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Abstract
Time-resolved photoelectron spectroscopy can give insights into carrier dynamics and offers the possibility of element and site-specific information through the measurements of core levels. In this paper, we demonstrate that this method can access electrons dynamics in PbS quantum dots over a wide time window spanning from pico- to microseconds in a single experiment carried out at the synchrotron facility BESSY II. The method is sensitive to small changes in core level positions. Fast measurements at low pump fluences are enabled by the use of a pump laser at a lower repetition frequency than the repetition frequency of the X-ray pulses used to probe the core level electrons: Through the use of a time-resolved spectrometer, time-dependent analysis of data from all synchrotron pulses is possible. Furthermore, by picosecond control of the pump laser arrival at the sample relative to the X-ray pulses, a time-resolution limited only by the length of the X-ray pulses is achieved. Using this method, we studied the charge dynamics in thin film samples of PbS quantum dots on n-type MgZnO substrates through time-resolved measurements of the Pb 5d core level. We found a time-resolved core level shift, which we could assign to electron injection and charge accumulation at the MgZnO/PbS quantum dots interface. This assignment was confirmed through the measurement of PbS films with different thicknesses. Our results therefore give insight into the magnitude of the photovoltage generated specifically at the MgZnO/PbS interface and into the timescale of charge transport and electron injection, as well as into the timescale of charge recombination at this interface. It is a unique feature of our method that the timescale of both these processes can be accessed in a single experiment and investigated for a specific interface.
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Details
1 KTH Royal Institute of Technology, Division of Applied Physical Chemistry, Department of Chemistry, Stockholm, Sweden (GRID:grid.5037.1) (ISNI:0000000121581746)
2 Uppsala University, Division of Molecular and Condensed Matter Physics, Department of Physics and Astronomy, Uppsala, Sweden (GRID:grid.8993.b) (ISNI:0000 0004 1936 9457)
3 Uppsala University, Department of Chemistry - Ångström Laboratory, Uppsala, Sweden (GRID:grid.8993.b) (ISNI:0000 0004 1936 9457)
4 Beihang University, School of Materials Science and Engineering, Beijing, China (GRID:grid.64939.31) (ISNI:0000 0000 9999 1211)
5 Helmholtz-Zentrum Berlin GmbH, Institute Methods and Instrumentation for Synchrotron Radiation Research, Berlin, Germany (GRID:grid.424048.e) (ISNI:0000 0001 1090 3682)
6 Helmholtz-Zentrum Berlin GmbH, Institute Methods and Instrumentation for Synchrotron Radiation Research, Berlin, Germany (GRID:grid.424048.e) (ISNI:0000 0001 1090 3682); University of Potsdam, Institute of Physics and Astronomy, Potsdam, Germany (GRID:grid.11348.3f) (ISNI:0000 0001 0942 1117)
7 Uppsala University, Division of Molecular and Condensed Matter Physics, Department of Physics and Astronomy, Uppsala, Sweden (GRID:grid.8993.b) (ISNI:0000 0004 1936 9457); Uppsala-Berlin Joint Laboratory on Next Generation Photoelectron Spectroscopy, Berlin, Germany (GRID:grid.8993.b)