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the amide does not bear a sterically demanding substituent
(16h), neither the amide nor the 4-alkyl substitution influences
the electronic structure of the ground state (absorption
maxima) or the excited state (fluorescence maxima, quantum
yield).
Table 4. Selected photophysical properties of 3-hydroxyisoquinolines 16.
Compound
lmax,abs [nm][a]
(e [LmolÀ1 cmÀ1])
lmax,em [nm][b]
(Ff [a.u.])
Stokes shift
[c]
(Dn˜) [cmÀ1
]
16a
16c
16d
358.5 (9000)
282.5 (3400)
358.5 (8600)
286.5 (3500)
359.0 (9400)
314.0 (5600)
249.5 (47300)
358.5 (8200)
308.0 (4600)
249.5 (44700)
358.5 (7500)
317.0 (4200)
249.0 (42300)
382.5 (7600)
260.5 (34900)
361.5 (10100)
287.0 (3800)
359.0 (9600)
282.0 (3700)
359.5 (8700)
281.0 (3300)
358.5 (8900)
282.0 (3100)
380.0 (6800)
258.0 (33500)
395.5 (0.87)[d]
396.0 (0.79)[d]
396.0 (0.20)[d]
2600
The second series is represented by 3-hydroxy-1,3-dioxol[4,5-
g]isoquinoline derivatives (16e, 16d, and 16 f), of which all
three derivatives are fluorescent. In the absorption spectra,
three distinct maxima can be found. The highest and lowest
energy transitions are located in the very narrow ranges of
249.0 to 249.5 nm and 358.5 to 359.0 nm, with molar extinc-
tion coefficients (e) of 42300–44700 and 7500–
9400 LmolÀ1 cmÀ1, respectively. However, it is noticeable that
the intermediate absorption maxima appearing between 308.0
and 317.0 nm, with molar extinction coefficients between 4200
and 5600 LmolÀ1 cmÀ1, are clearly affected by the substitution
pattern. This is surprising because the structural variation
occurs at a position that is not in conjugation with the isoqui-
noline chromophore. Hence, it can be concluded that this tran-
sition is sensitive to minute inductive substituent effects. All of
the emission maxima appear at around 395 nm, which indi-
cates that the vibrationally relaxed excited S1 state is unaffect-
ed by the substitution pattern. Also, the quantum yields deter-
mined with anthracene as a relative standard (Ff =0.36) fall
within the range of 0.20 to 0.40, that is, with lower fluores-
cence efficiencies relative to those of the unsubstituted series
(16a, 16c, 16i, 16k, 16j, and 16h).
The third series consists of the trimethoxy-substituted deriv-
atives 16l and 16g, in which methoxy groups as +M and ÀI
substituents exert their effects on the electronic properties.
The donor substitution on the benzo core of the isoquinoline
shifts both the absorption and emission maxima bathochromi-
cally. Two distinct absorption maxima are found. The higher
energy transitions appear at around 260.0 nm with molar ex-
tinction coefficients (e) of 33500 and 34900 LmolÀ1 cmÀ1, re-
spectively, and the longest wavelength maxima are found at
around 381.0 nm with molar extinction coefficients of 6800
and 7600 LmolÀ1 cmÀ1, respectively. The emission maxima
appear at 443.5 and 446.5 nm, respectively. In comparison to
the second series (see above), the fluorescence quantum yields
(Ff) are significantly higher (0.62 and 0.65) and the lumines-
cence appears brighter to the eye (Figure 1).
2600
2600
16e
16 f
394.5 (0.25)[d]
394.5 (0.38)[d]
2600
2600
16g
16h
16i
446.5 (0.65)[e]
401.0 (<0.01)[d]
399.5 (0.79)[d]
397.0 (0.90)[d]
395.5 (0.84)[d]
443.5 (0.62)[e]
3800
2700
2800
2600
2600
3800
16j
16k
16l
[a] Recorded in CH2Cl2 at RT. [b] Recorded in CH2Cl2 at RT with lexcitation
=
350.0 nm. [c] Dn˜ =1/lmax,absÀ1/lmax,em
.
[d] Quantum yields were deter-
mined with anthracene as a standard in cyclohexane (Ff =0.36).[40,41]
[e] Quantum yields were determined with 9,10-diphenylanthracene as
a standard in cyclohexane (Ff =1.00).[40,42]
be distinguished: unsubstituted (16a, 16c, 16i, 16k, 16j, and
16h), dioxolannelated (16e, 16d, and 16 f), and 5,6,7-trime-
thoxy-substituted (16l and 16g) derivatives. With the excep-
tion of the 5,6,7-trimethoxy-substituted derivatives 16l and
16g, the Stokes shifts (Dn˜; that is, 1/lmax,absÀ1/lmax,em) lie at
around 2600–2800 cmÀ1 for all of the other 3-hydroxyisoquino-
lines 16, whereas derivatives 16l and 16g display considerably
larger Stokes shifts of 3800 cmÀ1. In comparison to the parent
system, 3-hydroxyisoquinoline, derivatives 16 are unlikely to
undergo hydrogen-bond-assisted dimerizations. Moreover, the
1-amide functionality offers an intramolecular hydrogen-bond
donor for the isoquinoline nitrogen atom to stabilize the mo-
nomer structure. Obviously, this intramolecular hydrogen
bonding is hampered by the steric demand of the 2,6-dime-
thylphenyl amide substituent in compound 16h, which causes
a radiationless deactivation of the excited state (see below).
The spectra of the series of unsubstituted derivatives, that is,
16a, 16c, 16h, 16i, 16j, and 16k, display two distinct absorp-
tion maxima. The first shorter wavelength band with weaker
intensity (e values ranging from 3100 to 3800 LmolÀ1 cmÀ1) ap-
pears between 281.0 and 287.0 nm and the intense longest
wavelength maximum is found at around 360.0 nm (e values
ranging 8600 to 10100 LmolÀ1 cmÀ1). With exception of 16h,
all of the compounds of this series are strongly luminescent
and the quantum yields determined with anthracene as a rela-
tive standard (Ff =0.36) fall in the range of 0.79 to 0.90. Unless
For scrutinizing the solvent effects on the photophysical
properties of the 3-hydroxyisoquinolines, derivative 16k was
considered to be an appropriate model and the absorption
and emission maxima, molar extinction coefficients (e), Stokes
shift (Dn˜), and fluorescence quantum yield (Ff) were deter-
mined in dichloromethane, acetonitrile, and DMSO (Table 5).
The absorption properties are only slightly affected upon
variation of the solvent polarity. With increasing polarity, a very
modest bathochromic shift of the longest wavelength maxi-
mum can be observed (358.5 nm for CH2Cl2 and acetonitrile
and 361.0 nm for DMSO). It should be noted that, in DMSO,
the second maximum at 271.5 nm is shifted hypsochromically
(relative to 281.0 nm for acetonitrile) and hyperchromically,
that is, the molar extinction coefficient almost doubles in mag-
nitude, relative to the corresponding bands in the other sol-
&
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Chem. Eur. J. 2014, 20, 1 – 11
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