Enhanced hydrogen bonding induced by optical excitation: Unexpected subnanosecond photoinduced dynamics in a peptide-based [2]rotaxane [19]

Full text of DOI:10.1021/ja015919c

J. Am. Chem. Soc. 2001, 123, 11327-11328
Enhanced Hydrogen Bonding Induced by Optical
11327
Excitation: Unexpected Subnanosecond
Photoinduced Dynamics in a Peptide-Based
[2]Rotaxane
George W. H. Wurpel,† Albert M. Brouwer,*,†
Ivo H. M. van Stokkum,‡ Angeles Farran,§ and
David A. Leigh*,§
Laboratory of Organic Chemistry
UniVersity of Amsterdam, Nieuwe Achtergracht 129
NL-1018 WS Amsterdam, The Netherlands
Faculty of Sciences, Vrije UniVersiteit, De Boelelaan 1081
NL-1081 HV Amsterdam, The Netherlands
Centre for Supramolecular and Macromolecular Chemistry
Department of Chemistry, UniVersity of Warwick
CoVentry CV4 7AL, UK
Figure 1. Rotaxane 1 and thread 2. The hydrogen bond pattern shown
in 1 corresponds to that found in the X-ray structure of a similar exo-
pyridyl macrocycle containing rotaxane (Supporting Information).
ReceiVed March 30, 2001
Control of the shuttling process in rotaxanes using external
sources has been the subject of considerable recent research.1
Photoinduced motions are particularly interesting because of the
convenient use of this stimulus in possible future device applica-
tions. Up to now, however, translational shuttling in photoactive
rotaxanes has required external reagents or catalysts to occur
(sacrificial reductants, sensitizers etc.), and generally takes place
over relatively long time scales.2 Here we report on the excited-
state dynamics of rotaxane 1, and show that in nonpolar solvents
at room temperature an unexpected photoinduced co-conforma-
tional3 change takes place that requires no external assistance and
occurs on a subnanosecond time scale. It involves a rearrangement
in the pattern of hydrogen bonds between thread and macrocycle
leading to a shift of the latter from the peptide site toward the
anthracene-9-carboxamide stopper which has a greatly enhanced
hydrogen bonding affinity in the excited state.
Figure 2. (A) Fluorescence spectra of rotaxane 1 (continuous) and thread
2 (dotted) in DMSO (note the vertical offset). (B) Fluorescence spectra
of 1 (continuous) and 2 (dotted) in 1,4-dioxane and 2 in 2,2,2-trifluoro-
ethanol (dashed). All spectra have been scaled to the same absorbance at
the excitation wavelength (330 nm).
Rotaxane 1 (Figure 1) consists of a thread containing a glycyl-
glycine recognition motif used to promote rotaxane formation4,5
1
and a bulky anthracene stopper. H NMR studies, supported by
simultaneously binding to both amide carbonyl groups in the
normally preferred manner for peptide rotaxanes.4,5
X-ray crystallography of a close analogue of 1 (both included as
Supporting Information), show that in relatively nonpolar solvents
(e.g. CDCl3, 1,4-dioxane, etc.) 1 principally adopts co-conforma-
tions with the macrocycle surrounding the peptide part of the
thread (Figure 1). It appears that the nonplanarity of the
anthracene-9-carboxamide unit prevents the macrocycle from
Rotaxane 1 was originally intended as an “inactive” model
compound for studies aimed at investigating energy transfer or
electron transfer between the mechanically interlocked compo-
nents of rotaxanes. Since energy transfer or electron transfer from
the excited anthracene to this macrocycle is impossible on
thermodynamic grounds6 one would expect the fluorescence of
1 to be virtually identical with that of the thread 2. As shown in
Figure 2A, this is in fact the case in dimethyl sulfoxide (DMSO),
a solvent in which the hydrogen bonding between the peptide
station and the macrocycle is disrupted and the macrocycle resides
on the alkyl chain of the thread, far from the anthracene unit.4 In
non-hydrogen bond disrupting solvents such as 1,4-dioxane
(Figure 2B), however, the fluorescence of the rotaxane is
considerably broader and more intense than that of the thread.
Since some of the vibrational fine structure of the anthracene
emission is retained, it seems likely that the broad emission band
is composed of two contributions, viz. one that resembles the
thread spectrum and an additional broad red-shifted band.
The fluorescence of anthracene-9-carboxamide has been studied
by Werner and Rogers,7 who observed that the spectrum is
broadened and red-shifted in the strongly hydrogen bond donating
solvent 2,2,2-trifluoroethanol. The thread 2 shows the same effect
† University of Amsterdam. E-mail: fred@org.chem.uva.nl.
‡ Vrije Universiteit.
§ University of Warwick. E-mail: David.Leigh@ed.ac.uk. Current address:
Department of Chemistry, University of Edinburgh, The King’s Buildings,
West Mains Road, Edinburgh EH9 3JJ, UK.
(1) For comprehensive reviews see: (a) Benniston, A. C. Chem. Soc. ReV.
1996, 25, 427. (b) Sauvage, J. P. Acc. Chem. Res. 1998, 31, 611-619. (c)
Balzani, V.; Gomez-Lopez, M.; Stoddart, J. F. Acc. Chem. Res. 1998, 31,
405-414. (d) Balzani, V.; Credi, A.; Raymo, F. M.; Stoddart, J. F. Angew.
Chem., Int. Ed. 2000, 39, 3348-3391.
(2) (a) Murakami, H.; Kawabuchi, A.; Kotoo, K.; Kunitake, M.; Nakashima,
N. J. Am. Chem. Soc. 1997, 119, 7605-7606. (b) Armaroli, N.; Balzani, V.;
Collin, J. P.; Gavin˜a, P.; Sauvage, J. P.; Ventura, B. J. Am. Chem. Soc. 1999,
121, 4397-4408. (c) Ashton, P. R.; Ballardini, R.; Balzani, V.; Credi, A.;
Dress, K. R.; Ishow, E.; Kleverlaan, C. J.; Kocian, O.; Preece, J. A.; Spencer,
N.; Stoddart, J. F.; Venturi, M.; Wenger, S. Chem. Eur. J. 2000, 6, 3558-
3574. (d) Brouwer, A. M.; Frochot, C.; Gatti, F. G.; Leigh, D. A.; Mottier,
L.; Paolucci, F.; Roffia, S.; Wurpel, G. W. H. Science 2001, 291, 2124-
2128.
(3) “Co-conformation” refers to the relative positions of the mechanically
interlocked components with respect to each other, see: Fyfe, M. C. T.; Glink,
P. T.; Menzer, S.; Stoddart, J. F.; White, A. J. P.; Williams, D. J. Angew.
Chem., Int. Ed. Engl. 1997, 36, 2068-2070.
(4) Lane, A. S.; Leigh, D. A.; Murphy, A. J. Am. Chem. Soc. 1997, 119,
11092-11093.
(6) The lowest excited singlet state is located on the anthracene-
carboxamide moiety and has an E00 ) 3.22 eV. Its oxidation potential (1.6 V
vs SCE) is not sufficient to allow reduction of any group in the ring.
(7) Werner, T. C.; Rodgers, J. J. Photochem. 1986, 32, 59-68.
(5) Leigh, D. A.; Murphy, A.; Smart, J. P.; Slawin, A. M. Z. Angew. Chem.,
Int. Ed. Engl. 1997, 36, 728-732.
10.1021/ja015919c CCC: $20.00 © 2001 American Chemical Society
Published on Web 10/20/2001

11328 J. Am. Chem. Soc., Vol. 123, No. 45, 2001
Communications to the Editor
Figure 3. Fluorescence spectra of rotaxane 1 excited at 330 nm: (A)
CH2Cl2 at 307.7, 285.7, 266.7, 250.0, 235.3, 222.2, 210.5, 200.0, 190.5,
181.8 K and (B) glassy sucrose octaacetate at 30 °C (dashed) and molten
at 140 °C (continuous). All spectra were scaled to the same intensity at
24000 cm-1
.
(Figure 2). Werner and Rogers explained their observation by
assuming that in the excited singlet state the conformation changes
from one in which the planes of the amide group and the
anthracene ring are essentially perpendicular to a planar config-
uration, in which a considerable transfer of charge onto the
carbonyl oxygen atom occurs, leading to enhanced hydrogen
bonding.8
Considering that the broad red-shifted contribution to the
spectrum of 1 is not observed in DMSO, where the macrocycle
is displaced from the peptide station to the hydrocarbon tail, we
attribute the occurrence of the long-wavelength shoulder to
emission from a relaxed co-conformation in which the macrocycle
is bound to the anthracene amide. The question remains whether
this is a static or a dynamic effect.
Figure 4. (Left) Fluorescence decay traces of 1 in CH2Cl2 at two
wavelengths, together with their fit. The time axis is linear up to 0.2 ns,
and logarithmic thereafter. (Right) Results from the global and target
analysis, showing the Decay Associated Spectra (DAS) and Species
Associated Spectra (SAS). Key: 36 ps (dotted), 0.26 ns (dashed), 1.82
ns (dot-dashed), 4.33 ns (continuous).
Figure 5. Proposed mechanism for the excited-state dynamics of 1.
If the effect is dynamic, it should be possible to prevent it by
lowering the temperature and by placing the rotaxane in a solid
matrix (Figure 3). Indeed, upon lowering the temperature the long-
wavelength shoulder disappears. In solid sucrose octaacetate at
room temperature, a structured anthracene-like emission is
observed, and only upon melting of the matrix does the long-
wavelength band appear again.
states have been formed which evolve with different decay times
(0.26 and 1.82 ns) to the long-lived, broad, and red-shifted state.
The Species Associated Spectra (SAS) for this model are shown
in Figure 4.
Our results have led to the hypothesis that the emissive states
with anthracene-like character correspond to co-conformations
where the macrocycle is bound to the dipeptide motif. The broad,
strongly red-shifted emission then arises from a co-conformation
where the macrocycle forms hydrogen bonds with the carbonyl
directly attached to the anthracene in a mechanism as shown in
Figure 5.
In conclusion, we have shown that significant macrocycle
motion can be induced in a rotaxane on a short time scale without
the need for any additional external assistance besides photons.
Although in the present system the displacement caused is not
particularly large (approximately 3 Å), the concept of enhanced
hydrogen bonding induced by optical excitation may lead toward
more spectacular translational phenomena in molecular shuttles
designed on this principle.
Finally, time-resolved fluorescence spectroscopy was performed
by using picosecond Single Photon Counting. Decay traces were
recorded at a number of wavelengths and globally analyzed.9
Some of the results obtained in CH2Cl2 are shown in Figure 4.
In accordance with the proposed excited-state relaxation of
anthracene-9-carboxamide, the thread 2 shows a biexponential
decay. The initial perpendicular conformation relaxes in 78 ps to
a more planar conformation, which has a decay time of 3.43 ns
and is slightly red-shifted. For rotaxane 1 such a simple kinetic
scheme is not applicable; for a good fit at least four exponentials
are required. The Decay Associated Spectra (DAS, Figure 4) of
36 ps, 0.26 ns, and 1.82 ns possess negative amplitudes above
450 nm. This shows that the species emitting at long wavelength
(τ ) 4.33 ns) is formed from a number of precursors on time
scales of 36 ps, 0.26 ns, and 1.82 ns. The precursor species have
anthracene-like structured emission at short wavelengths, con-
sistent with the fact that they do not “distort” the chromophore
by hydrogen bonding.
Acknowledgment. This work was supported by the TMR initiative
of the European Union through contract FMRX-CT97-0097 (DRUM),
The Netherlands Organization for Scientific Research (Nederlandse
Organisatie voor Wetenschappelijk Onderzoek, NWO), and the EPSRC.
D.A.L. is an EPSRC Advanced Research Fellow (AF/982324). We thank
Dick Bebelaar for technical assistance with the time-resolved fluorescence
measurements.
If we assume a model with two groups of co-conformations
these fluorescence decays can be understood. The fastest com-
ponent corresponds with the short-lived state in the thread. In
this state, which is formed upon excitation, the various conforma-
tions of 1 are indistinguishable. After 36 ps two spectrally similar
Supporting Information Available: Synthesis and characterization
of 1 and 2 (PDF). This material is available free of charge via the Internet
at http://pubs.acs.org.
(8) Preliminary ab initio calculations (HF/6-31G* for the ground state and
CIS/6-31G* for the S1 state) support this view.
(9) van Stokkum, I. H. M.; Scherer, T.; Brouwer, A. M.; Verhoeven, J. W.
J. Phys. Chem. 1994, 98, 852-866.
JA015919C