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Thermodynamically, CuO is the only stable phase of copper oxide in air at RT, as the Cu-O phase stability diagram reveals21-23. To verify the presence of CuO on the surface of Cu2O, absorption spectra of the etched and unetched thermally oxidized Cu2O substrates were taken with photothermal deflection spectroscopy (PDS) — a highly sensitive technique which allows for sub-band gap absorption measurement24 (Figure 4). Both spectra showed absorption above 1.4 eV, which coincides with the band gap of CuO, before saturating at 2 eV (Cu2O band gap). The unetched substrate had a higher absorption below 2 eV, suggesting a thicker layer of CuO on the surface of unetched Cu2O than on the etched substrate. The inset in Figure 4 shows a grey layer of CuO on the as-oxidized (unetched) Cu2O substrate. While no grey film could be detected visually on the etched substrate, some CuO was still present on its surface, as the PDS measurements suggests. The presence of a very thin CuO film on the surface of Cu2O substrates was also confirmed with x-ray photoelectron spectroscopy (XPS)19,25. Cupric oxide present on the Cu2O surface introduces deep level trap states (Cu2+)18 at the heterojunction interface that can act as recombination centers and, therefore, CuO presence at the p-n junction is undesirable.
Heating Cu2O substrates in the presence of oxidants (e.g., air and moisture) facilitates the oxidation of Cu2O to CuO. In order to obtain polycrystalline ZnO by AP-SALD, the substrates are heated to 150 °C. As the substrate is held at elevated temperature in open-air or under the oxidant gas during the deposition, CuO quickly forms on the Cu2O surface. Figure 5 shows scanning electron microscopy (SEM) images of an etched Cu2O substrate before and after spending 3 min on the AP-SALD platen at 150 °C under the flow of nitrogen. Multiple CuO outgrowths can be seen on the annealed substrate, with their composition being close to that of CuO as verified by energy-dispersive X-ray spectroscopy (EDX).
Photovoltaic devices were made with ZnO deposited by AP-SALD at 150 °C for 400 sec on top of the etched thermally oxidized Cu2O substrates. Figure 6A shows the surface of this standard device. One can notice numerous rod- and flower-like outgrowths present in the device. As confirmed earlier with EDX and PDS, these outgrowths are cupric oxide and occur due to Cu2O exposure to air and oxidants. Table 1 and Figure 7 ('ZnO/Cu2O standard' curve) demonstrate the relatively poor performance of this device.
In order to avoid CuO formation on the Cu2O surface, the conditions for depositing ZnO by AP-SALD on the etched thermally oxidized Cu2O substrates were optimized. The following measures were taken in order to minimize CuO growth: reduction of deposition temperature (Figure 8A); reduction of deposition time (Figure 8B); scanning the substrate surface for a few oscillations without exposure to the oxidant gas, i.e., with only metal precursors and inert channels open (Figure 8C); and finally, avoidance of unnecessary heating of naked Cu2O substrates in air just before the start of deposition. The optimal parameters of ZnO deposition on Cu2O were found to be 100 °C, 100 sec and 5 water-free cycles. The surface of the optimized device was free of CuO outgrowths, as is demonstrated in Figure 6B. The current density–voltage (J-V) characteristic of the optimized ZnO/Cu2O device is compared with the standard device in Figure 7. The photovoltaic performance of both standard and optimized ZnO/Cu2O devices is presented in Table 1. It can be seen that by following the four above-mentioned measures, a six-fold increase in power conversion efficiency of the devices was achieved.
To further elucidate the effect of optimization of AP-SALD conditions on the reduction of CuO and the heterojunction quality, external quantum efficiency (EQE) measurements were performed on devices with ZnO deposited at 150 °C and 100 °C (Figure 9). The EQE spectra of the two devices, while similar at wavelengths above 475 nm, differed significantly at wavelengths below 475 nm, which is the range of wavelengths absorbed close to the interface. For the shorter wavelength radiation, the EQE of the device with ZnO made at higher temperature was less than half that of the device with ZnO made at lower temperature. This suggests that more cupric oxide was present at the ZnO/Cu2O interface made at higher temperature, which reduced charge collection from the region close to the heterointerface due to increased recombination.
Mg was incorporated into AP-SALD ZnO films in order to raise the conduction band of ZnO and to reduce recombination further15. Zn1-xMgxO/Cu2O solar cells were made with the optimized Zn0.8Mg0.2O films, resulting in 2.2% device PCE — the highest to date for Cu2O-based solar cells with open-air fabricated heterojunctions (see the device performance in Figure 7 and Table 1).

Figure 1. Cu2O-based solar cell efficiency by year of publication (This figure has been modified from Ref.8). Markers indicate whether the interface was formed in vacuum or in atmosphere (non-vacuum) and labels indicate the method of heterojunction formation. MSP - magnetron sputtering, IBS - ion beam sputtering, VAPE - vacuum arc plasma evaporation. Please click here to view a larger version of this figure.

Figure 2. Schematic of AP-SALD deposition process (compared with conventional ALD) and set-up for producing multicomponent metal oxides. (A) Sequential exposure of each precursor and purge step in conventional ALD (delta-doping) (This figure has been reproduced from Ref. 11). In the context of this manuscript, M1 is diethylzinc vapor, M2 bis(ethylcyclopentadienyl)magnesium vapor, and O1 and O2 water vapor. (B) Sequential exposure of metal precursor mixture (co-injection), inert gas channels (equivalent to 'purge' step) and oxidant in AP-SALD (This figure has been reproduced from Ref. 11). (C) Schematic of a general AP-SALD reactor, showing the precursors spatially separated by inert gas channels, with the substrate oscillated beneath the different channels (This figure has been reproduced from Ref.11, which is a modification from one in Ref.26). (D) Overview schematic of the important components of an AP-SALD system with atomic force microscopy (AFM) images showing the morphology of the substrate before and after Zn1-xMgxO deposition (This figure has been reproduced from Ref. 13). Please click here to view a larger version of this figure.

Figure 3. Cross-sectional SEM image of ITO/ZnO/Cu2O heterojunction (This figure has been reproduced from Ref.8). Conformal coating of Cu2O substrate with ZnO and ITO films can be observed. Please click here to view a larger version of this figure.

Figure 4. PDS spectra of etched and unetched (as-oxidized) Cu2O substrates (This figure has been modified from Ref.8). The insets show photographs of the etched and unetched cuprous oxide substrates. Please click here to view a larger version of this figure.

Figure 5. SEM images of the surface of a Cu2O substrate when (A) freshly etched and (B) after annealing at 150 °C in air for 3 min (This figure has been reproduced from Ref.8). Insets show surface composition acquired with EDX. Please click here to view a larger version of this figure.

Figure 6. SEM images of the surface of ZnO/Cu2O solar cells made using (A) standard conditions and (B) optimized conditions of AP-SALD ZnO (This figure has been reproduced from Ref.8). Various outgrowths can be seen in the standard device. Please click here to view a larger version of this figure.

Figure 7. Light J-V characteristics for Zn1-xMgxO/Cu2O solar cells fabricated at standard and optimized AP-SALD conditions (This figure has been modified from Ref.8). The J-V curves demonstrate solar cell performance improvement when the composition and AP-SALD conditions of the Zn1-xMgxO films are optimized. Please click here to view a larger version of this figure.

Figure 8. The effect of AP-SALD parameters on the performance of ZnO/Cu2O solar cells. (A) and (B) The effect of AP-SALD ZnO deposition time and temperature on the open-circuit voltage (Voc) of the devices (This figure has been reproduced from Ref.8), (C) correlation of water-free cycles with the Voc of the devices. Please click here to view a larger version of this figure.

Figure 9. EQE spectra of ZnO/Cu2O solar cells with ZnO deposited at 100 °C and 150 °C. (This figure has been reproduced from Ref.8). Open-circuit voltage of the devices is indicated in the legend. Please click here to view a larger version of this figure.
| Solar cell | Deposition temperature, °C | Deposition time, sec | Jsc, mA/cm2 | Voc, V | FF, % | PCE, % |
| ZnO/Cu2O Standard | 150 | 400 | 3.7 | 0.18 | 35 | 0.23 |
| ZnO/Cu2O Optimized | 100 | 100 | 7.5 | 0.49 | 40 | 1.46 |
| Zn0.8Mg0.2/Cu2O Optimized | 150 | 100 | 6.9 | 0.65 | 49 | 2.20 |
Table 1. Standard and optimized AP-SALD Zn1-xMgxO deposition parameters and performance of the best corresponding ITO/Zn1-xMgxO/Cu2O solar cells (This table has been modified from Ref.8). JSC- short circuit current density, FF - fill factor.