Synthesis and Properties of p-Si/n-Cd_1−xAg_xO Heterostructure for Transparent Photodiode Devices

Abstract

We developed silver-doped Cd₁–_xAg_xO thin films (where x = 0, 0.01, 0.02, 0.03 and 0.04) on amorphous glass substrate by an automated nebulizer spray pyrolysis set-up. The XRD patterns show rock salt cubic crystal structures, and the crystallite sizes vary with respect to Ag doping concentrations. SEM images exhibited a uniform distribution of grains with the addition of Ag; this feature could support the enhancement of electron mobility. The transmittance spectra reveal that all films show high transmittance in the visible region with the observed bandgap of about 2.40 eV. The room temperature photoluminescence (PL) studies show the increase of near-band-edge (NBE) emission of the films prepared by different Ag doping levels, resulting in respective decreases in the bandgaps. The photodiode performance was analyzed for the fabricated p-Si/n-Cd₁–_xAg_xO devices. The responsivity, external quantum efficiency and detectivity of the prepared p-Si/n-Cd₁–_xAg_xO device were investigated. The repeatability of the optimum (3 at.% Ag) photodiode was also studied. The present investigation suggests that Cd₁–_xAg_xO thin films are the potential candidates for various industrial and photodetector applications.

1. Introduction

Thin film technology is a quick-moving field which includes the application of structures, film processing and the manufacture of devices by controlling the shape and size of grains at the nanometer range [1]. Nanometer-range thin films have distinctive and specific physical properties associated with their size [2]. Metal oxide semiconductors have attracted increasing attention because of their wide range of applications in various devices, which include optical communications, photodiode, gas sensors, low emissive windows and solar cells [3]. In the last decade, researchers developed metal oxide-based transparent detectors such as gas sensors and photodetectors [4]. At present, photodetectors are widely studied for use in imaging scanners, switching, touch panels and light sensors. Zheng et al. [4] studied the flexible ZnO–CdO nanofiber arrays for UV photodetectors with 95% transparency. Metal oxides are very common and easily available on Earth, and they are used to fabricate transparent devices due to their low absorption in the visible region. The typical wide bandgap metal oxides such as SnO₂, ZnO, TiO₂ and In₂O₃ can perform as ultraviolet light sensors [5]. The visible range-absorbing CdO is commonly used to fabricate solar cell devices, and it also might be a potential candidate to detect the light spectrum [5].

CdO is an n-type semiconductor with a direct optical bandgap of 2.3–2.5 eV [6] and nonstoichiometric composition, owing to the defects of oxygen vacancies or cadmium interstitials that act as double-loaded donors [7,8]. The unique qualities of CdO metal oxide are its low cost, chemical stability and wide availability.

In general, different kinds of nanostructures offer more attractive properties due to their high surface-to-volume ratios, consequently enhancing the light-sensing ability. The different nanostructures can be grown by changing several parameters, such as the chemical synthesis process, rate of the growth time, substrate temperature, nature of the substrate, and doping. However, metal doping can effectively modify the nature of grains in the host lattice; consequently, it could affect the surface-to-volume ratio or the observing capability of light on the host film surface, whereas the doping can enhance the grain growth level and Debye length, resulting in improved optoelectrical properties. Moreover, doping is a key parameter to improve the performance of any semiconducting materials and used in wide range of device applications [9]. Previously, CdO systems were prepared with different doping elements such as aluminum [10], manganese [11], gallium [12], indium [13], zinc [14] and silver [15] for various applications. However, the silver (Ag) metal element has been commonly used because of its numerous good characteristics and its notable chemical reactivity in solutions [16]. Ag is one of the active metals that might be easily oxidized by the doping process. Therefore, it is very interesting to understand the role of silver in a transparent CdO matrix. Recently, scientists worked on pure and Ag-doped CdO nanostructures through various techniques [15,17,18,19]. To our knowledge, the silver-doped CdO thin film prepared by nebulizer spray pyrolysis has not been reported. Kumar et al. [20,21] reported the advantages of the nebulizer spray pyrolysis (NSP) technique. The main advantages of the NSP technique are good adherence, mechanical stability, being inexpensive, fine droplet formation and capability for mass production for large area deposition that are required for industrial device applications.

Therefore, the aim of the present study is to fabricate Cd_1–xAg_xO thin films (where x = 0, 0.01, 0.02, 0.03 and 0.04) via an automated nebulizer spray pyrolysis method. Ag doping induced the improvement of the optical and electrical properties for the performance of solar cells and other optical devices. Recently, Kathalingam et al. [22] reported the fabrication of an n-Sn:CdO/p-Si heterostructure for visible photodetectors. They suggested that a high-bandgap n-type semiconductor can be easily coated on p-Si substrates to fabricate heterojunction solar cells. In addition, the fabricated p-Si/n-CdO heterojunction could decrease the recombination loss due to a mixture of small-bandgap absorber material and high-bandgap window material. Based on the above work, we report the development of the n-Ag:CdO/p-Si heterostructure and study the photoresponse. This work is propounded for the first time and suggests that the CdO thin films could be utilized for the development of multilayer photodetectors.

2. Materials and Methods

Ag-doped CdO films were prepared on glass substrates using the automated nebulizer spray pyrolysis technique. A total of 0.1 M of high-purity (3N) cadmium acetate dehydrate (Cd(CH₃(COO)₂)·2H₂O) was liquefied by using a mixture of isopropyl alcohol and deionized water, with a volume ratio of 1:3 (20 mL). Silver nitrate (AgNO₃) was used as a dopant precursor with different concentrations, as given in Supplementary Table S1. The prepared precursor solution was sprayed onto the heated glass substrates with a surface area of 25 mm². The heated substrates were maintained at a constant temperature of 200 °C +/− 2 °C using a PID (select 500) controller. The parameters were maintained during spray deposition, including a carrier gas (compressed air) pressure of 14.7 × 10⁴ Nm⁻², a distance between the nozzle and substrate of 10 mm and a solution flow rate of 0.5 mL/min, which were previously optimized. When the sprayed solution fell on the heated substrates, thermal decomposition took place on the film surface, resulting in yellow-colored CdO particles being grown. The structural properties of films were analyzed by an X`PERT-PRO diffractometer (Malvern Pananalytical Ltf, Malvern, UK) (λ = 0.15406 nm) with CuKα radiation. The SEM investigation was performed by a scanning electron microscope (TESCAN VEGA-III, Tescan, Brno, Czech Republic). The elemental analysis was carried out using energy dispersive X-ray spectroscopy (EDX). The optical properties of the films were characterized by a UV-visible spectrophotometer (Shimadzu-UV 1800 model, Shimadzu, Kyoto, Japan). The reflectance spectrum of the samples was recorded by a UV-2400 PC Series. The photoluminescence (PL) spectra was recorded using a fluorescence spectrophotometer (HITACHI F-7000), Hitachi, Tokyo, Japan with an excitation wavelength of ~325 nm. A 532 nm laser wavelength was used as illumination light to measure the photosensitivity, external quantum efficiency (EQE) and detectivity values with the help of a Keithley source meter (model 2450, Tectronix Inc, Beaverton, OR, USA).

3. Results and Discussion

3.1. Structural Analysis

The phase structure of the Ag-doped Cd₁–_xAg_xO films (where x = 0, 0.01, 0.02, 0.03 and 0.04) was studied by XRD, which is shown in Figure 1. The identified diffraction peaks 2θ₍₁₁₁₎ = 33.03°, 2θ₍₂₀₀₎ = 38.44°, 2θ₍₂₂₀₎ = 55.34°, 2θ₍₃₁₁₎ = 66.03° and 2θ₍₂₂₂₎ = 69.35° matched well with the cubic structure of CdO (space group: Fm3m) (JCPDS Card No. 05-0640).

In Figure 1, a highly intense peak obtained at 2θ = 33.03° for all CdO films indicates a preferential growth orientation along the (111) direction. After the inclusion of Ag, the intensity of the XRD characteristic peaks increased gradually up to the optimum doping level (Ag = 0.03), due to Cd²⁺ ions being replaced by Ag⁺ ions because of the larger ionic radius of Ag⁺ (0.126 nm) compared with Cd²⁺ (0.095 nm). The increase in peak intensity or decrease of the full width at half maximum (β) indicated the enhancement of film crystallinity and grain sizes [23]. The comparative cure for 2 at.% and 3 at.% Ag-doped CdO films are given in Figure S1. The figure confirms that the (111) plane increased with the increasing Ag doping level. However, by increasing the Ag doping beyond the optimum level (Ag = 0.03), the peak intensity and film crystallinity started to decrease (Ag = 0.04). This may be attributed to the higher solution quantity or Ag precipitation, resulting a powder-like film being formed on the film surface. In addition, the peak reduction may have possibly occurred by the slight variation of both the Cd and Ag ionic radii, which led to the creation of lattice distortion or crystal imperfections [24]. It is worth noting that there were no impurity phase formations related to Ag or Ag₃O₄, even for a higher dopant level up to 4%. Rex et al. [24] reported the same trend in Ag-doped PbS (4% Ag) films under the NSP method. This could justify that the doping of Ag effectively substituted the site of Cd, resulting the formation of single-phase CdO. As expected, there was no observable peak shift in the predominant (111) plane, confirming the structural purity of CdO.

The lattice parameters were calculated using the standard relation of the cubic structure [25]. The calculated values increased with respect to the increase in Ag concentration up to 3% Ag and then reduced for higher doping levels, and they are tabulated in

Table 1. Structural properties of Cd₁^__xAg_xO thin films.

Ag Doping Level (at.%)	Crystallite Size (nm)	Strain ε	Lattice Constant a = b = c (Å)	Unit Cell Volume (v) (Å)3	TC
0	28	0.0042	4.6828	102.69	1.76
1	29	0.0040	4.6842	102.78	1.93
2	31	0.0038	4.6854	102.86	2.18
3	34	0.0034	4.6869	102.97	2.35
4	32	0.0038	4.6893	103.11	1.97

.

This behavior could be due to the change in the concentration of the native defects or structural defects developed in the prepared host films. The structural parameters, such as the crystallite size (D) and strain (ε), were determined using standard relations [26,27]. The calculated D and ε values of the Cd_1–xAg_xO films with respect to different Ag concentrations are given in Table 1. The crystallite size enhanced with the increase in Ag content, and then it slightly reduced for higher Ag (4 at.%) doping levels. This could possibly vary with the change of structural defects like ε. The defect factors of ε decreased initially as a function of the increasing Ag up to 3% and then slightly increased for the 4% Ag-doped CdO thin film. A decrease in defect values could be attributed to the enhancement of crystallinity caused by the periodic arrangement of atoms in the host crystal structure.

The texture coefficient TC_(hkl) values demonstrate the crystal orientation of the (111) plane of the prepared Cd_1–xAg_xO system by using X-ray data with the equation given below [26]:

$${\mathrm{TC}}_{(\mathrm{hkl})}=\frac{I_{(\mathrm{hkl})}/{I_0}_{(\mathrm{hkl})}}{N_r^{-1}\hspace{0.17em}{\displaystyle \sum I_{(\mathrm{hkl})}/{I_0}_{(\mathrm{hkl})}}}$$

(1)

where I_(hkl), I_0(hkl) and N denote the usual meanings. From Table 1, it is found that the calculated TC values increased with the increasing Ag doping concentration and then finally decreased. The obtained TCs for all the films were higher than 1 (TC > 1), which indicates the preferable grain growth in certain orientations. This result suggests that a lot of crystallites were gathered along the (111) plane, which helped improve the electrical performance. The variation of TC values was the same as in our previous report [26]. The XRD studies showed that the Ag, up to 3 at.%, maintained good structural quality (crystallinity) with minimum defects (strain) compared with that of other prepared films.

3.2. Surface Morphology Analysis

The observed SEM images of the pure CdO and Cd_1–xAg_xO films are shown in Figure S2. The pure CdO film showed densely packed, brain-like grains [28] uniformly distributed on the entire film surface, whereas the bunch of irregular spherical grains without the presence of voids were observed in 1–2 at.% Ag-doped films. The film with 3 at.% Ag doping exhibited spherical shaped grains with well-defined grain boundaries [29]. The particles were further agglomerated by increasing the doping beyond the optimum level (4 at.% Ag). Moreover, the grain sizes increased by increasing the doping concentrations up to 3 at.%. Thereafter, the grain size slightly decreased for higher-level doping (4 at.% Ag). Thus, various levels of Ag doping concentrations effectively modified the host CdO film surface, and this observation could be correlated with the XRD results. The change in grain size signified the change of grain boundaries in the host lattice. The composition of the pure and Ag-doped CdO (3 at.%) films were confirmed by energy dispersive X-ray spectroscopy (EDX). The obtained EDX spectra of the prepared films are shown in the inset of Figure S2. The expected elements of Cd, O and Ag are present with the desired atomic percentages which were taken. The composition percentages of Cd, O, and Ag were 48.07%, 49.06%, and 2.87%, respectively, for 3 at.% Ag.

3.3. Optical Analysis

The optical properties were explored with a UV-visible spectrophotometer. The optical transmittance and reflectance spectra of Cd_1–xAg_xO films are given in Figure 2a,b, respectively. From Figure 2a, the obtained transparency was ~70% in the visible wavelength range. Transmittance was reduced slightly with the increasing doping concentration, which may have been due to the decrement in oxygen vacancies. Furthermore, the lessening of transmittance was due to the change in grain size and film thickness [30]. The observed transmittance range confirmed that the prepared film could work as a transparent photodetector.

The transmittance value was not as close to the lower wavelength of the visible region due to the appearance of absorption. Furthermore, the primary absorption edge was shifted in the direction of the higher wavelength (redshift) with respect to the Ag concentration. This edge in the wavelength can decide the variation of the bandgap because the transmittance is associated with stimulating the charge carriers from the valence to conduction bands. The optical bandgap is related by the following equation [24]:

$$\alpha h\nu =B(h\nu { -E}_{\mathrm{g}}{)}^{\mathrm{n}}$$

(2)

where B is a constant and E_g is the bandgap of the material. The direct bandgaps of the Cd₁–_xAg_xO films were obtained from a plot of (αhν)² versus hν, as illustrated in Figure 3. The bandgap values of the prepared films are given in

Table 2. Optical properties of Cd_1–xAg_xO thin films.

Ag Doping Level (at.%)	For λ = Average of 600–900 nm			Bandgap Eg (eV)
	T%	R%	n
0	75	17	2.41	2.45
1	71	19	2.53	2.43
2	68	20	2.58	2.40
3	65	22	2.62	2.37
4	70	16	2.36	2.41

. The E_g value of the pure CdO was 2.45 eV, which matched well with the one reported by Usharani et al. [31], whereas the E_g values for the doped CdO films were found to decrease from 2.43 eV to 2.37 eV with the increase in the Ag doping level. This might be due to the substitution of Ag in the sites of Cd. A similar reduction in the bandgap was observed for the Ag-doped PbS film under the NSP method [24]. Moreover, redshift absorption (toward a higher wavelength) further confirmed the decrease of the bandgap. For a higher doping concentration (4 at.% Ag), the bandgap was slightly enhanced due to the doped Ag ions effectively modifying the band structure of the host CdO lattice. The reduction of film crystallinity (XRD) and blueshift of the near-band-edge (NBE) emission (PL) occurred from 3 at.% to 4 at.% Ag-doped CdO, as evidenced by the increase of the bandgap. As shown in Table 2, the bandgap was low for the film doped with 3 at.% Ag, which absorbed more visible light than the other films. Consequently, the photoelectric interaction was enhanced, resulting in improving the photosensor performance with respect to the applied voltage.

Other optical factors, such as the refractive index (n) and reflectance (R), play an important role for any optical device. The R and n values of the Cd₁–_xAg_xO thin films are listed in Table 2. The R values of the Ag-doped CdO thin films increased from 17% to 22% as a function of the doping concentration increasing from 1 at.% to 3 at.% Ag. The variation of reflectance was in oppositional behavior to the transmittance with respect to the doping concentration, as shown in Figure 2b. The refractive index n was determined from the values of reflectance and the extinction coefficient (k) using the following equation [32]:.

$$n=\frac{(1+R)}{(1-R)}+\sqrt{\frac{4R}{{(1-R)}^2}-k^2}$$

(3)

From Table 2, the observed low value of n confirmed the smooth surface morphologies and minimum reflectance of the prepared films. The variation of n systematically increased with the increasing Ag doping level due to the decrease of transmittance (T). Commonly, the n variation had the opposite trend of T, which may be attributed to the increase of light scattering of the photons. The estimated n values were in the range of 2.36–2.62 in the visible range for different doping concentration, as shown in Table 2.

3.4. Photoluminescence Analysis

Photoluminescence (PL) was used to investigate the factor of the electron hole pairs in the semiconductor materials [33].

Figure 4 presents the photoluminescence spectra of the prepared Cd₁–_xAg_xO films obtained by an excitation wavelength of ~325 nm. The room temperature PL spectra mainly consisted of one strong green emission band observed at ~520 nm (2.38 eV) in all the prepared films. The green emission was consistent with the near-band-edge emission (NBE), which originated from the recombination of the electron and holes. In addition, the observed NBE emission by PL correlated well with the bandgap obtained by the UV-visible study. Similar green emission was previously observed by Velusamy et al. [23] for CdO films. The overall peak intensity increased as a function of the Ag doping concentration. This might be representative of the increasing quantity of Ag ions on the host CdO lattice and the decrease in space between the Ag⁺ and Cd²⁺ ions, while for the higher doping level, the peak intensity decreased slightly, which may have been due to the increasing interstitial placement level of the Ag ions near the Cd sites. The NBE emission shifted gradually toward longer wavelength sides (from 517 to 522 nm) with increasing Ag doping levels. Consequently, there was a decrease in the energy gap, as evidenced from Figure 3. Gaussian curve fitting was used to find the additional defect peaks from the prepared Cd_1–xAg_xO films. From the fitted PL cure, a peak was observed at 521 nm for all the prepared films. This might have been the presence of Cd as interstitials or native state defects. As seen from the figure, the defect peaks were considerably increased with respect to the Ag doping concentration, and as a result, it could help to enhance the photoelectric performance. In addition, the other low-intensity green emission peak was identified at ~545 nm for all the films, which arose due to the presence of defects like oxygen vacancies, as is clearly shown in Figure 4. The film with 3 at.% Ag doping had more oxygen vacancy at the film surface than the others. Therefore, it could react well with the photon from the laser light. Moreover, the Ag doping induced a redshift, which may have been due to the surface area [34], resulting in a reduction of the bandgap. We believe that the Ag dopant can enhance the surface area and crystalline quality. The above factors might be evidence for enhancing light absorption and improving charge carrier generation. A similar result was observed for Nd-doped ZnO thin films by Paul et al. [35].

3.5. Photodiode Preparation and Properties

The schematic diagram of the fabricated heterojunction photodiode p-Si/n-Cd₁–_xAg_xO/Ag structure is shown in Figure 5. Before fabricating the heterostructure device, the native oxide should be removed from the Si substrate. Here, we used HF:H₂O (1:10) solution treatment and then rinsed it with deionized water. The Ag-doped CdO films were coated on the p-type silica substrate by the NSP method to form a heterojunction device. Silver paste was used as contact electrodes on both the p-Si and n-CdO surfaces to measure the photocurrent with respect to the bias voltage.

The photocurrent performance of the prepared photodiodes was measured using a ~532 nm laser with a Keithley source meter (model-2450) at room temperature. The current–voltage (I–V) characteristics were investigated at different bias voltages from −5 V to +5 V under dark and UV illumination conditions. The measured I–V spectra of the p-Si/n-Cd_1–xAg_xO/Ag structure are given in Figure 6. The observed dark and light currents both increased gradually with respect to the increase in applied voltage. However, the current level was higher for light illumination compared to the dark condition, due to the increase of electrons when the diode interacted with the incident photons obtained from light. The photocurrent (under light) was enhanced significantly for both the forward and reverse biases, indicating successful light sensing for the fabricated photodiodes. It was observed that the photocurrent was nearly two orders of magnitude higher than the dark current, likely due to the inner photoelectric effect (i.e., when a photon of sufficient energy falls on the photodiode, it creates an electron hole pair).

The external quantum efficiency (EQE), responsivity (R*) and specific detectivity (D*) values were calculated using the standard relations, which were $EQE=\frac{Rhc}{e\lambda }$, $R*=\frac{I_P}{A\times P_{in}}$ and $D*=R\sqrt{\frac{A}{2e{I}_d}}$ [35,36]. The calculated D* and EQE values were directly proportional to R, which increased for the Ag-doped CdO photodiodes, as shown in Figure 7.

The prepared photodiode responsivity increased from 0.05 AW⁻¹ to 0.28 AW⁻¹ for the pure CdO to 3 at.% Ag-doped CdO photodiode and then decreased to 0.03 AW⁻¹ for the higher doping of Ag (4 at.%). The maximum external quantum efficiency was ~98.21%, observed for the optimum CdO photodiode (3 at.% Ag-doped CdO) when compared with others. Ravikumar et al. [37] obtained an EQE value of 73.03% for a 5% Nd-doped CdO, which was a bit lower than our value. The specific detectivity was enhanced gradually from 5.07 × 10⁹ to 1.10 × 10¹¹ (jones) for the pure to 3 at.% Ag-doped CdO photodiode. This observed specific detectivity was comparably higher than the previously reported one for CdS:Ag/Si [38]. The observed good photoelectric properties may have been due to maximum electron hole pair generation when it interacted with high-energy photons.

The linear dynamic range (LDR) is one of the important factors to recognize the performance of any photodiode and photodetectors, and it can be estimated using the following equation [39]:

$$LDR=20\log \left(\frac{I_{\min }}{I_{\max }}\right)$$

(4)

where I_min and I_max represent the dark current and light current, respectively. The observed LDR of the prepared p-Si/n-Cd₁–_xAg_xO/Ag structure was 36.7 dB for the 3 at.% Ag-doped CdO. This value was close to the ZnO-based p-n junction diode [39], though it is worth noting that the CdO-based visible photodiode prepared by a simple spray method showed a reasonable LDR value compared with that of the other p-n junction [39,40]. Hence, we believe that this is an essential move to fabricate the flexible photodiodes.

To find the ideality factor, the I–V characteristics of the optimum p-Si/n-CdO:Ag photodiode (3 at.% Ag) under dark and light conditions are given in Figure 8. The observed photocurrent exponentially increased when compared with the dark current. In this work, the observed photocurrent level (11.6 × 10⁻⁶ A at 5V) was higher than the previously reported values. Recently, Xiao et al. [41] fabricated the Ga₂O₃:CdO-based amorphous thin-film transistor and observed a photocurrent of about 20 nA at 20 V.

The ideality factor (η) is one of the important parameters for any heterostructure diode for finding the recombination mechanisms ruling inside the diode. Based on the theory of thermionic emission (TE), the ideality factor (η) can be calculated with the use of dark I–V curves by the following relation [42]:

$$I=I_0\exp \left(\frac{eV}{\eta kT}-1\right)$$

(5)

where e is the electron charge, V is the voltage, I₀ is the saturation current, k is the Boltzmann constant and T is the absolute temperature (300 K). The η value of the diode was calculated from the slope of the linear part at the forward bias curves, and the value was 3.2. For an ideal diode, the η is equal to one, which means that the current flow is due to thermionic emission, though the reported value is commonly higher than unity. In our case, the ideality factor value was found to be higher than unity, indicating the existence of interface states or surface defects on the native oxide layer. This can possibly happen from thermionic emission and other electron transport mechanisms. Tunneling recombination in particular could play a leading role in controlling the junction behavior and increasing the η [43]. Yakuphanoglu et al. [44] observed an ideality factor of 5.41 for a nanocluster-based n-CdO/p-Si photodiode.

In order to understand the photosensing performance of the optimal photodiode (3 at.% Ag-doped CdO), the photocurrent experiment was performed under different light intensities from 1 mW/cm² to 5 mW/cm² at 0.5 V, as shown in Figure 9a. When the diode interacted with different intensities of light (turning on the light), the current quickly reached a specific level, and when the light was turned off, the photocurrent reached its beginning stage. This was because of the increase of the number of photo-generated charge carriers and the free electrons that supported the increase in the current for the light-on condition, whereas the numbers of free electrons went down when the light was off [45]. The photocurrent varied between the light-on and off conditions due to the trapping of deep levels of charge carriers [46]. The figure shows that the current values were increasing gradually with the increasing intensities of light from 1 mW/cm² to 5 mW/cm². The time taken for increasing and decreasing the current level was measured from the fabricated p-Si/n-CdO:Ag structure. The increase in time was considered to be ~90% of the time taken to reach the maximum value, and the reverse was the decrease in time. The increase in time (τ_inc) and decrease in time (τ_dec) were 0.8 s and 1.0 s, respectively.

To understand the photodetection capability (repeatability) of the prepared heterostructure, a constant laser power (5 mW/cm²) was used as a function of the increasing time. Figure 9b shows the transient photocurrent response of the prepared heterostructure under a bias voltage of 0.5 V. The transient photosensing performances maintained the same range with respect to the increase in time, which confirmed good sensing capability and repeatability. Figure 9c illustrates the variation of the current for fresh and 3 months-aged p-Si/n-CdO:Ag photodiodes to define the stability of the optimum sensor. It was found that the electrical current range reached above 95% of the fresh photodiode at 0.5 V, while the response time was a bit slower (1.2 s) when compared with the fresh photodiode (0.8 s). At the same time, the recovery time was nearly equal (~1.0 s) for both the fresh and aged photodiodes. Hence, we conclude that the aged photodiode still showed good photosensing performance and good stability (reproducibility) even after 3 months.

4. Conclusions

In summary, the successful preparation of transparent Cd₁–_xAg_xO thin films on glass and p-Si substrates for photodiode investigation. The XRD pattern revealed the formation of a cubic structured CdO lattice with a (111) preferential orientation, and there were no peak shifts in all the films, which confirmed the absence of an impurity phase. The SEM images revealed that all the films had spherical grains, and the grain size increased with the increase in the Ag doping level. EDX analysis revealed that the Cd, O and Ag elements were present in the prepared films. The undoped film showed the maximum transmittance of ~75%, and the corresponding bandgap was 2.45 eV, which confirmed the transparent nature of the CdO material. The obtained bandgap decreased with an increase in the doping level. From the present study, it is evident that the fabricated p-Si/n-CdO:Ag photodiode showed an improved photoresponse in the visible region.