<?xml version="1.0"?>
<metadata xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/"><dc:title>Fulleride superconductivity tuned by elastic strain due to cation compositional disorder</dc:title><dc:creator>Okur,	Esma H.	(Avtor)
	</dc:creator><dc:creator>Colman,	Ross	(Avtor)
	</dc:creator><dc:creator>Takabayashi,	Yasuhiro	(Avtor)
	</dc:creator><dc:creator>Jeglič,	Peter	(Avtor)
	</dc:creator><dc:creator>Ohishi,	Yasuo	(Avtor)
	</dc:creator><dc:creator>Kato,	Kenichi	(Avtor)
	</dc:creator><dc:creator>Arčon,	Denis	(Avtor)
	</dc:creator><dc:creator>Kubota,	Yoshiki	(Avtor)
	</dc:creator><dc:creator>Prassides,	Kosmas	(Avtor)
	</dc:creator><dc:subject>fullerides</dc:subject><dc:description>Dynamical fluctuations of the elastic strain in strongly correlated systems are known to affect the onset of metal-to-insulator or superconducting transitions. Here we report their effect on the properties of a family of bandwidth-controlled alkali-intercalated fullerene superconductors. We introduce elastic strain through static local structural disorder in a systematic and controllable way in the fcc-structured K$_x$Cs$_{3-x}$C$_{60}$ (with potassium content, 0.22 $\leq$ x$_K$ $\leq$ 2) series of compositions by utilizing the difference in size between the K$^+$ and Cs$^+$ co-dopants. The occurrence of the crossover from the Mott–Jahn–Teller insulating (MJTI) state into the strongly correlated Jahn–Teller metal (JTM) on cooling is evidenced for the compositions with x$_K$ &lt; 1.28 by both synchrotron X-ray powder diffraction (SXRPD) – anomalous reduction of the unit cell volume – and $^{133}$Cs NMR spectroscopy – sudden suppression in the $^{133}$Cs spin-lattice relaxation rates. The emerging superconducting state with a maximum critical temperature, T$_c$ = 30.9 K shows a characteristic dome-like dependence on the unit-cell volume or equivalently, on the ratio between the on-site Coulomb repulsion, U, and the bandwidth, W. However, compared to the parent Cs$_3$C$_{60}$ composition in which cation disorder effects are completely absent, the maximum T$_c$ is lower by ∼12%. The reduction in T$_c$ displays a linear dependence on the variance of the tetrahedral-site cation size, $\sigma_T^2$, thus establishing a clear link between structural-disorder–induced attenuation of critical elastic strain fluctuations and the electronic ground state.</dc:description><dc:date>2024</dc:date><dc:date>2024-10-24 13:36:59</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>164412</dc:identifier><dc:identifier>UDK: 53</dc:identifier><dc:identifier>ISSN pri članku: 2041-6539</dc:identifier><dc:identifier>DOI: 10.1039/d4sc03399j</dc:identifier><dc:identifier>COBISS_ID: 212103427</dc:identifier><dc:language>sl</dc:language></metadata>
