TY - JOUR
T1 - Photon correlations in colloidal quantum dot molecules controlled by the neck barrier
AU - Koley, Somnath
AU - Cui, Jiabin
AU - Panfil, Yossef E.
AU - Ossia, Yonatan
AU - Levi, Adar
AU - Scharf, Einav
AU - Verbitsky, Lior
AU - Banin, Uri
N1 - Publisher Copyright:
© 2022 Elsevier Inc.
PY - 2022/11/2
Y1 - 2022/11/2
N2 - The charge redistribution upon optical excitation of various necked homodimer colloidal quantum dot molecules (CQDMs) is investigated using single-particle emission spectroscopy. By tuning the hybridization of the electron wavefunctions at a fixed center-to-center distance through controlling the neck girth, we reveal two coupling limits: on one hand, a “connected-but-confined” situation where neighboring CQDs are weakly fused to each other, manifesting a weak-coupling regime, and on the other hand, a “connected-and-delocalized” situation where the neck is filled beyond the facet size, leading to a rod-like architecture manifesting strong coupling. The interplay between the radiative and non-radiative Auger decays of these states turns emitted photons from the CQDMs in the weak-coupling regime highly bunched unlike CQD monomers, while the antibunching is regained at the strong-coupling regime. This work sets an analogy for the artificial molecule CQDMs with regular molecules, where the two distinct regimes of weak and strong coupling correspond to ionic- or covalent-type bonding, respectively.
AB - The charge redistribution upon optical excitation of various necked homodimer colloidal quantum dot molecules (CQDMs) is investigated using single-particle emission spectroscopy. By tuning the hybridization of the electron wavefunctions at a fixed center-to-center distance through controlling the neck girth, we reveal two coupling limits: on one hand, a “connected-but-confined” situation where neighboring CQDs are weakly fused to each other, manifesting a weak-coupling regime, and on the other hand, a “connected-and-delocalized” situation where the neck is filled beyond the facet size, leading to a rod-like architecture manifesting strong coupling. The interplay between the radiative and non-radiative Auger decays of these states turns emitted photons from the CQDMs in the weak-coupling regime highly bunched unlike CQD monomers, while the antibunching is regained at the strong-coupling regime. This work sets an analogy for the artificial molecule CQDMs with regular molecules, where the two distinct regimes of weak and strong coupling correspond to ionic- or covalent-type bonding, respectively.
KW - Auger process
KW - MAP2: Benchmark
KW - colloidal quantum dots
KW - electronic coupling
KW - photon antibunching
KW - single-particle spectroscopy
UR - http://www.scopus.com/inward/record.url?scp=85140921250&partnerID=8YFLogxK
U2 - 10.1016/j.matt.2022.07.032
DO - 10.1016/j.matt.2022.07.032
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AN - SCOPUS:85140921250
SN - 2590-2393
VL - 5
SP - 3997
EP - 4014
JO - Matter
JF - Matter
IS - 11
ER -