To clarify the electronic states relevant to the occurrence of ferromagnetism, we investigated the band structure in the FM phase. Energy distribution curves (EDCs) measured along the \u0393K cut of the hexagonal Brillouin zone (inset) in Fig.\u00a01e<\/a> signify highly dispersive valence bands located at the binding energy (EB) of 1\u20133\u2009eV, whereas the intensity within the EB range of 0\u20131\u2009eV is suppressed due to the band-gap opening. A careful look in close vicinity of EF around the K point reveals the existence of a Fermi-edge cut-off indicative of the metallic nature. This is due to the appearance of an electron pocket as seen in the magnified EDCs and corresponding intensity plots (insets of Fig.\u00a01e, f<\/a>). The overall valence-band structure is better visualized by the ARPES-intensity plot as a function of ky and EB in Fig.\u00a01f<\/a> which displays the complex band structure characterized by several holelike bands centered at the \u0393 point and an M-shaped band around EB\u2009~\u20092\u20132.5\u2009eV. From the energy separation between the top of valence bands at the \u0393 point and the bottom of conduction bands at the K point, it is suggested that ML Cr2Se3 is a semiconductor in non-doped regime with an indirect band gap of ~0.8\u2009eV. As shown by a side-by-side comparison of Fig.\u00a01f, g<\/a>, the overall band structure determined by ARPES shows a qualitative agreement with the calculated band structure for free-standing ML Cr2Se3 obtained from first-principles calculations for the FM phase assuming out-of-plane magnetic moments and an on-site Coulomb energy of U\u2009=\u20093.5 eV31<\/a>. For example, the experimental holelike band topped at the \u0393 point shows a good correspondence to the top of calculated up-spin bands (red curves), and the M-shaped down-spin bands (blue curves) are commonly recognized at ~1\u2009eV below the valence-band top, in both the experiment and calculation. The momentum location (the K point) of the bottom of the conduction band which is assigned to the up-spin Cr 3d\u00a0eg\u2191 band is also well reproduced by the calculation although the calculation underestimates the band-gap magnitude by ~30%. The appearance of the eg\u2191 electron pocket suggests that ML Cr2Se3 grown on 2\u2009ML graphene is a doped semiconductor with half-metallic nature. To identify the orbital character of observed bands, we carried out resonant ARPES measurements using SX photons around the Cr L3 absorption edge (for details, see Fig. S5<\/a> of Supplementary Note\u00a04<\/a>). The results show a strong resonance enhancement of ARPES intensities at EB\u2009~\u20091.5\u20132.5\u2009eV associated with the Cr 3d-t2g\u2191 bands hybridized with the Se 4p states (for details of the orbital assignments, see Supplementary Note\u00a05<\/a>).<\/p>\n Temperature dependence of the band structure across T Now that the overall band structure in the FM phase is established, next we show temperature evolution of the band structure in Fig.\u00a02a\u2013c<\/a> (detailed T-dependence is shown in Fig. S13<\/a>). Key characteristics of the complex band structure seen at T\u2009=\u200940\u2009K in Figs.\u00a01<\/a>f, 2a<\/a>, such as the M-shaped band around EB\u2009~\u20092\u20132.5\u2009eV and a sharp valence-band top at the \u0393 point, still persist at T\u2009=\u2009150\u2009K (Fig.\u00a02b<\/a>). In contrast, at T\u2009=\u2009300\u2009K (Fig.\u00a02c<\/a>), the spectral feature becomes simpler and the M-shaped band is converted to a V-shaped band located around EB\u2009~\u20091.3\u20132.1\u2009eV. As shown later, the detailed analysis and temperature-dependent XMCD measurements suggest that TC lies between 225 and 250\u2009K, higher than the estimated TC value of ~200\u2009K in ML Cr2Se3 on HOPG30<\/a>.<\/p>\n Fig. 2: Temperature evolution of band structure and evidence for spin-valley polarization.<\/b> a<\/b>\u2013c<\/b> ARPES-intensity plots along the \u0393K cut measured at T\u2009=\u200940\u2009K, 150\u2009K, and 300\u2009K, respectively, measured with circularly polarized photons of h\u03bd\u2009=\u200975\u2009eV. Peaks p1 and p2 are also indicated. d<\/b>, e<\/b> Temperature-dependence of EDCs at selected k cuts at ky\u2009=\u20090.0\u00a0(\u0393), \u22121.1\u2009\u00c5\u22121\u00a0(K\u2019), respectively. f<\/b> Temperature dependence of the peak position for valence-band peaks at EB\u2009~\u20092\u20132.5\u2009eV at the \u0393 point (ky\u2009=\u20090\u2009\u00c5\u22121) estimated by numerical fittings to the EDCs assuming Voigt peaks and linear background with error bars \u00b1 20\u2009meV. g<\/b>, h<\/b> Second-derivative intensity plots of Fig.\u00a02d, e, respectively. i<\/b> EDCs for ML Cr2Se3, obtained at the K and K\u2019 points with C+ and C- polarized lights using h\u03bd\u2009=\u200975\u2009eV. Yellow and purple curves represent subtracted EDCs obtained with C+ and C- photons expanded vertically by 5 times. Inset shows the expansion near EF. One can recognize a clear circular dichroism (CD) associated with spin-valley polarization which reverses its sign between the K and K\u2019 points.<\/p>\n Besides a drastic change in the band structure, a systematic T-dependent energy shift is observed in the EDCs and corresponding second-derivative intensity plots at the \u0393 point (ky\u2009=\u20090.0\u2009\u00c5\u22121) in Fig.\u00a02d, g<\/a>. All the bands, including the topmost valence band and corresponding spin-orbit split Se 4p states separated by ~0.2 eV45<\/a>, systematically move toward EF on increasing temperature upto TC, with a gradual increase in the peak width associated with thermal broadening. This is also the case for the spectra at the K\u2019 point (ky\u2009=\u2009\u2212 1.1\u2009\u00c5-1; Fig.\u00a02e, h<\/a>). Besides the systematic band shift, some bands show additional energy splitting at low temperatures. For example, at the \u0393 point (Fig.\u00a02d<\/a>), a main peak at EB\u2009=\u20092.16\u2009eV with a shoulder feature at 2.36\u2009eV at T\u2009=\u200940\u2009K, signify the existence of a double peak (marked as p1 and p2 in Fig.\u00a02d<\/a>). This double peak consisting of Cr-Se hybridized states constituting the M-shaped band get merged into a single peak on increasing temperature, around T\u2009=\u2009225\u2013250\u2009K. We quantified the T-dependence of band energies from numerical fits to the EDCs and the peak positions are shown in Fig.\u00a02f<\/a>. The band splitting vanishes between T\u2009=\u2009225\u2013250\u2009K, corresponding to TC of ML Cr2Se3. The same trend is also recognized for the peaks at ~1.97\u2009eV and ~2.13\u2009eV at T\u2009=\u200940\u2009K for the K\u2019 point (Fig.\u00a02e, h<\/a>) and corresponding plots of the t2g band energies in Fig. S7c<\/a> (for details, see Supplementary Note\u00a06<\/a>). We attribute the above observation to the band splitting associated with the FM transition, since the splitting sets in around TC, as is also confirmed by the T-dependent XMCD signal shown in Fig. S18<\/a>. Such a clear T-dependent band splitting below TC has been rarely reported in 2D ferromagnets24<\/a>,46<\/a>.<\/p>\n Spin-valley coupling<\/p>\n We found a signature of circular dichroism (CD) for the t2g\u2191 bands at the K and K\u2019 points at T\u2009=\u200940\u2009K for ML Cr2Se3, as shown Fig.\u00a02i<\/a>. Using right and left circularly polarized light (C+ and C-), the obtained EDCs at the K point (red and pink curves) show a difference between their peak intensities, signifying a finite CD. This CD is also observed at the K\u2019 point (blue and light blue curves) but with a sign reversal compared to the K point, as shown by the subtracted EDCs expanded vertically (yellow and purple curves). We found a sign reversal of CD also for the eg\u2191 pocket between the K and K\u2019 points (see inset to Fig.\u00a02i<\/a>). Intriguingly, the sign is also reversed between the t2g\u2191 and eg\u2191 bands. These observations suggest that photoelectron excitations are asymmetric between the K and K\u2019 points, supporting the valley-selective CD (i.e., valley polarization) which is a necessary condition for realizing anomalous valley Hall effect31<\/a>. It is noted that the observed CD is not likely to originate from experimental artifacts such as incomplete CD polarization or sample degradation, but is an intrinsic property of our Cr2Se3 film (for details, see Supplementary Note\u00a07<\/a>). This is also corroborated by the observation of three-fold symmetric LEED pattern suggestive of the inequivalently mixed structure domains rotated by 60\u00b0 from each other (in this regard, it is different from ML 1\u2009T\u2019 TMDs with equivalently mixed 120\u00b0 rotated domains47<\/a>,48<\/a>,49<\/a>,50<\/a>), making our Cr2Se3 film a valid candidate to observe valley polarization (for details, see Fig. S8<\/a> and Supplementary Note\u00a07<\/a>).<\/p>\n We found that the overall magnitude of CD is reduced in the 2\u2009ML sample with lower TC (see Fig. S9<\/a> in Supplementary Note\u00a07<\/a>), signifying that the valley-selective CD is coupled to the ferromagnetism. This coupling of localized t2g-spins and itinerant eg-valley states is supported by considering the magnitude of experimental energy splitting for the strongly hybridized t2g bands at the K\/K\u2019 point for ML (~160\u2009meV) which is much larger than the SOC energy (\u0394SOC) of Cr3+ states (~50\u2009meV) and inversion-symmetry breaking of the crystal (at most a few tens meV)31<\/a>. But the observed splitting is comparable to the known \u0394SOC of ~200\u2009meV in Se bands45<\/a>, which is about half of the atomic SOC energy \u0394\u2019SOC\u2009=\u2009418\u2009meV for Se 4p states. In a recent study on V1\/3NbS2 crystals, a giant valley-Zeeman coupling in surface states of the NbS2-termination top layer was reported to originate from hybridized V d orbitals and planar NbS2 orbitals with an exchange splitting \u0394ex\u2009~\u200952\u2009meV and \u0394SOC\u2009~\u200959\u2009meV aiding each other at the K point and opposing each other at the K\u2019 point. Using known values of valley-Zeeman splitting of ~0.2 meVT\u22121 for TMDs51<\/a>, the authors estimated that a magnetic field exceeding 250\u2009T was operative in V1\/3NbS2 to give the observed splitting. However, the results showed that the surface states of V1\/3NbS2 exhibit the same magnetic ordering temperature as the bulk, with TN\u2009~\u200953 K37<\/a>. In the present case, we see ferromagnetism with a relatively high TC\u2009~\u2009225\u2009K for ML Cr2Se3 case compared to an antiferromagnetic TN\u2009~\u200945\u2009K for bulk Cr2Se326<\/a>. However, we see an experimental energy splitting for the t2g bands at the K\/K\u2019 point for ML (~160\u2009meV) suggesting a spin-splitting-dominated spin-valley coupling since the valley splitting is calculated to be just 18 meV31<\/a>. Moreover, the gradual reduction of the splitting energy with a small reduction in TC by increasing number of layers (see Fig. S7<\/a> in Supplementary Note\u00a06<\/a>) also supports the intimate coupling of spin and valley degrees of freedom for an enhanced TC in 2\u2009ML and 3\u2009ML films compared to bulk TN\u2009~\u200945\u2009K.<\/p>\n Besides the spin-valley coupling, another intriguing characteristic of ML Cr2Se3 is the evolution of the eg\u2191 electron pocket at the K\/K\u2019 point. The EDCs in Fig.\u00a03a<\/a> signify a sharp peak associated with the eg\u2191 band at T\u2009=\u200940\u2009K for both the K and K\u2019 points. Upon increasing temperature, the spectral weight of eg\u2191-peak is monotonically reduced and the peak has almost vanished at T\u2009=\u2009300\u2009K. This suggests that ferromagnetism in ML Cr2Se3 is associated with spectral weight of the eg\u2191 pocket. Figure\u00a03a<\/a> shows that the total spectral weight at fixed temperature is higher at the K point than at the K\u2019 point (see purple or blue curves). This intensity asymmetry is attributed to the inequivalent valley states at the K and K\u2019 points predicted by the density-functional-theory (DFT) calculation31<\/a> and associated with the spin-valley coupling. We have carefully examined this inequivalent valley states between the K and K\u2019 points, and found that the asymmetric nature is reproducible for different samples. More intriguingly, the asymmetry gets enhanced after applying out-of-plane magnetic field, supporting the spin-valley coupling (for details, see Figs. S10<\/a> and S11<\/a> in Supplementary Note\u00a08<\/a>).<\/p>\n Fig. 3: Thickness dependence of electronic states.<\/b> a<\/b>\u2013c<\/b> Temperature dependence of EDCs near EF at the K (ky\u00a0= 1.1 \u00c5\u22121; left panel) and K\u2019 (ky= \u22121.1 \u00c5\u22121\ufeff; right panel) points to the evolution of the eg\u2191 electron pocket for ML Cr2Se3. The spectral weight is normalized to the valence-band t2g peak. d<\/b>\u2013f<\/b> Temperature dependence of the peak position for valence-band peaks p1 and p2 at the \u0393 point estimated by numerical fittings to the EDCs for ML, 2\u2009ML, and 3\u2009ML Cr2Se3, respectively, suggesting the gradual reduction of TC upon increasing the number of layers n. g<\/b>\u2013i<\/b> ARPES-intensity plots as a function of ky and EB along the \u0393K cut measured with h\u03bd\u2009=\u200975\u2009eV photons at T\u2009=\u200940\u2009K for ML, 2\u2009ML, and 3\u2009ML Cr2Se3, respectively. Inset to (h<\/b>) shows the ARPES intensity with enhanced color contrast around the K point. B. E. stands for binding energy.<\/p>\n In particular, ARPES measurements on ML Cr2Se3 film with improved statistics were carried out to confirm the inequivalence of valley states at K and K\u2019 points. ARPES intensity maps around the K\u2019 and K points, obtained after normalizing the total spectral weight over the plotted EB range of EF to 2.7\u2009eV (Fig. S10<\/a>a, b<\/a>) indicate that the intensity of the electron pocket around the K point is higher than that around the K\u2019 point, confirming the inequivalent valley states around K and K\u2019. Overlapped EDCs at positive ky\u2019s and negative ky\u2019s (Fig. S10c<\/a>) clearly indicate that the spectral weight of the eg -derived peak for positive ky\u2019s is higher than that for negative ky\u2019s.<\/p>\n To clarify the possible coupling of inequivalent valley states to the spin degrees of freedom, we performed ARPES measurements after magnetizing the sample by applying an out-of-plane magnetic field with the strength of B<\/b>\u2009=\u2009+ 0.1\u2009T (see EDCs in Fig. S10d<\/a>). While the overall spectral intensity of the electron pocket is slightly reduced, the asymmetric intensity of the EDCs between the K and K\u2019 points indicate that the inequivalence is preserved even after applying B<\/b>. To our surprise, we found that a broad shoulder feature appears at EB\u2009~\u20090.2\u2009eV more prominently for negative ky\u2019s, i.e., around the K\u2019 point, suggesting that the shape of the EDCs becomes more inequivalent after applying B<\/b>. This change is highlighted by a direct comparison of EDCs at the K and K\u2019 points (Fig. S11<\/a>a, b<\/a>) indicating that the spectral weight of the shoulder feature is enhanced at the K\u2019 point after applying B<\/b>, which is also confirmed by our numerical analysis of EDCs (Fig. S12<\/a>). We found that the shoulder feature becomes much weaker and the EDC shows a simpler peak shape at the K\u2019 point upon reversing B<\/b>, becoming similar to the spectrum at the K point obtained by applying positive B<\/b> (Fig. S11c<\/a>). In addition, we confirmed that this result is reproducible for different samples, by measuring another ML Cr2Se3 sample (Fig. S11d<\/a>). This finding strengthens our argument on the observation of inequivalent valley states between the K and K\u2019 points and their coupling to the spontaneous ferromagnetism.<\/p>\n Band structure of multilayer Cr2Se3<\/p>\n Next, we fabricated 2\u2009ML and 3\u2009ML Cr2Se3 films to investigate thickness evolution of their band structure and relation with spin-valley states. We found that the energy bands of 2\u2009ML and 3\u2009ML films (Fig.\u00a03h, i<\/a>) are shifted upward by ~0.4 and ~0.5\u2009eV, respectively, compared to the ML film (Fig.\u00a03g<\/a>). Simultaneously, the Cr 3d t2g bands get significantly broadened, and also show larger band splitting at the \u0393 point. Detailed analysis at the \u0393 point (and the K point; see Fig. S7<\/a> in Supplementary Note\u00a06<\/a>) shown in Fig.\u00a03d\u2013f<\/a> suggests that the TC gradually decreases on increasing the number of layers n; TC\u2009=\u2009225\u2013250\u2009K, 175\u2013200\u2009K, and 150\u2013175\u2009K, for ML, 2\u2009ML, and 3\u2009ML, respectively (for detailed T-dependent ARPES data and quantitative analyses of the band splitting, see Figs. S13<\/a>\u201317<\/a> in Supplementary Note\u00a09<\/a>). We have confirmed that TC\u2019s estimated by ARPES and XMCD well coincide with each other, suggesting the validity of the TC estimation from the band splitting (for details, see Fig. S18<\/a> in Supplementary Note\u00a010<\/a>). The TC reduction is correlated with the spectral weight at EF of metallic eg\u2191 pocket seen for ML (Fig.\u00a03a<\/a>), which gets reduced in 2\u2009ML (Fig.\u00a03b<\/a>) and almost vanishes in 3\u2009ML (Fig.\u00a03c<\/a>) (note that a tiny electron pocket still exists at low temperatures for 2\u2009ML, as seen in the image with enhanced color contrast in the inset to Fig.\u00a03h<\/a>). This is consistent with the observed valence-band shifts on increasing n and indicates that the highest doping of electron carriers occurs in the ML film at low-T. It is noted that the asymmetric intensity distribution of the eg\u2191 band between the K and K\u2019 points observed for ML gets reduced for 2\u2009ML and 3\u2009ML (Fig.\u00a03b, c<\/a>), confirming the coupling of valley anisotropy and ferromagnetism. Interestingly, a very recent study24<\/a> on Cr2Te3 showed that 3\u2009ML and 6\u2009ML films with TC\u2009=\u2009170\u2009K and T-dependent band shifts, exhibit a reduced TC\u2009=\u200990\u2009K in ML with no energy band shifts, indicating a Stoner to Heisenberg (itinerant to localized)-type FM order. In contrast, Cr2Se3 shows an enhancement of TC in the ML case with TC\u2009~\u2009225\u2009K compared to 2\u2009ML (TC\u2009~\u2009175\u2009K) and 3\u2009ML films (TC\u2009~\u2009150\u2009K), derived from spin-valley coupling of localized and itinerant states.<\/p>\n The most reasonable explanation of the observed n-dependent band structure and FM TC\u2019s is the charge transfer from the graphene substrate39<\/a>,52<\/a>, which is also supported by directly comparing the binding energy of the Dirac point of graphene bands before and after the fabrication of ML Cr2Se3 (for details, see Fig. S19<\/a> in Supplementary Note\u00a011<\/a>). Accordingly, the doped electron carrier density per unit Cr2Se3 layer is expected to be reduced for multilayer films since the total amount of transferred charge carriers across the interface is fixed; this behavior is realized in the present study. Since the Mermin-Wagner theorem12<\/a> suggests that FM order is suppressed upon reducing n, in contrast to present observations, the enhancement of TC up to 225\u2013250\u2009K in ML is likely due to the RKKY mechanism associated with maximum carrier density in eg\u2191 valley states. This argument also explains why the insulating ML Cr2Se3 films fabricated on Al2O3 or SiO2\/Si do not show FM but AF order, as in the bulk crystal26<\/a>,28<\/a>,29<\/a>, because no charge transfer is expected from insulating Al2O3 or SiO2\/Si in contrast to the present study which uses a metallic 2\u2009ML graphene\/SiC substrate. It also explains the observation of high-TC ferromagnetism (TC\u2009~\u2009200\u2009K) for ML Cr2Se3 on HOPG30<\/a>, comparable to the present work because charge-transfer characteristics of graphene and HOPG are expected to be similar with nearly equal work functions.<\/p>\n Finally, we discuss important differences between Cr2Se3 and Cr-Te based van der Waals ferromagnets Cr2Ge2Te6 and CrTe2. A critical difference is that tellurium compounds commonly show ferromagnetism in the bulk whereas bulk Cr2Se3 is an antiferromagnetic (TN\u2009~\u200945\u2009K) semiconductor. Moreover, only Cr2Se3 transforms into a ferromagnetic metal with TC\u2009~\u2009225\u2009K for ML films grown on graphene (TC\u2009~\u2009200\u2009K for ML Cr2Se3\/HOPG; ref. 30<\/a>). In contrast, the van der Waals ferromagnets, namely Cr2Ge2Te6 (ref. 13<\/a>) and CrTe2 show a reduction in TC on decreasing thickness (although there are conflicting reports for Cr2Te3 as discussed above23<\/a>,24<\/a>). Reference 24<\/a> showed that the dominantly Te character orbitals cross EF in Cr2Te3 and form the Fermi surface, leading to an itinerant Stoner type ferromagnetism in thick Cr2Te3 films, but for ML Cr2Te3 film, the Stoner condition is not satisfied and a local moment Heisenberg exchange driven ferromagnetism is realized. In contrast, the Se bands in Cr2Se3 sink well below EF and the occupation of the valley electron pockets with Cr 3d eg character, which couple with localized t2g spins, promotes the ferromagnetism. These aspects suggest that the origin of ferromagnetism in Cr2Se3 films on graphene or HOPG can be expected to be qualitatively different from the van der Waals ferromagnets (it is noted here that, in the ML limit, Cr2Te3 suffers from a trigonal distortion24<\/a> with a 2\u2009\u00d7\u20092 superstructure whereas Cr2Se3 maintains its 1\u2009\u00d7\u20091 structure, which can lead to differences in their magnetic properties). Also, the double exchange mechanism is usually considered for the case of mixed valent materials, which is unlikely for Cr2Se3 films on graphene, distinct from the situation of Cr2Ge2Te6 (refs. 53<\/a>,54<\/a>); for a detailed discussion, see Supplementary Note\u00a012<\/a>. Our results in Fig.\u00a03<\/a>, corroborated by temperature-dependent XMCD, suggest that the reduction of TC on increasing the number of layers is caused by a reduction in the electron carrier density transferred from the substrate across the interface. The results taken together indicate that the TC is proportional to the carrier density (this is supported by the plot of TC vs spectral density of states at EF in Fig. S20<\/a>), and hence suggest that the ferromagnetism is likely due to the localized t2g spins coupled by the RKKY interaction active in the valley electron pockets of Cr2Se3 films grown on graphene.<\/p>\n","protected":false},"excerpt":{"rendered":"Fabrication and characterization of ML Cr2Se3 First, we present fabrication and characterization of a ML Cr2Se3 film. Since…\n","protected":false},"author":2,"featured_media":35517,"comment_status":"","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[3845],"tags":[20546,17715,3965,17354,3966,74,70,17353,16,15],"class_list":{"0":"post-35516","1":"post","2":"type-post","3":"status-publish","4":"format-standard","5":"has-post-thumbnail","7":"category-physics","8":"tag-electronic-properties-and-materials","9":"tag-ferromagnetism","10":"tag-humanities-and-social-sciences","11":"tag-interfaces-and-thin-films","12":"tag-multidisciplinary","13":"tag-physics","14":"tag-science","15":"tag-surfaces","16":"tag-uk","17":"tag-united-kingdom"},"share_on_mastodon":{"url":"https:\/\/pubeurope.com\/@uk\/114370169199973438","error":""},"_links":{"self":[{"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/posts\/35516","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/comments?post=35516"}],"version-history":[{"count":0,"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/posts\/35516\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/media\/35517"}],"wp:attachment":[{"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/media?parent=35516"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/categories?post=35516"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.europesays.com\/uk\/wp-json\/wp\/v2\/tags?post=35516"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}
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