posted on 2024-03-06, 20:15authored byAnuraj S. Kshirsagar, Katherine A. Koch, Ajay Ram Srimath Kandada, Mahesh K. Gangishetty
Luminescence quenching by hole transport layers (HTLs)
is one of
the major issues in developing efficient perovskite light-emitting
diodes (PeLEDs), which is particularly prominent in blue-emitting
devices. While a variety of material systems have been used as interfacial
layers, the origin of such quenching and the type of interactions
between perovskites and HTLs are still ambiguous. Here, we present
a systematic investigation of the luminescence quenching of CsPbBr3 by a commonly employed hole transport polymer, poly[(9,9-dioctylfluorenyl-2,7diyl)-co-(4,4′-(N-(4-sec-butylphenyl)
diphenylamine)] (TFB), in LEDs. Strong and weak quantum-confined CsPbBr3 (nanoplatelets (NPLs)/nanocrystals (NCs)) are rationally
selected to study the quenching mechanism by considering the differences
in their morphology, energy level alignments, and quantum confinement.
The steady-state and time-resolved Stern–Volmer plots unravel
the dominance of dynamic and static quenching at lower and higher
concentrations of TFB, respectively, with a maximum quenching efficiency
of 98%. The quenching rate in NCs is faster than that in NPLs owing
to their longer PL lifetimes and weak quantum confinement. The ultrafast
transient absorption results support these dynamics and rule out the
involvement of Forster or Dexter energy transfer. Finally, the 1D 1H and 2D nuclear overhauser effect spectroscopy nuclear magnetic
resonance (NOESY NMR) study confirms the exchange of native ligands
at the NCs surface with TFB, leading to dark CsPbBr3-TFB
ensemble formation accountable for luminescence quenching. This highlights
the critical role of the triarylamine functional group on TFB (also
the backbone of many HTLs) in the quenching process. These results
shed light on the underlying reasons for the luminescence quenching
in PeLEDs and will help to rationally choose the interfacial layers
for developing efficient LEDs.