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This paper presents an experimental how-to on time-resolved photoluminescence. The hardware used in many single photon-counting setups will be described and a basic how-to will be presented. This is intended to help students and experimenters understand the key system parameters and how to correctly set them in time-resolved photoluminescence setups.
Time-resolved photoluminescence (TRPL) is a key technique for understanding the photophysics of semiconductor nanocrystals and light-emitting materials in general. This work is a primer for setting up and conducting TRPL on nanocrystals and related materials using single-photon-counting (SPC) systems. Basic sources of error in the measurement can be avoided by consideration of the experimental setup and calibration. The detector properties, count rate, the spectral response, reflections in optical setups, and the specific instrumentation settings for single photon counting will be discussed. Attention to these details helps ensure reproducibility and is necessary for obtaining the best possible data from an SPC system. The main aim of the protocol is to help a student of TRPL understand the experimental setup and the key hardware parameters one must generally comprehend in order to gain useful TRPL data in many common single-photon-counting setups. The secondary purpose is to serve as a condensed primer for the student of experimental time-resolved luminescence spectroscopy.
Time-resolved photoluminescence (TRPL) is an important and standard method for studying the photophysics of luminescent materials. TRPL measurement systems can be open setups constructed by the experimenter or they can be self-contained units purchased directly from a manufacturer. Open setups are considered superior to "closed-box" TRPL units because they permit more experimental control and additional ways to collect useful data; however, they demand a more complete understanding of the measurement. TRPL is widely employed in the development of luminescent devices and should always be reported along with the basic emission spectrum of semiconductor nanocryst....
1. Preparation
A standard SPC decay curve is shown in Figure 3. The initial rise was shifted so that the peak corresponds to zero time (this is not the case in the raw data due to the electronic and optical delays). The signal-to-background ratio is about 100 because this sample has a long-lived but weak phosphorescence. A weak reflection is clearly observable on the log scale, which occurs about 50 ns after the main TRPL peak. This is due to reflections inside the 5-meter-long optical patch fiber, as repo.......
There are several important user-controlled parameters in any SPC setup that must be understood by the user. These parameters will explain the limitations of the SPC method for TRPL, allow the user to troubleshoot the setup more easily if something goes wrong, and help to understand the critical steps that are effectively required for good data collection. Moreover, different samples will often require different system settings - in other words, one cannot have a single procedure for all possible SPC decay traces. The se.......
The Natural Sciences and Engineering Research Council of Canada provides funding for this research. Thanks to Xiaoyuan Liu for performing the fit in Figure 3 and Dundappa Mumbaraddi for providing the rare-earth-doped perovskite sample. Thanks to Julius Heitz for making Reference20 available.
....Name | Company | Catalog Number | Comments |
AOM | Isomet | 1260C | |
Laser | Alphalas | Picopower | |
Laser | Coherent | Enterprise | |
MCS | Becker-Hickl | PMS-400 | |
PMT | Becker-Hickl | HPM100-50 | |
PMT | Hamamatsu | H-7422 | |
SPCM | Becker-Hickl | EMN130 |
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