Teitl: Transport of indirect excitons in high magnetic fields


Dyfyniad
Wilkes J, Muljarov EA (2017). Transport of indirect excitons in high magnetic fields. Cardiff University. https://doi.org/10.17035/d.2017.0032309924


Nid yw'r data hwn ar gael ar hyn o bryd oherwydd: Bwriad i gyhoeddi canlyniadau prosiect


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Dull Mynediad: I anfon cais i gael y data hwn, ebostiwch opendata@caerdydd.ac.uk


Crewyr y Set Ddata o Brifysgol Caerdydd


Manylion y Set Ddata

Cyhoeddwr: Cardiff University

Dyddiad (y flwyddyn) pryd y daeth y data ar gael i'r cyhoedd: 2017

Fformat y data: .dat, .txt

Amcangyfrif o gyfanswm maint storio'r set ddata: Llai na 100 megabeit

Nifer y ffeiliau yn y set ddata: 6

DOI : 10.17035/d.2017.0032309924

DOI URL: http://doi.org/10.17035/d.2017.0032309924

Related URL: https://arxiv.org/pdf/1610.03116.pdf


Disgrifiad

Simulation data for the transport, thermalization and optical decay of indirect-magnetoexcitons in coupled quantum wells. The data was used to generate the results presented in the article “Transport of indirect excitons in high magnetic fields” by Y. Y. Kuznetsova, C. J. Dorow, E. V. Calman, L. V. Butov, J. Wilkes, E. A. Muljarov, K. L. Campman and A. C. Gossard, published in Physical Review B in 2017, htp://doi.org/10.1103/PhysRevB.95.125304

GS.dat contains the magnetic field dependence of the properties of the exciton ground state. The columns are magnetic field [T], optical transition energy [meV], oscillator strength, Bohr radius [nm], effective mass [m_0], radiative lifetime [ns] and dipole moment [nm].

The following files contain data on the in-plane profiles of the exciton cloud. In all cases, the first column is the in-plane coordinate in micrometers. The remaining columns are the profiles for magnetic field 0, 2, 4, 6, 8 and 10 T.

density.dat – density [109/cm2]

diffCoeff.dat – diffusion coefficient [cm2/s]

PL.dat – photoluminescence intensity [arb. units]

temperature.dat – temperature [K]

lifetime.dat – optical lifetime [ns]


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Diweddarwyd y tro diwethaf ar 2022-29-04 am 14:41