Effect of Temperature on I-V Characteristic for ZnO/CuO

World Journal of Nuclear Science and Technology, 2018, 8, 128-135 http://www.scirp.org/journal/wjnst ISSN Online: 2161-6809 ISSN Print: 2161-6795 Effect of Temperature on I-V Characteristic for ZnO/CuO Mubarak Dirar1, Farhah Elfadel Omer1, Rawia Abdelgani1, Ali Sulaiman Mohamed2*, Abdelnabi Ali Elamin2, Bashir Elhaj Ahamed2, Mona Ali1, Abdelsakh Suleman Mohamed3 1 Department of Physics, College of Science, Sudan University of Science and Technology, Khartoum, Sudan Department of Physics, Faculty of Science and Technology, Omdurman Islamic University, Omdurman, Sudan 3 Department of Laser Physics, Faculty of Science, Meteorology Alneleen University, Khartoum, Sudan 2 How to cite this paper: Dirar, M., Omer, F.E., Abdelgani, R., Mohamed, A.S., Elamin, A.A., Ahamed, B.E., Ali, M. and Mohamed, A.S. (2018) Effect of Temperature on I-V Characteristic for ZnO/CuO. World Journal of Nuclear Science and Technology, 8, 128-135. https://doi.org/10.4236/wjnst.2018.83011 Received: April 29, 2018 Accepted: July 10, 2018 Published: July 13, 2018 Copyright © 2018 by authors and Scientific Research Publishing Inc. This work is licensed under the Creative Commons Attribution International License (CC BY 4.0). http://creativecommons.org/licenses/by/4.0/ Open Access Abstract Research on nonmaterials has become increasingly popular because of their unique physical, chemical, optical and catalytic properties compared to their bulk counterparts. Therefore, many efforts have been made to synthesize multidimensional nanostructures for new and efficient nanodevices. Among those materials, zinc oxide (ZnO) has gained substantial attention owing to many outstanding properties. ZnO besides its wide band gap of 3.34 eV exhibits a relatively large excitons binding energy (60 meV) at room temperature which is attractive for optoelectronic applications. Likewise, cupric oxide (CuO) has a narrow band gap of 1.2 eV and a variety of chemo-physical properties that are attractive in many fields. Moreover, composite nanostructures of these two oxides (CuO/ZnO) may pave the way for various new applications. So in this thesis, eight samples of CuO/ZnO junction were synthesized and exposed to temperatures 60, 70, 80, 90, 100, 110, 120 and 130. The electrical properties of Schottky diode junctions were analyzed by I-V measurements under the influence of direct solar radiation and, lag of radiation (darkness) which shows the semi-logarithmic I-V characteristic curve of the fabricated photodiodes. Also energy band gap was estimated and the morphology and particle sizes of the as-prepared sample were determined by SEM. The SEM images of ZnO + CuO sample films were annealed at 60˚C to 130˚C step 10. Keywords Copper Oxide, Zinc Oxide, Thin Films, Monoethanolamine, Temperature, Current-Voltage (I-V) Characteristic 1. Introduction During the last few decades, nanomaterials have been the subject of extensive DOI: 10.4236/wjnst.2018.83011 Jul. 13, 2018 128 World Journal of Nuclear Science and Technology M. Dirar et al. interest because of their potential use in a wide range of fields like, optoelectronics, catalysis and sensing applications. The physical and chemical properties of nanomaterials can differ significantly from their bulk counterpart because of their small size. In general, nanomaterials comprised novel properties that are typically not observed in their conventional, bulk counterparts. Nanomaterials have a much larger surface area to volume ratio than their bulk counterparts, which is one of the bases of their novel physical and/or chemical properties. Nanomaterials are classified into one-dimensional (1D), two-dimensional (2D) and three-dimensional (3D). In addition, metal oxide nanomaterials have drawn a particular attention because of their excellent structural flexibility combined with other attractive properties. These metal oxides nanostructures not only inherit the fascinating properties from their bulk form such as piezoelectricity, chemical sensing, and photo detection, but also possess unique properties associated with their highly anisotropic geometry and size confinement [1]. The combinations of the new and the conventional properties with the unique effects of nanostructures make the investigation of novel metal oxide nanostructures a very important issue in research and development both from fundamental and industrial standpoints. Among the various metal oxides, zinc oxide (ZnO) possessed a considerable attention due to its unique properties and applications. In particular, ZnO nanostructures (NSs) are of intense interest since they can be grown by a variety of methods with different morphologies. Among the different growth methods, the chemical bath deposition method is low temperature, simple, inexpensive and environmentally friendly method. These are all factors which further contribute to the resurgent attention in ZnO. Specifically, one-dimensional ZnO nanorods (NRs) amongst other nanostructures are attractive components for manufacturing nanoscale electronics and photonic devices as well as their biomedical applications because of their interesting chemical and physical properties [2] [3]. Also ZnO NRs can easily be grown on a variety of substrates like metal surface, semiconductors, glass, plastic and disposable paper substrates etc. [4] [5] [6] [7]. Furthermore, a direct wide band gap ~3.37 eV and relatively large excitonic binding energy ~60 meV of ZnO along with many radiative deep level defects, make ZnO attractive for its emission tendency in blue/ultraviolet and full colour lighting [8] [9]. To utilize theses properties of ZnO in LEDs application, another p-type material is necessary as ZnO NRs is unintentionally n-type material. Since mostly polymers are p-type and their special properties, like low cost, low power consumption, flexible and easy manufacturing, all make polymers a better choice to use with ZnO NRs to fabricate a flexible device that utilizes the properties of both materials for large area lighting and display application [10] [11]. On the other hand, natural abundance of copper (II) oxide (CuO) as well as its low production cost, good electrochemical and catalytic properties makes the copper oxide to be one of the best materials for various applications. CuO also DOI: 10.4236/wjnst.2018.83011 129 World Journal of Nuclear Science and Technology M. Dirar et al. has a variety of nanostructures and can be grown using the low temperature aqueous chemical method. It is one of the most important catalysts and is widely used in environmental catalyst. 2. Materials and Methods 2.1. Growth of CuO Thin Films Copper oxide (CuO) thin films were prepared by dissolving 0.2 molar copper acetate and monoethanolamine in a 1:1 Molar ratio in 20 ml of 2-methoxyethanol solvent. Acetic acid was added drop wise to achieve a homogeneous solution. The above stock solution was vigorously stirred at 80˚C for 120 min. The Cu aqueous solution was filtered through a 0.2 μm poly-tetrafluoroethylene membrane and was aged for 24 h. The colour of the solvent became dark green. The precursor solution was uniformly deposited on cleaned ITO glass substrates by spin coating technique at a spin speed of 2000 rpm for 60 s. The coating process was repeated to attain the desired thickness. The films were annealed at 90˚C for 5 min after each layer deposition. 2.2. Growth of ZnO Thin Films The precursor solution for fabricating zinc oxide thin films were prepared by dissolving 0.3 Molar zinc acetate and monoethanolamine (MEA) in a 1:1 Molar ratio in 20 ml of 2-methoxyethanol solvent. MEA was added as a stabilizer to ameliorate the solubility of the precursors. Acetic acid is then added to achieve a homogeneous solution. Above mixture was stirred at 70˚C for one hour. After stirring, the Zn aqueous solution was aged for 24 h. The colour of the solvent then became yellowish orange. The precursor solution was uniformly deposited on ITO cleaned glass substrates that coating in it CuO by spin coating technique at a spin speed of 2000 rpm for 60 s. The coatings were repeated to achieve the desired thickness of 561.56 nm. After each coating the films were baked at 70˚C for 5 min. 2.3. Samples of CuO and ZnO Films Annealed at Various Temperatures The 8 samples of CuO and ZnO films were finally air annealed at various temperatures ranging from (60, 70, 80, 90, 100, 110, 120 and 130)˚C for three hours. Each layer was characterized by studying structural, electrical and optical properties. Glancing angle X-ray diffraction analysis of the films was performed with (XRD) system. Surface morphology of the film was studied by (SEM). Optical absorbance measurements were performed with UV-Vis spectrophotometer 1240 was performed at room-temperature. Electrical characterization of the resistive thin films and current voltage characteristics of p-n junction were performed at room temperature using Kiethley 4200-SCS semiconductor parameter analyzer equipped with. DOI: 10.4236/wjnst.2018.83011 130 World Journal of Nuclear Science and Technology M. Dirar et al. 2.4. Characterization Studies Scanning Electron Microscopy (SEM) The morphology and particle sizes of the as-prepared sample were determined by SEM ((SEM, Tuscan Vega LMU).. The SEM images of ZnO + CuO sample films were annealed at 60˚C temperatures are shown in Figure 1. These indicate that sphere-like ZnO + CuO sample films were annealed at 60˚C temperatures nanostructures obtained by this method are uniform in both morphology and particle size, but have agglomeration to some extent. The average size was calculated to be 1.5 μm from the measurements on the SEM micrographs. Corresponding histograms, showing the particle size distribution, are also presented in Figure 2. The mean particle size 1.5 μm estimated from SEM is in close agreement with the average crystallite size 1.514 μm as calculated from histograms line broadening. The microstructure and chemical composition of the film surface were analyzed using a scanning electron microscope (SEM, Tuscan Vega LMU). Their sizes are found to range from 1.5 to 1.514 μm. 3. Results Table 1 clearly shows the lists of I-V reading for 8 samples for different temperature. The first column represents volts and the other columns show the current for different temperature. Figure 3 shows the relationship between volts ZnO/CuO p-n junction and current for 8 samples with annealed different temperatures from 60˚C to 130˚C in the darkness. From Figure 3, it clearly shows that upon increasing the temperature from 60 to 130 in steps of 10˚C, the current increases with temperature when the voltage is fixed. From Table 2 and Figure 4, it is clear that the current of Pixel = 1 60000 50000 40000 30000 20000 10000 0 60000 50000 40000 30000 20000 10000 0 0 200 0 D = 1.5 µm 100 107.5 Pixel = 1 200 129 Figure 1. SEM images of the ZnO+ CuO sample films were annealed at 60˚C temperatures. DOI: 10.4236/wjnst.2018.83011 131 World Journal of Nuclear Science and Technology M. Dirar et al. ZnO+CuO at 70 OC 448 392 Histogram 336 280 224 168 112 56 0 0 33 66 99 132 165 198 231 264 297 Particales Daimeeter ( nm ) Figure 2. Particle diameter distribution of ZnO + CuO sample films were annealed at 60˚C temperatures. Table 1. The I-V riding of ZnO/CuO p-n junction for 8 samples by heated for different temperatures in the darkness (without exposed to direct light). Voltage (V) −10 I at60˚C I at 70˚C I at 80˚C I at 90˚C I at 100˚C I at 110˚C I at 120˚C I at 130˚C (mA) (mA) (mA) (mA) (mA) (mA) (mA) (mA) −0.01408 −0.01498 −0.01628 −0.01809 −0.02033 −0.02236 −0.02459 −0.02705 −8.11712 −0.01359 −0.01445 −0.01571 −0.01746 −0.01962 −0.02158 −0.02373 −0.02611 −6.21522 −0.01255 −0.01336 −0.01452 −0.01613 −0.01812 −0.01994 −0.02193 −0.02412 −4.31331 −0.01042 −0.01108 −0.01205 −0.01339 −0.01504 −0.01654 −0.0182 −0.02002 −2.41141 −0.00609 −0.00648 −0.00704 −0.00782 −0.00879 −0.00967 −0.01063 −0.0117 −0.50951 0.00236 0.00251 0.00273 0.00303 0.0034 0.00374 0.00412 0.00453 1.39239 0.01766 0.01879 0.02042 0.02269 0.0255 0.02805 0.03085 0.03394 3.29429 0.04202 0.04471 0.04859 0.05399 0.06067 0.06673 0.07341 0.08075 5.1962 0.07379 0.0785 0.08533 0.09481 0.10653 0.11718 0.1289 0.14179 7.0981 0.10598 0.11274 0.12254 0.13616 0.15299 0.16829 0.18512 0.20363 ZnO/CuO p-n junction increase when temperature increases for each samples by annealed different temperatures under particular solar radiation. 4. Discussion In this work the ZnO/CuO junction V-I characteristics was studied in two cases firstly exposed to light directly secondly when it was no light (in darkness). DOI: 10.4236/wjnst.2018.83011 132 World Journal of Nuclear Science and Technology M. Dirar et al. When no light is exposed (in darkness), it was observed that upon increasing the temperature from 60 to 130 in steps of 10˚C, the current increases with temperature when the voltage is fixed. This may be attributed to the fact that the increase of temperature gives more electrons to gain thermal energy to move from the valance band to conduction band thus increases the current. It is also interesting to note that the current is nearly vanishes at a negative voltage equal to about −1.8 volt. This reflects the existence of reverse bias voltage and energy gap ZnO+CuO at 60oC ZnO+CuO at 70oC ZnO+CuO at 80oC ZnO+CuO at 90oC ZnO+CuO at 100oC ZnO+CuO at 110oC ZnO+CuO at 120oC ZnO+CuO at 130oC 0.252 0.216 Current ( mA ) 0.180 0.144 0.108 0.072 0.036 0.000 -0.036 -8.8 -6.6 -4.4 -2.2 0.0 2.2 4.4 6.6 8.8 Voltage ( V ) Figure 3. The I-V curves of ZnO/CuO p-n junction for 8 samples by annealed different temperatures in the darkness. Table 2. The I-V riding of ZnO/CuO p-n junction for 8 samples by annealed different temperature. Voltage I at60˚C I at 70˚C I at 80˚C I at 90˚C I at 100˚C I at 110˚C I at 120˚C I at 130˚C (V) (mA) (mA) (mA) (mA) (mA) (mA) (mA) (mA) DOI: 10.4236/wjnst.2018.83011 −15.000 −1.00916 −1.13389 −1.21924 −1.32526 −1.45633 −1.60196 −1.60196 −1.93837 −12.027 −0.8421 −0.94618 −1.01739 −1.10586 −1.21523 −1.33676 −1.33676 −1.61748 −9.0240 −0.65522 −0.7362 −0.79162 −0.86045 −0.94555 −1.04011 −1.04011 −1.25853 −6.0210 −0.44826 −0.50366 −0.54157 −0.58866 −0.64688 −0.71157 −0.71157 −0.861 −3.0180 −0.21915 −0.24624 −0.26477 −0.2878 −0.31626 −0.34789 −0.34789 −0.42095 −0.0150 0.03433 0.03857 0.04148 0.04508 0.04954 0.0545 0.0545 0.06594 2.9879 0.31463 0.35352 0.38013 0.41318 0.45405 0.49945 0.49945 0.60434 5.9909 0.6244 0.70157 0.75438 0.81998 0.90107 0.99118 0.99118 1.19933 8.9939 0.96649 1.08594 1.16768 1.26922 1.39474 1.53422 1.53422 1.8564 11.997 1.34399 1.5101 1.62376 1.76496 1.93951 2.13347 2.13347 2.58149 133 World Journal of Nuclear Science and Technology M. Dirar et al. 3.60 ZnO+CuO at 60oC ZnO+CuO at 70oC ZnO+CuO at 80oC ZnO+CuO at 90oC ZnO+CuO at 100oC ZnO+CuO at 110oC ZnO+CuO at 120oC ZnO+CuO at 130oC 2.88 Current ( mA ) 2.16 1.44 0.72 0.00 -0.72 -1.44 -2.16 -13.2 -9.9 -6.6 -3.3 0.0 3.3 6.6 9.9 13.2 Voltage ( V ) Figure 4. The I-V curves of ZnO/CuO p-n junction for 8 samples by annealed different temperatures under particular solar radiation. of order 1.8 eV. The existence of negative reverse current is clearly conforms to relation: ( ) = I I 0 e βV − 1 − I p With V and I p standing for operating voltage and photon generates current. For reverse bias the voltage is negative, thus the photon generates current dominance, thus I = − I p this current is assumed to be generated by invisible infra red photons in darkness. These infra red photons generated by human surrounding bodies and the building that exists near the ZnO/CuO diodes. These photon generate currents are less than that generated in light as we will see later The V-I characteristics in Figure 4 of ZnO/CuO unction in light shows again increase in current when temperature increases. This result again confirm the fact that, temperature increase, increases thermal energy, which in turn increases the number of electrons that absorb this energy and transfer to the conduction band. This causes electric current to increase. It is also very interesting to note that the energy gap Eg , which correspond to zero current, increases with temperature, which agrees with theoretical relations, when − Eg = and Eg KT ln n n= 0e KT n0 n where the energy gap Eg is equal to the voltage that corresponding to zero current. The effect of light can be observed clearly when comparing the values of reverse current at a certain voltage say (2.2 volt), where I in darks is 0.01 mA, and DOI: 10.4236/wjnst.2018.83011 134 World Journal of Nuclear Science and Technology M. Dirar et al. light is about 0.7 mA. This is relates to the fact that reverse current I ~ I p . Thus in light current generated by visible photons is considerately large than that generated in dark by only free infra red photons. 5. Conclusion The ZnO/CuO diode energy gap and V-I characteristics are sensitive to temperature as well as light. This sensitivity can be theoretically explained. Also it was found that for different temperature (60 to 130), the average Particle diameter varied from 1.5 micrometer to 92 nm which indicates that the particle size decreases with raising annealing temperature. References [1] Aksoy, S. and Caglar, Y. (2012) Effect of Ambient Temperature on Electrical Properties of Nanostructure n-ZnO/p-Si Heterojunction Diode. Superlattices and Microstructures, 51, 613-625. [2] Lupana, O., Pauportea, Th., Tiginyanu, I.M., Ursaki, V.V., Heinrich, H. and Chowc, L. 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International Journal of Current Research, 8, 31116-31118. DOI: 10.4236/wjnst.2018.83011 135 World Journal of Nuclear Science and Technology