Fig. 1: Reconfigurable Gires-Tournois monopixel array. a Schematic of the reconfigurable Gires-Tournois (r-GT) monopixel array and the reflective light showing full-colour chromaticity. b The relationship of pixels per degree (PPD) corresponds to the distance from the eyes (d), which determines the minimum pixel pitches (P). For example, pixel density ranges required for devices from electronic billboards to VR\/AR glasses vary from 87 pixels per inch (PPI) to 10,000 PPI, respectively. c Comparison of pixel thickness and its PPI of the electrically addressable pixel array and\/or display. The right-side axis represents the distance from the eyes, and the red solid lines indicate the corresponding PPD, ranging from 100 to 102 at each PPI level (See Fig. S1<\/a> (Supplementary Information) for details). d Schematic of the layered structure of r-GT cell consisting of a trilayer resonator (Au\/Pr-Ge\/PANI). The optical state of PANI determines the resonance mode of r-GT. e The molecular configuration of PANI and its electrically switchable optical state, alternating between insulating (PANI0), intermediate state (PANI1+), and metallic states (PANI2+). f Simulated reflectance of various resonator configurations (Asymmetric F.-P. cavity, Trilayer GT resonator, and Tailored trilayer GT resonator). The scattered dots indicate the complex refractive indices (n) and extinction coefficient (k) of PANI under different redox states. g Reflectivity of r-GT in various configurations: \u2170) asymmetric F.-P. resonator, where PANI is applied directly to an Au substrate; \u2171) trilayer GT resonator, which includes a dense amorphous Ge layer between Au and PANI; \u2172) tailored trilayer GT resonator, consisting of a porous Ge layer between Au and PANI. Reflectivity changes as PANI cycles through different redox states from PANI0 to PANI2+ under resonant wavelength. h Absorptivity of r-GT corresponding to the change of redox state of PANI. The red curves represent the absorptivity spectra in the fully reduced state of PANI, while the blue curves correspond to the fully oxidized state. i Photo images of the colour variation of r-GT. Scale bar is 1.5\u2009cm (more experimental results in movie S1<\/a> (Supplementary Information))<\/p>\n The outstanding abilities, including downscaling ability and vibrant colouration of the r-GT resonator, originate from three major points: (i) the ultrathin scale of the r-GT, (ii) the strong coupling between the conductive polymer and the GT resonator, and (iii) the sensitive shift in the resonance wavelength. The r-GT resonator developed in this study consists of a trilayer ITO\/PANI\/Pr-Ge\/Au architecture, where the engineered Pr-Ge lossy layer enables near-ideal impedance matching and supports a sharp resonance that responds sensitively to the redox-induced optical changes of PANI (Supplementary Information Fig. S2<\/a>). The GT resonator, which has been recently studied as a flat metasurface for generating strong resonance by controlling the speed of light, is utilized as a core photonic structure to integrate active material (PANI) strongly, resulting in a sensitive adjusting ability of resonances from single to dual mode (Fig. 1d<\/a>)34<\/a>,35<\/a>. During voltage sweeps in cyclic voltammetry, PANI undergoes two reduction\/oxidation steps, displaying three redox states: PANI0 at \u22120.2\u2009V, PANI1+ at 0.4\u2009V, and PANI2+ at 0.8\u2009V, including continuous complex refractive index variation (Fig. 1e<\/a>). PANI\u2019s significant refractive index change (\u2206n\u2009~\u20090.3, \u2206k\u2009~\u20090.6) during these transitions addresses the limitations of standalone conductive polymers, which do not provide sufficient light-matter interaction for effective full-colour switching across a broad hue range (Supplementary Information Fig. S3<\/a>). Thus, the GT resonator, integrated with PANI, is engineered to enable sensitive resonance shifts for enhanced colour purity in the additive colour regime, and to produce a precise and strong resonance with requiring only a 90\u2009nm thickness of PANI, achieving extremely low power consumption (<90\u2009\u03bcW\u2009cm\u22122, Supplementary Information Figs. S4<\/a> and S5<\/a>)36<\/a>. For example, as illustrated in Fig. 1f<\/a>, various GT resonator configurations are compared to a conventional Fabry\u2013Perot cavity. The conventional GT resonator exhibits a single resonance in the visible spectrum with limited sensitivity to absorptivity modulation, as shown in the bottom contour plot and Fig. 1g<\/a>. In contrast, the trilayered GT resonator, which incorporates a lossy interlayer to better match the optical impedance between interfaces, demonstrates enhanced resonance intensity and supports dual resonances within the visible range. However, its resonance peaks are relatively broad, limiting its ability to achieve high colour purity. On the other hand, the tailored trilayered GT resonator incorporating a porous Ge layer exhibits nearly perfect impedance matching, leading to near-unity absorption. This configuration enables strong resonance tuning in response to the redox activity of PANI, resulting in significantly higher colour purity due to the formation of narrow and well-defined spectral peaks (Supplementary Information Figs. S6<\/a>\u20138<\/a>). Furthermore, Numerical simulations confirmed that the device maintains consistent colour performance over a broad range of incident angles, corresponding to an effective field of view (FOV) of ~60\u00b0 (\u221230\u00b0 to 30\u00b0), demonstrating its potential applicability to commercial reflective displays, such as Magic Leap, which features an FOV of ~50\u00b0 (Supplementary Information Fig. S9<\/a>)37<\/a>.<\/p>\n By adjusting the redox states of PANI, one can finely tune the resonance conditions in the r-GT, achieving extensive hue modulation (Fig. 1h<\/a> and Supplementary Information Fig. S10<\/a>). Figure 1i<\/a> highlights its colour dynamics corresponding to the voltage range even below 1\u2009V (Movie S1<\/a>, Supplementary Information Figs. S11<\/a> and S12<\/a>). Figures S13<\/a> and S14<\/a> (Supplementary Information) show a tendency of a gradually adjusted resonance mode corresponding to the modulation in PANI\u2019s state. Considering that a newspaper typically exhibits a reflectance contrast of ~40%, our device demonstrates practical performance with ~40% reflectance in the OFF state and ~80% in the ON state38<\/a>,39<\/a>. The detailed design process will be discussed in the next section.<\/p>\n Building on these capabilities, the r-GT resonator stands out by achieving significant chromatic variation of 220.6\u00b0 at sub-1-volt levels. It exceeds the complementary colour range, which is essential for enhancing the perception of depth and realism in digital art and displays40<\/a>. This performance is notable compared to previous technologies, including active photonics integrated with redox-based tunable materials (e.g., conductive polymer), phase change\/transition materials, reconfigurable photonics via dimension tuning (e.g., electrically responsive photonic crystals), and electrostatic inkjet control (e.g., electrophoretic displays), highlighting its advanced capability in precise colour modulation across a wide spectrum with dimensional downscaling into micrometer-scale (Supplementary Information Tables S1<\/a> and S2<\/a>) Furthermore, the thin-film r-GT resonator exhibits a wide colour modulation efficiency per unit power compared to nanostructured photonic structures such as metasurfaces and nanocaves (Supplementary Information Fig. S15<\/a>, Tables S3<\/a> and S4<\/a>)8<\/a>,9<\/a>,41<\/a>,42<\/a>.<\/p>\n Full-colour expression of r-GT<\/p>\n This section delves into the vibrant colour modulation abilities and the universality facilitated by diverse structural combinations within the r-GT. The pronounced chromaticity changes in the r-GT are attributable to sensitive adjustments in resonance conditions, driven by each layer\u2019s precise engineering based on transmission line theory, allowing exact monitoring of the interactions between light and the layered structures. Notably, the introduction of a porous (Pr)-Ge structure in the lossy material medium enhances the responsiveness of the modulation environment to changes in PANI\u2019s complex refractive index (Supplementary Information Note 1<\/a>; Figs. S16<\/a> and S17<\/a>). As a result, the r-GT\u2019s reflectance shows a marked negative group delay, effectively preventing chromaticity cancellation in the absorptive state (Supplementary Information Note 2<\/a>; Fig. S18<\/a>). This mechanism contributes to strong and consistent colour modulation. Figure 2a, b<\/a> display chromaticity covering as thickness of PANI and redox state transitions through from PANI0 to PANI2+, illustrating 48.1% of sRGB coverage during these transitions (Supplementary Information Figs. S19<\/a> and S20<\/a>). The colour palette visually represents the range of colour modulation achievable within a single structure, highlighting the importance of active material thickness and selecting an optimal thickness (Fig. 2c<\/a>). Moreover, various material combinations have been utilized to enhance colour expression, achieving performance that spans the sRGB colour space. Each colour dot in the figure represents a configuration involving different combinations of lossy materials within the r-GT, highlighted by the white triangular line that marks the sRGB range (Supplementary Information Fig. S21<\/a>). Figure 2d, e<\/a> quantify the sRGB colour gamut coverage of the r-GT across PANI\u2019s various states, noting that the full sweep of redox states covers 69.9% of sRGB, enabling vibrant colour expression. Finally, Fig. 2f<\/a> visually presents the colour palette for each configuration, demonstrating the substantial variation and impact of these material integrations, including the primary RGB colours.<\/p>\n Fig. 2: Full-colour operation of r-GT. a CIE plot of the r-GT with lossy layer (Pr-Ge). The white triangle represents the standard RGB (sRGB) colour space, and the dashed line shows the voltage-dependent shift of the colour coordinates from \u22120.2\u2009V to 0.8\u2009V. b sRGB colour gamut coverage of r-GT across different states of PANI. c Colour palette associated with each configuration. d CIE chromaticity plots for various configurations of the r-GT with different material combinations. e, f sRGB colour gamut coverage (e) and associated colour palettes (f) of r-GT devices tailored to represent primary red, green, and blue (R, G, B) colour via PANI redox modulation<\/p>\n Self-passivation layer with enhanced stability and fast response time<\/p>\n Protons are essential for doping PANI, enabling fast diffusion and enhanced modulation speed; however, they also create an acidic environment, which may result in structural corrosion43<\/a>. To protect against the corrosion issue, Fig. 3a<\/a> illustrates the irreversible, intentionally applied oxidation of the Ge layer during the first cycle of voltage sweeps in cyclic voltammetry. The oxygen ions and electrons involved in oxidation are derived from the electrolyte and the conductive substrate, resulting in the formation of the GeO2 layer through processes (i) and (ii)44<\/a>. As shown in Fig. 3b<\/a>, the electrochemical reactions of the r-GT monopixel are examined during 100 cycles. The cyclic voltammetry curves show a high current peak intensity at a specific voltage during the first cycle, followed by stable redox reactions in the subsequent cycles (Supplementary Information Fig. S22<\/a>). This phenomenon suggests that partial oxidation of Ge occurs, leading to the formation of the self-passivation layer (SPL) to protect its porous structure from acidic electrolyte45<\/a>. During the first cycle of the cyclic voltammetry reaction, the peak current density of the r-GT resonator at 0.45\u2009V points to the oxidation of Ge to GeO2, in response to oxygen sources being absorbed during the deposition process and\/or hydroxyl groups diffusing from the electrolyte46<\/a>,47<\/a>. To confirm the necessity of the intentionally formed SPL through Ge oxidation, the device is fabricated using the conventional material (SiO2) for comparison. Under acidic conditions, the Ge medium is fully oxidized, resulting in degraded electrochromic properties. On the other hand, SPL-based r-GT provides great protection ability, showing great reversibly switchable ability, enabled by GeO2 passivation with inherently lower interface defect density than SiO2 passivation48<\/a>,49<\/a>,50<\/a>. (Fig. 3c<\/a>). As proof of our suggestion, energy dispersive spectroscopy (EDS) and X-ray photoelectron spectroscopy (XPS) were conducted, revealing a corresponding increase in the GeO2 proportion in the XPS O 1\u2009s signal (Supplementary Information Fig. S23<\/a>). In addition, the Ge 3\u2009d photoelectron spectrum before (blue line) and after redox reaction (red line) show a change in spectral intensity with a shift from the initial state to a higher binding energy corresponding to the GeO2 peak profile (Fig. 3d<\/a>). As shown in Fig. 3e<\/a>, comparison of the CV curves for Au\/Pr-Ge\/ITO, Pr-Ge\/PANI\/ITO, and the r-GT resonator reveals redox peaks in the PANI-containing structure relative to structure without PANI. In addition, the structure containing Au effectively suppresses excessive oxidation of Pr-Ge, enabling the formation of SPL. These results closely match the EDS mapping profile in terms of oxygen and nitrogen atomic proportion. Figure S24<\/a> (Supplementary Information) also presents EDS results showing an increase in nitrogen content, which occurred simultaneously with the doping\/de-doping process. Figure 3f<\/a> shows that the reflectance spectrum repeatedly activates and reverts to its initial state and different voltages (\u22120.2\u2009V and 0.6\u2009V, interval is 10\u2009s) during 700 cycles (Supplementary Information Figs. S25<\/a> and S26<\/a>). Figure 3g<\/a> shows that proton has the smallest cation radius and largest diffusion coefficient in comparison with other cations, resulting in a fast response time of doped in just 34\u2009ms (oxidation) and effectively de-doped to the reduced state within 171\u2009ms (reduction) (Fig. 3h<\/a>; Supplementary Information Figs. S27<\/a> and S28<\/a>). The r-GT resonator is measured into the other electrolyte containing either sodium ion (Na+) or potassium ion (K+), which have larger ionic radii and lower diffusion coefficients compared to protons. Figure 3i<\/a> displays a radar chart showing that both Na+ and K\u207a-based electrolytes exhibit overall lower performance in terms of modulated hue range (H), response time (T), and reversibility (R). Building on the results, it suggests that proton-based electrochemical reactions guarantee sufficient redox responses with fast reaction speeds. Although they may be limited by corrosive properties, we have overcome this issue using SPL, thereby expanding the range of applicability for PANI-based photonics (Supplementary Information Table S5<\/a>; Figs. S29<\/a> and S30<\/a>).<\/p>\n Fig. 3: Characterization of the self-passivation layer (SPL) of r-GT. a Illustration of the formation of SPL. The porous Ge layer undergoes oxidation through electrons and oxygen. b Cyclic voltammetry (CV) curve of the r-GT at first cycle (red line) and after 30 cycles (blue line) with a reference electrode (RE, Ag\/AgCl). A strong oxidation peak occurs during the initial oxidation stage, followed by a stable electrochemical response in subsequent cycles. c Schematic of the permeability of photons through the SPL and SiO2 layer, along with corresponding photo images of the reflective colours. d XPS spectra of O 1\u2009s and Ge 3\u2009d at the interface between PANI and porous Ge layer. The blue line represents the state of the r-GT before the redox reaction, while the red line shows the state after the reaction. e CV curve of Au\/Pr-Ge\/ITO (blue line), Pr-Ge\/PANI\/ITO (green line), and r-GT resonator (red line) at a scan rate of 0.05\u2009V\u2009s\u22121. Energy dispersive spectroscopy (EDS) analysis of a cross-sectional r-GT. The EDS mapping reveals that the atomic percentage of oxygen (blue) is increased in the SPL region after the redox reaction. f Reflectance spectrum with potential cycled from \u22120.2\u2009V to 0.6\u2009V (interval: 10\u2009s) over 700 cycles. g Comparison of various cations with photon based on cation radius and diffusion coefficient. h The electrically responsive reflectance exhibits a switching speed with a rise time of 34\u2009ms and a fall time of 171\u2009ms, respectively. i Comparison of different cation-based electrolytes in terms of hue range (H), response time (T), and reversibility (R)<\/p>\n Flexibility in scaling the dimensions of the r-GT resonator<\/p>\n The optical\/chemical robustness of r-GT offers the flexibility in scaling the pixel dimension from centimeter-scale to micrometer-scale. Particularly, in this section, we demonstrate the diverse scale of the reconfigurable pixel array with a colour switching function. Figure 4a<\/a> shows the Bayer-pattern with 16-unit dots, incorporating the painting Girl with a Pearl Earring (Johannes Vermeer), achieving a compact panel size smaller than a 1-dime coin. By varying the density of unit dots, the spatial fill factor can be adjusted to represent 16 graded intensity levels (4-bit) in the corresponding pixel array (Fig. 4b<\/a>; Supplementary Information Fig. S31a\u2013d<\/a>). The 5\u2009\u00b5m square pattern is defined as a unit pixel, and the array patterns display a clear high-density (HD) image (Fig. 4c<\/a>; Supplementary Information Fig. S32<\/a>). The chromaticity of the HD patterned r-GT resonator can be adjusted from yellow to blue under sub-1-volt conditions (Supplementary Information Fig. S31e<\/a>). Quantitatively, the pixel size can be classified according to target applications by considering the distance between the display and the observer\u2019s eyes. In this regard, we experimentally confirmed diverse sizes of pixels with the colour switching functionality. Figure 4<\/a>d, e illustrates the pixel size distribution ranging from the few micrometer-scale required for VR\/AR displays to the centimeter-scale needed for electronic billboards51<\/a>,52<\/a>. The active area of r-GT is successfully patterned with different pixel sizes: i) P\u2009=\u2009160\u2009\u00b5m; ii) P\u2009=\u2009370\u2009\u00b5m; iii) P\u2009=\u2009630\u2009\u00b5m; iv) P\u2009=\u20091300\u2009\u00b5m; and v) centimeter-scale image printing. Additionally, the experimental validation of scaling down has been confirmed up to a pixel pitch of 1.5\u2009\u00b5m, achieving 16,900 PPI (Supplementary Information Figs. S33<\/a> and S34<\/a>). Diverse sizes of each pixel are compared with previously reported reflective-type displays with pixel operation based on reconfigurable photonics using various types of active materials, such as electrochemical doping material (PANI53<\/a>,54<\/a>,55<\/a>, PEODT:PSS56<\/a>, WO357<\/a>,58<\/a>), phase-change materials (GST8<\/a>,9<\/a>,59<\/a>, VO260<\/a>), liquid crystal (LC)61<\/a>,62<\/a>, dielectric (SiO2) nanoparticles-based photonic crystal63<\/a>,64<\/a>, and metal electrodeposition65<\/a>,66<\/a> (Fig. 4f<\/a>; Supplementary Information Fig. S35<\/a>; Table S6<\/a>). As described, depending on the type of active materials, the feasible dimensions can be influenced. For example, when adjusting the period of a photonic crystal based on dielectric nanoparticles (i.e., categorized as a dimension change), there is a required vertical dimension, which may limit the adjustments in the lateral dimension. On the other hand, examples based on PCMs, which can alter colour by applying localized heat, have experimentally demonstrated very small pixelization down to ~300\u2009nm. However, in this case, the heating is applied via an atomic force microscope tip, and there is a lack of circuit-based pixel-by-pixel addressing capability. Also, from the viewpoint of colour adjusting, despite vibrant colour changes, there are no cases that achieve a sufficient complementary range (\u0394Hue > 180\u00b0). This may be due to \u2170) the limitations in the change in optical constants of the active materials themselves, or \u2171) the absence of synergistic coupling with the photonic structure necessary to induce sufficient light-matter interaction. In this context, r-GT successfully demonstrates great flexibility in scaling profits for diverse types of applications and also provides an extensive colour modulation.<\/p>\n Fig. 4: Electrically triggered optical response and programmable memory functions. a Photograph of the high-density (HD) patterned r-GT resonator alongside a 1-dime coin. b Bayer-pattern image of the painting \u201cGirl with a Pearl Earring\u201d with a 16-level scale. c Microscope image of a selected region at a voltage of HD r-GT array. The bluish image shows the r-GT in the PANI2+ state. d Recommended scale diagram of the pixel size corresponding to commercial display devices. e Optical microscopy images of each pixel showing electrically switchable dual states and the electrochromic emergency exit sign. f Comparison of optical modulation range versus span (~220.67\u00b0) of the operated pixel size with various tunable photonics systems. Scale bars, a 1\u2009cm, b 1\u2009mm, c 250\u2009\u03bcm, 15\u2009\u03bcm, and 10\u2009\u03bcm. e \u2170\u2013\u2173 300\u2009\u03bcm and \u2174 5\u2009mm<\/p>\n Addressable characteristics of r-GT monopixel array<\/p>\n To demonstrate the addressable r-GT array, we fabricated a 5 by 5 pixel array, each pixel measuring 9\u2009mm\u00b2. Figure 5a<\/a> presents a schematic and a photographic image of the r-GT array, which includes a working electrode (WE), counter electrode (CE), and reference electrode (RE). The potential applied to the WE is transferred via an anisotropic conductive film (ACF) attached to the addressing line (Ti\/Au). The CE and RE utilize Pt and Ag\/AgCl electrodes, respectively. Figure S36<\/a> (Supplementary Information) details the design and mask patterns of the addressable r-GT monopixel array. Each pixel is controlled by applying pre-programmed potentials that determine the colours, i.e., \u22120.2\u2009V for yellow and 0.6\u2009V for blue. By selectively applying the target voltage, the letter pattern \u2018ACTIVE MONOPIXEL\u2019 is displayed (Fig. 5b<\/a>; Supplementary Information Figs. S37<\/a> and S38<\/a>). Figure 5c<\/a> shows selectively controlled patterns in diverse colours achieved by applying different potentials: 0.2\u2009V for green, 0.4\u2009V for cyan, and 0.8\u2009V for magenta. By applying a series of pre-programmed, selective potentials to pixels with varying potentials and addresses, sequential image patterns are demonstrated. Intriguingly, PANI provides a temporal memory function with a metastable ability that maintains its redox states with open-circuit memory properties for over 4\u2009hours (Supplementary Information Fig. S39<\/a>)16<\/a>. Leveraging this property, we showcased a Memory-in-Pixel capability67<\/a>, resulting in significantly reduced power consumption for maintaining pre-patterned images. Figure 5d<\/a> illustrates four series of sequences by demonstrating the game of Tetris being played. Under these conditions, the power density required for colour switching is measured at only 2.31\u2009mJ, eliminating the need for continuous encoding of colour information (Fig. 5e<\/a>). To compare the power density of the r-GT resonator with that of a commercial display, we assumed the power consumption for an LED, calculated at 13.49\u2009mJ, to align with the minimum and maximum power values provided by the r-GT resonator (Fig. 5f<\/a>; Supplementary Information Fig. S40<\/a>).<\/p>\n Fig. 5: Electrochemical characterization and colouration performance of the r-GT monopixel array. a Schematic illustration of the optical measurement setup for the r-GT resonator and the photo images of a 5\u2009\u00d7\u20095 r-GT resonator array. b Photograph of the individually controlled pixel array with on\/off function, which represents letters of \u201cACTIVE MONOPIXEL\u201d. c Photo images of electrically addressable pixel array with pre-programmed scenarios including moving motion and colouration. d Optical memory properties of the r-GT monopixel for sequential visualization of the famous game of Tetris tasks over time. e, f Comparison of the power consumption of the r-GT resonator (e) and that of commercial light-emitting diode (LED) during sequence processing (f)<\/p>\n As a practical demonstration of reflective display, Fig. S41<\/a> (Supplementary Information) illustrates an energy-efficient display with excellent visibility, even in outdoor environments. The figure demonstrates how the r-GT resonator, utilizing ambient light as a light source, maintains clear visibility across various lighting conditions, with an illumination range of 5\u2013200\u2009W\u2009m\u22122. The captured pictures were converted to grayscale, and intensities were extracted from selected pixels (dashed red line in Supplementary Information Fig. S41d<\/a>) for highlighting the contrast between letters and the background. In the case of the r-GT display, increasing ambient illumination resulted in enhanced contrast, improving visual legibility. In contrast, the LED display exhibited an insufficient contrast ratio to meet the level 5 requirement of the WCAG 2.1 guidelines for optimal visibility in web conditions, as referred to the W3C Web Content Accessibility Guidelines68<\/a>. Consequently, LED displays exhibit lower visibility than this value under high illumination, even at the highest panel brightness with consuming higher power density.<\/p>\n","protected":false},"excerpt":{"rendered":"Concept of reconfigurable Gires-Tournois monopixels Reflective displays offer a compact and efficient design, leveraging external light without an…\n","protected":false},"author":2,"featured_media":512509,"comment_status":"","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[24],"tags":[64,63,53656,31794,55016,162147,30993,17479,59936,59935,51320,292,59937,128],"class_list":{"0":"post-512508","1":"post","2":"type-post","3":"status-publish","4":"format-standard","5":"has-post-thumbnail","7":"category-physics","8":"tag-au","9":"tag-australia","10":"tag-displays","11":"tag-lasers","12":"tag-microwaves","13":"tag-nanocavities","14":"tag-nanophotonics-and-plasmonics","15":"tag-optical-and-electronic-materials","16":"tag-optical-devices","17":"tag-optics","18":"tag-photonics","19":"tag-physics","20":"tag-rf-and-optical-engineering","21":"tag-science"},"_links":{"self":[{"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/posts\/512508","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/comments?post=512508"}],"version-history":[{"count":0,"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/posts\/512508\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/media\/512509"}],"wp:attachment":[{"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/media?parent=512508"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/categories?post=512508"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.newsbeep.com\/au\/wp-json\/wp\/v2\/tags?post=512508"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}![\"figure](\"https:\/\/www.newsbeep.com\/au\/wp-content\/uploads\/2026\/03\/41377_2026_2228_Fig1_HTML.png\")
<\/a><\/p>\n![\"figure](\"https:\/\/www.newsbeep.com\/au\/wp-content\/uploads\/2026\/03\/41377_2026_2228_Fig2_HTML.png\")
<\/a><\/p>\n![\"figure](\"https:\/\/www.newsbeep.com\/au\/wp-content\/uploads\/2026\/03\/41377_2026_2228_Fig3_HTML.png\")
<\/a><\/p>\n![\"figure](\"https:\/\/www.newsbeep.com\/au\/wp-content\/uploads\/2026\/03\/41377_2026_2228_Fig4_HTML.png\")
<\/a><\/p>\n![\"figure](\"https:\/\/www.newsbeep.com\/au\/wp-content\/uploads\/2026\/03\/41377_2026_2228_Fig5_HTML.png\")
<\/a><\/p>\n