2015
DOI: 10.1021/acs.jpcc.5b00204
|View full text |Cite
|
Sign up to set email alerts
|

Direct Femtosecond Observation of Charge Carrier Recombination in Ternary Semiconductor Nanocrystals: The Effect of Composition and Shelling

Abstract: Heavy-metal free ternary semiconductor nanocrystals are emerging as key materials in photoactive applications. However, the relative abundance of intrabandgap defect states and lack of understanding of their origins within this class of nanocrystals are major factors limiting their applicability. To remove these undesirable defect states which considerably shorten the lifetimes of photogenerated excited carriers, a detailed understanding about their origin and nature is required. In this report, we monitor the… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

10
45
1

Year Published

2015
2015
2017
2017

Publication Types

Select...
9

Relationship

7
2

Authors

Journals

citations
Cited by 40 publications
(56 citation statements)
references
References 52 publications
10
45
1
Order By: Relevance
“…We assign this to excited-state absorption and will discuss its possible nature in more detail below. The observation of photoinduced absorption in CIS NCs is consistent with previous TA measurements in the red and near-infrared, 25,40 and the data presented here reveal the true magnitude of this TA spectral feature. Both the positive and negative signals decay partially on the nanosecond time scale investigated.…”
supporting
confidence: 92%
“…We assign this to excited-state absorption and will discuss its possible nature in more detail below. The observation of photoinduced absorption in CIS NCs is consistent with previous TA measurements in the red and near-infrared, 25,40 and the data presented here reveal the true magnitude of this TA spectral feature. Both the positive and negative signals decay partially on the nanosecond time scale investigated.…”
supporting
confidence: 92%
“…The excitation pulse at 480 nm was generated using a spectrally tunable optical Parametric Amplifier (Light Conversion LTD) integrated to a Ti:sapphire femtosecond regenerative amplifier operating at 800 nm with 35 fs pulses and a repetition rate of 1 kHz. The white light probe pulse, on the other hand, was generated by a super continuum source2930. The pump and probe beams were overlapped spatially and temporally on the sample, and the transmitted probe light from the samples was collected and focused on the broad-band ultraviolet–visible-near-infrared detectors to record the time-resolved excitation-induced difference spectra.…”
Section: Methodsmentioning
confidence: 99%
“…TA decays were measured with a femto-nanosecond pump-probe setup. The detailed experimental setup has been described elsewhere5455. To estimate the lifetime ( t ) at higher excitation intensities, the data were fitted with a bi-exponential decay function ( y = y 0 + A 1 e −( x − x 0)/ t 1 + A 2 e −( x − x 0)/ t 2 ), while at lower excitation intensities, the data were fitted with a single-exponential decay ( y = y 0 + A 1 e −( x − x 0)/ t 1 ).…”
Section: Methodsmentioning
confidence: 99%