Structure, morphology and absorption characteristics of gold nanoparticles produced via PLAL method: Role of low energy X-ray dosage
Introduction
In response to the exponential growth and ever-increasing medical demands of various inorganic and organic nanoparticles, intensive researchers have been dedicated to synthesize some highly stable nanoparticles in a rapid, easy and economical manner. Amongst all types of inorganic NPs useful for diverse applications, the AuNPs are the celebrated one because of its non-toxicity, great stability and flexibility related to the surface manipulations. In fact, the small size (below 30 nm) AuNPs due to their excellent chemical stability have widely been used for the diagnosis (as preventive agent and radio-sensitizer) and treatment (in the radiation therapy, drug delivery and photothermal therapy). Some other factors that attract the AuNPs to the researchers include their non-toxic and biocompatible nature; rapid adjustment and conjugation with the antibodies, ligands and proteins; reasonable surface functionality; shape-dependent surface plasmon resonance; and speedy physical interaction with X-rays [1], [2], [3], [4], [5], [6], [7], [8].
In recent times, sundry physical methods, chemical reduction approaches, sonochemical and green techniques have been developed to produce good quality colloidal AuNPs with desired properties suitable for varied applications [9], [10], [11], [12], [13], [14], [15]. In the past, to synthesize AuNPs via laser ablation method, solid gold target has been irradiated using laser beams at various density, power, wavelength, repetition rate, pulse duration, number of pulses and exposure time [9].
The near-infrared ablation at 1064 nm results in a bottom-up synthesis process dominated by plasma ablation. Laser absorption frees electrons, which interfere with bound electrons and then free them. If the number of collisions increases, the solvent becomes ionized, igniting a plasma. The substance circling the plasma confines it, increasing its stability and absorption ever further. As the expanding plasma is quenched by the confining material, condensation happens in NPs in varying geometries [[16], [17], [18]]. It is worth mentioning some of the advantages of the laser ablation approach such as the ease of processing; elimination of chemical reagents, surfactants and stabilizers; and potential for the production of contaminants-free (pure) samples with customized properties needed for specific applications. Recent studies indicated that the lased ablated colloidal suspension containing the NPs shows aggregation tendency due to the feasibility of bigger size fragments ejected from the target surface, leading to the ill-defied morphology and broad size distributions of the NPs obtained from the laser-produced plasma [19], [20], [21]. Sylverstre et al. [22] lowered the laser energy enabled heating of the samples and demonstrated a remarkable size reduction of the AuNPs in aqueous cyclodextrins. In another study, the mean size of the AuNPs produced in sodium-dodecyl sulfate solution by the PLAL technique was reduced below 8 nm [23]. Despite constant efforts for tailoring various characteristics of the produced colloidal AuNPs in the liquid suspension by controlling the laser processing parameters in the PLAL process an optimized approach still remains deficient.
The -fluence of a geometrical parameter which can be calculated using energy and the spot size of laser beam.
The laser ablation of solid metallic targets in water typically results in the large and widely dispersed NPs due to the post-stabilization and coalescence of the atomic species ejected from the target surface. Utilization of the surfactant in the solution was proven to be useful at it encircles the NPs at an optimal growth rate and prevents the agglomeration. However, the use of surfactants often generates some impurities in the colloidal suspension that may further increase the samples toxicity and reduce the medical applications feasibility. To avoid this problem, Tarasenko et al. [24] prepared some AuNPs by laser ablation in pure water. The results indicated the complete absence of chemical impurities in the colloidal suspension containing AuNPs. Meanwhile, Kabashin et al. [8] proposed two different approaches to eliminate the potential chemical contamination of the samples which could define the standards for the treatment of almost monodispersed AuNPs in water. The first method suggested the use of the femtosecond laser ablation for the AuNPs preparation that rapidly cools the ablation products, thereby preventing the aggregation. The second method recommended the synthesis of the AuNPs in clean water at 532 and 266 nm using the PLAL technique combined with the irradiation from the nanosecond pulsed laser. Motivated by this post-treatment of the PLAL produced AuNPs, few researchers have tried to improve the overall properties of the NPs in the colloidal suspension.
Considering the immense fundamental and applied significance of the AuNPs especially in the nanomedicine we prepared some AuNPs in distilled water using the adaptable PLAL technique. The influence of low energy X-ray irradiation dose on various characteristics of the PLAL grown colloidal AuNPs was evaluated for the first time. Systematic characterizations of the produced colloidal AuNPs revealed their high purity, good stability and biocompatibility. The obtained results were analyzed, discussed and interpreted. The proposed strategy for the production of the colloidal AuNPs in distilled water via the combined methods was shown to be useful in terms of the simplicity, rapidity and cost-effectiveness. These AuNPs may be potential for the future nanomedicine and treatments.
Section snippets
Colloidal AuNPs preparation
The output signal from an Nd:YAG laser of wavelength 1064 nm was focused to the surface of the pure gold plate acted as the solid target for the AuNPs production. The Au target was immersed inside the bottom of a cell containing distilled water of volume 10 mL. The spot diameter of the laser beam was 2 mm operated at various fluences of 0.076, 3.846, and 7.692 J/cm2. Depending on the energy and spot size of the laser pulse, the measured fluences were ranged from 0.076 - 7.692 J/cm2. The period
Structures of AuNPs
-Fluence is a geometrical parameter of laser beam spot size that can be obtained by energy and spot size. A wide range of energy/fluence were focalized on gold target to synthesis AuNPs in aqueous solutions by ablation approaches using Nd:YAG laser. Al-Azawi et al. [25] prepare AuNPs average range size 15.12 to 9.5 nm using laser ablation (wavelength 1064 nm) at 15 J/cm2 in 4 min. Elsewhere, Khumaeni et al. [26] synthesized AuNPs by Nd:YAG laser, 1064 nm in a deionized water and 30 mJ energy in
Conclusions
Highly stable colloidal AuNPs were successfully produced in water via the simple and straight-forward PLAL strategy combined with low energy X-ray irradiation doses. The role of post-irradiation by the low energy X-ray dose on the structure, morphology and absorption traits of these colloidal AuNPs were determined. The SEM images confirmed the nucleation of spherical shape surfactant-free colloidal AuNPs (mean sizes of 24 nm). The hydrodynamic size of these AuNPs was inversely proportion to the
Financial support and sponsorship
The authors are thankful to the School of Physics (USM) for research assistance and support. The financial support from the RCMO (USM) via the short-term research grant (304/PFIZIK/6315514) is appreciated.
CRediT authorship contribution statement
Pegah Moradi Khaniabadi: Conceptualization, Methodology, Investigation, Writing – original draft. Naser M Ahmed: Conceptualization, Resources, Funding acquisition. Mohammed Ali Dheyab: Investigation, Visualization. Azlan Abdul Aziz: Resources, Writing – review & editing. M.A. Almessiere: Visualization.
Declaration of Competing Interest
There are no conflicts of interest.
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