Wenkai Zhong's research while affiliated with Shanghai Jiao Tong University and other places

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Publications (106)


Materials and solvent selection
a, The chemical structures of D18, 2BTh-2F-C2 and relevant solvents. Solvents with low volatility and low solubility for the polymer donor are framed by a blue box; solvents with high volatility and low solubility for the polymer donor are framed by a violet box; solvents with low volatility and high solubility for the polymer donor are framed by a green box; solvents with high volatility and high solubility for the polymer donor are framed by a bluish-purple box. b, The solubility of D18 in various solvents in the δv–δh diagram (δh, molecular hydrogen bonding interactions; δv, δV=δD2+δP2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\delta }_{{\rm{V}}}=\sqrt{{{\rm{\delta }}}_{{\rm{D}}}^{2}+{{\rm{\delta }}}_{{\rm{P}}}^{2}}$$\end{document}). c, Normalized absorption of D18 in various solvents. The blue rectangle represents the absorption peak of D18 in good solvents; the violet rectangle represents the absorption peak of D18 in bad solvents. d, Solvent classification diagram based on vapour pressure and solubility. Good solvents show a RED index smaller than 1, which are inside the solubility sphere; bad solvents have a RED index larger than 1, and the larger the RED number, the worse the solubility. e, Vapour pressure as a function of volume fraction in the binary solvent of CF&OXY. The solid vertical line represents 12% volume fraction of OXY in solvent mixture, the upper dashed horizontal line represents the CF vapour pressure in 12%-OXY solvent mixture for 142.26 torr, and the lower dashed horizontal line represents the OXY vapour pressure in 12%-OXY solvent mixture for 0.41 torr. When OXY takes up the majority of the solvent mixture, the vapour pressure of CF and OXY is both 4.88 torr with the same evaporation rate. f–h, Time-dependent contour maps of in situ UV–vis absorption spectra for D18:2BTh-2F-C2 blend precursor solutions in CF condition (f), OXY condition (g) and CF&OXY condition (h). The dashed lines and dashed box represent the spectral change time for D18 and 2BTh-2F-C2 of the CF-, OXY- and CF&OXY-based blend precursor solution in the film-forming process as shown in Supplementary Table 6.
Device performances
a, J–V curves and detailed parameters in different conditions under AM 1.5 G, 100 mA cm⁻². b, EQE spectra and integrated JSC in the corresponding conditions. c, Histogram of PCE measurement for devices in the corresponding conditions under AM 1.5 G, 100 mA cm⁻², obtained from 20 individual experimental data points. d, Plots of the PCE versus JSC for the efficient NFREAs reported in the literature. Detailed data based on 20 data points from 20 publications are presented in Supplementary Table 952–71. e, Macroscopic factor matrix of SC, FOM and PCE based on ITIC-4F, Y6, L8-BO and 2BTh-2F-C2. f, Efficiency for various solvent combinations under AM 1.5 G, 100 mA cm⁻².
Source data
Ultrafast process and devices’ physical characteristics
a, Hole-transfer process kinetics in the corresponding conditions. b, The carrier mobility of D18:2BTh-2F-C2 in various conditions (μe, the electron mobility; μh, the hole mobility). The whiskers represent the fitting standard error, and the centre of the error bars represents the value of mobility shown in Supplementary Fig. 29. The data are presented as mean values ± standard error of the mean. The values are fitted from one individual experimental data. c, Photocurrent density (Jph) versus effective bias (Veff) characteristics in different conditions (Pdiss, carrier collection efficiency). d, Derived charge lifetime as a function of charge density fitted from TPV and TPC results. The exponential factor λ is in relation to the non-geminate recombination order R (R = λ + 1, and R = 2 in ideal condition). The recombination rate coefficient can be determined, which is defined by k(n)=1τ(n)n\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$k(n)=\frac{1}{\tau (n)n}$$\end{document}. The τ as a function of n follows an approximated exponential law of τ=τ0(nn0)λ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\tau ={\tau }_{0}{(\frac{n}{{n}_{0}})}^{\lambda }$$\end{document}. e, Recombination rate coefficient as a function of charge density fitted from TPV and TPC results. f, Derived LUMO DOS from the capacitance spectra of devices and detailed parameters (Nt, the total density per unit volume; Et, the energy for exponential tail distribution that describes energetic disorder). DOS gn (EFn) is obtained by extracting the Cμn\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${C}_{\mu }^{n}$$\end{document} from Cμn=Lq2gn(EFn)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${C}_{\mu }^{n}=L{q}^{2}{g}_{n}({E}_{{Fn}})$$\end{document}.
Source data
Morphology of thin films
a–c, Tapping AFM-IR topography image for D18:2BTh-2F-C2 blends at a wavenumber of 1,700 cm⁻¹ in CF (a), OXY (b) and CF&OXY (c) conditions. d, Linecut profiles for D18:2BTh-2F-C2 blends in different conditions (blue rectangle represents lamellar area; yellow rectangle represents π–π area). e,f, Cryo-TEM images for CF-, OXY- and CF&OXY-based precursor solution at 50 nm scale (e) and 100 nm scale (f).
Rheological property and large-area devices
a, Measured thickness and surface profile linecut based on silicon wafer in CF, OXY and CF&OXY conditions. The inset is the corresponding photograph. b, Rheological measurement for D18 in CB and OXY solution, fitted by the Herschel–Bulkley model: σ=σy1+τHBγ̇n\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sigma {\boldsymbol{=}}{\sigma }_{y}\left[1+{\left({\tau }_{{{\mathrm{HB}}}}\dot{\gamma }\right)}^{n}\right]$$\end{document}. c, Thickness and efficiency distribution of the devices in CF, OXY and CF&OXY conditions. The bounds of the box represent the 25th percentile and 75th percentile, the bounds of the whiskers represent the maxima and minima values of points, and the centre lines represent the median. The values are obtained from 20 individual experimental data points. d, J–V curve and detailed parameters in CF, OXY and CF&OXY condition for 5.2 mm² (solid line) and 1 cm² (dashed line) devices. e, Surface roughness (Sa), series resistance (Rs), shunt resistance (Rsh) and large-area device loss (Pr) for various conditions.
Achieving 19% efficiency in non-fused ring electron acceptor solar cells via solubility control of donor and acceptor crystallization
  • Article
  • Publisher preview available

June 2024

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45 Reads

Nature Energy

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Xiaodong Wang

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Non-fused ring electron acceptors (NFREAs) potentially have lower synthetic costs than their fused counterparts. However, the low backbone planarity and the presence of bulky substituents adversely affect the crystallinity of NFREAs, impeding charge transport and the formation of bicontinuous morphology in organic solar cells. Here we show that a binary solvent system can individually control the crystallization and phase separation of the donor polymer (for example, D18) and the NFREA (for example, 2BTh-2F-C2). We select solvents such as chloroform and o-xylene that evaporate at different temperatures and rates and have different solubility for D18. Upon evaporation of chloroform, D18 starts to assemble into fibrils. Then, the evaporation of o-xylene induces the rapid formation of a fibril network that phase segregates 2BTh-2F-C2 into pure domains and leads to a bicontinuous morphology. The well-defined interpenetrating network morphology affords an efficiency of 19.02% on small-area cells and 17.28% on 1 cm² devices.

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High‐Efficiency Semitransparent Near‐Infrared Organic Photodetectors Enabled by a Molecular Crystal Network
Advanced Optical Materials

Advanced Optical Materials

Semitransparent organic photodetectors (ST‐OPDs) show immense promise for integration into optoelectronic devices, offering adjustable absorption and see‐through functionalities. However, achieving high‐performance ST‐OPDs remains challenging, necessitating a delicate balance of low dark current density, high external quantum efficiency, and optimal visible light transmission. Here, a strategy is presented using anode interfacial materials (AIMs) as the donor and narrow bandgap non‐fullerene acceptors (NFAs) to formulate the donor: acceptor light‐sensitive layer. Critical to the approach is the incorporation of 1,8‐diiodooctane during film processing, enabling the formation of morphology with an NFA molecular crystal network embedded within the donor polymer matrix. This optimized morphology substantially boosted device external quantum efficiency and reduced dark current under reverse bias, yielding a remarkable special detectivity of over 10¹³ Jones at 840 nm under a bias of −0.1 V. ST‐OPDs are achieved with detectivity surpassing 10¹² Jones and notable average visible transmittance of over 50%. These findings highlight the potential of AIM:NFA combinations for high‐efficiency ST‐OPDs by finely controlling morphology through multiple length scales, opening doors for various applications in transparent electronics and beyond.


3D Crystal Framework Regulation Enables Se‐Functionalized Small Molecule Acceptors Achieve Over 19% Efficiency

March 2024

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50 Reads

Se‐functionalized small molecule acceptors (SMAs) exhibit unique advantages in constructing materials with near‐infrared absorption, but their photovoltaic performance lags behind that of S‐containing analogs in organic solar cells (OSCs). Herein, two new Se‐containing SMAs, namely Se‐EH and Se‐EHp, are designed and synthesized by regulating bifurcation site of outer alkyl chain, which enables Se‐EH and Se‐EHp to form different 3D crystal frameworks from CH1007. Se‐EH displays tighter π–π stacking and denser packing framework with smaller‐sized pore structure induced by larger steric hindrance effect of outer alkyl chain branched at 2‐position, and a higher dielectric constant of PM6:Se‐EH active layer can be obtained. OSCs based on PM6:Se‐EH achieved very high PCEs of 18.58% in binary and 19.03% in ternary devices with a high FF approaching 80% for Se‐containing SMAs. A more significant alkyl chain steric hindrance effect in Se‐EH adjusts the molecular crystallization to form a favorable nanofiber interpenetrating network with an appropriate domain size to reduce rate of sub‐ns recombination and promote balanced transport of carriers. This work provides references for further design and development of highly efficient Se‐functionalized SMAs.


Enhanced Fibrillar Network and Molecular Crystallization via Volatile Solid Additives Enable Efficient Near‐Infrared Organic Photodetectors

December 2023

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39 Reads

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3 Citations

Advanced Optical Materials

Advanced Optical Materials

Controlling the phase separation and domain purity of organic semiconductors to form well‐developed nanoscale morphology optimization in the bulk‐heterojunction active layer is critical yet challenging for building high‐performance organic photodetectors. Herein, an effective morphology controlling method by applying a small molecule IC‐Br as the solid additive is demonstrated, which can effectively restrict the overmix of the PTzBI‐Si:IEICO‐4F in the process of film formation. The film processed with IC‐Br formed well‐developed nanoscale phase separation with bi‐continuous interpenetrating networks, which exhibited enhanced π–π stacking and the improved domain purity of the IEICO‐4F phase, resulting in a significant decrease in the density of the trap state compared to the pristine film. Consequently, the device processed with IC‐Br additive enabled a high specific detectivity of 3.8 × 10¹³ Jones at 860 nm under −0.1 V associated with the improved linear dynamic range and response speed, indicating the strong visible‐to‐near infrared detecting capability and potential for practical applications. The morphology optimization strategy established in this work may offer unprecedented opportunities to build state‐of‐the‐art OPDs.





Enhanced detectivity of organic photodetectors with a non-conjugated polymer additive

October 2023

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97 Reads

Applied Physics Letters

Organic photodetectors have attracted increasing attention in the scenario of low-cost imaging, health monitoring, and near-infrared sensing. However, relatively high dark current and trap density block the sensitivity for organic photodetectors. In this manuscript, a simple yet effective strategy is proposed to enhance the detectivity of organic photodetectors by incorporating a non-conjugated polymer additive of polystyrene into the functional layers. Systematic morphological investigation reveals that this strategy can not only enable suppressed amorphous phase but also effectively tune the phase separation in the bulk heterojunction blends. Electrical results suggest the suppressed trap density in optimized organic photodetectors. Consequently, a dark current density of 5.06 × 10−10 A cm−2 is achieved for PM6:Y6-BO-based organic photodetectors, showing a peak detectivity of 6.38 × 1013 cm Hz1/2 W−1 at 850 nm. This strategy is also applicable in various representative organic-semiconductor systems, including PTB7-Th:PC71BM and P3HT:PC61BM blends, superior to other optimization techniques.



The past and present of surface topology and its significance on device function
The comparison of surface topography between silicon solar cells and organic solar cells is shown in the left two figures, and the lower right image shows that the surface topography reduces light loss in organic solar cells. The figure on the top right indicates that organic solar cells with such surface topography are more suitable for urban environments.
Materials and devices performances
a Chemical structures of PM6 and PY-IT. bJ-V curves of the APSCs in different condition under AM 1.5 G, 100 mA cm⁻². c EQE spectra of the APSCs in corresponding condition. All the DIB condition in text is followed by a TA process. d Histogram of PCE measurement for devices of the APSCs in corresponding condition under AM 1.5 G, 100 mA cm⁻². e Plots of the PCE versus JSC for the efficient all-PSCs reported in the literature.
Nanoscale fibril crystallization morphology characteristics
a Tapping AFM-IR image at the wavenumber of 1650 cm⁻¹ and 2215 cm⁻¹ in optimal DIB/TA/SVA condition. b Line cut profiles for PM6:PY-IT blends in different conditions. c Individual in plane and out of plane line cut profiles of the 2D GIWAXS data.
Microscale surface optical morphology characteristics
a Optical microscope photograph of DIB/TA/SVA. b Three-dimensional AFM photograph of DIB/TA/SVA. c Three-dimensional AFM photograph of as-cast. dJ-V curve of as-cast and DIB/TA/SVA as function of light receiving angle. e Universality test for variable angle experiment. f Variation of JSC and PCE of as-cast and DIB/TA/SVA device in different light receiving angle. g Scheme for daily power output simulation at the summer solstice in Shanghai. h Efficiency corresponding to the incident angle at different times in as-cast and DIB/TA/SVA condition.
Ultrafast process and devices physical characteristics
a Hole transfer process kinetics in corresponding conditions. b Charge-transfer time and lifetime achieved through multi-exponential fitting in corresponding conditions. (τ1 is the fast components represent the kinetics of the exciton dissociation in mixing domain or at interfaces; τ2 is the slow components represent the kinetics of exciton diffusion in crystalline domain to interfaces; Ld is the exciton diffusion lengths; τp is the fitted decay lifetimes for positive polaron signal). c Derived charge lifetime as a function of charge density fitted from TPV and TPC results (λ is the exponential factor). d Recombination rate coefficient as a function of charge density fitted from TPV and TPC results. e Dark J-V curves for corresponding conditions. f Derived LUMO DoS from the capacitance spectra of devices, inset is the schematic illustration.
All-polymer organic solar cells with nano-to-micron hierarchical morphology and large light receiving angle

July 2023

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255 Reads

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86 Citations

Nature Communications

Distributed photovoltaics in living environment harvest the sunlight in different incident angles throughout the day. The development of planer solar cells with large light-receiving angle can reduce the requirements in installation form factor and is therefore urgently required. Here, thin film organic photovoltaics with nano-sized phase separation integrated in micro-sized surface topology is demonstrated as an ideal solution to proposed applications. All-polymer solar cells, by means of a newly developed sequential processing, show large magnitude hierarchical morphology with facilitated exciton-to-carrier conversion. The nano fibrilar donor-acceptor network and micron-scale optical field trapping structure in combination contributes to an efficiency of 19.06% (certified 18.59%), which is the highest value to date for all-polymer solar cells. Furthermore, the micron-sized surface topology also contributes to a large light-receiving angle. A 30% improvement of power gain is achieved for the hierarchical morphology comparing to the flat-morphology devices. These inspiring results show that all-polymer solar cell with hierarchical features are particularly suitable for the commercial applications of distributed photovoltaics due to its low installation requirement.


Citations (78)


... Finally, 3-ClTh with delicate balance between the side-and terminal-group torsion angles delivers an impressive PCE of 18.5% in D18-Cl-based OPV and enables a much better stability than the other isomers. A higher PCE of 19.15% is obtained in the derived system with a preferable vertical component distribution via tuning of selective interaction between solid additive and active-layer components, 99 indicating the great promise of coremoiety halogenation in facilitating the efficiency and lifetime of OPV. ...

Reference:

Non‐fullerene acceptors with heteroatom substitution on the core moiety for efficient organic photovoltaics
Understanding the Role of Removable Solid Additives: Selective Interaction Contributes to Vertical Component Distributions
  • Citing Article
  • May 2023

... 15 Ternary organic solar cells with an auxiliary third component incorporated into the donor/acceptor photoactive system is a promising approach that has been investigated extensively to broaden the absorption range of OPVs. [16][17][18][19] A typical ternary blend consists of an additional donor or acceptor component, generally expected to have complementary absorption. Besides the enhanced light absorption, the additives can affect other factors, such as morphology and charge carrier mobility, that can greatly improve the power conversion efficiency (PCE) values. ...

Improved performance of ternary polymer solar cells based on a nonfullerene electron cascade acceptor
  • Citing Article
  • June 2017

Advanced Energy Materials

Advanced Energy Materials

... It is anticipated that siloxane-functionalized side chains are expected to improve solubility, decrease steric repulsion, and enhance charge carrier transport, all of which boost PCEs. [35][36][37][38][39][40] On the other hand, thienothiophene was included to provide face-on molecular packing, electron delocalization, and enhanced neighboring unit stiffness to prevent twisting, increase mobility, and produce a desirable BHJ active layer film morphology. Notably, compared to the thiophene -bridge, the thienothiophene -bridge has a large dipole moment and acts as a backbone that promotes polymer planarity. ...

High‐performance thick‐film all‐polymer solar cells created via ternary blending of a novel wide‐bandgap electron‐donating copolymer
  • Citing Article
  • May 2018

Advanced Energy Materials

Advanced Energy Materials

... Halogenation on the skeleton and/or side-chain of organic semiconductors is considered to be a general method to modulate the opto-electrical and aggregation properties of resulting materials, thus is promising in addressing the trade-off between J SC and V OC . 86,87 The fluorination has been widely employed in multiple categories of materials to tune the electronic structures and interactions between molecules. 88 However, the incorporation of fluorine (F) usually increases the synthetic complexity of molecules. ...

Fine-tuning of the chemical structure of photoactive materials for highly efficient organic photovoltaics
  • Citing Article
  • December 2018

Nature Energy

... Recent endeavors to enhance the power conversion efficiency (PCE) of organic solar cells encompass tactics like the development of high-performance donor and acceptor materials, integration of ternary active layers, adoption of tandem device architectures, and refinement of carrier transport layers and fabrication techniques 4-17 . Accordingly, there has been a notable enhancement in PCEs, exceeding 16% for single-junction cells and surpassing 17% for ternary and tandem configurations [18][19][20][21][22] . ...

Achieving over 16% efficiency for single-junction organic solar cells
  • Citing Article
  • June 2019

Science China-Chemistry

... 88 However, the incorporation of fluorine (F) usually increases the synthetic complexity of molecules. 89 An alternative strategy is to implement the cost-effective chlorine (Cl) and bromine (Br) substitutions, because Cl and Br have weaker electron affinity than F and their empty d-orbitals can accommodate free π-electrons, resulting in up-shifted energy levels and broadened absorption spectra. 41,90 For Y6-type NFAs, all the attempts of F, Cl, and Br substitutions have been thoroughly demonstrated in the end-F I G U R E 5 Unit cell of CH1007 (four enantiomers) and Y6 (two enantiomers) in the single crystal. ...

Tailoring regioisomeric structures of π-conjugated polymers containing monofluorinated π-bridges for highly efficient polymer solar cells
  • Citing Article
  • May 2020

ACS Energy Letters

... Single-junction organic solar cells (OSCs) 1-4 based on conjugated polymer donors and fused ring electron acceptors (FREAs) [5][6][7][8][9] have achieved prominent power conversion efficiencies (PCEs) over 19% in recent years [10][11][12][13] . On the contrary, OSCs incorporating the more economically viable non-fused ring electron acceptors (NFREAs) [14][15][16][17] have been confined to efficiencies of approximately 16%, suffering from low short-circuit current density (J SC ) and fill factor (FF). ...

All-polymer organic solar cells with nano-to-micron hierarchical morphology and large light receiving angle

Nature Communications

... The subsequent evaporation of OXY induces the rapid formation of a fibril network, segregating 2BTh-2F-C 2 into a high-purity acceptor fibril phase in the residual solvent. Additionally, we introduce the solid-state additive of 1,4-diiodobenzene (DIB) 20 , which resides in the nearly dried photoactive thin film to further enhance material crystallization. The solvent mixture method could address excessive intermolecular mixing or phase separation, enabling an optimal and well-defined interpenetrating network morphology. ...

Understanding the Role of Removable Solid Additives: Selective Interaction Contributes to Vertical Component Distributions
Advanced Materials

Advanced Materials

... This is due to a higher miscibility of the fullerenes and non-fullerenes in the polymer matrix. Good miscibility between materials reduces the driving force for phase separation, which results in smaller impurity domains, Figure 3b, that support efficient electron-hole dissociation [31,33]. Higher-performance OSCs require compatible and favorable film morphology in the active layer. ...

Mastering morphology of non-fullerene acceptors towards long-term stable organic solar cells

Nature Communications