Giant multiphoton absorption for THz resonances in silicon hydrogenic donors

The absorption of multiple photons when there is no resonant intermediate state is a well-known nonlinear process in atomic vapours, dyes and semiconductors. The N -photon absorption (NPA) rate for donors in semiconductors scales proportionally from hydrogenic atoms in vacuum with the dielectric con...

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Bibliographic Details
Published in:Nature photonics Vol. 12; no. 3; pp. 179 - 184
Main Authors: van Loon, M. A. W., Stavrias, N., Le, Nguyen H., Litvinenko, K. L., Greenland, P. T., Pidgeon, C. R., Saeedi, K., Redlich, B., Aeppli, G., Murdin, B. N.
Format: Journal Article
Language:English
Published: London Nature Publishing Group UK 01-03-2018
Nature Publishing Group
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Summary:The absorption of multiple photons when there is no resonant intermediate state is a well-known nonlinear process in atomic vapours, dyes and semiconductors. The N -photon absorption (NPA) rate for donors in semiconductors scales proportionally from hydrogenic atoms in vacuum with the dielectric constant and inversely with the effective mass, factors that carry exponents 6 N and 4 N , respectively, suggesting that extremely large enhancements are possible. We observed 1PA, 2PA and 3PA in Si:P with a terahertz free-electron laser. The 2PA coefficient for 1 s –2 s at 4.25 THz was 400,000,000 GM (=4 × 10 −42  cm 4  s), many orders of magnitude larger than is available in other systems. Such high cross-sections allow us to enter a regime where the NPA cross-section exceeds that of 1PA—that is, when the intensity approaches the binding energy per Bohr radius squared divided by the uncertainty time (only 3.84 MW cm − 2 in silicon)—and will enable new kinds of terahertz quantum control. By using a terahertz free-electron laser, multiphoton transitions between impurity states in p-doped Si are investigated. The two- and three-photon integrated absorption cross-sections are found to be the highest ever reported for a discrete oscillator system.
ISSN:1749-4885
1749-4893
DOI:10.1038/s41566-018-0111-x