TY - JOUR
T1 - Spin-Polarized Photoluminescence in Au25(SC8H9)18 Monolayer-Protected Clusters
AU - Herbert, Patrick J.
AU - Knappenberger, Kenneth L.
N1 - Funding Information:
This work was supported by awards from the National Science Foundation to K.L.K., under Grant Number CHE‐1806222 and CHE‐1904876. The authors thank the Ackerson group at Colorado State University for providing the Au(SCH) sample. The authors also thank Dr. Tian Zhao for designing and creating the table of contents cover art. 25 8 9 18
Publisher Copyright:
© 2021 Wiley-VCH GmbH
PY - 2021/7/8
Y1 - 2021/7/8
N2 - Here, the observation of spin-polarized emission for the Au25(SC8H9)18 monolayer-protected cluster (MPC) is reported. Variable-temperature variable-field magnetic circular photoluminescence (VTV (Formula presented.) -MCPL) measurements are combined with VT-PL spectroscopy to provide state-resolved characterization of the transient electronic structure and spin-polarized electron-hole recombination dynamics of Au25(SC8H9)18. Through analysis of VTV (Formula presented.) -MCPL measurements, a low energy (1.64 eV) emission peak is assigned to intraband relaxation between core-metal-localized superatom-D to -P orbitals. Two higher energy interband components (1.78 eV, 1.94 eV) are assigned to relaxation from superatom-D orbitals to states localized to the inorganic semirings. For both intraband superatom-based or interband relaxation mechanisms, the extent of spin-polarization, quantified as the degree of circular polarization (DOCP), is determined by state-specific electron-vibration coupling strengths and energy separations of bright and dark electronic fine-structure levels. At low temperatures (<60 K), metal–metal superatom-based intraband transitions dominate the global PL emission. At higher temperatures (>60 K), interband ligand-based emission is dominant. In the low-temperature PL regime, increased sample temperature results in larger global PL intensity. In the high-temperature regime, increased temperature quenches interband radiative recombination. The relative intensity for each PL mechanism is discussed in terms of state-specific electronic-vibrational coupling strengths and related to the total angular momentum, quantified by Landé g-factors.
AB - Here, the observation of spin-polarized emission for the Au25(SC8H9)18 monolayer-protected cluster (MPC) is reported. Variable-temperature variable-field magnetic circular photoluminescence (VTV (Formula presented.) -MCPL) measurements are combined with VT-PL spectroscopy to provide state-resolved characterization of the transient electronic structure and spin-polarized electron-hole recombination dynamics of Au25(SC8H9)18. Through analysis of VTV (Formula presented.) -MCPL measurements, a low energy (1.64 eV) emission peak is assigned to intraband relaxation between core-metal-localized superatom-D to -P orbitals. Two higher energy interband components (1.78 eV, 1.94 eV) are assigned to relaxation from superatom-D orbitals to states localized to the inorganic semirings. For both intraband superatom-based or interband relaxation mechanisms, the extent of spin-polarization, quantified as the degree of circular polarization (DOCP), is determined by state-specific electron-vibration coupling strengths and energy separations of bright and dark electronic fine-structure levels. At low temperatures (<60 K), metal–metal superatom-based intraband transitions dominate the global PL emission. At higher temperatures (>60 K), interband ligand-based emission is dominant. In the low-temperature PL regime, increased sample temperature results in larger global PL intensity. In the high-temperature regime, increased temperature quenches interband radiative recombination. The relative intensity for each PL mechanism is discussed in terms of state-specific electronic-vibrational coupling strengths and related to the total angular momentum, quantified by Landé g-factors.
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U2 - 10.1002/smll.202004431
DO - 10.1002/smll.202004431
M3 - Article
C2 - 33511771
AN - SCOPUS:85099850426
SN - 1613-6810
VL - 17
JO - Small
JF - Small
IS - 27
M1 - 2004431
ER -