5 research outputs found
Confirmation of K-Momentum Dark Exciton Vibronic Sidebands Using <sup>13</sup>C-labeled, Highly Enriched (6,5) Single-walled Carbon Nanotubes
A detailed knowledge of the manifold of both bright and
dark excitons
in single-walled carbon nanotubes (SWCNTs) is critical to understanding
radiative and nonradiative recombination processes. Excitonâphonon
coupling opens up additional absorption and emission channels, some
of which may âbrightenâ the sidebands of optically forbidden
(dark) excitonic transitions in optical spectra. In this report, we
compare <sup>12</sup>C and <sup>13</sup>C-labeled SWCNTs that are
highly enriched in the (6,5) species to identify both absorptive and
emissive vibronic transitions. We find two vibronic sidebands near
the bright <sup>1</sup>E<sub>11</sub> singlet exciton, one absorptive
sideband âź200 meV above, and one emissive sideband âź140
meV below, the bright singlet exciton. Both sidebands demonstrate
a âź50 cm<sup>â1</sup> isotope-induced shift, which is
commensurate with excitonâphonon coupling involving phonons
of A<sub>1</sub><sup>â˛</sup> symmetry (D band, Ď âź
1330 cm<sup>â1</sup>). Independent analysis of each sideband
indicates that both sidebands arise from the same dark exciton level,
which lies at an energy approximately 25 meV above the bright singlet
exciton. Our observations support the recent prediction of, and mounting
experimental evidence for, the dark K-momentum singlet exciton lying
âź25 meV (for the (6,5) SWCNT) above the bright Î-momentum
singlet. This study represents the first use of <sup>13</sup>C-labeled
SWCNTs highly enriched in a single nanotube species to unequivocally
confirm these sidebands as vibronic sidebands of the dark K-momentum
singlet exciton
Charge Separation in P3HT:SWCNT Blends Studied by EPR: Spin Signature of the Photoinduced Charged State in SWCNT
Single-wall carbon nanotubes (SWCNTs)
could be employed in organic
photovoltaic (OPV) devices as a replacement or additive for currently
used fullerene derivatives, but significant research remains to explain
fundamental aspects of charge generation. Electron paramagnetic resonance
(EPR) spectroscopy, which is sensitive only to unpaired electrons,
was applied to explore charge separation in P3HT:SWCNT blends. The
EPR signal of the P3HT positive polaron increases as the concentration
of SWCNT acceptors in a photoexcited P3HT:SWCNT blend is increased,
demonstrating long-lived charge separation induced by electron transfer
from P3HT to SWCNTs. An EPR signal from reduced SWCNTs was not identified
in blends due to the free and fast-relaxing nature of unpaired SWCNT
electrons as well as spectral overlap of this EPR signal with the
signal from positive P3HT polarons. However, a weak EPR signal was
observed in chemically reduced SWNTs, and the <i>g</i> values
of this signal are close to those of C<sub>70</sub>-PCBM anion radical.
The anisotropic line shape indicates that these unpaired electrons
are not free but instead localized
Unraveling the <sup>13</sup>C NMR Chemical Shifts in Single-Walled Carbon Nanotubes: Dependence on Diameter and Electronic Structure
The atomic specificity afforded by nuclear magnetic resonance
(NMR)
spectroscopy could enable detailed mechanistic information about single-walled
carbon nanotube (SWCNT) functionalization as well as the noncovalent
molecular interactions that dictate ground-state charge transfer and
separation by electronic structure and diameter. However, to date,
the polydispersity present in as-synthesized SWCNT populations has
obscured the dependence of the SWCNT <sup>13</sup>C chemical shift
on intrinsic parameters such as diameter and electronic structure,
meaning that no information is gleaned for specific SWCNTs with unique
chiral indices. In this article, we utilize a combination of <sup>13</sup>C labeling and density gradient ultracentrifugation (DGU)
to produce an array of <sup>13</sup>C-labeled SWCNT populations with
varying diameter, electronic structure, and chiral angle. We find
that the SWCNT isotropic <sup>13</sup>C chemical shift decreases systematically
with increasing diameter for semiconducting SWCNTs, in agreement with
recent theoretical predictions that have heretofore gone unaddressed.
Furthermore, we find that the <sup>13</sup>C chemical shifts for small
diameter metallic and semiconducting SWCNTs differ significantly,
and that the full-width of the isotropic peak for metallic SWCNTs
is much larger than that of semiconducting nanotubes, irrespective
of diameter
Effect of Solvent Polarity and Electrophilicity on Quantum Yields and Solvatochromic Shifts of Single-Walled Carbon Nanotube Photoluminescence
In this work, we investigate the impact of the solvation
environment
on single-walled carbon nanotube (SWCNT) photoluminescence quantum
yield and optical transition energies (<i>E<sub>ii</sub></i>) using a highly charged aryleneethynylene polymer. This novel surfactant
produces dispersions in a variety of polar solvents having a wide
range of dielectric constants (methanol, dimethyl sulfoxide, aqueous
dimethylformamide, and deuterium oxide). Because a common surfactant
can be used while maintaining a constant SWCNTâsurfactant morphology,
we are able to straightforwardly evaluate the impact of the solvation
environment upon SWCNT optical properties. We find that (i) the SWCNT
quantum yield is strongly dependent on both the polarity and electrophilicity
of the solvent and (ii) solvatochromic shifts correlate with the extent
of SWCNT solvation. These findings provide a deeper understanding
of the environmental dependence of SWCNT excitonic properties and
underscore that the solvent provides a tool with which to modulate
SWCNT electronic and optical properties
Photoinduced Energy and Charge Transfer in P3HT:SWNT Composites
Using steady-state photoluminescence and transient microwave conductivity (TRMC) spectroscopies, photoinduced energy and charge transfer from poly(3-hexylthiophene) (P3HT) to single-walled carbon nanotubes (SWNTs) are reported. Long-lived charge carriers are observed for excitons generated in the polymer due to interfacial electron transfer, while excitation of the SWNTs results in short-lived carriers confined to the nanotubes. The TRMC-measured mobility of electrons injected into the SWNTs exhibits a surprisingly small lower limit of 0.057 cm<sup>2</sup>/(V s), which we attribute to carrier scattering within the nanotube that inhibits resonance of the microwave electric field with the confined carriers. The observation of charge transfer and the lifetime of the separated carriers suggest that the primary photoinduced carrier generation process does not limit the performance of organic photovoltaic (OPV) devices based on P3HT:SWNT composites. With optimization, blends of P3HT with semiconducting SWNTs (s-SWNTs) may exhibit promise as an OPV active layer and could provide good solar photoconversion power efficiencies