Open Access Article
Tawakalit D. Abdulyekeen
a,
Cécile Sicard-Roselli
a,
Vincent Huc
b,
Hynd Remita
a and
Isabelle Lampre
*a
aUniversité Paris-Saclay, CNRS, Institut de Chimie Physique UMR 8000, 91400 Orsay, France. E-mail: isabelle.lampre@universite-paris-saclay.fr
bUniversité Paris-Saclay, CNRS, Institut de Chimie Moléculaire et des Matériaux, UMR 8182, 91400 Orsay, France
First published on 15th April 2026
Gold nanoparticles (AuNPs) are widely studied due to their unique physicochemical properties, which are highly dependent on their size, shape, and composition. Efficient and environmentally friendly synthesis methods and effective stabilisation agents are essential for fabricating AuNPs with controlled sizes and shapes. This study explores the radiolytic synthesis method, a green synthesis approach using ionising radiation (gamma irradiation), and investigates the use of a thermosensitive polymer, poly(N-isopropylacrylamide) (PNIPAM), and its monomer, N-isopropylacrylamide (NIPAM), for stabilising gold nanoparticles in aqueous solutions. The resulting PNIPAM-AuNPs and NIPAM-AuNPs were spherical, homogenously dispersed, with average sizes of 5.4 nm and 3.5 nm, respectively, and exhibited high stability at room temperature over a long time. Thermal analysis revealed enhanced thermal responsiveness for PNIPAM-AuNPs, an effect not observed with the NIPAM-AuNPs. The AuNPs demonstrated excellent catalytic activity in the reduction of 4-nitrophenol (4-NP) in the presence of sodium borohydride and showed efficient plasmonic photocatalytic activity in the visible-light-driven reduction of 4-nitrothiophenol (4-NTP). These findings support the potential of radiolytically synthesised polymer-stabilised AuNPs for catalysis and environmental remediation applications.
One of the major challenges associated with synthesising metallic nanoparticles (MNPs) in solution is stabilising them against aggregation for a long period of time.15 This instability arises from their inherently high surface energy (excess energy associated with surface atoms), resulting from their high surface-to-volume ratio.15 This surface energy makes it difficult to control the morphology of MNPs, as they tend to aggregate easily due to attractive forces such as van der Waals forces, especially in the absence of counteracting forces. These attractive effects can be mitigated using a stabilising agent that can provide steric and/or electrostatic stability to the MNPs, allowing control over their size and shape and preserving their properties. These stabilisers include polymers,15–17 ligands,18 surfactants,19 and supports.20 They are chosen based on the morphology and specific applications desired for the MNPs. Polymer-based stabilisation is one of the most effective strategies for preventing nanoparticle aggregation over extended periods. This approach enhances the stability of nanoparticles and facilitates the formation of hybrid materials with unique physical and chemical properties.16 This dual functionality not only preserves the intrinsic characteristics of the nanoparticles but also introduces additional functionality by combining the intrinsic properties of both components, thereby broadening their range of potential applications.15,16,21 Various types of polymer networks have been employed for nanoparticle stabilisation, including latex particles,22 polyelectrolyte brushes,23 stimuli-responsive polymers, etc.24–27
Thermosensitive polymers are a class of stimuli-responsive polymers that exhibit changes in response to environmental modifications, in this case, temperature. The use of these temperature-responsive polymers has led to the development of novel materials whose physicochemical properties can be easily tuned for potential applications such as catalysis, medicine, smart material devices, etc.15,27,28 Usually, thermosensitive polymers exhibit a miscibility change in aqueous solutions in response to temperature: if dissolution is caused by heat, there is an upper critical solution temperature (UCST), while if a phase separation occurs by heating, a lower critical solution temperature (LCST) exists.29 These thermosensitive polymers, which can be either synthetic or natural, include poly(N-isopropyl acrylamide) (PNIPAM),30 poly(N-diethyl acrylamide) (PDEAm),31 poly[oligo (ethylene glycol) methacrylate] (POEGMA),32 etc. Poly(N-isopropylacrylamide) (PNIPAM) is a thermally responsive polymer that undergoes a reversible phase transition with a change in temperature in aqueous medium.25,33,34 This transition involves a conformational change in the PNIPAM chain, ranging from a disordered state and random coil to an ordered, collapsed globule state.35 Above its lower critical solution temperature (LCST) of about 32 °C, the PNIPAM polymer becomes hydrophobic and undergoes chain collapse, which leads to aggregation in solution due to hydrophobic interactions and hydrogen bonding fluctuation.27 In contrast, the polymer is hydrophilic and appears soluble below its LCST due to the hydrophilic group on the polymer chain undergoing strong hydrogen bonds with the surrounding water molecules.
PNIPAM has been one of the most widely used smart polymers in the stabilisation/coating of metallic nanoparticles (gold, silver, etc.), resulting in a core–shell system with the nanoparticles embedded in the polymer shell.16,17,26,36 The use of thermosensitive polymer (PNIPAM) for stabilising metallic nanoparticles enables the design of a nanomaterial composite with enhanced properties, combining the thermal switching properties of the polymer with the surface plasmon effect of the metallic nanoparticles for potential applications.27,37,38 These nanocomposite materials have been achieved utilising several methods, such as the mixing of pre-formed thiol-terminated PNIPAM and AuNPs,26 in situ chemical reduction of gold salts in the presence of PNIPAM,27,37 in situ polymerisation of NIPAM and reduction of gold salt,39 or the growth of polymer chains on the surface of the AuNPs.16,40
Several studies have reported the stabilisation of AuNPs with PNIPAM, investigated their thermal properties and explored their use in catalysis. Du et aI.27 synthesised noble metal nanoparticles (Au, Pt, Pd) stabilised by PNIPAM via liquid-phase reduction using ascorbic acid and sodium borohydride as reducing agents. The formed MNPs demonstrated efficient catalytic activity in the reduction of nitroarenes. Among them, PNIPAM-AuNPs stood out due to their excellent stability and high catalytic performance. Zhu et al.39 employed gamma radiation to prepare thermosensitive PNIPAM-AuNP composite hydrogels through in situ monomer polymerisation and simultaneous reduction of gold salts using a high irradiation dose (>70 kGy). The obtained composites also exhibited efficient catalytic activity. In efforts to study the thermosensitive properties of PNIPAM-AuNPs, Jones et al.16 and Li et al.26 examined the effect of free PNIPAM chains in the colloidal solutions on the conformational changes of PNIPAM anchored to the AuNP surface upon heating. Jones et al.16 suggested that hydrophobic interactions between free polymer chains and those on the nanoparticles' surface promoted aggregation upon temperature increase. In contrast, Li et al.26 argued that the observed turbidity was due to free PNIPAM alone, and not conformational changes in surface-bound PNIPAM. However, differences in the nanoparticle synthesis methods and end groups of PNIPAM used in these studies make direct comparisons difficult.
In order to better understand the thermoresponsive behaviour of PNIPAM and NIPAM-stabilised gold nanoparticles and to investigate their plasmonic activities, we present here the radiolytic synthesis of AuNPs stabilised by either PNIPAM or NIPAM monomers (Fig. 1). Indeed, radiolytic synthesis has emerged as a powerful technique for effectively controlling the size and shape of metallic nanoparticles in solutions or in heterogeneous media. This method involves the irradiation of the sample solutions containing metallic ions and stabilising agents by ionising radiation.41–44 Hence, the nanoparticles are formed via the reduction of the AuIII ions in aqueous solution in the presence of PNIPAM or NIPAM, using gamma radiation. In this paper, we investigate the thermal behaviour and study the catalytic and photocatalytic ability of the formed PNIPAM-AuNPs and NIPAM-AuNPs using model reactions easily followed spectroscopically: the reduction of hexacyanoferrate(III) ([Fe(CN)6]3−),45,46 and the reduction of 4-nitrophenol (4-NP) and 4-nitrothiophenol (4-NTP) used as model pollutants.47 Taking advantage of the thermosensitivity of the polymer, the present study aims to establish the role played by plasmonic heating and hot-electron generation upon plasmon excitation of the gold nanoparticles.
000, 100%), sodium hydroxide (NaOH, ≥98%), tert-butanol ((CH3)3COH, ≥99.7%), 4-aminophenol (4-AP, C6H7NO, 98%), 4-nitrothiophenol (4-NTP, C6H5NO2S, 80%), 4-nitrophenol (4-NP, C6H5NO3, ≥99.5%), sodium borohydride (NaBH4, 98%), 2-propanol (99.5%), potassium hexacyanoferrate(III) (K3[Fe(CN)6]), and triethanolamine (TEOA, C6H15NO3, ≥99%) were all purchased from Sigma-Aldrich, and used without any further purification. All the aqueous solutions were prepared with ultrapure water (Millipore system, 18.2 MΩ cm). All glassware were washed with aqua regia and thoroughly washed with deionised water before use.
Alkaline aqueous solutions of PNIPAM-AuNP or NIPAM-AuNP catalysts ([Au0] = 0.148 mM, pH around 11) were obtained by adding a few drops of 0.15 M NaOH aqueous solution. Aqueous solutions containing 2 mM [Fe(CN)6]3−, or 0.489 mM 4-NP, or 0.163 mM 4-NTP were prepared, and the pH of the solutions was adjusted in the range of 10–11 before use by adding a small amount of a 0.15 M NaOH aqueous solution.
In the case of 4-NP and 4-NTP, this adjustment resulted in a colour change of the solutions, from pale yellow to dark yellow (Fig. S1, inset) and changes in the UV-visible absorption spectra (Fig. S1). These changes are due to the formation of phenolate ions resulting from deprotonation of the phenolic group27 (pKa = 7.15 for 4-NP48 and 4.71 for 4-NTP49). The protonated form of 4-NP (4-NTP) absorbs at 317 nm (305 nm), while the phenolate ion presents a maximum absorption at 400 nm (405 nm) (Fig. S1). 0.5 mL of the alkaline 4-NP solution was then added to a reactor containing 2.49 mL of water ([4-NP] = 0.0815 mM). Then, 1.25 mg of NaBH4 was added to the mixture ([NaBH4] = 11 mM) to achieve a concentration of the reducing species 135 times greater than the initial concentration of 4-NP; subsequently, 10.9 µL of the catalyst solution was then added to the sample mixture ([Au0] = 0.538 µM). The solution was kept in the dark by covering the cuvette with aluminium foil due to the sensitivity of the catalysts and pollutants to light; then, UV-visible absorption spectra were recorded at 10-minute intervals. In the case of 4-NTP, 1.5 mL of the 4-NTP solution, 1.5 mL of water, 1.5 mg of NaBH4 and 10.9 µL of the catalyst solution were used to ensure similar concentrations of catalysts and pollutants as in the case of 4-NP, i.e., the reaction mixture contained 0.0815 mM 4-NTP, 11 mM NaBH4, and 0.538 µM catalyst.
For the reduction of [Fe(CN)6]3−, 750 µL of a K3Fe(CN)6 stock solution was added to a reactor, followed by 2.2 mL of the catalyst solution and 60 µL of TEOA. The solution containing 0.5 mM K3Fe(CN)6, 0.02 M TEOA, and 0.1077 mM catalyst (Au0) was then deaerated by bubbling nitrogen gas for 10 minutes and kept in the dark by wrapping the cuvette with aluminium foil. UV-visible absorption spectra were also recorded at 10-minute intervals.
For the nitroarene reduction, the reaction mixtures containing 4.35 × 10−5 M of either 4-NP or 4-NTP and 1.077 × 10−4 M of either PNIPAM-AuNPs or NIPAM-AuNPs were added to a 1 cm optical pathlength quartz cuvette sealed with a septum cap. The solutions were deaerated by bubbling nitrogen gas through them for 40 minutes to remove dissolved oxygen and to allow maximum adsorption of pollutant molecules on the surface of the NPs (Fig. S14). The solutions were then illuminated using a solar lamp (Solar Simulator LS0306, 300 W Xe light) positioned 16 cm from the sample to ensure uniform illumination or a homemade LED reactor (525 nm) (Fig. S2). A 500 nm long-pass colour filter (Fig. S2a) was used with the solar lamp to prevent the direct photoactivation of 4-NTP while exciting the AuNPs LSPR around 520 nm. The photocatalytic reaction was then monitored by recording the UV-visible absorption spectra at 1-hour intervals.
For the photocatalytic reduction of [Fe(CN)6]3−, solutions containing 5 × 10−4 M of K3Fe(CN)6 and 1.11 × 10−4 M of catalyst (Au0) were prepared. The solutions were deaerated by bubbling nitrogen gas for 10 minutes, and then illuminated using the LED reactor as described above.
The stability of the PNIPAM-AuNPs synthesised at an irradiation dose of 1.1 kGy was investigated. The nanoparticles remained stable over several days, as evidenced by the absence of significant changes in the spectra recorded a few days after synthesis (Fig. S3). Furthermore, the solution remained stable for several months, indicating effective stabilisation by PNIPAM. A similar result has already been reported by Du et al., who mentioned that the chemically synthesised PNIPAM-AuNPs remained stable for a long time (over six months).27
The TEM micrographs of the PNIPAM-AuNPs synthesised with an irradiation dose of 1.1 kGy and their particle size distribution are shown in Fig. 2b and c. The obtained nanoparticles have a spherical shape and appear polydisperse. The average diameter of the PNIPAM-AuNP gold core is estimated to be 5.4 ± 1.8 nm (Fig. 2c), which is consistent with the absorption spectra (Fig. 2a).
The TEM micrographs of the NIPAM-AuNPs synthesised with an irradiation dose of 1.1 kGy, and their particle size distribution are shown in Fig. 2e and f. The obtained nanoparticles are spherical and appear monodisperse, with an average size of 3.5 ± 0.9 nm, slightly smaller than that of PNIPAM-AuNPs (Fig. 2f). They also present a necklace-like organisation (Fig. 2e).
As for PNIPAM, the NIPAM-AuNPs are stable in solution as the absorption spectrum of the solution recorded a day after the irradiation is identical to that shown in Fig. 2d. Nevertheless, in contrast to the PNIPAM-AuNPs, these spectra were not recorded immediately after irradiation. Indeed, a change in colour of the NIPAM-AuNP solution is observed immediately after irradiation: the initially purple-coloured solution turns pink after a couple of hours (Fig. 3a, inset). The spectrum registered immediately after irradiation differs from the others as it presents a broader absorption band. To study this phenomenon, several parameters were varied, including the concentration of the metallic salt, the concentration NIPAM, and the use of tert-butanol as a scavenger instead of propan-2-ol. However, similar results were observed in all cases. The narrowing of the absorption band, coupled with the colour change, indicates an evolution in the particle size and distribution, which is confirmed by TEM images. Immediately after synthesis, the nanoparticles appear elongated (Fig. 3b), while a couple of hours after synthesis, the NIPAM-AuNPs were spherical, monodisperse, and free from aggregation (Fig. 2e).
Fig. 4 presents the hydrodynamic sizes of the PNIPAM-AuNPs, NIPAM-AuNPs, irradiated and non-irradiated PNIPAM measured in aqueous solution using dynamic light scattering at temperatures ranging from 25 °C to 45 °C. In the absence of irradiation, the phase transition temperature (PTT) of PNIPAM is found to be 33 °C, a typical value for pure PNIPAM, and the apparent hydrodynamic diameter changes from ∼25 nm below the LCST up to 220 nm above it. After irradiation, the PTT of PNIPAM is lowered, ∼30 °C, and the apparent diameters below and above the PTT are increased, 180 nm and 400 nm, respectively. These results indicate changes in the polymer structures due to reactions with the radiolytic species. This suggests that irradiation induces crosslinking within the PNIPAM chains, which restricts chain mobility and facilitates an earlier coil-to-globule transition upon heating. The smaller size observed in the non-irradiated PNIPAM (Fig. 4) can also be attributed to the absence of crosslinking, allowing polymer chains to remain more dispersed in solution.
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| Fig. 4 Hydrodynamic sizes measured by dynamic light scattering for PNIPAM-AuNPs, NIPAM-AuNPs, irradiated PNIPAM, and non-irradiated PNIPAM at different temperatures. | ||
For PNIPAM-AuNPs (Fig. 4), the PTT is observed to be slightly higher (∼30.5 °C) than that of the irradiated PNIPAM-only solution (∼30 °C). Below this PTT, no significant change in nanoparticle size is observed. However, above the PTT, a marked increase in the hydrodynamic size of PNIPAM-AuNPs is observed, reaching a plateau at around 34 °C. At elevated temperature, DLS measurements show a narrow size distribution with a single peak around 531 nm (Fig. S4), indicating the formation of a larger polymeric matrix with embedded AuNPs. The absence of additional peaks (Fig. S4) supports the idea that the nanoparticles are not freely dispersed but incorporated into the collapsed polymer network due to hydrophobic interactions of PNIPAM above the LCST. This thermal response confirms the thermosensitive behaviour of the PNIPAM layer.
The larger hydrodynamic sizes observed by DLS, compared to those measured via TEM, are expected due to the swollen state of the hydrated polymer layer in aqueous solutions below the LCST.15 The irradiated PNIPAM-only solution showed slightly larger hydrodynamic sizes below the PTT than the PNIPAM-AuNPs. This difference can be attributed to the absence of competition for reducing species produced during irradiation, which allows more polymer network formation, resulting in larger sizes in DLS measurements. However, above the PTT, the sizes of the irradiated PNIPAM-only solution were smaller than those of the PNIPAM-AuNPs. This is consistent with the formation of polymer aggregates in aqueous solution, where the PNIPAM collapses into compact structures, while in PNIPAM-AuNPs, the presence of embedded AuNPs leads to larger average particle sizes. It is worth noting that the decrease in size observed for the irradiated PNIPAM-only solution at temperatures of 40 °C and 45 °C can be attributed to the increased expulsion of water and enhanced collapse of the PNIPAM chains as the temperature rises. This leads to more compact structures due to stronger hydrophobic interactions.
In contrast, the hydrodynamic size of PNIPAM-AuNPs remains relatively constant from 34 °C and above, suggesting that the embedded AuNPs hindered additional polymer chain collapse. In contrast to PNIPAM-AuNPs, the hydrodynamic size of the NIPAM-AuNPs remains unchanged whatever the temperature (Fig. 4). This indicates the absence of the thermoresponsive behaviour typically associated with PNIPAM. However, the larger hydrodynamic sizes determined by DLS, compared to those measured by TEM, suggest the presence of oligomeric layers adsorbed onto the surface of the AuNPs.
Fig. 5 shows the UV-vis extinction spectra of the PNIPAM-AuNPs and NIPAM-AuNPs at 25 °C (below PTT), 40 °C (above PTT), and after cooling back down to 25 °C. PNIPAM-AuNPs showed noticeable broadening and deformation of the extinction spectrum at elevated temperature (Fig. 5a). This may be attributed to significant light scattering related to the formation of large polymer aggregates due to polymer hydrophobic interactions above the LCST, as evidenced from DLS measurements. It is important to note that no purification by centrifugation was performed prior to analysis, so possible free crosslinked PNIPAM chains remaining in the colloidal solution may favour such aggregation.16 Upon cooling back down to 25 °C, PNIPAM rehydrates and swells, recovering its original conformation and restoring the original SPR absorption spectra (Fig. 5a). This rules out the possibility of AuNP aggregation upon heating, as the strong interactions between the outer PNIPAM layer and water molecules stabilise the nanoparticles, thereby preventing irreversible aggregation.51,52 These spectral changes confirm the reversible thermoresponsive behaviour of the PNIPAM-AuNPs and strongly indicate the presence of a functional PNIPAM layer around the AuNPs. In contrast, for the NIPAM-AuNPs at 40 °C, no significant band broadening or deformation in the extinction spectrum is observed (Fig. 5b). The LSPR band of the NIPAM-AuNPs exhibits a minor red shift upon heating, but some light scattering is present. This suggests the formation of more compact, dense structures around the AuNPs, inducing changes in the local dielectric environment and slightly larger particles, as measured by DLS, but without polymer chain collapsing. The absence of pronounced thermoresponsive behaviour or spectra deformation supports the hypothesis that only monomers or short-chain NIPAM oligomers are present on the AuNPs surface. Upon cooling back down to 25 °C, the original spectrum is recovered, with a slight red shift observed, which remains constant after repeated heating and cooling cycles, suggesting a change in the local dielectric environment induced by heating.
Fig. S5 presents the UV-visible absorption spectra obtained before and after one hour of light-irradiation of the colloidal solutions of PNIPAM-AuNPs and NIPAM-AuNPs under the solar lamp and LED reactor. Prior to illumination, both colloidal solutions appear clear, and their absorption spectra present the characteristic LSPR band of AuNPs. After one hour of illumination under the solar lamp, the NIPAM-AuNP solution remains visually unchanged (Fig. S5b, inset), and a slight red shift is observed in the LSPR absorption band (Fig. S5b). In contrast, after one hour of irradiation, the PNIPAM-AuNP colloidal solution becomes visibly cloudy (Fig. S5a, inset), and the corresponding UV-vis absorption spectrum shows a very broad band with a non-well-defined maximum around 550 nm (Fig. S5). This spectrum resembles that registered at 40 °C (Fig. 5a) and could indicate an increase in temperature. Indeed, after 1 h of illumination under the solar lamp, the measured temperature is approximately 46 °C. This temperature is significantly higher than that measured after one hour of solar lamp illumination for non-irradiated and irradiated PNIPAM solutions (around 32.6 °C and 32 °C, respectively, close to the LCST). Indeed, even in the absence of AuNPs, a thermosensitive response is observed, as evidenced by changes in the absorption spectra (Fig. S6). This result indicates that the illumination by the solar lamp induces a rise in the temperature of the entire solution, which is increased by the presence of the AuNPs.54 Therefore, we deduce that the observed thermosensitive behaviour in the PNIPAM-AuNPs sample (Fig. S5a) is likely due to a combined effect of both an overall heating due to the lamp and a plasmonic heating from the AuNPs.
To further investigate the role of plasmonic heating, experiments were conducted using a 525 nm LED reactor. After one hour of illumination under the LED reactor (Fig. S5), the PNIPAM-AuNP and NIPAM-AuNP colloidal solutions remain visually unchanged, and no broadening or shift in the LSPR absorption was observed (Fig. S5c and d). The temperature changes were around 5 °C, slightly higher than the measured change for the PNIPAM solutions (∼4 °C). Since this temperature is below the LCST of PNIPAM, neither turbidity in the PNIPAM-AuNP solution nor spectral changes were observed. These results show that the general heating is mainly due to the absorption of the infrared photons emitted by the solar lamp since it is not observed with the LED reactor emitting only at 525 nm. However, they also suggest that, once the LCST is reached, the collapsed state of the polymer around the nanoparticles favours the diffusion of the heat due to the plasmonic excitation.55 Indeed, it was reported that for a gold NP surface coated by a polymer layer, the thermal resistance decreases as the polymer density increases, and that the heat transfer is favoured for a polymer with good terminal interactions with water to lower the contact resistance.56 Here, the final temperature (around 46 °C) obtained under solar lamp illumination for the PNIPAM-AuNP solutions is higher than that reached by the PNIPAM solutions (around 32 °C, the LCST). So, the observed temperature rise might be attributed to plasmonic heating from the gold nanoparticles upon light absorption, which contributes to the overall warming of the colloidal solution.54,57
The radiolytic reduction of AuIIICl4− ions and the formation of AuNPs in aqueous solutions have already been studied in detail.43,60 The AuIII ions in the solution are reduced to Au atoms by the strong reducing agents produced during radiolysis, the hydrogen atom (˙H), and solvated electrons (e−aq) with redox potentials of E°(H+/H˙) = –2.3 VSHE and E°(H2O/e−aq) = −2.87 VSHE respectively.41,42 However, strong oxidising species, ˙OH radicals with a redox potential of E°(˙OH/H2O) = +2.76 VSHE,41 are also generated and may oxidise Au atoms and ions to higher oxidation states. To prevent this, secondary or tertiary alcohols (propan-2-ol or tert-butanol in this study) are used to scavenge the oxidising species. The resulting propan-2-ol radicals may further participate in metallic ion reduction (E°(CH3)2CO/(CH3)2C˙OH) = −1.8 VSHE (eqn (1)–(5)).41,42
| AuIIICl4− + e−aq → AuIICl42− | (1) |
| 2AuIICl42− → AuIIICl4− + AuICl2− + 2Cl− | (2) |
| (CH3)2CHOH + ˙OH (H˙) → (CH3)2C˙OH + H2O (H2) | (3) |
| AuICl2− + e−aq → Au0Cl22− | (4) |
| AuICl2− + (CH3)2C˙OH → Au0Cl22− + (CH3)2CO + H+ | (5) |
In our study, at an irradiation dose of 0.7 kGy, all the AuIIICl4− ions present in the aqueous solution ([AuIIICl4−] = 1.48 × 10−4 M) are reduced, which corresponds to a reduction yield Gred of 0.63 × 10−6 mol J−1. This was estimated using the formula:
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| Fig. 6 Schematic illustration of the reactive species generated by the radiolysis of an aqueous solution and reduction process (created in https://BioRender.com). | ||
However, in the presence of PNIPAM or NIPAM, the generated radiolytic species may also react with PNIPAM and NIPAM molecules, and so, radicals and radical anions are generated from the PNIPAM or NIPAM through additions to the unsaturated or double bonds in these compounds (eqn (6) and (7)).58,61,62
| NIPAM + e−aq → (NIPAM)˙− | (6) |
| NIPAM + H˙ → (H–NIPAM)˙ | (7) |
During the reduction process involving NIPAM, a competition may arise between metallic ions and NIPAM for reducing species, particularly solvated electrons, due to their high reactivity with NIPAM. Using literature rate constants (k6 = 1.0 × 1010 M−1 s−1 for NIPAM and k1 = 5.7× 109 M−1 s−1 for AuIII),58,63 and the concentrations used in this study, the estimated rates of electron scavenging are 7.84 × 107 s−1 for NIPAM and 8.44 × 105 s−1 AuIII ions, indicating that NIPAM reacts preferentially with solvated electrons. Nevertheless, the high redox potential reported for AuIII and AuII (E°(AuIII/AuII) ≈ +0.7 VNHE, E°(AuII/AuI) ≈ +0.9 VNHE)60 compared to the estimated redox potential reported for NIPAM (E°(NIPAM/NIPAM˙−) ≈ –0.45 V),58 could lead to the metallic ions being reduced by the radical anion of NIPAM on the formed metal clusters. Subsequently, the Au0 formed can reduce NIPAM (E°(AuI/Au0) ≈ −1.5 VNHE).64 However, it should be noted that the redox potentials of AuIII, AuII, and AuI depend on their complexation state and increase with the nucleation n of the clusters (Aun),65 so several electron transfers may occur between gold and NIPAM, affecting the multistep reduction processes and the formation of AuNPs.
Depending on the concentration, the generated PNIPAM or NIPAM radicals can propagate to form either crosslinked hydrogels or linear polymers. In the case of PNIPAM, crosslinking is evidenced by the significant size increase observed both below and above the LCST via DLS in irradiated PNIPAM solution compared to non-irradiated PNIPAM solution (Fig. 4).66 The crosslinking also induces a slight decrease in the LCST. In the case of NIPAM, the large hydrodynamic diameter determined by DLS measurements, compared to the AuNP size obtained by TEM, suggests the presence of oligomers, which effectively stabilise the AuNPs by adsorption onto their surface through complexation between nitrogen atoms and the metal ions (Fig. 6). It is assumed that no polymer formation occurred during the reduction process, as the characteristic thermosensitive behaviour associated with PNIPAM is absent upon heating the NIPAM-AuNP colloidal solution (Fig. S5b, inset). However, further characterisation using 1H NMR spectroscopy has revealed the absence of peaks corresponding to the NIPAM monomer (Fig. S7 and S8), but the presence of broad peaks around 1.6 and 2.2 ppm in the NIPAM-AuNPs spectrum (Fig. S7). These peaks resemble those recorded for PNIPAM with a slight shift, indicating that polymerisation occurred during gamma irradiation. Due to the lack of thermosensitive behaviour, it is likely that only short-chain polymers or oligomers are formed. This may result from the competition reactions between the metallic ions and NIPAM with the radiolytic species, as well as multiple electron-transfer events between them, as previously discussed. Nevertheless, these oligomers are sufficient to efficiently stabilise the formed AuNPs, since the NIPAM-AuNP solutions are stable over several months, as are the PNIPAM-AuNP solutions.
Fig. 7a and b show the temporal evolution of the UV-visible absorption spectra of a solution containing K3Fe(CN)6, NIPAM-AuNPs, and TEOA in the dark and under LED illumination. In both cases, a gradual decrease in the absorption band at 420 nm, characteristic of [Fe(CN)6]3−, is observed at 10-minute intervals, with complete reduction achieved after 2 hours. The LSPR band of the AuNPs remains quite unchanged throughout the process, confirming their stability. TEOA being in excess, the reduction reactions are shown to follow first-order kinetics with a similar rate constant (Fig. S9), indicating no effect of light on the reaction rate, contrary to previous reports.57,67 To rule out direct reduction of [Fe(CN)6]3− by TEOA, a control experiment containing [Fe(CN)6]3− and TEOA in the absence of AuNPs under LED illumination was performed (Fig. 7c). Only a very slow decrease in the [Fe(CN)6]3− band is observed. In the absence of TEOA (Fig. 7d), both the [Fe(CN)6]3− band at 420 nm and the AuNPs LSPR band decrease upon illumination, whereas no significant decrease is observed in the dark (Fig. S10). This indicates that the reduction of [Fe(CN)6]3− is concomitant with AuNP degradation under light illumination. Similar results were also observed for PNIPAM-AuNPs (Fig. S11).
The plasmonic photocatalytic activity of PNIPAM and NIPAM-stabilised AuNPs for the reduction of 4-NTP in the absence of NaBH4 and under solar lamp illumination is represented in Fig. 9. Time 0 corresponds to the start of the illumination after 40 min of N2 bubbling in the dark, allowing adsorption of 4-NTP onto the surface of the AuNPs. The effective adsorption of 4-NTP onto the AuNP surface is indicated by the difference between the UV-visible spectrum recorded for the mixture and the one calculated by the sum of the spectra of the two compounds (Fig. S14). When the mixed solution is placed under visible light irradiation, the absorption peak of 4-NTP at 409 nm gradually decreases. This decrease is accompanied by the appearance of a weak absorption band at around 270 nm and, in the case of NIPAM-AuNPs, an isosbestic point at around 344 nm, which may correspond to the formation of 4-ATP. After 7 hours of light irradiation, roughly two-thirds of the 4-NTP have disappeared in the presence of NIPAM-AuNPs, and one-half with PNIPAM-AuNPs. A complete degradation of 4-NTP was observed after keeping the sample solution for one day without covering it with aluminium foil (Fig. 9). Throughout the reaction process, the LSPR bands at 530 nm and 534 nm for the NIPAM-AuNPs and PNIPAM-AuNPs, respectively, remain stable (Fig. 9a and b). However, it has to be noted that, while the solution of NIPAM-AuNPs with 4-NTP remains clear under visible light illumination, the solution of PNIPAM-AuNPs becomes turbid due to overall heating of the solution and thermal response of the polymer, as mentioned previously. So, the spectra shown in Fig. 9a were recorded a few minutes after illumination, after the solution had cooled down and become clear again. That may explain irregularities and the absence of an isosbestic point in the case of PNIPAM-AuNPs. Fig. 9c gives the temporal evolution of the absorbance at 409 nm due to 4-NTP (after subtraction of the NPs’ absorbance). The absorbance decays appear quasi-linear with time, suggesting that the reaction follows pseudo-zero-order kinetics with similar rate constants. The degradation of 4-NTP by NIPAM-AuNPs in the dark was also attempted with similar concentrations (Fig. S15). No decrease in the absorbance is observed. To test their recyclability, the PNIPAM-AuNPs were reused in a second experiment to photodegrade 4-NTP under solar lamp illumination (Fig. S16). As observed, the nanoparticles show efficient catalytic activity and remain stable throughout the photoreduction process, confirming their reusability.
The photocatalytic activity of the NPs was also tested for the reduction of 4-NP under similar conditions to those used for 4-NTP; however, no degradation was observed within 6 hours of illumination.
In order to avoid the temperature increase due to the solar lamp illumination, the plasmonic activity of the synthesised AuNPs in the reduction of 4-NTP was investigated under LED illumination (Fig. 9). Both PNIPAM-AuNP and NIPAM-AuNP solutions with 4-NTP remained clear under LED illumination, indicating only a minor temperature increase (below the LCST of PNIPAM). However, the gradual decrease in the 4-NTP absorption peak (Fig. 9d and e) indicates the degradation of 4-NTP due to the plasmonic effects of the AuNPs activated by visible light. The temporal evolution of the absorbance at 409 nm due to 4-NTP is shown in Fig. 9f. The absorbance decay appears quasi-linear over time for NIPAM-AuNPs, exhibiting kinetics similar as those observed under solar lamp illumination.
Considering the reduction of 4-NP, an induction time is observed before the reaction occurs, following pseudo-first-order kinetics, as already reported in other studies.47,69,71 This induction time, of the order of a few minutes, was attributed to a slow surface restructuring related to the presence of 4-NP. Several mechanisms have also been proposed, and the role of NaBH4 in AuNP-catalysed 4-NP reduction was previously studied.72 Our results are in favour of the Langmuir–Hinshelwood model as described by Wunder et al.:71 (i) BH4− ions react with the AuNPs surface and transfer a hydrogen to form a metal hydride, (ii) concomitantly, 4-NP molecules adsorb onto the surface, then, (iii) the reduction reaction takes place on the surface between adsorbed species to form 4-AP. Indeed, the reaction has been observed for 4-NP but not for 4-NTP, which can be attributed to the difference in the orientation of the pollutant molecules on the surface of the NPs, as evidenced by Cui et al.11,14 They reported the complete reduction of 4-NP by NaBH4 in the presence of gold nanostars (AuNS), but the absence of reaction for 4-NTP. They used surface-enhanced Raman scattering to monitor the interaction of the pollutants with the AuNS surface and found that 4-NP was absorbed via the nitro group, while 4-NTP was bound via the thiol group.14 So, the direct contact of the nitro group with the AuNP surface is necessary for the catalysis. Regarding the apparent first-order rate constants, comparisons with other studies are difficult because there are several differences. For instance, Du et al.27 observed a significantly faster catalytic reduction of 4-NP (within approximately 4 minutes) using chemically synthesised PNIPAM-AuNPs. The difference in the catalytic rate compared to the PNIPAM-AuNPs reported in this study can be attributed to differences in (i) nanoparticle size: while PNIPAM-AuNPs synthesised by Du et al.27 were ∼2.3 nm in diameter, those in this study are ∼5.4 nm; (ii) surface accessibility and available sites: in the chemically synthesised PNIPAM-AuNPs, there is no radical-induced crosslinking of PNIPAM during synthesis.
The plasmonic photocatalytic properties of the synthesised AuNPs have also been tested in the absence of any reducing species or sacrificial electron donor for the same reduction reactions. The plasmonic reduction of [Fe(CN)6]3− without TEOA occurs at the expense of the AuNPs. This indicates that hot electrons generated upon plasmon excitation are able to reduce [Fe(CN)6]3−, while the accompanying holes oxidise the nanoparticles. Similar results have already been reported by Garai et al.,67 who explained the dissolution by the complexation of the oxidised gold atoms by cyanide ions (CN−) to form stable Au(CN)2− in solution.
For the photoreduction of nitroarenes, the reaction is observed for 4-NTP but not for 4-NP, indicating that the way the molecules are adsorbed on the surface plays a role, as discussed for the catalysis. However, in this case, adsorption by the thiol group appears favourable. In the absence of BH4−, there is no hydrogen present on the surface to reduce the nitro group into an amino group, which may explain why 4-NP does not undergo photoreduction under these conditions. In the case of 4-NTP, the reduction reaction is known to proceed via two main mechanistic pathways (Fig. 10). The first is the direct reduction of 4-NTP to 4-ATP, accompanied by the formation of several intermediates, including dihydroxylaminothiophenol (DHATP), nitrosothiophenol (NSTP), and hydroxylaminothiophenol (HATP).73,74 The second is the indirect pathway, which involves the condensation of intermediates such as DHATP and HATP to form dimercaptoazobenzene (DMAB), which is subsequently reduced to 4-ATP.73,75 Nuclear magnetic resonance (NMR) spectroscopy and mass spectrometry (MS) were employed to analyse the photocatalytic products of 4-NTP; several products were detected, but no clear signature was obtained. It is also worth noting that while the plasmonic excitation of the AuNPs allows the degradation of 4-NTP, the AuNPs remain stable and are not oxidised as in the case of [Fe(CN)6]3−. Such results suggest that the holes produced by plasmon excitation are scavenged.
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| Fig. 10 Schematic representation of possible reaction pathways for the photocatalytic reduction of 4-nitrothiophenol to 4-aminothiophenol.73,74 | ||
The catalytic and photocatalytic activities of the synthesised PNIPAM-AuNPs and NIPAM-AuNPs were tested with two model reactions: the reduction of hexacyanoferrate, [Fe(CN)6]3−, and the reduction of the nitroarenes, para-nitrophenol (4-NP) and para-nitrothiophenol (4-NTP). The systems showed efficient catalytic activity towards the reduction of [Fe(CN)6]3− and 4-NP, in the presence of TEOA or NaBH4, respectively, used as electron donors or reducing agents. The systems also exhibited efficient photocatalytic properties by excitation of the plasmon resonance band of the AuNPs in the absence of an electron donor or reducing agent. However, in the case of [Fe(CN)6]3−, the reduction occurred at the expense of the AuNPs, which were oxidised and dissolved. In the case of 4-NTP, such degradation was not observed, and the AuNP systems remained stable throughout the reaction. This result indicated that while the generated hot electrons reduced 4-NTP, the concomitantly produced holes were scavenged.
Our results also showed that, while the PNIPAM-AuNPs and NIPAM-AuNPs could catalyse the reduction of 4-NP by NaBH4, no reaction took place with 4-NTP, and conversely, under plasmon excitation without a reducing agent, they could photodegrade 4-NTP but not 4-NP. These differences in reactivity might be explained by the different orientations of the adsorbed molecules on the metallic surface, through the nitro group for 4-NP and via the thiol group for 4-NTP.
Last but not least, the stabilisation of the AuNPs by the thermosensitive polymer appears highly efficient, as evidenced by the stability of the catalyst during the photocatalytic process and its reusability. Additionally, the thermosensitive polymer can offer more interesting catalytic properties to the AuNPs through its hydrophobic and hydrophilic properties, such as controlling the selectivity of the catalyst and hindering catalyst poisoning.27
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