Poly(3,4-Ethylenedioxythiophene) Nanoparticles as Building Blocks for Hybrid Thermoelectric Flexible Films

: Hybrid thermoelectric ﬂexible ﬁlms based on poly(3,4-ethylenedioxythiophene) (PEDOT) nanoparticles and carbon nanotubes were prepared by using layer-by-layer (LbL) assembly. The employed PEDOT nanoparticles were synthesized by oxidative miniemulsion polymerization by using iron(III) p -toluenesulfonate hexahydrate (FeTos) as an oxidant and poly(diallyldimethylammonium chloride) (PDADMAC) as stabilizer. Sodium deoxycholate (DOC) was used as a stabilizer to prepare the aqueous dispersions of the carbon nanotubes. Hybrid thermoelectric ﬁlms were ﬁnally prepared with di ﬀ erent monomer / oxidant molar ratios and di ﬀ erent types of carbon nanotubes, aiming to maximize the power factor (PF). The use of single-wall (SWCNT), double-wall (DWCNT), and multiwall (MWCNT) carbon nanotubes was compared. The Seebeck coe ﬃ cient was measured by applying a temperature di ﬀ erence between the ends of the ﬁlm and the electrical conductivity was measured by the Van der Pauw method. The best hybrid ﬁlm in this study exhibited a PF of 72 µ W m − 1 K − 2 . These ﬁlms are prepared from aqueous dispersions with relatively low-cost materials and, due to lightweight and ﬂexible properties, they are potentially good candidates to recover waste heat in wearable electronic applications.


Introduction
Most of the energy produced today comes from classical energy sources, which are unfortunately non-renewable and generate many environmental problems. There is, therefore, a serious need to look for more sustainable and environmentally friendly sources. Thermoelectric generators can significantly contribute to this purpose, recovering energy from waste heat. In the last decade, thermoelectric materials have been attracting great interest in the field of energy harvesting [1]. The thermoelectric efficiency is determined by the dimensionless figure of merit, ZT, given by the expression ZT = S 2 σT/κ, where S, σ, and κ are the Seebeck coefficient, electrical conductivity, and thermal conductivity, respectively. Thermoelectric materials should not only be highly efficient, but also low-cost, manufacturing-scalable, and eco-friendly. Traditionally, the use of inorganic semiconductors has dominated thermoelectric applications. However, their inherent problems, such as toxicity, scarcity of raw materials, and high production cost, have motivated the search of new materials capable to overcome such problems [2]. Because of their promising values of thermoelectric efficiency, conducting

Film Preparation
Carbon nanotubes (0.05 wt.%) were dispersed in an aqueous solution of DOC (0.1 wt.%). The CNT suspensions were placed in an ultrasound bath for 30 min, followed by 20 min of ultrasonication with a Branson Sonifier 450 (1/2 inch tip, 70% amplitude, continuous mode), while cooling in an ice bath. Finally, the suspensions were placed for 30 min in the ultrasound bath. CNT dispersions were then centrifuged at 4000 rpm for 5 min to discard the nonstabilized CNTs. The assembly of PEDOT nanoparticles and CNT layers was carried out by using the layer-by-layer (LbL) technique via dip coating on a pre-treated polyethylene terephthalate (PET) substrate to improve film adhesion [26]. PET substrates were immersed in a cationic PEDOT: PDADMAC suspension for 5 min, followed by 3 washing steps of dipping in water, immersion in the anionic CNT:DOC suspension for 5 min, and eventually 3 further steps of washing in water. This process results in one deposition sequence of a PEDOT: PDADMAC-CNT:DOC bilayer (bL). This cycle was repeated to deposit the desired number of bilayers. Deposited multilayer films were washed and air-dried overnight, and then stored in a desiccator prior to further processing or characterization. The process of formation of the nanoparticles and the subsequent films is schematically depicted in Figure 1.

Characterization Techniques
The morphological characterization of PEDOT nanoparticles was carried out by transmission electron microscopy (TEM) at an accelerating voltage of at 100 kV in a JEOL JEM-1010 microscope (JEOL Ltd., Japan, coupled with a digital camera MegaView III (GEMSIS GmbH, Germany). Zeta potential measurements of PEDOT:PDADMAC and CNT:DOC suspensions were measured in a Zetasizer Nano ZS (Malvern Instruments), diluting previously the samples in KCl 0.3 M (aqueous solution). Particle size of PEDOT:PDADMAC suspensions was measured by dynamic light scattering (Zetasizer Nano ZS).
The thickness of PEDOT-CNT films was measured by using a profilometer (Dektak 150, Veeco, USA). Reported values represent an average of at least 5 separate measurements of each film. Morphological characterization of the films was carried out by scanning electron microscopy (SEM) by using a Hitachi S-4800 microscope at an accelerating voltage of 20 kV and a working distance of 14 mm for palladium−gold coated surfaces. TEM was also conducted for samples prepared by embedding a small piece of coated PET in Durcupan ACM resin (Sigma-Aldrich), curing overnight, and then cutting cross-sections using an Ultra 45° diamond knife (Diatome, Hatfield, PA). These samples were imaged by using copper grids with the same equipment and accelerating voltage as for the nanoparticles.
For the electrical characterization, four contacts with silver paint were coated on the film surface. The electrical conductivity was measured with a Keithley 2400 SourceMeter equipment by using the Van der Pauw equation: where d is the thickness of the film, R1 and R2 are the electrical resistance along a vertical and horizontal edges, respectively, and σ is the electrical conductivity. The Seebeck coefficient is determined as the ratio between the electrical potential, ∆V, and the temperature difference, ∆T: The electrical potential was measured with an Agilent 34401 A digital multimeter and the temperature difference was measured using PT100 resistors connected to a Lakeshore 340 temperature controller.

Characterization Techniques
The morphological characterization of PEDOT nanoparticles was carried out by transmission electron microscopy (TEM) at an accelerating voltage of at 100 kV in a JEOL JEM-1010 microscope (JEOL Ltd., Japan, coupled with a digital camera MegaView III (GEMSIS GmbH, Germany). Zeta potential measurements of PEDOT:PDADMAC and CNT:DOC suspensions were measured in a Zetasizer Nano ZS (Malvern Instruments), diluting previously the samples in KCl 0.3 M (aqueous solution). Particle size of PEDOT:PDADMAC suspensions was measured by dynamic light scattering (Zetasizer Nano ZS).
The thickness of PEDOT-CNT films was measured by using a profilometer (Dektak 150, Veeco, USA). Reported values represent an average of at least 5 separate measurements of each film. Morphological characterization of the films was carried out by scanning electron microscopy (SEM) by using a Hitachi S-4800 microscope at an accelerating voltage of 20 kV and a working distance of 14 mm for palladium−gold coated surfaces. TEM was also conducted for samples prepared by embedding a small piece of coated PET in Durcupan ACM resin (Sigma-Aldrich), curing overnight, and then cutting cross-sections using an Ultra 45 • diamond knife (Diatome, Hatfield, PA). These samples were imaged by using copper grids with the same equipment and accelerating voltage as for the nanoparticles.
For the electrical characterization, four contacts with silver paint were coated on the film surface. The electrical conductivity was measured with a Keithley 2400 SourceMeter equipment by using the Van der Pauw equation: where d is the thickness of the film, R 1 and R 2 are the electrical resistance along a vertical and horizontal edges, respectively, and σ is the electrical conductivity. The Seebeck coefficient is determined as the ratio between the electrical potential, ∆V, and the temperature difference, ∆T: The electrical potential was measured with an Agilent 34401 A digital multimeter and the temperature difference was measured using PT100 resistors connected to a Lakeshore 340 temperature controller.

Results and Discussion
PEDOT nanoparticles were synthesized by chemical oxidation polymerization in miniemulsion with PDADMAC as a stabilizer, as schematically shown in Figure 1a. During the polymerization of EDOT in miniemulsion, different stages occur. After ultrasonication, EDOT droplets are stabilized by PDADMAC. The observations suggest that when FeTos is added, iron(III) ions move to the EDOT-water interface and may partially oxidize EDOT to PEDOT, resulting in a PEDOT shell. As a consequence, iron (III) ions are reduced to iron(II). Finally, the addition of hydrogen peroxide oxidizes iron(II) to iron(III), completing the oxidation of EDOT to PEDOT. In turn, iron(III) ions are regenerated due to the presence of hydrogen peroxide in the medium. The experimental observations also indicate that hydrogen peroxide is very important to maintain the spherical morphology and to prevent the droplet coalescence [27].
TEM micrographs of the synthesized nanoparticles are shown in Figure 2. The increase of the molar ratio EDOT:FeTos results in a greater aggregation of the particles. However, the stability of the suspension was not affected by this partial aggregation, with the samples being stable even after one month. The particle size of the PEDOT nanoparticles was determined by dynamic light scattering (DLS). The sizes of nanoparticles prepared with EDOT:FeTos molar ratios of 1:1, 1:1.5, and 1:2 were 180 ± 10, 260 ± 20, and 490 ± 70 nm, respectively. These results are in agreement with the observations in TEM images, which point out a higher formation of aggregates at higher contents of oxidant. The statistical treatment of TEM micrographs for the sample obtained at the lowest molar ratio confirms a size distribution centered around 180 nm.

Results and Discussion
PEDOT nanoparticles were synthesized by chemical oxidation polymerization in miniemulsion with PDADMAC as a stabilizer, as schematically shown in Figure 1a. During the polymerization of EDOT in miniemulsion, different stages occur. After ultrasonication, EDOT droplets are stabilized by PDADMAC. The observations suggest that when FeTos is added, iron(III) ions move to the EDOTwater interface and may partially oxidize EDOT to PEDOT, resulting in a PEDOT shell. As a consequence, iron (III) ions are reduced to iron(II). Finally, the addition of hydrogen peroxide oxidizes iron(II) to iron(III), completing the oxidation of EDOT to PEDOT. In turn, iron(III) ions are regenerated due to the presence of hydrogen peroxide in the medium. The experimental observations also indicate that hydrogen peroxide is very important to maintain the spherical morphology and to prevent the droplet coalescence [27].
TEM micrographs of the synthesized nanoparticles are shown in Figure 2. The increase of the molar ratio EDOT:FeTos results in a greater aggregation of the particles. However, the stability of the suspension was not affected by this partial aggregation, with the samples being stable even after one month. The particle size of the PEDOT nanoparticles was determined by dynamic light scattering (DLS). The sizes of nanoparticles prepared with EDOT:FeTos molar ratios of 1:1, 1:1.5, and 1:2 were 180 ± 10, 260 ± 20, and 490 ± 70 nm, respectively. These results are in agreement with the observations in TEM images, which point out a higher formation of aggregates at higher contents of oxidant. The statistical treatment of TEM micrographs for the sample obtained at the lowest molar ratio confirms a size distribution centered around 180 nm. The assembly of PEDOT nanoparticles and CNT layers is controlled by the electrostatic interaction of PDADMAC (cationic polyelectrolyte) and DOC (anionic surfactant). It is thus important to know the surface charge of the nanoparticles and the CNTs. The zeta potential of the synthesized nanoparticles was +19.3 ± 0.5 mV. This positive value indicates that PEDOT nanoparticles are positively charged due to the presence of PDADMAC at the surface. For the prepared CNTs dispersions, the zeta potential was −29.6 ± 0.3 mV, which is consistent with the functionalization with DOC. The zeta potential values confirm that the assembly of PEDOT-CNTs bilayers can be carried out by means of LbL deposition, through electrostatic interactions of the two components. The assembly of PEDOT nanoparticles and CNT layers is controlled by the electrostatic interaction of PDADMAC (cationic polyelectrolyte) and DOC (anionic surfactant). It is thus important to know the surface charge of the nanoparticles and the CNTs. The zeta potential of the synthesized nanoparticles was +19.3 ± 0.5 mV. This positive value indicates that PEDOT nanoparticles are positively charged due to the presence of PDADMAC at the surface. For the prepared CNTs dispersions, the zeta potential was −29.6 ± 0.3 mV, which is consistent with the functionalization with DOC. The zeta potential values confirm that the assembly of PEDOT-CNTs bilayers can be carried out by means of LbL deposition, through electrostatic interactions of the two components. After preparation of the films by the drop-casting method (approximate thickness of 1.5 ± 0.2 µm), their thermoelectric properties were measured. Figure 3 shows the variation of the electrical conductivity, Seebeck coefficient, and power factor as a function of the EDOT:FeTos molar ratio and the type of CNTs. As expected, the electrical conductivity increases with the FeTos content, since the oxidation level of PEDOT is higher when the EDOT:FeTos molar ratio increases. The Seebeck coefficient is also affected by the oxidant content. Normally, the evolution of the Seebeck coefficient is opposite to the electrical conductivity when the oxidation level of conducting polymers changes [28][29][30]. However, in this particular case, both parameters, electrical conductivity and Seebeck coefficient, follow the same trend. This fact can be explained by looking at the nanostructure of the particles. The interconnection degree between particles is greater for an EDOT:FeTos ratio of 1:2 than for 1:1, as a result of the tendency of the particles to agglomerate and create a more connected path, which improves the charger transport across the film. The electrical conductivity of SWCNTs is higher than for the other CNTs (Figure 3b), which is related to the electronic structure. In the case of DWCNTs, which are a subset of MWCNTs, there are four unique permutations of inner@outer wall combinations: semi@semi, metal@metal, semi@metal, and metal@semi [31]. Taking into account that the conductivity of semiconductor nanotubes is smaller, if we extrapolate these combinations to MWCNTs, the probability of having semiconductor nanotubes increases and, therefore, the conductivity decreases [32][33][34]. The Seebeck coefficient reached a value of 55 µV K −1 in agreement with previous work [35].
Coatings 2020, 10, x FOR PEER REVIEW 6 of 13 After preparation of the films by the drop-casting method (approximate thickness of 1.5 ± 0.2 µm), their thermoelectric properties were measured. Figure 3 shows the variation of the electrical conductivity, Seebeck coefficient, and power factor as a function of the EDOT:FeTos molar ratio and the type of CNTs. As expected, the electrical conductivity increases with the FeTos content, since the oxidation level of PEDOT is higher when the EDOT:FeTos molar ratio increases. The Seebeck coefficient is also affected by the oxidant content. Normally, the evolution of the Seebeck coefficient is opposite to the electrical conductivity when the oxidation level of conducting polymers changes [28][29][30]. However, in this particular case, both parameters, electrical conductivity and Seebeck coefficient, follow the same trend. This fact can be explained by looking at the nanostructure of the particles. The interconnection degree between particles is greater for an EDOT:FeTos ratio of 1:2 than for 1:1, as a result of the tendency of the particles to agglomerate and create a more connected path, which improves the charger transport across the film. The electrical conductivity of SWCNTs is higher than for the other CNTs (Figure 3b), which is related to the electronic structure. In the case of DWCNTs, which are a subset of MWCNTs, there are four unique permutations of inner@outer wall combinations: semi@semi, metal@metal, semi@metal, and metal@semi [31]. Taking into account that the conductivity of semiconductor nanotubes is smaller, if we extrapolate these combinations to MWCNTs, the probability of having semiconductor nanotubes increases and, therefore, the conductivity decreases [32][33][34]. The Seebeck coefficient reached a value of 55 µV K −1 in agreement with previous work [35]. The assembly of the PEDOT and CNTs layers was performed according to the procedure shown in Figure 1b, using MWCNT, DWCNT, and SWCNT with the different EDOT:FeTos molar ratios and different numbers of bilayers (10-60 bilayers). Figure 4 shows profilometry measurements of the different systems studied. Initially, the thickness of the film increases progressively up to ca. 2 µm when increasing the number of bilayers. Then, the thickness rises rapidly to 3.5-4 µm with only 10 bilayers more. This fact is anomalous and can be explained by an interdiffusion phenomenon between PDADMAC and DOC. Both charged molecules interact with each other due to the high concentration, forming agglomerates on the surface of the film [36]. This observation is in agreement with the SEM and TEM micrographs of the film cross-sections, presented in Figure 5. The assembly of the PEDOT and CNTs layers was performed according to the procedure shown in Figure 1b, using MWCNT, DWCNT, and SWCNT with the different EDOT:FeTos molar ratios and different numbers of bilayers (10-60 bilayers). Figure 4 shows profilometry measurements of the different systems studied. Initially, the thickness of the film increases progressively up to ca. 2 µm when increasing the number of bilayers. Then, the thickness rises rapidly to 3.5-4 µm with only 10 bilayers more. This fact is anomalous and can be explained by an interdiffusion phenomenon between PDADMAC and DOC. Both charged molecules interact with each other due to the high concentration, forming agglomerates on the surface of the film [36]. This observation is in agreement with the SEM and TEM micrographs of the film cross-sections, presented in Figure 5.  For 30 bilayers (Figure 5a,b), PEDOT nanoparticles are uniformly distributed over the MWCNTs fibers due to the electrostatic interactions between PDADMAC and DOC. The morphology of these nanoparticles remains essentially spherical. However, for 40 bilayers (Figure 5c,d), agglomerates of PEDOT nanoparticles that cover the nanotubes are observed on the surface of the films. These agglomerates increase the film thickness and the proportion of insulating material at the surface. TEM images of the cross-section of 30 and 40 bilayer films using MWCNTs (Figure 5e,f) indicate again an interdiffusion phenomenon, with a noticeable increase of the film thickness. Figure 5f shows that the formation of the first layers of MWCNT-PEDOT nanoparticles proceeds uniformly, but when reaching about 2 µm, the film formation is less uniform, with a much greater amount of insulating material. Photographs of the films obtained with 10 to 60 bilayers, shown in Figure 6, demonstrate how the homogeneity of the film is gradually lost with increasing the number of bilayers. Figure 7 shows the thermoelectric parameters of the different systems as a function of the number of bilayers. The electrical conductivity increases until reaching 30 (in case of MWCNTs) or 40 bilayers (for DWCNTs and SWCNTs). Then, it decreases due to the interdiffusion phenomenon between PDADMAC and DOC, which increases the proportion of insulating material on the surface of the film, as already described above. On the other hand, according to the Van der Pauw method for measuring electrical conductivity, an increase in thickness leads to a decrease in electrical conductivity [37]. The best result of electrical conductivity, with values up to 35 S cm −1 , was obtained by using SWCNTs with PEDOT nanoparticles with an EDOT:Fe-Tos molar ratio of 1:2. The Seebeck coefficient has a similar tendency: it increases until 40 bilayers and then it decreases because the agglomerates of PDADMAC and DOC hinder the passage of the current produced by the difference of temperature. Using SWCNTs with PEDOT nanoparticles at EDOT:FeTos molar ratio of 1:2, the Seebeck coefficient reached a maximum of 145 µV K −1 , higher than water-based polymer emulsion methods containing SWCNTs and PEDOT:PSS [9]. As the electrical conductivity increases with the number of bilayers, the Seebeck coefficient remains relatively constant. This decoupling between the Seebeck coefficient and the electrical conductivity does not occur in conventional thermoelectric bulk materials, which is explained by the fact that, in the composites with CNT, the thermal conductivity decreases and the electrical conductivity is improved [9]. Finally, the power factor follows the same trend as the electrical conductivity: it increases progressively until 30 (MWCNTs) or 40 bilayers (DWCNTs and SWCNTs) and then sharply decreases. The best power factor was 72 µW m −1 K −2 , achieved by using SWCNTs with PEDOT nanoparticles at an EDOT:FeTos molar ratio of 1:2. This value is three orders of magnitude higher than the power factor of pristine PEDOT nanoparticles prepared at the same molar ratio. We suggest that this fact might be explained by the synergistic π−π interaction between the benzene ring of the CNTs and the aromatic ring of the PEDOT, which induces a greater ordering of the polymeric chain thus improving thermoelectric properties. Interestingly, this value is also higher than previously reported ones for different PEDOT-based materials, including polymer emulsions of PEDOT:PSS/SWCNT/Arabic-gum [9], PEDOT:PSS/SWCNT deposited by spin-casting [38], composites by in situ polymerization of EDOT in the presence of MWCNT and graphene stabilized by PSS [39], and flexible thermoelectric composite films of polypyrrole and carbon nanotubes [40].   For 30 bilayers (Figure 5a,b), PEDOT nanoparticles are uniformly distributed over the MWCNTs fibers due to the electrostatic interactions between PDADMAC and DOC. The morphology of these nanoparticles remains essentially spherical. However, for 40 bilayers (Figure 5c,d), agglomerates of PEDOT nanoparticles that cover the nanotubes are observed on the surface of the films. These agglomerates increase the film thickness and the proportion of insulating material at the surface. TEM images of the cross-section of 30 and 40 bilayer films using MWCNTs (Figure 5e,f) indicate again an interdiffusion phenomenon, with a noticeable increase of the film thickness. Figure 5f shows that the formation of the first layers of MWCNT-PEDOT nanoparticles proceeds uniformly, but when reaching about 2 µm, the film formation is less uniform, with a much greater amount of insulating material. Photographs of the films obtained with 10 to 60 bilayers, shown in Figure 6, demonstrate how the homogeneity of the film is gradually lost with increasing the number of bilayers.    Figure 7 shows the thermoelectric parameters of the different systems as a function of the number of bilayers. The electrical conductivity increases until reaching 30 (in case of MWCNTs) or 40 bilayers (for DWCNTs and SWCNTs). Then, it decreases due to the interdiffusion phenomenon between PDADMAC and DOC, which increases the proportion of insulating material on the surface of the film, as already described above. On the other hand, according to the Van der Pauw method for measuring electrical conductivity, an increase in thickness leads to a decrease in electrical conductivity [37]. The best result of electrical conductivity, with values up to 35 S cm −1 , was obtained by using SWCNTs with PEDOT nanoparticles with an EDOT:Fe-Tos molar ratio of 1:2. The Seebeck coefficient has a similar tendency: it increases until 40 bilayers and then it decreases because the agglomerates of PDADMAC and DOC hinder the passage of the current produced by the difference of temperature. Using SWCNTs with PEDOT nanoparticles at EDOT:FeTos molar ratio of 1:2, the Seebeck coefficient reached a maximum of 145 µV K −1 , higher than water-based polymer emulsion methods containing SWCNTs and PEDOT:PSS [9]. As the electrical conductivity increases with the number of bilayers, the Seebeck coefficient remains relatively constant. This decoupling between the Seebeck coefficient and the electrical conductivity does not occur in conventional thermoelectric bulk materials, which is explained by the fact that, in the composites with CNT, the thermal conductivity decreases and the electrical conductivity is improved [9]. Finally, the power factor follows the same trend as the electrical conductivity: it increases progressively until 30 (MWCNTs) or 40 bilayers (DWCNTs and SWCNTs) and then sharply decreases. The best power factor was 72 µW m −1 K −2 , achieved by using SWCNTs with PEDOT nanoparticles at an EDOT:FeTos molar ratio of 1:2. This value is three orders of magnitude higher than the power factor of pristine PEDOT nanoparticles prepared at the same molar ratio. We suggest that this fact might be explained by the synergistic π−π interaction between the benzene ring of the CNTs and the aromatic ring of the PEDOT, which induces a greater ordering of the polymeric chain thus improving thermoelectric properties. Interestingly, this value is also higher than previously reported ones for different PEDOT-based materials, including polymer emulsions of PEDOT:PSS/SWCNT/Arabic-gum [9], PEDOT:PSS/SWCNT deposited by spin-casting [38], composites by in situ polymerization of EDOT in the presence of MWCNT and graphene stabilized by PSS [39], and flexible thermoelectric composite films of polypyrrole and carbon nanotubes [40]. Finally, the flexible behavior of the prepared films was determined by measuring the electrical conductivity by performing up to 3000 bends on a cylinder with a radius of 2 cm. Figure 8 shows the flexible behavior of the film of 20 bilayers based on SWCNT and PEDOT nanoparticles with an EDOT:FeTos molar ratio of 1:2. The electrical conductivity remains practically constant, decreasing only 6% after 3000 bends, which indicates that there is no layer delamination or decomposition of the films during the bending. The observations demonstrate that multilayer materials based on carbon nanotubes and nanostructured conducting polymers are potentially suitable materials for flexible thermoelectric devices. Finally, the flexible behavior of the prepared films was determined by measuring the electrical conductivity by performing up to 3000 bends on a cylinder with a radius of 2 cm. Figure 8 shows the flexible behavior of the film of 20 bilayers based on SWCNT and PEDOT nanoparticles with an EDOT:FeTos molar ratio of 1:2. The electrical conductivity remains practically constant, decreasing only 6% after 3000 bends, which indicates that there is no layer delamination or decomposition of the films during the bending. The observations demonstrate that multilayer materials based on carbon nanotubes and nanostructured conducting polymers are potentially suitable materials for flexible thermoelectric devices.

Conclusions
Hybrid thermoelectric flexible films with high Seebeck coefficient were prepared through layerby-layer (LbL) assembly by using as building blocks PEDOT nanoparticles functionalized with

Conclusions
Hybrid thermoelectric flexible films with high Seebeck coefficient were prepared through layer-by-layer (LbL) assembly by using as building blocks PEDOT nanoparticles functionalized with PDADMAC and different types of carbon nanotubes functionalized with DOC. Depending on the EDOT:FeTos molar ratio used during the nanoparticle synthesis, the electrical conductivity and the Seebeck coefficient increase in parallel to the molar ratio. The maximum power factor was achieved at an EDOT:FeTos molar ratio of 1:2. Thanks to the electrostatic interaction of PDADMAC with DOC, the layers of the films grew homogeneously. However, when the film reached 30 or 40 bilayers (for MWCNTs or DWCNTs/SWCNTs, respectively) an interdiffusion phenomenon of the components appeared, as observed by SEM and TEM, and the proportion of insulating material increased. This fact influence negatively the thermoelectric properties and the homogeneity, so that we conclude that 30 and 40 bilayers are the limit for these materials. The maximum power factor of the hybrid flexible films was achieved for 40 bilayers at an EDOT:FeTos molar ratio of 1:2 and SWCNT. According to the obtained results, PEDOT nanoparticles with carbon nanotubes, especially SWCNTs, are very suitable candidates to make flexible films for thermoelectric applications.