Open access peer-reviewed chapter

Polymer Architectures for Optical and Photonic Applications

Written By

Ana-Maria Albu and Vlad Marian Târpă

Submitted: July 3rd, 2021 Reviewed: July 29th, 2021 Published: September 28th, 2021

DOI: 10.5772/intechopen.99695

Chapter metrics overview

100 Chapter Downloads

View Full Metrics

Abstract

The last decade of the last century is marked by a revolution in the synthesis of materials for optical and photonic applications, against the background of the growing need for new high-performance materials to increase the efficiency, reliability and speed of response linked to environmental aspects. The diversity of requirements and the optimization of the responses has led to a major dispute over the structure and composition of these materials: Inorganic or Organic, Natural or Synthetic, Hybrid or Pure, which has stimulated interest in the development of various architectures. Special attention shall be paid to establishing a fundamental relationship to correlate the non-linear optical response and chemical structure, especially for the category of organic materials- particularly polymers- distinguished by structural/compositional versatility and suitable for processing by simple technique which allows serial production. In fact, optical nonlinearity (NLO) is not an exotic phenomenon. Indeed, all materials are optically nonlinear if light is sufficiently intense. The synthesis of functional photonic organic materials is a major challenge of contemporary community of material scientists to imagine new functional materials based of “collective” phenomena by virtue of the “engineered” molecule- molecule interactions and spatial relationships. In this context, this paper aims to highlight the most important features concerning the structural - compositional relationship of polymeric materials used in optoelectronic and photonic applications.

Keywords

  • polymer
  • azo-polymer
  • optical material
  • azo-chromophor
  • non linear optics
  • solvatochromic
  • photochromic
  • self anssembly

1. Introduction

Presently, one can remark a continuous increase of the need for new technologies adjusted to the market request. This involves obtaining new high-performance materials and new microelectronic, optical devices, whence appearing these requests. Because we begin will be habitually with these advantages, our expectations demand a higher efficiency, faster and more reliable materials answers, safe environmentally technologies.

Optical nonlinearity (NLO) is not an exotic phenomenon. Indeed, all materials are optically nonlinear if light is sufficiently intense.

The last decade of past century was marked by a revolution in the field of materials synthesis for optical and photonic applications. It is noteworthy major dispute regarding the origin of these materials: inorganic or organic, natural or synthetic, hybrid or pure?

Thus, the fundamental problem in the development of this class of materials still remains the formulation of a theoretical model, which generalizes the particularities of interaction of the stimulating electromagnetic field with the specific micromolecular constituents for each class of compounds.

In this regard, perhaps the greatest challenge is (outside the design synthesis, characterization and understanding of novel molecular and macromolecular assemblies with applicability in non-linear optical fields) the interfacing nature of research, which brings together specialists in chemistry, physics and materials science. Initially, a test stone for chemists, photonics materials require the rational construction of supramolecular assemblies characterized by preordained collective phenomena consequence of intermolecular interactions and their spatial relationships.

It is classic that the high values of the electronic polarization are characteristic for π-conjugated molecules. This justifies the many generalizing predictions that material systems with extended π- conjugation will be characterized by high values of hyperpolarizabilities.

Advertisement

2. Principles of the non-linear optical media

The basic nonlinear optical polarization can be studied at the molecular level. That involves an effort devoted to understanding the relation between the molecular structure and materials properties. Another perspective regards the discussion of the effective arrangement of the nonlinear molecules into macroscopic responses (single crystal, quasi-crystalline thin film, and a polymer matrix, etc.). To describe the nature of nonlinear optical response in materials is necessary to consider the aspects of frequency dependence and symmetry.

A molecular medium, such as an organic crystalline or polymeric solid, is generally non-conducting and non-magnetic and the electrons are regarded as being tightly bound to the nuclei. For such media, the interaction with light can generally be regarded within the framework of a dielectric subjected to an electric field [1, 2, 3].

At molecular level, the interaction of molecule with electric field can be described by the polarizability (p):

p=αE+βE2+γE3+E1

where: α, β, γ are the molecular polarizabilities (1st, 2nd, 3rd order).

The fundamental relationship describing the induced charge in molecular dipole moment (polarization) upon interaction with an oscillating external field (light) can be expressed in a power series:

pi=jαijEj+jkβijkEjEk+jklγijklEjEkEl+;E2

here pi is the electronic polarization induced along the ith molecular axis, Ej is the jth component of the applied electric field, α is the linear polarizability, β is the quadratic hyperpolarizabilitiy and γ is the cubic hyperpolarizability. Starting with the second term of equation are described the nonlinear response to the radiation field and account for terminology “nonlinear optics”. Importantly, the even order tensor, β is responsible for doubling frequency of incident light (second harmonic generation, SHG) and γ describe the third order response of material at molecular level (third harmonic generation, THG).

At macroscopic level, nonlinear optics is concerned with the electric polarization P (dipole moment per unit volume) induced in a material by an electric field E. Typically, P is proportional to E and oscillates at the same frequency. So, the response is linear!As the magnitude of the field increases, P deviates from proportionality and nonlinear phenomena appear:

Pi/ε0=jχij1ijEj+jkχijk2βijkEjEk+jklχij3EjEkEl+E3

χ(n) = electric susceptibilities of order n; linear for n = 1, quadratic: n = 2, cubic: n = 3.

Considering the dual character of light, electric and magnetic:

E=Eω+EΩ=E0cosωt+EΩ,E4

where E(ω) is the optical component of field and E(Ω) is characteristic for external applied field, can be written the mathematical expression of polarization as function of frequency:

Pω=χ1+2χ2EΩ+3χ3EΩ234χ3E02E0cosωt,E5

where: the second term describe the Pockels or linear electrooptic effect (1th order) the third is for the Kerr of quadratic electrooptic effect (2th order), and the last is specifically for optical Kerr effect.

P2ω=12χ2+32χ3EΩE02cos2ωt,E6

where the first terms specifically for second harmonic generation (SHG) and the second describe the electric-field induced SHG (EFISH),

P3ω=32χ3EΩ14χ3E03cos3ωtE=E0cosωt+EΩ,E7

which is specifically equation for third harmonic generation (THG).

Starting from this fundamental description of interaction light-material, without forgetting about the multicomponent structure of materials (different polar species), can be formulate two fundamental aspects for the researchers interested by the synthesis of such materials:

  • The design of this materials suppose an biunivocal interdependence of macroscopic and microscopic optimization;

  • If a microscopic level is very important to enlarge β and γ values, at macroscopic level very important is the effective arrangement of the nonlinear molecules into macroscopical response. So macroscopic susceptibility describe the nature of nonlinear optical response in materials; considering aspects of frequency dependence and symmetry. Generally:

χ2=Nfβ,respectivelyχ3=Nfγ,E8

where N is the number of molecular dipols (polar or polarizable molecules), f is the local field factor.

Synthetic materials of interest in ONL applications are not isotropic. For example:

  • Organic crystals consist of molecules with specific orientations of structuring the constituent motif. Thus, the molecules themselves often have electronic structures with a high degree of anisotropy and consequently, the response of the material to the applied electromagnetic field will not always respect the direction of incidence, as is usual in classical optics.

  • Similarly, in terms of orientation, polymeric chains comply with the principle of minimum energy. If these materials are generally characterized by the random orientation of chains - isotropic structure - depending on the composition, the chains constituting them may be oriented preferentially, so that their energy distribution will require their response to external stimuli.

For this reason, susceptibilities are tensor quantities related to the polarization response in one of the three directions of the field. The material characteristic that reflects the degree of anisotropy is the dielectric constant εij, defined by the electric field and the dielectric displacement, being a second-degree tensor. The birefringence phenomenon is one of the consequences of this dielectric anisotropy. Visualizing a uniaxial crystal with nx = ny + nz, the refractive index of the materials, n, is given as

nεE9

and with a light wave propagating from left to right along the x-axis with its electric field polarized in the z-direction, the propagation constant kz will be determined by nz from:

kz=ωcn2E10

Thus, while all material structures from the point of view of the optical properties, are characterized by the presence of the both hyperpolarizabilities (β, γ), do not display simultaneous second and third order nonlinear response. That is due to the peculiar structural requirement for the two NLO properties. The high concentration of chromophores with large product of the dipole moment, μ, and the first hyper-polarizability, β, stimulate aggregation tendency, diminishing their contribution to the electrooptic effect of materials. The last decade of the 1990s has established that high electro-optical coefficients for guest-host material systems, with polymeric matrix, are essentially due to electrostatic chromophore-chromophore interactions. Thus, when doping the polymer matrices with chromophe species characterized by high electrostatic interactions, there is a decrease of the electro-optical coefficients in the value with an increase of the chromophore concentration. As well, the poling efficiency is limited because a disrouption in alignment of chromophes appears when the polarization field is stoped, owing to the electrostatic interactions and thermal randomization. This behavior is the result of a major relaxation phenomena of chromophors’ in the first moments after stopping the polarization field [4, 5].

The improvement in the value of electro-optical coefficients requires intervention in the composition and structure of the chromophore, without perturbation of of the π-electron structure to avoid changing the molecular hyperpolarizability β. In such cases, the syntheses that favor the perpendicular orientation of constituent segments with distinct polarity (i.e. acceptor, donor) to the chromophore conjugation system, are preferred. Such sterical hidrance limits the distance at which chromophoric molecules can approach each other, thus reducing undesirable dipole–dipole interactions; finally becoming competitive with lithium niobate [6].

2.1 Origin and maximization of molecular hyperpolarizabillities χ(2), χ(3)

Early on, the correlation of the β size value with the permanent dipole moment difference, between the ground and excited electronic state, underlines the dependence of the SHG signal magnitude on the material structure. Although considerable efforts have been made to create new “push-pull” conjugate sequences, that generate a large charge in the excited state, the predicted response values have not always been obtained.

The correlation of the material response with the extension of double/single bonds alternation in the polyene structures served as a model in development of an elegant model for understanding the relationship of the chemical structure-nonlinear optical response. The model is still a useful guide to design the materials with predicted SHG properties, highlighting, as a key element in generating the NLO response, the size of the electronic conjugation at the level of the donor-acceptor substituted chains [7, 8, 9, 10, 11, 12, 13, 14, 15].

Centrosymmetric media are materials with a high density of polarizable electrons, which stimulates the apparition of strong third order NLO phenomena.

Increasing the magnitude of NLO phenomena in polarizable polymers involves either maximizing the intensity of the applied polarization field or designing molecules with intrinsic steric hindrance and an adequate maximization of electronic conjugation at level of the substituted donor-acceptor sequence [16, 17, 18].

As extended conjugation is a key element for third-order NLO materials, several constructive restrictions need to be observed [19]:

  • high molecular symmetry of the material sequences that generate the excited and de-excited states, respectively;

  • involving the high energy excited state in the material response;

  • a large molecular dipole moment variation for transition ground state to excited state.

Theoretical and experimental paper of the field highlights that the best candidates for these applications must be characterized by a high level of extended conjugation to the chain level as well as by strong monophotonic absorptions. Thus, structures similar to polyene compounds are ideal, such as: poly (di)acetylenes, polyarylenes or poly (vinylarylenes) as good as the aromatic structures of chinoids (push-pull). [10, 11, 20, 21, 22, 23].

The length of the conjugate sequences as well as the molecular geometry and the electrical charge of the ground state are the key factors for the type of application of the material.

Advertisement

3. Structural features of NLO polymer materials

In the previously outlined context, the researchers’ attention was focused on studies to generalize the NLO response-chemical structure correlation, while spending efforts on applied research aimed at creating new photonics and photoelectric devices.The variety of physicomechanical properties as well as the compositional versatility of conjugate organic materials placed them at the center of these studies. The π conjugate organic materials with large electronic polarizabilities and, since the nonlinear response is a weighted summation of higher molecular polarizabilities, it becomes reasonable for conjugate molecules to possess substantial hyperpolarizabilities.

3.1 NLO chromophors

The researches activities in the materials fields as well as application development mainly based on multiphoton absorption (MPA) process continue with consistency to demonstrate the successful proof-of-concept in diverse areas, such as microfabrication, bioimaging, photodynamic therapy, frequency upconverted lasing, etc. The mid-1990 is marked by tempestuously development in the design and synthesis of the new dyes, which are more efficient than those commercially available. Consequently, in the coming decades it became evident that these together with theirs processability, photostability, and durability, that depends on the application, are the basic elements for the specificity of physical motif. The great continuous challenge for technological exploration remain how to establish and fine-tune structure-properties relationships for these large numbers of organic, organic–inorganic materials assemblies, taking into account to the varied molecular structural factors preserving the reproducible NLO properties. It was known that molecular hyperpolarizability increases with the π-electron conjugation length of the chromophore. Although it would be expected that the increase in chemical reactivity and optical absorption would be directly proportional to the length of the conjugation at the chromophore level, it has experimentally proved that it is not the best approach to optimize nonlinearity. Theoretical models developed for molecules prone to charge transfer show that the strength and energy balance of donor-acceptor sequences, correlated with the length of the electronic bridge, directly affect the value of molecular hyperpolarization [24, 25, 26]. Thus, by adjusting the strength of the donor and acceptor sequences, the moment of the fundamental state, respectively excited, is directly determined. These peculiarities claim that the increase of the value β is the consequence of the mesomeric interactions of the strong donor-acceptor groups. In conclusion, in the case of organic compounds, the structure-properties relationship is closely related to the strength of the D-A bond, as well as to the widening of the conjugation in the structural unit:

βμeeμggμge2/Ege2,

where: g = ground sate index; e = excited state index; μgg = ground state molecular dipole; μee = excite state molecular dipole; μge = transition state molecular dipole; Ege = transition energy.

Pursuant to this equation, hyperpolarizability is directly determined by the change of the dipole moment and the oscillator power (expressed by the square of the matrix of the dipolar elements) and is inversely proportional to the square of the transition energy. Each of these parameters has a maximum value closely related to the chemical structure of the molecule.The specific function (electronic exchange) which determine the NLO character, as well as the strength D-A, shall decided by the variation of all mentioned factors.This dependence can be found in the dominant β value, approximate by Hückel series for molecular orbitals calculation.

Thus the coulombic energetical difference between donor (αD) and acceptor (αA) can be explained as energetical HOMO-LUMO dissimilarity. The parameters μ2ge and E−2ge show maxima value for the null molecular asymmetry, so: μeeμggαDαA(Figure 1) [8]. Consequently, at increasing of molecular asymmetry αDA > 0, μeegg increase with the difference αDA. Increasing the αDA, the mixing of bridge orbital’s D-A decrease in the same time with transition HOMO-LUMO. At the same time, there is a decrease in the charge transfer character, specific to stilbenic molecules substituted with D -A groups.

Figure 1.

The dependence of μeegg (1), β (2), μge2 (3), and 1/E2ge (4) as function toαDαA.

The D-A molecular structures are limited on the one hand by the coulombic factor (which may have negative, positive or zero values depending on the level of charge separation in the molecule) and on the other hand by the resonance energy, the consequence of the aromatic electrons involved in the conjugate DA.

In addition, the dipolar transition moment show a sinusoidal variation for β with D-A strength while maintaining a consistent bridge of the conjugate bridge (Figure 1). Chromophores that were initially used in the NLO study were of limited success as they failed to reach the required absorption maxima in the near IR wavelength range (Table 1). There is a strong correlation between intramolecular charge transfer processes and NLO response, if discussed in terms of electronic structures and physical processes. Therefore, the design of an ideal chromophore structure with high NLO activity is based on some fundamental aspects at the molecular level. In this idea the intermolecular charge transfer, as a driving force, is necessary but not enough, so it is clear that there must be a high electronic density in the material. On the other hand, another fundamental problem in the operation of NLO materials is the length of the conjugate (i.e., the path length), whit determine the hight and permanent charge separation at molecular level [18, 29, 30, 31, 32, 33, 34, 35].

Table 1.

Most investigated NLO chromophores and their βμ-values [27, 28].

At 1907 nm.

At the outset of reviling the particularities of molecular structures with NLO properties, two general types of organic molecules predisposed for these phenomena are defined (Figure 2) [36]:

  1. The Type I Cromophers have a symmetrical structure and, in general, are made up of an aromatic bridge, rich in electrons, flanked on both sides either by deficit heterocyclic groups or by electronic surplus;

  2. Type II chromophores are asymmetric molecules formed by an aromatic/olefinic bridge, rich in electrons, flanked by an electro-donating group, respectively, electron acceptors.

Figure 2.

Classical molecular structures for NLO chromophors: Ar aromatic block.

Improved solubility required the attachment of pendant alkyl chains to the aromatic sequence. At the same time, the attachment of electron-donor/acceptor groups models the intrinsic electronic density of high molecular weight polymers. The criteria for achieving symmetrical structures (type I (a) and I (b)) are based on the correlation between the large loads of the quadrupole moment during photoexcitation and the cross section. Consequently, molecules characterized by the alternation of vinyl and 1,4-arylene groups as well as the connectors between two identical end groups (i.e., electron- acceptor or donor) are preferred to realise of many NLO chromophores. Such structures are described generically as “push-push” (I (a)) or “pull-pull” (Type I (b)), depending on the direction of intramolecular load transfer: from the end to the centre of the molecule, or vice versa. This model has subsequently gained growing popularity, proving very useful in the design of one-dimensional molecules [29]. The molecular coplanarity is another key parameter in enhancing the intramolecular charge transfer efficiency [37]. At the same time, for organic molecules, the strength of dipole in the ground- state of nonsymmetric molecules as well as the multipolar transition-dipole strength in the centrosimetric molecules are also energy factors that determine the NLO response magnitude [29, 38, 39]. Both experimental and theoretical, it has been demonstrated that the multiplication of the number of conjugation path or the connection of more than one linear path to generate two- or three-dimensional configurations, leads, in the material, to a major increase of the NLO responses value [31, 32, 38, 40].

Remarkable is the fact that when assessing the properties of NLOs, the energy changes caused by the interaction with the environment should not be neglected [41]. Thus, the polarity of the solvent, expressed by its dielectric constant, is an important structuring parameter determining on the one hand solvation by hydrogen bonds or by promoting colloidal-microaggregate dissolution. Thus, the efficiency of the cross section is more sensitive to the polarity of the local environment than to the intrinsic NLO aspects (properties) of the material [42].

3.2 Functionalized polymer materials systems

The NLO polymeric films are usually composed of long chains with chromophore sequences. Thus, chromophores, which are seen as net dipoles, are the origin of optical non-linearity in polymers. The interaction between the ‘non-polar’ molecules from bulk material and the chromophore, the molecular orientation (either random or of a certain symmetry) can introduce an overall orientation of the molecular assembly. This orientation will tend to cancel the individual molecular contributions. It is therefore important to ensure that all molecules are aligned correctly. The first information on this issue can be obtained by analyzing the chromophe sequence.

The starting point in developing technical strategies for the real NLO polymers synthesis is both the design of the assembly at the molecular level and the design and characterization of chromophe molecules with high molecular hyperpolarizabilities (β, γ), able to be, easily and efficiently, incorporated in a polymeric matrix.

The generous literature information, both experimental and theoretical, on the use of organic materials (especially polymers) in NLO applications is based on the composition-properties relationship. A particularly important aspect relates, in addition to practical assembly techniques, to their composition, synthesis and characterization. Therefore, for polymerist researchers, it becomes defining the aspects of the synthesis and reactivity of the monomers bearing NLO sequences as well as the establishment of techniques for incorporating these NLO sequences into the global polymeric architecture.

A particular aspect in the synthesis of NLO polymers, beyond optimization of the individual response of the constituent chromophore, is how the chromophore density can be maximized while preserving micro- and supra-structuring properties, respectively. The experimental studies, developed in this context, outlined two alternative strategies (Figure 3):

  1. A first alternative is offered by the chemical modification of preformed macromolecular chains with chromophore sequences suitable for the desired application. This path offers the advantage of using chains with dimensions useful to the target application. The method is limited to relatively low degrees of transformation, does not provide a rigorous control of the distribution of the attached chromophore and last but not least, involves a series of purifications subsequent to the synthesis, in order to remove the unreacted chromophore.

  2. However, a macromolecular structure with a predefined architecture can be easily obtained by (co) polymerization of monomers carrying an electrooptically active sequence. The major advantage of this method is the rigorous control of the chromophore fraction in the macromolecular structure both as a weight and as a sequential distribution. The only restriction imposed concerns the intrinsic structure and purity of the monomers which should not impede the (co) polymerization process.

Figure 3.

Design Motifs of NLO polymers materials.

Based on theoretical prediction and quantum the most promising macromolecular materials were, initially, the electron -conductive polymers such polyacetylenes, polythiophene or poly(p-vinyl phenylene)‘s. Few research groups underlined that the lengths of conjugate sequences is not a necessary preconditions for increasing the intern polarity value (implicit χ(2), χ(3)). Therefore the oligomers segments can be understood as inactive spacer with broaden the NLO activity, simultaneous facilitate the processability of materials [43, 44, 45]. Moreover, the susceptibility tensor calculus, with theory the disturbing torque- Hertree-Fock, for polyene series C22H24, underline the dependence γxxxx ≈ L4; (L chain length) [45]. Afterwards were demonstrate that γxxxx ≈ L4,6 ± 0,22 [46].

For poly (p-vinyl phenylene), the predictions of the value rapport γ/N, pointing out a decreasing with increasing N(dipols number). In this context, it is outlined the idea that the best polymeric structures are those consisting of conjugated oligomeric segments, connected with spacers with or without NLO activity (Figure 4) [22, 47].

Figure 4.

The structural scheme proposed for NLO copolymers: A = segments with low NLO activity; B = oligomers segments with high NLO activity; G = functional groups [22].

Through processing limitations (low solubility in the usual solvents) the researcher works were directed towards finding a new modality for including these sequences in polymer structure. So, the ladder hyperconjugate moieties thiophene oligomers and/or polyamide/imide were attached to the polyenic skeletons. Such materials were characterized by high values of hyperpolarizabillity, 10−11÷10−12 esu/cm.

The copolyamides structures with polyvinylthiophene, obtained by interfacial polymerization (Mn = 105), were characterized by thermal resistance until 400°C. The electro-optical analysis of these films denotes the existence of conjugate phase which generated χ(3)/α ∼ 10−3 esu/cm. This technique offers the possibility to tune the NLO activity by the number of the electrooptic segments of different species [48, 49].

The similarity of poly(urea)s properties with NLO “piezoelectrical polymers” (poly(vinyl fluorine), poly(vinyl triflourine), copolymers of the triflourine ethylene and tetra- fluorine ethylene, nylon, vinyl cyanide entitle their NLO activity. The strong interchains bond (hydrogen bonds) rule the dipoles alignment in the electric field, [50].

The d33 coefficients evolution highlight a very slow relaxation, emphasize the lead of hydrogen bond for maintaining the NLO properties of the material. Starting with these conclusions great efforts were dedicated to investigation of the polymer structures showed in the Figure 5 [51]. The NLO properties are due to the junction of the donating electrons (2) with the π electrons system. The flexible chain (σ bonds (3) (Figure 5) play an important role regarding the solubility, transparence and fusibility of the polymers.

Figure 5.

Macromolecular materials structure used for waveguide fabrication.

The constitutive- compositional similitude with polyureeas and the peculiar features: (i) the easy chromophores alignment for each synthesis step, the relative low viscosity; (ii) the high rate of polymerization (few seconds to several minutes) –reaction izocianate/alcohol; stabilization of NLO response by the hydrogen bonds, characteristics for polyurethanes; justifying the investigations of NLO polyurethane comportment [52, 53, 54]. The study of stability discloses in this case the importance of simultaneous development of polymerization and poling. So, by this procedure were diminished the phenomena of loss of property to reorientation (keeping 40–60% of the initial value) [54].

The contribution of π-electron sequence, their length, is not crucial for increasing the hyperporarizability value (specially χ(3)). In this case significant is the sequence planarity. On the other hand, the symmetrical substitution, broadening results the enlargement of the transition bands fromHOMO-1 to HOMO and similarly from LUMO to LUMO-1. These transitions promote the third order susceptibility, theoretical prevue by relation showed in the Figure 6.

Figure 6.

Representation of the two excited states which contribute to the γ value:E: energy of band gapes; P: transition dipole moment; for conversion the three electronic states are denoted as: 0 = G(1Ag); 1 = 1Bu; 2 = 2Ag [51].

A special attention was granted to the epoxy macromolecular structures. These investigations are supported by the potential stabilization of the chromophore, by its covalent binding to the carrier matrix [55, 56, 57]. Another very important aspect, especially if the polymer precursor has a high reactivity, was giving rise to the crosslinked structures. The major advantage, in these cases, is using an amine chromophore monomer. So, the dipoles chromophores alignment is accomplished by crosslinking control simultaneous with polymerization process. A wide range are getting the epoxydic compounds, which is a gain for the electrooptics coefficients (10–50 pm/V) [58, 59, 60, 61, 62, 63].

Also of interest for the NLO has proved to be polysiloxane structures (Figure 7). This orientation is justified by their versatility, ability to form the films, very useful for monolayers deposition (Lagmuir-Blodgett) and the possibility of obtaining the self- stabilized dipolar structures [64, 65, 66]. The assessment of the SHG value, for all monolayers, highlights a significant increase while increasing the substituant polarity. This suggests that the package of each polymer chain in the monolayer is orderly, and the interchain bonds are essential in achieving the non-centrosymmetric structure.

Figure 7.

General structure of polyorganosiloxanes for NLO applications: R”, m = 6 ± 2; n = 8 ± 2 (R and R’ are hydrogen’s atoms) [65].

Perhaps the most investigated NLO material class is azobenzene derivatives, known and studied for a very long time, their initial use being dye for a variety of substrates. Azobenzenes Photoisomerization is a well-known phenomenon, dedicated to reference materials [67, 68].

The key to exploiting the unique behavior of the azobenzene sequence is defined by how it can be included in the functional materials. For the generation of new properties, the most effective method of incorporation of azobenzene is the covalent attachment to polymers. The materials thus obtained will show both properties specific to polymers: inherent stability, rigidity and processability as well as conformational change under the action of electromagnetic radiation, specific to azo segments - photoisomerization processes. The covalent incorporation of the azo sequence in the polymer, through its photoisomerization process can generate a wide range of phenomena, even unexpected ones [69].

About 25 years ago, at dispersing of azobenzene groups in the polymer matrix, the unique phenomenon recorded was associated with their photoisomerization [70].

Under the action of polarized laser radiation, in polymer films with azobenzene sequence, their orientation is perpendicular to the polarization direction. Dichroic phenomena are thus generated.

This type of phenomenon is reported in the years ‘80 in liquid crystal polymers with photoactive azobenzene mesogenic sequences [71, 72]. Simultaneously, in Japan, the “command surfaces”concept [73] is opened, in which the azobenzene group acts as ‘commander’ and the Langmuir — Blodgett liquid films play as ‘soldiers’, which are aligned in trans/cis conformations by azoderivatives —the switching initiated by illumination [69]. After 1991, the applicative exploitation of these phenomena expanded worldwide, highlighting interesting and unexpected phenomena, which diversify use in reversible optical memory applications as well as photonic applications. Over the last 40 years, an exponential development of the domain has been observed and there is still no analysis covering all these new implications of azobenzene photoisomerization in polymeric structures. Remarkable and still of real interest remain the reviews which treat, generally or in a specific way, phenomena generated by the presence of azoderived sequences [74, 75, 76, 77, 78]. However, the best available analysis covering both photoinduced birefringence and surface relief grating dates back to 2000 [79].

The special interest in azobenzene polymers is the result of their particular properties, which are useful in the processing and storage of optical information [69, 80, 81, 82]. The sin-anti conformational conversion process at the bond N = N, presumes some distinct transformations, highlighted in Figure 8a): (i) decoupling of the π electrons from the double bond, (ii) rotation around the single bond N-N followed by (iii) restoring the double bond, N=N, in a new configuration. Assisted by the adequate wavelength radiation, this phenomenon is governed by electronic transitions π-π*, respectively n-π [23].

Figure 8.

Conformational changes in azobenzene: (a) A: Rotation of substitutes around–N = N- bond; B: Inversion of substitutes; (b) the azobenzene - light interaction.

The molecular photoorientation of chromophe sequences is governed by anisotropic absorption, so that under the action of incident radiation, the dipole moment of chromophe sequence aligns along the molecular axis (Figure 8b). The linear polarized light is capable to induce a centro-symmetrical orientation in which the azoic sequence is directed perpendicular to the light plane. These oriental oscillations of the dipole moment’s are transferred to the macro-scopical level, stimulating the emergence of optical dicroism and birefringence.

Therefore, the energy metastability of the sin-isomer plays a decisive role in both the theoretical interpretation and the practical application of the photoinduced phenomena in azoic polymers. For example, applications that rely on the modulation of the molecular alignment of CL will use materials with high stability of the sin-isomer (holography, optical data storage) while operational devices based on optical birefringence and dicroism phenomena will only use structures with rapid reversion of the sin-isomer.

The Red Dispers-based materials are the most representative in the class of polymers with the azobenzene side-chain NLO sequence [83, 84, 85, 86, 87]. Although noted by good temporal stability of the orientation (preserving about 80–90% of the maximum property value at 1000 hours after orientation) and, in addition, they admit a wide range of refractive index values from UV exposure, a still ongoing problem remains the stabilization of their orientation through photo crosslinking [88].

As the free radical mechanism is easily accessible, an informational richness covers the synthesis, characterization and use of (meta)acrylic and styrenic (co)polymers, with side-chain azo sequence (Figure 9) [74, 88, 89, 90, 91, 92, 93, 94, 95, 96, 97, 98].

Figure 9.

Structures for methacrylate and styrene materials for NLO applications: a) R = CN; NO2; N(CH3)2; OCH3, CH3; X = alkyl; Chemical modifications of polystyrene and/or chloromethylestyrene; c) synthesis of NLO styrene monomer structure.

The versatility and easily processing of methacrylic polymers recommend these for NLO applications. The new monomers structures are investigated for chemical reactivity in the (co)polymerization [99, 100, 101] as well their electrooptic characterization [102, 103, 104, 105]. These research points the inclusion of these cromogene sequences in copolymer structures without major difficulties. A peculiarity of these monomers is their predisposition to an hight chain transfer, which involves the design of syntheses in compositional-operational conditions so as not to drastically reduce the degree of polymerization. In addition, the presence of coloured monomers leads an increase in the rate of polymerization, the phenomenon of self-acceleration becoming obvious. The sequential distribution confirms the predictions obtained from the capitalization of the reactivity ratios and at the same time, the characterization of the material proves the preservation of the optical characteristics of the chromophore.

The styrene materials are preferred relative to methacrylic materials. They are so much easier obtained by chemical modifications (Figure 9b): usually is used one of the vinyl benzyle chloride isomers. The drawback of these polymers is the relative rigidity of the chromogen sequence due to the aromatic spacer. The major advantage for these SC structures is the decupling of the chromogene, which facilitates the molecular dipole orientation; but the poling-induced order in organic/polymeric materials is thermodynamic unstable. Thus, an important objective for the NLO polymer synthesis is the structural induction of slow relaxation in the acquired polarization orientation.

A promising alternative is azobenzene SC liquid crystalline polyester architecture [106, 107]. These, by their own nature, extend flexibility at the base-catene level by interactions with both acid and glycolic sequences that can serve as the link sequence of the mesogene. Thus, by modular construction, can be adjusted the length of the flexible methylene spacer in the lateral chain, the substitute on the azobenzoic fragment, the length of the methylene sequence in the main chain (all aliphatic) and the molecular weight of the polyester. Moreover, each parameter obtained by the versatility of the esthetically bond significantly influences the optical storage behaviour of the materials [108]. All materials (with a wide range of substitutes: cyano, nitro, methoxy, hydrogen, methyl, n-butyl, phenyl, fluorine, trifluoromethyl, chlorine, brom) have a diffraction efficiency of over 50%, giving these materials great diffraction properties. The stored information on azo copolymer media (75–100% azo- dye content) can be partially erased up to 80°C [109].

The copolymers of maleamic monomers with styrene and vinyl benzyl chloride and theirs preliminary characterizations of these materials proves that these monomers can be used for build NLO materials [110, 111, 112].

A critical issue of materials used in applications based on NLO properties is their thermal stability. This shortcoming can be addressed by promoting (after polarization) cross-linked structures, in particular by photochemical processes. Preferred for this direction are aromatic polyimides (PIm), attached to the polymer frame. The chromophore can be ‘grafted’ onto PIm sequence through transformation reactions. The method is advantageous because it allows the attachment of a different range of chromophores to polymer supports with a wide compositional variety, promoting the production of materials with high Tg (around 220°C), excellent solubility and processability. In addition, the topological stiffness, induced by the aromatic sequence, results in the preservation of high values of electro-optical coefficients during long periods of use [113]. In this way, by coupling reaction, was synthesized the poly(phenylene- imide thiophene) materials (PPIT) (Figure 10) [114]. They showed high Tg and consequently high temporal stability of the SHG, as demonstrated by dynamic signal decay behaviour studies that attest their stability at temperatures up to 150°C, preserved more than 82% of the SHG signal after 1500 h of operation.

Figure 10.

Structure of new poly(phenyleneimide) (50.85% chromophores, Tg = 170°C; Td = 245°C, Φ = 23; r33 = 35 pm/V).

An elegant and efficient method of synthesis of PImss functionalized with second-order NLO, is the one-step synthesis (Figure 11) [115], which allows the use of the most popular electron-acceptor moieties. This give the materials with Tg values in the range 205–224°C [113, 116, 117, 118, 119], whose thin films, corona-poled and SHG analyzed, are characterized by enhanced d33 value (30 pm / V at λ = 1064 nm). The study of the preservation of SHG properties under thermal stress – as a function of annealing time at 125°C - reveals that the NLO response, after 9–20% initial decrease, does not change significantly over a period of 210 h for polymers: (PIc-e). (PIc), (PId) and (PIe), with better stability than PIb at 125° C, retaining about 70% of the NLO properties (Figure 11).

Figure 11.

Poly(imide)s containing NLO chromophores based on 2-(5, 5-dimethyl-cyclohex-2-enylidene)-malonitrile and conventional chromophores.

Step-by-step polyaddition reactions is another tool for synthesis of thermally stable, second-order NLO chromophore PIms and poly (urea), starting from 2,3-bis (4-aminophenyl) -5,6-dicyanopyrazine (BAPDCP), who’s the first order molecular hyperpolarizability, β, was evaluated as 123.5 × 10–30 esu [120].

Using a new polymerization methodology, were produced the high Tg polymers [121] introducing into polymer backbone an imide–siloxane linkage containing NLO-active chromophores. As expected, introduction of dimethylsiloxane linkages in the backbone led to enhanced solubility and thermal stability of the functionalized PIms while retaining their useful physical characteristics, such as Tg: These polymers show SHG efficiencies comparable to those for functionalized PIms or polyurethanes and exhibit high temporal stability of resultant SHG signals.

Poly (maleimide) polymers functionalized with aminoalkyl sequences have a transition temperature in the range of 178–228° C, as well as a stable NLO response at high temperatures: such systems lose 24% of their property after 1000 hours at 125° C. The value d33 of SHG coefficient, 64.0 pm/V measured at 1064 nm, suggests that these polymers could be useful for NLO-applications [122].

The synthesis of polymers with electro-optical characteristics by sequential self-repetitive reaction (SSRR) [123] offers the possibility of making poly (amide-imide) structures. The promotion, in this case, of the reaction between dysfunctional azo chromophores (DR19, NDPD, DNDA), with an excess of 4,4-methylene-diphenylisocyanate (MDI), ends with the formation of a carbamic structure, useful for obtaining poly (carbamate diphenylisocyanate) (poly CDI- Figure 12). Subsequent addition of trimellitic anhydride (TMA) to the poly-CDI solution leads to the poly (N-acylurea) intermediate, characterized by good solubility. The in-situ poling and curing process, of this reactive mixture, favors the formation of the amide-imide structure of the N-acylurea sequence. The correlation of the thermal behaviour with the electro-optical characteristics, for these polymers, highlights values of r33, in the range of 5.2–25.2 pm / V at 830 nm. There is also a proportionality of these values with the chromophore concentration. Such structures are characterized by good thermal stability- (80°C and optical waveguide losses (3.8–6.6 dB/cm at 830 nm) [124], which argues that when using the SSRR technique, the values of the EO coefficients are the consequence of the orientation of the chromophores on the polarization direction before lattice hardening.

Figure 12.

Poly(amide-imide)s NLO polymers structures obtained by SSRR.

Carbazole and its derivatives remain in the attention of chemists, mainly due to the fact that the carbazole skeleton has proven to be a versatile platform for the development of materials with applications in specialized fields such as optics, thermoelectronics as well as medical and pharmaceutical applications.

Belonging to a very interesting and relatively new class of material-conjugated polymers, carbazole and its derivatives are manly characterized by the existence of π-mobile electrons, which can be used as chromophores, respectively electrophores [125]. The size of the energy difference between the conduction band and valence band, customizes the wavelength of absorption and / or radiative emissions, configuring the conduction capacity. What differentiates conductive polymers, expressly carbazoles, in the vast class of polymeric materials (known as true insulators) is their ability to carry electrical charges. This behaviour brings them closer to the electrical conductors - metallic or semiconductor.

Such materials are used both in the field of powerful light transmitters for sensors or as active components in electronic (opto) devices and batteries [126, 127, 128, 129].

The main advantages of carbazole compounds are related to the economical, processability and their properties, particularly regarding few aspects:

  • a cheap raw material readily available from coal–tar distillation, furthermore a large category is retrieved in the plants

  • Different substituents can be easily introduced into the carbazole ring the presence of the nitrogen atom in the centre of symmetry, facilitates functionalization with various substituents. Consequently, the properties of the material can be modulated without potentiating the steric interactions with the basic carbazole backbone (Figure 13).

  • The aromatic configuration gives them high thermal and photochemical stability as well as relatively high mobility of charge carriers;

  • Carbazolyl groups easily forms relatively stable radical cations (holes).

Figure 13.

Carbazole structures: reactive positions correlated with material structure and its particular properties.

Due to the mentioned advantages, a wide range of materials for transporting holes [130, 131], molecular glasses [132, 133, 134, 135] or light-emitting materials [136, 137, 138, 139, 140] have been designed with carbazole. Favourable to the synthesis of different dyes architectures (push-pull dyes; push-push or pull-pull), through substitution reactions to aromatic nuclei, carbazole was and remains an excellent candidate for the design of light harvesting materials for solar cells and numerous dyes with large and wide molar extinction coefficients the absorption spectra were obtained with this plan electron donor [141, 142].

Carbazole derivatives are intensely studied because of their well-known potential as precursors of materials for optical/ optoelectronic applications. The characteristics that recommend them for use are their special photorefractive, electrical, and chemical properties. Carbazoles are well known as a conjugated, good hole-transporting, electron-donor, planar compound and ease to introduce solubilizing groups to rigid ring structure. Carbazole can polymerize and couple in positions 3, 6, 9 and 1, 8 respectively. However, due to the very rigid structure of the carbazole, the last pair of positions is sterically hindered [143, 144]. The very high reactivity of positions 3, 6, favors the rapid synthesis of carbazole derivatives starting from 9H-carbazole, by direct bromination of the carbazole group with N-Bromo succinimide (NBS) [145].

In the context of the progress of new techniques for the manufacture of intelligent devices, the constructive versatility of the carbazole sequence, stimulated the development of design new dyes classes with photoinitiation activity in UV, near-UV or visible light, very useful in the development of 3D printing [146].

Substitution reactions at the carbazole unit can generate poly (3,6-carbazole) and poly (2,7-carbazole), respectively. These structures, due to the effective difference in the length of the conjugate sequence ((2, 7) is the longest, being similar to polyp phenylenes) have different properties and potential applications. In addition, using specialized modification strategies, the properties of both polycarbazole classes can be improved / fine-tuned, thus diversifying high-performance applications in the electronic and electro-optical field, such as polymeric light emitting diodes (PLEDs), organic field-effect transistors (OFETs), and photovoltaic cells (PCs). For both categories of polycarbazoles, an elegant and very complete presentation of the structure-properties-application correlation is summarized in several reviews, among which we recommend [147, 148, 149].

From this multitude of papers, the authors summarize studies dealing with novel aspects in poly (3,6-carbazole) synthesis, particular aspects of the photoactive properties of polyvinyl carbazole copolymers, as well as other derivatives with polymerizable group in position 9 of carbazole, adjacent to the poly (2,7 carbazole) derivatives, strongly predisposed for optoelectronic applications such: organic LED, photovoltaic cells and biosensors.

Thus, the first decades of the 21st century are distinguished by the extension of studies dedicated to the synthesis and characterization of new optically active photochromic polymeric structures, with two distinct functional sequences: azo and a chiral group [150, 151, 152, 153]. The simultaneous presence of these functions, sensitive to electromagnetic stimuli, creates the premises to display both the typical properties of asymmetric systems (optical activity, exciton division of dichroic absorption) and the typical characteristics of photochromic materials (photo refractivity, photo reactivity, N properties). In this context, it seemed interesting to investigate the properties of new multifunctional copolymer materials containing both photo responsive azobenzene and the photoconductive carbazole chromophore directly bound to the polymeric side chain through the chiral fragment: the presence of the electron-rich carbazole sequence as partner of the electron-poor azobenzene chromophores can induce charge transfer interactions fundamental in the operation of photoconductive materials [154].

The literature highlights the appearance of charge transfer interactions in achiral copolymers of N-vinyl carbazole (NVK) with methacrylic azoderivatives, the intensity of which is stimulated by the alternation of monomer sequences [155, 156, 157, 158, 159].

Due to their complexity of structural behaviour, they are able to generate sophisticated synthetic architectures, with high sensitivity and selectivity, which expands the application range. By consequence, they may be adopted special applicative functions, such: with molecules and ions they can be utilized in different separation and purification techniques; by interactions with the electromagnetic stimulus in solar cells fabrication, organic light emitents and optical elements, by specifical interaction with the biological sequences they developed applications in anti-biofouling or specific binding proteins, by specifical interactions in adhesive assemblies, they can generated bonding-disbonding phenomena’s, by peculiarity of theirs response to the stimulus action they can behave as self-healing agent for other different materials, by interactions between different polymer’s sequences can be achieved a multi-layered polymer materials with different functionalities in applications: screen printing, stamping ink-jet-as commercial used technology or optical waveguide, elastomeric light-emitting devices and displays or molecularly stretchable electronics- as specialized technologies.

Advertisement

4. Conclusions

Exhausting analyzing of the bibliographic information of the NLO materials shows great promise of polymer for device applications in the communications and photonics industries. Usually, these were use as host for chromophore structures as well as statistical (co)polymers, which include the NLO sequence in the macromolecular assembly.

At present there are a large number of NLO applications that use inorganic crystals. A few of these processes include optical switches, EO modulators, optical data storage, and optical fiber-based devices. The study of organic NLO chromophore-doped polymers would allow them to replace their inorganic counterparts. It should be clear to the reader that chromophore design has progressed significantly due to new classes of heterocyclic moieties used to optimize chromophore properties. However, with such novel designs, considerable research is required to achieve highly improved EO activities.

NLO chromophore functionalized polymers (obtained by polymerization or chemical transformation method) were found to be more effective because chromophore mobility is hindered by its attachment to the polymer. Functionalized SC NLO polymer systems with high and stable NLO effects, i.e. χ(2) and χ(3) were synthesized. The rigid aromatic backbone approach was found to be promising for making highly stable NLO polymeric systems. Polymers with rigid polymer backbone exhibiting high Tg values were found to suppress reorientation significantly. Theirs exhibiting high thermal stability in dipole orientation, relatively high optical nonlinearity and low optical loss are very promising for practical applications as has been reported.

Few work directions were showed for synthesis of the new stable NLO organic materials:

  • Copolymerization provides a general approach to the enhancement of the thermal stability and the NLO stability of the materials within a tolerable trade-off range in optical nonlinearity. Introduction of an imide– siloxane linkage into polymer backbone containing NLO-active chromophores led to enhanced solubility and thermal stability, high glass transition temperatures and exhibit high temporal stabilities of the resultant SHG signals.

  • Another strategy for stable polymeric systems is crosslinking technique. Extensive research on this topic for the past few years has shown that the NLO stability is profoundly enhanced by crosslinking the MC.

  • More recently, functional dendrimers have been proposed to prepare multi-chromophore material systems that possess unique molecular architecture and characteristics. It is noticeable that a polymer host is not required for certain dendrite materials because they have unique film forming properties due partly to the reasonably high molecular weight and partly to the polymeric character inherent in these molecules. These dendrimer properties allow an appropriate solution viscosity when mixed with traditional spin-casting solvents to create amorphous glassy films. Those demonstrate dramatic enhancements in poling efficiency due to larger free volume and reduced dipolar interactions allowing diminished mobility constraints in comparison to the tethered polymer systems.

  • Finally, it should be pointed out that our aim was to underline the main aspects regarding the relation structure- material properties and for that is practically impossible to mention here all investigations. What is not understood for real materials is how medium and chromophore-chromophore interactions modify/can be used to tune, the response of the individual chromophore molecules.

References

  1. 1. Armstrong, J. A., Bloembergen, N., Ducuing, J.; Pershan, P. S, (1962), Interactions between light waves in a nonlinear dielectric, Phys. Rev., 127, 6, 1918-1939. DOI: 10.1103/PhysRev.127.1918
  2. 2. Hurst, M.; Munn, R.W., (1986), Theory of Molecular Opto-Electronics. I. Macroscopic and microscopic response, J. Molec. Electron., 2, 35-41. DOI: 10.1007/978-1-4615-3818-9_20
  3. 3. Boyd, R. W., Nonlinear Optics, Academic Press, San Diego, 1992. DOI: 10.1016/B978-0-444-89304-8.50010-9
  4. 4. Chen, A., Chuyanov, V., Zhang, H., Garner, S., Steier, W. H., Chen, J., Zhu, J., He, M., Mao, S. S. H., & Dalton, L. R., (1998), Low-Vπ electro-optic modulator with a high-μβ chromophore and a constant-biasfield, Opt. Lett., 23, 6, pp. 478-80, ISSN: 0146-9592. DOI: 10.1364/OL.23.000478
  5. 5. Chen, A., Chuyanov, V., Zhang, H., Garner, S., Lee, S.-S, Steier, W. H., Chen, J. Zhu, J., Wang, F., He, M., Ra, Y., Mao, S. Dalton, L. R &Fetterman, H. R., (1998), Low-Vπ high-thermal-stabilityelectro-optic polymer waveguidemodulatorsusingthe full potenetial of high-μβ chromophoreswith a DC biasvoltage, Polymer PhotonicDevices, USA Conference, 28 January 1998, Proc. SPIE 3281, San Jose, CA, Kippelen, B, Bradley D. D. C., Eds, pp. 94-105. The International Society for Optical Engineering. ISSN (printed): 0277-786X. ISSN (electronic): 1996-756X. DOI: 10.1117/12.305409
  6. 6. Dalton, L., Harper, A., Ren, A., Wang, F., Todorova, G., Chen, J., Zhang, C. & Lee, M., (1999), PolymericElectro-optic Modulators: FromChromophore Design toIntegrationwith Semiconductor VeryLarge Scale Integration Electronics and Silica FiberOptics, Ind. Eng. Chem. Res., 38, 1, pp.8-33. DOI: 10.1021/ie9705970
  7. 7. Marder, S. R.; Beratan, D. N.; Tiemann, B. G.; Cheng, L.T.; Tam, W., (1991), Organometallic Materials with Second-order Optical Non-linearities, in Organic Materials for Non-Linear Optics II, Volume 91 of Special publication - Royal Society of Chemistry (Great Britai. Hannand R. A &Bloor D., GhrahamHouse ed., Cambridge, pp. 165-176, ISBN 0851863973, 9780851863979. DOI: 10.1021/bk-1991-0455
  8. 8. Marder, S. R., Beratan, D. N., &Cheng, L.-T., (1991), Approaches for OptimizingtheFirst Electronic Hyperpolarizability of Conjugated Organic Molecules, Science, 252, 5002, pp. 103-106. ISSN: 0036-8075. DOI: 10.1126/science.252.5002.103
  9. 9. Marder, S. R., Gorman, C. B., Tiemann, B. G. &Cheng, L.-T., (1993), Stronger acceptors can diminish nonlinear optical response in simple donor-acceptor polyenes, J. Am. Chem. Soc. 115, 7, pp. 3006-3007. ISSN: 0002-7863. DOI: 10.1021/ja00060a071
  10. 10. Marder, S. R., Perry, J. W., Bourhill, G., Gorman, C. B., Tiemann, B. G., & Mansour, K. (1993), RelationBetween Bond-LengthAlternation and Second Electronic Hyperpolarizability of Conjugated Organic Molecules, Science, 261, 5118, pp. 186-189, ISSN 0036-8075. DOI: 10.1126/science.261.5118.186
  11. 11. Marder, S. R. & Perry, J. W., (1993), Direct observation of reduced bond-lengthalternation in donor/acceptor polyenes, J. Ame. Chem. Soc., 115, 6, pp. 2524-2526. ISSN: 0002-7863. DOI: 10.1021/ja00059a067
  12. 12. Marder, S. R., Gorman, C. B., Meyers, F., Perry, J. W., Bourhill, G., Bredas, J. L., Pierce, B. M., (1994), A Unified Description of Linear and Nonlinear Polarization in Organic Polymethine Dyes, Science, 265, 51720, pp. 632-635. ISSN: 0036-8075.DOI: 10.1126/science.265.5172.632
  13. 13. Meyers, F., Marder, S. R., Pierce, B M., &Bredas, J. L., (1994), Electric Field Modulated Nonlinear Optical Properties of Donor-Acceptor Polyenes: Sum-Over-States Investigation of the Relationship between Molecular Polarizabilities (α, β and γ) and Bond Length Alternation, J. Am. Chem. Soc., 116, pp 10703–10714, ISSN: 0002-7863. DOI: 10.1021/ja00102a040
  14. 14. Meyers, F., Marder, S. R., Pierce, B M., &Bredas, J. L., (1994), Tuning of large second hyperpolarizabilities in organic conjugated compounds, Chem. Phys. Lett., 228, 1-3, pp. 171-176, ISSN: 0009-2614. DOI: 10.1016/0009-2614(94)00905-8
  15. 15. Risser, S. M., Beratan, D. N. &Marder, S. R., (1993), Structure-functionrelationships for beta., thefirst molecular hyperpolarizability, J. Am. Chem. Soc., 115, 17, pp. 7719–7728. ISSN: 0002-7863. DOI: 10.1021/ja00070a016
  16. 16. Haller, M., Luo, J., Li, H., Kim, T. D., Liao, Y., Robinson, B. H., et al. (2004), A novel lattice-hardening process to achieve highly efficient and thermally stable nonlinear optical polymers, Macromolecules, 37, 3, pp. 688–690, ISSN: 0024-9297. DOI: 10.1021/ma035393b
  17. 17. Hambir, S. A., Wolfe, D., Blanchardand, G. J. & Baker, G. L., (1997), Adjusting the Third-Order Nonlinear Optical Properties of a Conjugated Polymer Film, J. Am. Chem. Soc., 119, 31, pp 7367–7373, ISSN: 0002-7863. DOI: 10.1021/ja9705194
  18. 18. Marder, S. R.; Torruellas, W. E.; Blanchard-Desce, M.; Ricci, V.; Stegeman, G. I.; Gilmour, S.; Bredas, J. L.; Li, J.; Bublitz, G. U. & Boxer, S. G., (1997), Large Molecular Third-Order Optical Nonlinearities in Polarized Carotenoids Science, 276, 5316, pp. 1233-1236, ISSN 0036-8075 DOI: 10.1126/science.276.5316.1233
  19. 19. Bredas, J. L., Adant, C., Tackx, P. & Persoon, A., (1994), Third-Order Nonlinear Optical Response in Organic Materials: Theoretical and Experimental Aspects, Chem. Rev., 94, 1, pp. 243–278, ISSN: 0009-2665. DOI: 10.1021/cr00025a008
  20. 20. Esser A., Fich, H.; Hadicke, K. H., Paust, J., Schrof, W.&Ticktin, A., (1992), Wavelength Dependent χ(3) Measurements of Long Chain Carotenoid Derivates, in Organic Materials for Non-Linear Optics III, Volume 137 of Special publication - Royal Society of Chemistry (Great Britain), Ashwell G. J., Bloor D., Ed., Thomas, GhrahamHouse ed., Cambridge, p. 213-217, ISBN: 0851866255, 9780851866253
  21. 21. Nickel, E. G.; Spanker, C. W.; Tang, N.; Hellwarth, R. & Dalton, L. R., (1993), Composites Containing Stabilized Bipolarons in Organic Materials for Non-Linear Optics III, Volume 137 of Special publication - Royal Society of Chemistry (Great Britain), Ashwell G. J., Bloor D., Ed., Thomas, GhrahamHouse ed., Cambridge, pp. 237-240, ISBN: 0851866255, 9780851866253.
  22. 22. Spangler, C. W. & Havelka, K. O., (1991), Stabilization of Polaronic and Bipolaronic States in Electro-active Oligomeric Segments of Non-linear Optic Active Copolymers, in Organic Materials for Non-Linear Optics II, Volume 91 of Special publication - Royal Society of Chemistry (Great Britain),. Hannand R. A, Bloor D., GhrahamHouse ed., Cambridge, pp. 281-288. ISBN 0851863973, 9780851863979.
  23. 23. Natansohn, A. & Rochon, P., (2002), Photoinduced Motions in Azo-Containing Polymers, Chem. Rev., 102, 11, pp. 4139-4176, ISSN: 0009-2665. DOI: 10.1021/cr970155y
  24. 24. Albert, I. D. L.; Marks, T. J.; Ratner, M. A., (1996), Rational design of molecules with large hyperpolarizabilities. Electric field, solvent polarity, and bond length alternation effects on merocyanine dye linear and nonlinear optical properties, J. Phys. Chem. B, 100, 23, pp.9714–9725 ISSN: 1520-6106. DOI: 10.1021/jp960860v
  25. 25. Castellano, O., Bermudez, Y., Giffard, M., Mabon, G., Cubillan, N., Sylla, M., Nguyen-Phu, X., Hinchliffe, A., Soscun, H., (2005), Ab initio and DFT study of the geometric structures and static dipole (hyper)polarizabilities of aromatic anions, J. Phys. Chem. A; 109, 45, pp.10380–7, ISSN: 1089-5639 DOI: 10.1021/jp051136s.
  26. 26. Jacquemin, D.; Femenias, A., Chermette, H., Andre, J. M. &Perpete, E. A., (2005), Second-order Moller-Plesset evaluation of the bond length alternation of several series of linear oligomers,J Phys Chem A, 109, 25, pp. 5734–41. ISSN: 1089-5639 DOI: 10.1021/jp0509111
  27. 27. Sohn, J. E.; Singer, K. D.; Kuzyk, M. G.; Holland, W. R.; Katz, H. E.; Dirk, C. W.; Schilling, M. L. &Comizzoli, R. B.; (1989), Orientationally Ordered Nonlinear Optical Polymer Films, in “Nonlinear Optical Effects in Organic Polymers” NATO Advanced Research Workshop on Nonlinear Optical Effects in Organic Polymers, Sophia-Antipolis, Nice, France 19-20 May 1988, Messier, J., Kajzar, F., Prassad, P., Ulhich, D., Kluwer ed., Acad. Publ., Derdrech, Boston, London, NATO ASI series: Appl. Sc. ser. E, 162, pp. 291-299, ISBN: 0-7923-0132-3. DOI: 10.1007/978-94-009-2295-2_23
  28. 28. Reinhardt, B. A.; Brott, L. L.; Clarson, S. J.; Dillard, A. G.; Bhatt, J. C.; Kannan, R.; Yuan, L.; He, G. S. & Prasad, P. N., (1998),Highly Active Two-Photon Dyes: Design, Synthesis, and Characterization toward Application, Chem. Mater., 10, 7, pp. 1863-74, ISSN: 0897-4756. DOI: 10.1021/cm980036e.
  29. 29. Albota, M.; Beljonne, D.; Bredas, J. L.; Ehrlich, J. E.; Fu, J. Y.;Heikal, A. A.; Hess, S. E.; Kogej, T.; Levin, M. D.; Marder, S. R.; McCord-Maughon, D.; Perry, J. W.; Rockel, H.; Rumi, M.; Subramaniam,G.; Webb, W. W.; Wu, X. L. & Xu, C., (1998), Design of Organic Molecules with Large Two-Photon Absorption Cross Sections, Science, 281, 5383, pp. 1653-1656, ISSN 0036-8075. DOI: 10.1126/science.281.5383.1653
  30. 30. Norman, P.; Luo, Y. & Ågren, H., (1998), Structure-to-property relations for two-photon absorption of hydrocarbon oligomers, Chem. Phys. Lett., 296, 1-2, pp. 8-18, :” ISSN: 0009-2614. DOI: 10.1016/S0009-2614(98)01008-2
  31. 31. Norman, P.; Luo, Y. & Ågren, H., (1999), Two-photon absorption in five-membered heteroaromatic oligomers, Opt. Commun., 168, 1-4, pp. 297-303, ISSN: 0030-4018. DOI: 10.1016/S0030-4018(99)00250-3
  32. 32. Norman, P.; Luo, Y. & Agren, H., (1999), Large two-photon absorption cross sections in two-dimensional, charge-transfer, cumulene-containing aromatic molecules J. Chem. Phys., 111, 17, pp. 7758-7766, ISSN: 0021-9606. DOI: 10.1063/1.480111
  33. 33. Porres, L.; Charlot, M.; Entwistle, C. D.; Beeby, A.; Marder, T. B. & Blanchard-Desce, M., (2005), Novelboronquadrupolar NLO-phores: optimization of TPA/transparency trade-off via molecular engineering, Nonlinear Optical Transmission and Multiphoton Processes in Organics III, Proceedings of SPIE Volume: 5934,Yeates, A. T. Ed., pp. 62-73, ISBN: 9780819459398 DOI: 10.1117/12.618425
  34. 34. Nguyen, K. A.; Rogers, J. E.; Slagle, J. E.; Day, P. N.; Kannan, R.; Tan, L.-S.; Fleitz, P. A. & Pachter, R., (2006), Effects of Conjugation in Length and Dimension on Spectroscopic Properties of Fluorene-Based Chromophores from Experiment and Theory, J. Phys. Chem. A, 110, 49,13172-182, ISSN: 1089-5639. DOI: 10.1021/jp0642645
  35. 35. Ramakrishna, G. & Goodson, T., (2007), Excited-State Deactivation of Branched Two-Photon Absorbing Chromophores: A Femtosecond Transient Absorption Investigation J. Phys. Chem. A, 111, 6, 993-1000, ISSN: 1089-5639. DOI: 10.1021/jp064004n
  36. 36. Yang, Y; Wang, H. et alt.; (2015)The synthesis of new double-donor chromophores with excellent electro-optic activity by introducing modified bridges,Phys. Chem. Chem. Phys., 2015,17, 5776-5784;doi.org/10.1039/C4CP05829A
  37. 37. Lee, S.; Thomas, K. R. J.; Thayumanavan, S. & Bardeen, C. J., 2005, Dependence of the Two-Photon Absorption Cross Section on the Conjugation of the Phenylacetylene Linker in Dipolar Donor−Bridge−Acceptor Chromophores, J. Phys. Chem. A, (2005), 109, 43, pp. 9767-9774, ISSN: 1089-5639. DOI: 10.1021/jp053864l
  38. 38. Barzoukas, M. & Blanchard-Desce, M., (2000), Molecular engineering of push–pull dipolar and quadrupolar molecules for two-photon absorption: A multivalence-bond states approach, J. Chem. Phys., 113, 10, pp. 3951-3959, ISSN: 0021-9606. DOI: 10.1063/1.1288367
  39. 39. Bartkowiak, W.; Zalesny, R. & Leszczynski, J., (2003), Relation between bond-length alternation and two-photon absorption of a push-pull conjugated molecules: a quantum-chemical study, Chem. Phys., 287, 1-2, pp. 103-112, ISSN: 0301-0104. DOI: 10.1016/S0301-0104(02)00982-5
  40. 40. Drobizhev, M.; Karotki, A.; Rebane, A.& Spangler, C. W., (2001), Dendrimer molecules with record large two-photon absorption cross section, Opt. Lett. 26, 14 , pp. 1081-1083, ISSN: 0146-9592. DOI: 10.1364/OL.26.001081
  41. 41. V. Punjabi et al. (Jefferson Lab Hall A Collaboration) 2005, Phys. Rev. C71, 055202, Proton elastic form factor ratios to Q2=3.5GeV2 by polarization transfer DOI: 10.1103/PhysRevC.71.055202
  42. 42. Baur, J. W.; Alexander, M. D. J.; Banach, M.; Denny, L. R.; Reinhardt, B. A.; Vaia, R. A.; Fleitz, P. A. & Kirkpatrick, S. M., (1999), Molecular Environment Effects on Two-Photon-Absorbing Heterocyclic Chromophores, Chem. Mater. 11, 10 , pp. 2899-2906, ISSN: 0897-4756. DOI: 10.1021/cm990258s
  43. 43. Agrawal, G. P. &Flytzanis, C., (1976); Delocalization and superalternationeffects in the nonlinear susceptibilities of one-dimensional systems, Chem. Phys. Lett, 44, 2, pp. 366-370, ISSN: 0009-2614. DOI: 10.1016/0009-2614(76)80532-5
  44. 44. Agrawal, G. P., Cojan, C. &Flytzanis, C., (1978), Nonlinear optical properties of one-dimensional semiconductors and conjugated polymers, Phys. Rev. B, 17, 2, pp. 776-789; ISSN: 1098-0121. DOI: 10.1103/PhysRevB.17.776
  45. 45. Beratan, D. N., Onuchic, J. N. & Perry, J. W., (1987), “Non-linear susceptibilities of finite organic polymers”, J. Phys. Chem., 91, 11, pp. 2696-2698, ISSN 0022-3654. DOI: 10.1021/j100295a009
  46. 46. Garito, A. F.; Heflin, J. R.; Wong, K. Y. &Zamaki-Khamiri, O., (1989), Enhancement of Non-linear Optical Properties of Conjugated Linear Chain throughLoweredSymmetry, in “Organic materials for non-linear optics: the proceedings of a conference organised by the Applied Solid State Chemistry Group of the Dalton Division of the Royal Society of Chemistry, Oxford, 29th-30th June 1988, Issue 69 of Special publication Volume 69 of Special publication // Royal Society of Chemistry”, editat de R. A. Hann si D. Bloor, Roy. Soc. Chem., London, pp. 16-28, ISBN:0851868061, 9780851868066
  47. 47. Prasad, P. N., (1989), Studies of Ultrafast Third-order Non-linear Optical Processes in Polymer Films, in Organic materials for non-linear optics: the proceedings of a conference organized by the Applied Solid State Chemistry Group of the Dalton Division of the Royal Society of Chemistry, Oxford, 29th-30th June 1988, 69 of Special publication // Royal Society of Chemistry, Hann, R. A. & Bloor, D., Ed., London 1989, pp. 264-278; ISBN: 0851868061, 9780851868066. DOI: 10.1007/978-94-009-2295-2_28
  48. 48. Spangler, C. W.; Hall, T. J.; liu, P. K.; Dalton, L. R.; Polis, D. W. &Sapochak, L. S., (1991), The design of New Copolymers for χ(3) Applications: Copolymers Incorporating Ladder Subunits, in Organic Materials for Non-Linear Optics II, Volume 91 of Special publication - Royal Society of Chemistry (Great Britain), Hannand, R. A, Bloor, D., GhrahamHouse ed., Cambridge, pp. 260-267, ISBN 0851863973, 9780851863979.
  49. 49. Spangler, C. W.; Liu, P. K.; Hall, T. J.; Polis, D. W.; Sapochak, L. S. & Dalton, L. R., (1992), The design of new copolymers for x(3) applications, Polymer, 33, 18, pp. 3937-3941, ISSN: 0032-3861. DOI: 10.1016/0032-3861(92)90386-B
  50. 50. Nalwa, S. H., (1991), Recent Developments in Ferroelectric Polymers, J. Macromol. Scie., Part C: Polym. Rev., 31, 4, 341-432, ISSN: 1532-1797. DOI: 10.1080/15321799108021957
  51. 51. Kurihara, T.; Tomaru, S.; Mori, Y.; Shuto, Y.; Hikita, M.; & Kaino, T., (1993), A New Main-chain Polymer for All-optical Waveguide Devices, in Organic Materials for Non-Linear Optics III, Volume 137 of Special publication - Royal Society of Chemistry, Issue 137 of Special publication, Royal Society of Chemistry (Great Britain), Ashwell, G. J., Bloor D., Ed., Thomas Graham Hause, ed., Cambridge, pp. 344-448; ISBN: 0851866255, 9780851866253.
  52. 52. Foss, R. P.; Tam, W.& Zumsteg, F. C., (1991); Preparation of Polymeric Films for NLO Applications, Papers presented at the New York, NY Meeting: Polymeric Materials for Photonic and Optical Applications, 4th Chemical Congress of North America and 202nd ACS National Meeting Published by The Division of Polymer Chemistry, Inc., American Chemical Society, Polym. Prepr. (Am. Chem. Soc, Div. Polym. Chem.), 32(2), 76-78. ISSN: 0032-3934.
  53. 53. Meyrueix, R.; Mignani, G. &Tapolsky, G., (1991), Study of a Novel class of Second Order Non-linear Optical (NLO) Polyurethanes, in Organic Materials for Non-Linear Optics, II, 91, ,. Hann, R. A & Bloor, D. Ed., Roy. Soc; Chem., London, ed., pp. 273-280, ISSN: 0851863973, 9780851863979 DOI: 10.1007/978-94-011-3370-8_11
  54. 54. Kitipichai, P.; la Peruta, R., Korenowski, G. M. & Winek, G. E., (1993), In-situ poling and synthesis of NLO chromophore-bearing polyurethanes for second harmonic generation, J. Polym. Sci., A: Polym. Chem., 31, 6, pp. 1365-1375, ISSN: 1089-5639. DOI: 10.1002/pola.1993.080310603
  55. 55. Eich, M.; Reck, B.; Yoon, Y.; Willson, C. G., Bjorklund, G. C.; (1989), Novel second order nonlinear optical polymers via chemical cross-linking induced vitrification under electric field, J. Appl. Phys., 66, 7, pp. 3241-3247, ISSN 0021-8979. DOI: 10.1063/1.344115
  56. 56. Hann, R. A., (1989), “Organic Materials for Non-linear Optics”, Roy. Soc. Chem., London, Roy. Soc. Chem., ISBN: 0851868061, 9780851868066, London. DOI: 10.1002/adma.19890011214
  57. 57. Prasad, P. N. & Reinhard, B. A., (1990); Is there a role for organic materials chemistry in nonlinear optics and photonics?, Chem. Mater., 2, 6, 660-669, ISSN: 0897-4756. DOI: 10.1021/cm00012a014
  58. 58. Jungbauer, D.; Reck, B.; Twieg, R. J.; Yoon, D. Y.; Willson, C. G. &Swalen, J. D., (1990), Highly efficient and stable nonlinear optical polymers via chemical cross-linking under electric field, Appl. Phys. Lett., 56, 26, pp. 2610-2616, ISSN: 0003-6951. DOI: 10.1063/1.102853
  59. 59. Jungbauer, D.; Teraoka, I.; Yoon, D. Y.; Reck, B.; Swalen, J. D.; Twieg, R. J. & Willson, C. G., (1991); Second order nonlinear optical properties and relaxation characteristics of poled linear epoxy polymers withtolanechromophores, J. Appl. Phys., 69, 12, pp. 8011-8017, ISSN 0021-8979. DOI: 10.1063/1.347497
  60. 60. Reck, B.; Eich, M.; Jungbauer, D.; Twieg, R. J.; Willson, C. G.; Yoon, D. Y. & Bjorklund, C. G., (1990), Crosslinked Epoxy Polymers with Large and Stable Nonlinear Optical Susceptibilities in Proc. SPIE 1147: Proceedings of SpieNonlinearopticalproperties of organic materials II: 10-11 August 1989, San Diego, California, 74-83,G. Khanarian; Ed., Society of Photo Optical ed., ISBN: 0819401838, 9780819401830. DOI: 10.1117/12.962109
  61. 61. Swalen, J. D.; Bjorklund, G. C.; Fleming, W.; Herminghaus, S.; Jungbauer, D.; Jurich, M.; Moerner, W. E.; Reck, B.; Smith, B. A.; Twieng, R.; Willson, C. G. &Zentel, R., (1991), Poled Epoxy Polymers for Optoelectronics, in Organic molecules for nonlinear optics and photonics, 194, NATO Advanced Study Institutes series. Series E, Applied sciences, J. Messier,F. Kajzar, P. N. Prasad, Ed. , Kluwer Academic Publishers, ed. Jluwer Acad. publ., Netherlands, 433-477, ISBN: 0792311817, 9780792311812. DOI: 10.1007/978-94-011-3370-8_31
  62. 62. J. Nordmann, P. Rohl, Cross-linked polymers for non-linear opticswithimprovedlong-termostability, Organic Materials for Non-linear Optics III, Eds. (1993), pp.190–196.
  63. 63. Zentel, R.; Jungbauer, D.; Twieg, R. J.; Yoon, Do Y. & Grant Willson, C.;Synthesis and non-linear opticalcharacteristics of crosslinked and linear epoxy polymers with pendant tolanechromophores. Die Makromol. Chem. Macromol., 1993, 194, 859-868. DOI: 10.1002/macp.1993.021940310
  64. 64. Frinkelman, H.; Ringsdorf, H. & Wendorff, J. H., (1978), Model considerations and examples of enantiotropic liquid crystalline polymers. Polyreactions in orderedsystems, Makromol. Chem., 179, 1 pp. 273-276, ISSN: 1521-3935 DOI: 10.1002/macp.1978.021790129
  65. 65. Ashwell, G. J.; Dawnay, E. J. C.; Kuczynski, A. P. & Martin, P. J.,Highestobservedsecondharmonicintensityfrom a multilayered Langmuir-Blodgett film structure, in “Physical Concepts of Materials for Novel Optoelectronic Device Applications”, Physical Concepts of Materials for Novel Optoelectronic Device Applications I: Materials Growth and Characterization Aachen, Federal Republic of Germany, Sunday 28 October 1990, SPIE Proc. 1361, ManijehRazeghi, Ed., pp. 589-598 ISBN: 9780819404220. DOI: 10.1117/12.24423
  66. 66. Stone, P. J. W.; Miller, L. S.; Walton, D. J. & Sethi, R S., (1993), Langmuir-Blodgett Films of Preformed Polymers for Second Harmonic Generation, in “Organic Materials for Non-linear Optics III”, Ashwell, G. J. &Bloor, D., Eds., Royal Society of Chemistry (Great Britain) Special publication; no.137 , Thomas Graham Hause, ed., Cambridge, pp. 88-96; ISBN: 0851866255, 9780851866253.
  67. 67. Rau, H., (1983), Asymmetric photochemistry in solution, Chem. Rev., 83, 5,535–547. ISSN: 0009-2665. DOI: 10.1021/cr00057a003
  68. 68. Rau, H. In Photochemistry and Photophysics; J. K. Rabek, Ed; CRC Press: Boca Raton, FL, (1990); Vol. 2 (chp. 4), p 119-141.
  69. 69. Kumar G. S., (1992), Azo functional polymers: functional group approach in macromolecular design. Lancaster: Technomic Publication; ISBN: 0877629366, 9780877629368
  70. 70. Todorov, T.; Nikolova, L.; Tomova, N., (1984), Polarization holography. 1: A new high-efficiency organic material with reversible photoinduced birefringence Appl. Opt., 23, 23, pp. 4309-4312, ISSN: 1559-128X. DOI: 10.1364/AO.23.004309
  71. 71. Eich, M.; Wendorff, J. Makromol. Chem. (1987), M. Eich and J. H. Wendorff, “Erasable holograms in polymeric liquid crystals,” Makromol. Chem. Rappid Comm., 8, 9 pp. 467-471, ISSN: 1521-3927. DOI: 10.1002/marc.1987.030080909
  72. 72. Eich, M.; Wendorff, J.; Reck, B.; Ringsdorf, H., (1987) , Reversive digital and holographic optical storage in polymer liquidcrystals, Makromol. Chem., 8, 1, pp. 59-63, ISSN: 1521-3927. DOI: 10.1117/12.939643
  73. 73. Ichimura, K.; Suzuki, Y.; Seki, T.; Hosoki, A. & Aoki, K., (1988), Reversible change in alignment mode of nematic liquid crystals regulated photochemically by command surfaces modified with an azobenzene monolayer, Langmuir, 4, 5, pp.1214-1216, ISSN: 0743-7463. DOI: 10.1021/la00083a030
  74. 74. Xie, S.; Natansohn, A. & Rochon, P., (1993), Recent developments in aromatic azo polymers research, Chem. Mater., 5, 4, pp. 403-411, ISSN: 0897-4756. DOI: 10.1021/cm00028a003
  75. 75. Ichimura, K.; Seki, T.; Kawanishi, Y.; Suzuki, Y.; Sakuragi, M.; Tamaki, T., (1994), Photocontrol of liquid crystal alignment by command surfaces, In Photoreactive Materials for Ultrahigh-Density Optical Memory: MITI research and development program on basic technologies for future industries; M. Irie, Ed.; Elsevier: Amsterdam, pp. 55-75, ISBN-10: 044481936; ISBN-13: 978-0444819369.
  76. 76. Ichimura, K., (1996), Photoregulation of Liquid Crystal Alignament by Photochromic Molecules and Polymeric Thin Films, In Polymers as Electrooptical Components Macromolecular systems, materials approach Macromolecular Systems Series ResearchReportsEsprit, Shibaev, V. P., Ed.; Springer-Verlag: New York, pp. 138-158; ISBN: 3540594868, 9783540594864. DOI: 10.1007/978-3-642-79861-0_4
  77. 77. Natansohn, A. & Rochon, P., (2001), 2000 Macromolecular Science and Engineering Award LectureThe versatility of azobenzene polymers,Canadian Journal of ChemistryVolume 79, 1093-1100;doi: 10.1139/v01-098
  78. 78. Ichimura, K., (2000), Photoalignment of Liquid-Crystal Systems, Chem. Rev., 100, 5, pp. 1847-1874; ISSN: 0009-2665. DOI: 10.1021/cr980079e
  79. 79. Delaire, J. A.; Nakatani, K., (2000), Linear and Nonlinear Optical Properties of Photochromic Molecules and Materials Chem. Rev., 100, 5, pp. 1817-1846, Print Edition ISSN: 0009-2665; Web Edition ISSN: 1520-6890.DOI: 10.1021/cr980078m
  80. 80. Sutherland R. L., Handbook of nonlinear optics, New York: Marcel Dekker; (1996), ISBN: 0824794265, 9780824794262.
  81. 81. Demus, D., Godby, J., Gray, G.W., Spiess, H.-W., Vill, V., Eds., 1998, Handbook of Liquid Crystals, vol. 3, WILEY-VCH. DOI: 10.1002/9783527620760
  82. 82. Sekkat, Z. &Knoll, W., (2002), Chapter II 4: Photoisomerization and Photo-Orientation of Azo Dyes in Films of Polymer: Molecular Interaction, Free Volume, and Polymer Structural Effects, in Photoreactive organic thin films, pp. 108-144 Amsterdam: Academic Press; ISBN: 0-12-635490-1 DOI: 10.1016/B978-012635490-4/50005-6
  83. 83. Tsutsumi, N., Matsumoto, O., Sakai, W. &Kiyotsukuri T., (1996), Nonlinear optical polymers. 2. Novel NLO linear polyurethane with dipole moments aligned transverse to the main backbone, Macromolecules; 29, 2 (January 15, 1996), 592–597, ISSN: 0024-9297. DOI: 10.1021/ma951077o
  84. 84. Tsutsumi, N., Morishima, M. & Sakai, W., (1998), Nonlinear optical (NLO) polymers. 3. NLO polyimide with dipole moments aligned transverse to the imide linkage, Macromolecules; 31, 22, 1998), pp. 7764–7769, ISSN: 0024-9297. DOI: 10.1021/ma9803436
  85. 85. Tirelli, N., Solaro, R. A., Ciardelli, F., Follonier, S., Bosshard, C. H. & Günter P., (2000), Structure–activity relationship of new NLO organic materials based on push–pull azodyes: 4. Side chain polymers., Polymer; 41, 2, pp. 415–421, ISSN: 0032-3861. DOI: 10.1016/S0032-3861(99)00202-5
  86. 86. Liu, Y., Jiang, A., Xiang, L., Gao, J. & Huang, D., (2000) Nonlinear optical chromophores with good transparency and high thermal stability, Dyes &Pigments, 45, 3, 189–193, ISSN: 0143-7208. DOI: 10.1016/S0143-7208(00)00018-8
  87. 87. Luh, T. Y., Chen, R. M., Hwu, T. Y., Basu, S., Shiau, C. W., Lin, W. Y., Jin, B. Y. & Hsu, C. C., (2001), Rational design of polymers for optoelectronic interests, Pure Appl Chem, 73, 2, pp. 243–246, ISSN: 0033-4545. DOI: 10.1351/pac200173020243
  88. 88. Takase, H., Natansohn, A. & Rochon, P., (2001), Effect of crosslinking on the photoinduced orientation of azo groups in thin polymer films, J. Polym. Sci., Part B: Polym. Phys., 39, 14, 1686-1696 (2001), ISSN: 109-0488. DOI: 10.1002/polb.1140
  89. 89. Li, Z., Li, J., Qin, J., & Ye, C., (2003), Second-order nonlinear optical property of polysiloxane containing indole-based multifunctional chromophore, Synth. Met., 135-136, pp. 467–468, ISSN: 0379-6779. DOI: 10.1016/S0379-6779(02)00692-6
  90. 90. Natansohn, A., Rochon, P., Gosselin, J. & Xie, S., (1992), Azo polymers for reversible optical storage. 1. Poly[4′-[[2-(acryloyloxy)ethyl]ethylamino]-4-nitroazobenzene] Macromolecules, 25, 8, pp. 2268-2273., ISSN: 0024-9297. DOI: 10.1021/ma00034a031
  91. 91. Cojocariu, C., Rochon, P., (2004), Light-induced motions in azobenzene-containing polymers, Pure Appl. Chem., 76, 7-8, 1479-1497. ISSN: 0033-4545. DOI: 10.1351/pac200476071479
  92. 92. Meng, X., Natansohn, A., Barrett, C. & Rochon, P. (1996), Azo Polymers for Reversible Optical Storage. 10. Cooperative Motion of Polar Side Groups in Amorphous Polymers, Macrom., 29, 3, pp. 946-952, ISSN: 0024-9297. DOI: 10.1021/ma951255d
  93. 93. L. Angiolini; T. Benelli; L. Giorgini; F. Mauriello; E. Salatelli; R. Bozio; A. Daurù; D. Pedron,Synthesis, chiroptical properties and photoinduced birefringence of optically active methacrylic copolymers bearing side-chain bisazoaromatic moieties, Eur. Polym. J.; 2007, 43, pp. 3550 – 3561;doi.org/10.1016/j.eurpolymj.2007.05.020
  94. 94. Angiolini, L., Caretti, D., Giorgini, L., Salatelli, E., (2000), Optically active methacrylic polymers bearing side-chain conjugated azoaromatic chromophores, Synth. Met., 115, 1-3 , pp. 235-239. ISSN: 0379-6779 DOI: 10.1016/S0379-6779(00)00341-6
  95. 95. Angiolini, L., Caretti, D., Giorgini, L., et al., (2000), Optically active polymethacrylates with side-chain l-lactic acid residues connected to push–pull azobenzene chromophores, Polymer, 41, 13, pp. 4767-4780. ISSN: 0032-3861. DOI: 10.1016/S0032-3861(99)00701-6.
  96. 96. Buffeteau, T., Labarthet, F. L., Pezolet, M., Sourisseau, C., (1998), Photoinduced Orientation of Azobenzene Chromophores in Amorphous Polymers As Studied by Real-Time Visible and FTIR Spectroscopies, Macromolecules, 31, 21, pp. 7312-7320, ISSN: 0024-9297. DOI: 10.1021/ma980843z
  97. 97. Poncin-Epaillard, F., Beunet, J., Bulou, A. &Bardeau, J. F., (2001), Synthesis of a new polymer surface bearing grafted azo polymer chains, J. Polym. Sci., Part A: Polym. Chem., 39, 18, pp. 3052-3061, ISSN: 1060-1325. DOI: 10.1002/pola.1286
  98. 98. Wu, Y., Zhang, Q., Kanazawa, A., (1999), Photoinduced Alignment of Polymer Liquid Crystals Containing Azobenzene Moieties in the Side Chain. 5. Effect of the Azo Contents on Alignment Behavior and Enhanced Response, Macromolecules, 32, 12, pp. 3951-3956, ISSN: 0024-9297. DOI: 10.1021/ma990197j
  99. 99. Bellebia, S.; Mesli, A.; Florescu (Albu), A.-M.; Chatzopoulos, F. &Montheard, J. P., (1995), “Nouveaux Colorants pour L'optique Non LinéairePréparés a Partir de Bases schiffDérives du Chloroméhylstyrène”, J. Soc. Alger. Chim., 5, 2, pp. 1-9; ISSN:0024-9297.
  100. 100. Albu, A.-M.; Mărculescu, B.; Boborodea, A. G. & Vasilescu, D. S., (1999), “Synthesis and Characterisation of some Polymers with Applications in Non-linear Optics: I. Polymerisation of Styrene and Methyl methacrylate in the Presence of Coloured Comonomers”, E. Polym. J., 35, 12, pp. 2197-2202, ISSN: 0014-3057. DOI: 10.1016/S0014-3057(99)00018-X
  101. 101. Albu, A.-M.; Mărculescu, B. & Vasilescu, D. S., (1999), “Synthesis and Characterization of Some Polymers with Applications in Non-linear Optics: II. Copolymerisation of Styrene with some Monomers containing Azo-Dyes”, E. Polym. J., 35, 12, pp. 2203-2205, ISSN: 0014-3057. DOI: 10.1016/S0014-3057(99)00019-1
  102. 102. Albu, A.-M., Marculescu, B.; Manaila- Maximean, D. &Trouillet, A., (2000), Preparation of a copolymer for second-order nonlinear optics, SIOEL '99: Sixth Symposium on Optoelectronics, Proc SPIE—Int Soc Opt Engen,4068 ,NecsoiuT. ; Robu, M. &Dumitras, D. C., Ed. pp. 59–64; ISBN: 9780819437051. DOI: 10.1117/12.378725
  103. 103. Sylla, M.; Mănăila-Maximean, D.; Albu, A. M. & Delaunay, J., (2000), “Synthesis, and Non-linear Optical Properties of New Polymers Based on Coloured Monomers”, Polymer, 41, 10, pp. 3507-3511, ISSN 0032-3861. DOI: 10.1016/S0032-3861(99)00610-2
  104. 104. Albu, A.-M., Marculescu, B.; Manaila- Maximean, D. &Trouillet, A., (2000), Preparation of a copolymer for second-order nonlinear optics, SIOEL '99: Sixth Symposium on Optoelectronics,Proc SPIE—Int Soc Opt Engen,4068 ,NecsoiuT. ; Robu, M. &Dumitras, D. C., Ed. pp. 59–64; ISBN: 9780819437051. DOI: 10.1117/12.378725
  105. 105. Albu, A.-M.; (2009), “Second and Third Nonlinear Optical Response in Azoic Pendant Macromolecular Structures”, Rev. Chim., 60, 1, pp. 38-41; ISSN:.
  106. 106. Hvilsted S, Andruzzi F, Ramanujam P. S., (1992), Side-chain liquid-crystalline polyesters for optical information storage, Opt Lett. 17, 17, pp. 1234-1236, ISSN: 0146-9592. DOI: 10.1364/OL.17.001234
  107. 107. Hvilsted S, Andruzzi F, Kulinna C, Siesler, H. W., Ramanujam, P. S., (1995) Novel Side-Chain Liquid Crystalline Polyester Architecture for Reversible Optical Storage, Macromolecules, 28, 7, pp. 2172-2183, ISSN: 0024-9297. DOI: 10.1021/ma00111a011
  108. 108. Pedersen M., Hvilsted, S., Holme, N. C. R., Ramanujam, P. S., (1999), Influence of the substituent on azobenzene side-chain polyester optical storage materials, Macromol. Symp., 137, 1, pp. 115-127, ISSN: 1022-1360; 1521-3900. DOI: 10.1002/masy.19991370112
  109. 109. Andruzzi, L., Altomare, A., Ciardelli, F., Solaro, R., Hvilsted, S., Ramanujam, P. S., (1999), Holographic Gratings in Azobenzene Side-Chain Polymethacrylates, Macromolecules, 32, 2 , pp. 448-454, ISSN: 0024-9297. DOI: 10.1021/ma980160j
  110. 110. Nicolescu, F. A., Jerca, V. V., Albu A.-M., Vuluga , D. M. & Draghici, C., (2008), “Synthesis and Copolymerization Study of New Polyimide Precursors with Potential Application in Optical and Photonic Field”, Mol. Cryst. Liq. Cryst., 486, 1, 38–49; ISSN: 1542-1406; 1563-5287. DOI: 10.1080/15421400801917338
  111. 111. Nicolescu, F. A.; Jerca; V. V., Albu, A.- M.; Vuluga, D. M. & Vasilescu, D. S., (2009), Poly(maleic-amic) Structures for Potential Nonlinear Optical Applications, U.P.B. Sci. Bull., Series B, 71, 1 pp. 75-82, ISSN: 1454-2331.
  112. 112. Nicolescu, F. A.; Jerca, V. V; Albu, A.- M; Vasilescu, D. S. &Vuluga, M. D., (2009), “Synthesis and characterization of organic-inorganic polymers from new methacrylate monomers and silane derivatives”, Optical Materials in Defence Systems Technology VI, 31 August 2009, Berlin, Germany, Proc. SPIE 7487, 748701 (octomber, 2009), Grote, J. G.; Kajzar, F.& Zamboni, R., Ed, 74870N DOI: 10.1117/12.832282
  113. 113. Chen T, Jen A. K. Y., Cai Y., (1996), Two-step synthesis of side-chain aromatic polyimides for second-order nonlinear optics, Macromolecules; 29, 2, pp. 535–539, ISSN: 0024-9297. DOI: 10.1021/ma9512566
  114. 114. Bao Z, Chan WK, Yu L., (1995); Exploration of the stille coupling reaction for the synthesis of functional polymers, J Am. Chem. Soc., 117, 50, 12426–12435, ISSN: 0002-7863. DOI: 10.1021/ja00155a007
  115. 115. Gubbelmans, E.; Verbiest, T.; Van Beylen, M.; Persoons, A.; Samyn, C., (2002), Chromophore-functionalisedpolymides with high-poling stabilities of the nonlinear optical effect at elevated temperature. Polymer, 43, 5, pp. 1581–1585, ISSN: 0032-3861. DOI: 10.1016/S0032-3861(01)00678-4
  116. 116. Yu, D.; Gharavi, A. & Yu, L., (1995), A generic approach to functionalizing aromatic polyimides for second-order nonlinear optics, Macromolecules; 28, 3, pp. 784–786, ISSN: 0024-9297, 1520-5835. DOI: 10.1021/ma00107a017
  117. 117. Yu D.; Gharavi, A. & Yu, L., (1996), Highly stable copolyimides for second-order nonlinear optics. Macromolecules; 29, 19, pp.6139–6142, ISSN: 0024-9297. DOI: 10.1021/ma951511m
  118. 118. Van den Broeck, K.; Verbiest, T.; Van Beylen, M.; Persoons, A. & Samyn, C., (1999), Synthesis and nonlinear optical properties of high glass transition polyimides, Macromol Chem Phys., 200, 12, pp.2629–2635, ISSN:1521-3925. DOI: 10.1002/(SICI)1521-3935(19991201)200:12<2629::AID-MACP2629>3.0.CO;2-K
  119. 119. Van den Broeck, K.; Verbiest, T., Degryse, J.; Van Beylen, M.; Persoons, A. & Samyn, C., (2001), High glass transition chromophore functionalised polyimides for second-order nonlinear optical applications, Polymer, 42, pp.3315–3322, ISSN: 0032-3861. DOI: 10.1016/S0032-3861(00)00761-8
  120. 120. Davey, M. H.; Lee, V. Y. ; Wu, L.-M.; Moylan, C. R.; Volksen, W.; Knoesen, A.; Miller, R. D.; Marks, T. J.; (2000), Ultrahigh-Temperature Polymers for Second-Order Nonlinear Optics. Synthesis and Properties of Robust, Processable, Chromophore-Embedded Polyimides, Chem. Mater., 12,1679-1693, doi: 10.1021/cm990483+
  121. 121. Hongwei J. & Kakkar A. K. , (1998), Soluble high-Tg polymers for second-order nonlinear optics from an unusual mix of imide and siloxane linkages in the backbone, Macromolecules, 31, 13, 4170–4176, ISSN: 0024-9297. DOI: 10.1021/ma980309r
  122. 122. Samyn, C., Verbiest, T., Kesters, E., Van den Broeck, K., Van Beylen, M. &Persoons, A., (2000), High glass transition chromophore functionalized poly(maleimide-styrene)s for second order nonlinear optical applications, Polymer; 41, 16, pp. 6049–6054, ISSN: 0032-3861. DOI: 10.1016/S0032-3861(99)00834-4
  123. 123. Chang, H. L; Lin H. L., Wang, Y. C., Dai S. A., Su W. C. & Jeng, R. J., (2007), Thermally stable NLO poly(amide-imide)s via sequential self-repetitive reaction, Polymer, 48, pp. 2046–2055, ISSN: 0032-3861. DOI: 10.1016/j.polymer.2007.02.010
  124. 124. Clays, K. & Coe, B.J., (2003), Design strategies versus limiting theory for engineering large second-order nonlinear optical polarizabilities in charged organic molecules, Chem Mater;15, 3, pp. 642–648, ISSN: 0897-4756. DOI: 10.1021/cm0212111
  125. 125. Qiu, Z., Hammer, B. A.G.; Müllen, K.; 2020, Conjugated polymers – Problems and promises, Progr. in Polym. Scie., 100, 2020, 101179, ISSN 0079-6700,https://doi.org/10.1016/j.progpolymsci.2019.101179.
  126. 126. Wu W, Bazan GC, Liu B. Conjugated-polymer-amplified sensing, imaging,and therapy. Chem 2017;2:760–90.
  127. 127. McGehee MD, Heeger AJ. Semiconducting (conjugated) polymers asmaterials for solid-state lasers. Adv Mater 2010;12:1655–68.
  128. 128. Grimsdale AC, Chan KL, Martin RE, Jokisz PG, Holmes AB. Synthesis oflight-emitting conjugated polymers for applications in electroluminescentdevices. Chem Rev 2009;109:897–1091.
  129. 129. Cheng YJ, Yang SH, Hsu CS. Synthesis of conjugated polymers for organicsolar cell applications. Chem Rev 2009;109:5868–923.
  130. 130. F. Dumur, Carbazole-based polymers as hosts for solution-processed organic lightemitting diodes: simplicity, efficacy, Org. Electron. 25 (2015) 345–361.
  131. 131. F. Dumur, L. Beouch, S. Peralta, G. Wantz, F. Goubard, D. Gigmes, Solution-processed blue phosphorescent OLEDs with carbazole-based polymeric host materials, Org. Electron. 25 (2015) 21–30.
  132. 132. G. Puckyte, B. Schmaltz, A. Tomkeviciene, M. Degbia, J.V. Grazulevicius, H. Melhem, J. Bouclé, F. Tran-Van, Carbazole-based molecular glasses for efficient solid-state dye-sensitized solar cells, J. Power Sources 233 (2013) 86–92.
  133. 133. T.-T. Bui, S.K. Shah, M. Abbas, X. Sallenave,G. Sini, L. Hirsch, F. Goubard, Carbazole-based molecular glasses as hole-transporting materials in solid state dye-sensitized solar cells, ChemNanoMat 1 (2015) 203–210.
  134. 134. F. Goubard, R. Aîcha, F. Tran-Van, A. Michaleviciute, F. Wünsch, M. Kunst, J. Grazulevicius, B. Ratier, C. Chevrot, Investigation of solid hybrid solar cells based on molecular glasses, Proc. Estonian Acad. Sci. Eng. 12 (2006) 96–110.
  135. 135. T.-T. Bui, L. Beouch, X. Sallenave, F. Goubard, Carbazol-N-yl and diphenylamino end-capped triphenylamine-based molecular glasses: synthesis, thermal, and optical properties, Tetrahedron Lett. 54 (2013) 4277–4280.
  136. 136. D. Liu, D. Li, H. Meng, Y. Wang, L. Wu, Multifunctional applications of triazine/ carbazole hybrid thermally activated delayed fluorescence emitters in organic light emitting diodes, J. Mater. Chem. C 7 (2019) 12470–12481.
  137. 137. X.-D. Zhu, Q.-S. Tian, Q. Zheng, X.-C. Tao, Y. Yuan, Y.-J. Yu, Y. Li, Z.-Q. Jiang, L.-S. Liao, A sky-blue thermally activated delayed fluorescence emitter based on multimodified carbazole donor for efficient organic light-emitting diodes, Org. Electron. 68 (2019) 113–120.
  138. 138. J.-L. Cai, W. Liu, K. Wang, J.-X. Chen, Y.-Z. Shi, M. Zhang, C.-J. Zheng, S.-L. Tao, X.-H. Zhang, Highly efficient thermally activated delayed fluorescence emitter developed by replacing carbazole with 1,3,6,8-tetramethyl-carbazole, Front. Chem. 7 (2019) 17.
  139. 139. T.-T. Bui, F. Goubard, M. Ibrahim-Ouali, D. Gigmes, F. Dumur, Thermally activated delayed fluorescence emitters for deep blue organic light emitting diodes: a review of recent advances, Appl. Sci. 8 (2018) 494.
  140. 140. T.-T. Bui, F. Goubard, M. Ibrahim-Ouali, D. Gigmes, F. Dumur, Recent advances on organic blue thermally activated delayed fluorescence (TADF) emitters for organic light-emitting diodes (OLEDs), Beilstein J. Org. Chem. 14 (2018) 282–308.
  141. 141. K. Karon, M. Lapkowski, Carbazole electrochemistry: a short review, J. Solid State Electrochem. 19 (2015) 2601–2610.
  142. 142. F. Dumur, Carbazole-based polymers as hosts for solution-processed organic lightemitting diodes: simplicity, efficacy, Org. Electron. 25 (2015) 345–361.
  143. 143. Elkhidr HE, Ertekin Z, Udum YA, Pekmez K (2020) Electrosynthesis and characterizations of electrochromic and soluble polymer films based on N- substituted carbazole derivates. Synth Met 260:116253.https://doi.org/10.1016/j.synthmet.2019.116253
  144. 144. Madhavan S, Santhanam KSV (1988) Structurally Modified Polymer of Carbazole with Specif ic Cat lysis in Electrooxidation of Organic Molecules. Mol Cryst Liq Cryst Inc Nonlinear Opt 160:111–119.https://doi.org/10.1080/15421408808083006
  145. 145. Boudreault P-LT, Beaupré S, Leclerc M (2010) Polycarbazoles for plastic electronics. Polym Chem 1:127–136.https://doi.org/10.1039/B9PY00236G
  146. 146. Dumur, F., 2020, Recent advances on carbazole-based photoinitiators of polymerization, Eur. Polym J., 125, 109503, ISSN 0014-3057,https://doi.org/10.1016/j.eurpolymj.2020.109503
  147. 147. Blouin, N.; Leclerc, M., 2008; Poly(2,7-carbazole)s: Structure−Property Relationships, Accounts of Chemical Research, 41, 1110-1119; DOI: 10.1021/ar800057k;
  148. 148. Georgiades, S. N.; Nicolaou, P. G., 2019, Chapter One - Recent advances in carbazole syntheses, in Advances in Heterocyclic Chemistry, Editor(s): Scriven, E. F.V.; Ramsden, C. A.; Academic Press, 129, 1-88, ISSN 0065-2725, ISBN 9780128174739,https://doi.org/10.1016/bs.aihch.2018.10.001;
  149. 149. Nayana, V., Kandasubramanian, B., (2020) Polycarbazole and its derivatives: progress, synthesis, and applications, J Polym. Res. 27, 285, .https://doi.org/10.1007/s10965-020-02254-7
  150. 150. L. Angiolini, R. Bozio, A. Daurů, L. Giorgini, D. Pedron, G. Turco, Chem. Eur. J. 8, (2002) 4241.
  151. 151. L. Angiolini, T. Benelli, L. Giorgini, A. Painelli, F. Terenziani, Chem. Eur. J. 11, (2005) 6053–6353.
  152. 152. L. Angiolini, T. Benelli, R. Bozio, A. Daurů, L. Giorgini, D. Pedron, E. Salatelli, Eur., Polym. J. 41 (2005) 2045.
  153. 153. L. Angiolini, T. Benelli, R. Bozio, A. Daurů, L. Giorgini, D. Pedron, E. Salatelli, Macromol. 39 (2006) 489.
  154. 154. A. Altomare, F. Ciardelli, L. Mellini, R. Solaro, Macromol. Chem. Phys. 205, (2004) 1611.
  155. 155. L. Angiolini, T. Benelli, L. Giorgini, F. Mauriello, E. Salatelli, Macromol. Chem. Phys. 207 (2006) 1805.
  156. 156. H. Li, R. Termine, L. Angiolini, L. Giorgini, F. Mauriello, A. Golemme, Chem. Mater. 21 (2009) 2403.
  157. 157. L. Angiolini, L. Giorgini, F. Mauriello, P. Rochon, Macromol. Chem. Phys. 210, (2009) 77.
  158. 158. L. Angiolini, D. Caretti, L. Giorgini, E. Salatelli, Macromol. Chem. Phys. 201, (2000) 533.
  159. 159. Luigi Angiolini, Tiziana Benelli, Loris Giorgini, Francesco Mauriello, Elisabetta Salatelli, 2009, Relevant chiroptical and thermal properties in optically active methacrylic copolymers containing carbazole and azoaromatic chromophores in the side-chain, Reactive and Functional Polymers, 69, 898-904, ISSN 1381-5148,https://doi.org/10.1016/j.reactfunctpolym.2009.09.005

Written By

Ana-Maria Albu and Vlad Marian Târpă

Submitted: July 3rd, 2021 Reviewed: July 29th, 2021 Published: September 28th, 2021