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New Chiral-Photochromic Dopant with Variable Helical
Twisting Power and its use in Photosensitive
Cholesteric Materials
Alexey Yu. Bobrovsky a; Natalia I. Boiko a; Valery P. Shibaev ab
Faculty of Chemistry, Moscow State University, Moscow, Russia
Prof. V.P. Shibaev Faculty of Chemistry, Moscow State University, Moscow,
Russia
a
b
Online Publication Date: 01 July 2001
To cite this Article: Bobrovsky, Alexey Yu., Boiko, Natalia I. and Shibaev, Valery P.
(2001) 'New Chiral-Photochromic Dopant with Variable Helical Twisting Power and
its use in Photosensitive Cholesteric Materials', Molecular Crystals and Liquid Crystals, 363:1, 35 - 50
To link to this article: DOI: 10.1080/10587250108025256
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0 2001 OPA (Overseas Publishers Association) N.V.
Published by license under the
Gordon and Breach Science Publishers imprinl.
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Mol Ctyr Ltq. Cvrt.. Vol. 363. pp. 35-50
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New Chiral-Photochromic Dopant
with Variable Helical Twisting Power
and its use in Photosensitive Cholesteric
Materials
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ALEXEY YU. BOBROVSKY, NATALIA I. BOIKO and
VALERY P.SHIBAEV*
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Faculty of Chemisty, Moscow State University, Leninskie goy, Moscow, 119899,
Russia
(Received April 05, 2000; In final form August 28, 2000)
A new photosensitive c h i d dopant based on cinnamic acid and isosorbide was syntbesised. UV light
action leads to E-Z photoisomerization of the dopant about C=C double bond of cinnamoyl fragment.
Mixtures of the dopant with nematic and cholestric polymers were studied. It was shown, that
planarly-oriented films of mixtures possess a selective light reflection in ultraviolet, visible and infrared regions of spectrum depending on the dopant concentration. The helical twisting power of the
chiral dopant was calculated. UV light action on mixture films leads to a shift of selective light reflection peak to the long wavelength region of spectrum, which is explained by photoisomerization and
decrease of the helical twisting power of the dopant. Kinetics of the process of photoinduced untwisting of the cholesteric helix was studied. Advantages of the use of the synthesised dopant and of mixtures based on it were demonstrated in comparison to earlier studied chiral-photochromic materials
for optical data recording and storage.
Keywordst photosensitive c h i d dopant; chiral-photochromic cholesteric materials
INTRODUCTION
Low-molar-mass and polymer cholesteric liquid crystals attract a great attention
of researchers owing to their unique optical properties (selective reflection of circularly polarized light, high optical activity, circular dichroism etc. [ 11). The possibility for regulation of the pitch of the helix and, as a consequence, of selective
* Address for correspondence: Prof. V.P. Shibaev Faculty of Chemistry, Moscow State University,
Leninskie gory, Moscow, 119899, Russia Telephone: +7 (095) 9391189 Fax: +7 (095) 939 0174
E-mail: Icp@libro.genebee.msu.su
35
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36
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ALEXEY YU. BOBROVSKY et al.
light reflection wavelength, under influence of different external factors (light,
heat, mechanical field) makes such materials very perspective for optical data
recording and storage [2-151.
Over last several years a number of publications devoted to low-molar-mass
[4-81 and polymeric cholesteric liquid crystals with the pitch of the helix
smoothly regulated under the light action have appeared [9-151. It was shown,
that cholesteric copolymers with photosensitive chiral side groups [ 10-141 and
mixtures of cholesteric copolymers with chiral-photochromic dopants [ 151 can
be used as optically active materials and, in particular, for optical data recording
and storage. UV light irradiation of planarly-oriented films of these materials
leads to E-Z photoisomerization of chiral-photochromic groups, that is accompanied by a decrease of the helical twisting power and a shift of the selective light
reflection peak. In the case of polymeric photosensitive cholesteric liquid crystals there is a unique possibility for the local variation of the pitch of helix and of
storage of recorded “information” for a prolonged time.
In spite of obvious progress, achieved in this field, the number of the effective
photo-optical (or photochromic) polymeric materials with the photoregulated
pitch of the helix is rather small and is mainly limited by some menthone derivatives [6,9-151.
In the work [15] we demonstrated the advantages of mixtures of cholesteric
copolymers and low-molar-mass photosensitive dopants in comparison with the
copolymers having a similar chemical structure, in which both chiral-photochromic and nematogenic groups are chemically linked to polymer backbone. In the
case of such mixtures we did not observed a widening of selective light reflection
peak during UV irradiation of the films owing to their homogeneous planar
structure caused by more “fast mixing” of low-molar-mass dopant with polymer
matrix. In addition helix untwisting rate and virtual quantum yields of photoprocesses for the mixtures have been several times higher as compared with the
pure copolymers [ 151.
The main objectives of this work is to synthesize a new family of chiral-photochromic dopants for cholesteric mixtures based on isosorbide and cinnamic acid:
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NEW PHOTOSENSITIVE CHIRAL DOPANT
37
As seen from the chemical formula, this substance contains an optically active
fragment based on isosorbide and two double C=C bonds capable of E-Z photoisomerization. The selection of cinnamoyl fragment as photosensitive group is
explained by the fact that peculiarities of E-Z isomerization (including other possible processes in such substances) have been studied earlier [ 16-19]; moreover,
it is well-known that isosorbide derivatives as chiral dopants in cholesteric mixtures have the greater values of the helical twisting power [20].
As for polymeric matrixes for this dopant we used nematogenic phenylbenzoate polyacrylate (mixtures of series I)
Irl
CH2
&H-COO-(CH2
U-J
zyxw
zyx
zy
) 5 - ~ O
~ ~O -O
C-OOCH,
and I-menthyl-containing copolymer forming the chiral nematic phase with a
left-handed cholesteric helix (mixtures of series 11):
dl
CH2
~H-CO0-(CH2)5-C0O~00C-@cH3
I
0.9
!
i
m l
CH2
I
CH-COO-(CH2)io-C00- B C O O -
uJ 0.1
zy
The main goals of this work are, firstly, the synthesis and investigation of photochemical behavior of the new chiral-photochromic dopant; secondly, the study
of photo-optical properties of cholesteric mixtures of this dopant with polymeric
substances aimed at their use for optical data recording and storage.
38
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zyxwvuts
ALEXEY YU. BOBROVSKY rt al.
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EXPERIMENTAL PART
Synthesis
Menthyl-containing and nematogenic monomers were synthesized according to
the procedures described in [21,22].
The following chemicals were used without further purification: Dicyclohexylcarbodiimide (Fluka), N,N'-dimethylaminopyridine (Fluka), 4-methoxycinnamic
acid (REAKHIM) and isosorbide (Lancaster Synthesis Ltd).
Synthesis of chiral-photochromic dopant
2,5-bis(4-methoxycinnamoyl)-1,4;3,6-dianhydro-D-sorbitol
To a solution of 3.42 mmoles of I ,4;3,6-dianhydro-D-sorbitol
and 10.27 mmoles
of 4-methoxycinnamic acid in 10 ml of purified absolute THF 1.03 mmoles of
N,N'-dimethylaminopyridinewas added. Then 10.27 mmoles of dicyclohexylcarbodiimide was added and the resulting solution was stirred for 3 days. The
formed precipitate was filtered, washed with THF, and diethyl ether (50 ml) was
added to a filtrate. The solution was washed successively with water, a 5% solution of acetic acid, and finally with water until pH 7 was achieved. The ether
extract was dried with anhydrous MgS04. After removal of solvent the white
crude product was purified by column chromatography (eluent-chloroform).
Yield: 96 % m.p.: 170-173 "C. IR (cm-') 2936, 2884, 2856 (CH2), 1706 (CO),
1634 (C=C), 1600, 1512 (C-C in Ar), 1254 (COC). UV (in dichloroethane):
hmax=312 nm, lgq,,,,=4.63.
Polymerization
The homo- and copolymer were synthesized by radical polymerization of appropriate monomers in benzene solution at 60°C; AIBN was used as an initiating
agent. The synthesized polymers were purified by the repeated precipitation with
methanol and dried in vacuum.
Physical Properties
IR spectra were recorded on a Bruker IFS-88 spectrophotometer using KBr pellets. Gel permeation chromatography (GPC) analysis was performed in THF on
Knauer set up equipped with Ultrastyragel 8x300 mm column (Waters) having
pore size lo3 A, detector - UV spectrometer Knauer. Waters 19x300 mm column
fulfilled with Ultrastyragel lo3 was used for preparative GPC.
a
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NEW PHOTOSENSITIVE CHIRAL DOPANT
39
zy
Phase transitions of the synthesized copolymers and mixtures were studied by
differential scanning calorimetry (DSC) with a scanning rate of 10 Wmin. All
experiments were performed using a Mettler TA-400 thermal analyzer and a
LOMO P-112 polarization microscope. Selective light reflection of the films of
chiral polymers was studied with a Hitachi U-3400 UV-Vis-IR spectrometer
equipped with a Mettler FP-80 hot stage. The 20-pm-thick samples were sandwiched between the two flat glass plates. The thickness of the test samples was
preset by Teflon spacers. Planar texture was obtained by shear deformation of the
samples, which were heated to temperatures above glass transition temperature.
Prior to tests, the test samples were annealed for 20-40 min at appropriate temperatures.
X-ray diffraction analysis was carried out using an URS-55 instrument (Ni-filtered CuK,-radiation, h = 1.54 A).
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Photo-optical Investigations
Photochemical investigations were performed using a special instrument [ 131
equipped with a DRSh-250 ultra-high pressure mercury lamp. Using filters, the
313 and 366 nm bands of linear radiation spectrum of mercury lamp were
selected. To prevent heating of the samples due to IR irradiation of the lamp,
water filter was used. To obtain plane-parallel light beam, quartz lens was used.
During irradiation, the constant temperature of the test samples was maintained
using a Mettler FP-80 heating unit. The intensities of UV irradiation were determined actinometrically [23] and were equal to 1.Ox
Einsteinxs-Ixcm-2
(hi,=3 13 nm) and 1. l x lo-* Einsteinxs-'xcm-* (hi,=366 nm).
In our photochemical studies dichloroethane was used as solvents. Concentrations of the solution was 1 . 6 5 ~ 1 0 -m~o l L For illumination, the solution was
kept in a 2-cm-thick quartz cell. The process of isomerization was controlled by
recording the absorption spectra of the illuminated solutions.
RESULTS AND DISCUSSION
Photochemical study of chiral-p..otochromic dopant in dilute
solution
UV-light irradiation of the dilute solution of the chiral dopant in dichloroethane
leads to the significant changes in the absorbance spectra (Figure la, b). A
decrease of extinction coefficients corresponding to n-n* and n-n* electronic
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40
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ALEXEY YU. BOBROVSKY et al.
1.s
1.o
2so
300
h/nm
350
400
z
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NEW PHOTOSENSITIVE CHIRAL DOPANT
0
10
zyxw
41
zyxw
zy
zyxwv
20
t/
30
40
min
FIGURE I (a) Changes of absorbance spectra of dichloroethane solution of chiral-photochromic
dopant during UV-irradiation (313 nm). Spectra were recorded each 5 min of irradiation; (b) absorbance decrease (at 3 13 nm) during UV irradiation
transitions of cinnamoyl chromophore is observed. It should be noted, that the
spectral peaks corresponding to the above-mentioned electronic transitions practically fully overlap (Figure 1). Such spectral changes during UV irradiation provide evidence of E-Z photoisomerization of the chiral-photochromic dopant [ 16181, as it is shown in Scheme 1.
In the course of phototransformations described above a noticeable decrease in
chiral molecules anisometry occurs, which is more clearly seen from molecular
models of the dopant (Figure 2). Using experimental data obtained earlier by
several authors [6, 9-15] one can assume that these structural changes must have
a marked influence on the helical twisting power of the chiral dopant.
Photo-optical properties of mixtures of chiral-photochromic
dopants with nematogenic homopolymer (mixtures I)
and cholesteric copolymer (mixtures 11)
Until describing photo-optical properties of mixtures based on synthesized chiral-photochromic dopant, let us consider their phase behavior and optical properties.
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zy
zyxwvu
42
ALEXEY YU. BOBROVSKY et al.
zyxwvu
P
CHJO
-
Z, E isomer
coo
zyxwvutsrqponm
-
Z, Z isomer
CHJO
SCHEME 1 Schematic representation of E-Z photoisomerization process of chiral-photochromic
dopant
All prepared mixtures with the chiral dopant concentration less then 10 mol%
form the chiral nematic phase (N*)*;as clearly seen from Figure 3, an increase of
the chiral dopant content leads to a decrease in clearing temperature.
zyxwvut
* The prolonged annealing of the mixtures leads to the formation of ordered TDK* phase with
melting temperature about 6 M 5 'C; structure of this phase was studied in detail in [24, 251. Nevertheless the formation of TDK*phase does nor affect on texture and optical properties of cholesteric
mixtures, that is why we do not take into consideration an existence of this phase.
43
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NEW PHOTOSENSITIVE CHIRAL DOPANT
zyxwvutsrqp
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FIGURE 2 Schematic representation of molecular shape changes of chiral-photochromic dopant during UV-irradiation
Downloaded By: [Bobrovsky, A.] At: 14:20 23 October 2007
44
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zyxw
zyxw
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ALEXEY YU.BOBROVSKY et al.
120
u 100
0
1
B
80
60
0
2
4
zyx
6
8
10
X I mol%
FIGURE 3 Dependence of clearing temperature on chiral dopant contents for cholesteric mixtures of
series I and 11
According to the DSC data all mixtures have approximately the same glass
transition temperatures, equal to about 20 - 25°C.
As shown in Figure4, planar texture of all mixtures selectively reflects the
light with wavelength corresponding to the visible and infrared regions of the
spectrum. The maximum of selective light reflection Amax weakly depends on
temperature.
In order to determine the handedness (sign) of cholesteric helix of the mixtures, the sandwich-like samples were prepared using the mixtures of series I and
cholesterol-containing chiral nematic copolymers [26]. Cholesterol-containing
copolymer composition was selected in such a way, so that the selective reflection bands of the mixtures and the copolymers would coincide [26]. The transmittance spectra analysis showed that in the case of mixtures I the transmittance
in selective reflection band is about zero. As known from literature data [27,28],
cholesterol derivatives with the long alkyl substituents usually stimulate
left-handed cholesteric helix formation. This fact allowed to conclude that in
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NEW PHOTOSENSITIVE CHIRAL DOPANT
45
mixtures I the right-handed cholesteric helix is formed, in the mixtures I, i.e. the
synthesized chiral dopant induces the right-handed cholesteric helix [29, 301.
A more complicated situation takes place in the case of mixtures of series I1
obtained by introduction of the chiral dopant in the left-handed cholesteric menthyl-containing copolymer (see Figure 4b). The introduction of 2.5 mol% of the
dopant leads to the compensation of “chirality” of the mixture: helix untwisting
is observed (as showed investigations of sandwich-like sample; the sense of helix
in this case coincides with the helical sense of the initial copolymer used as a
“matrix”). The mixtures with concentration of the dopant more then -2.7 mol%
of the chiral dopant form the right-handed helix (Figure 4b and 5).
In order to calculate the helical twisting power of the chiral-photochromic
dopant, dependencies of the reciprocal wavelength of the selective light reflection on mole fraction of the chiral dopant were plotted (Figure 5). The helical
twisting power was calculated from the slope of the dependencies of bias angle:
zy
zy
zyxwvu
zyxwv
p = fi(dX-’/dX)x=o,
were fi is the average refractive index, x is the mole fraction of the chiral dopant
in mixture. The apparent helical twisting power (/?/n) of the chiral-photochromic dopant is equal to 44.9k2.4 pm-’ for mixtures of series I and 39.9k2.5 pm-’
for mixtures of series 11. The @/ii values obtained are actually 5-5.5 times
higher than the helical twisting power of the chiral menthyl-containing side
groups of the copolymer used as matrix for dopant introduction (7.9iO. 1 pm-’)
[25]. It should be pointed out, that values of the helical twisting power are very
high, that is why the introduction of only 3-5 mol% of the chiral dopant give us a
possibility to obtain films with selective light reflection in the visible region of
the spectrum.
Thus, the above-mentioned peculiarities of the optical properties of mixture of
series I1 are explained by the fact, that the helical twisting power of the chiral-photochromic dopant is several times higher than the helical twisting power
of menthyl-containing chiral side groups of copolymer.
UV-light irradiation of planarly-oriented films of the mixtures leads to a
noticeable shift of selective light reflection peak to the long-wavelength region
of the spectrum (Figures 6 and 7). This effect is explained by a decrease in anisomery of the chiral dopant molecules during E-Z isomerization process
(Figure 2). It is important to underline that, as shown in Figure 6, during the photoinduced shift of the peak its widening does not occur; that is an advantage of
the obtained mixtures, comparing to the previously studied photosensitive cholesteric copolymers [ 10-151.
It is very interesting that the rate of the selective light reflection shift in the
case of the mixture I1 with 10 mol% of the dopant is higher (Figures 6, 7b). In
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46
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zyxwv
ALEXEY YU. BOBROVSKY et al.
I
900
I
1
I
t
3.0
E
700
E
.
x 6001
400
40
20
60
80
120
100
TPC
2500-
2000 -
E
1500-
\
x
I000 -
zyxwv
500 -
20
2.5
~
1
40
0
7.5
.
10.0
60
80
0
100
120
TPC
FIGURE 4 Temperature dependencies of selective light reflection maximum for mixtures of series I
(a) and I1 (b) with different chiral-photochromic dopant content (shown in mol% in figure)
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NEW PHOTOSENSITIVE CHIRAL DOPANT
I
0.00
47
zy
zyxw
zyxwvut
I
I
0.05
0.10
X
FIGURE 5 Dependence of the inverse selective light reflection wavelengths on molar fraction of chiral-photochromic dopant for mixtures of series I and 11 at temperature T=0.95TC,;x is the mole fraction of chiral-photochromic dopant
the case of the mixtures 11, a the right-handed dopant was introduced in the
left-handed cholesteric matrix of menthyl-containing copolymer, that is why in
this case the pitch of the helix is more sensitive to the helical twisting power
decrease during UV irradiation.
Other interesting feature of the helix untwisting kinetics is connected with
two-stage process. As clearly seen from Figure 7a, this process actually can be
considered as consisted of the fast and slow steps. In our opinion, the first stage
of helix untwisting is explained by E-Z isomerization, whereas the slow stage of
the decrease in the helical twisting power may occur due to a possible ( 2 + 2 )
photocycloaddition of dopant’s double bonds with formation of cyclobutane ring
[ 16-1 91. The dimers formation must lead to a supplementary decrease of the helical twisting power of the dopant, however the rate of this process is not high, as
zy
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48
zyxwvutsrqp
zyxw
ALEXEY YU. BOBROVSKY er 01.
*
I
zyxw
8
zyxwvut
FIGURE 6 Transmittance spectra changes during UV irradiation (366 nm) of planarly-oriented film
of mixture of series I (a) and I1 (b) with 5 and 10 mol% of chiral dopant, respectively. Spectra were
recorded each 40 s (in the case a) and 20 s (b) of irradiation. Irradiation temperature was 90 "C (a)
and 70 O C (b)
NEW PHOTOSENSITIVE CHIRAL DOPANT
..
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2500
.
.
.
I
I
zyxw
zyxw
zy
I
1
fs\
-/
i
2000 4
-z
zy
\
x
.
49
I ( 5 mol%)
-0- I 1 (10 mol%)
-
1000
-
500-
2000
1500
E
E
\
x 1000
500
0.0
0.2
zyxwvut
0.6 0.8
t/~ x l o - ~
0.4
1.0
FIGURE 7 (a) Changes of selective light reflection wavelength of the films obtained on the base of
mixtures of series I and 11 under U V irradiation (366 nm); (b) initial part of the plot (a)
it is controlled topochemically: a close contact of two C=C bonds is needed for
this process [31]. The analysis of the mixtures irradiated during two hours by the
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50
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ALEXEY YU. BOBROVSKY et 01.
gel permeation chromatography showed that the concentration of the chiral
dopant dimers after irradiation is neglectably small.
The analysis of the obtained experimental data allows to conclude that the synthesized new chiral-photochromic dopant possesses a number of undoubtable
merits, such as a large value of the helical twisting power, a good compatibility
with liquid crystalline polymers. Under UV light irradiation on cholesteric mixtures containing this dopant no widening of the selective light reflection peak is
observed, the rate of untwisting of cholesteric helix being high.
This research was supported by the Russian Foundation of Fundamental
Research (Grant 9943-33493, International Soros Science Educational Program (Grant a99-1495), Russian Research Program “Universities of Russia”
(grant 5 177), and partially by ESF-Program RESPOMAT.
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zyxwvuts
zyxw
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