Metallophthalocyanines are p-type semiconductors which possess very interesting optical and electrical properties. Due to their low cost of production, high thermal and chemical stability, metallophthalocyanines, especially in the form of thin films, can be applicable in many advanced technological devices [1–3]. Thin layers of metallophthalocyanines (MPc) as well as their junctions with a number of organic and inorganic semiconductors or metals can be applicable in optoelectronics as for example light-emitting diodes, photovoltaic cells, and organic field effect transistors. Charge injection at the interface between metallic electrodes and organic semiconductors are crucial for the performance of organic optoelectronic devices. Moreover, the metallophthalocyanines are very useful as transporting and injection layers in optoelectronic devices [4, 5]. For this reason the knowledge of their optical and electrical properties is very important.
Due to these exceptional properties, thin films of metallophthalocyanine have been recently intensively investigated especially by the optical methods such as absorption, ellipsometry, harmonic generation and Raman spectroscopy [6–11]. The Raman spectroscopy can be a useful tool to study various intra- and intermolecular energy transfer processes.
In order to improve devices technology, the deposition technique must provide a film with reproducible electrical and optical response characteristics.
In case of CoPc thin films, the knowledge of the surface morphology and the preferred orientation of the crystallites and their electrical parameters are essential for potential successful applications. The preferred orientation is usually determined by sample preparation conditions such as type of substrate, method of evaporation and deposition temperature. Very important are also heating and cooling processes of organic thin layers, which in many cases lead to the changes in polymorphic forms and structure arrangement, changing the physical properties of the layer. In case of CoPc the structure at room temperature is determined by flat molecules with D4h symmetry . The heating process changes the polymorphic form of the layer changing also its physical, electrical and optical properties.
In this paper, we present the results of the research on the structural orientation and electrical parameters of CoPc thin films deposited on silicon substrate.
The main aim of our work was to determine the CoPc molecular orientation and distribution of polymorphic phases. The electrical parameters of p-n junction (p-CoPc/n-Si - organic diode) were also investigated.
2.1 Preparation of the thin films
The cobalt phthalocyanine (CoPc) layers have been prepared in a vacuum chamber at a pressure of about p = 2 × 10–4 Pa. Purified CoPc powder (97 % Sigma Aldrich, Co.) was loaded onto a quartz effusion cell with a nozzle of 3 mm in diameter on the top. The n-type (0 0 1)Si substrates, which before loading into the vacuum chamber, were sonificated in acetone, distilled water, isopropanol, and finally in distilled water. During evaporation process the Si substrates were held at room temperature. The deposition rate of thin CoPc layers was 0.2 nm/s.
2.2 Raman scattering spectroscopy
The Raman scattering spectra (RS) of cobalt phthalocyanine (CoPc) were recorded by Renishaw inVia micro-Raman system. As an excitation source, a 488 nm wavelength from ion argon laser was used. The spectral range was chosen from approximately 1000 cm-1 to 1800 cm-1. Two types of polarized RS were collected in the scattering geometry VV and VH. Motorized stages were used to perform Raman surface mapping measurements. The laser beam was focused on the sample by a Leica microscope objective (magnification × 100) with numerical aperture (NA) equal to 0.85. Those parameters correspond to laser spot diameter about 1 μm. To prevent any damages caused by excessive excitation power, the power was fixed at 1 mW. Raman maps were measured on a surface of 20 μm2 × 20 μm2 with a step of 2 μm. Because all measurements were recorded in backscattering geometry we could neglect the angle dependence of reflection coefficients of both thin layer and substrate for different polarizations of the incident light.
2.3 Atomic force spectroscopy
Atomic Force Microscopy (AFM) images were performed with use of Catalyst Bruker Nanoscope. Height images were recorded using silicon nitride cantilevers with a spring constant of 0.4 N/m and resonant frequency 70 kHz. All images were recorded in tapping mode and at room temperature.
2.4 I-V measurements
Current-voltage measurements (I-V characteristics) were carried out using Keitley 6485 picoammeter within voltage range —5 V to +5 V using homemade software to support the picoammeter voltage source and collection of measured I-V data. I-V characteristics were carried out at different temperatures in the range of 210 K to 440 K. During electrical measurements organic thin layer was electrically insulated from external conditions.
3 Results and discussion
It has been shown that the orientation of metal phthalocyanine thin films relatively to the surface can be determined by different approaches. The angle of inclination of a molecule plane to the substrate can be resolved by electron diffraction techniques or high resolution transmission electron microscopy (HRTEM). Polarization Raman study of films allows one to define the structural parameters (polymorphism of the molecules). As the advantages of Raman spectroscopy, high spatial resolution, absence of substrate influence and lack of requirements on sample preparation can be mentioned.
At room temperature CoPc molecule is planar and possesses D4h point group symmetry. The determination of orientation of phthalocyanine molecules layer from Raman scattering measurements was based on the analysis of external molecular vibration. The method which allows one to determine the inclination angle of the molecules of phthalocyanine to the substrate was proposed by Kolesov .
where A1g, B1g, B2g and Eg modes are Ramanactive. The nondegenerate A1g, B1g, B2g modes are in-plane vibrations, and double degenerate Eg are out-of-plane vibrations.
It is crucial to know the IVV/IVH ratio of symmetry types vibrations (A1g, B1g) to estimate the molecular orientation (polymorphic form of molecules/CoPc), where IVV and IVH are integral intensities of Raman scattering for vertical and horizontal polarization of scattered light, respectively. The inclination angle of the molecule plane to the substrate plane is calculated from intensities ratio IVV/IVH for B1g Raman mode achieved from Raman spectra. The detailed description has been given in our previous works [13–15]. The angle β is a parameter representing the angle between molecule plane and substrate surface. This can be obtained from the following formula:
The molecular orientation of CoPc thin film was investigated for a film with the thickness equal to 300 nm. Fig. 1 shows the polarized Raman spectra (VV and VH) of CoPc 300 nm thin film on silicon substrate obtained before annealing process.
The position of the most intense band (B1g Raman mode) is 1542 cm-1 and is associated with the cobalt ion (Co2+) adapted to the phthalocyanine molecule and can be designated by the displacement of C-N-C bridge bonds of molecule macrocycle. From the previous study it is known that for different metal atoms substituted in the center of phthalocyanine the energy of B1g band is related to the mass of the metal atom, metal ion size and diameter of phthalocyanine cavity [13–15]. In Fig. 1, it can be seen that the intensity of Raman spectrum recorded at parallel polarization of scattered light (VV) is approximately 3 times higher than for the spectrum recorded at cross polarization (VH).
In order to determine and assess the distribution of inclination angle of molecules surface, Raman mapping measurements were performed before and after the annealing process. The procedure was conducted at temperature 473 K for 6 hours in air condition. Each map (Fig. 2) covers an area of 20 μm2 × 20 μm2, and consists of 121 point measurements (done every 2 μm). Using numerical procedure, each spectrum was fitted to the theoretical Lorentz curve (using Wire 3.0 inVia software) to obtain integral intensity of B1g pyrrole stretch Raman mode at 1542 cm-1. Using relation 2 the intensities ratio and then the angle between molecule and substrate were calculated. An average angle of inclination for CoPc 300 nm film before annealing process was calculated from the map (Fig. 2a) and was 41.35°. After the annealing procedure (Fig. 2b) the angle of inclination slightly decreased to the value of 41.15°. Both values are very close to each other and when the standard deviation is taken into account, it can be assumed that they are equal. The estimated values of the inclination angles show that CoPc 300 nm film deposited on silicon had the β polymorphic form before and after annealing (β-form is equal to 40° to 49°). Important is the fact that the distribution of the angle on the measured surface changes after the annealing process . Additionally, we present in Fig. 3 the distribution of the molecular form for CoPc thin layers before and after annealing process.
In our case (300 nm thick film), dominant form of molecular orientation is β orientation. This feature can be explained in terms of different molecule-substrate and molecule-molecule interactions. For various growth processes, the strength of molecule-substrate and molecule-molecule interactions is a crucial parameter which can be changed by different chemical substitutions. The metal-substrate interaction is particularly crucial for the first few layers of the molecules on the metal substrate, whereas for higher coverages the molecule-substrate interaction becomes negligible. Thus, for thicker layers we obtain β polymorphic form, where the dominant interaction is molecule-molecule interaction.
In order to compare the results obtained from Raman mapping before and after the annealing process the AFM studies for CoPc film were performed. AFM images were made for an area of 10 μm2 × 10 μm2. The analysis of AFM images was carried out using Gwydion 2.33 software. The results achieved for a studied film before and after annealing process are shown in Fig. 4a and Fig. 4b, respectively. To investigate the structure of the thin layer, couple of parameters evaluated from AFM images were used. Root mean square (RMS) roughness was calculated at 6.37 and 20.8 nm before and after annealing, respectively. Almost threefold increase of RMS roughness is probably caused by the presence of oxygen during the annealing process [17, 18].
The annealing process was carried out in air. Annealing of a film leads to oxidation of cobalt phthalocyanine with adsorbed oxygen. In the annealed films, the rod like crystals deform and become small particles as a result of the oxidation of MPc with adsorbed oxygen. Therefore, the formation of the fine particles may proceed as a result of the interaction between the absorbed oxygen and phthalocyanine. This in turn, increases the porosity and, thus, the surface roughness, which is observed by AFM technique. It shows the β phase films which consist of larger grain size than before the annealing process.
Despite this fact, the average grain size increased from 71.37 nm (before annealing) to 83.97 nm (after annealing) . As can be seen in Fig. 4, very well defined globular structures are observed, which can be connected with similar results from our previous work . After the annealing process, we obtained more homogenous structure, where the grains (with larger diameter) form aggregates and flake-like structure. Prolonged annealing process caused an increase in the value of the parameters characterizing the surface which are collected in Table 1. In this Table we have compiled the most important parameters characterizing surface, obtained from AFM of CoPc images recorded before and after annealing process such as: grain size, average roughness, roughness RMS, average height, maximum height, ratio of average height to maximum height.
Fig. 5 shows the current density-voltage characteristics (J-V) of Au/CoPc/n-Si/Al structure under forward and reverse bias, performed under dark current conditions before annealing process in temperature range of 216 K to 432 K within voltage range —5 V to +5 V. Fig. 6 shows current-voltage characteristics (I-V) of Au/CoPc/n-Si/Al before and after annealing process obtained at room temperature . The series resistance (Rs) and the shunt resistance (Rsh) are directly related to the device performance, determined from the plot of the junction resistance (Rj) against voltage where:
which was determined from the current-voltage characteristics and Rj plotted versus voltage. The series and shunt resistances (Rs and Rsh), which are important factors in improving cell performance and design, obtained at room temperature by the method presented in the literature , using the relation between junction resistance, Rj, and the applied voltage, V, are shown in Fig. 7.
As observed in Fig. 7, at sufficiently high forward bias, the junction resistance approaches a constant value characterizing the series resistance Rs ≈ 5.2 kΩ. In addition, in Fig. 7, the junction resistance shows almost constant value at sufficiently high reverse bias, which equals the diode shunt resistance Rsh Ω 5.69 MH.
Thus, we can observe changes in current characteristics due to the annealing process of thin film structure. This is probably due to the reorientation of the molecules and alignment of the molecular structure of the organic thin film during long time annealing process. It is known from our previous work that prolonged annealing process causes changes in the polymorphic forms of MPc thin layer structure [14, 15].
Using Cheung’s functions and thermionic emission theory [23, 24] describing the current-voltage characteristics and the resulting electrical parameters for semiconductors, we calculated electrical parameters of the Au/CoPc/n-Si/Al structure such as series resistance and potential barrier for Au/CoPc/n-Si/Al structure before and after annealing process. These parameters are shown in Table 2.
The electrical conductivity of phthalocyanines is very sensitive to the presence of adsorbed oxygen in the organic thin films. The annealing process in air causes adsorption of oxygen on the surface of the thin film. Adsorbed oxygen causes creation of the depletion region and next oxygen diffuses into the crystalline organic film. This, in turn, increases surface roughness. This fact can be ascribed to the increase in the conductivity of CoPc layer induced by oxygen adsorption, which causes a change of the capacity of the thin layer. The model proposed here assumes that oxygen molecules diffuse into the CoPc film and act as electron acceptor sites. In this case, we can observe drastic changes in capacitance-voltage curves and change in electrical properties of the thin layers . Thus, electrical conductivity and surface topography is closely linked to the amount of oxygen adsorbed in the thin film.
The dark current-voltage measurements suggest that the forward current transport in these heterojunctions involves thermionic emission of electrons from n-Si over the CoPc/Si barrier at low forward bias. Moreover, a space-charge-limited transport across the CoPc layer dominates due to the exponential distribution of traps above the valence band in the band gap of the CoPc layer at high forward bias.
In this paper we performed the orientation study of CoPc thin layers deposited on silicon substrate using micro-Raman scattering spectroscopy, AFM measurement and I-V characteristics. It has been shown, that the Raman scattering method, atomic force microscopy (AFM) and current-voltage (I-V) characteristics are very useful to investigate molecular orientation and electrical parameters of molecules deposited on a solid substrate as a potential molecular devices. We have studied how the annealing process affects the optical and electrical characteristics of organic thin film structures. The obtained results showed that the annealing process of the thin layer causes molecular ordering and thus improves the electrical properties of organic thin film. The knowledge of derived parameters is important for modification of the technological process for obtaining thin film structures. From obtained results it can be shown that annealing process improves the structural and electrical properties of the structures. The extracted diode parameters are consistent with those obtained from the techniques of Cheung for organic thin films deposited on Si substrate. It was revealed that annealing process affects the structural organization and homogeneity of organic thin layers. A better description of electrical parameters connected with the orientation and polymorphic form of organic thin layers requires further studies which will be carried out in future.
The Project was supported through the European Union - European Social Fund and Human Capital - National Cohesion Strategy (RS) and in part by the Research Project of Poznan University of Technology 06/65/DSPB/0516.
Simon J., Andre J.J., Molecular Semiconductors, Springer Verlag, New York, 1985. Google Scholar
Hanack M., Turk. J. Chem., 22 (1998), 13.Google Scholar
Kerp H.R., Faassen Van E.E., Chem. Phys. Lett., 332 (2000), 5. Google Scholar
Carpi F., Rossi De D., Opt. Laser Technol., 38 (2006), 292. Google Scholar
Kobayashi N., Curr. Opin. Solid St. M., 4 (1999), 345. Google Scholar
Granito C., Goldenberg L.M., Bryce M.R., Monkman A.P., Troisi L., Pasimeni L., Petty M., Langmuir, 12 (1996), 472. Google Scholar
Hanack M., Lang M., Adv. Mater., 6 (1994), 819.Google Scholar
Brozek-Pluska B., Jarota A., Kurczewski K., Abramczyk H., J. Mol. Struct., 924 - 926 (2009) 338.Google Scholar
Kolesov B.A., Basova T.V., Thin Solid Films, 304 (1997), 166. Google Scholar
Zawadzka A., Plociennik P., Strzelecki J., Pranaitis M., Dabos-Seignon S., Sahraoui B., Thin Solid Films, 545 (2013), 429.Google Scholar
Zawadzka A., Plociennik P., Strzelecki J., Ko-Rcala A., Arof A.K., Sahraoui B., Dyes Pigments, 101 (2014), 212. Google Scholar
Tackley D.R., Dent G., Smith W.E., Phys. Chem. Chem. Phys., 3 (2001), 1419. Google Scholar
Szybowicz M., Runka T., Drozdowski M., Bała W., Wojdyła M., Grodzicki A., Piszczek P., Bratkowski A., J. Mol. Struct., 830 (2007), 14. Google Scholar
Szybowicz M., Runka T., Drozdowski M., Bała W., Grodzicki A., Piszczek P., Bratkowski A., J. Mol. Struct., 704 (2004), 107. Google Scholar
Szybowicz M., Bała W., Fabisiak K., Pa-Procki K., Drozdowski M., Cryst. Res. Technol., 45 (2010), 1265. Google Scholar
Shihub S.I., Gould R.D., Phys. Status Solidi A, 139 (1993), 129. Google Scholar
Dijken Van J.G., Brett M.J., Molecules, 17 (2012), 10119. Google Scholar
Shihub S.I., Gould R.D., Gravano S., Physica B, 222 (1996), 136. Google Scholar
Hussein M.T., Nasir E.M., Kasim T., Senaed F.A., Int. J. Cur. Eng. T., 4 (2014), 3263. Google Scholar
Szybowicz M., Makowiecki J., J. Mater. Sci., 47 (2012), 1522. Google Scholar
Soliman H.S., El-Barry A.M.A., Khosifan N.M., El Nahass M.M., Eur. Phys. J-Appl. Phys., 37 (2007), 1. Google Scholar
Darwish S., El-Zawawi I.K., Riad A.S., Thin Solid Films, 485 (2005), 182. Google Scholar
Cheung S.K., Cheung N.W., Appl. Phys. Lett., 49 (1986), 85. Google Scholar
Wahab F., Sayyad M.H., Khan D.N., Tahir M., Aziz F., Shahid M., Munawar, M.A., Chaudry J.A., Mat. Sci. Semicon. Proc., 26 (2014), 101. Google Scholar
Buchholtz J.C., Appl. Surf. Sci., 1 (1978), 547. Google Scholar
About the article
Published Online: 2016-09-28
Published in Print: 2016-09-01
Citation Information: Materials Science-Poland, Volume 34, Issue 3, Pages 676–683, ISSN (Online) 2083-134X, DOI: https://doi.org/10.1515/msp-2016-0086.
© 2016 Wroclaw University of Technology. This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License. BY-NC-ND 3.0