Abstract

Conjugated polymers are promising materials for various cutting-edge technologies, especially for organic conducting materials and in the energy field. In this work, we have synthesized a new conjugated polymer and investigated the effect of distance between bond layers, side-chain functional groups (H, Br, OH, OCH3 and OC2H5) on structural characteristics, phase transition temperature (T), and electrical structure of C13H8OS using Density Functional Theory (DFT). The structural characteristics were determined by the shape, network constant (a, b and c), bond length (C–C, C–H, C–O, C–S, C–Br and O–H), phase transition temperatures, and the total energy (Etot) on a base cell. Our finding shows that the increase of layer thickness (h) of C13H8OS–H has a negligible effect on the transition temperature, while the energy bandgap (Eg) increases from 1.646 eV to 1.675 eV. The calculation of bond length with different side chain groups was carried out for which C13H8OS–H has C–H = 1.09 Å; C13H8OS–Br has C–Br = 1.93 Å; C13H8OS–OH has C–O = 1.36 Å, O–H = 0.78 Å; C13H8OS–OCH3 has C–O = 1.44 Å, O–H =1.10 Å; C13H8OS–OC2H5 has C–O = 1.45 Å, C–C = 1.51Å, C–H = 1.10 Å. The transition temperature (T) for C13H8OS–H was 500 K < T < 562 K; C13H8OS–Br was 442 K < T < 512 K; C13H8OS–OH was 487 K < T < 543 K; C13H8OS–OCH3 was 492 K < T < 558 K; and C13H8OS–OC2H5 was 492 K < T < 572 K. The energy bandgap (Eg) of Br is of Eg = 1.621 eV, the doping of side chain groups H, OH, OCH3, and OC2H5, leads to an increase of Eg from 1.621 eV to 1.646, 1.697, 1.920, and 2.04 eV, respectively.

Highlights

  • Scheme 1 presents the synthetic procedure of the poly (C13 H8 OS–X) where X are H, Br, OH, OCH3 and OC2 H5

  • The results show that at the E = −5 eV the electron density is 29.462%, which shows that in the valence band, the electronic density reaches the maximum value, which proves that poly(C13 H8 OS–H)

  • The results show that the material shape is poly(C13 H8 OS–H) (Figure 4a), with the bandgap

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Summary

Introduction

In recent years, conjugated polymers have been being widely studied and used in science and technology as well as in semiconductor devices [1,2], sensors [3,4,5,6,7,8,9], batteries [10,11], supercapacitors [10,12], electromagnetic shielding materials [13,14], and corrosion-resistant materials [15,16,17,18,19,20] The properties of these materials may be greatly affected by doping/introduction of various substituents groups due to a modification of the electronic density of the molecules. The use of quantum calculations by the ab initio methods at a simple level cannot accurately describe the electronic structure of polypyrrole

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