Photo doping is a photo induced charge separation process at a donor/acceptor interface as depicted schematically in Figure 1, where a photon can be captured by an electron in donor which is excited from donor HOMO to the donor LUMO forming a Frenkel type of electron-hole pair or exciton [1,2,3,4]. The Frenkel exciton can then diffuses via energy transfer to a nearby donor/acceptor interface at where it is dissociated into electron at the acceptor and a hole at the donor by a potential field due to the LUMO orbital offset (∆E₁) between the donor and the acceptor, and that the electron transfers from the donor LUMO to the acceptor LUMO, and the hole remains in the donor HOMO [2]. After the exciton dissociation and the electrons/holes moving away from D/A interface, the charge separation or a voltage can be achieved [1,2]. A popular polymer based photo doping D/A pair is P3HT/PCBM whose chemical structures are shown in Figure 2, and P3HT/PCBM pair based polymer solar cells have been widely studied and reported [1,3,4,5,6]. Previous studies have found that P3HT’s chemical structural regio-regularity induced solid-state ordered packing or crystallinity result in one of best hole mobility (> 1.0 cm²/Vs) among conjugated polymers with a strong visible light absorption down to 650 nm [3,4,5,6]. With the addition of a minority amount of photo doping acceptor phenyl-C₆₁-butyric acid methyl ester (PCBM), a p-type photo sensing device may be fabricated as schematically shown in Figure 3, where a potential non-uniform illumination on left side generated mobile holes are diffusing toward right dark area via P3HT HOMOs, while the photo generated electrons are trapped in minority PCBM LUMOs on the left bright area, thus a photo generated voltage between the bright area and the dark area may be achieved. Previous studies of non-uniform illumination on photovoltaic cells have been mainly focused on analysis of solar cell conversion efficiencies of uniform versus non-uniform illuminations [7,8]. When P3HT/PCBM are equal amount mole ratio, then photo doping would yield equal amount of mobile electrons that can move in acceptor PCBM phase, and equal amount of mobile holes that can diffuse in donor P3HT phase, thus a solar cell can be realized between the positive ITO and negative Al electrodes (Figure 4 and Figure 5), or a photo conductor can be materialized between the same Al electrodes as show in Figure 5 and Figure 6.

Most or typical solar cells including P3HT/PCBM cells are fabricated with equal amount of donor/acceptor pair under uniform illumination mode, i.e., light illuminate the whole cell surface area uniformly generating equal mobile electrons and holes followed by their separation and migration to corresponding electrodes [1,3,4,5,6]. In this work, however, bright-dark non-uniform light illumination in a p-type P3HT/PCBM photo doping pair are being investigated for potential non-uniform photovoltage generation applications. As Figure 3 shows, while photo generated immobile/minority electrons are trapped at PCBM LUMOs and cannot move, majority/mobile holes at P3HT HOMOs can diffuse from the higher density area (brighter areas) toward the lower density areas (darker areas) driven by at least the hole density gradients and potential temperature gradients. Such mobile charge diffusion would cease until the density gradient force is countered or balanced by the Columbic attraction force as a result of separated electrons and holes. This charge separation and voltage generation mechanism is very similar in principle to the charge separation and mobile charge diffusion resulting in voltage generation of the thermoelectric (TE) Seebeck effects [9], except that the charge generation is due to light in the photo doping case, and is due to heat in thermoelectric case.

Measurement system calibration: A commercially purchased silicon reference solar cell (ABET Technologies Inc., Device code: RK5N3726, Ref#: RR213KG5) was first measured, where an open circuit voltage (V_oc=0.48 volt) and short circuit current (I_sc = -10 mA) were obtained under our solar simulator. Both values are lower than the expected or specified values (V_oc = 0.56 volt and I_sc= -60 mA under 1.0 Sun) indicating our measurement system are under estimated, for instance, our light illumination intensity is much lower than one Sun (estimated at about 0.4 Sun). However, the system is good enough to characterize the photo cells with self comparison purpose.

Photo cell measurements: In pure or pristine P3HT (0% PCBM doping) film, due to photo generated Frenkel type excitons and there are no photoelectric charge separation, dark, uniform or non-uniform light illuminations are not expected to generate any charges or electrical voltages/currents, and indeed our measurements confirmed this for pristine P3HT cells. In about 100% PCBM doped sample (sample #7), due to both donor and acceptor are roughly equal, both photo generated electrons and holes can be mobile in its phase, both charges have the same density gradient and diffusion even if non-uniform light illuminations are applied, and therefore no asymmetric photo voltages (V_oc) are expected between the two in-plain Al electrodes. This was indeed confirmed in our sample cell #7 as it does not exhibit any asymmetric photo diode style IV curves under non-uniform illuminations. For p-type photo doing (PCBM doping levels between 0-90%), while in-plain measured uniform light illumination IV curves are expected to be higher than dark IV cures due to photo doping generated charges, asymmetric V_oc are not expected due to charge generaton symmetry in uniform illuminations. However, in non-uniform illuminations of two in plain Al electrode pairs, IV curves could exhibit asymmetric or non-zero V_oc due to charge density gradient between light and dark Al electrode area. Indeed, Figure 7 exhibits IV curves between two in plain Al electrode pair of sample #6 (about 80% PCBM doping ratio) with cell thickness of about 60 nm under dark (dark dashed line), under uniform light illumination (red long dashed line), and under non-uniform light illumination (Purple solid line). Uniform illumination current is higher than dark current can be explained by the photo doping generated charges (trapped electrons and mobile holes), however, the V_oc is zero due to both cells are exposed to the same light and the increased charge density are the same so there is no charge or voltage differential. When the bottom cell is blocked from light illumination and only top cell is exposed to light, the photo generated holes at top cell are diffused to the corresponding bottom cell while the electrons are being trapped at the top cell, thus a photo voltage (V_oc = 0.47 volt) between top and bottom cell are generated as shown in Figure 7. To our knowledge, this is the first demonstration of photo voltage generated as a result of non-uniform illumination.

The term non uniform illumination here was coined to refer to subjecting a solar cell surface to bright and dark areas of illumination simultaneously, with the intention of generating a charge density gradient and a resulting photovoltage. Specifically, a polymeric composite thin film composed of P3HT (p-type photo doping semiconductor) and PCBM (photo doping electron acceptor) at varying p-type doping levels ranging from 0-100% were investigated in our studies. As Table 1 exhibits, while non-uniform photovoltages for samples 1-5 (below 80% PCBM doing levels) were not obvious, sample/device #6 with about 80% PCBM doping level film of about 60 nm thick exhibited a 0.47 photovoltage under non-uniform illumination. Further experiments to repeat results of a 80% PCBM doping level at a thicker film of over 80nm also confirmed the symmetric photo conductive IV curves under uniform illumination, and asymmetric photo diode IV curves under non-uniform illuminations with a photovoltage between 1.2-1.3 volts observed as illustrated in Figure 8. All cells are not optimized so IV curve shapes or fill factors are not optimal, as the main objective of this work is to demonstrate a non-uniform generated photovoltage.

When ITO layer was absent, i.e., only P3HT:PCBM composite films were spun coated on top of the glass (with or without PSS:PEDOT layer), the non-uniform illumination photovoltages were not obvious or measurable between any in plain Al electrode. This implies, the ITO layer appears essential for the non-uniform light illumination generated photovoltages in the current device configuration. We hypothesis that, due to relatively high electrical resistance of P3HT [10], photo generated mobile holes in the light area went vertically down to ITO layer and then transport directly and efficiently to the dark area through ITO and then move up vertically toward the dark area below Al electrode, as the resistivity is relatively small for P3HT film thickness of less than 100nm. However, with improvement of P3HT morphology and hole transport mobility, or with careful design of device geometries, it is possible that holes may be able to diffuse efficiently in plain from light area to dark area via P3HT HOMO orbitals for more than 100nm distances.

Photo voltage V_oc generation in a p-type photo doping semiconductor pair P3HT: PCBM under non-uniform light illumination has been successfully observed and demonstrated. Such novel optoelectronic or photovoltaic polymer based devices may be further developed and optimized for potential applications where non-uniform light illuminations are being used or available for either solar cell or image sensing purposes.