195
1.00

4700
4500
a
|
1

4300

T

i

Ly

4100
i

+

WAVELENGTH

hal
4.

(A)

oe

at00

4s 4" -D] HEXAHY DROFRANESOXY -P-TEAPHENTL
0.90 |

SOLVENT

ao
o

4 32000

EXCITING WAVELENGTH

3040A

)

s

oa

0027 G/L

.

4 28000 ~~

DECAY TIME 0.95 NSEC
WAVELENGTH (AVE)

Qo

Ww

0.09 MM

WAVELENGTH (CG)

-| 24000

2700 CM!

4 20000

PHOTON INTENSITY

+d

STOKES LOSS

J649A
3677A

16000

s

0.40

0,30 L

EMISSION

ABSORPTION 12000

0.20 |

0.10 L

0.00
21000

L
22000

i
23000

1
24000

7
25000

rn
26000

1
27000

L
28000

1
29000

k
30000

WAVE NUMBER

HaCiso-—{_)—{_)—{(_))—00Hs
31 000)

(CM 3

33000

33000

34000

35000

3e000

+

8000

4

4000

MOLAR EXTINCTION COEFFICIENT

=]

Qa

a
'

T

n
Oo

SLIT WIDTH

T

(ARBITRARY SCALE)

T

CONC.

BENZENE

37000

158.—Compound XIX, 4,4”-dihexahydrofarnesoxy-p-terphenyl, solvent benzene

systems of the similar size. Among the compounds
tested, XI is the longest molecule and, as expected,
has the shortest computed lifetime, 0.8 nsee.
It has been postulated by Suzuki‘® that the larger

readily noted in comparing the data for II with III,

VI with VII, and VII with IX, as shown in Table 67
and Figures 140, 141, and 143-146. If it were not for
steric crowding by the substituents with the hydrogen

mophor in the ground state. In support of this as-

atoms on the basic chromophor in VII, X (Figure
147) and XI (Figure 148), the natural fluorescence

become smaller as the chromophor becomes larger as

IV (Figure 142) can be considered as tetraphenyl-p-

the p-oligophenylene, the more planar is the chro-

sumption, the FWREvalues of the absorption spectra

shown in Table 67 for compoundsII, VI, and VIII.
Alkyl chains substituted in the para and meta posi-

lifetimes would be even shorter than those tabulated.

terphenyl and is an illustration of an extreme case of

steric hindrance. For this latter compound the quan-

tions of terminal rings are effective in increasing the

tum yield is very small, the intense transition that is

planarity of the chromophor or the strength of the
transition. For these reasons, these substituted com-

ward shorter wavelengths, and Stokes loss is very

solubility of the compound and yet do not affect the

pounds possess characteristics very similar to those

of the unsubstituted compounds. On the other hand,
if these same substituents are positioned on the ortho
position of the end rings or on meta or ortho positions

of phenylene rings, the planarity of the basic chromophoris disturbed, and its fluorescence characteristics are affected in the followmg manner: The long

wavelength absorption bond is shifted toward shorter
wavelengths, the value of enax Is reduced, the value

of FWRE of the absorption curve is increased, the
fluorescence spectrum becomes less structured, the
value of Stokes loss is increased, and the quantum
yield is reduced. These effects of steric hindrance are

the hallmark of the p-oligophenylenes is shifted tolarge. Surprisingly FWRE (Fl) is abnormally small.
This result may be explained by the fact that the six
phenyl rings make large angles with the central benzene rings so that there is no effective conjugation
between the rings and the fluorescence characteristics
correspond to a 1L, — 1A transition of the basic

chromophor, the central benzene ring.

The angle between successive phenyl rings can be
held fixed by means of a bridging group as in XII,
XIII, XIV, XV, and XVI, Figures 149-153, respec-

tively. This added planarity is responsible for the
structure in both the absorption and fluorescence

spectra, and their shift toward longer wavelengths, for
the increase in the value of emax, and for the de-

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