A single-phase high pressure (HP) modification of CsxFe2-ySe2 was synthesized at 11.8 GPa at ambient temperature. Structurally this polymorph is similar to the minor low pressure (LP) superconducting phase, namely they both crystallize in a ThCr2Si2-type structure without ordering of the Fe vacancies within the Fe-deficient FeSe4 layers. The HP CsxFe2-ySe2 polymorph is found to be less crystalline and nearly twice as soft compared to the parent major and minor phases of CsxFe2-ySe2. It can be quenched to low pressures and is stable at least on the scale of weeks. At ambient pressure the HP polymorph of CsxFe2-ySe2 is expected to exhibit different superconducting properties compared to its LP minor phase (Tc = 27 K).
IntroductionThe phenomena of superconductivity was discovered more than a century ago (Hg with a Tc = 4 K) [1], but to date no material exhibiting a superconducting response at ambient temperature has been reported. While the recently discovered FeSe phase also possesses a low critical temperature (Tc = 8 K [2]), there exist a number of ways to enhance its superconducting performance. For instance, the transition temperature drastically increases for FeSe in a monolayer form (Tc > 100 K [3]). In addition, its Tc can be enhanced by intercalation: for the Fe-deficient FeSe systems intercalated by alkali metals (A), the Tc was reported to reach 30 K [4][5][6]. Further increase in the Tc of AxFe2-ySe2 can be achieved through a control of Fe occupancies. Phases with Tc exceeding 40 K can be achieved through specific synthetic procedures, including precise control of stoichiometry and annealing conditions, and are characterized by fully, or close to fully, occupied Fe sites [7][8][9]. In addition, their formation can be mediated by NH3 molecules [10][11][12][13].Application of external pressure is yet another tool that allows control of physical properties, including FeSe-based superconducting materials. For the FeSe phase itself, high-pressure (HP) induces more than a four-fold increase in its critical temperature (Tc = 36 K around 7 GPa [14]). Above 7 GPa, structural transformation of FeSe into a topologically-different polymorph suppresses superconductivity and results in the a formation of the famous superconducting dome, with a complex phase composition [15]. In contrast, the Tc of the intercalated AxFe2-ySe2 (Aalkali metals) decreases upon application of external pressure, and eventually superconductivity vanishes [16,17]. Upon further pressure increase (P > 11.5 GPa) a new superconducting phase (denoted as SCII) with a Tc reaching 48 K was reported [18]. This result, however, has not yet been experimentally reproduced with independent studies reporting much lower critical temperatures (~5 or ~20 K depending on sample preparation procedures [19,20]).The structural properties of alkali-intercalated FeSe phases are complex, as are the ones of the parent FeSe phase [15]. Firstly, the AxFe2-ySe2 family features intrinsic phase separation and the second minor phase is responsible for the observed supercond...