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. 2021 Dec 30;7(1):844–862. doi: 10.1021/acsomega.1c05504

Bithieno Thiophene-Based Small Molecules for Application as Donor Materials for Organic Solar Cells and Hole Transport Materials for Perovskite Solar Cells

Alvina Rasool †, Saba Zahid †, Muhammad Ans †,*, Shabbir Muhammad ‡, Khurshid Ayub §, Javed Iqbal †,∥,*
PMCID: PMC8757340  PMID: 35036751

Abstract

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This quantum mechanical study focuses on the designing of twelve (MPAM1–MPAM12) bithieno thiophene (BTTI) central core-based small molecules to explore optoelectronic properties as donor candidates for organic solar cells (OSCs) and hole transport materials (HTMs) accompanied by enhanced charge mobility for perovskite solar cells (PSCs). MPAM1–MPAM6 have been designed by the substitution of thiophene-bridged end-capped acceptors on both side terminals of reference (MPAR). MPAM7–MPAM12 are tailored by adopting the same tactic on one side terminal only. MPW1PW91/6-311G (d,p) has been employed for all computational simulations. MPAM12 revealed the highest λmax at 639 nm in dichloromethane (DCM) solvent with the lowest Eg of 1.78 eV and dipole moment (20.74 D) in the solvent phase, showing excellent miscibility as compared to the reference. All designed chromophores (MPAM1–MPAM12) demonstrated higher estimated VOC and power conversion efficiency (PCE) when compared to MPAR, suggesting their prominent operational efficiency. Among all, MPAM4 manifested the highest PCE (47.86%). MPAM2 portrayed the highest electron mobility (0.0041573 eV) and MPAM3 exhibited the highest hole mobility (0.0047178 eV). The outcomes highlight the adequacy of the planned strategies, paving a new route for the development of small-molecule HTMs for PSCs and donor contributors for OSCs.

1. Introduction

The skyrocketing energy consumption appears to be a major stumbling blockage in satisfying the requirements of a dynamically developing world population. Although fossil fuels provide 80 percent of the world’s energy needs, burning of carbonaceous stores produces tons of CO2, which contributes to global warming. Scientists are progressively keen on finding amiable and sustainable wellsprings of energy that have a continuous and sustainable impact on the economy as energy utilization increases.1 The photovoltaic effect (first discovered in 1839 by Edmund Becquerel) is one of the best tools for converting the sun’s inexhaustible energy into electricity.2 Different technologies are based on this principle, organic photovoltaics (OPVs) being the dominant one, thanks to their minimal expense potential, semitransparency, and adaptability.3 They made use of light-capturing organic materials that could be synthesized.4−6 Until recently, inorganic silicon-containing solar gadgets were considered to be the most useful and productive constituents for solar cell assembly. Because of their rigid design, low proficiency, and high cost, their applications have been severely limited.7

As a solution to energy crisis, OPVs have attracted a great deal of attention. OPV systems are thought to be more compelling due to their flexible and tunable energy levels. In addition, OPVs’ surface morphology makes them more absorbent, and their high purity makes them more productive than inorganic alternatives.3,8 The working efficiency of fullerene organic solar cells (OSCs) has grown by 11.7% over the past few decades.9 However, due to poor absorption in the visible region, small band gaps, and expensive sanitization and assembly, the non-fullerene (NF) alternative options got the lead in the last few decades.10−13 The high synthetic flexibility, full spectral coverage, ease of structural adaptability, tunable optoelectronic properties, and low voltage losses of NFAs satisfied the shortages as well as empowered to accomplish the power conversion efficiencies (PCEs) of over 17 percent.13−20

Furthermore, the general problem regarding OSCs is efficiency that is much lower than that of inorganic-based devices, which is a major flaw at the moment. The reason for this is that organic semiconductors have a substantially larger band gap than inorganic semiconductors.21 That is why researchers and industry have recently become engaged in perovskite solar cells (PSCs) composed of metal halide because of their interesting photophysical properties, high operational efficiency, and considerable potential in terms of low-cost assembling techniques.22,23 The tremendous instability of high yielding perovskite devices toward air, water, moisture, light, and heat might be owing to instability in both the perovskite and transporting layers.24 The lack of stability caused by frequently employed hole transport materials (HTMs) with dopants is one hurdle for marketing of PSCs. These hygroscopic dopants not only degrade long-term stability by allowing moisture and ion diffusion but also add to the complexity and total expense. As a result, the development of dopant-free HTMs is extremely important. As a result, the focus of this research is on selecting appropriate organic materials for use as HTMs in solar cell technology.25 Dopant-free bithieno thiophene (BTTI) central core-based HTMs are highly anticipated for their potential to provide PSCs with good consistency and long-term durability. Due to the more expanded and conjugated system, MPA-BTTI adopted an H-aggregation style, resulting in more efficient charge transportation and better hole mobility. With a root-mean-square (rms) roughness of 0.44 nm, the MPA-BTTI film had a considerably smoother surface.26 Due to the low hysteresis, improved thermal stability, and long-term stability, the MPA-BTTI-based dopant-free PSCs achieve a phenomenal efficiency of 21.17 percent.27 The MPA-BTTI’s film morphology and well-aligned energy levels are credited with this accomplishment. MPA-BTTI showed tremendous energy-level synchronization with the perovskite layer, suitable hole transport, and brilliant film shape.28

Twelve small donor molecules (MPAM1–MPAM12) have been drafted by thiophene-bridged end-capped acceptor engineering of already synthesized MPA-BTTI taken as reference (MPAR) in the current study. The methoxy group of MPAR has been substituted with different acceptor moieties in all designed molecules. Herein, cyano-, fluoro-, and carbonyl-containing thiophene-bridged acceptor moieties have been substituted in the MPAR-conjugated framework to tune its optoelectronic properties. Cyano, fluoro, and carbonyl groups have potential to congest the band gap, escalate the molecular conjugation, and push the absorption toward a longer wavelength by attaching to the conjugated framework of the molecule.29 All reported molecules constitute 4-methoxy-N-(4-methoxyphenyl)-N-phenylaniline as the donor and imide-based thiophene derivative as the acceptor moiety. The phenylamine empowers productive hole transport, while the imide-functionalized centers guarantee great intermolecular π–π stacking because of their planar molecular layout. The foundation of the acceptor moiety is 2,2′-bithieno[3,2-b]thiophene to tune subatomic arrangements along with resultant optoelectronic and film morphological properties. In MPAM1–MPAM6, thiophene-bridged end-capped acceptor engineering has been performed on both side terminals of MPAR, while in MPAM7–MPAM12, the structural alteration has been performed on one side terminals only, as shown in Figure 1. This paper describes many design concepts for high-performance small donor molecules for proficient OSCs and productive HTMs for PSCs, which display similar optoelectronic properties, but different molecular configuration and film properties, in a synergistic manner. A new route for building high-performance dopant-free HTMs in PSCs has been opened by the results, which confirm the usefulness of designed strategies.

Figure 1.

Figure 1

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Molecular structures of the reference (MPAR) and devised molecules (MPAM1–MPAM12).

2. Results and Discussion

In this current report, first, the absorption profile of the model molecule (MPAR) was computed via the five DFT functionals (B3LYP, CAM-B3LYP, MPW1PW91, PBEPBE, and WB97XD) in the gaseous phase (Figure 2a) and DCM solvent, as displayed in Figure 2b. The λmaxcal of the reference molecule (MPAR) achieved by MPW1PW91 (596 nm) under 6-311G (d,p) show precise compromise with λmaxexp (532 nm),27 as displayed in Figure 3. Therefore, all computational simulations of all freshly designed molecules have been carried out via MPW1PW91/6-311G (d,p).

Figure 2.

Figure 2

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UV–vis spectra of MPAR at five different DFT functionals using 6-311G (d,p) in (a) gas (b) DCM.

Figure 3.

Figure 3

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Comparative analysis of absorption in the bar chart of reference (MPAR) at five different DFT functionals.

2.1. Structural Optimization, Dihedral Angle (θ), and Bond Length (d)

Molecular geometry has a notable impact on optoelectronic properties.30 The optimally selected DFT functional has been used to optimize the model molecule (MPAR) together with the currently designed molecules (MPAM1–MPAM12). Figure S1 (in the Supporting Information) shows the optimized framework of all reported chromophores. The optimized geometry is manifesting that the central acceptor core has arrayed itself in one plane, while the thiophene bridge alongside acceptor units have lined up themselves out of the plane to limit the potential energy surface.

Examined dihedral angles (θ) and bond lengths (d) of chromophores are illustrated in Scheme 1.

Scheme 1. Calculated Bond Angle (θ) and Bond Length (d) of Molecules.

Scheme 1

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Herein, θ1 and d1 are the dihedral angle and bond length between the TPA moiety and thiophene bridge, respectively, whereas θ2 and d2 are the dihedral angle and bond length between the thiophene spacer and acceptor group, respectively. It is evident from Table 1 that values of bond length d1 and d2 lie in the range of 1.36–1.46 and 1.41–1.43 Å, respectively, commending the presence of double and triple bonds leading to aggrandized conjugation. The reduced values of θ2 in all chromophores (MPAR–MPAM12) are authorizing the planarity in the optimized geometries gained by the acceptor moieties. The significant change in θ2 as compared to θ1 is due to the possibility of free rotation in less sterically restricted acceptor moieties attached to the thiophene bridge.

Table 1. Computed Dihedral Angle (θ) and Bond Length (d) of Molecules (MPAR–MPAM12).

molecules θ1 (deg) θ2 (deg) d1 (Å) d2 (Å)
MPAR 61.34 0.34 1.36 1.41
MPAM1 24.48 0.64 1.46 1.42
MPAM2 24.74 0.61 1.46 1.42
MPAM3 23.98 0.60 1.46 1.43
MPAM4 24.50 0.88 1.46 1.42
MPAM5 25.16 0.90 1.46 1.43
MPAM6 23.42 0.72 1.45 1.41
MPAM7 24.28 0.65 1.46 1.42
MPAM8 24.60 0.61 1.46 1.42
MPAM9 23.84 0.64 1.46 1.43
MPAM10 25.08 1.02 1.46 1.42
MPAM11 25.09 0.87 1.46 1.43
MPAM12 22.99 0.69 1.45 1.41
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2.2. Quantum Mechanical Descriptors

Chromophore orbitals with the highest occupied (HOMO) and lowest unoccupied (LUMO) energies have a considerable effect on the charge transport, electronic, and absorption attributes.31−33 Charge transport and electronic density distribution patterns are characterized by Frontier molecular orbitals (FMOs).34−39 A molecule accompanied by a small band gap is highly polarizable and has low kinetic stability but great chemical reactivity (i.e., it is a soft molecule).40

To study the effect of the thiophene moiety and different end-capped acceptors on photophysical properties of studied molecules MPAR and MPAM1–MPAM12 HOMO and LUMO energy levels along with their band gaps (Eg) are studied at elected functionals and their values are illustrated in Table 2. MPAR reflects an Eg of 2.54 eV with HOMO and LUMO energy levels of −5.01 and −2.47 eV, respectively. HOMO and LUMO levels of all designed chromophores (MPAM1–MPAM12) are low lying in energy as compared to MPAR. Among chromophores (MPAM1–MPAM6) in which additional modification is executed on both side terminals of reference, MPAM5 (2.07 eV) and MPAM6 (2.38 eV) disclosed narrow Eg. All chromophores (MPAM7–MPAM12) in which morphological transformation is implemented on our model molecule revealed a reduced band gap (Eg) within the limit of 1.78–2.45 eV, as displayed in Figure 4. A significant decrease in Eg is attributable to strong electron-withdrawing end-capped groups that shift the electron density from HOMO to LUMO. MPAM12 has conveyed the lowest value of 1.78 eV owing to the cyano group-containing strong acceptor moiety (2-ethylidene-1,3-dioxo-2,3-dihydro-1H-indene-5,6-dicarbonitrile). Hence, it is inferred that end-capped alteration on one side terminal of MPAR is the best strategy to acquire excellent photophysical properties.

Table 2. Computed HOMO and LUMO Energies, Band Gap (Eg), Ionization Potential, and Electron Affinity.

molecules HOMO (eV) LUMO (eV) Eg (eV) IP (eV) EA (eV)
MPAR –5.01 –2.47 2.54 5.68 1.45
MPAM1 –5.73 –3.11 2.62 6.26 2.64
MPAM2 –6.03 –3.20 2.83 6.12 2.43
MPAM3 –5.85 –3.06 2.79 6.13 2.48
MPAM4 –6.18 –3.55 2.63 6.55 2.79
MPAM5 –5.92 –3.85 2.07 6.30 2.43
MPAM6 –6.35 –3.97 2.38 6.59 3.23
MPAM7 –5.20 –3.05 2.15 5.96 2.33
MPAM8 –5.17 –2.86 2.31 5.90 2.17
MPAM9 –5.19 –2.89 2.30 5.90 2.20
MPAM10 –5.37 –3.24 2.13 6.07 2.42
MPAM11 –5.33 –2.88 2.45 5.97 2.14
MPAM12 –5.38 –3.60 1.78 6.09 2.88
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Figure 4.

Figure 4

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Graphical representation of band gap (a) for MPAR and MPAM1–MPAM6 molecules (b) for MPAR and MPAM7-MPAM12.

FMO plots (Figure S2 in the Supporting Information) and individual energy levels of studied molecules (MPAR–MPAM12) are shown in Figure 5. The red and green color symbolizes the positive and negative charge, respectively.41 The donor unit is symbolized by HOMO and the acceptor is represented by LUMO. HOMO electronic density of the model molecule (MPAR) is completely populated on the central core and TPA donor portion, while LUMO is inhabited on the electron-withdrawing central core.

Figure 5.

Figure 5

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3D graphical representation of HOMO and LUMO (a) for MPAR and MPAM1–MPAM6 molecules (b) for MPAR and MPAM7–MPAM12.

The FMO pattern of MPAM1–MPAM6 seems to be similar. In these molecules, HOMOs are majorly populated on the central acceptor core and TPA donor fragment and partially concentrated on the bridge moiety, while LUMOs are assembled partially on the TPA donor moiety, completely on the bridge and end-capped acceptors. In the case of MPAM5, LUMO is colonized utterly on the central core, minorly on the donor, bridge, and acceptor moiety. FMO distribution of MPAM7–MPAM12 is quite similar in such a way that their HOMOs are inhabited completely on the central core and TPA unit, while LUMOs are populated entirely on bridge and acceptor units, partially on thiophene bridge units. HOMO electronic cloud is primarily diffused on the donor moiety, and LUMO electronic cloud is scattered on thiophene bridge and acceptor units.

2.3. Ionization Potential and Eelectron Aaffinity

Trademark boundaries to investigate the charge transmission nature are ionization potential (IP) and electron affinity (EA). Both IP and EA are equivocally associated with one another. Proficient charge transfer is characterized by chromophores exhibiting the greater value of EA and lower IP. Chromophores with electron-donating groups have low IP because of the destabilization of the HOMO energy level, hence accelerating the easy removal of electrons during charge transfer. Contrarily, molecules accompanied by electron-withdrawing groups possess a high value of IP due to stabilization of HOMO. IP and EA values of all investigated molecules (MAPR and MPAM1–MPAM12) evaluated using eqs 1 and 2 are summarized in Table 2.

2.3. 1
2.3. 2

Among all designed molecules, MPAM8 and MPAM9 possess low IPs of 5.90 eV each because of their high-lying HOMO levels. The highest IP (6.59 eV) is exhibited by MPAM6 credited to its low energy HOMO. As all newly architecture molecules are tailored by acceptor moiety modification, they reveal a high value of EA as compared to reference MPAR, thus promoting charge transfer, as illustrated in Table 2.

2.4. Absorption Profile

Harvesting and absorption of light energy are the central parameters that have gained momentum in photocurrent generation. The UV–visible spectra provide an insight into the electronic excitations and charge transfer analysis, so UV–visible spectra should be evaluated.9,42 The absorption profile of newly engineered molecules (MPAM1–MPAM12) was computed via the selected optimal DFT functional in the gaseous (Figure 6a) and solvent [dichloromethane (DCM)] phase as expressed in Figure 6b. The employment of solvent has red-shifted the λmax owing to the stabilization of delocalized π electrons. In the present investigation, the absorption profile by employing the TD-DFT calculations in the IEFPCM model has been pictured as the results have been reported in Tables 3 and 4, respectively.

Figure 6.

Figure 6

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UV–vis spectra of reference (MPAR) along with devised molecules (MPAM1–MPAM12) at MPW1PW91/6-311G (d,p) in (a) gaseous phase and (b) DCM.

Table 3. Calculated Absorption Maximum (λmaxcal), Binding Energy (Eb), Band Gap (Eg), Highest Oscillator Strength (f), Light-Harvesting Efficiency (LHE), and Major Molecular Transitions of the Reference (MPAR) and Devised Moieties (MPAM1–MPAM12) in the Gaseous Phase.

molecule λmaxcal (nm) λmaxexp (nm) Eb (eV) Eg (eV) F LHE major molecular transitions
MPAR 564 532 0.34 2.54 1.61 0.975 H → L (70%)
MPAM1 548   0.36 2.62 2.34 0.995 H → L (48%)
MPAM2 547   0.56 2.83 2.54 0.997 H → L (46%)
MPAM3 551   0.54 2.79 2.54 0.997 H → L (31%)
MPAM4 534   0.31 2.63 2.13 0.993 H → L (56%)
MPAM5 533   –0.25 2.07 2.35 0.995 H → L (66%)
MPAM6 575   1.07 2.38 1.73 0.981 H → L (47%)
MPAM7 544   –0.12 2.15 1.25 0.943 H → L (70%)
MPAM8 575   0.16 2.31 1.35 0.955 H → L (68%)
MPAM9 577   0.15 2.30 1.10 0.920 H → L (61%)
MPAM10 570   –0.04 2.13 1.14 0.927 H → L (70%)
MPAM11 576   0.30 2.45 1.36 0.956 H → L (70%)
MPAM12 586   –0.36 1.78 1.55 0.971 H → L (71%)
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Table 4. Calculated Absorption Maximum (λmaxexp), Binding Energy (Eb), Band Gap (Eg), Highest Oscillator Strength (f), Light-Harvesting Efficiency (LHE), and Major Molecular Transitions of the Reference (MPAR) and Devised Moieties (MPAM1–MPAM12) in DCM.

molecules λmaxcal (nm) λmaxexp (nm) Eb (eV) Eg (eV) f LHE major molecular transitions
MPAR 596 532 0.46 2.54 1.68 0.980 H → L (70%)
MPAM1 588   0.51 2.62 2.63 0.997 H → L (47%)
MPAM2 575   0.67 2.83 2.70 0.998 H → L (52%)
MPAM3 570   0.62 2.79 2.45 0.996 H → L (44%)
MPAM4 562   0.17 2.63 2.27 0.995 H → L (58%)
MPAM5 556   –0.16 2.07 2.35 0.995 H → L (57%)
MPAM6 651   0.48 2.38 2.45 0.996 H → L (50%)
MPAM7 600   0.08 2.15 1.37 0.957 H → L (64%)
MPAM8 593   0.22 2.31 1.34 0.954 H → L (51%)
MPAM9 582   0.17 2.30 0.93 0.882 H → L (54%)
MPAM10 565   –0.06 2.13 0.42 0.619 H → L (68%)
MPAM11 561   0.24 2.45 0.39 0.592 H → L (63%)
MPAM12 639   –0.16 1.78 1.42 0.961 H → L (69%)
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The absorption profile illustrates that among all newly devised molecules, MPAM6, MPAM7, and MPAM12 are accompanied by a higher λmaxcal value than the model molecule (MPAR) in DCM. The λmax value is in strong alliance with the band gap. The lower the band gap, the more will be the λmax value. The absorption profile supports the fact that MPAM6 and MPAM12 are accompanied by cyano-containing (2-ethylidene-1,3-dioxo-2,3-dihydro-1H-indene-5,6-dicarbonitrile) strong electron-pulling moieties. Cyano and carbonyl groups serve as electron-capturing moieties to facilitate the charge transmission from donor to acceptor.

Cyano, fluoro, and carbonyl groups also escalate the molecular conjugation and push the absorption toward a longer wavelength by attaching to the conjugated framework of the molecule. MPAM7 has also displayed a higher λmaxcal value than the model molecule (MPAR) due to the presence of carbonyl- and fluoro-containing (2-ethylidene-5,6-difluoro-2H-indene-1,3-dione) strong electron-pulling moieties. Cyanide, fluorine, and carbonyl groups augment the photovoltaic activity of the device by lowering the energy of FMOs.

From the absorption profile, it is overall illustrated that molecules (MPAM7–MPAM12) accompanied by electron-withdrawing moieties on one side terminals exhibit a higher λmaxcal value and lower band gaps as compared to molecules (MPAM1–MPAM6) having electron-withdrawing moieties on both side terminals, as displayed in Figure 7.

Figure 7.

Figure 7

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UV–vis spectra at MPW1PW91/6-311G (d,p) in DCM (a) of MPAR along with devised molecules MPAM1–MPAM6 (b) of MPAR and MPAM7–MPAM12.

In the present quantum simulation, the first excitation energy has been calculated using the selected functional in both gas and solvent medium as the results have been displayed in Figure 8. The first excitation energy is the amount of energy necessary for the electrons to excite from the ground to the first excited state. Excitation energy is in direct alliance with the band gap energy. The lower the band gap value, the lower will be the excitation energy and more considerable will be the excitation of electrons from the ground to the excited state. More excitation of electrons leads to efficient charge transfer and hence results in intensified photocurrent generation.

Figure 8.

Figure 8

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Graphical representation of the first excitation energy (eV) (a) for MPAR and MPAM1–MPAM6 molecules (b) for MPAR and MPAM7–MPAM12.

In the current report, all reported molecules have manifested a higher value of excitation energy in the gas phase as compared to the solvent phase, as displayed in Figure 8. The higher values of excitation energy of molecules in the gas phase are advocating the fact that freshly planned molecules have greater miscibility in the solvent (DCM) and more charge transfer, hence proving that all reported molecules are solution-processable molecules responsible for the augmented photocurrent generation.

Another essential technique to examine the optical utility of the investigated compounds is the light-harvesting efficiency (LHE). LHE is computed through the oscillatory strength (f) value and represents the compound photocurrent response.43

2.4. 3

LHE is in direct relation with the f value. Compounds accompanied by large LHE values manifest large photocurrent responses and vice versa. LHE of currently reported structures in both gas and solvent medium has been calculated using eq 3,43 and the results have been summarized in Tables 3 and 4, respectively. A pronounced shift in LHE values of newly devised structures has been observed by structural modifications. Among all reported structures, MPAM1–MPAM6 having structural tailoring at both side ends are accompanied by higher f and LHE values, which is attributed to their augmented photocurrent generation.

2.5. Quantum Chemical Parameters

To scrutinize the chemical reactivity and kinetic stability of newly engineered molecules, different chemical parameters have been calculated and results have been summarized in Table 5.

2.5. 4

Table 5. Chemical Potential (μ), Chemical Hardness (η), Chemical Softness (S), Electronegativity (χ) and Electrophilicity Index (ω), and Total Amount of Charge Transfer (ΔNmax) of Reference (MPAR) and Newly Engineered Molecules (MPAM1–MPAM12).

molecules μ (eV) η (eV) S (eV) χ (eV) ω (eV) ΔNmax (e)
MPAR –3.74 1.27 0.79 3.74 5.51 2.94
MPAM1 –4.42 1.31 0.76 4.42 7.46 3.37
MPAM2 –4.61 1.42 0.70 4.61 7.48 3.24
MPAM3 –4.46 1.40 0.71 4.46 7.10 3.19
MPAM4 –4.87 1.32 0.76 4.87 8.98 3.69
MPAM5 –4.89 1.04 0.96 4.89 11.50 4.70
MPAM6 –4.86 1.19 0.84 4.86 11.19 4.08
MPAM7 –4.13 1.08 0.93 4.13 7.90 3.82
MPAM8 –4.02 1.16 0.86 4.02 6.97 3.47
MPAM9 –4.04 1.15 0.87 4.04 7.10 3.51
MPAM10 –4.31 1.07 0.93 4.31 8.68 4.03
MPAM11 –4.11 1.23 0.81 4.11 6.87 3.34
MPAM12 –4.49 0.89 1.12 4.49 11.33 5.04
PC61BM –4.90 1.20 0.83 4.90 10.00 4.08
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Equation 4(44) has been used for calculating chemical potential. Chemical potential describes the electronic cloud escaping capability.45 The freshly designed molecules are accompanied by higher values of negative chemical potential indicating that they are highly reactive and stable compounds hence cannot decompose easily. The designed molecules exhibit a greater value of chemical potential than PC61BM indicating that they have a greater ability to donate electrons.

2.5. 5
2.5. 6

Chemical hardness and softness values calculated using eqs 5 and 6,44 respectively, demonstrate that among all reported molecules, MPAM5–MPAM12 are soft molecules accompanied by the lowest band gaps and enhanced chemical reactivity, while MPAM1–MPAM4 molecules are relatively hard molecules accompanied by enhanced kinetic stability owing to their increased band gaps than the reference (MPAR).

2.5. 7
2.5. 8

Electronegativity and electrophilicity index values have been simulated using eqs 7 and 8,44 respectively. Both are usually correlated and quantitatively explain the electron-accepting nature of molecules.45 All designed molecules have manifested higher values of the electronegativity and electrophilicity index than the reference (MPAR) advocating the fact that newly designed molecules are accompanied by strong electron-withdrawing moieties. All reported molecules are accompanied by low values of the electronegativity and electrophilicity index as compared to PC61BM indicating that they have less ability to attract electrons from PC61BM and behave as an electron donor.

The total amount of charge transfer is another parameter to scrutinize the charge-transferring capability of all freshly planned molecules, calculated using eq 9.46 The summarized results in Table 5 have shown that all newly engineered molecules have a greater ability to transfer charge than the reference (MPAR). Keeping in view the abovementioned discussion, the freshly designed molecules ought to be focused to prepare elite materials for future proficient solar devices.

2.5. 9

2.6. Density of State Analysis

FMO results have been assured via Mulliken charge distribution. The density of state (DOS) analysis expresses the contribution of the molecular fragment in raising the bonding (HOMO) and antibonding (LUMO) molecular orbitals. DOS calculations also compute the energies of HOMO and LUMO.47−49 The DOS simulations were computed at the selected DFT functional for MPAR and MPAM1–MPAM12 and transfigured via PyMolyze 1.1. To study DOS, MPAR is partitioned into donor (red color) and core (green color) sections, while all other designed molecules MPAM1–MPAM12 are fractioned into four segments acceptor, spacer, TPA donor, and core presented by red, green, blue, and pink colors, respectively, in DOS plots, as illustrated in Figure 9. Negative and positive values along the x-axis in DOS diagrams address HOMO and LUMO values, respectively, while the energy difference between them represents band gap.

Figure 9.

Figure 9

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DOS graphs of reference (MPAR) and devised molecules (MPAM1–MPAM12).

Table 6 outlines the role of different fragments in devising HOMO and LUMO. In MPAR, HOMO is formed majorly by the contribution of the TPA donor and minorly by the central core, while LUMO is formed mainly by the core which is an acceptor in nature. The contribution of different fragments in the formulation of HOMO and LUMO in MPAM1–MPAM6 is analogous. In these molecules, HOMO is obtained predominantly by the TPA donor fragment, partially by core and insignificantly by acceptor and spacer units, while in the formation of LUMO, the end-capped acceptor and thiophene bridge play a significant role. Likewise, in MPAM7–MPAM12, HOMO is obtained by 80% participation of TPA donor fragment and almost negligible contribution of the acceptor and spacer. LUMO is modeled by acceptor and spacer fragments majorly with no significant assistance of the central core.

Table 6. Acceptor, Spacer, TPA Donor, and Core Contribution in Raising the HOMO and LUMO of Reference (MPAR) and Designed Chromophores (MPAM1–MPAM12).

  HOMO = H        
molecules LUMO = L acceptor (eV) spacer (eV) TPA donor (eV) core (eV)
MPAR H     72.5 27.5
  L     9.8 90.2
MPAM1 H 5.6 9.6 55.1 29.8
  L 57.7 30.0 12.3 0.0
MPAM2 H 5.9 10.5 56.3 27.3
  L 56.5 30.3 12.9 0.2
MPAM3 H 10.2 12.3 53.9 23.6
  L 55.2 25.6 12.1 7.0
MPAM4 H 4.0 7.4 51.7 36.9
  L 48.5 36.8 14.6 0.1
MPAM5 H 4.5 8.9 54.5 32.0
  L 11.5 9.1 13.9 65.6
MPAM6 H 4.8 7.3 50.6 37.2
  L 62.0 27.6 10.4 0.0
MPAM7 H 0.1 0.1 79.3 20.5
  L 57.7 30.0 12.3 0.0
MPAM8 H 0.1 0.2 78.3 21.4
  L 46.0 30.4 23.6 0.0
MPAM9 H 0.2 0.2 78.3 21.3
  L 60.1 27.9 11.9 0.1
MPAM10 H 0.0 0.1 80.7 19.2
  L 48.7 36.9 14.4 0.0
MPAM11 H 0.1 0.1 79.1 20.7
  L 46.5 36.7 16.8 0.0
MPAM12 H 0.0 0.1 81.3 18.7
  L 62.1 27.6 1.3 0.0
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2.7. Molecular Electrostatic Potential Surface

Charge transfer between donor and acceptor moieties in an excited state has been assessed with the molecular electrostatic potential (MEP) surface.42 In the current study, MEP simulations have been performed at an optimum DFT functional to determine the electrophilic and nucleophilic areas. The electrophilic region is symbolized by the red color, which epitomizes a negative value of electrostatic potential and an abundance of electrons in that region, while the green color transcribes an electrically neutral region, and the blue color represents a positive value of electrostatic potential and an absence of electrons, which transcribes the nucleophilic region.9,37

The MEP surface plot of the model molecule (MPAR) explored that the entire molecule is covered by shades of blue representing the positive region only, while the central acceptor core is covered by shades of red representing the negative region having an abundance of electrons. MEP surface plots of studied molecules (MPAM1–MPAM12) manifest that the donor portion is covered by shades of blue (positive region) and end-capped acceptor moieties are covered by shades of red (negative region) advocating their compliance for electrophilic reactivity (readily susceptible to nucleophile attack), as depicted in Figure 10. To sum up, based on colonization of electron density in varying regions, all newly planned molecules being reactive exhibit efficient charge transmission during excitation and can be employed as optimistic candidates for future proficient solar gadgets.

Figure 10.

Figure 10

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MEP surface plots of reference (MPAR) and devised molecules (MPAM1–MPAM12).

2.8. Transition Density Matrix and Exciton Binding Energy

The most persuasive tool for quantifying the electronic excitation processes (generation, diffusion, recombination, and separation of charges) is the transition density matrix (TDM).50 TDM demonstrates the quantum geometry of molecules in the excited state. TDM figures out the interrelation between donating and accepting moieties during excitation.51

TDM analysis of MPAR and currently aimed MPAM1–MPAM12 has been carried out by employing the selected hybrid DFT functional. Figure 12 displays the pictorial view of the model (MPAR) along with devised molecules (MPAM1–MPAM12). MPAR has been divided into two components, core (C) and donor (D), while the devised molecules (MPAM1–MPAM12) have been sequestered into four fractions, namely, core (C), donor (D), bridge (B), and acceptor (A). In TDM plots, atom numbers are displayed on the bottom and left axis, while electron density in the molecule is located on the right axis.

Figure 12.

Figure 12

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Graphical representation of the dipole moment (a) for MPAR and MPAM1–MPAM6 molecules (b) for MPAR and MPAM7–MPAM12.

Because of the insignificant contribution in transitions, hydrogen atoms have been ignored. In the model molecule (MPAR), the charge consistency can be seen in the donor and core fraction. In the devised molecules (MPAM1–MPAM12), uniform distribution of charge along with charge coherency in the acceptor region can be seen accompanied by the salutary diagonal and off-diagonal charge transfer. The TDM plots in Figure 11 demonstrate that the excellent charge transmission from donor to acceptor via the bridge has been seen expressing that freshly planned molecules are accompanied by less electron coupling exhibiting the greater exciton dissociation potential. The major electronic transitions of the reference molecule (MPAR) and the newly devised molecules (MPAM1–MPAM12) in the gas phase and DCM have been displayed in Tables 3 and 4, respectively.

Figure 11.

Figure 11

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TDM plots of reference (MPAR) and devised molecules (MPAM1–MPAM12).

Exciton binding energy is another parameter to scrutinize the charge transmission potential. In the current study, the binding energies of all molecules have been calculated in the gaseous and solvent phase using eq 10 and results have been reported in Tables 3 and 4, respectively.

2.8. 10

Eb is the binding energy, Eg represents the band gap, and Ex symbolizes the first excitation energy in eq 13. From the summarized results of binding energy, it is illustrated that molecules (MPAM7–MPAM12) accompanied by electron-withdrawing moieties on one side terminals of MPAR are accompanied by lower values of binding energy in gas and DCM as compared to molecules (MPAM1–MPAM6) having electron-withdrawing moieties on both side terminals of MPAR, thus endorsing greater exciton dissociation potential, leading to efficient charge transfer.

Keeping in view the TDM and exciton binding energy analysis, the devised moieties have manifested improved charge transmission from the donor fragment to acceptor group via thiophene. Therefore, MPAM1–MPAM12 exhibit marvelous charge dissociation ability as compared to MPAR thus can be employed as fortuitous aspirants for future OSCs and PSCs.

2.9. Dipole Moment (μ)

Dipole moment is a crucial assumption in calculating the solubility of chromophores in the organic solvent. The larger the dipole moment, the greater is the solubility. The solubility of the molecule is strongly correlated to the smooth structure of the donor–acceptor blend layer in OSCs. Insights into charge transfer efficiency are revealed by the smooth morphology of the thin film, which is the distinctive trait of effective OSCs.52,53

The dipole moment of investigated molecules (MPAR–MPAM12) is theoretically evaluated at the elected DFT functional. Summarized values of the dipole moment figured in the ground state (μg), the excited state (μe), and the difference between them (Δμ) are presented in Table 7, and graphical representation of the dipole moment in the ground state, as well as excited state, is pictured in Figure 12.

Table 7. Computed Dipole Moment for MPAR–MPAM12 in the Ground State (μg), Excited State (μe), and Difference between Them (Δμ).

molecules μg (D) μe (D) Δμ (D)
MPAR 3.52 4.98 1.46
MPAM1 2.71 4.13 1.42
MPAM2 3.00 4.39 1.39
MPAM3 3.67 5.41 1.74
MPAM4 2.74 4.40 1.66
MPAM5 6.41 8.52 2.11
MPAM6 2.49 4.04 1.55
MPAM7 10.25 10.93 0.68
MPAM8 6.50 7.26 0.76
MPAM9 11.03 12.91 1.88
MPAM10 16.25 17.85 1.60
MPAM11 10.43 12.03 1.60
MPAM12 19.21 20.74 1.53
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μe is calculated in DCM solvent to project the solubility of studied molecules. MPAR reveals a μg and μe of 3.52 and 4.98 D, respectively. In MPAM1–MPAM6, where structural modification was performed on both end terminals of MPAR, elevated μg is observed for MPAM3 (3.67 D) and MPAM5 (6.41 D) when contrasted with our model molecule (MPAR). While molecules in which structural adjustments were accomplished on one end terminal of reference, all molecules (MPAM7–MPAM12) demonstrate a remarkable increase in μg and their values lie in the range of 6.50 to 19.21 D. μe assessed in the solvent phase shows that all molecules (MPAR–MPAM12) in DCM have evident intensified dipole moment. A significant increase in the dipole moment is certified with an increase in solubility of molecules in DCM solvent and the presence of polar regions in their structures.

MPAM1, MPAM2, MPAM4, and MPAM6 show lower μe among all designed chromophores (MPAM1–MPAM12) attributing to the greater symmetry in molecules. The highest value of μe is revealed by MPAM12 because of its more solubility in DCM solvent which facilitates self-assembly, reduces exciton recombination, and aids in multilayer fabrication. The abovementioned discussion explores that the freshly designed molecules (MPAM1–MPAM12) are solution-processable, ought to be focused to contrive elite charge-transferring candidates for upcoming solar gadgets.

2.10. Reorganization Energy (RE) and Charge Transfer Integral

The most probable metric to quantify the charge carrier transport characteristics is reorganization energy (RE).54 It is defined as the energy required to modify and deform the structural properties of the reactant and its integrated solvent molecules.55 The external reorganization has been overlooked since it is hard to quantify.

The charge transfer alliance between the donor unit and the acceptor unit in the respective molecule is evaluated via internal reorganizational energy. It varies inversely with the charge transmission rate. The lower the value of internal reorganizational energy, the higher will be the charge transmission rate. The structure of the anion and cation plays a crucial role in determining the probability of electron transfer from the donor and hole transfer in the acceptor, respectively. In this current investigation, the focus is on the internal reorganization energy. It is statistically evaluated using eqs 11 and 12.

2.10. 11
2.10. 12

E+0, E–0 = neutral molecule energy for the cation or anion. E0+, E0– = energy of the cation or anion from optimized geometry of the neutral molecule. E0, E+, E– = single-point energy of the neutral molecule, cation, and anion from their optimized geometry.

RE of MPAR and newly architecture chromophores (MPAM1–MPAM12) is assessed and results are presented in Table 8 and pictured in Figure 13. Molecules having lower values of λe than MPAR manifest higher mobilities of an electron from donor to acceptor moiety. The findings of Table 8 validate that all our newly engineered molecules (MPAM1–MPAM12) evince lower λe when equated with our model molecule MPAR (0.0160913 eV). The theoretically calculated lowest λe is procured for MPAM6 (0.0028063 eV) which is conceived by end-capped acceptor modification on both side terminals of our model molecule MPAR. Likewise, computationally computed λh of designed molecules MPAM1–MPAM12 covers a range from 0.0047178 to 0.0108845 eV. Among all designed molecules, MPAM2 (0.0068553 eV), MPAM3 (0.0047178 eV), and MPAM9 (0.0068754 eV) reflect lower values of λh when contrasted to reference MPAR (0.0071995 eV) which are accredited to the acceptor moieties that assist hole transport. It is deduced that our designed molecules are empowering charge-transporting materials for future proficient solar devices.

Table 8. Reorganization Energy of Electron (λe) and Hole (λh), and Transfer Integral of Electrons (te) and Hole (th) of MPAR and MPAM1–MPAM12.

molecules λe (eV) λh (eV) te (eV) th (eV)
MPAR 0.0160913 0.0071995 0.705 0.09
MPAM1 0.0042799 0.0077049 –0.065 0.075
MPAM2 0.0041573 0.0068553 0.15 –0.14
MPAM3 0.0060241 0.0047178 0.06 –0.05
MPAM4 0.0042479 0.0095449 0.125 0.005
MPAM5 0.0052275 0.0080696 0.465 0.005
MPAM6 0.0028063 0.0099475 0.15 –0.05
MPAM7 0.0072771 0.0082084 0.055 0.25
MPAM8 0.0060033 0.0076755 0.05 0.215
MPAM9 0.0064652 0.0068754 0.045 0.21
MPAM10 0.0066191 0.0086163 0.01 0.255
MPAM11 0.0082533 0.0082651 0.06 0.195
MPAM12 0.0058227 0.0087601 0.06 0.275
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Figure 13.

Figure 13

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Graphical view of reorganization energy of electron (λe) and hole (λh) (a) for MPAR and MPAM1–MPAM6 molecules (b) for MPAR and MPAM7–MPAM12.

Another factor affecting the charge rate in the Marcus equation is the transfer integral of electrons and holes. The charge transfer integral is the internal molecular stacking of modeled molecules. It represents the ease of charge transfer. More values of charge integral ensure fewer abnormal states in the way to charge mobility. The charge integral values were calculated using following eqs 13 and 14(56,57)

2.10. 13
2.10. 14

The summarized calculated values of transfer integral of electrons (te) and hole (th) have been expressed in Table 8. Among all, MPAM7–MPAM12 have displayed higher hole transfer integral values (0.195–0.275 eV), as displayed in Figure 14, advocating their enhanced hole mobility rate and empowering their potential use as HTMs for future elite PSCs.

Figure 14.

Figure 14

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Graphical view of electron transfer integral (te) and hole transfer integral (th) (a) for MPAR and MPAM1–MPAM6 molecules (b) for MPAR and MPAM7–MPAM12.

2.11. OSC Device Photovoltaic Performance

For the theoretical assessment of the OSC performance, the open-circuit voltage (VOC) has been utilized as the most reasonable parameter. VOC is the voltage obtained for the device at zero current. The HOMO and LUMO of the donor and acceptor, respectively, have been taken into account to evaluate the PCE.53 To calculate VOC, the optimal chosen functional was used. Equation 15 is used to analyze VOC of OSCs statistically.57,58

2.11. 15

In eq 15, e symbolizes the charge on molecule and 0.3 represents a constant computed from voltage drop. PC61BM has been used as an acceptor. The HOMO and LUMO of PC61BM have been explored as −6.1 and −3.7 eV, respectively. The low-energy LUMO of the acceptor computes the highest VOC. Figure 15 manifests VOC of MPAR and MPAM1–MPAM12 with PC61BM. In this current study, MPAM1–MPAM12 are donors, which is why their HOMO has been scaled with the LUMO of PC61BM.

Figure 15.

Figure 15

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VOC pictorial view of (a) MPAR and MPAM1–MPAM6 (b) MPAR and MPAM7–MPAM12.

The VOC of MPAR has been explored as 1.01 eV. A pronounced shift in VOC values has been manifested by tailoring the end-capped acceptors of the model molecule (MPAR), as summarized in Table 9. The newly devised chromophores (MPAM1–MPAM12) have shown high open-circuit voltage than the MPAR owing to their low-lying HOMO advocating the fact that all reported molecules have great potential to be used as efficient HTMs. Briefly, the newly drafted molecules (MPAM1–MPAM12) should be focused to assemble upcoming proficient solar devices.

Table 9. Computed VOC (eV), Normalized VOC, Fill Factor (FF), and Percentage Fill Factor (FF %) of Reference (MPAR) and Newly Engineered Molecules (MPAM1–MPAM12).

molecules VOC (eV) normalized VOC FF FF %
MPAR 1.01 39.3308 0.9020 90.20
MPAM1 1.73 67.3685 0.9343 93.43
MPAM2 2.03 79.0509 0.9419 94.19
MPAM3 1.85 72.0415 0.9376 93.76
MPAM4 2.18 84.8921 0.9450 94.50
MPAM5 1.55 60.3591 0.9286 92.86
MPAM6 2.05 79.8298 0.9423 94.23
MPAM7 1.20 46.7296 0.9136 91.36
MPAM8 1.17 45.5614 0.9119 91.19
MPAM9 1.19 46.3402 0.9131 91.31
MPAM10 1.37 53.3496 0.9217 92.17
MPAM11 1.33 51.7919 0.9199 91.99
MPAM12 1.38 53.7391 0.9221 92.21
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2.12. Fill Factor

To calculate the PCE of solar devices, the fill factor (FF) is an integral parameter. The FF has been calculated using eq 16.57

2.12. 16

In eq 16, Voc is open-circuit voltage, KB is the Boltzmann constant, T is the temperature at 298 K, and e is an elementary charge (1) on the molecule. The term Inline graphic is normalized voltage. The summarized results of the calculated FF have been displayed in Table 9. All newly engineered molecules (MPAM1–MPAM12) have manifested a higher FF value than the reference (MPAR). The higher FF endorses the effectiveness of freshly engineered structures for future elite solar gadgets.

2.13. Power Conversion Efficiency

PCE of solar devices has been estimated using eq 18.59 The estimated values of PCE values of all reported molecules have been displayed in Table 10.

2.13. 17

Table 10. Computed VOC (eV), Normalized VOC, Percentage Fill Factor (FF %), and Estimated PCE of Reference (MPAR) and Newly Engineered Molecules (MPAM1–MPAM12).

molecules VOC (eV) Jsc mA cm–2 (assumed short circuit current from reference paper.) FF % PCE
MPAR 1.01 23.23 90.20 21.16
MPAM1 1.73 23.23 93.43 37.55
MPAM2 2.03 23.23 94.19 44.42
MPAM3 1.85 23.23 93.76 40.29
MPAM4 2.18 23.23 94.50 47.86
MPAM5 1.55 23.23 92.86 33.44
MPAM6 2.05 23.23 94.23 44.87
MPAM7 1.20 23.23 91.36 25.47
MPAM8 1.17 23.23 91.19 24.78
MPAM9 1.19 23.23 91.31 25.48
MPAM10 1.37 23.23 92.17 29.33
MPAM11 1.33 23.23 91.99 28.42
MPAM12 1.38 23.23 92.21 29.56
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In eq 17, the short circuit current value (JSC) (23.23 mA cm–2)27 has been taken from the reference paper and has been assumed for all freshly planned molecules for estimating their PCE. The Pin is the power of incident rays on the solar cells during the estimation of PCE which is commonly fixed at AM 1.5G, 100 mW cm–2.

The pictographic representation of the estimated PCE values has been manifested in Figure 16, illustrating that all newly contrived molecules (MPAM1–MPAM12) have explored enhanced PCE than the reference molecule (MPAR) due to structural modification by the introduction of thiophene-bridged end-capped strong electron-pulling moieties.

Figure 16.

Figure 16

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Graphical view of power conversion efficiency (PCE %) (a) for MPAR and MPAM1–MPAM6 molecules (b) for MPAR and MPAM7–MPAM12.

In a nutshell, the thiophene-bridged end-capped acceptor alteration tactic has been proved compelling in providing the new gateway for boosting the optoelectronic properties and newly customized molecules should be targeted to contrive future proficient solar devices.

3. Conclusions

The current study relies on offering donor contributors for OSCs and productive HTMs for PSCs. Selected MPW1PW91/6-311G has been used for the computational simulations in the current study. As a result, the newly designed molecules (MPAM1–MPAM12) have manifested impressive outcomes. MPAM5–MPAM12 displayed reduced band gaps ranging from 1.78 to 2.45 eV and then MPAR (2.54 eV). MPAM7 (600 nm), MPAM6 (651 nm), and MPAM12 (639 nm) are accompanied by higher λmaxcal values in DCM as compared to MPAR (596 nm). The newly planned molecules (MPAM7–MPAM12) are enriched with a higher dipole moment varying from 7.26 to 20.74 D in DCM than the ground state addressing their good solubility and less charge recombination. The RE values indicate that newly engineered molecules exhibit paramount charge mobility than reference. Among all, MPAM7-MPAM12 displayed higher hole transfer integral values (0.195–0.275 eV) advocating their enhanced hole mobility rate and empowering their potential use as HTMs for future elite PSCs. Moreover, all newly planned molecules when scaled with the PC61BM acceptor displayed higher VOC values 1.17 to 2.18 eV than MPAR (1.01 eV) which suggested that these donor contributors hold a compelling position in achieving escalating operational efficiency. All designed molecules are accompanied by a higher estimated PCE (24.78–47.86%) than the reference (MPAR) proving their effectiveness for upcoming solar devices. Thus, the thiophene-bridged end-capped acceptor alteration strategy is a promising way to design optimistic photovoltaic materials. Therefore, all newly designed molecules might potentially contribute in improving the device’s functioning ability and can be used as the aristocratic materials in planning future elite solar devices.

4. Computational Details

All ground-state geometry optimization of MPAR and MPAM1–MPAM12 was executed using Gaussian 09 software package,60 while GaussView 5.0.8 program61 was used for drawing structures and presentation of results. The DFT computations were accomplished for auxiliary streamlining of MPAR reference at B3LYP,62 CAM-B3LYP,63 PBEPBE,64 MPW1PW91,65 and ωB97XD66 functionals in alliance with the 6-311G (d,p) basis set. Low-lying excited state’s characteristics were assessed at the ground state applying TD-DFT. The accomplished λmax of MPAR from four different functionals was certified with the experimental value given in the literature to validate the hypothetical strategy. The MPW1PW91 functional manifested precise compromise between experimentally (532 nm)27 and theoretically (596 nm) determined absorption values and consequently presented a realistic argument for its manipulation in quantum chemical computations. All designed molecules (MPAM1–MPAM12) were geometrically optimized at the MPW1PW91/6311G (d,p) level of theory. DCM solvent impact has been simulated using the solvation model IEFPCM.67 The λmax of MPAR and MPAM1–MPAM12 was computed both in gas and solvent phases. Computational transfiguration of λmax was performed using the Swizard program.68 Collectively, λmax values were plotted via Origin 6.0 program.69 FMO analysis, DOS calculations, TDM examination, reorganization energy, and dipole moment simulations were computationally accomplished by the optimal theoretical DFT-selected functional. To analyze the contribution of molecular fragments, DOS files were pictured via PyMOlyze 1.1 software. Estimation of electron densities and electronic transitions was executed using the Multiwfn 3.7 software.70 To model the electron and hole transfer rate, eq 1 is the key parameter. Total reorganization energy is the sum of internal (λi) and external reorganization energy (λo).

4. 18

Inner-sphere and outer-sphere reorganization energies peak for alteration within the structure of molecules and external environment modification during the charge transport, respectively. To model the changes in cationic and anionic geometry of reference and newly devised molecules, the focus is on the λi. The λo has been neglected in the present investigation. The mobility rate of the electron (λe) and hole (λh) was computed using subsequent eqs 11 and 12.

Acknowledgments

The authors acknowledge the Department of Chemistry for financial and technical support, University of Agriculture (UAF), Faisalabad 38000, Pakistan. The author from the King Khalid University of Saudi Arabia extends his appreciation to the Deanship of Scientific Research at King Khalid University for funding the work through research project (RGP.2/156/42).

Supporting Information Available

The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acsomega.1c05504.

  • Comparative analysis of absorption in the bar chart and Cartesian coordinates (PDF)

Author Contributions

A.R. major contribution to acquisition, drafting, analysis, writing the original paper, working, and interpretation of data. S.Z. acquisition, drafting, analysis, working, and interpretation of data. M.A. substantial contribution to research design, acquisition, analysis, interpretation of data, and approval of the submitted and final version. S.M. substantial contribution to research design, acquisition, analysis, and interpretation of data. K.A. substantial contribution to research design, acquisition, analysis, and interpretation of data. J.I. substantial contribution to research design, acquisition, analysis, interpretation of data, and approval of the submitted and final version.

The authors declare no competing financial interest.

Supplementary Material

ao1c05504_si_001.pdf (2.2MB, pdf)

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