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Electron–hole liquid in a van der Waals heterostructure photocell at room temperature
In semiconductors, photo-excited charge carriers exist as a gas of electrons and holes, bound electron–hole pairs (excitons), biexcitons and trions 1 – 4 . At sufficiently high densities, the non-equilibrium system of electrons ( e − ) and holes ( h + ) may merge into an electronic liquid droplet 5...
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Published in: | Nature photonics 2019-04, Vol.13 (4), p.245-250 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In semiconductors, photo-excited charge carriers exist as a gas of electrons and holes, bound electron–hole pairs (excitons), biexcitons and trions
1
–
4
. At sufficiently high densities, the non-equilibrium system of electrons (
e
−
) and holes (
h
+
) may merge into an electronic liquid droplet
5
–
10
. Here, we report on the electron–hole liquid in ultrathin MoTe
2
photocells revealed through multi-parameter dynamic photoresponse microscopy (MPDPM). By combining rich visualization with comprehensive analysis of very large data sets acquired through MPDPM, we find that ultrafast laser excitation at a graphene–MoTe
2
–graphene interface leads to the abrupt formation of ring-like spatial patterns in the photocurrent response as a function of increasing optical power at
T
= 297 K. The sudden onset to these patterns, together with extreme sublinear power dependence and picosecond-scale photocurrent dynamics, provide strong evidence for the formation of a two-dimensional electron–hole liquid droplet. The electron–hole liquid, which features a macroscopic population of correlated electrons and holes, may offer a path to room-temperature optoelectronic devices that harness collective electronic phenomena.
Photoexcited charge carriers are typically approximated as a gas, but now it is shown that electrons and holes can behave as a liquid in MoTe
2
photocells. |
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ISSN: | 1749-4885 1749-4893 |
DOI: | 10.1038/s41566-019-0349-y |