Noshin Fatimaa,
Fakhra Aziz*b,
Zubair Ahmad*c,
M. A. Najeebc,
M. I. Azmeerb,
Kh. S. Karimovde,
M. M. Ahmeda,
S. Basheerb,
R. A. Shakoorc and
K. Sulaimanb
aDepartment of Electrical Engineering, Capital University of Science and Technology, Pakistan
bLow Dimensional Material Research Center, Department of Physics, University of Malaya, Kuala Lumpur 50603, Malaysia. E-mail: fakhra69@yahoo.com; Tel: +60 14 2746400
cCenter for Advanced Materials (CAM), Qatar University, P. O. Box. 2713, Doha, Qatar. E-mail: zubairtarar@qu.edu.qa; Tel: +974 4403 7729
dGhulam Ishaq Khan Institute of Engineering Sciences and Technology, Pakistan
eCentre for Innovative Development of Science and Technologies of Academy of Sciences, Tajikistan
First published on 4th April 2017
This study exhibits a solution-processed organic semiconductor humidity sensor based on vanadyl 2,9,16,23-tetraphenoxy-29H,31H-phthalocyanine (VOPcPhO), tris-(8-hydroxy-quinoline)aluminum (Alq3), and their composites. Compositional engineering of the VOPcPhO:Alq3 complex was performed to develop a sensitive humidity sensor with a linear response. Thin films of VOPcPhO, Alq3, and composites were spin-coated over pre-deposited aluminum (Al) electrodes, whereas the other electrodes were deposited through a thermal evaporation technique. Both capacitive and resistive responses were measured as a function of different relative humidity levels. Morphological and structural properties of the organic thin films were characterized by atomic force microscopy (AFM), field emission scanning electron microscopy (FESEM), and Fourier transform infrared spectroscopy (FTIR). Compared to the VOPcPhO and Alq3 stand-alone sensors, the VOPcPhO:Alq3 composite-based sensor demonstrated superior performance with significantly improved sensing parameters, highlighting unique advantages of the low-molecular composite-based thin film organic humidity sensors.
Humidity is a universal phenomenon because of the general presence of moisture contents in air. Control or measurement of humidity is becoming more important, not only for human well-being but also for various industrial applications such as meteorology, process control techniques, agriculture, and medical equipment. Based on requirements or applications, various kinds of humidity sensors are used and they can be classified based on their sensing mechanisms. Humidity sensors based on inorganic materials10,11 are costly, and require high power for operation, whereas organic material-based humidity sensors have advantages of low cost, light weight, flexibility, and simple technology.
Even though organic materials are highly responsive to humidity, many of them are easily dispersed in water12,13 which makes them impractical in highly humid conditions. Among organic materials, the phthalocyanines group has hydrophobic properties and is insoluble in water and hence, is considered as a good candidate for humidity meters.14 Phthalocyanines are macro-cyclic and hetero-cyclic compounds which exhibit a ring structure containing nitrogen atoms in addition to carbon as a part of the ring. Most phthalocyanines are considered as p-type semiconductors15 and they possess sufficiently good charge carrier mobility16 and significant conductivity for utilization in potential applications with organic electronic devices. Among the phthalocyanines, VOPcPhO is available as a green colored dye that is insoluble in water. It exhibits very good chemical and environmental stability and has been extensively studied for various types of sensors17–21 whereas Alq3 is a pi-conjugated small molecular material.22 In pi-conjugated materials, single and double or single and triple bonds alternate throughout the backbone of a molecule. The second and third bonds of a double or triple bond are pi-bonds.23 The gap between LUMO and HOMO is typically in the 1.5–3 eV range, i.e. the materials are organic semiconductors.23 Even though Alq3 is mostly utilized as an exciton blocking layer and a light emitting layer in photovoltaic applications, it can be utilized to obtain a high-quality thin film with high electron mobility by a simple spin-coating method.24
In this work, the compositional engineering of the pi-conjugated small molecular VOPcPhO:Alq3 complex was performed to develop a sensitive humidity sensor with a linear response. The bulk heterojunction of the two materials was expected to have the characteristics of the both components and is assumed to be more linear in response towards humidity than VOPcPhO and more sensitive than Alq3 alone. The aim of this research is to boost the humidity sensing potential of VOPcPhO by making its complex with Alq3 to develop a cheap and reliable sensing element for assessing humidity in the surrounding environment.
Fig. 2 Capacitance vs. humidity sensing behavior of (a) Alq3, (b) VOPcPhO, (c) composite (VOPcPhO:Alq3) at various ambient temperatures, and (d) resistance response of the best selected sensors i.e. composite (V1:A2)@75 °C, Alq3@125 °C, and VOPcPhO@25 °C. The capacitance measurement was recorded at 100 Hz frequency and the frequency–capacitance response is presented in Fig. S2 in a ESI file.† Normalized capacitance to temperature response of the desired composite at (a) 25 °C and (b) 75 °C is shown in Fig. S4.† |
Many factors, including porosity of the sensing films, dielectric constant, the material's dynamic sensing area, and polarizability, significantly participate in capacitance/resistance variation in response to ambient relative humidity levels. Relative permittivity of organic-based materials with small molecular sizes lies between 4–8;25 on the other hand, water permittivity is ∼80.4 The dielectric constant of water remarkably increases capacitance of a sensor because of a large difference between the relative permittivity of water and active thin film of respective materials and their composites. Fig. 2d shows the relationship between resistances vs. relative humidity levels for the composites (V1:A2)@75 °C, Alq3@125 °C, and VOPcPhO@25 °C based humidity sensors. The sensitivity of composite (V1:A2), Alq3, and VOPcPhO was found to be 14.5, 12.81, and 9.68, respectively. It was observed that the resistance responses of VOPcPhO and Alq3 were more obvious in the range of 15–60% RH; after that they seem to tend to be saturated values. However, in the case of V1:A2, the resistive device was sensitive over the whole measured range.
Surface morphology of thin films of Alq3, VOPcPhO, and their composites was studied using atomic force microscopy (AFM) and field emission scanning electron microscope (FESEM). Fig. 3 shows the AFM and FESEM micrographs of VOPcPhO annealed at@25 °C (Fig. 3a and b), Alq3 annealed at@125 °C (Fig. 3c and d), and composite VOPcPhO:Alq3 annealed at@75 °C (Fig. 3e and f), respectively. Micrographs of the composite films (Fig. 3e and f) display a rough surface with uniform distribution of the textured appearance. The image of Fig. 3e indicates that the Alq3:VOPcPhO composite thin film, when annealed at 75 °C, results in much rougher surface with a sharp peak like structures. The rms roughness measured for VOPcPhO and Alq3 thin films were 0.832 nm and 0.597 nm, respectively. The composite film V1:A2 has rms roughness of 0.937 nm which exhibits a slightly rougher surface than the stand-alone films. The annealed composite thin film provides more absorption sites for moisture content to be adsorbed. Sensitivity of the humidity sensors depends upon the amount of water absorbed corresponding to the increased surface area. It can be inferred that the greater roughness with uniform distribution leads to larger surface area exposure and more moisture adsorption as well.26 Sensitivity (S) of the humidity sensors can be assessed by using the following equations:27 S(R) = ΔR/ΔRH and S(C) = ΔC/ΔRH, where ΔR, ΔC and ΔRH are increments in resistance, capacitance, and change in the relative humidity, respectively. A summary of the devices is described in Table 1.
Fig. 3 AFM images of (a) VOPcPhO@25, (c) Alq3@125, (e)V1:A2@75, and FESEM (b) VOPcPhO@25, (d) Alq3@125, and (f) V1:A2@75. |
S. no | Thin film | Annealing temperature (°C) | Sensitivity SSC (pF/%) | Sensitivity SSR (MΩ/%) | τres (s) | τrec (s) | Surface roughness (nm) |
---|---|---|---|---|---|---|---|
1 | VOPcPhO | 25 | 1.06 | 9.68 | 13 | 8 | 0.83 |
2 | Alq3 | 125 | 0.3125 | 12.81 | 6 | 4 | 0.57 |
3 | V1:A2 | 75 | 0.325 | 14.5 | 4 | 3 | 0.937 |
The chemical bonding structures of Alq3, VOPcPhO, and their blend thin films were investigated by FTIR and the results are shown in Fig. 4. In line (a), CC aromatic stretching vibrations are observed in the range of 1601–1497 cm−1. The absorption bands at 1385 cm−1 to 1114 cm−1 represent the resonance of aromatic amine (C–N–C).28 The band at 918 cm−1 is due to an Al–N stretching vibration. Moreover, out-of-plane quinoline CH wagging vibration can be seen at 744 cm−1. The weaker band at 555 cm−1 originates from the stretching vibration of Al–O.29 Line b in Fig. 4 represents the characteristic spectrum of VOPcPhO. The peak at 1057 cm−1 shows the presence of a single V–O stretching motion which was already reported by Miller and Cousins.30 This peak has been assigned to shorter V–O bonds. However, the peak at 895 cm−1 also shows the presence of V–O bonds but this band is due to the characteristic of longer V–O bonds.31 Moreover, the band at 746 cm−1 corresponds to out-of-plane C–H bending modes and this peak is a characteristic of almost all phthalocyanines.32 The FTIR of the blend of Alq3 and VOPcPhO is presented in Fig. 4 (line c).
Response times τres and recovery times τrec for Alq3, VOPcPhO, and their composite (V1:A2) are given in Fig. 5a–c; they are 6 s, 13 s, and 4 s and 4 s, 8 s, and 3 s, respectively. The response and recovery time of the composite is better than others. The response time and recovery time of the sensors were measured as follows: initially the sensors were placed in a sealed chamber with 20% RH and then they were exposed to an environment with 70% RH level, thereby enabling them to adsorb water vapor and hence increasing their capacitance. The recovery time of a sensor was achieved by first exposing it to a humidity level of 70% RH and then immediately back to 20% RH. Fig. 5d–f show the hysteresis of Alq3, VOPcPhO, and their composites at the ratio V1:A2 at 100 Hz frequency. The up and down arrows show the increase and decrease in % RH, respectively.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra02525d |
This journal is © The Royal Society of Chemistry 2017 |