Strong quantum confinement in semiconductors compresses
the wavefunctions of band carriers to nanometer-scale volumes, significantly enhancing their interactions with dopants. In magnetically doped
semiconductors, where paramagnetic dopants couple to band carriers via strong sp–d spin
exchange, giant magneto-optical effects can be
realized using few, or even single,
impurity spins. Importantly, however, thermodynamic spin fluctuations become increasingly relevant in this few-spin limit: the statistical N^1/2 fluctuations of N
spins are expected to generate giant effective magnetic fields
B_eff, which dramatically impacts carrier spin dynamics,
even in the absence of an applied field.
Here, I present measurements of both the initial and final stages of exciton magnetic polarons (EMPs) in lightly doped Cd_1-xMn_xSe colloidal nanocrystals. In the first section, I show our ultrafast spectroscopic investigations of the large B_eff in this system. At B_applied= 0T, extremely rapid
(300–600 GHz) electron spin precession is
observed, indicating B_eff∼15−30 T [1]. In the second part of the talk, I show our work on fully-formed EMPs. Using the highly sensitive technique of resonant photoluminescence, we directly measure the EMP binding energy to be tens of meV. Temperature- and field-dependent studies reveal that the exchange field is approximately 10 T, which agrees with theoretical estimates [2]. Taken together, the measurements of initial, ultrafast coherent dynamics and final, static formation states, give us a comprehensive picture of EMPs in doped nanocrystals.
[1] W. D. Rice et al. Nature Nanotech. 11, 137 (2016).
[2] W. D. Rice et al. Nano Lett. 17, 3068 (2017).
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