a weight ratio of 90:5:5, respectively. N-methyl-2-pyrrolidone was used as the solvent. The slurries were stirred in a sealed glass bottle for 3 h. The resultant LiFePO4 and Li4Ti5O12 slurries were then coated on Al and Cu foils, respectively.

The LIBs were assembled as the CR 2032 coin-type cells in an Ar-lled glove box. The LFPOLi and LTOLi half-cells were assembled from LiFePO4 or Li4Ti5O12 with a mass loading of 1113 mg cm 2 as the working electrode, using Li foils as the counter electrode and reference electrode, porous polypropylene lm as separator and 1 M LiPF6 in a 1:1:1 (v/v/v) mixture of ethylene carbonate, dimethyl carbonate and diethyl carbonate as the electrolyte. The LFPOLTO full cell was assembled by using LFPO and LTO as the cathode and anode, respectively. The LFPOLi, LTOLi and LFPOLTO cells were measured using an automatic battery tester system (Land, China) as PS and photo-charged or galvanostatically charged and discharged at various current densities in the voltage ranges of 2.54.0, 1.03.0 and 1.02.6 V, respectively (1 C 170 mA g 1 for all three samples).

For the PSC construction, ITO glass substrates were cleaned sequentially with detergent, de-ionized water, acetone and iso-propanol, followed by drying with N2 ow and ultravioletozone treatment for 15 min. The PEDOT:PSS solution (Al4083 from H. C. Starck) was spin-cast onto ITO electrodes at 5,000 r.p.m. for 40 s. The PEDOT:PSS lm was annealed at 140 C for 10 min to remove residual water. The ITO/PEDOT:PSS substrate was then transferred to evaporator in an Ar-lled glove box for PbI2 evaporation (125 nm), followed by dipping the PbI2-deposited substrate into a solution of CH3NH3I in 2-propanol (10 mg ml 1) for 40 s to form the

CH3NH3PbI3 perovskite layer and being rinsed with 2-propanol for 10 s. Similarly, a second PbI2 layer was thermally evaporated onto the pre-formed rst layer of CH3NH3PbI3 perovskite lm, followed by dipping into the CH3NH3I solution to form the second layer of CH3NH3PbI3 perovskite, and the process was repeated for three times for a desired thickness. The CH3NH3PbI3 perovskite was then thermally annealed at 100 C for 10 min in the glove box to complete crystallization for the perovskite lm. After the thermal annealing, PC61BM in chlorobenzene solution (17 mg ml 1) was deposited onto the perovskite layer by spin coating at 1,000 r.p.m.

for 60 s. Finally, the device was transferred to the evaporator for thermal evaporation of Ca (20 nm) and Al (100 nm) at 10 7 torr. All the devices were tested in an

Ar-lled glove box using a Keithley 2400 source meter and a Newport Oriel sol 2A solar simulator (300 W). We used the 91150V Reference Cell and Meter (ORIEL instrument) to calibrate the light intensity to be 100 mW cm 2 before the device

testing. The device performance parameters were obtained from the currentvoltage curves of the solar cells under illumination. The IPCE was measured on a Solar Cell Measurement System from PV Measurement Inc. The PSCs (single PSC or four single PSCs connected in series) thus fabricted were kept in the glove box under high-purity Ar gas for further electrochemical measurements and long-time rest measurements. The PSCsLIB units were fabricated by integrating PSCs and a LIB into the system, as shown in Fig. 1.

Calculations. 1. The energy-conversion efciency of the PSC (Z1):

Z1 PSC

Jc FF Voc = P 100 % 1 where FF, Voc, Jc and P are ll factor, open-circuit voltage (V), short-circuit current density (mA cm 2) and incident light power density (100 mW cm 2), respectively.

2. The energy-conversion and storage efciencies for the entire PSCsLIB integrated unit:

Z2 PSCs LIB

Ed= P S t

100 % 2 where Ed, P, S and t are discharge energy of LIB (mWh, from Land machine), light power density (100 mWcm 2 ), effective area of PSCs in series (cm 2) and photo-charge time (h), respectively.

3. The energy storage efciency for PSC to photo-charge LIB:

Z3 PSCs LIB

Z2=Z1 100 % 3

4. The energy storage efciency for galvanostatically charging LIB with Land machine as power supply (PS-LIB):

Z3 PS LIB

Ed=Ec 100 % 4

where Ed and Ec are the discharge and charge energy (mWh), in which the LIB was galvanostatically charged using Land machine.

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Acknowledgements

We are grateful for nancial support from the National Science Foundation

(NSF-CMMI-1400274, DMR-1106160).

Author contributions

J.X. and L.D. conceived the concept and designed the experiments; J.X and Y.C.

fabricated the LIBs and PSCs, respectively, performed the materials characterization,

assembled the PSCsLIB and PS-LIB devices, carried out their electrochemical mea

surements and analysed the data; L.D. was responsible for planning and supervising the

project; J.X., Y.C. and L.D. co-wrote the paper and all authors discussed the results and

commented on the manuscript.

Additional information

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How to cite this article: Xu, J. et al. Efciently photo-charging lithium-ion

battery by perovskite solar cell. Nat. Commun. 6:8103 doi: 10.1038/ncomms9103

(2015).

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