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Circularly Polarized Optical Stark Effect in CdSe Colloidal Quantum Wells
Author(s) -
Benjamin T. Diroll
Publication year - 2020
Publication title -
nano letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 4.853
H-Index - 488
eISSN - 1530-6992
pISSN - 1530-6984
DOI - 10.1021/acs.nanolett.0c02409
Subject(s) - stark effect , quantum confined stark effect , quantum well , electro absorption modulator , absorption (acoustics) , quantum dot , absorption edge , atomic physics , femtosecond , photon energy , blueshift , photon , exciton , band gap , materials science , condensed matter physics , optoelectronics , chemistry , photoluminescence , physics , laser , optics , quantum dot laser , electric field , quantum mechanics
Colloidal quantum wells, or nanoplatelets, exhibit large, circularly polarized optical Stark effects under sub-band-gap femtosecond illumination. The optical Stark effect is measured for CdSe colloidal quantum wells of several thicknesses and separately as a measure of pump photon energy, pump fluence, and temperature. These measurements show that optical Stark effects in colloidal quantum wells shift the absorption features up to 5 meV, at the intensities up to 2.9 GW·cm -2 and large detuning (>400 meV) of the pump photon energy from the band edge absorption. Optical Stark shifts are underpinned by large transition dipoles of the colloidal quantum wells (μ = 15-23 D), which are larger than those of any reported colloidal quantum dots or epitaxial quantum wells. The rapid (<500 fs), narrow band blue shift of the excitonic features under circular excitation indicates the viability of these materials beyond light emission such as spintronics or all-optical switching.

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