2007 APS March Meeting
Volume 52, Number 1
Monday–Friday, March 5–9, 2007;
Denver, Colorado
Session A28: Focus Session: Carbon Nanotube Optics I
8:00 AM–11:00 AM,
Monday, March 5, 2007
Colorado Convention Center
Room: 302
Sponsoring
Unit:
DMP
Chair: Stephen Doorn, Los Alamos National Laboratory
Abstract ID: BAPS.2007.MAR.A28.1
Abstract: A28.00001 : Magnetic Brightening of Dark Excitons in Carbon Nanotubes
8:00 AM–8:36 AM
Preview Abstract
Abstract
Author:
Junichiro Kono
(Department of Electrical and Computer Engineering, Rice University)
To gain insight into the internal energy structure and
radiative properties of excitons in single-walled carbon
nanotubes (SWNTs), we have studied photoluminescence (PL) from
individualized HiPco and CoMoCAT samples as a function of
magnetic field ($B$) and temperature ($T$). The PL intensity
increased, or ``brightened,'' with $B$ applied along the tube
axis and the amount of
brightening increased with decreasing $T$. These results are
consistent with the existence of a dark state below the first
bright state~[1]. In the presence of time reversal symmetry,
exchange-interaction-induced mixing between excitons in two
equivalent valleys (the K and K' valleys) is expected to result
in a set of exciton states, only one of which is optically
active.
This predicted bright state, however, is not the lowest in
energy. Excitons would be trapped in the dark, lowest-energy
state without a radiative recombination path. When a
tube-threading $B$ is applied, addition of an Aharonov-Bohm
phase modifies the circumferential boundary conditions on the
wave functions and lifts time reversal symmetry~[2,3]. This
symmetry breaking splits the K and K' valley transitions,
lessening the intervalley mixing and causing the recovery of
the unmixed direct K and K' excitons, which are both optically
active. We have calculated PL spectra through $B$-dependent
effective masses, populations of finite-$k$ states, and
acoustic phonon scattering, which quantitatively agree with the
observations. These results demonstrate the existence of dark
excitons, their influence on the PL quantum yield, and their
elimination through symmetry manipulation by a $B$. This work
was performed in collaboration with J.~Shaver, S.~Zaric,
O.~Portugall, V.~Krstic, G.~L.~J.~A.~Rikken, X.~Wei,
S.~A.~Crooker, Y.~Miyauchi, S.~Maruyama, and V.~Perebeinos and
supported by the Robert A.~Welch Foundation, the NSF, and
EuroMagNET.
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[1]~V.~Perebeinos {\it et al}.,
Phys.~Rev.~Lett.~{\bf 92}, 257402 (2004); H.~Zhao and
S.~Mazumdar, Phys.~Rev.~Lett.~{\bf 93}, 157402 (2004);
V.~Perebeinos {\it et al}., Nano Lett.~{\bf 5}, 2495 (2005);
C.~D.~Spataru {\it et al}., Phys.~Rev.~Lett.~{\bf 95}, 247402
(2005).
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[2]~T.~Ando, J.~Phys.~Soc.~Jpn.~{\bf 75}, 024707 (2006).
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[3]~S.~Zaric {\it et al}., Science {\bf 304}, 1129 (2004);
Phys.~Rev.~Lett.~{\bf 96}, 016406 (2006).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2007.MAR.A28.1