Tunable room-temperature spin-selective optical Stark effect in solution-processed layered halide perovskites
Author(s) -
David Giovanni,
Wee Kiang Chong,
Herlina Arianita Dewi,
Krishnamoorthy Thirumal,
Ishita Neogi,
R. Ramesh,
Subodh G. Mhaisalkar,
Nripan Mathews,
Tze Chien Sum
Publication year - 2016
Publication title -
science advances
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.928
H-Index - 146
ISSN - 2375-2548
DOI - 10.1126/sciadv.1600477
Subject(s) - exciton , halide , optoelectronics , photonics , perovskite (structure) , materials science , quantum dot , semiconductor , spin (aerodynamics) , ultrashort pulse , spin engineering , stark effect , condensed matter physics , dielectric , quantum well , electric field , physics , optics , spin polarization , chemistry , laser , electron , quantum mechanics , inorganic chemistry , thermodynamics , crystallography
Ultrafast spin manipulation for opto–spin logic applications requires material systems that have strong spin-selective light-matter interaction. Conventional inorganic semiconductor nanostructures [for example, epitaxial II to VI quantum dots and III to V multiple quantum wells (MQWs)] are considered forerunners but encounter challenges such as lattice matching and cryogenic cooling requirements. Two-dimensional halide perovskite semiconductors, combining intrinsic tunable MQW structures and large oscillator strengths with facile solution processability, can offer breakthroughs in this area. We demonstrate novel room-temperature, strong ultrafast spin-selective optical Stark effect in solution-processed (C6H4FC2H4NH3)2PbI4 perovskite thin films. Exciton spin states are selectively tuned by ~6.3 meV using circularly polarized optical pulses without any external photonic cavity (that is, corresponding to a Rabi energy of ~55 meV and equivalent to applying a 70 T magnetic field), which is much larger than any conventional system. The facile halide and organic replacement in these perovskites affords control of the dielectric confinement and thus presents a straightforward strategy for tuning light-matter coupling strength.
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