Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films

The derivatives of phenylazobenzoic, phenylazosalicylic acids and azobenzeneazonaphthalene were synthesized and employed to prepare polarizing films based on polyvinyl alcohol (PVA). The single-piece transmittance (T0), polarizing efficiency (PE), dichroic ratio (Rd) of films and order parameter...

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Дата:2013
Автори: Filippovich, L.N., Ariko, N.G., Almodarresiyeh, H.A., Shahab, S.N., Malashko, P.M., Agabekov, V.E.
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Опубліковано: Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України 2013
Назва видання:Semiconductor Physics Quantum Electronics & Optoelectronics
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Цитувати:Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films / .N. Filippovich, N.G. Ariko, H.A. Almodarresiyeh, S.N. Shahab, P.M. Malashko, V.E. Agabekov // Semiconductor Physics Quantum Electronics & Optoelectronics. — 2013. — Т. 16, № 2. — С. 220-23. — Бібліогр.: 7 назв. — англ.

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spelling irk-123456789-1176972017-05-27T03:03:40Z Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films Filippovich, L.N. Ariko, N.G. Almodarresiyeh, H.A. Shahab, S.N. Malashko, P.M. Agabekov, V.E. The derivatives of phenylazobenzoic, phenylazosalicylic acids and azobenzeneazonaphthalene were synthesized and employed to prepare polarizing films based on polyvinyl alcohol (PVA). The single-piece transmittance (T0), polarizing efficiency (PE), dichroic ratio (Rd) of films and order parameter of dyes (Sdye) were calculated. It was found that parameters Rd and Sdye increased as electron-donating of substituents in molecules of phenylazobenzoic and phenylazosalicylic acids derivatives was grown, and the polarizing efficiency of film increased with increasing the order parameter of dye. Development of PVA films dyed with the derivatives of phenylazosalicylic acid and azobenzeneazonaphthalene allowed to obtain polarizers for near UV and visible range of spectrum, respectively. It was also developed a broadband polarizer for 300-610 nm. 2013 Article Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films / .N. Filippovich, N.G. Ariko, H.A. Almodarresiyeh, S.N. Shahab, P.M. Malashko, V.E. Agabekov // Semiconductor Physics Quantum Electronics & Optoelectronics. — 2013. — Т. 16, № 2. — С. 220-23. — Бібліогр.: 7 назв. — англ. 1560-8034 PACS 42.79.Ci http://dspace.nbuv.gov.ua/handle/123456789/117697 en Semiconductor Physics Quantum Electronics & Optoelectronics Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description The derivatives of phenylazobenzoic, phenylazosalicylic acids and azobenzeneazonaphthalene were synthesized and employed to prepare polarizing films based on polyvinyl alcohol (PVA). The single-piece transmittance (T0), polarizing efficiency (PE), dichroic ratio (Rd) of films and order parameter of dyes (Sdye) were calculated. It was found that parameters Rd and Sdye increased as electron-donating of substituents in molecules of phenylazobenzoic and phenylazosalicylic acids derivatives was grown, and the polarizing efficiency of film increased with increasing the order parameter of dye. Development of PVA films dyed with the derivatives of phenylazosalicylic acid and azobenzeneazonaphthalene allowed to obtain polarizers for near UV and visible range of spectrum, respectively. It was also developed a broadband polarizer for 300-610 nm.
format Article
author Filippovich, L.N.
Ariko, N.G.
Almodarresiyeh, H.A.
Shahab, S.N.
Malashko, P.M.
Agabekov, V.E.
spellingShingle Filippovich, L.N.
Ariko, N.G.
Almodarresiyeh, H.A.
Shahab, S.N.
Malashko, P.M.
Agabekov, V.E.
Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films
Semiconductor Physics Quantum Electronics & Optoelectronics
author_facet Filippovich, L.N.
Ariko, N.G.
Almodarresiyeh, H.A.
Shahab, S.N.
Malashko, P.M.
Agabekov, V.E.
author_sort Filippovich, L.N.
title Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films
title_short Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films
title_full Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films
title_fullStr Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films
title_full_unstemmed Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films
title_sort structure effect and orientation distribution of azo dyes on optical anisotropy of dyed pva-films
publisher Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України
publishDate 2013
url http://dspace.nbuv.gov.ua/handle/123456789/117697
citation_txt Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films / .N. Filippovich, N.G. Ariko, H.A. Almodarresiyeh, S.N. Shahab, P.M. Malashko, V.E. Agabekov // Semiconductor Physics Quantum Electronics & Optoelectronics. — 2013. — Т. 16, № 2. — С. 220-23. — Бібліогр.: 7 назв. — англ.
series Semiconductor Physics Quantum Electronics & Optoelectronics
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fulltext Semiconductor Physics, Quantum Electronics & Optoelectronics, 2013. V. 16, N 2. P. 220-223. © 2013, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 220 PACS 42.79.Ci Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films L.N. Filippovich1, N.G. Ariko1, H.A. Almodarresiyeh1, S.N. Shahab1, P.M. Malashko2, V.E. Agabekov2 1Institute of Physical Organic Chemistry, National Academy of Sciences of Belarus 13, Surganova str., 220072 Minsk, Belarus; 2Institute of New Materials Chemistry, National Academy of Sciences of Belarus 36, F. Skaryny str., 220141 Minsk, Belarus; e-mail: luda1977@list.ru Abstract. The derivatives of phenylazobenzoic, phenylazosalicylic acids and azobenzeneazonaphthalene were synthesized and employed to prepare polarizing films based on polyvinyl alcohol (PVA). The single-piece transmittance (T0), polarizing efficiency (PE), dichroic ratio (Rd) of films and order parameter of dyes (Sdye) were calculated. It was found that parameters Rd and Sdye increased as electron-donating of substituents in molecules of phenylazobenzoic and phenylazosalicylic acids derivatives was grown, and the polarizing efficiency of film increased with increasing the order parameter of dye. Development of PVA films dyed with the derivatives of phenylazosalicylic acid and azobenzeneazonaphthalene allowed to obtain polarizers for near UV and visible range of spectrum, respectively. It was also developed a broadband polarizer for 300-610 nm. Keywords: dichroic polarizers, polyvinyl alcohol, mono- and disazodyes, spectral- polarizing properties. Manuscript received 21.12.12; revised version received 12.02.13; accepted for publication 19.03.13; published online 25.06.13. 1. Introduction Dichroic film polarizers are polymer uniaxially oriented films colored with molecular iodine or organic dyes. Polarizers based on polyvinyl alcohol (PVA) have the most practical application. The study of spectral properties of PVA films colored by different classes of dyes showed that the azocompounds can get film material with a high polarizing ability. However, the optical properties of these polarizers are dependent on many factors: the structure and the orientation distribution of the dye molecules in the polymer matrix, phase state and supramolecular structure of PVA, intermolecular interactions between dye molecules and macromolecules of the polymer [1 – 3]. In this work, the derivatives of phenylazobenzoic, phenylazosalicylic acids and azobenzeneazonaphthalene were synthesized, and then they were used for dyeing the PVA-films polarizing in near UV and visible regions of the spectrum. The purpose of this study is to determine the influence of the molecular structure (type and location of auxochrome group) of the synthesized compounds and the orientation distribution of dyes molecules in the polymer matrix on dichroism of PVA-films. Semiconductor Physics, Quantum Electronics & Optoelectronics, 2013. V. 16, N 2. P. 220-223. © 2013, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 221 2. Experiment Disazodyes: N=N N=NNaO3S NH2 OH NaO3S OCH3 М1 N=N N=N SO3Na NH2 HO М2 N=N N=N NH2 OH NaO3S М3 N=N N=N OCH3 NaO3S SO3Na NH2 OH IV N=NN=N NaO3S SO3Na NH2 OH V N=N NaO3S SO3Na NH2 N N VI and monoazodyes (Table 2) of the general formula: N=N R1 R2 R3 were synthesized in the form of free acids or their sodium salts by the diazotization of aromatic amines or diamines followed by azocoupling with salicylic, aminonaftolsulfo and acetoacetic acid in acidic or alkaline medium [4]. Preparation of polarizing films is described in [5]. Absorption and transmission spectra of films were measured using a UV-NIR Spectrometer HR4000CG (Ocean Optics, USA) equipped with wire-grid polarizer UBB01A (Moxtek, USA). Optical properties of the polarizers were expressed in terms of such optical characteristics as the single- piece transmittance (T0), polarizing efficiency (PE) and dichroic ratio (Rd) of dyed PVA-films. The order parameter (Sdye) characterized the degree of aligning dye molecules toward the orientation film axis. These parameters were calculated by means of the equations [6]: Т0 = (Т|| + Т)/2, PE = {(Т  Т||) / (Т|| + Т)}∙100%, Rd = D|| / D, Sdye = (Rd  1)/(Rd + 2), where D||, D  absorption and Т||, Т  film transmittance of linearly polarized light in parallel (||) and perpendicular () orientation of the electric vector of linearly polarized light towards the orientation axis of the film. 3. Results and discussion Investigated PVA-films colored with mono- and disazodyes have a positive dichroism, which proves that the long-wave absorption dye oscillator is directed along its main molecular axis. The latter, in its turn, is oriented in the direction of the film orientation axis. Polarization efficiency of a film is determined primarily by the structure of dye molecules embedded in polymer. So, the samples obtained under identical conditions and polarized in the visible range of spectrum have the values of PE from 33 up to 98% (Table 1). Besides, the similar change of the order parameter Sdye can be seen. Ab initio SCF MO LCAO RHF/MINI (3d) method was used in order to model the spatial structure of the dyes. It was found that the highest value of PE is inherent to the films colored with molecules that have a flat “extension” frame of two benzene and single naphthalene rings without volume substitutes causing steric hindrance for the alignment of dye molecules along the polymer chains and towards the drawing direction (compounds M1, M2 and M3). Semiconductor Physics, Quantum Electronics & Optoelectronics, 2013. V. 16, N 2. P. 220-223. © 2013, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 222 Table 1. Sdye and PE for films dyed with disazodyes. The dye concentration is 0.2-0.4 mas.%. The film thickness is 60 μm. Dye max, nm D D Rd Sdye PE, % М1 595 1.52 0.15 10.1 0.75 92 М2 585 2.22 0.50 4.4 0.53 96 М3 580 2.19 0.26 8.4 0.71 98 IV 495 1.57 0.40 3.9 0.49 87 V 570 0.80 0.46 1.7 0.19 61 VI 507 0.62 0.33 1.9 0.23 33 Table 2. Order parameter and spectral-polarization characteristics of the films dyed by monoazodyes. The dye concentration is 0.2 to 0.3 mas.%. The film thickness is close to 50…60 µm. Т Т Substituent Cipher of dye max, nm % D D Т0, % Rd Sdye PE, % R1= COONa, R2 = Н, R3= COONa VII 351 75.6 2.8 0.122 1.553 39.2 12.7 0.80 93 R1= COOH, R2 = Н, R3= COOH VIII 351 91.4 11.5 0.039 0.939 51.4 24.0 0.89 78 R1= OH, R2 = COONa, R3= CH3-C(O) IX 381 43.0 1.4 0.367 1.854 22.2 5.1 0.58 94 R1= OH, R2 = COOH, R3= CH3-C(O) X 381 42.5 0.5 0.372 2.301 21.5 6.2 0.63 98 R1= OH, R2 = COONa, R3= CH3-C(O)-NH XI 376 28.6 0.01 0.544 4.000 14.3 7.4 0.68 99 R1= OH, R2 = COONa, R3= NaOOC XII 380 78.1 4.2 0.107 1.377 41.1 12.9 0.80 90 R1= OH, R2 = COONa, R3= NH2 XIII 399 64.7 0.5 0.189 2.301 32.6 12.2 0.79 99 R1= OH, R2 = COONa, R3= CH3O-C6H4-C2H2-C(O) XIV 386 51.4 1.3 0.289 1.886 26.4 6.5 0.65 95 R1= OH, R2 = COOH, R3= CH3O-C6H4-C2H2-C(O) XV 382 41.7 0.6 0.380 2.222 21.2 5.8 0.61 97 Sulfo-groups do not violate flatness of molecules M1 and M3. Violation of coplanarity of the dye molecules IV and V reduces the intensity of the long- wave absorption bands and decrease values of Sdye and PE. Molecules of dye VI, the length of which is comparable with their width, are oriented in polymer matrix with different angles of deviation of its main absorption axis along the drawing axis, which is the reason for the low polarizing ability of dyed PVA-film. Monoazoderivatives of benzoic and salicylic acid are effective dichroic components of films polarizing in the near UV range of the spectrum (Table 2). The nature of substituents in the dye molecule affects not only on the position and intensity of the long- wave absorption band of the film, but also on its dichroism. “Delete” from the conjugation one of the NaO(O)C-group in the dye VII and the introduction of the e-supplying group OH on its place: N=N COONaNaOOC VII N=N OH COONa NaOOC XII does not practically change the value of the order parameter Rd, but replacing the second NaO(O)C-group on e-withdrawing substituent R = СН3С(О) – (IX), CH3C(O)NH- (XI), CH3(O)Ar-CH = CH – C(O) – (XIV) N=NR OH COONa reduces Rd from 12.2…12.7 to ~5-7. With the e- supplying group NH2: N=N OHNH2 COONa XIII Semiconductor Physics, Quantum Electronics & Optoelectronics, 2013. V. 16, N 2. P. 220-223. © 2013, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 223 Rd returned to 12.2. In general, with increase of electron- donating of substituents the value of dichroic ratio increases: R: NH2- > CH3C(O)NH- > СН3(O)Ar-CH=CH-C(O)- > СН3С(О) Rd: 12.2 > 7.4 > 6.5 > 5.1 The value of Sdye (Table 2) also depends on the structure of dye and for the compounds VII-XV is: R: NaO(O)C-NH2-CH3C(O)NH-СН3(O)Ar-CH=CH-C(O)- СН3С(О) Scr: 0.80 0.79 0.68 0.65 0.63 Since the orientation of the dye strongly depends on the spatial structure of its molecules [7], introduction of larger volume substituents   -NHOCCH3 ,     -OC-CHCH-ArOCH3  and CH3C(O) compared to groups NaO(O)C- and NH2- reduces Sdye. The order parameter Sdye decreases with increasing the dye concentration (C) in the film. For example, the increase of C for dye IX from 0.15 up to 0.30 mas.% reduces the value of Sdye from 0.63 to 0.58, and in the case of dye XIII the growth of C from 0.2 up to 0.4 mas.% causes the decrease in Sdye from 0.88 down to 0.71. This dependence CSdye  was predicted using the mathematical model worked out to describe the spectral- polarizing properties of dyed PVA films and was experimentally proved with film samples containing azo dye “direct blue”[6]. The orientation degree of the dye molecules increases in films with a quasi-crystalline structure of PVA that is formed after the heat treatment of the PVA- film and the processing by “cross-linking” agent (boric acid) [5]. This structure is characterized by a highly ordered polymer chains with respect to the drawing axis of the film, and as a result increase the degree of orientation of the dye molecules in the polymer matrix. For example, the parameter Sdye of the dye M1 in films untreated and treated with boric acid is equal to 0.63 and 0.78, respectively [5]. Studying the optical properties of PVA-films dyed by (M3H) obtained by treatment of dye M3 with hydrochloric acid, we found that M3H is an effective dichroic component of films polarizing in near UV and visible ranges of spectrum (Fig. 1). The polarization efficiency of this film is 92 to 99% (300…400 nm) and 96 to 99% (400…610 nm). Fig. 1. Transmission spectra and polarizing ability of PVA- film dyed by M3H. 1 – Т||, 2 – Т┴, 3 – PE; film thickness is 60 μm; dye concentration is 0.4 mas.%. 4. Conclusion The structure of molecules of derivatives of phenylazobenzoic and phenylazosalicylic acids as well as azobenzeneazonaphtalene influences on optical properties of polarizing PVA films and orientation alignment of azodyes in polymeric matrix. With rising electron-donating of the substituents conjugated with the chain of double bonds in derivatives of phenylazobenzoic and phenylazosalicylic acids, the dichroic ratio of film and the order parameter of dye (a degree of dye orientation in polymer matrix) increase. The polarizing ability of films grows with rising the order parameter of dye, the value of which depends on the concentration of dye and the supramolecular structure of polymer matrix. From PVA dyed by synthesized mono- and disazodyes we obtained the polarizers for UV and visible ranges of the spectrum as well as the broadband polarizer for the range 300…610 nm. Acknowledgement The authors are grateful to Dr. V. Zelenkovskii for assistance in the work to optimize the geometry of dye structure. References 1. J.B. Cnang, J.H. Hwang, S. Jong, The effect of dye structure on the dyeing and optical properties of dichroic dyes for polarizing film // Dyes and pigmentes, 88, р. 366-371 (2011). 2. D.H. Song, H.Y. Yoo, J.P. Kim, Synthesis of stilbene-based azo dyes and application for dichroic materials in poly(vinyl alcohol) polarizing films // Dyes and pigments, 75, р. 727-731 (2007). 3. A. Altomare, F. Ciardelli, M. Marchini, R. Solaro, Polymer dispersions of model azobenzele dyes // Polymer, 46, р. 2086-2096 (2005). 4. B.А. Poraj-Koshitz, Аzodyes. Chemistry, Leningrad, 1972 (in Russian). 5. V.Е. Аgabekov, N.G. Аriko, S.N. Shahab, L.N. Filippovich, P.M. Malashko, The influence of dyes nature and structure of polymer on optical and thermal properties of film polarizers // Dokl. BGYIR, 5, p. 109-118 (2008). 6. S.E. Han, I.S. Hwang, Modeling of the optical anisotropy of a dye polarizer // J. Polymer Sci. Part B. Polymer Physics, 40, р. 1363-1370 (2002). 7. B.T. Kobayashi, Y. Tanizaki, N. Ando, Absorption spectra of dyes. VI. Steric effects in conjugated systems of benzidine disazo dyes and their copper derivatives // Bull. Chem. Soc. Japan, 33, р. 913- 917 (1960). Semiconductor Physics, Quantum Electronics & Optoelectronics, 2013. V. 16, N 2. P. 220-223. PACS 42.79.Ci Structure effect and orientation distribution of azo dyes on optical anisotropy of dyed PVA-films L.N. Filippovich1, N.G. Ariko1, H.A. Almodarresiyeh1, S.N. Shahab1, P.M. Malashko2, V.E. Agabekov2 1Institute of Physical Organic Chemistry, National Academy of Sciences of Belarus 13, Surganova str., 220072 Minsk, Belarus; 2Institute of New Materials Chemistry, National Academy of Sciences of Belarus 36, F. Skaryny str., 220141 Minsk, Belarus; e-mail: luda1977@list.ru Abstract. The derivatives of phenylazobenzoic, phenylazosalicylic acids and azobenzeneazonaphthalene were synthesized and employed to prepare polarizing films based on polyvinyl alcohol (PVA). The single-piece transmittance (T0), polarizing efficiency (PE), dichroic ratio (Rd) of films and order parameter of dyes (Sdye) were calculated. It was found that parameters Rd and Sdye increased as electron-donating of substituents in molecules of phenylazobenzoic and phenylazosalicylic acids derivatives was grown, and the polarizing efficiency of film increased with increasing the order parameter of dye. Development of PVA films dyed with the derivatives of phenylazosalicylic acid and azobenzeneazonaphthalene allowed to obtain polarizers for near UV and visible range of spectrum, respectively. It was also developed a broadband polarizer for 300-610 nm. Keywords: dichroic polarizers, polyvinyl alcohol, mono- and disazodyes, spectral-polarizing properties. Manuscript received 21.12.12; revised version received 12.02.13; accepted for publication 19.03.13; published online 25.06.13. 1. Introduction Dichroic film polarizers are polymer uniaxially oriented films colored with molecular iodine or organic dyes. Polarizers based on polyvinyl alcohol (PVA) have the most practical application. The study of spectral properties of PVA films colored by different classes of dyes showed that the azocompounds can get film material with a high polarizing ability. However, the optical properties of these polarizers are dependent on many factors: the structure and the orientation distribution of the dye molecules in the polymer matrix, phase state and supramolecular structure of PVA, intermolecular interactions between dye molecules and macromolecules of the polymer [1 – 3]. In this work, the derivatives of phenylazobenzoic, phenylazosalicylic acids and azobenzeneazonaphthalene were synthesized, and then they were used for dyeing the PVA-films polarizing in near UV and visible regions of the spectrum. The purpose of this study is to determine the influence of the molecular structure (type and location of auxochrome group) of the synthesized compounds and the orientation distribution of dyes molecules in the polymer matrix on dichroism of PVA-films. 2. Experiment Disazodyes:N =N N =N N a O 3 S N H 2 O H N a O 3 S O C H 3 N=N N=N NaO 3 S NH 2 OH NaO 3 S OCH 3 М1 N =N N =N S O 3 N a N H 2 H O N=N N=N SO 3 Na NH 2 HO М2 N =N N =N N H 2 O H N a O 3 S N=N N=N NH 2 OH NaO 3 S М3 N =N N =N O C H 3 N a O 3 S S O 3 N a N H 2 O H N=N N=N OCH 3 NaO 3 S SO 3 Na NH 2 OH IV N =N N =N N a O 3 S S O 3 N a N H 2 O H N=N N=N NaO 3 S SO 3 Na NH 2 OH V N =N N a O 3 S S O 3 N a N H 2 N N N=N NaO 3 S SO 3 Na NH 2 N N VI and monoazodyes (Table 2) of the general formula: N = N R 1 R 2 R 3 N=N R 1 R 2 R 3 were synthesized in the form of free acids or their sodium salts by the diazotization of aromatic amines or diamines followed by azocoupling with salicylic, aminonaftolsulfo and acetoacetic acid in acidic or alkaline medium [4]. Preparation of polarizing films is described in [5]. Absorption and transmission spectra of films were measured using a UV-NIR Spectrometer HR4000CG (Ocean Optics, USA) equipped with wire-grid polarizer UBB01A (Moxtek, USA). Optical properties of the polarizers were expressed in terms of such optical characteristics as the single-piece transmittance (T0), polarizing efficiency (PE) and dichroic ratio (Rd) of dyed PVA-films. The order parameter (Sdye) characterized the degree of aligning dye molecules toward the orientation film axis. These parameters were calculated by means of the equations [6]: Т0 = (Т|| + Т()/2, PE = {(Т( ( Т||) / (Т|| + Т()}∙100%, Rd = D|| / D(, Sdye = (Rd ( 1)/(Rd + 2), where D||, D( ( absorption and Т||, Т( ( film transmittance of linearly polarized light in parallel (||) and perpendicular (() orientation of the electric vector of linearly polarized light towards the orientation axis of the film. 3. Results and discussion Investigated PVA-films colored with mono- and disazodyes have a positive dichroism, which proves that the long-wave absorption dye oscillator is directed along its main molecular axis. The latter, in its turn, is oriented in the direction of the film orientation axis. Polarization efficiency of a film is determined primarily by the structure of dye molecules embedded in polymer. So, the samples obtained under identical conditions and polarized in the visible range of spectrum have the values of PE from 33 up to 98% (Table 1). Besides, the similar change of the order parameter Sdye can be seen. Ab initio SCF MO LCAO RHF/MINI (3d) method was used in order to model the spatial structure of the dyes. It was found that the highest value of PE is inherent to the films colored with molecules that have a flat “extension” frame of two benzene and single naphthalene rings without volume substitutes causing steric hindrance for the alignment of dye molecules along the polymer chains and towards the drawing direction (compounds M1, M2 and M3). Sulfo-groups do not violate flatness of molecules M1 and M3. Violation of coplanarity of the dye molecules IV and V reduces the intensity of the long-wave absorption bands and decrease values of Sdye and PE. Molecules of dye VI, the length of which is comparable with their width, are oriented in polymer matrix with different angles of deviation of its main absorption axis along the drawing axis, which is the reason for the low polarizing ability of dyed PVA-film. Monoazoderivatives of benzoic and salicylic acid are effective dichroic components of films polarizing in the near UV range of the spectrum (Table 2). The nature of substituents in the dye molecule affects not only on the position and intensity of the long-wave absorption band of the film, but also on its dichroism. “Delete” from the conjugation one of the NaO(O)C-group in the dye VII and the introduction of the e-supplying group OH on its place: N = N C O O N a N a O O C N=N COONa NaOOC VII N = N O H C O O N a N a O O C N=N OH COONa NaOOC XII does not practically change the value of the order parameter Rd, but replacing the second NaO(O)C-group on e-withdrawing substituent R = СН3С(О) – (IX), CH3C(O)NH- (XI), CH3(O)Ar-CH = CH – C(O) – (XIV) N = N R O H C O O N a N=N R OH COONa reduces Rd from 12.2…12.7 to ~5-7. With the e-supplying group NH2: N = N O H N H 2 C O O N a N=N OH NH 2 COONa XIII Rd returned to 12.2. In general, with increase of electron-donating of substituents the value of dichroic ratio increases: R: NH2- > CH3C(O)NH- > СН3(O)Ar-CH=CH-C(O)- > СН3С(О) Rd: 12.2 > 7.4 > 6.5 > 5.1 The value of Sdye (Table 2) also depends on the structure of dye and for the compounds VII-XV is: R: NaO(O)C-NH2-CH3C(O)NH-СН3(O)Ar-CH=CH-C(O)- СН3С(О) Scr: 0.80 0.79 0.68 0.65 0.63 Since the orientation of the dye strongly depends on the spatial structure of its molecules [7], introduction of larger volume substituents ( ) - NH O C CH 3 , ( ) ( ) - O C - CH CH - Ar O CH 3 = and CH3C(O) compared to groups NaO(O)C- and NH2- reduces Sdye. The order parameter Sdye decreases with increasing the dye concentration (C) in the film. For example, the increase of C for dye IX from 0.15 up to 0.30 mas.% reduces the value of Sdye from 0.63 to 0.58, and in the case of dye XIII the growth of C from 0.2 up to 0.4 mas.% causes the decrease in Sdye from 0.88 down to 0.71. This dependence C S dye - was predicted using the mathematical model worked out to describe the spectral-polarizing properties of dyed PVA films and was experimentally proved with film samples containing azo dye “direct blue”[6]. The orientation degree of the dye molecules increases in films with a quasi-crystalline structure of PVA that is formed after the heat treatment of the PVA-film and the processing by “cross-linking” agent (boric acid) [5]. This structure is characterized by a highly ordered polymer chains with respect to the drawing axis of the film, and as a result increase the degree of orientation of the dye molecules in the polymer matrix. For example, the parameter Sdye of the dye M1 in films untreated and treated with boric acid is equal to 0.63 and 0.78, respectively [5]. Studying the optical properties of PVA-films dyed by (M3H) obtained by treatment of dye M3 with hydrochloric acid, we found that M3H is an effective dichroic component of films polarizing in near UV and visible ranges of spectrum (Fig. 1). The polarization efficiency of this film is 92 to 99% (300…400 nm) and 96 to 99% (400…610 nm). Fig. 1. Transmission spectra and polarizing ability of PVA-film dyed by M3H. 1 – Т||, 2 – Т┴, 3 – PE; film thickness is 60 μm; dye concentration is 0.4 mas.%. 4. Conclusion The structure of molecules of derivatives of phenylazobenzoic and phenylazosalicylic acids as well as azobenzeneazonaphtalene influences on optical properties of polarizing PVA films and orientation alignment of azodyes in polymeric matrix. With rising electron-donating of the substituents conjugated with the chain of double bonds in derivatives of phenylazobenzoic and phenylazosalicylic acids, the dichroic ratio of film and the order parameter of dye (a degree of dye orientation in polymer matrix) increase. The polarizing ability of films grows with rising the order parameter of dye, the value of which depends on the concentration of dye and the supramolecular structure of polymer matrix. From PVA dyed by synthesized mono- and disazodyes we obtained the polarizers for UV and visible ranges of the spectrum as well as the broadband polarizer for the range 300…610 nm. Acknowledgement The authors are grateful to Dr. V. Zelenkovskii for assistance in the work to optimize the geometry of dye structure. References 1. J.B. Cnang, J.H. Hwang, S. Jong, The effect of dye structure on the dyeing and optical properties of dichroic dyes for polarizing film // Dyes and pigmentes, 88, р. 366-371 (2011). 2. D.H. Song, H.Y. Yoo, J.P. Kim, Synthesis of stilbene-based azo dyes and application for dichroic materials in poly(vinyl alcohol) polarizing films // Dyes and pigments, 75, р. 727-731 (2007). 3. A. Altomare, F. Ciardelli, M. Marchini, R. Solaro, Polymer dispersions of model azobenzele dyes // Polymer, 46, р. 2086-2096 (2005). 4. B.А. Poraj-Koshitz, Аzodyes. Chemistry, Leningrad, 1972 (in Russian). 5. V.Е. Аgabekov, N.G. Аriko, S.N. Shahab, L.N. Filippovich, P.M. Malashko, The influence of dyes nature and structure of polymer on optical and thermal properties of film polarizers // Dokl. BGYIR, 5, p. 109-118 (2008). 6. S.E. Han, I.S. Hwang, Modeling of the optical anisotropy of a dye polarizer // J. Polymer Sci. Part B. Polymer Physics, 40, р. 1363-1370 (2002). 7. B.T. Kobayashi, Y. Tanizaki, N. Ando, Absorption spectra of dyes. VI. Steric effects in conjugated systems of benzidine disazo dyes and their copper derivatives // Bull. Chem. Soc. Japan, 33, р. 913-917 (1960). Table 1. Sdye and PE for films dyed with disazodyes. The dye concentration is 0.2-0.4 mas.%. The film thickness is 60 μm. Dye� (max, nm� D((� D(� Rd� Sdye� PE, %� � М1� 595� 1.52� 0.15� 10.1� 0.75� 92� � М2� 585� 2.22� 0.50� 4.4� 0.53� 96� � М3� 580� 2.19� 0.26� 8.4� 0.71� 98� � IV� 495� 1.57� 0.40� 3.9� 0.49� 87� � V� 570� 0.80� 0.46� 1.7� 0.19� 61� � VI� 507� 0.62� 0.33� 1.9� 0.23� 33� � Table 2. Order parameter and spectral-polarization characteristics of the films dyed by monoazodyes. The dye concentration is 0.2 to 0.3 mas.%. The film thickness is close to 50…60 µm. Substituent� Cipher of dye� (max, nm� Т(� Т((� D( � D((� Т0, %� Rd � Sdye� PE, %� � � � � %� � � � � � � � R1= COONa, R2 = Н, R3= COONa� VII� 351� 75.6� 2.8� 0.122� 1.553� 39.2� 12.7� 0.80� 93� � R1= COOH, R2 = Н, R3= COOH� VIII� 351� 91.4� 11.5� 0.039� 0.939� 51.4� 24.0� 0.89� 78� � R1= OH, R2 = COONa, R3= CH3-C(O)� IX� 381� 43.0� 1.4� 0.367� 1.854� 22.2� 5.1� 0.58� 94� � R1= OH, R2 = COOH, R3= CH3-C(O)� X� 381� 42.5� 0.5� 0.372� 2.301� 21.5� 6.2� 0.63� 98� � R1= OH, R2 = COONa, R3= CH3-C(O)-NH� XI� 376� 28.6� 0.01� 0.544� 4.000� 14.3� 7.4� 0.68� 99� � R1= OH, R2 = COONa, R3= NaOOC� XII� 380� 78.1� 4.2� 0.107� 1.377� 41.1� 12.9� 0.80� 90� � R1= OH, R2 = COONa, R3= NH2� XIII� 399� 64.7� 0.5� 0.189� 2.301� 32.6� 12.2� 0.79� 99� � R1= OH, R2 = COONa, R3= CH3O-C6H4-C2H2-C(O)� XIV� 386� 51.4� 1.3� 0.289� 1.886� 26.4� 6.5� 0.65� 95� � R1= OH, R2 = COOH, R3= CH3O-C6H4-C2H2-C(O)� XV� 382� 41.7� 0.6� 0.380� 2.222� 21.2� 5.8� 0.61� 97� � © 2013, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 220 _1433772489.unknown _1442414437.unknown _1433772487.unknown