Abstract:The recent synthesized helical tetraphenylethylene (TPE) exhibits broad application prospects such as display, catalysis, and medical imaging. A full understanding of the intricate relation between structure and property is rather important to structural design and performance improvement. Here, we employed density functional theory (DFT) and timedependent DFT to calculate their ground-and excited-state structures, electron transition properties, optical rotation (OR), and second-order nonlinear optical (NLO) … Show more
“…It has previously been used successfully as an imaging agent [155,155,180], and, in contrast to many fluorophores, it is well-known for exhibiting aggregation-induced-emission (AIE) [171,181] in which the emission intensity increases as the molecules aggregate. One study measured the nonlinear optical activity of a series of TPE structures ( Figure 6) [170]. In this study of eight different structures, the second-order NLO polarizabilities was increased as much as 27 times by tuning the substituent groups and their positions even when the primary chemical composition (the TPE core) was relatively unchanged.…”
Section: Organic Materialsmentioning
confidence: 97%
“…As mentioned, the n2 depends on the molecular density and molecular orientation with the optical field. One study measured the nonlinear optical activity of a series of TPE structures (Figure 6) (170). In this study of eight different structures, the second-order NLO polarizabilities was increased as much as 27 times by tuning the substituent groups and their positions even when the primary chemical composition (the TPE core) was relatively unchanged.…”
Section: Organic Materialsmentioning
confidence: 97%
“…TPE is an intriguing material with a unique chemical structure. In previous work, it has demonstrated large NLO coefficients, particularly the first hyperpolarizability or the second-order NLO coefficient, and the four-leaf clover architecture facilitates the design of push-pull chromophores that allows electron charge transfer across the π conjugation of the TPE molecule [170][171][172][173][174][175][176][177][178][179]. It has previously been used successfully as an imaging agent [155,155,180], and, in contrast to many fluorophores, it is well-known for exhibiting aggregation-induced-emission (AIE) [171,181] in which the emission intensity increases as the molecules aggregate.…”
AbstractAlthough the first lasers invented operated in the visible, the first on-chip devices were optimized for near-infrared (IR) performance driven by demand in telecommunications. However, as the applications of integrated photonics has broadened, the wavelength demand has as well, and we are now returning to the visible (Vis) and pushing into the ultraviolet (UV). This shift has required innovations in device design and in materials as well as leveraging nonlinear behavior to reach these wavelengths. This review discusses the key nonlinear phenomena that can be used as well as presents several emerging material systems and devices that have reached the UV–Vis wavelength range.
“…It has previously been used successfully as an imaging agent [155,155,180], and, in contrast to many fluorophores, it is well-known for exhibiting aggregation-induced-emission (AIE) [171,181] in which the emission intensity increases as the molecules aggregate. One study measured the nonlinear optical activity of a series of TPE structures ( Figure 6) [170]. In this study of eight different structures, the second-order NLO polarizabilities was increased as much as 27 times by tuning the substituent groups and their positions even when the primary chemical composition (the TPE core) was relatively unchanged.…”
Section: Organic Materialsmentioning
confidence: 97%
“…As mentioned, the n2 depends on the molecular density and molecular orientation with the optical field. One study measured the nonlinear optical activity of a series of TPE structures (Figure 6) (170). In this study of eight different structures, the second-order NLO polarizabilities was increased as much as 27 times by tuning the substituent groups and their positions even when the primary chemical composition (the TPE core) was relatively unchanged.…”
Section: Organic Materialsmentioning
confidence: 97%
“…TPE is an intriguing material with a unique chemical structure. In previous work, it has demonstrated large NLO coefficients, particularly the first hyperpolarizability or the second-order NLO coefficient, and the four-leaf clover architecture facilitates the design of push-pull chromophores that allows electron charge transfer across the π conjugation of the TPE molecule [170][171][172][173][174][175][176][177][178][179]. It has previously been used successfully as an imaging agent [155,155,180], and, in contrast to many fluorophores, it is well-known for exhibiting aggregation-induced-emission (AIE) [171,181] in which the emission intensity increases as the molecules aggregate.…”
AbstractAlthough the first lasers invented operated in the visible, the first on-chip devices were optimized for near-infrared (IR) performance driven by demand in telecommunications. However, as the applications of integrated photonics has broadened, the wavelength demand has as well, and we are now returning to the visible (Vis) and pushing into the ultraviolet (UV). This shift has required innovations in device design and in materials as well as leveraging nonlinear behavior to reach these wavelengths. This review discusses the key nonlinear phenomena that can be used as well as presents several emerging material systems and devices that have reached the UV–Vis wavelength range.
“…For instance, Liu et al designed the helical TPE compound with the inherent chirality and fixed propeller-like conformation, and predicted its second-order NLO properties via density functional theory (DFT) and time-dependent DFT calculations. [128] Nevertheless, the realistic reports about AIE molecules exhibiting SHG responses are rare. The classical AIEgen TPE also has been certified to be the SHG active.…”
Section: Second-order Nlo In Aie Materialsmentioning
Aggregation‐induced emission (AIE) is a vital photophysical phenomenon that the luminogens in the concentrated or aggregated cases will engender the dramatically boosted emission in comparison with the dispersive states. Given this extraordinary emitting capacity exactly resolves the aggregation‐caused quenching (ACQ) situations residing in the traditional luminophores, the booming AIE luminogens have drawn tremendous interest owing to their advanced performances and colossal potential applications in various areas. Further exploitations of AIE molecules also drive the research interests in the midst of these AIE materials toward the nonlinear optical (NLO) regime. The combination of AIE and NLO effects have nurtured some unforeseen properties of AIE materials and extended their application spheres. Therefore, some NLO‐active AIE materials have been wielded in many crucial applications, for example, optical limiting, laser, bioimaging, and photodynamic therapy. Meanwhile, the impacts of aggregate on the NLO effect also deserve deep considerations and pursuits, and the modifications of aggregates promise an easy, efficient, and prompt avenue to tune the NLO properties of materials. The recent achievements and progress in the NLO properties of AIE materials have been summarized in this review. The second‐order and third‐order NLOs of the AIE materials have been introduced and their correlative applications have been discussed.
“…[17][18][19][20][21][22][23][24][25][26][27][28] Nevertheless, designs trategies that employa mino acids and sugars lead to AIEgens with poor thermal stability that lacks cope forw avelengthtunability.B INOL, vastly explored in asymmetric catalysis [29][30][31][32][33] and bearing at remendous resemblance to the rotorlike structures of typical AIEgens such as tetraphenylethene (TPE) or tetraphenylsiloles, has been used to design chiralluminogens through the appendage of well-known AIEgensa ta ppropriate positions of BINOL ( Figure 1). [34][35][36] However, these existing design strategies are mostly limited to scaffolds such as TPE or tetraphenylsiloles. The dearth of protocols to generate chiral AIEgens withouta ny AIEgens (e.g.,T PE or tetraphenylsilole) externally tagged to the chiral scaffold remains al ongstanding challenge.…”
Designing chiral AIEgensw ithouta ggregation-induced emission (AIE)-active molecules externally tagged to the chiral scaffold remains al ong-standing challenge for the scientific community.T he inherenta ggregation-caused quenching phenomenon associated with the axially chiral (R)-[1,1'-binaphthalene]-2,2'-diol ((R)-BINOL)s caffold, together with its marginal Stokes shift, limits its applicationa sa chiral AIE-active material. Here, in our effort to designc hiral luminogens, we have developed ad esign strategy in which 2-substitutedf urans, when appropriately fused with the BINOLs caffold,w ill generates olid-state emissive materials with high thermala nd photostability as well as colour-tunable properties. The excellent biocompatibility,t ogetherw ith the high fluorescenceq uantum yield and large Stokes shift, of one of the luminogens stimulated us to investigate its cell-imaging potential. Thel uminogen was observedt ob e well internalised and uniformlyd ispersed within the cytoplasm of MDA-MB-231 cancer cells,s howingh ighf luorescence intensity.
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