Optical Properties of Polyvinyl Chloride Doped with DCM dye Thin Films

Abstract

Optical properties such as absorption coefficients, refractive indices, and extinction coefficients of pure polyvinyl-chloride (PVC) and DCM laser dye doped with PVC thin films where prepared using casting method have been determined in the range between 190-1100nm. Measurement have been performed in pure and doped (PVC). The direct electronic transition and indirect energy gaps were calculated using the behaver of absorption coefficient with wavelength. The direct energy gap was 3.9e.V for pure PVC and 2e.V for doped PVC, but indirect energy gap was 2.4e.V for pure PVC and 1.1e.V for doped. The phonon energy was 1.05e.V for pure PVC and was 0.55e.V for DCM doped with PVC thin film.

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WSN 30 (2016) 45-56 EISSN 2392-2192
Optical Properties of Polyvinyl Chloride Doped with
DCM dye Thin Films
Ahmed Namah Mohamed1,*, Akeel Shaker Tuhaiwer1, Zaid Saud Razzaq2
1Physics Department, College ofScience, Muthanna University,
Al-Muthanna, Samawa, Iraq
2Department of Science, College of Basic Education, Muthanna University,
Al-Muthanna, Samawa, Iraq
*E-mail address: aljeashie@gmail.com
ABSTRACT
Optical properties such as absorption coefficients, refractive indices, and extinction coefficients
of pure polyvinyl-chloride (PVC) and DCM laser dye doped with PVC thin films where prepared
using casting method have been determined in the range between 190-1100nm. Measurement have
been performed in pure and doped (PVC). The direct electronic transition and indirect energy gaps
were calculated using the behaver of absorption coefficient with wavelength. The direct energy gap
was 3.9e.V for pure PVC and 2e.V for doped PVC, but indirect energy gap was 2.4e.V for pure PVC
and 1.1e.V for doped. The phonon energy was 1.05e.V for pure PVC and was 0.55e.V for DCM doped
with PVC thin film.
Keywords: PVC; DCM; optical properties; thin films
1. INTRODUCTION
The doped material and precipitated as thin films is one of the appropriate technique to
study many of the physical and chemical properties that are difficult to obtain when the

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material in natural form [1]. The term thin-film using to describe a single or several layers of
the material atoms does not exceed a thickness one macron [2].
Thin films have special and import properties can be used in scientific and industrial
fields [3]. There are number of materials which have been used as solid hosts for laser dyes
such as: polymers, porous glasses, organically modified silicates or silicate nanocomposites,
and polycom glass (combination of polymer and sol–gel) [4].
Some important characteristics gave polymers forefront to be a host for dyes which
possess many favorable optical properties in comparison with other types of solid hosts. The
high homogeneity of polymers is important for narrow line width oscillators, and one can quit
efficiency control the chemical composition at the formation stage, and the show much better
compatibility with organic laser dye [5].
Incorporating laser dyes in polymer hosts decreases the degradation the dye, the
stability of the dye increases and the fluorescence intensity increases as well. This is due to
the dimmers decomposition which terminates the absorption process that accrues in the same
region of fluorescence resulting from re-absorption [6].
Figure 1. Structural formula of DCM laser dye.
Figure 2. Structural formula of PVC [8].

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A laser dye used in this study was DCM laser dye, structural formula is shown in figure
(1), Synonym: [2-[2-[4-(dimethylamino)phenyl]ethenyl]-6-methyl-4H- pyran-4-ylidene]-
propanedinitrile and the chemical formula is C19H17N3O[7].
This laser dye mixed with PVC with structural formula shown in Figure (2), with
chemical formula (C2H3Cl)n.
2. EXPERIMENTAL PART
2. 1. Sample preparation
Polyvinyl chloride was used as a host polymeric material in this work, supplied by
(BDH chemicals) with high purity, the aqueous solution of this polymer were prepared by
dissolving 1 gm of PVC in 30ml THF and thoroughly stirred using a magnetic stirrer for
about one hour until PVC was completely dissolved.
Preparation the desired concentration of the dye by weighting the right amount of dye
using the equation [9]
  
 (1)
where: W weight of the dissolved dye (g)
Mw Molecular weight of the dye (g/ml)
V the volume of the solvent (ml)
C the dye concentration (ml/lit)
To prepare 5×10-3 mol/lit DCM dye solution, firstly dissolving 0.015 gm in 10 ml of
THF to obtain 10 ml of dye solution.
Mixing 5ml of PVC solution with 5ml of dye solution and stirrer about 20 minutes to
obtain homogenous solution. This mixture casting on glass substrate at room temperature and
atmospheric pressure to obtain the final thin films.
2. 2. Thin films thickness measurement
Thickness of the prepared thin films was measured using the optical interferometer
method employing He-Ne laser 0.632 μm with incident angle 45° as shown in Fig. (3)
This method depends on the interference of the laser beam reflected from thin film
surface and then substrate, the films thickness (d) can be calculated using the following
formula [10]:
  

 (2)

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Figure 3. The optical interferometer method.
2. 3. Optical properties measurements
The optical absorption spectra of pure PVC and DCM doped with PVC thin films were
recorded at room temperature using UV-VIS double beam spectrometer in the wave length
range from 190 to 1100 nm.
The optical absorption coefficient (α) of pure PVC and DCM doped with PVC films is
very important because it provides information on the electronic band structure. This
coefficient was calculated using the following relation [11]:
  

(3)
The reflectance was calculated after determined the transmittance (T) from the UV-VIS
spectrometer using the following formula [12]
A + T + R = 1
(4)
and the linear refractive index (n) is given by [13]

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  

(5)
The extinction coefficient is obtained in terms of the absorption coefficient using the
following formula [14]
  

(6)
3. RESULTS AND DISCUSSION
Figure (4) shows the optical absorption spectrum of pure PVC thin film sample. In the
UV region, the absorption decreases with increasing the wavelength which is related to high
energy absorption. While in the visible region there are no absorption bands since the films
are transparent, and the absorbance will be constant in this region.
Figure 4. Absorption spectra of pure PVC and DCM doped with PVC thin films
But when the PVC doped with DCM laser dye the absorption spectrum shifted to a
higher wavelength in the visible region as shown in Figure (4). The absorbance intensity
increases with a little shifting towards higher wavelengths, these agree with beer-Lambert
law.
0
0,5
1
1,5
2
2,5
3
3,5
0 100 200 300 400 500 600 700 800
Absorption (a.u.)
Wavelength (nm)
PVC
PVC with dye

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Figure (5) illustrates the dependence of the liner absorption coefficients on the photon
wavelength for pure PVC thin film and PVC doped with DCM, where their values increase
rapidly beyond absorption edge regions for the two samples (pure and doped PVC).
Figure 5. Absorption liner coefficient of pure PVC and DCM doped with PVC thin films.
Figure 5. Absorption liner coefficient of pure PVC and DCM doped with PVC thin films
0
2000
4000
6000
8000
10000
12000
14000
16000
0 1 2 3 4 5
α(cm-1)
hν (e.V)
PVC with dye
PVC
0
2000
4000
6000
8000
10000
12000
14000
16000
0 1 2 3 4 5
α(cm-1)
hν (e.V)
PVC with dye
PVC

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From the shape of the (α > 104 cm-1), one can deduce the transfer represents the
electronic direct transfer [15]. Based on this result has been drawing the relationship between
the values of (αhν)2 as a function of energy is a straight line tangent to the curve is determined
by the values of the direct energy gap [16]. These energy gap values was calculated from
Figure (6) for pure PVC thin film and from Figure (7) for DCM doped with PVC's.
Figure 6. Dependence of (αhν)2 on the photon energy for pure PVC thin film
The direct electronical transition energy gap was 3.9e.V for pure PVC thin film, while
this energy was 2e.V foe DCM doped with PVC thin film.
Figure 7. Dependence of (αhν)2 on the photon energy for DCM doped with PVC thin film
0
1
2
3
4
5
6
7
8
0 1 2 3 4 5
(αhν)2 ×10-9
hν(e.V)
0
1
2
3
4
5
6
7
8
9
10
012345
(αhν)2 ×10-9
hν(e.V)

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Figure (8) shows the relation between (αhν)1/2 and photon energy for pure PVC thin
film. It has been observed from this figure that the indirect electronic energy gap; Eg = 2.4e.V
and the phonon energy; Ep = 1.1e.V.
Figure 8. Dependence of (αhν)1/2 on the photon energy for pure PVC thin film
Figure (9) shows the dependence of (αhν)1/2 and photon energy for DCM doped with
PVC thin film. It has been observed from this figure that the indirect electronic energy gap;
Eg = 1.05e.V and the phonon energy; Ep = 0.55e.V.
Figure 9. Dependence of (αhν)1/2 on the photon energy for DCM doped with PVC thin film
0
20
40
60
80
100
120
140
160
180
0 1 2 3 4 5
(αhν)1/2
hν(e.V)
0
20
40
60
80
100
120
140
160
180
200
0 1 2 3 4 5
(αhν)1/2
hν(e.V)

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Figure 10. Refractive index variation with the wavelength for pure PVC thin film
Figure 11. Refractive index variation with the wavelength for DCM doped with PVC
thin film

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Figure 12. Extinction coefficient of pure PVC thin film variation with the wavelength
Figure 13. Extinction coefficient of DCM doped with PVC thin film variation with the
wavelength
0
0,05
0,1
0,15
0,2
0,25
0,3
0 100 200 300 400 500 600 700 800
Extinction coefficient(K)
Wavelength(nm)
0
0,1
0,2
0,3
0,4
0,5
0,6
0 100 200 300 400 500 600 700 800
Extinction coefficient(K)
Wavelength(nm)

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Figure (10) shows the variation of refractive index of thin film consist of casting PVC
polymer. As shown from this figure, the refractive index decreases as the wavelength increase
until 400 nm and then become nearly constant with increasing wavelength; the value of
refractive index within the constant range was varying from 1.42-1.75.
On the other hand the refractive index of the thin film composed of DCM doped with
PVC polymer shown in Fig. (11). It is obviously that the refractive index of the thin film
initially decreasing to the lowest value at 559 nm after that it increases readily at 562 nm then
the refractive index clears to be constant with increasing the photon energy.
The extinction coefficient allows for estimation the molar concentration of the mixture
before casting the solution on the glass substrate. Figure (12) shows the plot between the
extinction coefficient against the wavelength of the pure PVC thin film. The extinction
coefficient decreasing with increasing the photon energy, then it is increasing beyond 400 nm
wavelength. Figure (13) shows the variation of the extinction coefficient with the wavelengths
of the DCM doped with PVC thin film. It is undergoing a shifting toward the longer
wavelength.
4. CONCLUSIONS
In the current work, the optical properties of the prepared thin films shows that the red
shifting in absorption spectrum of dopant film caused by the doping while inverse occurs in
linear absorption coefficient. From the linear absorption spectra on can deduce that the direct
electronic transition energy gap decreasing from 3.9 e.V for pure PVC thin film to 2 e.V in
dopant thin film. The same thing happens for in direct electronic transition where Eg = 2.4
e.V for pure PVC and decreasing to be 1.1 e.V for dopant PVC. The phonon energy in
indirect transition was 1.05 e.V for pure PVC and equal to 0.55 e.V for DCM doped with
PVC thin film.
Acknowledgement
Author(s) would like to express him (their) thanks to Dr. Jafer Fahdel Odah to his helped and supported him
(their) during the period of preparing this work.
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( Received 07 November 2015; accepted 19 November 2015 )