Chapter 13
Electronic Spectroscopy of Squaraine Its Relationship with the Stabilization Mechanism of Squaraine Particles in Polymer Solutions Kock-Yee Law Downloaded by UNIV OF ARIZONA on November 29, 2012 | http://pubs.acs.org Publication Date: November 30, 1987 | doi: 10.1021/bk-1987-0358.ch013
Xerox Corporation, Webster Research Center, Webster, NY 14580
The fluorescence emission of bis(4dimethylaminophenyl)squaraine, 1, in CH Cl containing varying concentration of poly(vinyl formal) (PVF) has been studied. Three emission bands ( α , β and γ in the order of decreasing energy) are observed 2
in
2
CH Cl 2
solution and are
2
found to
be
the
emission from the excited state of 1, from the excited state of a solute-solvent complex and from a relaxed twisted excited state of the solute-solvent complex, respectively. Model compound studies show that squaraine forms strong solute-solvent complexes with alcoholic solvent molecules. Analogous complexation process between 1 and the OH groups in PVF is also shown to occur. A model for the stabilization of particles of 1 in polymer solution is put forward where we propose that the s t a b i l i z a t i o n mechanism is a steric effect achieved by adsorption of PVF macromolecules onto particles of 1 via the formation of the PVF:1 complex. Bis(4-dimethylaminophenyl)squaraine, of
its
derivatives
photoconductive Although optical 670
class
absorption
nm,
solid
and
this €
m a
state
in
x~3x105 is
are
known
1 to
(J_),
semi-conductive of
compounds
the red i n cm-lM-1),
intense
and
properties. sharp
(X ax ~ 6 2 0 m
absorption
panchromatic
many
useful
exhibits
solution its
and
possess
in
from
0097-6156/87/0358-0148506.00/0 © 1987 American Chemical Society
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
the the
13. L A W
Electronic Spectroscopy of Squaraine
visible
to
the
near-IR
characteristics xerographic
by
casting
various
appropriate in
quality squaraine the
(2)
the
the
dispersity but
also
S c i . ,
1
generally
was
in
and
superior
dispersing
because
poly(vinyl
on
1
Here property effect
studies, is
solution, the
Further
the
emission solvent
hydroxy
is
twisted strong
on
formal). process
particles
1 in
of
the
polymer
various K.Y.
poly
The acetal)
principle for
the
1. multiple
structure-
and
temperature
that
of
the
free
multiple
squaraine
solute-solvent relaxed
using
2
excited
as
a
is
complex-
1
and
the
chains
role
stabilization
shows
complexes
Analogous
important
state.
model
between
in
complex
solute-solvent
solution
of
(vinyl
From
effect show
J .
used.
on
2.
on
particles
macromolecular
The on
of
solvents
detected
the
in
poly(vinyl
molecules.
also
complexation
the
study
solvent
groups
poly(vinyl
of
a
forms
process
to
1
solubility
and
emission
effect
alcoholic
ation
able
the of
1
the
device.
(Law,
results
solvent
emission
squaraine
with
of
we a r e
from
of
when
poor
film
in
influence
were
general are
the
resulting
these
preliminary
relationships,
emission
that
against
emission
profound
butyral) of
technological
particles
studied
onto
squaraine
of
except
effect
solvents
we r e p o r t
fluorescence
and
is
ethereal
of
Flocculation
observed
of
affects
particles
been
press).
formal) polymers
of
has
squaraine
dispersions
thus
the
cell
fabricated
only
has
of
stability
solutions
Imaging
is
not
for
solar
generally
stability
solution
photoconductivity
polymer
organic
are
The
it
optical
attractive
applications,
devices
because
layer,
Recently,
and
these
These
very
squaraine-polymer
polymer
and
nm).
them
substrates.
significance
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In
(3).
photoconductive
particles
(400-1000 made
photoreceptor
applications based
have
149
of
of this
mechanism
of
discussed.
Experimental Squaraines and
1 and
described
by PVF,
hydroxy
content
Polymer
Products
Fisher
molecular
formal
and
sieves
synthesized
derivatives
Sprenger
formal),
from
were
2
Ν,Ν-dialkylaniline
and
Ziegenbein
content
6%,
was
Inc. were before
from
using
82%,
(4).
acetate
purchased
Solvents
acid
procedure Poly(vinyl
content
from
were
routinely use.
squaric the
12%,
Scientific
spectro
stored
Fluorescence
grade
over
3A
spectra
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
PHOTOPHYSICS OF POLYMERS
150 were
t a k e n
on
a
spectrofluorimeter differential Results
corrected
And
Figure
shows
was
Downloaded by UNIV OF ARIZONA on November 29, 2012 | http://pubs.acs.org Publication Date: November 30, 1987 | doi: 10.1021/bk-1987-0358.ch013
spectrum. are
(b)
state
any
some
effects as
a
its
model
Results
in
Figure
bathochromic this
is
composition Figure the
2).
For
emission
with
identical
641 of
to
the and
result
and
in
emission
Figure
emission
XF
698
nm
emission according
to
structures, the the
(0,0)
also are
their
multiple
the
splitting
a
seen
in
assigned Stokes
α-band (0,1)
between
Figure the
shifts. due
and
the
transitions a-
and
a
3a βIf
to
of
the
between
the
α-band
is
state
of
and and
these the
two that
vibrational
would
β-band
2. at
y-band
be
respectively. the
an
band
assumes
fine
j3-band
spectral
small
one
is is
the
the and
α-band and
Because
excited
nm
to
the
in 3a),
spectrum
wavelength
that
the
(Figure
spectrum,
is
the
in
by
a
increases inset
relationship
660
XF
undergoes
(see
ether
of
solvents.
change
spectrum.
suggests
chosen
because
π*
dominated
image
multiple
was
2
excitation
monitoring
emission
and
is
The
at
the 2
of
spectra
Franck-Condon
shoulder are
Xmax
emission
3a
the
bands
2
on
organic
diethyl
absorption the
from
An
of
mirror
In the
with
in
nm. the
overlap
absorption
the
example,
(c)
excited
complex.
parameter
emission
spectrum
at
λγ
independent good
the
or
an
p o s s i b i l i t i e s ,
various
accompanied
of
of
emission
state or
investigation
that
the any
emission
excited
solvent)
solvent
that from
the
Squaraine
our
are
1.
of
temperature
show
as
than of
—702
y-band
showed
multiple
these
in
2
shift
the
solute-solvent
for
solubility
and
states
studied.
compound
they
the
(with
and
were
and
relaxed
of
solvent
bands
high
and
kind
660 and
structure
differentiate
of
emission
a
monitoring absorption
X F 646,
rather
1
for
exciplex
the the
experiments
fine
from
of
and
excitation
spectrum β-
aggregational
an
The
to
at
the
explanations
from
to
bands
from
vibronic
of
order
is
emission
emission
a
excitation
CH2CI2.
emission
Controlled
or
(a)
band;
44A
with
(DCSU-2).
independent
α-,
emission
Probable are
the
the
respectively.
1
unit
identical
emission in
as
impurities
be
was
Three
designated
in
1
to
and
observed
multiple
MPF
equipped
fluorescence
of
found
wavelengths nm
spectra
the
spectra
spectrum
was
Discussions
1
emission
P e r k i n - E l m e r
which
in
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
from From Figure
151
Electronic Spectroscopy of Squaraine
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13. LAW
Figure emission
1.
Corrected
spectra
of
fluorescence
1 i n methylene
excitation
chloride
and
([1]—3x10-7
M).
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
PHOTOPHYSICS OF POLYMERS
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152
Figure emission (b)
3·
Corrected
spectra
a t 77°K
(cone.
of
2
fluorescence in
diethyl
- 5 x 1 0 -7 M ) .
excitation
ether
(a)
at
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
and 298°K
13. LAW 3a,
the
(0,2)
γ-band
3a,
emission the
the
effect
taken
of
solvent
on
(Ham e f f e c t )
relative
emission
in
of
intensity
structure
of
be
vibrational the
in
(0,2)
Major observed
in
found
depart
in
to
2
to
around
nature,
in
the
nm
secondary
alcohols In
accompanying and
identical
significance
to
that
the
and
(rather
emission
between
dimethylaminobenzonitrile reported long to
by
Wang
wavelength the
spectra
interactions also
short
solvent that
sensitive
in
effect
steric
in
α-band
short of
assigned
the
sensitive, and
observed
suggests
alkyl in
that
solvent 2
forms
of
be
the
soluteSince
published)
squaraines around
the
molecules
solvents. to
pwas
DMABN
(Law, K . Y . ,
both
amines
between
that
the
of
state
he
work
The in
similar
steric
dependence
the
alcohols 2.
is
factors
amyl shift,
lies
where
emissions
in
the
and a l k y l
alcoholic
studies
is
nm
between
2
Very
We p r o p o s e in
the multiple to
this
Xmax
dependence)
2 and a l c o h o l i c
range.
complexes
structural show
between
steric
for
excited
which
emission
The s i m i l a r
electronic
recently
Xmax
tertiary
Figure
π*
(DMABN)
emission,
exciplex
amines.
is
(U))
e.g.
of
is
hindrance
—639.4
alcohols
the
2
relationship
Instead,
in
in
than
effects of
steric
spectra in
structure
hypsochromic
composition.
interactions
π*
correlation
seen
results
spectra
Xmax
intensity
The
emission
dependence
range
in
4).
nm
the well
absence
solvent
versus
the
as
best.
increases,
with
the
may
emission
alcohols,
the
of
y-band
The
—634.1
increase
(Figure
absorption
Xmax
and
conjunction
observed
steric
group
in
persistent
the
on
variation
vibronic
as
of
solvent
vary
at
in the
structure
solvents.
primary
alcohol. is
Xmax
wavelengths
in
an
the
affect
are
The
specific
alcoholic
hydroxy
642.6±0.2
is
the
to
of
the
50
solvents.
from
shorter
the
tentative, the
to
structure
and
over
against
fails
bands
fine
solvent
but in
from
known
(6-9).
the
in the
corresponding
effect
fine
the βand
alcoholic
Figure
the
pyrene
transition
comes
the
nm
a l l
examples
absorption
of
of
vibrational
and
α - ,
evidence
are
The
—675
laboratory
the
an assignment
assignment
shifts
of
of
be
shoulder
(5)
squaraine
of
such
the
our or
Notable
intensity
fluorescence
transition. to
inspection
Solvents
intensity
hydrocarbons.
benzene
makes
in band
transition.
relative
(0,3)
expected
Careful
emission
(0,2)
the
is
missing.
any
aromatic
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is
be
which
spectra
identify
the
would
transition
Figure
to
153
Electronic Spectroscopy of Squaraine
are
the
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
not
N,N-
154
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PHOTOPHYSICS OF POLYMERS
Figure
4.
Corrected
i n amyl a l c o h o l s
fluorescence
emission
spectra
([1]—3X10~7M) .
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
of 2
13. LAW
Electronic Spectroscopy of Squaraine
155
DIALKYLAMINO GROUP, OUR RESULTS SUGGEST THAT THE SITES OF COMPLEXATION IN ALCOHOLS ARE THE OH GROUP OF THE ALCOHOL AND THE FOUR-MEMBERED RING OF THE SQUARAINE (SCHEME I ) . Scheme
I
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Η
AS THE STERIC HINDRANCE AROUND THE OH GROUP DECREASES, SOLUTE-SOLVENT COMPLEXATION INCREASES, RESULTING IN THE BATHOCHROMIC SHIFT OF XMAX AND AN INCREASE IN /3EMISSION INTENSITY. THE GENERAL SOLVENT EFFECT ON THE XMAX AND THE EMISSION COMPOSITION OF 2 (FIGURE 2) SUGGESTS THAT THE COMPLEXATION PROCESS IS VERY GENERAL AND COMPLEXATION BECOMES VERY PRONOUNCED IN SOLVENTS OF Π* > 0 . 6 5 . ACCORDINGLY, Α-BAND IS THE FRANCKCONDON EMISSION OF THE EXCITED STATE OF THE SOLUTE AND J3-BAND IS THE FRANCK-CONDON EMISSION OF THE EXCITED STATE OF THE SOLUTE-SOLVENT COMPLEX. ADDITIONAL EXPERIMENTAL EVIDENCE IN FAVOR OF THE SOLUTE-SOLVENT COMPLEX MODEL COMES FROM THE LOW TEMPERATURE ELECTRONIC SPECTRA OF 2 IN ETHER. SQUARAINE 2 EXHIBITS AN ABSORPTION AT XMAX 654 NM AND A SINGLE EMISSION AT X F 664 NM AT 77°K IN ETHEREAL MATRIX (FIGURE 3 B ) . THE OBSERVATION OF A BATHOCHROMIC SHIFT IN THE EMISSION SPECTRUM IS CERTAINLY AGAINST GENERAL EXPECTATION FROM VIBRATIONAL FINE STRUCTURES WHERE A HYPSOCHROMIC SHIFT OF X F SHOULD BE OBTAINED (JUL). THE ANOMALOUSLY LARGE SHIFT LEAD US TO CONCLUDE THAT THE ABSORPTION IS FROM THE SOLUTE-SOLVENT COMPLEX AND THAT ITS FORMATION IS PROBABLY A TEMPERATURE STABILIZATION EFFECT. SINCE THE EXCITATION SPECTRUM AT 77°K IS IDENTICAL TO THE ABSORPTION SPECTRUM AND SHOWS GOOD OVERLAP AND MIRROR IMAGE RELATIONSHIP WITH THE EMISSION SPECTRUM, THE SINGLE EMISSION AT XMAX 664
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
156 nm
PHOTOPHYSICS OF POLYMERS can
the
be
study
of
towards in of
assigned 2
ether, the
that is
solute.
from
Another emission
Since the
of
suggest
of
four
membered
the
C-C
the
y-emission
in
previous
results,
rotation
is
the
both
however,
complexing Addition
known
to
ternary
(e=4.7) hexane
in
red
as
of
and
isoemissive spectral
results is
of
is
at
we
bond
nm
positive
not
In
our
€
and
only the
is
also
order
chloroform
addition
of
n-
constant
as
the
Results shift
XF
at
the M.
the
a and
experiment
ether
The
point
red
that
process.
Xmax
the
an
the As
increases
performed
that
from
in
j3-
solvent
the
fact
medium,
keep
the
increase to
also
ether
to
—662
give
indeed
of our
C-C
and
polar
the
isosbestic
point
a and
with
complex.
Such
solvent
chloroform
an
a-
the
(e=1.9).
show
ring
complexing
shift
more
increases
[CHCI3]
Simultaneously,
emission
b
a
by
absence
the
should
by
namely
mixture
concentration 5a
2
complexation
n-hexane
the
a
but
dilemma,
system,
and
Figures
the
this
the
of
increase.
complexing
affect
phenyl The
of
should
XF
(e)
from
formed
complementary
of
are
constant
circumvent a
a
of
published)
is
that
of
quantum
emission
the
at
effects
77°K.
complexation,
dielectric
is
temperature
be
solute-solvent
solvents
the that
emission
squaraine.
addition
should
of
with
the
an
indicating
and
an ot-
y-emission
which
between
complicated
of
induces
in
Xmax
can
is
The
low
to
simply
the
β-emission
is,
is
state
solution
of
we
fluorescence
K.Y.
assignment
ethereal
result,
total
at
b,
state
the on
3b
correct,
concentration
the of
Figure
above
was
and
fluorescence (Law,
prohibited
the
in
results
of
nm
comparison
temperature
excited
absence
bond
— 660
by
study.
the
ring
insensitive λγ(β)
identical
y-emission
the
of
effect
complex.
the is
excited
rotation
an
on
the
twisted
If
the
multiple
that
3a
room
finding
squaraines
relaxed,
emission
from
recent
changes
number
at
effect
is
structural
(e.g.
Figures
deduction
yield
relatively
solute-solvent
solvent
emission
solvent
acetonitrile),
in
emission
spectrum
and
is
polarity
in
significant
nm.
Since
/^-emission
This
obtained
nm
the
an
Franck-Condon
XF
data
the
from
emission
—700
that
solvent
XF(J3)=665
emission
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shows
spectral
the
complex.
increasing
conclude
in
to
solute-solvent
that state
an
These the of
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
J8the
13. LAW
157
Electronic Spectroscopy of Squaraine
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(a)
600
Figure (a)
5.
Effect
absorption
spectra 0.28
M,
4.48
M).
of
2
i i i .
of
650 700 X(nm) chloroform
([2]—10-5
([2]~3x10-7 0.56
M,
M) M)
iv.
(b) in
750
concentration corrected
ether
1.12
M,
([CHCl3] = i v.
2.24
on
the
fluorescence M,
0 M, and
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
i i . v i .
PHOTOPHYSICS OF POLYMERS
158 solute-solvent excited complex
is
of
in
emission
2
to
the
(Ιβ)
Complexation
and
versus
however,
of
the
emission.
and β
further
bathochromic
increase
Absorption through
curves
their
observation solvation as
the
of of
shell
As acetal) in
the
polymers
are
organic
these found
to
have
no
experiments. are
the
latter
is
complexes model
shown with
the
studied. that
the
of
In
typical
a
PVF
effective exists
are
as
of
1
in
interaction
between squaraine
of
macromolecules of
1
and
groups
the for
representation
PVF
and
CH2CI2
with
the of
occurs in
onto
groups
in
the PVF
adsorption the
on
of
the to
majority the
the
OH
CH2CL2«
Due
the of
1
major
surfaces
solution.
As
p r o c e s s ,
a
PVF
of
particles
actually
anchoring
process.
adsorption
the
the
in
that
surfaces are
as
that 1
show
dispersion, Μ),
a is
6a-d
increases
implies
c o m p l e x a t i o n
adsorb OH
PVF
as
CH2CI2
—10-2 M .
particles
the
strong PVF
Figures
(:2.24
curves
events
as
overlapping
Xmax
at
concentration
of
in
the
isoemissive
complexation
noted
chloroform close
on
M the
Figure
and
attributed
two
the
of
of
solute-solvent
these
the
of
the
chloroform
1:n
localized
solvation
or
be
of
inset
observed
solute-solvent
a
of
highly
2 to
emission
either
the
solute-solvent
1
and
from
[CHCL3]J_2) ·
pigment
the
acid
of
of
organic
using
carboxylic
stabilizes
resulting
dispersion
stabilization
interactions
able
sterically
solution,
of
these
polymers
anchoring
effect
process,
which
p a r t i c l e s experiments
functional
in also
groups,
In Photophysics of Polymers; Hoyle, C., et al.; ACS Symposium Series; American Chemical Society: Washington, DC, 1987.
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13. L A W
Electronic Spectroscopy of Squaraine
161
e.g., cyano g r o u p , c a n a l s o be u s e d a s an a n c h o r i n g group f o r t h e p o l y m e r i n t h e a d s o r p t i o n p r o c e s s and s t a b l e d i s p e r s i o n s c a n be p r e p a r e d a c c o r d i n g l y . For example, b e t t e r d i s p e r s i o n s t a b i l i t y i s o b t a i n e d from s t y r e n e - a c r y l o n i t r i l e c o p o l y m e r i n C H 2 C I 2 a s compared to p o l y s t y r e n e itself. In summary, the s t a b i l i z a t i o n mechanism of squaraine particles in organic solvents h a s been understood as a steric stabilization process by spectroscopic technique. The knowledge g a i n e d i n t h i s work has enabled us t o formulate other stable squaraine-polymer dispersions using polymers other than p o l y ( v i n y l a c e t a l s ) .
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