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Electronics 2014, 3(1), 122-131; doi:10.3390/electronics3010122
Published: 6 March 2014
Abstract: Recently, MoO3, which is typically used as an anode buffer layer in organic photovoltaic cells (OPVCs), has also been used as a cathode buffer layer (CBL). Here, we check its efficiency as a CBL using a planar heterojunction based on the CuPc/C60 couple. The CBL is a bi-layer tris-(8-hydroxyquinoline) aluminum (Alq3)/MoO3. We show that the OPVC with MoO3 in its CBL almost immediately exhibits lower efficiency than those using Alq3 alone. Nevertheless, the OPVCs increase their efficiency during the first five to six days of air exposure. We explain this evolution of the efficiency of the OPVCs over time through the variation in the MoO3 work function due to air contamination. By comparison to a classical OPVC using a CBL containing only Alq3, if it is found that the initial efficiency of the latter is higher, this result is no longer the same after one week of exposure to ambient air. Indeed, this result is due to the fact that the lifetime of the cells is significantly increased by the presence of MoO3 in the CBL.
Recent studies show that if current progress is continued, organic photovoltaic cells (OPVCs) will have a unique advantage for large scale power generation . The method often used to increase the efficiency of OPVCs consists of the introduction of buffer layers between the electrodes and the organic films [2,3]. These buffer layers must improve the collection efficiency of one type of carrier and must be selective by opposing the passage of carriers of the opposite sign. Moreover, these buffer layers improve the band matching between the electrodes and the organic materials. In classical OPVCs, the anode buffer layer (ABL) can also smooth the surface of the ITO electrode, while the cathode buffer layer (CBL), often called the exciton blocking layer, protects the electron acceptor from metal diffusion during thermal evaporation of the cathode. However, the lifetime of OPVCs is far from satisfactory. The lifetime is mainly dependent on the environment. Important environmental parameters that influence the lifetime of organic solar cells are the diffusion of oxygen and water into the active layers of the cells through the upper electrode [4,5,6]. A possible solution to the problem of contaminant diffusion into the active organic layers could be the use of barrier layers with low oxygen and water permeability. The use of buffer layers could contribute to this solution. MoO3 is a very efficient ABL [7,8]. However, there is some controversy about its band structure. It is now well accepted that its band gap is approximately 3.1 eV and that it is an n-type material, yet the values of its ionization potential (IP), its electronic affinity (χ) , and its Fermi level (Wf) are still under discussion. These values measured in situ by ultraviolet photoelectron spectroscopy (UPS) after deposition in ultra-high vacuum are IP = 9.7 eV, χ = 6.7 eV and Wf = 6.9 eV. After air contamination, these values decrease significantly. It is well known that after five minutes or more of air exposure, these values decrease by approximately 1 eV [7,9]. However, as shown in recent studies, these values remain high enough to allow MoO3 to stay an efficient ABL if the highest occupied molecular orbital (HOMO) of the organic material is less than 5.9–6 eV, which is often the case in the typical electron donor materials . It has also been shown that oxygen deficiency promotes hole transfer through the creation of band gap states.
Due to the high values of the IP energy of MoO3, any hole transport via the valence band is prohibited, while the energy alignment between the band conduction minimum, BC, of MoO3 and the HOMO of the organic material is favorable for electron transfer between the two materials. That means that hole injection into the organic film proceeds via an electron transfer from the HOMO of the organic material to the band conduction of MoO3 in the case of organic light emitting diodes, whereas in the case of OPVCs, the photogenerated hole recombines with an electron at the interface between MoO3 and the organic layer, indicating that MoO3 works as a charge recombination layer. From this discussion, MoO3 cannot be an electron blocker because its conduction edge, CB, is too low. Therefore, the proposition of using MoOx as a CBL is not an incongruous idea, especially because MoOx tends to be metallic. Moreover, Vasilopoulou et al.  showed that the electron injection in an OLED based on poly[(9,9-di-n-octylfluorenyl-2,7-diyl)-alt-(benzo[2,1,3]thiadiazol-4,8-diyl)] (F8BT) can be significantly improved by inserting a very thin layer (5 nm) of partially reduced molybdenum oxide (MoO2.7) between the aluminum cathode and the organic emitting layer. Actually, after measuring the valence band maximum energy of MoOx by UPS to be equal to 7.1 eV and the band gap of MoO3 to be 3 eV, they conclude that the conduction band minimum is at approximately 4.1 eV, which is in good agreement with the work function of Al (4.3 eV). This energy alignment results in a relatively low electron injection barrier height. In addition, the states present in the band gap of MoOx may increase both the electron injection from Al and the conductivity of the oxide layer. More recently, Jin et al.  showed that the efficiency of OPVCs can be improved through the use of bathophenanthroline/molybdenum oxide (Bphen/MoOx) as a compound cathode buffer layer. OPV cells based on planar CuPc/C60 diodes were used in this work. It was shown that optimum performances are achieved when the thickness of layers constituting the Bphen/MoOx CBL is 2 nm/5 nm, respectively. They attributed this improving effect to the fact that the presence of Bphen prevents the formation of a diode at the contact MoO3/C60, while MoO3 prevents damage to Bphen during Al deposition. To justify good band matching among Al (Wf = 4.3 eV), MoO3 (Wf = 5.3–6.2 eV depending on the experimental conditions) and C60 (lowest unoccupied molecular orbital (LUMO) 3.7 eV), Jin et al. proposed a dipole value of 3 eV at the interface of MoOx/Bphen, using a value issued from the bibliography.
As a matter of fact, the work function of MoO3 is not the only important parameter at such complex interfaces; the Alq3/MoO3 interface is also crucial. In the case of conventional CBL, Alq3 protects C60 from damage incurred during aluminum deposition onto the organic material. Earlier studies show that there is actually some cathode metal diffusion into the organic under layer . However, if the CBL should be thick enough to protect the electron accepting layer, it should also not block all charge carriers. The HOMO and LUMO values of Alq3 are 5.9 and 3 eV, respectively. Because the LUMO value of the fullerene is 4.4 eV, the offset energy between the LUMO of the fullerene and that of the Alq3 is large, and the electrons must overcome a large energy barrier to reach the Al cathode in the case of electron transport via LUMO levels. To circumvent this difficulty, it has been proposed  that the charge transport in the CBL is due to damage induced during deposition of the cathode, which introduces conducting levels below its LUMO and explains why the transport of electrons is not impeded. Therefore, in the case of a double CBL, the relative thickness of both layers will either allow or disallow the presence of these gap states in Alq3. Furthermore, the position of these energy levels relative to the Fermi level of MoO3 will be decisive as regards the passage of electrons.
Thus, because we used nearly similar structures in our laboratory, i.e., planar heterojunctions based on the CuPc/C60 junction , in the present paper, we probed OPVCs using tris-(8-hydroxyquinoline) aluminum (Alq3) as the EBL, leading to an Alq3/MoO3 compound CBL. Even if our results are not identical to those mentioned above, they converge on those of Jin et al. , based on the time of exposure in air. These results are discussed in terms of the variation in the MoO3 work function due to air contamination. Moreover, we show that the lifetime of the OPVCs with MoO3 in their CBL is significantly improved.
The OPVCs used were ITO/MoO3/CuPc/C60/Alq3/MoO3/Al/a-Se with different thicknesses constituting the Alq3/MoO3 couple. The different films were deposited in thin film form by sublimation under vacuum (10−4 Pa), without breaking the vacuum.
The standard substrate dimensions were 25 mm by 25 mm. Because ITO covered the entire glass substrate, some ITO must be removed to obtain the under electrode. After masking a broad band of 25 mm by 20 mm, the ITO was etched using Zn + HCl as the etchant . Before thin film deposition, the ITO coated glass substrate was scrubbed with soap, rinsed with distilled water, dried and then placed in the vacuum chamber.
To test the effect of MoO3 on the performance of the OPVCs when introduced into the CBL, we used the classical planar heterojunction structure CuPc/C60; the ABL was, as discussed above, a thin MoO3 film, and the cathode was an aluminum film. The CBL was a double layer of aluminum tris(8-hydroxyquinoline) (Alq3)  and MoO3.
Without a protecting layer, the instability of solar cells in ambient air causes rapid deterioration in all performance, and non-encapsulated devices are practically dead after approximately 8 h in air. To mitigate this instability, prior to breaking the vacuum, an encapsulating layer of amorphous selenium (a-Se) approximately 40 nm in thickness was thermally evaporated. The selenium protective coating layer has been proven to be efficient in protecting the under layers from oxygen and water vapor contamination, at least during the early hours of ambient air exposure . This encapsulation hinders, but does not eliminate, the oxygen and water vapor diffusion processes. Therefore, the protective layer, which increases the lifetime of solar cells and prolongs the duration of the process, thus improves the precision of this study on the effect of an EBL on this process.
The thickness of the thin films and deposition rates were estimated in situ using a quartz monitor. We used a 3 nm thick MoO3 layer as the ABL because, as discussed above, MoO3 is well known as a very efficient ABL in optoelectronic organic devices. According to a previous study , the thickness of the CuPc layer was 35 nm, and that of the C60 layer was 40 nm.
The relative thickness of the constituents of the Alq3/MoO3 CBL was used as a parameter. The cathode was an aluminum film 100 nm thick, deposited by evaporation. The effective area of each cell was 0.16 cm2.
The main focus of this work was to study the influence of the value of the MoO3 work function, when used as the CBL, on the OPV cell performance, i.e., on the band matching at the interface cathode/EA. We varied the thickness of the Alq3/MoO3 couple from 9 nm/0 nm to 2 nm/7 nm, with intermediary values of 6 nm/3 nm and 3 nm/6 nm. The lifetime of the OPVCs was studied through the protocol proposed in ref . Following this protocol, the procedure used to study the aging process of our OPV cells corresponds to the intermediate level labeled “Level 2” The operational lifetimes have been measured under AM1.5, in air and at room temperature. The experimental conditions during the experiment were quite stable, i.e., the temperature was maintained at T = 20 ± 2 °C and the humidity at 60% ± 5%. Between each measurement, samples were stored in air and in the light of day, without artificial light. Cells were maintained in open circuit conditions. It should be noted that at least nine diodes are used in a cycle of deposit and that three cycles of deposits were used for the aging study.
The work functions of different CBLs have been measured using a Kelvin probe instrument (KPTechnology Model SKP5050). The vibrating probe consists of a stainless steel tip 10 mm in diameter having a work function of 4.947 eV. For the measurements, the tip is calibrated against a gold surface. This calibration value varied by approximately 20–30 meV before and after each measurement, thus keeping the measurement error at 30 meV. The non-scanning mode is used to measure the work function with approximately 500 repetitions for a single point. The work function of the sample is obtained by adding the measured work function (WF) to the correction factor (4.947 eV). The Kelvin method measures the contact potential difference (CPD) between the tip and the surface of the sample that are brought into contact as a result of Fermi energy equalization. The vibrating capacitor consists of the surface of the sample being tested, the reference surface of the electrode and the insulating medium between them. The CPD is evaluated by inducing an AC current flow and by the vibration of one of the surfaces with respect to the other in the vibrating capacitor. The contact potential difference is then measured by determining the compensating voltage required to null this current. The resolution of the measurements is 3 meV.
3. Results and Discussion
The measurements made just after the realization of cells show that the presence of MoO3 in the CBL systematically induces degradation of the OPV cell performance, which worsens with increasing thickness of the MoO3 layer (Figure 1). However, when MoO3 is present in the CBL, there is a continuous, systematic improvement in the OPVC efficiency during the first 5–6 days of room air exposure, whereas its efficiency decreases continuously when the CBL contains only Alq3 (Figure 2, Figure 3 and Figure 4).
In fact, just after realization, when MoO3 is 3 nm thick (Figure 1), the J-V characteristics are S-shaped. This effect increases dramatically with MoO3 thickness (Figure 1) because when the MoO3 thickness is 6 nm, the sign of the photocurrent is inverted, and this effect is accentuated for 7 nm thick MoO3.
Nevertheless, after air exposure, there is progressive improvement of the OPVC performance during the first few days, regardless of the thickness of the MoO3 layer in the CBL.
Therefore, ultimately, if we compare the performances of the different OPVCs after approximately 6 days of air exposure, the OPVCs with MoO3 in their CBL exhibit similar efficiencies as those without MoO3, as can be seen in Figure 4. Moreover, the efficiency of the OPVCs with MoO3 in their CBL becomes higher than that obtained with the classical Alq3 CBL after 11–12 days of air exposure.
In Figure 3, we show the typical evolution of the different OPVC parameters as a function of air exposure time for the OPVCs using “Alq3 (3 nm)/MoO3 (6 nm)” as the CBL. The sign of the photocurrent has a striking effect. Immediately after device preparation, there is a positive photocurrent in the second quadrant, but its value is very small (Figure 1 and Figure 2). After aging, the sign of the photocurrent becomes negative, as expected (Figure 2). The absolute values of Jsc and the OPVC efficiency η increase gradually over the first 5–6 days of air exposure. Then, there is a progressive decrease in Jsc and η. After 15 days, η reduces to approximately half its maximum value, which is attributed to degradation of the device from C60 contamination . The device then stabilizes for a long time (t > 4 months) at a value that is slightly less than half of the initial yield.
Regardless of the MoO3 thickness in the CBL and the duration of aging, the J-V characteristics are S-shaped, except when they reach their maximum performance level. It is known that S-shaped J-V characteristics are typical for the formation of a reverse diode at the contact electrode/organic material [17,18]. This effect means that in the present structures, band bending occurs not only at the CuPc/C60 interface but also at the C60/cathode interface (Figure 5).
These S-shaped J-V characteristics indicate the formation of a barrier at the C60/cathode interface. In the case of the J-V characteristics of Figure 1, the band bending near the C60/cathode interface must be larger than that at the CuPc/C60 interface, resulting in an opposite sign of the short circuit current. The formation of a barrier at the C60/cathode interface is due to the presence of MoO3 in the CBL because there are no S-shaped characteristics when the CBL is only a film of Alq3 (Figure 1). The formation of this barrier can be explained by the very high work function of MoO3. Actually, it is now well accepted that after deposition under vacuum by sublimation, the work function of MoO3 is approximately 6.2 eV . With this high Wf value, the band structure of the interface is such that at the C60/Alq3/MoO3/Al interface, the passage of holes is easier than that of electrons (Figure 6a). This result explains the reversal of the structure when the thickness of the MoO3 layer (6 nm) is such that the probability of charge carriers crossing by the tunnel effect is very low. However, it was also shown that air exposure of MoO3 induces a Wf decrease of approximately 1 eV .
In our case, using a Kelvin probe, we found that the work function of our MoO3 thin films is 5.1–5.2 eV after air exposure, regardless of the CBL, whereas it is 5.6 and 5.9 eV for a fresh CBL containing Alq3 (6 nm)/MoO3 (3 nm) and Alq3 (3 nm)/MoO3 (6 nm), respectively. This result means that the band alignment at the interface Allq3/MoO3 depends on the relative thickness of these layers. Nevertheless, just after deposition, regardless of the value of the MoO3 work function, the work function remains sufficiently high to induce the formation of a barrier at the C60/cathode interface.
If, in the present study, the OPVCs were covered with a Se film, it would not prevent progressive air contamination. Furthermore, we have already shown that even if the amorphous selenium film used as an encapsulation layer stabilizes the OPVCs, it only delays oxygen/water contamination of the cells. Therefore, the evolution of the J-V characteristics of the OPVCs for the duration of air exposure corresponds to the progressive air contamination of the OPVCs. The first layer encountered by the diffused contaminant after crossing the Al polycrystalline film is the MoO3 layer. Therefore, due to this progressive contamination, the Wf of MoO3 will decrease gradually until it reaches its minimal value of 5.1 eV. In parallel, the height of the barrier present at the C60/cathode interface decreases, which justifies the progressive improvement in the efficiency of the OPVCs over the first 6 days of air exposure (Figure 6b).
For a longer exposure time, the contamination reaches the C60 layer, and the performance of the OPVCs decreases. In fact, the oxygen/water contamination of C60 increases its resistivity . However, this contamination is significantly limited by the presence of MoO3 in the ABL because the efficiency of the OPVCs with a classical CBL tends regularly towards 0, whereas that of OPVCs with MoO3 in their CBL tends to stabilize at a value of nearly half their initial efficiency (Figure 4). The greater stability of the OPVCs with an Alq3/MoO3 bilayer as the CBL can be attributed to the fact that MoO3 deposited by the Joule effect under vacuum is oxygen deficient and tends to trap oxygen, thus preventing the lower organic layer from a high degree of contamination.
The difference between our results and those of reference 6 may be attributed to the facility of the Wf in varying with the history of the MoO3 layer. Indeed, the films deposited by Vasilopoulou et al.  are strongly oxygen deficient, which ensures that the Wf of their MoO3 is small.
The presence and height of a barrier at the C60/Alq3/MoO3/Al interface strongly depends on the Wf function of the MoO3 layer. This value depends on the composition and degree of contamination of the MoO3 layer. In the case of an uncontaminated layer, the Wf is so high that the OPVCs are inverted. When the MoO3 layer is sufficiently oxygen deficient and/or oxygen/air contaminated, its Wf decreases significantly to provide OPVCs with acceptable performance levels. Moreover, except for the first few days, the efficiency of the OPVC with a classical EBL is lower than that with MoO3 in the CBL. This result means that, although the initial performance of the OPVCs without MoO3 in their CBL is greater than that of OPVCs with MoO3, the OPVCs with MoO3 in their CBL become the most promising later on, as their performance quickly exceeds that of the former and tends to remain stable over time.
The three authors, Linda Cattin, Mustapha Morsli, and Jean Christian Bernède, contributed equally to the cell realization experiments, characterization and interpretation of the results.
Conflicts of Interest
The authors declare no conflict of interest.
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