42
R. Wawrzinek, P. Wessig / Dyes and Pigments 123 (2015) 39e43
Table 1
Spectroscopic properties of 1, 2, 7 and calculated FRET parameters of 1.
[M 1 cm
ꢀ
ꢀ1
]
R
0
[nm]
E
Compound
labs [nm]
lem [nm]
F
F
t
F
[ns]
3
1
2
7
307, 403
403
307
495
495
378
0.74a (0.62)
0.56
0.99
1.54b (15.40)
15.40
1.66
e
2.9
0.88
[3]
4680 (403 nm)
35700 (301 nm)
a
Value includes donor and acceptor emissions. In brackets: only acceptor emission.
Excitation at 254 nm, detection at 353 nm. In brackets: detection at 495 nm.
b
ꢀR
ꢁ
To further characterise the system we determined the fluores-
6
k
T
ðrÞ ¼ 1
(3)
0
cence quantum yield at different excitation wavelengths and its
fluorescence lifetime. The F o€ rster distance R
(e.g. the distance
t
r
D
0
between donor and acceptor in which the FRET efficiency is 0.5)
was derived from the spectral overlap integral J using the nor-
malised spectra of the donor's emission and the acceptor's molar
extinction coefficient plotted against the fourth power of the
wavelength (inset Fig. 2) and used in Eq. (1) [8].
3
. Conclusion
In this work we presented a new pair of FRET active fluo-
rophores containing two small molecules; PPO as an UV absorbing
donor and a green emitting ester-DBD dye acting as an acceptor.
Using mild reaction conditions and peptide coupling techniques
gave an easily accessible proof-of-concept molecule which than
was spectroscopically investigated. Irradiated with light at the
donor's excitation wavelength of 307 nm this molecule emitted
acceptor fluorescence at 495 nm with a pseudo Stokes shift close to
∞
Z
2
9
$F $k
D
5
6
4
R ¼
0
FDðlÞ
3
ðlÞl dl
(1)
A
4
1
28$p $N $n
A
D
0
2
Here
k
is the orientation factor (2/3), n
D
the refractive index of
the used solvent (1.344 for acetonitrile) and
D
F the fluorescence
quantum yield of the donor in absence of an acceptor (0.99). The
integral term represents the mentioned spectral overlap J in which
190 nm and a fluorescence lifetime of 15 ns in acetonitrile. An FRET
efficiency of 0.88 and a F o€ rster distance of 2.90 nm were found. This
new promising FRET pair could be a very useful addition to the DBD
based tool box for microenvironmental probing. We are currently
working on first applications and other FRET systems containing
DBD dyes. Their large Stokes shifts, high fluorescence quantum
yields and long fluorescence lifetimes provide huge advantages
especially in FLT based microscopic and spectroscopic
investigations.
Especially systems where a DBD moiety would function as FRET
donor are of interest because the long FLT of DBD dyes would be
transferred to the acceptor allowing for time gated temporal
discrimination of background emission at a more red-shifted range
of the visual spectrum.
F
D
(
l
) is the donor's normalised fluorescence intensity and
acceptor's molar extinction coefficient. R was determined to be
.90 nm.
The fluorescence quantum yield (
A
3 (l) the
0
2
F
F ) of 1 revealed a remarkable
high value of 0.74 which, however, needed to be corrected as there
was little donor emission detected. Measurements using excitation
at 403 nm gave the fluorescence quantum yield
A
F exclusively
caused by the acceptor (0.62). This value was then subtracted from
the initial measurement to obtain
in presence of the acceptor (0.12).
FDA, the donor's quantum yield
Because this system shows no ‘crosstalk’ (the simultaneous
excitation of donor and acceptor) and F (the donor’s quantum
D
yield in absence of an acceptor) is 0.99, we used Eq. 2 to calculate a
FRET efficiency E of 0.88.
4. Experimental
F
DA
E ¼ 1 ꢀ
(2)
4.1. Spectroscopy
F
D
We have chosen the fluorescence quantum yield to determine E
rather than the often used fluorescence lifetime of the donor. The
reason for that is the marginal influence of the acceptor on the
already short lifetime of the donor (see Table 1), which causes
larger errors due to a poor signal-noise ratio. Furthermore, it would
be only legitimate to use lifetime measurements for a fixed distance
between donor and acceptor and a monoexponential decay which
is not complied by compound 1 due to its flexible linker.
UVevis measurements were performed with a JASCO V-630
spectrophotometer and analysed with Spectra Manager 2 (v
2.08.01). For all measurements square quartz cells (1 ꢁ 1 cm) were
used.
Steady-state fluorescence spectra were measured with a Horiba
Jobin Yvon Fluoromax 4 and analysed with FluorEssence (v 2.5.2.0).
Fluorescence lifetime spectroscopy was performed on a Horiba
Jobin Yvon Single Photon Counting Controller (TCSPC) Fluorohub
with various LASER-diodes (NanoLED-254/372/447) used in com-
bination with the mentioned spectrometer and the Datastation (v
2.5) software. To analyse the spectra DAS6 (v 6.4) was used. Fluo-
rescence quantum yields were measured with a Hamamatsu Pho-
tonic Multi-Channel Analyzer C10027.
At this point it is important to note that an efficiency of
greater than 0.99 was expected because the distance between
the fluorophores' centres could be maximal 1.3 nm (found by
computational modelling). This means the in Eq. (1) used
2
assumption of
[
k
¼ 2/3 for that particular molecule 1 is not correct
14]. However, it is legitimate to determine R
0
to generally
describe a donoreacceptor system under the assumption of fully
randomised orientation [15]. Furthermore, compound 1 falls into
the category of FRET systems in which donor and acceptor
are considered to be “too close” to each other (r > 2 nm) causing
deviation from the ideal dipole approximation (IDA) [16]. As
a consequence it is not valid for that particular system 1 to
calculate parameters based on Eq. (1) such as the transition rate
4.2. Syntheses
4.2.1. Diethyl 2-(2-oxo-2-((4-(5-phenyloxazole-2-yl)benzyl)amino)
ethyl)benzo-[1,2-d:4,5-d ]bis([1,3]dioxol)4,8-dicarboxylate (1)
Acid chloride 3 (53 mg, 0.136 mmol) was dissolved in 10 mL dry
dichloromethane and cooled down to 0 C. Amine 7 (68 mg,
0
ꢂ
0.271 mmol) and N,N-diisopropylethylamine (23
mL, 0.136 mmol)
T
k (r) (Eq. (3)).
were added and the mixture was stirred over night at room