Abstract
Metal-free organic compounds with highly ordered π-conjugated twisted skeletons are capable of generating brilliant multi-colored light. Additionally, the co-existence of numerous other multi-functional properties have endowed them with the potential to be a promising class of materials for several electronic and photonic applications and next-generation advanced luminescent material-based devices. This review highlights the recent developments made in this fascinating class of multi-property encompassing materials, involving a highly twisted donor-acceptor based single molecular platform with synchronized photophysical behavior such as thermally activated delayed fluorescence (TADF), mechanoresponsive (MR), room-temperature phosphorescence (RTP), and aggregation induced emission (AIE) with associated unique and inherently manifested structure-property relationship investigations. Furthermore, a brief summary of the optoelectronic behavior of TADF materials are also presented by correlating their performances in the organic light-emitting diodes (OLEDs) and corresponding EL devices. In addition to mechanochromic luminescence (MCL) with TADF behavior, new types of emitters are also being developed, with tunable color changes such as blue-green, yellow-orange, yellow-red, etc., with some emitters crossing the entire visible span to produce white OLEDs. These developments have enriched the library of fascinating organic materials in addition to providing new directions of multifunctional material design for solutions processed OLED and several other advanced devices.
Introduction
Light is an auspicious source of existence in the living world, especially multicolored bioluminescence from natural light emitting pigments, making the universe more beautiful. Inspired by nature, human beings imagined and developed organic, inorganic, and hybrid materials as a source of chemiluminescence to generate light affordably and created many exciting ways in which to use it, for the benefit of living beings. In view of this, organic light emitting diodes (OLEDs) which are widely exploited in the field of lighting technology and emerging luminescent organic materials, have wielded considerable importance over the past 30 years, to advance the material design and its related functionality, since the first pioneering technology was introduced in 1987 by Tang and VanSlyke (). However, in the last 5 years, metal free modern luminescent organic materials with thermally activated delayed fluorescence (TADF) behavior have been gaining prominence as an inevitable class of luminophores, following the invention of first TADF material 4CZIPN by C. Adachi and coworkers in 2012 (Uoyama et al., ). Along with notable progress in material synthesis, researchers have devoted persistent efforts to develop underlying fundamental mechanisms and an effective design strategy for multifunctional TADF materials. In particular, TADF materials have a high potential to evolve into versatile applications like flat panel displays and solid-state-lighting (Zhang et al., ; Wu et al., ; Liu et al., ) including photodynamic therapy (Li et al., ), sensors (Kinami et al., ), security (Yamashita et al., ), bioimaging (Hirata and Watanabe, ), memory chips (Meher and Iyer, ) etc. In the early stages of research, exploration of conventional fluorescence small molecules and polymers had aroused immense research interest. Certain limitations in the device efficiency, however, suffered mainly by non-radiative triplets with a share of ~75% of all excitons, generated directly under electrical excitation with their poor spin-orbit coupling (SOC), weak intersystem crossing (ISC) and solely singlet excitons contribution, restricted their internal quantum efficiency (IQE) to only 25% and external quantum efficiency (EQE) to 5% (Xu et al., ). Further, the involvement of Iridium (Ir), Platinum (Pt) and Ruthenium (Ru) based heavy metal complexes greatly enhanced the SOC, activating the phosphorescence emission from triplet state achieving theoretical 100% IQE (Bolton et al., ). However, assimilation of highly expensive and non-environmentally friendly precious heavy metals are not preferred in practical applications. In this regard tremendous effort has been made to explore alternative approaches such as hybridized local charge transfer (HLCT) (Li et al., ), triplet-triplet annihilation (TTA) (Chou et al., ), including TADF, in order to harvest 100% excitons and to overcome the obstacle faced by conventional fast degradable fluorescence/phosphorescence materials (Scholz et al., ). Unlike other discoveries, the most successful breakthrough was achieved in the case of TADF materials, which has been realized as a promising material for lighting applications due to the decent EQE and very high photoluminescence quantum yield (PLQY), as compared to inorganic phosphorescence materials (Zhao et al., ). In spite of this exciting phenomenon, of additional extreme importance is the discovery of more closely associated functional features accompanying these TADF materials, that include (but are not limited to) aggregation-induced emission (AIE), white-light emission, and multi-color tunability upon severe external stimuli/mechanical force, which creates a mechanochromism property or so-called TADF-mechanophore, which extends their conceivable application manifold (Tonge and Hudson, ). The molecule showed multiple color emissions on application of some external stimuli like grinding, recrystallization, and solvent fuming due to the change in its molecular packing mode and intra and inter molecular interactions. Owing to the unique and easy to tune chemical and optical properties, wide range of color switching ability, and huge possibilities on structural flexibility in an economical organic molecular platform, these TADF materials are considered to be a promising avenue for the development of next-generation electronic devices (Das et al., ). Moreover, an ever-increasing demand to use them as a solution-processed non-doped fabrication technique gives them an extra edge over other existing methods for solid-state lighting. However, the major issues of efficiency improvement affected by emission quenching in non-doped thin-film state is mainly due to singlet-triplet annihilation (STA), long lifetime triplet-polaron, and triplet-triplet annihilation (TTA) (Ban et al., ). Yet, quenching the effect of TADF emitters can be fixed by co-existing with an impressive solid state emission property, called aggregation induced emission (AIE), a condensed state emission behavior that can arrest the rotation or vibration in a highly twisted molecular configuration likewise TADF molecular structure. Further, expanding the functionality and accessibility of the multifunctional-TADF molecules enables it to evolve in new processing techniques such as ink-jet printing, spin coating etc. (Müller et al., ; Cho et al., ), offering enormous advantages over expensive thermal deposition techniques, and which can be effectively integrated in optoelectronic device fabrication platforms (Albrecht et al., ).
Impressively, white-light-generating TADF-single emitters have great potential for use in flat-panel displays and have attracted broad interest in future light sources (Sun et al., ; Reineke et al., ). Most of the reported organic white-light emitters were accomplished by rational blending of red/green/blue or blue/orange emitters, which covers the complete visible-light emission spectrum region (Shao et al., ). Notably, single organic white-light solids were often found by harnessing singlet excitons, like monomer/excimer complex, excited-state intramolecular proton transfer (ESIPT) etc. (Tang et al., ). However, white radiative decay from both singlet and triplet excitons have recently been found in TADF molecules (Wu et al., ). Moreover, development of single molecule white light emitters (SMWLEs) with multi-functional additional exciting key properties are under investigations due to their superior performance, no phase segregation, no color aging with improved stability, good reproducibility, and simple device fabrication protocols (Sun et al., ). In addition, by introducing AIE-ML functionality in white TADF emitters, efficient device results have been realized by overcoming the complex material arrangements and by appropriate doping of materials into the host to achieve high electroluminescence (EL) and high external quantum efficiencies (Zheng et al., ). Simple material based high performance organic white-light emitter fabrication therefore remains a challenge.
Fundamental Aspects and Working Principles of TADF and MCL Materials
Approaches to Realize TADF Property
Organic luminogens with electron donor (D) and electron acceptor (A) containing moieties connected either directly or via spacer units in a hindered orientation, are considered to be promising candidates for multifunctional luminescence behavior in terms of high quantum-efficiency, good charge transporting ability in either an intramolecular or intermolecular fashion, which endows them with tunable electronic properties (Tao et al., ). Principally, TADF molecules must exhibit strong spin–orbit coupling which is generally induced by rapid conversion of the singlet and triplet manifolds, without the use of heavy elements and simultaneously without a small energy gap between low lying singlet and triplet states. Consequently to achieve high quantum-efficiency, the molecule should exhibit faster radiative decay via charge transfer states, which minimizes the exchange energy and therefore the singlet-triplet gap (Penfold et al., ). In particular, most efficient TADF emitters are based on covalently bonded donors and acceptor conjugated backbones, with features of through-bond charge transfer (TBCT) which is crucial to realize efficient TADF (Ahn et al., ), while few of them report to date are through-space and polymers (Tsujimoto et al., ). Nonetheless, a strong electron coupling between donors and acceptors mediated by covalent bonds enables the display of large oscillator strength and high PLQY (Nobuyasu et al., ). However, due to the lack of universal design methodologies and principles, the development of organic luminogens with multicolor and white-light emissions are predominantly still under investigation. Generally, these types of materials possess numerous versatile photophysical phenomenon brought about by radiative emission, generally mediated through intramolecular charge transfer (ICT), vibrational relaxation, singlet-triplet intersystem crossing (ISC), internal conversion (IC), vibrational relaxation, etc., resulting in either fluorescence and phosphorescence (Itoh, ). Emission and relaxation processes are thus carefully investigated by manipulating excited states for donor-acceptor structural configurations (Berberan-Santos and Garcia, ), where emission depends on their different excited state's energy levels and probable excitons transition over these states. Therefore, by tuning the excitons of electronically excited states with effective transitions, different and distinct excited energy levels with effective transitions evolved through which photophysical processes can be precisely controlled by means of lifetime and quantum yield (Wu et al., ) (summarized in Jablonski diagram Figure 1).
Figure 1
According to the El Sayed rule, the photophysical processes under photonic/electronic irradiation of luminogens typically produce 25% of singlet and 75% of triplet excitons, which can travel from excited singlet (S1) to ground state (S0) (i.e., fluorescence), which radiates instantly with the lifetime of a nanosecond (ns), and where the transition from triplet excited state (T1) leads to non-radiative decay due to spin being forbidden (Lower and El-Sayed, ). However, TADF is a delayed emission that originates from designing an aromatic compound with bulky steric hindrance and which is expected to resolve the issue of sinking triplet excitons. Surprisingly, triplet excitons can be upconverted into singlet, giving it additional enhanced fluorescence and a lifetime of up to several microseconds. Moreover, the reverse intersystem crossing (RISC) process was efficiently facilitated through a very low ΔEST (energy gap between S1 and T1) value (~0.3 eV, Sun et al., ; Wong and Zysman-Colman, ; Wei et al., ) which is correlated with the molecular structure of the TADF emitter, as it is proportionate to the exchange integral (J) as given in equation 1 & 2 (Shizu et al., ). Importantly, exchange integral, J depends on the electron density overlap between the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO), assuming that the S1 and T1 states are influenced by HOMO to LUMO transitions and a minimum energy difference is derived/devised from a well-separated HOMO/LUMO in a highly twisted aromatic D-A skeleton (Sun et al., ).
Where, ∅HOMO and ∅LUMO are termed as spatial distributions of the HOMO and the LUMO, and r1 r2 are position vectors, respectively (Moral et al., ). It obeys the very small overlap between the HOMO and the LUMO, hence, decreases the exchange integral (J) and ΔEST value. Subsequently, if the ΔEST is sufficiently moderate, or is in the presence of a non-metallic heavy atom, carbonyl, thioesters, or when assisted by polymer host matrix, both SOC and faster ISC processes were favored, thereby leading to triplet emission at room temperature, called room temperature phosphorescence (RTP), which has a lifetime span of microseconds to seconds (Chen and Liu, ). Therefore, the primary goal is to utilize triplet excitons to achieve 100% internal quantum efficiency (IQE) by utilizing the concept of either TADF or RTP. Moreover, accurate quantum yields of fluorescent (φF) and TADF (φTADF) materials with the rate constants of fluorescent (kF), internal conversion (kIC), TADF (kTADF), intersystem crossing (kISC), reverse intersystem crossing (kRISC), and efficiency of ISC (φISC), RISC (φRISC) can be obtained from formulas 3–8 in the solid state (Lin et al., ). By following the aforementioned equation, ΔEST can also be calculated from formula-9, where R and T signify the ideal gas constants, respectively.
Approaches to Realize MCL Properties
Mechanochromic luminescence (MCL)/electroluminescence (EL) properties are switchable optical processes, which involve many other types of emissions in a viable functional molecule that co-exists with TADF and RTP properties. Furthermore, it remains extremely challenging to design a molecule with different optical properties in a single molecular platform and has aroused a broad potential utility and inherent luminescence mechanism to develop a new class of multi-functional materials. Considering this view, the phenomenon of altering the material properties by external factors such as light, heat, pH, pressure, magnetic, or by electric field of stimuli, is known as “Piezo luminescence” and other terms like mechanofluorochromism, mechanochromic luminescence, and piezochromism are also often used in the literature for the interchangeable properties (Sagara et al., ). However, the exact mechanism of MCL is not deliberated precisely, although many strategies that have been investigated, provide certain requirements to design molecules with MCL/MR properties. Yet, the reported MR materials with thermodynamically metastable states which have varying supramolecular assemblies or high order crystallinity, including the possibilities of conformational change, excimer formation, excitons coupling, and other intermolecular interactions such as hydrogen bonding, ionic interactions, π-π stacking, Van der-Waals forces, etc., are found to exist (Kasha et al., ; Birks, ; Schmidbaur and Schier, ). Furthermore, aggregation induced emission (AIE) has also been included as a fascinating condensed state property that meets a few requirements such as TADF and MCL/MR, enabling comprehensive and versatile explorations such as security, sensors, data-storage and many other applications (Sagara et al., ).
Therefore, TADF materials with multicolor and multi-functional inclusive properties and with a significant AIE-ML field of research, has been in the spotlight recently. Additionally, single molecule white-emissive TADF material with bicolor ML strategies and molecular systems are highly desirable and have rarely been reported so far.
Recent Progress on Multi-Functional TADF Emitters
Dual-Color Emission Switching TADF-MCL/ECL
Metal free organic compounds which exhibit tunable emission and TADF, are commonly found in donor-acceptor type molecular systems which possess strong charge transfer ability, including well-separated HOMO/LUMO, resulting in a very low ΔEST value (~0.3 eV), thereby facilitating the RISC process effectively and exhibiting the TADF property with high quantum efficiency (Data and Takeda, ). D-A materials therefore display reversible and distinct emission in response to external stimuli such as rubbing, grinding, shearing, pressing, temperature, electric field, and vapor and have found multiple applications in organic electronics, sensors, probes, security inks, and many more (Chi et al., ). This type of MCL behavior is due to the reversible changes in chemical structures or reformed conformations that do not necessarily, at all times, require breaking chemical bonds, or in physical structures with their different packing modes in the same molecule but thermodynamically stable and metastable states mostly enabling tunable emission. Multi-color changing MCL materials are therefore promising tools toward sensitive sensing of physical environments such as temperature, pressure, and pH and hence they have emerged as a fascinating area of research within the last 5 years.
A TADF emitter (3,5-di(9H-carbazol-9-yl)phenyl)(pyridin-4-yl)methanone (mDCBP) comprising two meta carbazolyl units as electron donating moieties and a benzoylpyridine core as an electron accepting moiety was developed by Rajamalli et al. () (Figure 2). The D-A type molecular system was clearly revealed by the DFT study, where, HOMO of the molecule is mostly localized over the donor moiety, whereas the LUMO is localized over the acceptor unit resulting in a very small ΔEST value of 0.06 eV. This small ΔEST value facilitates the RISC process to exhibit TADF property. The molecule exhibited highly enhanced emission in solid state, in addition to a reversible, externally tunable emission (blue emission in the crystalline form and green emission in the amorphous form) response, investigated by alternating applied mechanical stimuli and solvent fuming, (detail theoretical and photophysical results for mDCBP-emitters are summarized in Table 1). The different colored emission by the same molecule was due to the change in its molecular packing mode under a different mechanical force and external stimuli. For example, the emission maximum was red shifted from 460 to 500 nm after grinding of mDCBP. The red shifting is likely due to the enhancement in the intermolecular interactions triggered by the applied external pressure. The TADF properties were clearly revealed by the transient PL measurements and the lifetime of the delayed component was found to be 0.02 μs, and the excited state lifetime was lower than the phosphorescent complexes with iridium. TADF-based blue and green OLEDs have been fabricated using mDCBP as the emissive layer, where maximum EQE were found to be 18.4 to 14.7%, respectively (detailed device configuration and performances are summarized in Table 2).
Figure 2
Table 1
| Emitter | HOMO (eV) | LUMO (eV) | Osc. Strength(f) | Theo. ΔEST (eV) | Exp. ΔEST (eV) | λmax, abs (nm) | λmax, PL (nm) | aτP(ns) | bτT(μs) | cϕ [%] | dBSλmax, PL (nm) | eASλmax, PL (nm) | fTd/Tg (°C) | References |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| mDCBP | 5.72 | 2.72 | - | 0.15 | 0.06 | 334, 372 | 467 | 6.2 | 0.2 | 90 | 460 | 500 | 394/105 | Rajamalli et al., |
| T2 | −4.97 | −2.34 | - | 0.18 | - | - | - | 4.23 | 78.5 | 33.6 | 433 | 382/95 | Ganesan et al., | |
| 2CzPN | - | - | - | - | - | 374 | 533 | 33.3 | 20 | 11 | Ishimatsu et al., | |||
| 1_R | −5.31 | −2.85 | 0.08 | 416 | 657 | 57.8 | 1.1 | 7 | 568 (1_Y), 640 (1_O) | 673 (1_R) | Okazaki et al., | |||
| 5TzPm-PXZ | −5.16 | −3 | - | 0.21 | 0.10 | 317, 421 | 567 | - | 2.9 | 64 | 583 | 599 | 471/107 | Zeng et al., |
| MeO2Qx | −5.75 | −2.90 | - | - | 0.14 | 437 | 582 | - | - | - | 534 | 586 | 365/110 | Pashazadeh et al., |
| DMAC-CNQ (Y_crystal) | −5.41 | −2.94 | - | 0.04 | - | 347, 453 | 572 | 28 | 9.6 | 34 | 539 | 610,576 | Zheng et al., | |
| FDMAC-CNQ (Y_crystal) | −5.49 | −3.02 | - | 0.03 | - | 343, 442 | 552 | 7.3 | 5.1 | 13 | 603 | 620,561 | Zheng et al., | |
| PTZ-AQ (R-crystal) | – | - | 0.0137 (S1), 0.0594 (S2) | 0.51 | 0.01 | 239, 299, 443 | 606 | - | 275.6 | 84 | 606 | ~545 | - | Huang et al., |
| TATC-BP | −5.30 | −2.83 | - | 0.08 | 0.125 | 324 | 524 | 53.5 | 0.94 | 22 | 483 | 542 | >400/ >95 | Chen et al., |
| QBP-DMAC | −5.28 | −2.83 | - | 0.40 | 0.33 | 342 | 508 | 15, 13 (doped) | 1.57, 1870(d-oped) | 78 | 463 | 525 | 427/137 | Zheng et al., |
| DPPZS–DBPHZ | - | - | 0.652 | 0.30 | - | 397, 420 | 484 | - | - | 34 | 497 | 534 | - | Takeda et al., |
| OIDBQx | −5.26 | −2.75 | - | - | 0.49 | 287, 315, 411 | 534 | 1.7 ± 0.2 | - | 31 | 494 | 522 | 398/146 | Pashazadeh et al., |
| PTZ-DBPHZ (1_R) | - | - | - | - | - | - | - | 38.42 | 0.98 | 66 | 568 (1_Y) | 673 (1_R), 640 (1_O) | - | Data et al., |
| Mono-DMACDPS | −5.30 | −2.22 | - | 0.014 | 0.09 | 362 | 471 | - | 3.8 | 39 | - | ~470 | 298/69 | Zhan et al., |
| 3-DPH-XO (crystal-C) | - | - | - | - | 0.02 | 280, 370 | 540 | 8.61 | 221 | 44 | - | - | - | Zhang et al., |
Computational and Photophysical characterizations of TADF-MCL emitters.
Prompt fluorescence lifetime (τP),
TADF lifetime (τT),
photoluminescence quantum yield (ϕ),
before stimuli (BS),
after stimuli (AS),
thermal decomposition temperature (Td)/glass transition (Tg) temperature.
N.B. All photophysical studies in toluene Rajamalli et al.,
Table 2
| Emitter | Device structure | Turn on Voltage (V) | CIE values | aEQE (%) | Brightness (Cd/m2) | bCE (Cd/A) | cLE (lm/W) | Ref. |
|---|---|---|---|---|---|---|---|---|
| mDCBP | ITO/NPB /mCP /DPEPO:mDCBP /PPT/TmPyPb /LiF /Al | 3.6 | (0.16; 0.25) | 18.4 | 1,870 | 34.0 | 26.5 | Rajamalli et al., |
| T2 | ITO/TAPC/mCP:T2/DPEPO:T2/TmPyPB/LiF/Al | 3.0 | (0.20, 0.39) | 14.2 | 7,385 | 34.2 | 29.8 | Ishimatsu et al., |
| 1 | ITO/NPB/CBP:1/TPBi/LiF/Al | - | - | 16.8 | ≥25,000 | 19.6 | - | Okazaki et al., |
| 5,7TzPmPXZ | ITO/(PEDOT:P-SS)/ CBP:5,7TzPmPXZ / (TmPyPB)/Liq/Al | - | (0.43, 0.53) | 14.3 | 12,210 | 41.9 | - | Zeng et al., |
| MeO2Qx | ITO/HIL)/PVK: PBD-MeO2QX/TPBi/LiF/Al | 5.0 | (0.41, 0.53) | 10.9 | 16,760 | Pashazadeh et al., | ||
| TATC-BP | ITO/PEDOT:PSS/TATC-BP/TmPyPB/LiF/Al | 2.6 | (0.41, 0.54) | 5.9 | - | 17.8 | 20.0 | Chen et al., |
| TATC-BP | ITO/PEDOT:PSS/TATC-BP (30 wt%) :H2/TmPyPB/LiF/Al | 2.8 | (0.37, 0.53) | 15.9 | - | 48.1 | 47.8 | Chen et al., |
| QBP-DMAC | ITO/ TAPC/ TCTA/CBP: QBP-DMAC/ TmPyPB/LiF/Al | 3.6 | (0.30, 0.53) | 18.8 | 2,264 | 56.8 | 55.8 | Zheng et al., |
| 1 | ITO/HIL PEDOT:PSS /CBP:1–DEVEVP/TPBi/LiF/Al | 2.7 | 16 | 28,642 | Zheng et al., |
TADF-OLED device configurations and related EL-device performances.
External quantum efficiency (EQE),
current efficiency (CE),
luminous efficiency (LE).
In previous work pyridine moiety was found to be an important role to realize both TADF and MCL: Later, pyrimidine moiety was introduced by Ganesan et al. (
Figure 3

(A) Chemical structures of pyrimidine-acceptor core based TADF molecules. (B) Frontier molecular orbitals (HOMOs and LUMOs) related to the minimum optical transitions with calculated dihedral angles between the planar dimethyl acridine to the central phenylene substituent are 88.91° and 90.38° 89.97°, and 89.99° for T1-T4 in DCM, respectively. (C) Photographs of the ambient and luminescence materials under UV-lamp; color changes of T2 in response to mechanical grinding. (D) Current density (J) -voltage (V)-luminance, and (E) EQE-luminance plots of the white OLEDs. Reproduced with permission from Ganesan et al. (
Notably, a series of D-A type TADF molecules (2CzPN, 4CzPN, 4CzIPN, and 4CzTPN) have been reported by Ishimatsu et al. (
Figure 4

(A) Electronic transitions representation (B,C) Four TADF molecules and their molecular structure normalized electrogenerated chemiluminescence (ECL) spectra of TADF molecules in DCM (top) and MeCN (bottom). Reproduced with permission from Ishimatsu et al. (
Multi-Color and Multi-Functional Emission Switching From Crystalline TADF-MCL
In general donor-acceptor systems are very flexible to show dual emission switching under external stimuli. However, it is very challenging to obtain multicolor emission switching from a single molecular system unless it bears a non-planar geometry, either of the donor or acceptor group. Interestingly, most of the materials in this category are very crystalline in nature enabling it to exhibit multi-color emission and multiple forms of crystals, through a simple tuning of the crystal growth environment and non-covalent interactions, to address the structure-property relationship with the TADF phenomenon. In this regard, some of the emitters showed room temperature phosphorescence (RTP), a rare class of photophysical properties of purely organic compounds. Impressively, all the non-radiative excitons can be easily harvested, and device efficiency could be improved by this additional functionality of TADF-MCL emitters.
On the aforementioned view, Okazaki et al. (
Figure 5

(A) Molecular configurations of DBHZ-cored D-A-D triads. (B,C) Schematic representation of mechanoluminescence property of 1 and 2, respectively, under a 365 nm UV lamp. Reproduced with permission from Okazaki et al. (
Lateron Zeng et al. (
Figure 6

(A) Molecular structures of studied compounds. Photos and PL spectra of (B) 5TzPmPXZ, (C) 7TzPmPXZ, and (D) 5,7TzPmPXZ in response to external stimuli. Under 365nm UV irradiation (G: grinding with a mortar and a pestle; H: heating at 150°C for 5TzPmPXZ and 7TzPmPXZ, 200°C for 5,7TzPmPXZ; F: fuming with CH2Cl2 vapor; R: recrystallization from n-hexane/CHCl3). (E) OLED performances: (a) the energy level diagrams for the devices A, B, and C, (b) chemical structures of HTL-PEDOT:PSS, CIL-Liq, Host-CBP, and ETL-TmPyPB. (c) J-V-L curves for devices A, B, and C (inset: the normalized EL spectra of devices). (d) EQE and LE vs. luminance curves for devices A, B, and C. Reproduced with permission from Zeng et al. (
A series of four new D-A-D type TADF-MCL luminogens with reversible turn-on/off TADF properties in the solid state have been reported by the group of J. V. Grazulevicius (Pashazadeh et al.,
Figure 7

(A) TADF chemical structure of D-A-D triads. (B) Images of tCzQx at different forms (top-left); Distinct PL-decay plots of different states of tCzQx (bottom-left). (C) Time- resolved PL- spectra of the compound (solid lines: prompt fluorescence, dashed lines: delayed fluorescence). Reproduced with permission from Pashazadeh et al. (
In a very recent report, another exciting finding by Zheng et al. (
Figure 8

(A–F) Chemical structures, Photographs, normalized emission spectra of obtained polymorphic solids of DMAC-CNQ and FDMAC-CNQ, respectively. (G,H) Photographs and normalized PL spectra of mechanochromism properties and (I,J) transient PL decay spectra of the two TADF-emitters. Reproduced with permission from Zheng et al. (
Huang et al. (
Figure 9

(A) Structure of D-A type PTZ-AQ molecule. (B) Photographs taken at different solid states (under ambient light-left; under UV irradiation- right; scale bar: 200 μm). (C) Intermolecular non-covalent interactions (along the b axis) of Y-crystal, O-crystal and R-crystal, respectively. (D) P-XRD pattern of different solid states of PTZ-AQ. (E) Image of the drown “ML” shape by the R-solid of PTZ-AQ under daylight (top); the image of shape “ML” (up) under heating condition at 150°C for 30 s in daylight (bottom). Reproduced with permission from Huang et al.,
Two new solution-processable triazatruxene-based small molecules, Bis(4-(10,15-dihexyl-10,15-dihydro-5H-diindolo[3,2-a:30,20-c]carbazol-5-yl)phenyl) methanone (TATC-BP) and bis(4-(10, 15-diphenyl-10,15-dihydro-5H-diindolo[3,2-a:30,20-c]carbazol-5-yl)phenyl) methanone (TATP-BP), were designed and synthesized by Chen et al. (
Figure 10

(A) Molecular structures of TATC-BP and TATP-BP (B) Luminescence images (under 365 UV-lamp) of the pristine crystalline, ground, and vapor fumed powders of the emitters. (C) Normalized MCL PL spectra of the emitters. Device configuration. (D) J-V-L graph (E) EQE and EL characteristics. Inset: EL spectra of the OLED devices at 1,000 cd Reproduced with permission from Chen et al. (
Zheng et al. (
Figure 11

(A) Chemical structure of QBP-PXZ and QBP-DMAC (B) molecular configurations in single crystal XRD (hydrogen excluded). (C) PL spectra and MCL images of QBP-DMAC in (under 365 nm UV light) (D) PXRD patterns of QBP-DMAC. (E) Energy level diagram, device and material structures (F) luminance vs. EQE plots. Inset: Normalized EL spectra. (G) Luminance–voltage–current density plots. Reproduced with permission from Zheng et al. (
Multi-properties of a novel π-conjugated remarkably twisted D-A-D were investigated in purely organic triad DPPZS–DBPHZ, by Takeda et al. (
Figure 12

(A) Chemical structures of investigated molecules and the frontier orbitals of the conformers of 1. (B) Summary of the Mechanoluminescence property of 1 (C) Emission intensity at various temperatures of DPPZS-DBPHZ against delay time (D) PL spectra (Normalized) of 1 at various temperatures. Reproduced with permission from Takeda et al. (
Tashazadeh et al. reported four new derivatives of quinoxaline-containing iminodibenzyl and iminostilbene moieties with TADF, RTP, and MCL properties (shown in Figure 13) (Pashazadeh et al.,
Figure 13

(A) Structures of AzQx, IDBQz, ISBQx, OIDBQx. (B) DF intensity vs. laser pulse energy plot of OIDBQx (at 295 K); (C) PL decay transients of OIDBQx at different temperature; (D) DF and RTP spectra (at 295 K) with different excitation pulse energy. Reproduced with permission from Pashazadeh et al. (
A multi-color-changing D-A-D type MCL-TADF-RTP material PTZ-DBPHZ was developed by Data et al. (
Figure 14

(A) Chemical structure of 1 with respective conformers (B) A comparison of characteristics of OLED devices and EL spectra (C) MCL properties in various conformers. Reproduced with permission from Data et al. (
Zhan et al. (
Figure 15

(a) Configurations and XRD structures of the molecules. (b) Energy level diagrams (of the monomer and dimer of mono-DMACDPS). (c,d) PL spectra of studied molecules (at 300 K). (e,f) The TRPL spectra of studied molecules. Bottom Crystal images of mono-DMACDPS (UV lamp—on and off). Reproduced with permission from Zhan et al. (
Single Emitting White-TADF-MCL
Single molecule based white-light emitting TADF emitters have long-standing demand in solid-state lighting, display, and OLED applications due to their high triplet energy and full width at half maximum (FWHM). In addition, very few white-TADF emitters inherently manifest MCL behavior which are strongly governed by weak non-covalent interactions and constructed by a dual color emissive entity in a single molecular platform, enabling the transfer of full energy either to counter the green and red fluorescent emitter or by the complementary yellow emitter. Hence, a smart design and effective non-covalent interactions are prerequisites to realizing TADF-white light in the accompanying tunable emission.
Xu et al. (
Figure 16

(A) Molecular configuration of the compounds. (B) Decays associated with corresponding electronic transitions in SCP. (C) PL study of the parent molecules in solid-powder form. (D) Mechanochromism in SCP molecule. (E) Compound images under the UV-irradiation of 365 nm. (F) Single crystal analysis and crystalline molecular packing of the compounds along with corresponding photo luminence spectra of the single crystals and normal compounds. Insets: fluorescence images (365 nm UV-excitation). Reproduced with permission from Xu et al. (
An efficient and simple D-A approach to achieve white light from organic solids with a polymorph dependent TADF property has been developed by Ban et al. (
Figure 17

(A) Chemical structure of 3-DPH-XO (left side-top) followed by single crystal structure (left side-bottom) and theoretical spatial HOMO-LUMO distribution. (B) Photographs of the polymorphs with normalized fluorescence spectra (bottom) recorded under 365 nm UV excitation. (C) Result of 20 combined emission spectra of powdered-3-DPH-XO under 365 nm UV irradiation; inset: (1 and 2) fluorescence microscopy image of the powder. (D) Respective color-coordinates (CIE 1931) of 20 random emission spectra of solid- 3-DPH-XO under 365 nm UV excitation. (E) Intermolecular interactions and overlaps in A (a), B (b), and C (c) crystals. Reproduced with permission from Zhang et al. (
Conclusion and Outlook
In summary, the rapid development of TADF research has resulted in a new dimension of luminescence features, by building up the substantial information into new material designs, exciting and unique key functional behaviors, and essentially providing a mechanistic understanding of TADF processes. However, this review has attempted to concentrate on the recent progress made in the development of multifunctional metal free organic emitters, focusing on aggregate state emissions, TADF, and other multi-functionalities such as ML, MCL, ECL, and white light emission properties in a single molecular platform. Furthermore, a brief overview was provided on the structure-property relationship between self-assembled solid state and excited state dynamics in order to explore the opportunities for the rational design of multiple emission functions into single organic molecules and the further implementation into lighting applications, which are still in their infancy. In addition, this review includes the “state of the art” simple OLED device fabrications protocol and emphasized impressive output by exploiting multi-function TADF materials. More importantly, these multifunctional emitters are considered to be promising candidates for solution processed economical device fabrications owing to their tunable condensed state emissions. We believe that the rapid developments taking place in this field is generating enthusiasm, motivating researchers to explore a deeper understanding and finding new advancements in this exciting area of research. We expect this review to provide a clear prospect and to attract researchers with diverse interests to these novel multi-functional materials, to devote themselves to the development of materials, methods, and applications in this interesting interdisciplinary topic.
Statements
Author contributions
DB planned and compiled the review article. RG compiled the text, figures, and references. KN compiled the text and references. PI initiated, planned, and compiled the review. All authors contributed to the article and approved the submitted version.
Acknowledgments
The authors thank DST (TSG and CRG), India project numbers CRG/2019/002614, DST/TSG/PT/2009/23, Max-Planck-Gesellschaft project number IGSTC/MPG/PG(PKI)/2011A/48 and DeiTy, India project no. 5(9)/2012-NANO (Vol. II) for financial support. No funding agency has supported for open access publication fees, neither has out host institution supported us.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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Summary
Keywords
delayed fluorescence (DF), phosphorecence, donor - spacer - acceptor structure, organic light emitting diode (OLEDs), mechanochromic fluorescence, aggregation induced emission (AIE), structure property correlation
Citation
Barman D, Gogoi R, Narang K and Iyer PK (2020) Recent Developments on Multi-Functional Metal-Free Mechanochromic Luminescence and Thermally Activated Delayed Fluorescence Organic Materials. Front. Chem. 8:483. doi: 10.3389/fchem.2020.00483
Received
31 January 2020
Accepted
11 May 2020
Published
30 June 2020
Volume
8 - 2020
Edited by
Chihaya Adachi, Kyushu University, Japan
Reviewed by
Dianming Sun, University of St Andrews, United Kingdom; Paloma Lays Dos Santos, University of Cambridge, United Kingdom; Rajamalli Pachaiyappan, Indian Institute of Science (IISc), India
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*Correspondence: Parameswar Krishnan Iyer pki@iitg.ac.in
This article was submitted to Organic Chemistry, a section of the journal Frontiers in Chemistry
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