마지막 인쇄한 날짜: 2007-04-29 오후 10 시 46 분마지막 저장한 사람: 김현정작성자: 김현정

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Ratiometry of monomer/excimer emission of dipyrenyl calix[4]arene in aqueous media

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Hyun Jung Kim,1 Duong Tuan Quang,1 Jooyeon Hong,2 Guipeun Kang,2 Sihyun Ham,2,* and Jong Seung Kim1,* 1

Department of Chemistry, Dankook University, Seoul 140-714, Korea Department of Chemistry, Sookmyung Women’s University, Seoul 140-742, Korea

2

In vacuo

In aqueous media

Tetrahedron

1

TETRAHEDRON Pergamon

Ratiometry of monomer/excimer emission of dipyrenyl calix[4]arene in aqueous media Hyun Jung Kim,1 Duong Tuan Quang,1 Jooyeon Hong,2 Guipeun Kang,2 Sihyun Ham,2,* and Jong Seung Kim1,* 1

Department of Chemistry, Dankook University, Seoul 140-714, Korea

2

Department of Chemistry, Sookmyung Women’s University, Seoul 140-742, Korea

Abstract— Monomer and excimer variations of calix[4]arene 1 having two facing amide groups linked to pyrene units were investigated in different ratios of H2O/CH3CN solvents. By the addition of more than 50 % water to the CH3CN, monomer emission declines and the excimer emission concomitantly increases. The DFT calculation supports this fluorescence spectral change that lacking intramolecular H bonds between NH and OH by inserting water molecules to 1 contributes to the favorable geometry between two pyrenes that result in a strong excimer band. When Fe3+ ion is added to the H2O/CH3CN (4:1, v/v) solution of 1 at pH 6.1, both pyrene monomer and exciemr emissions are selectively quenched because of the electron transfer (eT) from the pyrene units to Fe(III) ion. © 2007 Elsevier Science. All rights reserved

1. Introduction Calix[4]arene-based fluorogenic chemosensors are good candidates as recognition moieties for cation and anion probes because of their high selectivity toward specific metal ions.1-4 For the calix[4]arene-based fluorescent sensors, it is well known that the photochemical changes in a sensing mechanism are mainly based on the photoinduced electron/energy transfer (PET),5-7 fluorescence resonance energy transfer (FRET),8 photo-induced charge transfer (PCT),9 and excimer/exciplex formation.10 Pyrenes are one of the most useful fluorogenic units for the calix[4]arene-based fluorescent sensors because they display not only a well-defined monomer emission at 370– 430 nm but also an efficient excimer emission at around 480 nm.11,12 With an intensity ratio of excimer to monomer emission (IE/IM), which is sensitive to conformational changes of the pyrene-appended receptors, variation in IE/IM values upon metal-ion binding with the receptor molecule can be an informative parameter in the sensing systems.12,13 Corresponding authors: [email protected] (S. Ham); [email protected] (J. S. Kim), Fax: +82-2-797-3277

A variety of interesting molecules having pyrene moiety as basic signaling functions in fluorescent probes have been reported.14,15 Utilizing the characteristics of excimer emissions, a number of molecular probes for the signal transduction toward alkaline earth metal ions,16 Cu2+ ion,17,18 phosphate,6 and molecular logic circuits19 are successfully devised. We recently found interesting phenomena of ratiometric changes in monomer and excimer emissions of 1, which depends on the extent of the intramolecular H-bonding between H atom of pyrenyl amide group and O atom of the calixarene lower rim. Herein, we now report the fluorescence changes of 1 in different ratio of H2O/CH3CN to verify the excimer formation, which can be supported by DFT calculation results. In addition, we report on the Fe(III) ion selectivity of 1 regarding fluorescence intensity changes.

O OH O

O HO H H N N OO

1

O

O O

O O NH

HN

O

O

OO

2

Figure 1. Structures of fluorescent chemosensors 1 and 2.

Fluorescence Intensity (a.u.)

Tetrahedron

2

2. Results and Discussion

Meanwhile, we have studied the nature of the H-bonding of 1. In a ratio variation of H2O/CH3CN as a solvent, we found a ratiometry of monomer and excimer emissions. Figure 2 shows the fluorescence spectra of 1 as a function of H2O amount. Excitation of free 1 at 343 nm exhibits only a monomer emission at 398 nm in 100 % CH3CN due to an event of the intramolecular H-bonding interaction, which subsequently leads to have the pyrene groups pointed away from each other, thus only monomer emission of pyrene can be observed. Addition of H2O to a solution of CH3CN until the amount of water reaches to 50 % gave the monomer emission intensity of free 1 increased as shown in Figure 2(a). For the fluorescence enhancement, it is attributable to the suppression of the PET (photo-induced electron transfer) effect from N to the pyrene groups. Interestingly, we found further addition of water into the solution of 1 induces a declined monomer emission, at the same time, an increased excimer emission at 472 nm as indicated in Figure 2(b). This behavior can be ascribed to that addition of water molecule disrupts the H-bonding between NH and phenolic OH in 1 and thus makes two pyrenes have a preferential HOMO-LUMO interaction to provide the excimer emission.

(a)

600

Composition of H2O 50% 40% 30% 20% 0%

400

200

0

Fluorescence Intensity (a.u.)

In previous work, we demonstrated that free 1 exhibited only a monomer emission at around 398 nm without an excimer emission,20 which is distinguished from that found by Broan.21 He reported a fluorogenic calix[4]arene chemosensor with two facing ester groups and two pendant pyrene units linked to the ester groups which forms a strong intramolecular excimer band. Compared with those of Broan’s compound, this unique fluorescence behavior of 1 could be rationalized by its solid-state structure.20 From the crystal structure, we noticed that the intramolecular H bonds are formed between the phenolic OH groups and the amide H atoms, which is believed to preclude face-to-face π-stacking of the pyrene units and consequently to a strongly quenched excimer emission from 1. The fluorescence spectrum of 2, however, shows a strong pyrene excimer emission band and a weak monomer band because 2 does not have the two OHs in calix[4]arene lower rim to have the intramolecular H-bonding.

800

800

(b)

Composition of H2O 60% 70% 72% 74%

600

80% 78% 76%

400

200

0 350

400

450

500

550

600

Wavelength (nm) Figure 2. Fluorescent spectra of 1 (5.0 μM ) in the mixed solvent of water and CH3CN with different ratios (pH 6.1, λexc=343 nm).

For this distinctive fluorescent behavior upon the solvent ratio change, we have tried to interpret it by theoretical calculation using density functional theory (DFT).22 Ground state geometry optimization for the global minimum structure of free 1 in vacuo has been executed using B3LYP hybrid functional with 3-21G basis set.23 Several different starting geometries were used for the geometry optimization to ensure that the optimized structure corresponds to a global minimum. The lowest energy structure at this level for free 1 is displayed to be a cone conformer. As shown in Figure 3(a), two H bonds are found between the phenolic OH groups and the amide H atoms (1.70 Å) and two H bonds are between the hydrogen in OH groups and the phenolic oxygen (1.57 Å) in lower rim. Total four H bonds contribute to the stability of the cone conformer and the molecular shape is in a sound agreement with the X-ray determined structure.20

3

Tetrahedron (b)

Figure 3. Computed geometry for (a) free 1 in vacuo and (b) 1 with three water molecules.

The time dependent density functional theory (TDDFT) calculation24 was executed to characterize the nature of the fluorescence behavior. The molecular orbital energies and the singlet-singlet electronic transitions followed by their compositions were calculated from the optimized geometry of the S0 state by TDDFT/B3LYP/3-21G. Several studies have provided that hybrid functionals give better performance for evaluating electronic transition properties of organic molecules.25 Moreover, recently we have reported the computed electronic transition properties by TDDFT which is in good agreement with the experimental fluorescence spectra.4d According to the TD-B3LYP/3-21G calculation of free 1 in vacuo, the main electronic transition involves the promotion of an electron from the highestoccupied molecular orbital (HOMO) to the lowestunoccupied molecular orbital (LUMO) (see Figure 4) of each pyrene independently. Consequently, it was not detected the HOMO-LUMO transition from one pyrene to the other pyrene (Py-Py* interaction) which presumably results fluorescence excimer band. Overall, in the presence of the intramolecular H bonds between amide H and phenolic O, the eminent Py-Py* interactions are prohibited resulting quenched excimer emission of 1 due to the geometrical restriction of two pyrenyl moieties.

(a)

(b)

hydrogens (1.64Å and 1.67Å) and the third H2O imports slight reorientation to one pyrene group. Concomitantly, inserted water molecules pushed down two pyrenyl moieties away from the calix[4]arene cavity, as a result, two pyrenes are placed closer in distance to each other. The TDDFT/B3LYP/3-21G calculation of 1 with three water molecules exhibits that the HOMO is localized in one pyrene and the LUMO is in the other pyrene, and also the dominant contribution to the most probable excitation refers to the HOMO-LUMO transition which corresponds to the strong Py-Py* excimer emission band in the fluorescence spectra. (Figure 5) (a)

(b)

Figure 5. HOMO and LUMO for 1 with three water molecules computed at the TDDFT/B3LYP/3-21G level.

Based on the excimer emission enhanced, we have tested the complexation ability of 1 towards metal cations (Li+, Na+, K+, Rb+, Ag+, Mg2+, Ca2+, Ba2+, Zn2+, Cd2+, Fe2+, Co2+, Cu2+, Pb2+, Hg2+, Al3+, Fe3+, Nd3+, Er3+, and In3+) in 80 % aqueous CH3CN solution (CH3CN/H2O = 1:4, v/v) at pH 6.1, from which we observed a characteristic monomer emission at 380 nm and a broad excimer emission centered at 480 nm. Upon interaction with each cation, the fluorescence of 1 was found to show a remarkable selectively for Fe3+ ion with which the excimer emission is quenched (Figure 6). In anion test using HSO4-, CH3COO-, Br-, Cl-, F-, and I-, no changes of fluorescence in 1 were observed.

To understand the effect of water addition to the fluorescence spectra of 1, we performed the DFT calculation for 1 in the presence of explicit water molecules. We placed up to six water molecules around the amide and the hydroxyl groups to allow potential H bonds between the host and solvent H2O. Based on the B3LYP/3-21G optimization, three distinct water molecules execute conformational distortion by forming intermolecular H bonds with 1 and the resting water molecules play a minor role in determining the overall geometry. Thus we only show three water molecules in Figure 3(b). Two water molecules added to 1 allow tight H bonds with two amide

HSO4

I

-

-

-

Br

-

Cl

F

3+

3+

Er

3+

Nd

3+

Al

In

Fe

2+

3+

Fe

2+

2+

2+

Pb

Cd

Co

2+

2+

Hg

Cu

2+

2+

Mg

Ca

Zn

+

2+

2+

Ba

+

Rb

Ag

+

K

+

+

Na

20

Li

Figure 4. HOMO and LUMO for free 1 in vacuo computed at the TDDFT/B3LYP/3-21G level.

Fluorescence difference (a.u.)

-

-

40

CH3COO

(a)

0 -20 -40 -60 -80 -100 -120 -140

Figure 6. Fluorescence intensity changes of 1 in the presence of various metal ions in 80 % aqueous acetonitrile solution (CH3CN/H2O = 1:4, v/v, λexc=343 nm) at pH 6.1.

Tetrahedron

4

The titration fluorescence spectra (λ ex=343 nm) of 1 (2.5 µM) at pH 6.1 in the presence of various concentrations of Fe3+ are shown in Figure 7. The fluorescence intensity (λ em =372 nm) of 1 is continuously decreased upon addition of Fe3+ without any wavelength change. According to the excimer band change, we could obtain the association constants of 1 (Ka=2.5×104 M-1) for Fe3+ ion.

4. Experimental Section 4.1. Synthesis Compounds 1 and 2 were prepared following literature procedures.20

Fluorescence Intensity (a.u.)

4.2. General Procedure for Fluorescence Studies

200

Fluorescence spectra were recorded with a RF-5301PC spectrofluorophotometer. Stock solutions (1.00 mM) of metal perchlorate salts were prepared in CH3CN. Stock solutions of free 1 (0.050 mM) were prepared in different ratios of CH3CN and water. Excitations were carried out at 343 nm with all excitation slit widths at 3 nm and emission slit widths at 1.5 nm. Titration experiments were performed with 2.5 μM solutions of 1in CH3CN/H2O = 80:20 and various concentrations of metal perchlorates in CH3CN. From the calculated concentrations of the free ligands and complexed forms of 1in the fluorescence titration experiments, association constants were obtained with the computer program ENZFITTER.27

3+

Fe equiv 0 eq

150 100 eq

100

50

0 350

400

450

500

550

600

Wavelength (nm)

4.3. Computational Method

The quenching phenomenon of 1 upon Fe3+ ion binding is attributable to the reverse-PET mechanism. When the Fe3+ ion strongly interacts with the lone pair electrons of the amide oxygen atoms (Fe3+ ·····O=C), then the eT occurs from the excited pyrene moiety behaving as a PET donor to electron deficient Fe3+.26 For complexation ratio between ligand and Fe3+ ion, we carried out Job’s plot experiment by varying concentration of both 1 and Fe3+ ion and found a typical 1:1 (ligand:metal) complexation.

Geometry optimizations, vibrational analysis, and molecular orbital calculations were done using Gaussian 03 package.28 The geometry optimizations for 1 in vacuo and 1 with explicit water molecules were performed by density functional theory (DFT) with hybrid functional B3LYP and 3-21G basis set. Different starting geometries have been used for optimization to obtain the global minimum structure for each system. Vibrational frequency analyses were performed to verify the identity of each stationary point as a minimum. The electronic vertical excitation energy and the oscillator strength of the fluorescent spectra of 1 in vacuo and in explicit water molecules were determined by time dependent density functional theory (TDDFT) using the same functional and basis set.

3. Conclusions

Acknowledgments

A fluorogenic calix[4]arene 1 with two facing amide groups linked to pyrene units exhibits exclusively monomer emission due to the intramolecular H-bonding between phenolic OH groups and the amide hydrogen atoms, which disturbs the two pyrene units to have a preferential HOMOLUMO interaction. Addition of H2O to the CH3CN solution gave monomer emission declined and excimer emission enhanced because the water molecule interrupts the Hbonding between the phenolic OH groups and the amide groups. Interestingly, when Fe3+ was added to a solution of 1 (80 % water), the fluorescence emission was selectively quenched. The DFT calculation supports the effect of water addition to the solution of 1 to the fluorescence spectral change that lacking intramolecular H bonds between NH and OH by inserting water molecules contribute to the favorable geometry for Py-Py* interactions between two pyrenes that results observed strong excimer band.

This work was supported by the SRC Research center for Women’s Diseases of Sookmyung Women’s University.

Figure 7. Fluorescence spectra of 1 (2.5 μM) upon addition of Fe3+ ions in 80% aqueous acetonitrile solution (CH3CN/H2O = 4:1, v/v, λexc=343 nm) at pH 6.1.

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6. 7. 8. 9. 10. 11. 12. 13.

14.

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19. Guo, X.; Zhang, D.; Wang, T.; Zhu, D. Chem. Commun. 2003, 914. 20. Kim, J. M.; Min, S. J.; Lee, S. W.; Bok, J. H.; Kim, J. S. Chem. Commun. 2005, 3427. 21. Broan, C. J. Chem. Commun. 1996, 699. 22. Stratmann, R. E.; Scuseria, G. E.; Frish, M. J. J. Chem. Phys. 1998, 109, 8218. 23. Becke, A. D. J. Chem. Phys. 1993, 98, 5648. 24. (a) Gross, E. K. U.; Kohn, W. Adv. Quantum Chem. 1990, 21, 255; (b) Casida, M. E. In Recent Advances in Density Functional Methods, Part I; Chong, D. P., Ed.; World Scientific: Singapore, 1995; p 155; (c) Bauernschmitt, R.; Ahlrichs, R. Chem. Phys. Lett. 1996, 256, 454. 25. Wilberg, K. B.; Stratmannm R. E.; Frisch, M. J. Chem. Phys. Lett. 1998, 297, 60. Bruel, R.; Amos, R. D.; Handy, N. C. Chem. Phys. Lett. 2000, 330, 152. 26. Xiaoping Li, Victoria L. McGuffin Anal. Chim. Acta. 2004, 526, 155. 27. (a) Association constants were obtained with the computer program: ENZFITTER; Elsevier-BIOSOFT: Cambridge, U.K. (b) Connors, K. A. Binding Constants; Wiley: New York, 1987. 28. Gaussian 03, revision D.02: Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.; Cheeseman, J. R.; Montgomery, J. A., Jr.; Vreven, T.; Kudin, K.; Burant, J. C.; Millam, J. M.; Iyengay, S. S.; Tomasi, J.; Barone, V.; Mennucci, B.; Cossi, M.; Scalmani, G.; Rega, N.; Petersson, G. A.; Nakatsuji, H.; Hada, M.; Ehara, M.; Toyota, K.; Fukuda, R.; Hasegawa, J.; Ishida, M.; Nakajima, T.; Honda, Y.; Kitao, O.; Nakai, H.; Klene, M.; Li, X.; Knox, J. E.; Hratchian, H. P.; Cross, J. B.; Adamo, C.; Jaramillo, J.; Comperts, R.; Startmann, R. E.; Yazyev, O.; Austin, A. J.; Cammi, R.; Pomelli, C.; Ochterski, J. W.; Ayala, P. Y.; Morokuma, K.; Voth, G. A.; Salvador, P.; Dannenbuerg, J. J.; Zakrzewski, V. G.; Dapprich, S.; Daniels, A. D.; Strain, M. C.; Farkas, O.; Malick, D. K.; Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Ortiz, J. V.; Cui, Q.; Baboul, A. G.; Clifford, S.; Cioslowski, J.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.; Komaromi, I.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.; Peng, C. Y.; Nanayakkara, A.; Challacombe, M.; Gill, P. M. W.; Johnson, B.; Chem, W.; Wong, M. W., Gonzalez, C.; Pople, J. A. Gaussian, Inc.: Wallingford CT, 2004.

Graphical Abstract

emissions are selectively quenched because of the electron transfer (eT) from the pyrene units to ... between H atom of pyrenyl amide group and O atom of the.

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