Introduction

Over the past five decades, the semiconductor industry has provided infinite scope for improvement. Many inorganic materials and devices were investigated, leading to developments in artificial intelligence (AI)-such as Alphago1,2. Recently, the rate of progress in inorganic materials has saturated, and Moore’s law has probably approached its limit.3 To overcome these limitations, we ought to incorporate new candidates such as antibiotics and biomaterials instead of Silicon or other conventional elements, to form the next generation of devices.4,5 For organic optoelectronics such as organic light-emitting diodes (OLEDs) and photovoltaics (OPVs), Poly(3,4-ethylenedioxythiophene): poly(styrenesulfonate) (PEDOT:PSS) is one of the most widely used materials for various purposes, such as hole transporting layer (HTL), anode buffer layer, and transparent conducting electrode.6,7,8 Recently, significant endeavors and effective approaches have been demonstrated for enhancing the conductivity of PEDOT:PSS.9 For example, Zhang et al.10 demonstrated that the addition of glycerol or sorbitol could increase the conductivity of the PEDOT:PSS by two orders of magnitude. Ouyang et al.11 utilized meso-erythritol or dimethyl sulfoxide to modify PEDOT:PSS properties. Rivney et al.12 showed that the addition of ethylene glycol improves conductivity and generates a controlled aggregation (such as a J or H aggregation, with marginally tighter π-stacking) to empower electronic and ionic transport for attaining energy efficient devices. Wang et al.13 also reported a parallel J-aggregation in poly(diallyldimethylammonium) chloride (PDDA) with the help of amine group (-NH2) and -PSS, which acted as a bridge for faster exciton transfer between quantum dots. In search of a proper addition to PEDOT:PSS to make it more favorable, we investigated the chemical, optical, and electronic properties of ampicillin and studied its interaction with PEDOT:PSS.

Ampicillin is most widely used as an antibiotic for animal health (like penicillin is for human health)14,15,16,17 because of its stability in acidic conditions. Even though, most research on optoelectronic devices demonstrated vertical (orthogonal) dipole formation;18,19,20 the spatial orientation of the generated horizontal (or inclined) interfacial dipole in ampicillin molecule with respect to changes in pH was recently simulated by Malloci et al.21 The primary, secondary, and tertiary (cyclic amide in lactam ring) amine along with the carbonyl group (-C = O) present in ampicillin’s structure provide a specific charge distribution over the molecule.21 This resulted in an interfacial dipole with a larger magnitude (30.28 Debye)21,22 as compared with the dipole from other amine-based molecules such as polyethyleneimine (PEI) (1.3 Debye)23 and even penicillin (5.99 Debye).24 The utilization of amine-based molecules including biomaterials and amino acids have been previously reported to alter the work function (φ) of the layers/substrates owing to the generation of interfacial dipole for various optoelectronic and OPV applications.25,26,27,28 Mostly, a reduction in the φ of the indium tin oxide (ITO) substrates was achieved by treatment with the amine-based molecules having a dipole away from the ITO.26,28 In addition, Kotagiri et al.29 highlighted the emission properties of ampicillin as an efficient fluorescent agent and the energies of the aggregated molecules with respect to their arrangement could be expressed by Brick theory.30 So, we chose ampicillin to be incorporated in optoelectronics because materials with such interfacial dipoles, whether utilized as thin films18,19,31 or in bulk form,20 has proven to be beneficial for OLED’s performance.

In terms of enhancements in device performance of green OLEDs to date, Huang et al.32 reported an external quantum efficiency (EQE) of 32.5% and a current efficiency (CE) of 117.5 cd A−1 in a tandem structure. Xu, et al.33 reported a maximum EQE of 36.85% and CE of 135.74 cd A−1 also in a tandem structure. In addition, thermally activated delayed fluorescence devices have demonstrated an EQE of 35–37.8% owing to the horizontal dipole molecular orientation and intramolecular charger transfer processes.34,35,36 Helander et al.37 utilized a chlorinated ITO in single unit OLED to present an EQE of 29.1% owing to the tuning of the anode φ (charge balance strategy) without any modifications in the molecular orientation of host/dopant or light out-coupling. Meanwhile, Kim, et al.38 experimentally demonstrated an EQE of 30% by horizontal dipole orientation and theoretically analyzed that a maximum of 46% EQE could be achieved in ITO-based single unit OLEDs.

In this work, we demonstrate a substantial increment in the device performance of a single-unit OLED without any out-coupling aid (EQE ~ 35.1%). The performance was boosted by horizontal/inclined interfacial dipole, charge balance and extra J/H-aggregated exciton generation, which was achieved by the contribution of ampicillin in PEDOT:PSS (ampicillin-PEDOT:PSS). For further evaluation, OLED devices with similar concentrations (25–75%) were also fabricated by the addition of penicillin, which has an identical chemical structure, but the only difference is the absence of primary -NH2. This provided a progressive insight about the specialty and significance of the ampicillin’s structure and specific interfacial dipole characteristics in the enhancement of OLED’s device performance. The physical, chemical, optical, and electronic properties, along with the concentration- and time-dependent interactions of ampicillin with PEDOT:PSS, leading to its role in optoelectronic performance, was investigated.

Results

Electrical and optical properties of ampicillin-PEDOT:PSS

Figure 1a shows the schematic of the OLED device (ITO/(0–75%) ampicillin-PEDOT:PSS/N,N-bis-(1-naphthyl)-N,N′-diphenyl-1,1′-biphenyl-4,4′-diamine (NPB)/Tris(4-carbazoyl-9-ylphenyl)amine (TCTA)/4,4′-Bis(N-carbazolyl)-1,1′-biphenyl (CBP)+Tris[2-phenylpyridinato-C2,N]iridium(III) (Ir(ppy)3)/2,2′,2′′-(1,3,5-benzinetriyl)-tris(1-phenyl-1-H-benzimidazole) (TPBi)/lithium fluoride (LiF)/aluminum (Al)) layout with the bandgap alignments of layers as shown in Fig. 1b. The carrier injection barrier heights (i.e., difference in Fermi levels (Ef) between layers) determine the performance of an optoelectronic device.39 The valence electronic energy levels of ampicillin-PEDOT:PSS were analyzed using ultraviolet photoelectron spectroscopy (UPS as shown in Fig. 1c) by depositing on a clean Au surface. The analysis of the ampicillin-PEDOT:PSS layers revealed a decrease in Ef with an increase in amount of ampicillin. At 0% (only PEDOT:PSS), the φ was found to be 4.74 eV, which decreased to 4.10 eV at 25% ampicillin addition. The φ values of the ampicillin-PEDOT:PSS further decreased to 3.75 and 3.72 eV, with the addition of 40% and 75% concentrations, respectively. Moreover, we compared the measured φ using UPS with the one analyzed by kelvin probe force microscopy (KPFM) (Supplementary Fig. 1). Even though the surface φ obtained by the KPFM was slightly higher owing to different nature of the analysis (atmospheric conditions might have caused some contamination/oxidation),40 the overall trend of decrease in φ with the addition of ampicillin was found to be in agreement with the UPS measurements.

Fig. 1
figure 1

Electrical and optical properties of (0–75%) ampicillin-PEDOT:PSS layers. a Schematic of the fabricated organic light-emitting diodes (OLED) devices with (0–75%) ampicillin in PEDOT:PSS. b Bandgap alignment of the utilized layers in the device structure along with the triplet energies of the layers and the chemical structure of ampicillin. c Ultra-violet photoelectron spectroscopy (UPS) analysis with secondary cutoff regions of indium tin oxide (ITO)/(0–75%) ampicillin-PEDOT:PSS. d X-ray photoelectron spectroscopy (XPS) analysis of the PEDOT:PSS layers showing -COOH and -N confirming the presence of ampicillin’s carbonyl and -NH2 groups, respectively. e pH analysis (standard deviation from the mean, obtained average from five number of measurements) of different concentrations of ampicillin-PEDOT:PSS solutions showing the shift from acidic (pH < 7) to alkaline (pH > 7) nature of solutions with increase in concentration of ampicillin

We attribute this decrease in φ for ampicillin-PEDOT:PSS layers to the shift of Ef towards the lowest unoccupied molecular orbital owing to the generation of an opposite interfacial dipole directed towards the anode. This indicated a concentration-dependent interaction of the ampicillin-PEDOT:PSS, which was analyzed using X-ray photoelectron spectroscopy (XPS) as shown in Fig. 1d. The carboxylic acid-related photoelectronic peak in C-1s profile (-COOH at 288.1 eV)41,42 detected with an addition of 25% confirmed the presence of ampicillin in the ampicillin-PEDOT:PSS. The intensity of the peak (at 400 eV)41,42 of N at 0% increased when the ampicillin concentration rose to 25% and so on, which refers to the presence of -NH2 from the ampicillin in ampicillin-PEDOT:PSS. We also observed a small N 1 s peak for PEDOT:PSS material which does not contain N in its molecular structure as reported before.43,44 We speculate that the peak was due to contamination from the atmosphere during the transfer of samples from the preparation facility to the XPS analysis tool. We prepared several samples at different conditions including glove box, open air followed by placement in the loading chamber, however, we still observed this N 1 s peak for PEDOT:PSS.43,44 On analyzing the S-2p profile, a large -PSS peak was encountered for 0%, which was reduced in intensity for 25% film, and almost disappeared in 40%, indicating that the majority of -PSS group in PEDOT:PSS was attached to -NH2 side chain. The shifting realized in ITO peaks (Supplementary Fig. 1) also corroborated the lowered φ45 of ampicillin-PEDOT:PSS as supported with UPS analysis, where the overall φ of the system reduced with increased addition of ampicillin.18,19,31

In addition to the changes in φ, charge transport properties are highly affected by the structure (amorphous/crystalline) and surface morphology. Surface morphology and structure of the ampicillin-PEDOT:PSS were analyzed using atomic force microscopy (AFM), x-ray diffraction (XRD), and high-resolution transmission electron microscopy (HR-TEM), as illustrated in (Supplementary Fig. 1). However, we did not observe any major changes in surface morphology (except 25% ampicillin-PEDOT:PSS) and any crystallinity from XRD and HR-TEM analysis was not detected. Absorbance/transmittance analysis was also in accordance with the slight variations detected in the surface morphology of the layers (Supplementary Fig. 2). Hence, the analysis indicates that the interaction of ampicillin in PEDOT:PSS purely depends on volume concentrations.

Concentration-dependent chemical interactions of ampicillin

The ampicillin chemical structure46,47 contains an electrophile -NH2 (primary amine) group, secondary amine, nucleophile -C = O, and a lactam ring (tertiary amine) (Supplementary Fig. 3). The amine side chain of ampicillin gives it stability in acidic conditions (pH ~ 4.48 (25%)) but, makes ampicillin unstable in alkaline (~ 7.36 (40%), ~ 8.28 (75%)) conditions by opening up the lactam ring.47,48 An increase in pH was analyzed with an increase in concentration of ampicillin in PEDOT:PSS (Fig. 1e). At 25% concentration, the acidic nature of the solution permits the existence of ampicillin’s stable monomer form. The asymmetry in this stable ampicillin monomer charge distribution owing to the presence of primary -NH2 and -C = O, results in the generation of a net interfacial dipole with a large magnitude of 30.28 Debye.21,22 This ampicillin’s dipole was found to be many orders higher than other amine-based molecules (Supplementary Fig. 3) such as PEI, which has a dipole of 1.3 Debye.23 With just the absence of primary amine, such as in penicillin structure, the dipole moment was also greatly reduced to 5.99 Debye.24 This indicates that unlike other amine-based molecules, the specific molecular structure of ampicillin is a crucial aspect, which could significantly contribute in the resulting device performance. The spatial orientation of the generated dipoles in ampicillin molecules with respect to pH was simulated before (Supplementary Fig. 3).21 Based on the simulated dipole characteristics, the interaction of 25% ampicillin-PEDOT:PSS could be demonstrated as shown in Fig. 2. The interaction was experimentally analyzed using high-performance liquid chromatography (HPLC) (Supplementary Fig. 4), which indicated a reduction in -PSS peak together with an increment in ampicillin peak. This was coherent with the peak variations analyzed using XPS (Fig. 1d). Hence, from XPS and HPLC analysis, it was acquired that -O group from -SO3 molecules of -PSS interacted with -NH2 and -H groups of ampicillin monomers through hydrogen bonding (Fig. 2). The ampicillin molecules attached with PEDOT:PSS chain, which formed a head-to-tail arrangement to induce J-aggregation also cross-examined by S-parameter analysis of molecular orientation (Supplementary Fig. 5).49,50,51 Owing to the parallel location of primary, secondary, and tertiary amines in the main chemical structure of ampicillin (Supplementary Fig. 3), the placement might be beneficial to form a horizontal (parallel) interfacial dipole with PEDOT:PSS, as shown in Fig. 2.

Fig. 2
figure 2

Schematic of the chemical interaction of ampicillin (0–75%) with PEDOT:PSS. The 25% ampicillin monomers attached with PEDOT:PSS in a horizontal fashion contribute extra excitons by J-aggregation. With 40% ampicillin addition (due to the start of polymerization) some of the monomers formed dimers in a more perpendicular manner, which resulted in the generation of H aggregations. With 75% addition ampicillin became unstable and decomposed to conjugated forms owing to high pH

Evaluation and analysis of J/H-aggregated excitons

Figure 3a, b shows the mechanism of the efficiency contribution in the device by the horizontal/inclined interfacial dipole and the generated J/H aggregations. The changes in energy of the resulting molecular arrangement owing to horizontal and inclined dipoles would differ (Fig. 3c)52 and the detailed mechanism of J/H aggregations is demonstrated in Supplementary Fig. 5. It is to be noted, that in previous reports, other amine-based layers such as PEI,19,23 PEI:PSS18 and polyallylamine19 lowered the φ of the cathode and reduced the electron transport barrier. However, in our work, the high magnitude of the dipole by ampicillin, lowered the φ, which suppressed the hole injection owing to the dipole direction towards the ITO anode. Also, the hole injection was relatively higher for 25% ampicillin-PEDOT:PSS as compared with 40%, which could be due to the orientation of the inclined interfacial dipole that suppressed hole injection more than the horizontal dipole.18,19,20 We examined this effect of interfacial dipole in different concentrations of ampicillin using transport stability analysis through forward (0–8 V) and reverse (8–0 V) applied voltage (Fig. 3d). A similar current density trend observed for 0% (PEDOT:PSS) layer revealed a negligible charge trapping/de-trapping phenomena. However, with an addition of ampicillin (e.g., 40%), the current density difference between forward and reverse bias indicated that ampicillin addition in PEDOT:PSS induced a charge trapping/de-trapping or accumulation, which might be owing to the interfacial dipole (Fig. 3d).18,19,20 Further, the expected efficiency contribution of this high magnitude dipoles and J/H aggregations was analyzed by the obtained EQE from heterojunction devices (Fig. 3e), which were fabricated without a proper EML. Here, the pristine (without ampicillin) PEDOT:PSS devices presented a very low efficiency of ~ 0.5%. The efficiency of the devices was increased to ~ 4–6% with the addition of ampicillin, which indicates that even without EML, light emission was obtained. This emission by the ampicillin-PEDOT:PSS layer in heterojunction devices could be attributed to the additional/extra J/H-aggregated excitons generated due to the ampicillin’s molecular dipole. The mechanism for the generation of such aggregations with the addition of dipole in the –NH2 based dyes has been systematically reviewed by Brixner et al.53 Also, the J-aggregations were found to be preferable where less electrical loss and better optical model was required.38 Moreover, Qin et al.54 also demonstrated that an aggregates-based single thin film was utilized as both HTL and EML purposes where ~ 3.5% EQE was obtained. Therefore, the obtained results from the heterojunction devices (Fig. 3e) provided a strong evidence that a boosted emission by J/H-aggregated excitons could be possible and expected in the full OLED device structure. The overall summary of the mechanism is presented in Fig. 3a, b where two different emissions could be concluded: one at the EML with ~ 25–30% EQE owing to the charge (hole-electron) recombination; the second at the ampicillin-PEDOT:PSS layer with ~ 4–6% EQE in case of 25%, and 1–4% for 40% addition of ampicillin. These excitons were also confirmed by the picosecond time-resolved photoluminescence (TRPL) and time-resolved area normalized emission spectrum (TRANES), and are discussed in the coming section. Here, the out-coupling factor could be overlooked because we did not observe any significant changes in the analyzed angle dependent optical spectra even with various backing temperatures and substrates (data not shown).

Fig. 3
figure 3

Mechanism of the efficiency contribution by J/H-aggregated excitons. a, b Schematic of the overall efficiency contribution by J/H-aggregated excitons, emission layer (EML) along with the interfacial dipole orientations for (a) 25% and (b) 40% ampicillin addition. c demonstrates the excitation types involved in relation to monomers, horizontal (J-aggregate)/inclined (H-aggregates). Where, S represents absorption, W for fluorescence, wavy arrows for internal conversion, and crossed lines for forbidden transitions, M for transition dipole moments and m for excitonic states52. d Current density-voltage (J–V) of ampicillin-PEDOT:PSS layers (0–75%) under forward and reverse applied potential (standard deviation from the mean, obtained by averaging five number of measurements is shown as error bars). e External quantum efficiency (EQE) analyzed (errors are standard deviation from the mean, obtained average eight number of measurements) for heterojunction devices without the addition of EML. f showing the camera images of ampicillin fluorescence under UV and steady state photoluminescence (PL)

Another significant effect of ampicillin is the fluorescence emission,29 owing to the exciton’s generation demonstrated in Fig. 3f. To understand this J/H-aggregated exciton generation, which helps to boost the device efficiency, we compared the TRPL and TRANES analysis of 2 days and 1-month-old ampicillin as shown in Fig. 4a–o and Supplementary Fig. 2. In 2 days, fresh ampicillin-PEDOT:PSS mixtures, we observed a strong excimer emission in the region 500–750 nm, in addition to the main fluorescence peak (460 nm), which confirmed the presence of J-aggregation (horizontal dipole interaction) in 25% ampicillin-PEDOT:PSS thin film (Fig. 4a, g).49,50,51 Interestingly, increased ampicillin concentration in PEDOT:PSS (i.e., at 40%) improved the number of monomers more than it did in a 25% mixture, hence another type of interfacial dipole (inclined dipole interaction, H aggregation) was generated in 40% ampicillin-PEDOT:PSS (shown in Fig. 2, Fig. 3b) by breaking the lactam ring of the previously attached ampicillin monomer, to form dimers. This is in accordance with the ampicillin molecular changes at high concentration and pH, as reported before.55 Owing to the more perpendicular orientation, or stacking structure (Fig. 2) of these occasionally occurring dimers, we proposed the formation of H-type aggregation51,56 in addition to J-aggregation for 40% ampicillin-PEDOT:PSS. TRANES analysis of 40% showed the excimer emission (Fig. 4h) with a slight blue-shift (at 530 nm peak) as compared with 25% (550 nm peak) (Fig. 4g). This peak was attributed to the emission by allowed transition to the ground state from the lower-energy excited state56 of the occasional H aggregations as shown in Figs. 3b, 4h. In addition to the TRANES analysis, we could conclude the formation of J/H aggregation in ampicillin-PEDOT:PSS layers by analyzing the horizontal/inclined molecular orientation using S-parameter (Supplementary Fig. 5). Interestingly, the above-mentioned additional emissions encountered around 500–750 nm in TRANES could not be realized in 1-month-old samples (Fig. 4e, k). This clearly conveyed the fact that after 1 month, J/H-aggregated excitons were affected due to the generation of trimer and polymer in the mixtures as shown in Supplementary Fig. 6. In the case of 75% TRANES data, excimer emission shows a red-shift owing to the decomposed form of ampicillin as explained in Fig. 2. To eliminate the substrate-oriented emissions, we recorded TRANES for the same set of samples deposited on fused silica substrate (Fig. 4p–r), which reiterates the aggregations mentioned above (and ITO substrate peak as shown in Supplementary Fig. 2).

Fig. 4
figure 4

Time-resolved photoluminance (TRPL)/Time-resolved area normalized emission spectrum (TRANES) analysis of (0–75%) ampicillin-PEDOT:PSS layers on indium tin oxide (ITO) and fused silica substrate. ac TRANES analysis for 2 days fresh ampicillin-PEDOT:PSS. a J-aggregation emission at about 500–750 nm for 25% ampicillin-PEDOT:PSS on ITO. b J and H aggregation emission for 40% ampicillin-PEDOT:PSS on ITO. c Excimer emission for 75% ampicillin-PEDOT:PSS on ITO showing chromophores emission for decomposed forms of ampicillin. df TRANES analysis of 1-month-old ampicillin-PEDOT:PSS samples showing negligible excimer emissions. Corresponding TRANES for each concentration of gi 2-days fresh jl 1-month-old ampicillin-PEDOT:PSS. mo Normalized intensity comparison for 2-days and 1-month (25–75%) ampicillin-PEDOT:PSS for 0 ns exciton lifetime. pr TRANES mapping images of intensity and lifetime variation of PEDOT:PSS films with ampicillin addition deposited on fused silica. s solid-state emission spectra of PEDOT:PSS films with various concentrations (25–75%) of ampicillin deposited on fused silica. Inset depicts the exciton lifetime (TRPL) of corresponding concentrations

Moreover, we analyzed the solid-state PL spectra (Fig. 4s) for the pristine and ampicillin incorporated PEDOT:PSS layers where we could not obtain a proper emission by the pristine PEDOT:PSS. However, the PL spectra was obtained only when the ampicillin was added to the PEDOT:PSS, which indicated that the J/H-aggregated excitons would have contributed to the cultivation of more photons from the devices. Also, a shorter exciton lifetime (TRPL) was observed for 25% ampicillin-PEDOT:PSS (inset Fig. 4s) as compared with 40%. This is in accordance with the J-aggregations (horizontal dipole with shorter lifetime) and H aggregations (inclined dipole and longer lifetime) mechanism reported before.51,56 At 75%, the new longer lifetimes can be attributed to the formation of new composites based on ampicillin and PEDOT:PSS, as shown in the inset of Fig. 4i. Two mechanisms could be invoked for the origin of the red-shifted emission in 75% ampicillin-PEDOT:PSS—(1) the aggregation between chromophores57 is dominant in this condition, and may induce fast excimer formation at an early stage, or (2) the aggregation between ampicillin and PEDOT:PSS is negligible. Here, the polymer matrix is further modified to reveal that each chromophore has more rigid and planar conformation in ground state. Some portion of chromophores, whose configuration is suitable for the intermolecular reaction, shows weak emission at ~555 nm of 75%. The other portion follows the conformational change observed in the 25 and 40% cases, and then shows the long decay lifetimes because of the rigid geometry from the aggregation.

At high concentration (75%), ampicillin became unstable and it decomposed to conjugated forms such as penicilloic acid, penilloic acid, and 2-Hydroxy-3-phenylpyrazine.46,47,48 HPLC analysis (Supplementary Fig. 4) of 1-month-old 75% ampicillin-PEDOT:PSS confirmed this possible polymerization/conjugated forms. In addition, nuclear magnetic resonance (NMR) data presented in Supplementary Fig. 7 further reiterates the formation of polymer moieties.58 The interfacial dipole at 75% is speculated to be gone, as its presence has not been observed in such conjugated forms previously either.46,47,48 The highest alkaline nature of 75% sample is further tested, and confirmed with contact angle (CA) measurements (Supplementary Fig. 7), which expect to solve the acidic problems created by PEDOT:PSS on device electrodes.59

Performance enhancement by charge balance and J/H aggregations

The performance of single-unit OLED devices containing 0–75% of ampicillin-PEDOT:PSS is summarized in Fig. 5, Tables 1 and 2. Efficient light emission in an OLED is possible through charge (electron-hole) balance, by avoiding the recombination near the electrodes and confining within the EML.32,33,38 The device without ampicillin showed a low CE of ~ 48 cd A−1. This is because the electron injection/mobility in CBP + Ir(ppy)3 based EML through electron transport layer (ETL) is weaker than the hole injection/mobility from PEDOT:PSS. Therefore, more holes could reach the EML following the Ohmic-type contact, causing a large charge imbalance (Supplementary Fig. 8). With an addition of ampicillin in PEDOT:PSS in small concentrations (2, 10, 15%) we analyzed a linear increase in device performance with increase in concentration of ampicillin as shown in Supplementary Fig. 9. However, a significant increase in OLED performance was observed by utilization of 25% ampicillin-PEDOT:PSS layer, with CE, EQE, and power efficiency (PE) values of 120 cd A−1, 35.1%, and 70 lmW−1, respectively, (Fig. 5a–d) in the green wavelength region (495–570 nm, electroluminance (EL) of the devices shown in Supplementary Fig. 9). As electron injection remained constant for all ampicillin-PEDOT:PSS devices, a suitable hole suppression was provided by 25% ampicillin-PEDOT:PSS layer observed by hole-only devices (HODs) as shown in Supplementary Fig. 8. The hole mobility calculation for ampicillin-PEDOT:PSS layers in relation to electron injection/mobility of the ETL (TPBi) layer were also analyzed at low- and high-voltage regions, which demonstrated the closest match for 25% ampicillin-PEDOT:PSS device. This hole suppression owing to an adequate decrease in φ (caused by an opposite interfacial dipole towards anode) would be critically beneficial for the charge balance as shown in Supplementary Fig. 5, where the lowest injection difference (0.11 eV) between holes and electrons was observed for 25% ampicillin-PEDOT:PSS device.

Fig. 5
figure 5

Device performance analysis of organic light-emitting diodes (OLEDs) with (0–75%) ampicillin-PEDOT:PSS. a J–V and luminance analysis showing the trend of current density. b Current efficiency (CE) analysis demonstrating 25% ampicillin-PEDOT:PSS with best efficiency (of 120 cd A−1). c External quantum efficiency (EQE) of the devices. Inset showing Lambertian emission using the variable-angle analysis (luminance) obtained from the devices (solid lines) with the ideal Lambertian pattern (dotted line). d Power efficiency (PE) of the devices. e EQE measurement using half-moon integrating sphere. Inset showing schematic of the total luminance flux measurement system (half-moon integrating sphere) analyzed at (7 ± 1 V) using one-point-measurement. f EQE comparison with penicillin (without primary -NH2) based devices. Inset showing the difference of the chemical structure between penicillin (without primary -NH2) and ampicillin (with primary -NH2). Errors in bf are standard deviation from the mean, obtained averaging eight measurements

Table 1 Comparison of (0–75%) ampicillin-PEDOT:PSS device performances current efficiency (CE), external quantum efficiency (EQE), and power efficiency (PE) with the standard deviations at the low luminance region (1170 cd/m2) along with their color coordinates (CIE (International Commission on Illumination)–1931)
Table 2 Comparison of (0–75%) ampicillin-PEDOT:PSS device performances current efficiency (CE), external quantum efficiency (EQE), and power efficiency (PE) with the standard deviations at high luminance regions (1000 and 2000 cd/m2) along with their color coordinates (CIE (International Commission on Illumination)–1931)

When the holes injected from the ITO combined with the electrons in ampicillin-PEDOT:PSS layer, they formed excitons owing to the presence of an interfacial dipole. These J/H-aggregated extra or additional excitons (4~6%) when dissociated resulted in the generation of photons at the ampicillin-PEDOT:PSS layer in addition to the emitted photons (25~30%) from the EML layer. These excimer/exciton generation in ampicillin-PEDOT:PSS layer was confirmed using TRANES and TRPL data in 500–600 nm wavelength region (Fig. 4). The contribution of these excitons in the device was analyzed using the device performance by heterojunction devices (Fig. 3e, without EML). This indicated that the addition of ampicillin (25%) enhanced the efficiency by at least 4–6% in addition to the EML efficiency, thus delivering one of the top device performances.32,33,38 The variable-angle performance (shown as inset in Fig. 5c) demonstrated that including 25% ampicillin-PEDOT:PSS device, all OLED devices (solid colored lines) presented near-perfect Lambertian emission compared with the simulated ideal (dotted line) curve. The quantum efficiency of the devices was cross-examined with half-moon integrating sphere measurement system (at 7 ± 1 V using one-point measurement) (Fig. 5e) and was found to be similar with the obtained performance. To further understand the contribution of ampicillin’s molecular structure, specific interfacial dipole and J-aggregations in the ampicillin-based OLEDs, we incorporated penicillin in PEDOT:PSS and fabricated the OLED devices (with the same layout) as shown in Fig. 5f. The major difference between ampicillin and penicillin is the absence of primary -NH2 group and can be attributed to the presence of weaker interfacial dipole than ampicillin. The comparison shows that the penicillin-PEDOT:PSS devices demonstrated an EQE of ~ 24% in comparison with ampicillin-PEDOT:PSS device with an EQE of ~ 35%. This emphasizes that ~ 11% EQE was additionally reinforced (boosted). As mentioned before this enhanced EQE as compared to the devices with penicillin could be due to charge balance and the formation of J/H-aggregated excitons. The injected holes from ITO and the electrons in the ampicillin-PEDOT:PSS layer combined to form excitons, which were dissociated causing an emission. The emission by these excitons in addition to that by the EML led to the overall increase of the resulting luminance.

Interestingly, 40% ampicillin-PEDOT:PSS infused devices also demonstrated comparable CE of 118 cd A−1, EQE of 33%, and PE of 58.6 lmW−1, especially in the higher luminance region. The larger decrease in φ and hole injection by 40% ampicillin-PEDOT:PSS layer would not be well-matched with the electron injection from the ETL, which could have induced a charge imbalance in EML at low luminance region. However, we speculate that at higher luminance (increased voltage) hole injection was improved (became similar to 25%) owing to overcome of conduction barrier (Supplementary Figs. 8, 10), which could consequently lead to better charge balance thus improving the efficiency. Occasionally, a large fluctuation in 40% ampicillin-PEDOT:PSS devices efficiency was observed (shown as standard deviation in Fig. 5b–d) and on investigation the reason was found to be the absence/presence of long rod-like ampicillin crystals60,61 (Supplementary Fig. 11) in the spin coated 40% ampicillin-PEDOT:PSS layer. As the ampicillin crystal formation could be supported by instability of various factors such as temperature60 and pH61, the temperature was kept constant during the preparation of ampicillin solution. However, as the pH of 40% ampicillin-PEDOT:PSS solution was around the same as reported crystal formation region (pH 7.8~6)61, the observed infrequent crystallization (Supplementary Fig. 11) could be owing to rare variations in pH. We speculate that in the presence of such crystals the 40% ampicillin-PEDOT:PSS device efficiency fluctuated, but overall 25% and 40% ampicillin added devices showed remarkable improvement in device efficiency as compared with reference device (without ampicillin) (Tables 1, 2).

In 75% concentrated ampicillin devices, the potential barrier for holes increased further, and hole injection was strongly suppressed, which caused a severe charge imbalance and reduced efficiency. The optimum conditions of ampicillin for the best OLED efficiency was found to be 50 mg ml−1 (ampicillin/sterilized deionized water (SDIW) having a maximum shelf-life of 2 days, kept at 2~5 °C in a refrigerator. The role of ampicillin-PEDOT:PSS shelf-life and concentration (mg ml−1) of ampicillin-PEDOT:PSS were investigated using device fabrication (Supplementary Fig. 12) and devising the chemical interaction of 1-month-old ampicillin (Supplementary Fig. 6) for better understanding. Hence, we concluded that the pH control by ampicillin-PEDOT:PSS preservation in refrigerator (2–5 °C) are the key factors to attain efficient performances in OLEDs. Figure 6a–d demonstrate the schematic of the overall mechanism of the ampicillin-PEDOT:PSS layers with different concentrations. It has been configured based on the obtained charge injection, orientation of interfacial dipole, J/H aggregations, chromophores interaction and the resulting contribution in the device efficiencies. The energy band diagram illustrated in Fig. 6e–h exemplifies the vacuum level shift and hole/electron barrier from UPS, XPS, and HOD/electron-only devices investigations, with various ampicillin volume concentrations. Furthermore, the UPS analysis of the ampicillin-PEDOT:PSS with different thicknesses of the NPB layer (1–20 nm) was analyzed and the interface barriers/vacuum level shifts were investigated as shown in Supplementary Fig. 13. The ampicillin-PEDOT:PSS layer was also applied in forward and inverted OPVs as transport layers (data not shown), where inverted OPV with ampicillin-PEDOT:PSS exhibited superior performance than the forward structure, due to the decreased Ef.

Fig. 6
figure 6

Schematic of the overall mechanism and role of (0–75%) ampicillin-PEDOT:PSS layers with Fermi levels (Ef) alignment for a PEDOT:PSS only device, b 25% ampicillin-PEDOT:PSS. The interfacial dipole drawn as a yellow arrow directed towards anode. The hole injection and electron injection are shown as blue and red spheres, respectively. The dotted circles around hole-electron pair show the charge recombination. c 40% ampicillin-PEDOT:PSS. d 75% ampicillin-PEDOT:PSS with similar information. eh Energy-level alignment with 0–75% ampicillin-PEDOT:PSS concentrations illustrated from hole-only-device (HOD) measurement. Vacuum level shift (δ) mentioned by ultra-violet photoelectron spectroscopy (UPS) analysis. The red arrows demonstrate the difference between the hole and electron injection barriers

Discussion

In this work, we combined ampicillin with PEDOT:PSS to enhance the performance of OLEDs. With an increase in the concentration of ampicillin in PEDOT:PSS, a decrease in the φ was analyzed. The presence of primary, secondary, and tertiary -NH2 along with the lactam ring in the ampicillin’s molecular structure provided a specific charge distribution, which resulted in an interfacial dipole with high magnitude. With 25% ampicillin addition, a strong horizontal interfacial dipole, efficient J-aggregations and enhanced charge balance was achieved in the OLED devices. In particular, we measure a CE of 120 cd A−1, EQE of 35% and PE of 70 lmW−1, which to our knowledge is among the highest reported performances for green ph-OLEDs. The achieved high-device efficiency was cross-evaluated with penicillin-based (without primary -NH2) devices. We observed that the penicillin-based devices showed an EQE of ~ 24%, which was ~ 11% less than the ampicillin-based devices (35.1%). Hence, it could be concluded that the enhanced performance by ampicillin-PEDOT:PSS device was due to the presence of horizontal interfacial dipole and exciton emission from J-aggregations. Comparable device efficiencies were observed for 40% ampicillin-PEDOT:PSS devices as well, however, the ampicillin’s crystallization caused strong deviations in the obtained results. On the other hand, 25% ampicillin-PEDOT:PSS devices showed a quite stable performance, which makes this concentration preferable for OLED applications. A wide range of properties obtained by the combination of ampicillin in PEDOT: PSS represents a significant advance towards the fabrication of highly efficient biocompatible AIs, optoelectronic, and biomedical devices.

Methods

ITO glass substrate cleaning and surface treatment

The patterned ITO glass substrate was cleaned by acetone and isopropyl alcohol (IPA) for 10 min using sonication at 40 kHz. ITO substrate was boiled in IPA for 15 min and finally treated with ultraviolet-ozone (254 nm) for 20 min. The sheet resistance of ITO substrate was 15 Ω sq−1.

Ampicillin preparation with PEDOT:PSS

Ampicillin aqueous solution was prepared by dissolving 50 mg ampicillin powder (Purchased from VWR AMRESCO, 99.0% purity, USP Grade) in 1 ml of SDIW. The 1-D (one-time distilled) SDIW was prepared by sterilizing the DIW in an autoclave equipment at 121 °C for 15 mins. The SDIW was with a neutral pH (~ 7.5) and a resistance of ~0.18 MΩ cm. Ampicillin dissolved SDIW solution was filtered using 21 µm size meshed filter, which could screen out unwanted biomaterials with even very small sizes (i.e., < 40 µm). The filter was also utilized to remove the ampicillin crystals formed by variations in the pH of the solution. Different concentrations (25%, 40%, and 75% with volume ratios of 1 ml:3 ml, 2 ml:3 ml, and 3 ml:1 ml, respectively) of ampicillin solution was added to PEDOT:PSS (CLEVIOS P VP AL 4083, Heraeus). Devices with lower concentrations (2–15%) of ampicillin in PEDOT:PSS were also fabricated using the same forward device structure for comparison purposes. The amounts and ratios of all concentrations from 2 to 75% of ampicillin in PEDOT:PSS have been presented in Supplementary Fig. 13. Further, during the preparation of ampicillin-PEDOT:PSS, 25–40% solutions exuded an ammonia-like smell, whereas 75% solution did not exhibit any kind of smell. This indicated the extent of evaporation or removal of CO2 gas molecules in such solutions. Moreover, the device performances are quite dependent on the pH of the ampicillin-PEDOT: PSS solution status and should be properly monitored for reproducibility of the results. The penicillin solution was also prepared using the same method mentioned above.

OLED device fabrication

In all, (0–75%) ampicillin-PEDOT:PSS as a hole injection layer was spin coated onto the cleaned ITO glass with a spin speed of 4000 rpm for 30 s and baked at 120 °C for 10 min. NPB as HTL (~ 20 nm) was deposited by thermal evaporation with a base pressure of 5.0 × 10−8 torr. TCTA as an exciton blocking layer with thickness 10 nm was deposited on NPB. CBP and Ir(ppy)3 (15 nm, 8% doping) were combined as a thin EML (15 nm). This EML has been reported to have a random orientation,62 therefore does not have a critical effect in our work. TPBi (20 nm) was deposited as an ETL layer and the effect of ETL thickness on the charge balance has been investigated before.63 The thin EML usually requires a thin ETL for the optimized charge balance or better device performance, and vice versa. It was observed that low thicknesses (< 50 nm) were preferable for better device performance owing to the exciton confinement while the high thickness (> 50 nm) resulted in an efficiency roll-off. LiF/Al cathode was patterned on ETL using shadow masks (4 mm2) by thermal evaporation with a base pressure of 5.0 × 10−8 torr. The deposition rates were fixed to 0.2 Å s−1 and 8 Å s−1 for the LiF and Al electrodes. LiF and Al thicknesses were 1 nm and 120 nm, respectively, which were analyzed using crystal quartz and re-confirmed using the surface profiler. The tooling process was introduced in Supplementary Fig. 14, and three kinds of different evaporators were utilized to confirm the reproducibility of the device performance. The penicillin-based OLED devices were also prepared using the same method mentioned above.

XPS/UPS analysis

XPS (AXIS-NOVA, Kratos. Inc.) with monochromatic Al-Kα (1486.6 eV) radiation as a photon source with a hemispherical analyzer was employed to investigate the bonding of the species (C-1s, N-1s, and S-2p) in the sample (base pressure = 1 × 10−9 torr). The resolution of the electron analyzer was 0.47 eV as measured from the full width at half maximum (FWHM) of the Ag 3d5/2 peak. The binding energy of XPS spectra was calibrated by the position of C-1s (285.0 eV) of adventitious carbons in the air. High-resolution XPS spectra were obtained using an analysis area of 400 μm of the 40 eV pass energy with an energy step of 0.05 eV. UPS with an excitation energy of He I (21.2 eV), which is integrated with XPS, was performed to characterize the electronic structure of the PEDOT:PSS. The UPS spectra were obtained using the sample biased at − 15.0 V to clear the secondary cutoff. An energy resolution in UPS of 0.05 eV was determined from the slope of the Fermi edge of a cleaned polycrystalline Au surface.

AFM analysis

The surface morphology of ampicillin-PEDOT:PSS layers was analyzed with a multimode 8 AFM (Bruker) equipped with a Nanoscope V controller. We used Al coated silicon probe (NCHR, Nanoworld, Germany) with a nominal spring constant of 40 Nm−1 and a resonance frequency of 320 kHz. All images were obtained in tapping mode AFM at room temperature, with 384 × 384 pixels in a 3 × 3 μm of scan size at a scan rate of 1 Hz.

XRD analysis

The structural characteristics of the samples were measured using a PANalytical X’Pert PRO-MPD XRD equipped with X-ray mirrors (as an incident and a diffracted optics), and operated with Cu–Kα radiation at 40 kV and 30 mA. The crystallite size of the samples was determined by means of XRD, using the Scherrer equation (\(L = \frac{{K\lambda }}{{\beta \cos \theta }}\)).

HR-TEM analysis

Structural properties of 25% ampicillin-PEDOT:PSS layers were analyzed using HR-TEM with JEOL-ARM 200 F (JEOL, USA Inc,) microscope operating at 200 kV with a point-to-point resolution of 0.19 nm.

Optical Properties (transmittance and absorption analysis)

UV-vis spectrophotometer (JASCO V-570) was utilized for light transmittance and absorbance spectra.

HPLC and NMR analysis

The samples were analyzed by reverse-phase HPLC conducted under the following conditions: the reaction samples were applied to a Mightysil RP-18 GP column (4.6 × 250 mm, 5 μm; KANTO Reagents, Japan), elution of ampicillin-PEDOT:PSS (0–20 min, 75–0% B and 20–25 min, 0–75% B; where A = water containing 0.1% trifluoroacetic acid and B = Acetonitrile) was monitored at 259 nm, at a flow rate of 0.5 mL min−1 at 30 °C. HPLC analysis was beneficial for analyzing molecules with low molecular weight such as ampicillin. Even though, gas-pressure chromatography)64 would have been beneficial to characterize large molecule weight polymers such as PEDOT:PSS but, we could observe the -PSS peak by HPLC and a minor shift in retention time as well by the addition of ampicillin.

For proton (1H) NMR, crude samples of 75% ampicillin-PEDOT:PSS were dried by lyophilization and dissolved in dimethyl sulfoxide-d6 followed by centrifugation at 12,000 rpm to remove the insoluble components. NMR was performed to clarify the structures of both samples. NMR was performed using Varian Unity Inova 300 MHz spectrometry (Varian, USA) with a TCI CryoProbe (5 mm) and the data were analyzed by TopSpin 3.1 (Bruker) and MestReNova 8.0 (Mestrelab Research S. L., Spain) software.

TRPL/TRANES analysis

Picosecond TRPL/TRANES measurements were conducted using commercial fluorescence lifetime measurement system (Hamamatsu streak camera, C11200). A commercial optical parametric amplifier (TOPAS-prime, Light-Conversion) seeded with a commercial regenerative amplifier system (Spitfire-Ace, Spectra-Physics) operating at 1 KHz was utilized as the light source. FWHM of the instrumental response function were ~ 20 ps in a 1 ns time window. All data were obtained in single photon counting mode using the Hamamatsu U8167 software.

Ellipsometry with refractive index and S-factor analysis

The refractive index and extinction coefficient for S-factor were investigated using spectroscopic ellipsometry (SE) of V-VASE (J.A. Woollam) with rotating analyzer system, in the wavelength range from 410 to 700 nm, and incident angles of 65°, 70°, and 75°. To calculate the S-factor, we performed anisotropic optical modeling (uniaxial model) in which the x–y plane and the z axis were considered to have different dielectric function properties. In addition, the optical model and the best-fit parameter values were calculated using the WVASE32 software (J.A. Woollam). Finally, based on the results of SE analysis, we calculated the molecular orientation parameter S using the following equation:

$$S = {\frac{3}{2}}\left\langle {{\cos}^{2}\, {\theta} } \right\rangle - {\frac{1}{2}} = {\frac{{k_{e}} - {k_{o}}}{{k_{e}} + {2k_{o}}}}$$

OLED device performance analysis

The J–V was analyzed using the probe station and Electroluminescence (EL) measurements were conducted using a Keithley 2400 voltmeter and Minolta CS-2000 spectrometer. For viewing angle measurement, the device performance (Luminance) was obtained by automatic rotating the device holding jig (stage) at various angles 0–70° with a regular interval of 5° (Supplementary Fig. 15). To avoid the OLED degradation after consecutive measurements from 0 to 70° and 70 to 0° (at each 5° angle variation), average values were taken for analysis and multiplied with cosθ in accordance to Lambertian cosine law (I = I0.cosθ)65. The obtained luminance from devices (solid lines) was plotted against the ideal Lambertian curve, which indicated that a near-perfect Lambertian (uniform) luminance.

Integrating sphere analysis

The EQE of the devices were cross-analyzed using integrating sphere, total luminance flux measurement system (Otsuka half-moon (HM) series) with constant voltage one-point measurement, (at 7 ± 1 V). The EL of OLEDs was measured at room temperature in a controlled voltage (C–V) mode and integration time of 5 s. The spectrometer (LE-5400) CCD type, TE-cooled (350–930 nm) with 6” hemi sphere having coating reflectance of 98% (spectraflect) were utilized. (Supplementary Fig. 15).

Conductivity measurement

A thick layer (~ 1 µm) of ampicillin-PEDOT:PSS was prepared on a glass substrates using the drop casting method. The conductivity was analyzed at a constant current of 100 nA using 4-probe source measurement units (Keithly 236 source, 700 switch system, 6485 picoammeter by Jeong Yeon Systems, Korea).

Optical microscope

The surface morphology of the spin coated samples of ampicillin-PEDOT:PSS were analyzed using optical microscope (KSM-BA3T, Samwon scientific Ind. Co. Ltd., Korea)

Device lifetime measurement

The devices were encapsulated using a glass or acrylic adhesive tape before measurement. The analysis was conducted using an OLED lifetime test system (M6000, McScience Inc., Korea) enclosed in a chamber with controlled temperature and humidity. The tool provides multi-channel testing frame with various control mode power driving. The samples were analyzed at 1000 cd m−2 until 50% drop in device performance was observed.

CA analysis

The CA was analyzed using the smart drop standard (FEMTOBIOMED, South Korea) and this system uses the GEM ‘single non-approximated algorithm numerical calculation of Bash forth-adams equation.

pH value measurement

The pH value was analyzed using the MP511 of pH meter (SANXIN, China) and 201 T pH measuring electrode with an automatic temperature compensation function for a three-in-one electrode.