Synthesis and Characterization of Photoluminescence Liquid Crystals Based on Flexible Chain-Bearing Pentaﬂuorinated Bistolanes

: The liquid-crystalline (LC) and photophysical properties of molecules are very sensitive to their electronic and molecular aggregate structures. Herein, to shed light on the structure–property relationships of pentaﬂuorinated bistolane-based photoluminescence (PL) liquid crystals (PLLCs) previously reported by our group, we synthesized pentaﬂuorinated bistolanes with variable ﬂexible chains and evaluated their LC and photophysical properties. The incorporation of an oxygen atom (to a ﬀ ord a 2-methoxyethoxy unit) or an oxygen atom and a methyl group (to a ﬀ ord a 1-methoxyprop-2-oxy unit) into the ﬂexible butoxy chain signiﬁcantly decreased the temperature of the crystalline-to-LC phase transition, and a chiral nematic phase comprising helical molecular aggregates was observed for the chiral 1-methoxyprop-2-oxy group–bearing bistolane. The synthesized bistolanes exhibited strong blue PL in both solution and crystalline phases; the featuring PL characteristics were maintained in the LC phase (produced by the crystalline-to-LC phase transition) except for a slight PL color change. Thus, it was concluded that the PL behavior of pentaﬂuorinated bistolanes can be modulated by the choice of a suitable ﬂexible chain, and the obtained insights are believed to facilitate the application of PLLCs in thermosensing PL materials.


Introduction
The development of novel light-emitting (LE) materials has attracted much attention, as they are widely used to detect cancer cells and protein localization/activity [1][2][3][4][5] and can also find optoelectronic applications, e.g., in lighting or displays [6][7][8][9][10]. Therefore, the exploration of efficient LE molecules for practical applications remains a hot research topic. Although various kinds of LE molecules featuring extended π-conjugated structures have been reported thus far [11], most of them display luminescence only in the solution phase because of aggregation-caused luminescence quenching in the solid phase [12]. Tang and co-workers [13][14][15][16] advocated several light emission phenomena, e.g., crystallization-or aggregation-induced emission; however, the development of LE molecules intensely emitting even in molecular aggregated (e.g., crystalline and liquid-crystalline (LC)) states remains challenging.
Over the past few years, our group has pursued the development of fluorine-containing organic materials and has developed negative-type LC molecules with the CF 2 CF 2 -containing carbocycles A and the mesogenic structure B [17][18][19]. Moreover, the scope of π-conjugated photoluminescence (PL) molecules was extended to include a pentafluorinated aromatic scaffold, as exemplified by fluorinated tolanes C and bistolanes D (Figure 1a) [20][21][22]. The investigation of pentafluorinated bistolane-based

General
1 H and 13 C NMR spectra were recorded using an AVANCE III 400 NMR spectrometer (Bruker, Rheinstetten, Germany) ( 1 H: 400 MHz, 13 C: 100 MHz) in chloroform-d (CDCl3) solution, and chemical shifts were reported in parts per million (ppm) and referenced to the residual proton signal of the NMR solvent. 19 F NMR (376 MHz) spectra were acquired in CDCl3 solution with CFCl3 (δF = 0 ppm) as an internal standard using the same instrument. Infrared (IR) spectra were recorded on a FT/IR-4100 type A spectrometer (JASCO, Tokyo, Japan) using the KBr pellet method. High-resolution mass spectrometry (HRMS) analysis was performed on a JMS-700MS instrument (JEOL, Tokyo, Japan) using fast atom bombardment (FAB) as an ionization method. All reactions were performed using dried glassware and a magnetic stir bar. All chemicals were of reagent grade and were purified in the usual manner prior to use when necessary. Column chromatography was conducted using silica gel (FUJIFILM Wako Pure Chemical Corporation, Wako-gel® 60N, 38-100 μm; Osaka, Japan), while thin layer chromatography (TLC) was performed on silica gel TLC plates (Merck, Silica gel 60F254; New Jersey, NJ, USA).

General
1 H and 13 C NMR spectra were recorded using an AVANCE III 400 NMR spectrometer (Bruker, Rheinstetten, Germany) ( 1 H: 400 MHz, 13 C: 100 MHz) in chloroform-d (CDCl 3 ) solution, and chemical shifts were reported in parts per million (ppm) and referenced to the residual proton signal of the NMR solvent. 19 F NMR (376 MHz) spectra were acquired in CDCl 3 solution with CFCl 3 (δ F = 0 ppm) as an internal standard using the same instrument. Infrared (IR) spectra were recorded on a FT/IR-4100 type A spectrometer (JASCO, Tokyo, Japan) using the KBr pellet method. High-resolution mass spectrometry (HRMS) analysis was performed on a JMS-700MS instrument (JEOL, Tokyo, Japan) using fast atom bombardment (FAB) as an ionization method. All reactions were performed using dried glassware and a magnetic stir bar. All chemicals were of reagent grade and were purified in the usual manner prior to use when necessary. Column chromatography was conducted using silica gel (FUJIFILM Wako Pure Chemical Corporation, Wako-gel®60N, 38-100 µm; Osaka, Japan), while thin layer chromatography (TLC) was performed on silica gel TLC plates (Merck, Silica gel 60F 254 ; New Jersey, NJ, USA).

Typical Synthesis of R-5b
A two-necked round-bottomed flask with a Teflon ® -coated stir bar was charged with freshly prepared R-4b (2.17 g, 6.0 mmol) and K2CO3 (0.12 g, 9.0 mmol) in methanol (20 mL), and the mixture was stirred at 25 °C for 12 h. The precipitate was separated by atmospheric filtration, and the filtrate was poured into saturated aqueous NH4Cl (20 mL). The mixture was extracted with EtOAc (3 × 40 Scheme 1. Syntheses of pentafluorinated bistolanes 2a and 2b.

Typical Synthesis of R-5b
A two-necked round-bottomed flask with a Teflon ® -coated stir bar was charged with freshly prepared R-4b (2.17 g, 6.0 mmol) and K 2 CO 3 (0.12 g, 9.0 mmol) in methanol (20 mL), and the mixture was stirred at 25 • C for 12 h. The precipitate was separated by atmospheric filtration, and the filtrate was poured into saturated aqueous NH 4 Cl (20 mL). The mixture was extracted with EtOAc (3 × 40 mL), and the organic layer was washed with brine (20 mL), dried over anhydrous Na 2 SO 4 , filtered, and concentrated in vacuo using a rotary evaporator. The obtained residue was purified by silica gel column chromatography using n-hexane:EtOAc (15:1, v/v) as an eluent to obtain the desired product (R-5b; 1.6 g, 5.3 mmol) as a pale-green solid in 89% yield.

Computations
All computations were performed using density functional theory (DFT) and the Gaussian 16 (Revision B.01) software package [27]. Geometry optimizations were executed using the M06-2X hybrid functional [28,29] and the 6-31+G(d) basis set with the implicit solvation model (conductor-like polarizable continuum model (CPCM) [30][31][32]) for CH 2 Cl 2 . The vertical excitation energies and dipole moments of optimized structures were calculated using the time-dependent DFT (TD-DFT) method at the same level of theory.

Phase Transition Behavior
Phase transition behaviors were observed by polarizing optical microscopy (POM) using a BX53 microscope (Olympus, Tokyo, Japan) equipped with a cooling and heating stage (Linkam Scientific Instruments, 10002L; Surrey, UK). Thermodynamic characterization was performed by DSC (Shimadzu DSC-60 Plus; Kyoto, Japan) at heating and cooling rates of 5.0 • C min −1 under N 2 .

Photophysical Behavior
UV-vis absorption spectra were recorded on a V-500 absorption spectrometer (JASCO, Tokyo, Japan). Samples for absorption measurements were prepared by dissolving crystalline 2a or 2b in a common organic solvent to a concentration of 1.0 × 10 −5 mol L −1 and transferring the solution to a quartz cuvette with an optical path length of 1 cm. Steady-state photoluminescence (PL) spectra and PL quantum yields (PLQYs) in solution and crystalline states were obtained using a FP-6000 fluorescence spectrometer (JASCO, Tokyo, Japan) and an absolute PLQY measurement system (Hamamatsu Photonics KK., C11347-01, Hamamatsu, Japan). PL measurements were performed for 1.0 × 10 −6 mol L −1 solutions using quartz cuvettes with an optical path length of 1 cm. The excitation wavelength (λ ex ) corresponded to the maximum absorption wavelength. For excitation and PL measurements, crystalline powder samples were placed between two quartz glass plates. PL samples containing LC phases were prepared by flash-freezing in a liquid N 2 bath after the thermal phase transition and were placed between two quartz glass plates. For measurements of PLQY in the crystalline state, samples were placed above a quartz Petri dish and characterized using a calibrated integrating sphere.

Theoretical Molecular Design and Synthesis
The validity of our molecular design for 2a and 2b was ascertained by the theoretical assessment of these compounds using M06-2X/6-31+G(d)-level DFT calculations and the CPCM for CH 2 Cl 2 . In addition, previously reported compound 1 bearing a simple butoxy chain was characterized as a reference. Figure 2 shows the optimized geometries as well as highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) distributions for 1, 2a, and S-2b, while Table 1 summarizes the calculated HOMO and LUMO energy levels, molecular dipole moments  S15-S17 and Tables S1-S6).  μ||, which helps one to quantitatively understand the electron density distribution, was  µ || , which helps one to quantitatively understand the electron density distribution, was calculated as 5.28, 6.21, and 6.73 D for 1, 2a, and S-2b, respectively, i.e., the induction effect of the electronegative oxygen atom in the flexible units of 2a and 2b increased µ || . Accordingly, the change of the flexible unit from a simple alkoxy chain to the 2-methoxyethoxy fragment allowed one to control the electron density distribution on the pentafluorinated bistolane moiety and thus enabled the easy tuning of phase transition and photophysical properties. Regarding the molecular geometries of 1 and 2a, the oxygen atom in the flexible unit did not induce any change in the molecular structure, whereas in the case of 2b, the methyl substituent significantly altered the molecular geometry, effectively inducing a large deviation of the flexible chain from the plane of the bistolane scaffold. These deviations were quantified by comparison of C1-O1-C2-C3 (φ 1 ), C2-C3-C4(O2)-C5 (φ 2 ), C1-O1-C2-H1 (φ 3 ), and C1-O1-C2-C6 (φ 4 ) dihedral angles, and (φ 1 , φ 2 , φ 3 ) values of (179.4 • , 178.5 • , 59.8 • ) for 1 and (179.6 • , 178.8 • , 60.8 • ) for 2a, and (φ 1 , φ 2 , φ 4 ) values of (159.2 • , 178.2 • , 79.9 • ) for S-2b were obtained. These data suggested that the incorporation of a methyl substituent into the flexible unit (i.e., branching) significantly altered molecular geometry and could therefore affect aggregation behavior. As a whole, the transition from 1 (carrying a simple alkoxy unit) to 2a (carrying a linear 2-methoxyethoxy unit) and 2b (bearing a branched 1-methoxyprop-2-oxy unit) was used to elucidate the effect of molecular structure on the phase transition behaviors and photophysical properties of PLLC molecules.

Phase Transition Behavior
The phase transition behaviors of freshly prepared 2a, rac-2b, R-2b, and S-2b were probed by DSC and POM. Figure 3 shows the corresponding DSC thermograms recorded during the second heating and cooling cycles, with the obtained phase transition sequences and enthalpies summarized in Table 2 and Tables S7-S10.  Upon heating to 134 • C, the crystalline (Cr) phase of 2a changed to an LC phase with a fluidic bright-view optical texture. Optical imaging of the LC phase afforded a four-brush Schlieren image typical of the nematic (N) phase; thus, 2a formed the nematic LC phase in the second heating step. Further heating of the N-phase of 2a to 212 • C resulted in a new phase transition that was accompanied by a POM texture change from a Schlieren image to a fluidic dark-view field. The latter image was assigned to an isotropic (Iso) phase with no directional and positional orders. During the cooling step, two phase transitions were observed at 212 • C (Iso→N) and 127 • C (N→Cr). Compared to that of 1 (Figure 1b), the Cr→N transition temperature of 2a was higher by approximately 10 • C, and hence, the incorporation of oxygen into the flexible unit was concluded to enhance the stability of the Cr-phase, possibly by allowing for intermolecular hydrogen bonding.

Molecule Phase Transition Sequence (Enthalpy [kJ mol
was purified by column chromatography followed by recrystallization. Other analogues bearing a 1methoxyprop-2-yloxy flexible chain, namely rac-2b, R-2b, and S-2b, were obtained using a similar three-step protocol and purified as in the case of 2a. As a result, 2a and 2b were found to be sufficiently pure for phase transition and photophysical behavior characterization (Figure S1-S14).

Phase Transition Behavior
The phase transition behaviors of freshly prepared 2a, rac-2b, R-2b, and S-2b were probed by DSC and POM. Figure 3 shows the corresponding DSC thermograms recorded during the second heating and cooling cycles, with the obtained phase transition sequences and enthalpies summarized in Table 2 and Table S7-S10. In the case of rac-2b, the nematic LC phase was also detected by POM and DSC, with Cr→N and N→Iso transitions observed at 97 and 129 • C, respectively, i.e., at temperatures much lower (by approximately 40 • C for Cr→N and by 83 • C for N→Iso) than those of 2a. This behavior was not unexpected, as the methyl substituent of 2b readily destructed the ordered crystalline lattice and directionally ordered N phases. The chiral species, i.e., R-2b and S-2b, exhibited Cr→mesophase (at 102 • C) and mesophase→Iso (at 130 • C) phase transitions during the second heating process. Careful POM observation of the mesophase revealed a fingerprint texture typical of the chiral nematic (N*) phase and thus suggested the formation of helical molecular aggregates in the chiral LC phases of R-2b and S-2b. Compared to those of rac-2b, the phase transitions of chiral R-2b and S-2b (Cr→N* and N*→Iso) occurred at slightly higher temperatures, which is a generally reported phenomenon [33].
Thus, the change from a simple alkoxy chain to a linear or a branched 2-methoxyethoxy-type flexible unit strongly influenced phase transition behavior, while the incorporation of an oxygen atom and a methyl substituent significantly reduced the temperature of both Cr LC and LC Iso transitions. In addition, a chiral flexible unit was concluded to be essential for the generation of helical structures induced by the formation of a chiral LC (i.e., N*) phase [34].

Photophysical Behavior in Solution
To gain more insights into flexible-chain structures, we focused on their effect on photophysical behavior. First, the absorption and PL properties of 2a, rac-2b, R-2b, and S-2b were investigated in dilute CH 2 Cl 2 solutions (1.0 × 10 −5 mol L −1 for absorption and 1.0 × 10 −6 mol L −1 for PL measurements). Figure 4a and Figure S22 shows the absorption and PL spectra of CH 2 Cl 2 solutions as well as photographs of these solutions under UV irradiation (λ ex = 365 nm), with the collected photophysical data summarized in Table 3. In addition, Figure 4b shows the positions of the investigated samples on the PL color diagram defined by the Comission Internationale de l'Eclairage (CIE).
Crystals 2020, 10, x FOR PEER REVIEW 9 of 15 summarized in Table 3. In addition, Figure 4b shows the positions of the investigated samples on the PL color diagram defined by the Comission Internationale de l'Eclairage (CIE).
(a) (b)   Figure 4a shows that the spectra of 2a, rac-2b, R-2b, and S-2b featured a single absorption band with a maximum (λabs) at around 333 nm and exhibited identical shapes, which indicated that in dilute solution, these species possessed the same (i.e., flexible chain-independent) electronic structure. The observed maximum absorption wavelengths (333 nm) were almost in accord with the theoretical vertical transition energies (334 nm or 335 nm) predicted by TD-DFT calculations (Table 1), and the electronic transitions observed in absorption spectra were therefore identified as HOMO→LUMO ones. Analysis of the HOMO and LUMO of 2a and S-2b showed that the HOMO lobes were largely localized on the electron-rich aromatic ring attached to the flexible unit, while LUMO lobes were localized on the electron-deficient pentafluorobenzene ring. The above distributions and the relatively large longitudinal molecular dipole moment suggested that the present HOMO→LUMO electronic transition was of the intramolecular charge transfer (ICT) type.
Irradiation of dilute sample solutions in CH2Cl2 at λabs resulted in strong PL with maxima (λPL) at 406 nm (2a) and 412 nm (2b), with PL efficiency (ΦPL) reaching 0.90. According to the CIE color   Figure 4a shows that the spectra of 2a, rac-2b, R-2b, and S-2b featured a single absorption band with a maximum (λ abs ) at around 333 nm and exhibited identical shapes, which indicated that in dilute solution, these species possessed the same (i.e., flexible chain-independent) electronic structure. The observed maximum absorption wavelengths (333 nm) were almost in accord with the theoretical vertical transition energies (334 nm or 335 nm) predicted by TD-DFT calculations (Table 1), and the electronic transitions observed in absorption spectra were therefore identified as HOMO→LUMO ones. Analysis of the HOMO and LUMO of 2a and S-2b showed that the HOMO lobes were largely localized on the electron-rich aromatic ring attached to the flexible unit, while LUMO lobes were localized on the electron-deficient pentafluorobenzene ring. The above distributions and the relatively large longitudinal molecular dipole moment suggested that the present HOMO→LUMO electronic transition was of the intramolecular charge transfer (ICT) type.
Irradiation of dilute sample solutions in CH 2 Cl 2 at λ abs resulted in strong PL with maxima (λ PL ) at 406 nm (2a) and 412 nm (2b), with PL efficiency (Φ PL ) reaching 0.90. According to the CIE color diagram, the CH 2 Cl 2 solutions of 2a and 2b showed deep blue PL that was independent of the flexible chain structure, although slight differences were observed between samples ((x, y) = (0.16, 0.19) for 2a, (0.15, 0.11) for rac-2b, (0.16, 0.10) for R-2b, and (0.16, 0.09) for S-2b). Considering the almost identical PL behavior of the above species in CH 2 Cl 2 solution, their strong deep blue PL was concluded to originate from the same process of radiative exciton deactivation (i.e., ICT).
To gain further insights into electronic transitions from the ground state to excited states, we investigated the effect of solvent on the photophysical behavior of S-2b. Figure 5a and Figure S23 shows the results of absorption and PL measurements for common organic solvents, namely toluene, chloroform (CHCl 3 ), tetrahydrofuran (THF), acetonitrile (MeCN), and N,N-dimethylformamide (DMF), with the corresponding CIE color diagram shown in Figure 5b. To gain further insights into electronic transitions from the ground state to excited states, we investigated the effect of solvent on the photophysical behavior of S-2b. Figure 5a and S23 shows the results of absorption and PL measurements for common organic solvents, namely toluene, chloroform (CHCl3), tetrahydrofuran (THF), acetonitrile (MeCN), and N,N-dimethylformamide (DMF), with the corresponding CIE color diagram shown in Figure 5b. The values of λabs obtained by UV-vis absorption measurements (330-333 nm) were almost independent of solvent polarity, in contrast to λPL (381-443 nm). The relationship between solvent polarity and photophysical behavior was quantitatively evaluated with the help of a Lippert-Mataga plot (Figure 5c, Table S11) [35][36][37], which shows the dependence of Stokes' shift (Δν) on orientation polarizability (Δf) calculated from the solvent dielectric constant (ε) and refractive index (n) (Eq. 1): Here, μe and μg are the dipole moments of the ground and excited states, respectively, a is the  Table S11) [35][36][37], which shows the dependence of Stokes' shift (∆ν) on orientation polarizability (∆f ) calculated from the solvent dielectric constant (ε) and refractive index (n) (Equation (1)): ∆ν = [2(µ e − µ g ) 2 /hca 3 ]∆f + constant.
Here, µ e and µ g are the dipole moments of the ground and excited states, respectively, a is the Onsager cavity radius, h is Planck's constant, and c is the speed of light in vacuum. Figure 5c shows that the relationship between orientation polarizability and Stokes' shift could be expressed as ∆ν = 13922∆f + 3079.7, which allowed µ e − µ g to be calculated as 17.1 D and thus indicated that the molecular dipole moment of the excited state is much larger than that of the ground state. Therefore, it could be safely concluded that the electronic transition from the ground to excited states corresponds to ICT process.

Photophysical Behavior in Molecular Aggregated Phases
Subsequently, we focused on the PL behavior of 2a and 2b in the Cr-phase, with the corresponding PL spectra and CIE color diagram presented in Figure 6 and Figure S24. Table 4 lists photophysical data measured for the Cr-phase at 25 • C and for the LC phase. Subsequently, we focused on the PL behavior of 2a and 2b in the Cr-phase, with the corresponding PL spectra and CIE color diagram presented in Figure 6 and S24. Table 4 lists photophysical data measured for the Cr-phase at 25 °C and for the LC phase.  As shown in Figure 6a, 2a showed blue PL ((x, y) = (0. 16, 0.19)) with a single band (λPL ≈ 465 nm) red-shifted by approximately 60 nm relative to that in CH2Cl2 solution. For rac-2b, R-2b, and S-2b, deep blue PL with a single band at 432-449 nm was observed at 25 °C, and the PL bands were also red-shifted (by 20-37 nm) relative to those in CH2Cl2 solution. The red shift of λPL observed for the Cr-phase is a common phenomenon that is typically ascribed to non-radiative exciton deactivation via intermolecular interactions. Much to our delight, the ΦPL of Cr phases lied in the range of 0.39-0.74. As mentioned above, the PL of molecules with extended π-conjugation is rapidly quenched in  As shown in Figure 6a, 2a showed blue PL ((x, y) = (0.16, 0.19)) with a single band (λ PL ≈ 465 nm) red-shifted by approximately 60 nm relative to that in CH 2 Cl 2 solution. For rac-2b, R-2b, and S-2b, deep blue PL with a single band at 432-449 nm was observed at 25 • C, and the PL bands were also red-shifted (by 20-37 nm) relative to those in CH 2 Cl 2 solution. The red shift of λ PL observed for the Cr-phase is a common phenomenon that is typically ascribed to non-radiative exciton deactivation via intermolecular interactions. Much to our delight, the Φ PL of Cr phases lied in the range of 0.39-0.74. As mentioned above, the PL of molecules with extended π-conjugation is rapidly quenched in the solid state, possibly because of energy transfer through π/π stacking. In the present cases, the flexible unit was believed to facilitate the expansion of the interfacial π···π distance to avoid tight π/π stacking, although the accurate structures of aggregates in the Cr-phase remain unclear [38].
The LC and PL behavior of the synthesized bistolanes inspired us to probe their PLLC properties. To ascertain the applicability of these bistolanes to PLLC molecules, we investigated the PL behavior of LC phases. For these measurements, samples were prepared by flash-freezing through dipping into a liquid N 2 bath after the thermal phase transition to the LC phase, which allowed us to probe PL behavior at 25 • C while preserving the molecular aggregates in the LC phase. Figure 7 and Figure S25 shows the PL spectra of powder samples containing molecular aggregates in Cr and LC phases, with related photophysical data listed in Table 4. For 2a, the LC powder sample prepared as described above after the transition to the N-phase upon the first heating to 160 °C exhibited deep blue PL with a single band at around 442 nm and a shoulder peak at around 412 nm. Compared to that of the as-prepared Cr sample, the above PL band was blue-shifted, slightly broadened, and less intense, probably because of the promotion of nonradiative deactivation through thermal molecular motions in the latter case. Similarly, the LC powder samples of rac-2b with N-phase molecular aggregates also emitted deep blue PL with a blue-shift of λPL by 15 nm. Although the LC powder of R-2b and S-2b successfully showed deep blue PL with a single band at around 435 nm even in the N*-phase molecular aggregates, it was observed almost . PL spectra of (a) 2a with Cr-phase (green) and N-phase (yellow) molecular aggregates, (b) rac-2b with Cr-phase (pink) and N-phase (yellow) molecular aggregates, (c) R-2b with Cr-phase (red) and N*-phase (yellow) molecular aggregates, and (d) S-2b with Cr-phase (blue) and N*-phase (yellow) molecular aggregates. Abbreviations: Cr: crystal, N: nematic, N*: chiral nematic, Iso: isotropic phases.
For 2a, the LC powder sample prepared as described above after the transition to the N-phase upon the first heating to 160 • C exhibited deep blue PL with a single band at around 442 nm and a shoulder peak at around 412 nm. Compared to that of the as-prepared Cr sample, the above PL band was blue-shifted, slightly broadened, and less intense, probably because of the promotion of non-radiative deactivation through thermal molecular motions in the latter case. Similarly, the LC powder samples of rac-2b with N-phase molecular aggregates also emitted deep blue PL with a blue-shift of λ PL by 15 nm. Although the LC powder of R-2b and S-2b successfully showed deep blue PL with a single band at around 435 nm even in the N*-phase molecular aggregates, it was observed almost similar PL spectra to those of the as-prepared Cr sample. Thus, 2a, rac-2b, R-2b, and S-2b exhibited PL not only in the Cr-phase but also in the LC phase after the thermal phase transition. In addition, a slight shift of PL band position with a similar tendency to our previous report [25] was observed after the formation of other molecular aggregates through the thermal phase transition, although the effect of the Cr LC phase transition on PL behavior was not fully clear.

Conclusions
Pentafluorinated bistolanes with two types of flexible units (linear 2-methoxyethoxy and branched 1-methoxyprop-2-oxy) were prepared from readily accessible the corresponding 4-substituted phenylacetylene derivatives using a facile four-step procedure and subjected to phase transition and photophysical behavior evaluation. All of the synthesized bistolanes formed an LC phase upon both heating and cooling, and the temperature of this phase transition significantly decreased (compared to that of a simple butoxy-substituted derivative) upon the incorporation of oxygen and the introduction of a methyl substituent. For the chiral species, a fingerprint optical texture was observed in the mesophase, which clearly indicated the formation of a chiral nematic phase with helical molecular aggregates. Consequently, suitable modifications of flexible unit structure were found to affect the emergence of the LC phase and the phase transition temperature. UV-vis absorption measurements revealed that the four bistolanes exhibited identical electronic structures, and deep blue PL emission was observed in all cases in dilute solution. The species with a 1-methoxyprop-2-oxy chain showed solvatochromic PL (originating from radiative deactivation through ICT), i.e., the PL band shifted to the longer wavelengths with increasing solvent polarity. The present bistolanes showed significant PL (Φ PL of up to 0.74) even in the crystalline phase, in which case the methyl substituent was believed to enhance Φ PL by promoting the expansion of interfacial π···π distances to avoid tight π/π stacking. In addition, LC powders with preserved molecular aggregates in the LC phase also exhibited PL, which clearly indicated that the synthesized bistolanes are promising components of light-emitting liquid crystals and, hence, of next-generation functional materials.