{"id":40983,"date":"2021-09-30T10:38:33","date_gmt":"2021-09-30T10:38:33","guid":{"rendered":"https:\/\/biomedpharmajournal.org\/?p=40983"},"modified":"2021-10-11T10:07:46","modified_gmt":"2021-10-11T10:07:46","slug":"synthesis-processing-condition-optimization-of-citrate-stabilized-superparamagnetic-iron-oxide-nanoparticles-using-direct-co-precipitation-method","status":"publish","type":"post","link":"https:\/\/biomedpharmajournal.org\/staging\/vol14no3\/synthesis-processing-condition-optimization-of-citrate-stabilized-superparamagnetic-iron-oxide-nanoparticles-using-direct-co-precipitation-method\/","title":{"rendered":"Synthesis Processing Condition Optimization of Citrate Stabilized Superparamagnetic Iron Oxide Nanoparticles using Direct Co-Precipitation Method"},"content":{"rendered":"<p><strong>Introduction<\/strong><\/p>\n<p>Metallic nanoparticles (MNP) have been proved useful in the biomedical field and have been studied vastly in recent years, specifically superparamagnetic iron oxide nanoparticles (SPION). These MNP diagnostic agents are useful for magnetic resonance imaging (MRI) <sup>1\u20133<\/sup>. Diagnostic agents in delivery systems will aid to confirm the precise and successful biodistribution of therapeutic agents <sup>4<\/sup>. This unique MNP only shows magnetization properties under the influence of a magnetic field<sup>5<\/sup>, making them instantly detectable through MRI to trace drug distribution in the human body<sup>6<\/sup>. Moreover, they can also become an important component in drug delivery and targeting systems and nevertheless hyperthermia therapy<sup>3,4,7,8<\/sup>.<\/p>\n<p>Despite being biocompatible, the biomedical effectiveness of SPION heavily depends on their physical stability. Since SPION are lyophobic, in an aqueous environment, they tend to aggregate to one another. Thermodynamically, these nanoparticles are more stable to interact with one another than with water because of their incapability to form hydrogen bonds<sup>9\u201311<\/sup>. Ensuring the physical stability of synthesized SPION is crucial to prevent the growth of its particle size and platelet aggregation after administration.<\/p>\n<p>Stabilization of SPION has previously been accomplished with molecules including trisodium citrate dihydrate, oleic acid, and polymers. These molecules decrease and prevent particle growth and guarantee its physical stability. Advantages of trisodium citrate dihydrate as a stabilizer include affordable, abundant, and can create high dispersible SPION in aqueous solvents.<\/p>\n<p>The direct co-precipitation method for superparamagnetic iron oxide nanoparticle synthesis is known to be convenient, uses lower temperatures, nonetheless produces high yields. Meanwhile, this cost-effective method isn\u2019t free from drawbacks; mainly high polydispersity and large particle size. For superparamagnetic properties, core size of below 20 nm would have to be reached, though different works of literature have also stated 30 \u2013 50 nm<sup>12<\/sup>, or &lt;150 nm for magnetic particle imaging<sup>13<\/sup>. Besides achieving the desired nanoparticle size, the surface coating can also prevent oxidation of SPION from the environment<sup>14<\/sup>.<\/p>\n<p>To overcome the limitations of the direct co-precipitation method, this research focuses on optimizing the processing conditions including stirring speed, stabilizer concentration, and stabilizer adsorption temperature. The stability of SPION will be measured by hydrodynamic size, polydispersity index, and zeta potential. Furthermore, physicochemical characteristics from the most preferable processing condition will be observed by FTIR, fluorescence spectroscopy, XRD, and TEM. The stable SPION-C produced is expected to be used directly or conjugated onto another molecule.<\/p>\n<p><strong>Materials and Methods<\/strong><\/p>\n<p><strong>Reagents and Instruments<\/strong><\/p>\n<p>Iron (III) chloride hexahydrate (FeCl<sub>3<\/sub> \u2022 6H<sub>2<\/sub>O), iron (II) chloride tetrahydrate (FeCl<sub>2<\/sub> \u2022 4H<sub>2<\/sub>O), ammonia solution (25%), and trisodium citrate dihydrate, were from Merck, Germany. Nanoparticles were analyzed by a NANO-ZS series Malvern Zetasizer (Malvern Instruments, Malvern, UK) particle size analyzer, and a Hitachi HT-7700 transmittance electron microscope (TEM), Institut Teknologi Bandung. Crystalline characteristics were observed using an X-ray diffractometer (PANalytical X&#8217;Pert), whilst other physicochemical properties were observed using an FTIR spectrophotometer 8400 S (Shimadzu, Japan); and Horiba FluoroMax Hybrid Fluorescence Spectroscopy Steady State and Life Time System (Integrated Laboratory &amp; Research Center Universitas Indonesia).<\/p>\n<p><strong>Synthesis of Citrate Stabilized Superparamagnetic Iron Oxide Nanoparticles<\/strong><\/p>\n<p>Citrate stabilized superparamagnetic iron oxide nanoparticles were synthesized using the direct co-precipitation method based on previous literature15<sup>,<strong>16<\/strong><\/sup> with some modifications. FeCl<sub>3<\/sub> solution (50 mL, 0.08 M) and FeCl<sub>2 <\/sub>solution (50 mL, 0.04 M) were prepared separately in demineralized water. The prepared solution of FeCl<sub>3<\/sub> was poured carefully into the three-neck round bottom flask, followed by the solution of FeCl<sub>2<\/sub> under a nitrogen atmosphere. Both solutions were mixed under vigorous stirring (3000 \u2013 12000 rpm) using an IKA EUROSTAR 20 high-speed digital overhead stirrer. The volume of the mixture was then added to 150 mL with continued stirring and its temperature was increased to 60<sup>o<\/sup>C before adding the ammonia solution dropwise until the solution reached above pH 9. Instantly, the solution turned dark brown to black and the reaction was held for 15 minutes at a constant temperature. Trisodium citrate dihydrate solution (10 mL, 0.503 M or 10 mL, 1.006 M) was added to the reaction after the product reached 90<sup>o<\/sup>C and left for an hour while maintaining stable temperature and stirring speed. Molar ratio of FeCl<sub>3<\/sub> \u2022 6H<sub>2<\/sub>O to FeCl<sub>2<\/sub> \u2022 4H<sub>2<\/sub>O of all batches was 2:1. Once the optimal speed and stabilizer concentration was determined, the temperature for stabilizer adsorption was studied.<\/p>\n<p><strong>Particle Size, PDI, and Zeta Potential Measurement<\/strong><\/p>\n<p>Hydrodynamic particle size, polydispersity index (PDI), and zeta (\u03b6) potential of SPION and SPION-C were analyzed by dynamic light scattering (DLS) at room temperature. The sample solution was prepared with a concentration of 5 \u00b5L\/mL in water.<\/p>\n<p><strong>FTIR Analysis<\/strong><\/p>\n<p>Chemical functional groups present on the synthesized SPION and SPION-C were analyzed and confirmed by infrared spectroscopy with transmittance (%) measured at a 4000 \u2013 400 cm<sup>-1<\/sup> wavelength range.<\/p>\n<p><strong>Fluorescence Spectroscopy<\/strong><\/p>\n<p>The excitation and emission spectrum of SPION and SPION-C were determined by fluorescence spectroscopy.<\/p>\n<p><strong>XRD Analysis<\/strong><\/p>\n<p>Crystalline characteristics of SPION and SPION-C were observed by X-ray diffraction (XRD),\u00a0 using a Copper K-\u03b1 (\u03bb = 1.5 A<sup>o<\/sup>) radiation source with generator settings of 30 mA and 40 kV, and a 0.02<sup>o<\/sup> step size; Bragg angle from 10<sup>o<\/sup> to 90<sup>o<\/sup>. Rietveld refinement was done using the PANalytical X\u2019Pert HighScore Plus program.<\/p>\n<p><strong>Morphological Analysis<\/strong><\/p>\n<p>Individual SPION-C and their core size along with their morphological shape were analyzed by TEM where a drop of diluted SPION-C was placed on a 20 nm Cu: Carbon TEM mesh grid and let dry before analysis.<\/p>\n<p><strong>Stability During Storage<\/strong><\/p>\n<p>The stability study of SPION-C at 4<sup>o<\/sup>C was to resemble the storage condition of the nanoparticles. Particle size, PDI, and zeta potential were observed for up to 30 weeks.<\/p>\n<p><strong>Results and Discussion<\/strong><\/p>\n<p>SPION stabilized by trisodium citrate dihydrate has successfully been synthesized through direct co-precipitation by optimizing their processing conditions (Table 1).<\/p>\n<p><strong>Table 1: Processing Conditions of SPION and SPION-C.<\/strong><\/p>\n<table style=\"width: 95%;\" border=\"1\" cellspacing=\"0\" cellpadding=\"4\">\n<tbody>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>Batch<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\"><strong>Stirring speed (rpm)<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"40%\"><strong>Stabilizer concentration<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"23%\"><strong>Stabilizer adsorption<\/strong><\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>A<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">3000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">&#8211;<\/td>\n<td style=\"text-align: center;\" width=\"23%\">&#8211;<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>B<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">3000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"23%\">90<sup>o<\/sup>C<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>C<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">6000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"23%\">90<sup>o<\/sup>C<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>D<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">&#8211;<\/td>\n<td style=\"text-align: center;\" width=\"23%\">&#8211;<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>E<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"23%\">90<sup>o<\/sup>C<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>F<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">12000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"23%\">90<sup>o<\/sup>C<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>G<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">1.006 M<\/td>\n<td style=\"text-align: center;\" width=\"23%\">90<sup>o<\/sup>C<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"13%\"><strong>H<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"40%\">1.006 M<\/td>\n<td style=\"text-align: center;\" width=\"23%\">60<sup>o<\/sup>C<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p><strong>Influence of Stirring Speed<\/strong><\/p>\n<p>The mean of size distribution by number of SPION-C from smallest to largest was Batch E, C, B, and F (Table. 2). Batches C (6000 rpm) and E (9000 rpm) obtained smaller hydrodynamic sizes than previous studies of citrate stabilized SPION synthesized by co-precipitation which were larger than 200 nm<sup>17<\/sup>, 100 nm<sup>18<\/sup>, and 55 nm<sup>19<\/sup>.<\/p>\n<p><strong>Table 2: Influence of Stirring Speed on SPION and SPION-C.<\/strong><\/p>\n<table style=\"width: 95%;\" border=\"1\" cellspacing=\"0\" cellpadding=\"4\">\n<tbody>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>Batch<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"13%\"><strong>Stirring speed (rpm)<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"20%\"><strong>Stabilizer concentration<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"16%\"><strong>Size<sup>I<\/sup> \u00b1 SD<sup>II<br \/>\n<\/sup><\/strong><strong>(nm)<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"18%\"><strong>PDI \u00b1 SD<sup>II<\/sup><\/strong><\/td>\n<td style=\"text-align: center;\" width=\"22%\"><strong>\u03b6<\/strong> <strong>\u00a0potential \u00b1 SD<sup>II\u00a0 <\/sup>(mV)<\/strong><\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>A<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"13%\">3000<\/td>\n<td style=\"text-align: center;\" width=\"20%\">&#8211;<\/td>\n<td style=\"text-align: center;\" width=\"16%\">1357.07 \u00b1 583<\/td>\n<td style=\"text-align: center;\" width=\"18%\">&#8211;<\/td>\n<td style=\"text-align: center;\" width=\"22%\">-24.3 \u00b1 1.1<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>B<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"13%\">3000<\/td>\n<td style=\"text-align: center;\" width=\"20%\">10 mL, 0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"16%\">39.95 \u00b1 16<\/td>\n<td style=\"text-align: center;\" width=\"18%\">0.243 \u00b1 0.02<\/td>\n<td style=\"text-align: center;\" width=\"22%\">-48.63 \u00b1 3.0<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>C<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"13%\">6000<\/td>\n<td style=\"text-align: center;\" width=\"20%\">10 mL, 0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"16%\">36.56 \u00b1 8<\/td>\n<td style=\"text-align: center;\" width=\"18%\">0.339 \u00b1 0.05<\/td>\n<td style=\"text-align: center;\" width=\"22%\">-37.1 \u00b1 6.5<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>D<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"13%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"20%\">&#8211;<\/td>\n<td style=\"text-align: center;\" width=\"16%\">854.97 \u00b1 169<\/td>\n<td style=\"text-align: center;\" width=\"18%\">&#8211;<\/td>\n<td style=\"text-align: center;\" width=\"22%\">-30.8 \u00b1 0.6<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>E<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"13%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"20%\">10 mL, 0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"16%\">25.58 \u00b1 7<\/td>\n<td style=\"text-align: center;\" width=\"18%\">0.346 \u00b1 0.01<\/td>\n<td style=\"text-align: center;\" width=\"22%\">-41.67 \u00b1 2.1<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>F<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"13%\">12000<\/td>\n<td style=\"text-align: center;\" width=\"20%\">10 mL, 0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"16%\">161.27 \u00b1 33<\/td>\n<td style=\"text-align: center;\" width=\"18%\">&#8211;<\/td>\n<td style=\"text-align: center;\" width=\"22%\">-38.17 \u00b1 1.8<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><sup>I<\/sup>Size distribution by number<\/p>\n<p><sup>II<\/sup><em>SD<\/em> standard deviation (n=3)<\/p>\n<p>As the hydrodynamic sizes of SPION of batch A and batch D were similar (Table. 2), our study demonstrates that stirring speed greatly influences the success of stabilizer adsorption and eventually the SPION-C end particle size. Stirring speed effects, the reaction environment of SPION-C during the addition and adsorption of citrate ions onto SPION. Hence, the surface modification of the nanoparticles by the addition of a stabilizer drastically suppresses the nanoparticle size<sup>20<\/sup>.<\/p>\n<table style=\"width: 70%;\" border=\"1\" cellpadding=\"5\">\n<tbody>\n<tr>\n<td><img decoding=\"async\" class=\"alignnone size-thumbnail wp-image-41002\" src=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig1-150x150.jpg\" alt=\"Figure 1: Particle Size of SPION-C.\" width=\"150\" height=\"150\" srcset=\"https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig1-150x150.jpg 150w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig1-256x256.jpg 256w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig1.jpg 797w\" sizes=\"(max-width: 150px) 100vw, 150px\" \/><\/td>\n<td><strong>Figure 1: Particle Size of SPION-C.<\/strong><\/p>\n<p><a href=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig1.jpg\" target=\"_blank\">Click here to view Figure<\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p>Superparamagnetic iron oxide nanoparticle synthesis starts with the core formation, followed by nucleus growth. The latter needs to be prevented at the correct designate to achieve the intended size for nanoparticles to obtain superparamagnetic properties. Nuclei or crystal growth is inhibited by the adsorption of citrate ions on the surface of SPION which stabilizes and prevents these particles from aggregation<sup>20<\/sup>. Amid this step, the rate of inhibition by the stabilizer will influence the resulting hydrodynamic size of the nanoparticles. After the black precipitate formation at basic conditions, the stabilizer solution should be rapidly distributed throughout the SPION solution.<\/p>\n<p>An increase of stirring speed from 3000 rpm to 9000 rpm improved nanoparticle hydrodynamic size from thousands of nanometers to below 30 nm, as shown by batch B and E (Table 2). Essentially, the purpose of stirring is to create a homogenous solution. Stirring speed influences fluid flow, where within the fluids are the residing nanoparticles, and therefore different stirring speeds will cause the SPION and TCD to migrate and interact with each other at different rates<sup>21<\/sup>. Nonetheless, in our case, at very high speeds (12000 rpm), parameters of SPION-C were found to be less preferable. Agglomeration leading to higher hydrodynamic size initiated by the immense interaction of particles is believed to be the reason. Smaller SPION-C might also have aggregated, forming larger clusters leading to an increase in hydrodynamic size and poor polydispersity due to various cluster sizes<sup>22<\/sup>, but similar \u03b6 potential for all SPION-C batches. Our findings show that different stirring speeds influence the hydrodynamic size of the SPION-C, and at very high speeds, their polydispersity indexes.<\/p>\n<p>All SPION showed negative \u03b6 potential ranging from 23.23 mV to 31.3 mV, and \u03b6 potential of SPION-C for batches B, C, E, and F ranged from -37.1 mV to -54.8 mV (B &gt; E &gt; F &gt; C) as seen in Table. 2, meaning that all SPION-C have moderate (31 \u2013 40 mV) to fairly good (41 \u2013 60 mV) colloidal stability<sup>23<\/sup>. The increase in \u03b6 potential of SPION after stabilization was up to 31 mV, surpassing previous literature<sup>10,25<\/sup>. Without stabilization, SPIONs acquired less stability shown by their lower \u03b6 potential. Visually, SPION would sediment substantially faster than SPION-C for all process conditions. After approximately 15 minutes<sup>12<\/sup>, a clear borderline between the sediment (SPION) and the solvent can be distinguished, whereas the SPION-C still presented a black homogenous solution (Table 2).<\/p>\n<p>Citrate posses\u2019 three carboxylate functional groups where at least one will face outwards on the SPION-C\u2019s surface upon adsorption which accounts for their negative and higher \u03b6 potential compared to SPION<sup>23,24<\/sup>. The citrate ions create steric hindrance to prevent SPION from interacting with each other<sup>12<\/sup>. Such steric hindrance is categorized as electro kinetic stabilization originating from anionic carboxyl groups. Besides fabrication of hydrophilic SPION, the free carboxyl group facing out to the solvent will aid SPION to be conjugated or functionalized to another molecule, for example, a drug, carrier, or a fluorescent dye.<\/p>\n<p><strong>Influence of Stabilizer Concentration<\/strong><\/p>\n<p>Comparing batch E to G, twice as much stabilizer concentration resulted in a narrower polydispersity index (0.346 to 0.311) and better stability (-41.7 mV to -50.8 mV) of SPION-C. The availability of the stabilizer was more precise as it had better coverage on the surface of the SPION. Moreover, as its concentration was higher, the time for it to be distributed in the solution was fast enough to prevent larger nanoparticle growth.<\/p>\n<p><strong>Table 3: Influence of Stabilizer Concentration on SPION-C.<\/strong><\/p>\n<table style=\"width: 95%;\" border=\"1\" cellspacing=\"0\" cellpadding=\"4\">\n<tbody>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>Batch<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"16%\"><strong>Stirring speed (rpm)<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"24%\"><strong>Stabilizer concentration<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"17%\"><strong>Size<sup>I<\/sup> \u00b1 SD<sup>II<br \/>\n<\/sup><\/strong><strong>(nm)<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"17%\"><strong>PDI \u00b1 SD<sup>II<\/sup><\/strong><\/td>\n<td style=\"text-align: center;\" width=\"16%\"><strong>\u03b6<\/strong> <strong>potential \u00b1 SD<sup>II <\/sup>(mV)<\/strong><\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>E<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"16%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"24%\">0.503 M<\/td>\n<td style=\"text-align: center;\" width=\"17%\">25.58 \u00b1 7<\/td>\n<td style=\"text-align: center;\" width=\"17%\">0.346 \u00b1 0.01<\/td>\n<td style=\"text-align: center;\" width=\"16%\">-41.67 \u00b1 2.1<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"8%\"><strong>G<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"16%\">9000<\/td>\n<td style=\"text-align: center;\" width=\"24%\">1.006 M<\/td>\n<td style=\"text-align: center;\" width=\"17%\">25.94 \u00b1 2<\/td>\n<td style=\"text-align: center;\" width=\"17%\">0.312 \u00b1 0.09<\/td>\n<td style=\"text-align: center;\" width=\"16%\">-50.8 \u00b1 3.9<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><sup>I<\/sup>Size distribution by number<\/p>\n<p><sup>II<\/sup><em>SD<\/em> standard deviation (n=3)<\/p>\n<p><strong>Influence of Stabilizer Adsorption Temperature<\/strong><\/p>\n<p>Two different temperatures for citrate adsorption experimented were at 60<sup>o<\/sup>C and 90<sup>o<\/sup>C. It was shown that the temperature affects the reaction temperature during stabilizer addition and highly determines the success of citrate adsorption onto the SPION surface (Table 4.) Over the SPION growth phase, an elevated temperature is required to aid citrate adsorption onto the nanoparticles\u2019 surface, as higher temperatures accelerate the chemical adsorption process<sup>22<\/sup>. SPION-C produced with the lower temperature sedimented at a higher velocity. This can be explained by failure the of the citrates\u2019 carboxyl groups to be adsorbed completely onto the SPION surface. Therefore, on its surface areas where citrate isn\u2019t available, SPION can interact with each other, meaning less stabilization and leading to particle growth<sup>12<\/sup>. After 3 hours there was a clear difference between batch D, G, H, and being the most stable, was batch G. Visual results are also reinforced by the particle size and \u03b6 potential where the partially stabilized SPION (batch H) have a larger particle size and lower \u03b6 potential than fully stabilized SPION (batch G), however a smaller particle size and higher \u03b6 potential than SPION (batch D).<\/p>\n<table style=\"width: 70%;\" border=\"1\" cellpadding=\"5\">\n<tbody>\n<tr>\n<td><img decoding=\"async\" class=\"alignnone size-thumbnail wp-image-41006\" src=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_tab4-150x150.jpg\" alt=\"Table 4: Influence of Stabilizer Adsorption Temperature on SPION-C.\" width=\"150\" height=\"150\" srcset=\"https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_tab4-150x150.jpg 150w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_tab4-256x256.jpg 256w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_tab4.jpg 765w\" sizes=\"(max-width: 150px) 100vw, 150px\" \/><\/td>\n<td><strong>Table 4: Influence of Stabilizer Adsorption Temperature on SPION-C.<\/strong><\/p>\n<p><a href=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_tab4.jpg\" target=\"_blank\">Click here to view Table<\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p><strong>FTIR Analysis <\/strong><\/p>\n<p>The fingerprint of iron oxide (Fe-O) from SPION is noticeable at 584.45 cm<sup>-1<\/sup> (Fig. 1) where stated in previous literature corresponds to magnetite. The appearance of new bands at 1200 cm<sup>-1<\/sup>, 900 cm<sup>-1<\/sup>, and 850 cm<sup>-1<\/sup> on SPION-C proves the presence of citrate on the nanoparticles. The chemical bond is believed to happen between carboxyl groups from trisodium citrate dihydrate and hydroxyls of iron oxides through esterification12<sup>,26<\/sup>.<\/p>\n<p>Strong broad bands stretching from 3500 \u2013 2500 cm<sup>-1<\/sup> correspond to the vibrational stretching of -CH and -OH of carboxylate functional groups of SPION-C which are also found on the trisodium citrate dihydrate (TCD) spectrum but have slightly shifted to a higher wavelength. The vibrational asymmetric stretching of SPION-C at 1589.40 cm<sup>-1<\/sup> assigns to carbonyl (C=O), and at 1200 cm<sup>-1<\/sup> points the C-O single bond of the adsorbed citrates. Crowded peaks between 1600 \u2013 1200 of \u00a0TCD have shifted after TCD conjugation to SPION as seen in SPION-C<sup>27<\/sup>. Analyzing the FTIR spectrum confirms that citrate has been successfully coated onto the surface of SPION.<\/p>\n<table style=\"width: 70%;\" border=\"1\" cellpadding=\"5\">\n<tbody>\n<tr>\n<td><img decoding=\"async\" class=\"alignnone size-thumbnail wp-image-41008\" src=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig2-150x150.jpg\" alt=\"Figure 2: FTIR Spectrum of SPION, Trisodium Citrate Dihydrate, and SPION-C.\" width=\"150\" height=\"150\" srcset=\"https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig2-150x150.jpg 150w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig2-256x256.jpg 256w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig2.jpg 786w\" sizes=\"(max-width: 150px) 100vw, 150px\" \/><\/td>\n<td><strong>Figure 2: FTIR Spectrum of SPION, Trisodium Citrate Dihydrate, and SPION-C.<\/strong><\/p>\n<p><a href=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig2.jpg\" target=\"_blank\">Click here to view Figure<\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p><strong>Fluorescence Spectroscopy<\/strong><\/p>\n<p>Both SPION and SPION-C had excitation maximum at \u03bb 467 nm and emission maximum at \u03bb 554 \u2013 555 nm. The emission peak of Fe<sub>3<\/sub>O<sub>4<\/sub> previously reported was identified near 560 nm<sup>28<\/sup>. No shift in maximum wavelengths was found which demonstrates the perseverance of magnetite after stabilization with citrate.<\/p>\n<table style=\"width: 70%;\" border=\"1\" cellpadding=\"5\">\n<tbody>\n<tr>\n<td><img decoding=\"async\" class=\"alignnone size-thumbnail wp-image-41009\" src=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig3-150x150.jpg\" alt=\"Figure 3: Fluorescence Spectroscopy of SPION and SPION-C.\" width=\"150\" height=\"150\" srcset=\"https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig3-150x150.jpg 150w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig3-256x256.jpg 256w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig3.jpg 797w\" sizes=\"(max-width: 150px) 100vw, 150px\" \/><\/td>\n<td><strong>Figure 3: Fluorescence Spectroscopy of SPION and SPION-C.<\/strong><\/p>\n<p><a href=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig3.jpg\" target=\"_blank\">Click here to view Figure<\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p><strong>XRD Analysis<\/strong><\/p>\n<p>X-ray diffractograms of SPION and SPION-C show crystalline peaks representing magnetite. The 2\u03b8 positions of 18.35<sup>o<\/sup>, 30.26<sup>o<\/sup>, 35.56<sup>o<\/sup>, 43.31<sup>o<\/sup>, 53.74<sup>o<\/sup>, 57.30<sup>o<\/sup>, and 62.74<sup>o<\/sup> were for SPION and 18.21<sup>o<\/sup>, 30.07<sup>o<\/sup>, 35.34<sup>o<\/sup>, 43.07<sup>o<\/sup>, 53.31<sup>o<\/sup>, 56.83<sup>o<\/sup>, 62.41<sup>o<\/sup> for SPION-C confirming hkl values (111), (220), (311), (400), (422), (511), and (440) (ICSD 98-015-8742). Intensity weakening of peaks resembling magnetite is due to the citrate coating on the surface<sup>29<\/sup>. Our diffractograms show no (210), (300), (213), or (110) peaks known to indicate the presence of maghemite<sup>30\u201332<\/sup>. Nonetheless, the oxidized phase of magnetite is hard to distinguish using XRD owing to the similarity of lattice type and constant<sup>24<\/sup>. The magnetite phase of SPION was found to have a cubic crystal structure with an Fd-3m space group, and a cubic cell lattice parameter of 8.37 \u00c5, in accordance with reported studies. Furthermore, citrate stabilization proved to decrease the crystalline size of SPION and SPION-C from 6.03 nm to 2.79 nm. This can also be supported by broader peaks in SPION-C indicating the decrease in crystalline size9<sup>,33<\/sup>.<\/p>\n<table style=\"width: 70%;\" border=\"1\" cellpadding=\"5\">\n<tbody>\n<tr>\n<td><img decoding=\"async\" class=\"alignnone size-thumbnail wp-image-41010\" src=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig4-150x150.jpg\" alt=\"Figure 4: XRD Intensity Peaks of SPION-C.\" width=\"150\" height=\"150\" srcset=\"https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig4-150x150.jpg 150w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig4-256x256.jpg 256w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig4.jpg 613w\" sizes=\"(max-width: 150px) 100vw, 150px\" \/><\/td>\n<td><strong>Figure 4: XRD Intensity Peaks of SPION-C.<\/strong><\/p>\n<p><a href=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig4.jpg\" target=\"_blank\">Click here to view Figure<\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p><strong>Morphological Analysis<\/strong><\/p>\n<p>The morphology of SPION-C is almost spherical shaped (Fig. 6), and that they exist in clusters or agglomerates due to agglomeration during processing. Based on the TEM results, it is visually distinguishable between the SPION core and its citrate coating with particle sizes below 20 nm. This critical size provides the mean for SPION-C to possess superparamagnetic properties. When compared results from dynamic light scattering (DLS), a larger particle size compared to TEM results was generated because DLS measures the hydrodynamic diameter and will put into account the solvent layer where the citrate molecules penetrate in the solvent playing a role in the hydration of the SPION-C<sup>34<\/sup>. The D<sub>V10<\/sub> of SPION-C show that the DLS method was able to detect nanoparticles below 20 nm, though due to the formation of agglomerates during fabrication and the possibility of aggregation of SPION-C in aqueous media, the Z-avg shifted to higher values, whereas TEM facilitates the visualization of the individual core size of each nanoparticle<sup>35<\/sup>.<\/p>\n<table style=\"width: 70%;\" border=\"1\" cellpadding=\"5\">\n<tbody>\n<tr>\n<td><img decoding=\"async\" class=\"alignnone size-thumbnail wp-image-41011\" src=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig5-150x150.jpg\" alt=\"Figure 5: TEM Images of SPION-C Magnified x30000 (Left) and x200000 (Right)\" width=\"150\" height=\"150\" srcset=\"https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig5-150x150.jpg 150w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig5-256x256.jpg 256w, https:\/\/biomedpharmajournal.org\/staging\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig5.jpg 783w\" sizes=\"(max-width: 150px) 100vw, 150px\" \/><\/td>\n<td><strong>Figure 5: TEM Images of SPION-C Magnified x30000 (Left) and x200000 (Right)<\/strong><\/p>\n<p><a href=\"https:\/\/biomedpharmajournal.org\/wp-content\/uploads\/2021\/10\/Vol14No3_Syn_Sut_Fig5.jpg\" target=\"_blank\">Click here to view Figure<\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<p><strong>Stability of SPION-C<\/strong><\/p>\n<p>During storage, the SPION-C produced with the optimized processing condition showed great colloidal stability. The pH of the environment surrounding the nanoparticles will affect its \u03b6 potential and hence determine its colloidal stability10<sup>,24<\/sup>. In this study, the use of trisodium citrate dihydrate (TCD) contributed to the end solution of all SPION-C batches having a pH ranging from 6.74 \u2013 7.33 which helped maintain the \u03b6 potential of the nanoparticles. The physical stability of the nanoparticle was also ensured by size and PDI during the storage period. These results prove that our method has succeeded in creating highly stable citrate stabilized superparamagnetic iron oxide nanoparticles as shown in Table 5.<\/p>\n<p><strong>Table 5: Stability of SPION-C.<\/strong><\/p>\n<table style=\"width: 95%;\" border=\"1\" cellspacing=\"0\" cellpadding=\"4\">\n<tbody>\n<tr>\n<td style=\"text-align: center;\" width=\"155\"><strong>Storage<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"175\"><strong>Size<sup>I<\/sup> \u00b1 SD<sup>II<br \/>\n<\/sup><\/strong><strong>(nm)<\/strong><\/td>\n<td style=\"text-align: center;\" width=\"119\"><strong>PDI \u00b1 SD<sup>II<\/sup><\/strong><\/td>\n<td style=\"text-align: center;\" width=\"199\"><strong>\u03b6<\/strong> <strong>\u00a0potential \u00b1 SD<sup>II\u00a0 <\/sup>(mV)<\/strong><\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"155\">Initial<\/td>\n<td style=\"text-align: center;\" width=\"175\">25.94 \u00b1 2<\/td>\n<td style=\"text-align: center;\" width=\"119\">0.312 \u00b1 0.09<\/td>\n<td style=\"text-align: center;\" width=\"199\">-50.8 \u00b1 3.9<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"155\">Week 3<\/td>\n<td style=\"text-align: center;\" width=\"175\">19.8 \u00b1 7<\/td>\n<td style=\"text-align: center;\" width=\"119\">0.339 \u00b1 0.03<\/td>\n<td style=\"text-align: center;\" width=\"199\">-42.2 \u00b1 4.2<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"155\">Week 10<\/td>\n<td style=\"text-align: center;\" width=\"175\">21.29 \u00b1 6<\/td>\n<td style=\"text-align: center;\" width=\"119\">0.336 \u00b1 0.05<\/td>\n<td style=\"text-align: center;\" width=\"199\">-43.9 \u00b1 2.3<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"155\">Week 30<\/td>\n<td style=\"text-align: center;\" width=\"175\">23.98 \u00b1 2<\/td>\n<td style=\"text-align: center;\" width=\"119\">0.275 \u00b1 0.08<\/td>\n<td style=\"text-align: center;\" width=\"199\">-39.5 1.6<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" width=\"155\">Range<\/td>\n<td style=\"text-align: center;\" width=\"175\">11.95 \u2013 28.64 nm<\/td>\n<td style=\"text-align: center;\" width=\"119\">0.204 \u2013 0.393<\/td>\n<td style=\"text-align: center;\" width=\"199\">-37.9 \u2013 -54.8<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><sup>I<\/sup>Size distribution by number<\/p>\n<p><sup>II<\/sup><em>SD<\/em> standard deviation (n=3)<\/p>\n<p><strong>Conclusion<\/strong><\/p>\n<p>Superparamagnetic iron oxide nanoparticles stabilized by trisodium citrate dihydrate have been produced using the direct co-precipitation method. The optimized processing condition was 9000 rpm stirring speed, accompanied by 1.006 M of stabilizer and stabilizer adsorption at 90<sup>o<\/sup>C. Characterization of nanoparticles below 20 nm which is critical for biomedical use, was confirmed by DLS, FTIR, fluorescence spectroscopy, XRD, and TEM. Furthermore, stability of SPION-C during storage had been achieved. The optimized SPION-C can be further conjugated to a carrier or even to the desired therapeutic agent without additional modification.<\/p>\n<p><strong>Funding Source<\/strong><\/p>\n<p>This research was funded by Universitas Indonesia, grant number NKB-1467\/UN2.RST\/HKP.05.00\/2020.<\/p>\n<p><strong>Authors\u2019 Contributions<\/strong><\/p>\n<p>All authors have contributed according to their duties and responsibilities.<\/p>\n<p><strong>Conflict of Interests<\/strong><\/p>\n<p>No conflict of interests has been declared by all authors.<\/p>\n<p><strong>References<\/strong><\/p>\n<ol>\n<li>Unterweger H, D\u00e9zsi L, Matuszak J, Janko C, Poettler M, Jordan J, et al. Dextran-coated superparamagnetic iron oxide nanoparticles for magnetic resonance imaging: Evaluation of size-dependent imaging properties, storage stability and safety. Int. J. 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