An All-Organic Flexible Visible Light Communication System

Visible light communication systems can be used in a wide variety of applications, from driving to home automation. The use of wearables can increase the potential applications in indoor systems to send and receive specific and customized information. We have designed and developed a fully organic and flexible Visible Light Communication system using a flexible OLED, a flexible P3HT:PCBM-based organic photodiode (OPD) and flexible PCBs for the emitter and receiver conditioning circuits. We have fabricated and characterized the I-V curve, modulation response and impedance of the flexible OPD. As emitter we have used a commercial flexible organic luminaire with dimensions 99 × 99 × 0.88 mm, and we have characterized its modulation response. All the devices show frequency responses that allow operation over 40 kHz, thus enabling the transmission of high quality audio. Finally, we integrated the emitter and receiver components and its electronic drivers, to build an all-organic flexible VLC system capable of transmitting an audio file in real-time, as a proof of concept of the indoor capabilities of such a system.


Introduction
Visible light communication (VLC) which provides simultaneous illumination and wireless data transmission has received great attention in the past decade. VLC uses the visible spectrum from 380 nm to 750 nm corresponding to a frequency range from 430 THz to 790 THz, and it offers, in indoor environments, a real alternative to RF/microwave communication systems that have limited bandwidth and overcrowded spectrum. VLC presents several advantages over other data transmission technologies such as potentially high data rates [1][2][3], hundreds of THz of license-free channels [4], safety of the data transport medium compared to RF system in medical environments [5], and low power consumption. Potential applications of VLC systems include communications in healthcare

Flexible OPD Fabrication and Characterization
The device structure of the laboratory printed OPD devices is shown in Figure 1a. Please note that the primary function of this device structure is to act as an organic solar cell, but in this system it is used as an organic photodetector. The OPD devices were constructed on top of ITO-coated PET roll (40-60 Ω sq −1 ) purchased from Eastman (Kingsport, TN, USA). The ITO was patterned with Isishape HiperEtch 09S Type 40 paste (Merck KGaA, Darmstadt, Germany) as a negative image to the desired pattern. Roll to roll (R2R) rotary screen printing was performed with a printing speed of 1.5 m min −1 . After printing, the printed film was placed directly into the R2R hot air drying units set to a temperature of 140 • C for 160 s. The paste was washed off in baths of water and 2-propanol. After patterning, the surface was ultrasonically washed and dried in the R2R process. ZnO nanoparticle suspension (Avantama, Stäfa, Switzerland) was used for the electron transport layer. The ZnO ink was kept in an ultrasonic bath for 10 min prior to the printing. The ZnO layer was gravure-printed in the Sensors 2018, 18, 3045 3 of 12 laboratory (Schläfli, Zofingen, Switzerland) and dried at 120 • C for 5 min in an oven. The printing plate contained engravings with a line density of 120 lines cm−1. Regioregular P3HT (#4002-E, Rieke Metals, Lincol, NE, USA) was used as the donor and [60]PCBM as acceptor (purity 99.5%, Nano-C). The photoactive layer of P3HT:[60]PCBM was gravure printed in laboratory with a printing plate having a line density of 120 lines cm −1 . The photoactive layer was slowly dried, and devices were transferred to the glove box for pre-thermal annealing (120 • C for 10 min) and thermal evaporation of MoO 3 and Ag. Subsequently, the hole transport layer of MoO 3 (10 nm) and hole contact of Ag (200 nm) were thermally evaporated. Devices were encapsulated with flexible barrier substrate and pressure sensitized adhesive.
Sensors 2018, 17, x FOR PEER REVIEW 3 of 12 Metals, Lincol, NE, USA) was used as the donor and [60]PCBM as acceptor (purity 99.5%, Nano-C). The photoactive layer of P3HT:[60]PCBM was gravure printed in laboratory with a printing plate having a line density of 120 lines cm −1 . The photoactive layer was slowly dried, and devices were transferred to the glove box for pre-thermal annealing (120 °C for 10 min) and thermal evaporation of MoO3 and Ag. Subsequently, the hole transport layer of MoO3 (10 nm) and hole contact of Ag (200 nm) were thermally evaporated. Devices were encapsulated with flexible barrier substrate and pressure sensitized adhesive. Current-voltage (I-V) curves were measured with a FAS-2 Gamry four-probe potentiostatgalvanostat, a green laser and a lens set-up to ensure that the light fell upon the OPD surface homogeneously. EQE was recorded using a lock-in amplifier, a GaSb-detector, a halogen tungsten lamp and a mechanical chopper. The OPD frequency response was measured modulating the optical emission with a transconductance amplifier that varied the current flowing through the LED. The OPD was reverse biased and connected to a transimpedance amplifier with an equivalent input impedance of 50 Ω. Frequency response was recorded using a high sensitive lock-in amplifier (Zurich Instruments HF2LI, Zurich, Switzerland), suitable for frequencies from DC up to 50 MHz.

VLC System Layout
We have validated the performance of the flexible device in a real and novel application by designing and developing a full-flexible organic VLC system. The aim is to show the possibilities of the system in a real environment in which the requirements of bandwidth, responsivity and flexibility are mandatory. The receptor system is intended to be integrated in wearables, since both the photodetector (Figure 2a In this way, a communication link is established between a source of light, typically an OLED lamp emitting under modulating conditions, and a gadget that any user could wear integrated on a cap, jacket, trousers or even the skin. Hospitals, museums, crowded buildings or big malls are examples of possible scenarios where this system is ideal to overcome the drawbacks of low or Current-voltage (I-V) curves were measured with a FAS-2 Gamry four-probe potentiostat-galvanostat, a green laser and a lens set-up to ensure that the light fell upon the OPD surface homogeneously. EQE was recorded using a lock-in amplifier, a GaSb-detector, a halogen tungsten lamp and a mechanical chopper. The OPD frequency response was measured modulating the optical emission with a transconductance amplifier that varied the current flowing through the LED. The OPD was reverse biased and connected to a transimpedance amplifier with an equivalent input impedance of 50 Ω. Frequency response was recorded using a high sensitive lock-in amplifier (Zurich Instruments HF2LI, Zurich, Switzerland), suitable for frequencies from DC up to 50 MHz.

VLC System Layout
We have validated the performance of the flexible device in a real and novel application by designing and developing a full-flexible organic VLC system. The aim is to show the possibilities of the system in a real environment in which the requirements of bandwidth, responsivity and flexibility are mandatory. The receptor system is intended to be integrated in wearables, since both the photodetector (   Current-voltage (I-V) curves were measured with a FAS-2 Gamry four-probe potentiostatgalvanostat, a green laser and a lens set-up to ensure that the light fell upon the OPD surface homogeneously. EQE was recorded using a lock-in amplifier, a GaSb-detector, a halogen tungsten lamp and a mechanical chopper. The OPD frequency response was measured modulating the optical emission with a transconductance amplifier that varied the current flowing through the LED. The OPD was reverse biased and connected to a transimpedance amplifier with an equivalent input impedance of 50 Ω. Frequency response was recorded using a high sensitive lock-in amplifier (Zurich Instruments HF2LI, Zurich, Switzerland), suitable for frequencies from DC up to 50 MHz.

VLC System Layout
We have validated the performance of the flexible device in a real and novel application by designing and developing a full-flexible organic VLC system. The aim is to show the possibilities of the system in a real environment in which the requirements of bandwidth, responsivity and flexibility are mandatory. The receptor system is intended to be integrated in wearables, since both the photodetector (Figure 2a  In this way, a communication link is established between a source of light, typically an OLED lamp emitting under modulating conditions, and a gadget that any user could wear integrated on a cap, jacket, trousers or even the skin. Hospitals, museums, crowded buildings or big malls are examples of possible scenarios where this system is ideal to overcome the drawbacks of low or In this way, a communication link is established between a source of light, typically an OLED lamp emitting under modulating conditions, and a gadget that any user could wear integrated on a cap, Sensors 2018, 18, 3045 4 of 12 jacket, trousers or even the skin. Hospitals, museums, crowded buildings or big malls are examples of possible scenarios where this system is ideal to overcome the drawbacks of low or collapsed WiFi access, or to ensure privacy in the communication by using a punctual light source that could be driven using a home automation system. The basic scheme is shown in Figure 3. A cell phone is the data transmission source, in this case an audio file, though the data source could come from any device provided that the bandwidth is sufficient as to support the data link. In a real application, the emitter system would be integrated in the luminaries of the roofs or walls in a building, or in a desk lamp. This emitter driver is composed of a circuit for transmitting the data fully made of off-the-shelf components, such as, a voltage amplifier as conditioning circuit for the input signal, an FM modulator based on a voltage controlled oscillator (VCO), and a signal conditioning circuit to modulate the current of the power transistors driving the OLED panel. This circuit follows the indications of the integrated circuit CD4046 datasheet. The last one is a 99 × 99 × 0.88 mm LG N6SA30 commercial panel with a power consumption of 1.28 W and an efficacy of 60 lm/W, which could be used as a spotlight in any of the abovementioned applications. The electrical characteristics and optical data are shown in Figure 4. collapsed WiFi access, or to ensure privacy in the communication by using a punctual light source that could be driven using a home automation system. The basic scheme is shown in Figure 3. A cell phone is the data transmission source, in this case an audio file, though the data source could come from any device provided that the bandwidth is sufficient as to support the data link. In a real application, the emitter system would be integrated in the luminaries of the roofs or walls in a building, or in a desk lamp. This emitter driver is composed of a circuit for transmitting the data fully made of off-the-shelf components, such as, a voltage amplifier as conditioning circuit for the input signal, an FM modulator based on a voltage controlled oscillator (VCO), and a signal conditioning circuit to modulate the current of the power transistors driving the OLED panel. This circuit follows the indications of the integrated circuit CD4046 datasheet. The last one is a 99 × 99 × 0.88 mm LG N6SA30 commercial panel with a power consumption of 1.28 W and an efficacy of 60 lm/W, which could be used as a spotlight in any of the abovementioned applications. The electrical characteristics and optical data are shown in Figure 4.   collapsed WiFi access, or to ensure privacy in the communication by using a punctual light source that could be driven using a home automation system. The basic scheme is shown in Figure 3. A cell phone is the data transmission source, in this case an audio file, though the data source could come from any device provided that the bandwidth is sufficient as to support the data link. In a real application, the emitter system would be integrated in the luminaries of the roofs or walls in a building, or in a desk lamp. This emitter driver is composed of a circuit for transmitting the data fully made of off-the-shelf components, such as, a voltage amplifier as conditioning circuit for the input signal, an FM modulator based on a voltage controlled oscillator (VCO), and a signal conditioning circuit to modulate the current of the power transistors driving the OLED panel. This circuit follows the indications of the integrated circuit CD4046 datasheet. The last one is a 99 × 99 × 0.88 mm LG N6SA30 commercial panel with a power consumption of 1.28 W and an efficacy of 60 lm/W, which could be used as a spotlight in any of the abovementioned applications. The electrical characteristics and optical data are shown in Figure 4.   The receiver circuit (block diagram in Figure 5, schematics in Supplementary Figure S1) contains the fabricated flexible OPD as the light-to-current transducer, and a conditioning circuit that receives the signal from the OPD and converts it into voltage using a simple transimpedance amplifier. The information received is demodulated in frequency with a phase locked loop (PLL) based on a CD4046 integrated circuit. This commercial circuit was also used as FM modulator in the emitter circuit, but configured to play the VCO role. Finally, an amplifier circuit using an LM386 operational amplifier drives a loudspeaker. The receiver circuit (block diagram in Figure 5, schematics in Supplementary Figure S1) contains the fabricated flexible OPD as the light-to-current transducer, and a conditioning circuit that receives the signal from the OPD and converts it into voltage using a simple transimpedance amplifier. The information received is demodulated in frequency with a phase locked loop (PLL) based on a CD4046 integrated circuit. This commercial circuit was also used as FM modulator in the emitter circuit, but configured to play the VCO role. Finally, an amplifier circuit using an LM386 operational amplifier drives a loudspeaker. The bandwidth requirements of this simple system are determined by those of the audio system, i.e., at least around 44 kHz to properly transmit the signal, according to the Nyquist criterion. The system design must take into account that any of the electronic components used may limit the bandwidth, therefore the authors payed special attention to the low pass filters using ICs CD4046 and LM386, the first one to retrieve the modulated signal and avoid aliasing, and the second one to generate a clean audio signal to drive the speaker.

Results and Discussion
In this section we show the characterization of the main parts of the VLC system, i.e., the OPD, the OLED and the performance of the whole system. The goal is to show that our whole-flexible setup is able to maintain an audio link in an indoor environment. Figure 6a shows the current-density voltage (J-V) characteristic of the flexible OPD in dark and under green-light illumination. The dark curve exhibits a shunt resistance (RSH) of around 2 MΩ, reverse current of 1.42 × 10 −5 mA/cm 2 at 0 V, and Rs = 40 Ω at 1 V that may be attributed to poor electrical contacts at the ITO-covered flexible substrates. The photocurrent density under green-light illumination varies from 4.7 × 10 −2 mA/cm 2 to 2.5 × 10 −2 mA/cm 2 between 0 V and −2 V for a 0.5 mW incident light power. The calculated responsivity, R (A/W) results in 0.144 A/W at 532 nm and 0.065 A/W at 635 nm, which agrees well with the EQE at zero bias shown in Figure 6b exhibiting a maximum of 24.3% at 550 nm. Using the responsivity value, the current value of 2 × 10 −3 mA/cm 2 at −1 V (Figure 6a), and following the methods described in [33], we have calculated a noise equivalent power (NEP) of 2.78 × 10 −12 W/Hz −1/2 , and a specific detectivity of D* = 1.8 × 10 11 Jones. The linearity is also over 99% (see the Supplementary Materials). The bandwidth requirements of this simple system are determined by those of the audio system, i.e., at least around 44 kHz to properly transmit the signal, according to the Nyquist criterion. The system design must take into account that any of the electronic components used may limit the bandwidth, therefore the authors payed special attention to the low pass filters using ICs CD4046 and LM386, the first one to retrieve the modulated signal and avoid aliasing, and the second one to generate a clean audio signal to drive the speaker.

Results and Discussion
In this section we show the characterization of the main parts of the VLC system, i.e., the OPD, the OLED and the performance of the whole system. The goal is to show that our whole-flexible setup is able to maintain an audio link in an indoor environment. Figure 6a shows the current-density voltage (J-V) characteristic of the flexible OPD in dark and under green-light illumination. The dark curve exhibits a shunt resistance (R SH ) of around 2 MΩ, reverse current of 1.42 × 10 −5 mA/cm 2 at 0 V, and R s = 40 Ω at 1 V that may be attributed to poor electrical contacts at the ITO-covered flexible substrates. The photocurrent density under green-light illumination varies from 4.7 × 10 −2 mA/cm 2 to 2.5 × 10 −2 mA/cm 2 between 0 V and −2 V for a 0.5 mW incident light power. The calculated responsivity, R (A/W) results in 0.144 A/W at 532 nm and 0.065 A/W at 635 nm, which agrees well with the EQE at zero bias shown in Figure 6b exhibiting a maximum of 24.3% at 550 nm. Using the responsivity value, the current value of 2 × 10 −3 mA/cm 2 at −1 V (Figure 6a), and following the methods described in [33], we have calculated a noise equivalent power (NEP) of 2.78 × 10 −12 W/Hz −1/2 , and a specific detectivity of D* = 1.8 × 10 11 Jones. The linearity is also over 99% (see the Supplementary Materials). The frequency response was measured using the lock-in amplifier, sweeping the frequency from 10 Hz to 10 MHz. The bandwidth of the OPD is obtained by illuminating the sample with a pulsed red LED biased with a square signal driven by the lock-in amplifier. The response of the OPD was conditioned by a transimpedance amplifier, with bandwidth over 10 MHz to avoid affecting the measured response. Using this amplifier, the OPD was reverse biased between 0 and 2 volts.

OPD Optolectronic Characterization
The bandwidth increases from 100 kHz for the OPD biased at 0 V, up to 200 kHz for the OPD reverse biased at 2 V (see Figure 7). As expected, reverse biasing improves the bandwidth due to the increase of carriers. In any case, for the audio file Li-Fi transmission purpose, the OPD widely covers the bandwidth requirements to be used as optical receptor. In addition, impedance spectroscopy has been measured in the 1 Hz-3 MHz frequency range at different voltages in dark conditions. Figure 8 shows the electrical impedance at 0.1, 0, −0.5 and −1 V. The spectra resemble a semicircle that has been modelled with an RpC element in series with resistance, Rs. Rp accounts for the parallel of the shunt resistance (modelling leakage current due to The frequency response was measured using the lock-in amplifier, sweeping the frequency from 10 Hz to 10 MHz. The bandwidth of the OPD is obtained by illuminating the sample with a pulsed red LED biased with a square signal driven by the lock-in amplifier. The response of the OPD was conditioned by a transimpedance amplifier, with bandwidth over 10 MHz to avoid affecting the measured response. Using this amplifier, the OPD was reverse biased between 0 and 2 volts. The bandwidth increases from 100 kHz for the OPD biased at 0 V, up to 200 kHz for the OPD reverse biased at 2 V (see Figure 7). As expected, reverse biasing improves the bandwidth due to the increase of carriers. In any case, for the audio file Li-Fi transmission purpose, the OPD widely covers the bandwidth requirements to be used as optical receptor. The frequency response was measured using the lock-in amplifier, sweeping the frequency from 10 Hz to 10 MHz. The bandwidth of the OPD is obtained by illuminating the sample with a pulsed red LED biased with a square signal driven by the lock-in amplifier. The response of the OPD was conditioned by a transimpedance amplifier, with bandwidth over 10 MHz to avoid affecting the measured response. Using this amplifier, the OPD was reverse biased between 0 and 2 volts.
The bandwidth increases from 100 kHz for the OPD biased at 0 V, up to 200 kHz for the OPD reverse biased at 2 V (see Figure 7). As expected, reverse biasing improves the bandwidth due to the increase of carriers. In any case, for the audio file Li-Fi transmission purpose, the OPD widely covers the bandwidth requirements to be used as optical receptor. In addition, impedance spectroscopy has been measured in the 1 Hz-3 MHz frequency range at different voltages in dark conditions. Figure 8 shows the electrical impedance at 0.1, 0, −0.5 and −1 V. The spectra resemble a semicircle that has been modelled with an RpC element in series with resistance, Rs. Rp accounts for the parallel of the shunt resistance (modelling leakage current due to In addition, impedance spectroscopy has been measured in the 1 Hz-3 MHz frequency range at different voltages in dark conditions. Figure 8 shows the electrical impedance at 0.1, 0, −0.5 and −1 V. The spectra resemble a semicircle that has been modelled with an R p C element in series with resistance, R s . R p accounts for the parallel of the shunt resistance (modelling leakage current due to fabrication defects) and the diode dynamical resistance. C is the total capacitance of the device, which, in general, fabrication defects) and the diode dynamical resistance. C is the total capacitance of the device, which, in general, is a combination of geometrical and chemical capacitance. At reverse bias C is dominated by the geometrical capacitance. Rs accounts for the series resistance modelling metallic contacts and wires. Circuital parameters are obtained from the fit of the impedance spectra in dark conditions to the circuit of the inset. Rs has a quasi-constant value of 30 Ω, as can be obtained in the high frequency part of the Cole-Cole plot (Figure 8, inset). C ranges between 6 and 9 nF, and Rp ranges from 0.37 to 1.9 MΩ in the voltage range from −1 V up to 0.1 V. A simple calculation using the 25 mm 2 area, a relative dielectric permittivity of around 4 and an active area thickness of 230 nm results in a capacitance of the order of 4 nF, close to the one measured, reinforcing that the geometrical capacitance is the main contribution to the overall capacitance.
According to Ref. [33] the device bandwidth can be estimated from the values of the diode capacitance. The capacitance obtained from the fit of impedance of the OPD under green LED is 12.6 nF at 0 V. This value is close to the one obtained without illumination, thus showing again that the capacitance is mainly the geometrical one. This value yields a cut-off frequency of approximately 250 kHz, which is in the same order of the measured value shown in Figure 7.

OLED Characterization
As the luminaire of the VLC system, we use a commercial flexible OLED (N6SA30C) from LG Chem© (Seoul, South Korea) with 3000 K of correlated color temperature, operating temperature between 0 to 40 °C, 8.1 V forward voltage and luminous flux of 75 lm. The manufacturer claims r 40,000 operation hours and 1.8 W of power consumption. It is a thin light weight square luminaire of 20 g and dimensions 99 × 99 × 0.88 mm.
We measured the I-V curve using the Gamry potentiostat, though it only reached up to 7.6 V, which is under the standard operation for this LED (Figure 9 Left). In order to increase the operation bias, we built a classical current source using an operational amplifier with a MOSFET IRF530 circuit in the negative feedback loop (Figure 9 Left, inset). The OLED current is established with the voltage input signal applied to the op amp non-inverting terminal. By using our current source circuit we obtained the same curve as with the Gamry, but increasing bias up to 8.3 V. The current measured at that point is around 228 mA. It is clear that the forward voltage is around 8 V, as expected. Circuital parameters are obtained from the fit of the impedance spectra in dark conditions to the circuit of the inset. R s has a quasi-constant value of 30 Ω, as can be obtained in the high frequency part of the Cole-Cole plot (Figure 8, inset). C ranges between 6 and 9 nF, and R p ranges from 0.37 to 1.9 MΩ in the voltage range from −1 V up to 0.1 V. A simple calculation using the 25 mm 2 area, a relative dielectric permittivity of around 4 and an active area thickness of 230 nm results in a capacitance of the order of 4 nF, close to the one measured, reinforcing that the geometrical capacitance is the main contribution to the overall capacitance.
According to Ref. [33] the device bandwidth can be estimated from the values of the diode capacitance. The capacitance obtained from the fit of impedance of the OPD under green LED is 12.6 nF at 0 V. This value is close to the one obtained without illumination, thus showing again that the capacitance is mainly the geometrical one. This value yields a cut-off frequency of approximately 250 kHz, which is in the same order of the measured value shown in Figure 7.

OLED Characterization
As the luminaire of the VLC system, we use a commercial flexible OLED (N6SA30C) from LG Chem© (Seoul, South Korea) with 3000 K of correlated color temperature, operating temperature between 0 to 40 • C, 8.1 V forward voltage and luminous flux of 75 lm. The manufacturer claims r 40,000 operation hours and 1.8 W of power consumption. It is a thin light weight square luminaire of 20 g and dimensions 99 × 99 × 0.88 mm.
We measured the I-V curve using the Gamry potentiostat, though it only reached up to 7.6 V, which is under the standard operation for this LED (Figure 9 Left). In order to increase the operation bias, we built a classical current source using an operational amplifier with a MOSFET IRF530 circuit in the negative feedback loop (Figure 9 Left, inset). The OLED current is established with the voltage input signal applied to the op amp non-inverting terminal. By using our current source circuit we obtained the same curve as with the Gamry, but increasing bias up to 8.3 V. The current measured at that point is around 228 mA. It is clear that the forward voltage is around 8 V, as expected.
We characterized the OLED also using impedance spectroscopy (Figure 9 Right). The Cole-Cole diagram was fitted to an equivalent circuit composed of a resistance R S in series with the parallel of a shunt resistance (the dynamic resistance of the diode, R P ) and a capacitor C OLED , a similar circuit to that of the OPD (Figure 8 Right, inset). Due to the limitations of our model 1260 impedance analyzer (Solartron, West Sussex, UK), we injected only a current range from 5 to 85 mA. Fits reveal that the OLED has a C OLED ranging from 1.95 µF at 5 mA up to 2.34 µF at 85 mA, with a constant R S of 2.41 ± 0.02 Ω. Dynamic resistance R P ranges from 30.4 down to 2.9 Ω when increasing the operation current. All these values have an error under 2%.
The cutoff frequency is given by f c = (2π × C OLED × (R S || R P )) −1 according to its equivalent circuit (Figure 9 Right, inset). Biasing the OLED with 5 mA, we obtain a cutoff frequency of 9.22 kHz. Increasing the bias current up to 85 mA the cutoff frequency increases up to 56 kHz (Figure 10 Left), though this could be even improved by increasing the bias current, as R P would decrease (Figure 9 Right). Moreover, increasing the output resistance of the driving circuit, R O , reduces the signal at the OLED (Figure 10 Right), worsening the OLED performance. As a conclusion, the OLED will not limit the bandwidth in an audio link, providing it is polarized at a high enough bias current and the driving circuit is carefully selected. We characterized the OLED also using impedance spectroscopy (Figure 9 Right). The Cole-Cole diagram was fitted to an equivalent circuit composed of a resistance RS in series with the parallel of a shunt resistance (the dynamic resistance of the diode, RP) and a capacitor COLED, a similar circuit to that of the OPD (Figure 8 Right, inset). Due to the limitations of our model 1260 impedance analyzer (Solartron, West Sussex, UK), we injected only a current range from 5 to 85 mA. Fits reveal that the OLED has a COLED ranging from 1.95 µF at 5 mA up to 2.34 µF at 85 mA, with a constant RS of 2.41 ± 0.02 Ω. Dynamic resistance RP ranges from 30.4 down to 2.9 Ω when increasing the operation current. All these values have an error under 2%.
The cutoff frequency is given by fc = (2π × COLED × (RS || RP)) −1 according to its equivalent circuit (Figure 9 Right, inset). Biasing the OLED with 5 mA, we obtain a cutoff frequency of 9.22 kHz. Increasing the bias current up to 85 mA the cutoff frequency increases up to 56 kHz (Figure 10 Left), though this could be even improved by increasing the bias current, as RP would decrease (Figure 9 Right). Moreover, increasing the output resistance of the driving circuit, RO, reduces the signal at the OLED (Figure 10 Right), worsening the OLED performance. As a conclusion, the OLED will not limit the bandwidth in an audio link, providing it is polarized at a high enough bias current and the driving circuit is carefully selected.  We characterized the OLED also using impedance spectroscopy (Figure 9 Right). The Cole-Cole diagram was fitted to an equivalent circuit composed of a resistance RS in series with the parallel of a shunt resistance (the dynamic resistance of the diode, RP) and a capacitor COLED, a similar circuit to that of the OPD (Figure 8 Right, inset). Due to the limitations of our model 1260 impedance analyzer (Solartron, West Sussex, UK), we injected only a current range from 5 to 85 mA. Fits reveal that the OLED has a COLED ranging from 1.95 µF at 5 mA up to 2.34 µF at 85 mA, with a constant RS of 2.41 ± 0.02 Ω. Dynamic resistance RP ranges from 30.4 down to 2.9 Ω when increasing the operation current. All these values have an error under 2%.
The cutoff frequency is given by fc = (2π × COLED × (RS || RP)) −1 according to its equivalent circuit (Figure 9 Right, inset). Biasing the OLED with 5 mA, we obtain a cutoff frequency of 9.22 kHz. Increasing the bias current up to 85 mA the cutoff frequency increases up to 56 kHz (Figure 10 Left), though this could be even improved by increasing the bias current, as RP would decrease (Figure 9 Right). Moreover, increasing the output resistance of the driving circuit, RO, reduces the signal at the OLED (Figure 10 Right), worsening the OLED performance. As a conclusion, the OLED will not limit the bandwidth in an audio link, providing it is polarized at a high enough bias current and the driving circuit is carefully selected.

VLC System
A demonstration video of the proposed proof of concept can be found in the Supplementary Materials of this paper. A snapshot of the video is shown in Figure 11 and serves as a view of the entire system. The full-organic flexible VLC system was built in the lab as described in Section 2.2. On the left side of Figure 11, the transmission circuit is receiving the signal coming from the jack connection of a cell phone. The information is FM modulated, i.e., the signal with varying frequency is superimposed to the OLED DC bias current needed for illumination, which produces an imperceptible modulation in the light. The light is received at the OPD, and then conditioned with a flexible driver (see right side of Figure 11) as described in Figure 4. The receptor circuit sends the demodulated and processed signal to the loudspeaker. The signal is reproduced at high quality, with the only limitations coming from the output circuit and the loudspeaker rather than the OLED and the OPD.

VLC System
A demonstration video of the proposed proof of concept can be found in the Supplementary Materials of this paper. A snapshot of the video is shown in Figure 11 and serves as a view of the entire system. The full-organic flexible VLC system was built in the lab as described in Section 2.2. On the left side of Figure 11, the transmission circuit is receiving the signal coming from the jack connection of a cell phone. The information is FM modulated, i.e., the signal with varying frequency is superimposed to the OLED DC bias current needed for illumination, which produces an imperceptible modulation in the light. The light is received at the OPD, and then conditioned with a flexible driver (see right side of Figure 11) as described in Figure 4. The receptor circuit sends the demodulated and processed signal to the loudspeaker. The signal is reproduced at high quality, with the only limitations coming from the output circuit and the loudspeaker rather than the OLED and the OPD. The limitations of the system are mainly coming from the electronics and OLED rather than the OPD. This can be due to the use of the simplest design and electronic components, both in emission and reception circuits. Transmission is achieved using a simple modulating integrated circuit, by means of a voltage controlled oscillator tuned in the carrier frequency by the connection of external passive components: resistances and capacitors. The reception circuit is demodulating the signal using the same commercial integrated circuit but configured in a phase locked loop, also tuned using external resistances and capacitors. The use of simple and cheap both OLED luminaire and integrated circuits finally could limit the frequency response of the system. Nevertheless, it can operate at a frequency high enough to be used in audio applications. This should be at least 44 kHz, and our system begins to decay at 40 kHz. According to the Nyquist criterion, we may lose information at frequencies over 20 kHz when retrieving the audio signal, but those frequencies are over the usual audio frequency threshold for humans. The key point for the proper operation system is to bias the OLED near the forward voltage, which eases the switching to transmit the information without affecting the lighting operation, and enhances the switching speed of the OLED.
The performance of the audio system is not significantly affected by the bending of the OPD, as the video shows (nevertheless, further research on the performance under bending must be made in future works). Then, this system can be used in a wide variety of applications. We propose one here: as the OLED is suitable for ambient illumination, it could send customized and personal information to a specific target. In a smart automated building, for instance, it could be suitable to transmit information via audio files to a person that wears an audio system like this one (receptor + headphones instead of a loudspeaker) integrated in a wearable. Using the flexible condition of both the OPD and the circuit, the reception system can be integrated in a cap or clothes, or even in a small hearing-aid. In an office building this could be used to send information to a specific worker. It should The limitations of the system are mainly coming from the electronics and OLED rather than the OPD. This can be due to the use of the simplest design and electronic components, both in emission and reception circuits. Transmission is achieved using a simple modulating integrated circuit, by means of a voltage controlled oscillator tuned in the carrier frequency by the connection of external passive components: resistances and capacitors. The reception circuit is demodulating the signal using the same commercial integrated circuit but configured in a phase locked loop, also tuned using external resistances and capacitors. The use of simple and cheap both OLED luminaire and integrated circuits finally could limit the frequency response of the system. Nevertheless, it can operate at a frequency high enough to be used in audio applications. This should be at least 44 kHz, and our system begins to decay at 40 kHz. According to the Nyquist criterion, we may lose information at frequencies over 20 kHz when retrieving the audio signal, but those frequencies are over the usual audio frequency threshold for humans. The key point for the proper operation system is to bias the OLED near the forward voltage, which eases the switching to transmit the information without affecting the lighting operation, and enhances the switching speed of the OLED.
The performance of the audio system is not significantly affected by the bending of the OPD, as the video shows (nevertheless, further research on the performance under bending must be made in future works). Then, this system can be used in a wide variety of applications. We propose one here: as the OLED is suitable for ambient illumination, it could send customized and personal information to a specific target. In a smart automated building, for instance, it could be suitable to transmit information via audio files to a person that wears an audio system like this one (receptor + headphones instead of a loudspeaker) integrated in a wearable. Using the flexible condition of both the OPD and the circuit, the reception system can be integrated in a cap or clothes, or even in a small hearing-aid. In an office building this could be used to send information to a specific worker. It should be very useful to help workers suffering from any kind of disability or limited hand use. The transmitted information helps the worker to do the job, giving instructions while operating. A bidirectional system can add a handbook interactive query, a usual environment for astronauts at the International Space Station. Another interesting environment could be the illumination of a piece of art in a museum, where the information can be transmitted to the visitor placed in front of it, using a passive reception system in a hearing device. The visitor using this system will not be aware of the fact that the lighting is transmitting the information played in the headphone, since the light environment is indistinguishable of the OLED for the human eye.

Conclusions
We have demonstrated a fully organic flexible visible light communication system using off-the-shelf components, flexible circuits, a flexible commercial OLED and a flexible organic photodiode manufactured in a roll-to-roll process. This demonstration follows an integral methodology: first, we designed the whole system, setting the objective of transmitting an audio file from an OLED luminaire to a flexible OPD. Second, we performed a full characterization of every component of the link in terms of frequency response to guarantee the require data transmission rate. Third, we built the complete system, connecting a mobile phone to our emitter circuit, modulating the OLED transmission, sending the light signal to a flexible OPD, and transducing the signal with a demodulator flexible circuit that finally sends the audio signal to a loudspeaker. Both the emitter and receiver drivers are made as simple as possible, using the minimum number of commercial components, demonstrating a low cost VLC proof of concept. The only feature that increases the price of the system is the flexible condition of the printed circuit board.
Potential system improvements are related to enhance the system bandwidth. This requires increasing the frequency response of the electronics and emitter/receiver components. Large area commercial OLEDs are the bottleneck of the system. The bigger the OLED, the longer the operation distance but the slower is the switching. The future goal is to design the driving circuits operating over hundreds of MHz, both in emission and transmission, and to build an OPD that could support this operation frequency. Such bandwidths would even allow video transmission.