8 research outputs found
Direct Measurement of Ballistic and Diffusive Electron Transport in Gold
We experimentally show that the ballistic length of hot
electrons
in laser-heated gold films can exceed âŒ150 nm, which is âŒ50%
greater than the previously reported value of 100 nm inferred from
pumpâprobe experiments. We also find that the mean free path
of electrons at the peak temperature following interband excitation
can reach upward of âŒ45 nm, which is higher than the average
value of 30 nm predicted from our parameter-free density functional
perturbation theory. Our first-principles calculations of electronâphonon
coupling reveal that the increase in the mean free path due to interband
excitation is a consequence of drastically reduced electronâphonon
coupling from lattice stiffening, thus providing the microscopic understanding
of our experimental findings
Using Laser-Induced Thermal Voxels to Pattern Diverse Materials at the SolidâLiquid Interface
We
describe a high-resolution patterning approach that combines the spatial
control inherent to laser direct writing with the versatility of benchtop
chemical synthesis. By taking advantage of the steep thermal gradient
that occurs while laser heating a metal edge in contact with solution,
diverse materials comprising transition metals are patterned with
feature size resolution nearing 1 ÎŒm. We demonstrate fabrication
of reduced metallic nickel in one step and examine electrical properties
and air stability through direct-write integration onto a device platform.
This strategy expands the chemistries and materials that can be used
in combination with laser direct writing
Modification of the Poly(bisdodecylquaterthiophene) Structure for High and Predominantly Nonionic Conductivity with Matched Dopants
Four p-type polymers
were synthesized by modifying polyÂ(bisdodecylquaterthiophene)
(PQT12) to increase oxidizability by p-dopants. A sulfur atom is inserted
between the thiophene rings and dodecyl chains, and/or 3,4-ethylenedioxy
groups are appended to thiophene rings of PQT12. Doped with NOBF4,
PQTS12 (with sulfur in side chains) shows a conductivity of 350 S
cm<sup>â1</sup>, the highest reported nonionic conductivity
among films made from dopantâpolymer solutions. Doped with
tetrafluorotetracyanoquinodimethane (F4TCNQ), PDTDE12 (with 3,4-ethylenedioxy
groups on thiophene rings) shows a conductivity of 140 S cm<sup>â1</sup>. The converse combinations of polymer and dopant and formulations
using a polymer with both the sulfur and ethylenedioxy modifications
showed lower conductivities. The conductivities are stable in air
without extrinsic ion contributions associated with PEDOT:PSS that
cannot support sustained current or thermoelectric voltage. Efficient
charge transfer, tighter ÏâÏ stacking, and strong
intermolecular coupling are responsible for the conductivity. Values
of nontransient Seebeck coefficient and conductivity agree with empirical
modeling for materials with these levels of pure hole conductivity;
the power factor compares favorably with prior p-type polymers made
by the alternative process of immersion of polymer films into dopant
solutions. Models and conductivities point to significant mobility
increases induced by dopants on the order of 1â5 cm<sup>2</sup> V<sup>â1</sup> s<sup>â1</sup>, supported by field-effect
transistor studies of slightly doped samples. The thermal conductivities
were in the range of 0.2â0.5 W m<sup>â1</sup> K<sup>â1</sup>, typical for conductive polymers. The results point
to further enhancements that could be obtained by increasing doped
polymer mobilities
Molecular Tuning of the Vibrational Thermal Transport Mechanisms in Fullerene Derivative Solutions
Control
over the thermal conductance from excited molecules into
an external environment is essential for the development of customized
photothermal therapies and chemical processes. This control could
be achieved through molecule tuning of the chemical moieties in fullerene
derivatives. For example, the thermal transport properties in the
fullerene derivatives indene-C<sub>60</sub> monoadduct (ICMA), indene-C<sub>60</sub> bisadduct (ICBA), [6,6]-phenyl C<sub>61</sub> butyric acid
methyl ester (PCBM), [6,6]-phenyl C<sub>61</sub> butyric acid butyl
ester (PCBB), and [6,6]-phenyl C<sub>61</sub> butyric acid octyl ester
(PCBO) could be tuned by choosing a functional group such that its
intrinsic vibrational density of states bridge that of the parent
molecule and a liquid. However, this effect has never been experimentally
realized for molecular interfaces in liquid suspensions. Using the
pumpâprobe technique time domain thermotransmittance, we measure
the vibrational relaxation times of photoexcited fullerene derivatives
in solutions and calculate an effective thermal boundary conductance
from the opto-thermally excited molecule into the liquid. We relate
the thermal boundary conductance to the vibrational modes of the functional
groups using density of states calculations from molecular dynamics.
Our findings indicate that the attachment of an ester group to a C<sub>60</sub> molecule, such as in PCBM, PCBB, and PCBO, provides low-frequency
modes which facilitate thermal coupling with the liquid. This offers
a channel for heat flow in addition to direct coupling between the
buckyball and the liquid. In contrast, the attachment of indene rings
to C<sub>60</sub> does not supply the same low-frequency modes and,
thus, does not generate the same enhancement in thermal boundary conductance.
Understanding how chemical functionalization of C<sub>60</sub> affects
the vibrational thermal transport in molecule/liquid systems allows
the thermal boundary conductance to be manipulated and adapted for
medical and chemical applications
Thermal Conductance across Phosphonic Acid Molecules and Interfaces: Ballistic versus Diffusive Vibrational Transport in Molecular Monolayers
The influence of planar organic linkers
on thermal boundary conductance across hybrid interfaces has focused
on the organic/inorganic interaction energy rather than on vibrational
mechanisms in the molecule. As a result, research into interfacial
transport at planar organic monolayer junctions has treated molecular
systems as thermally ballistic. We show that thermal conductance in
phosphonic acid (PA) molecules is ballistic, and the thermal boundary
conductance across metal/PA/sapphire interfaces is driven by the same
phononic processes as those across metal/sapphire interfaces without
PAs, with one exception. We find a more than 40% reduction in conductance
across henicosaÂfluoroÂdodecylÂphosphonic acid (F21PA)
interfaces, independent of metal contact, despite similarities in
structure, composition, and terminal group to the variety of other
PAs studied. Our results suggest diffusive scattering of thermal vibrations
in F21PA, demonstrating a clear path toward modification of interfacial
thermal transport based on knowledge of ballistic and diffusive scattering
in single monolayer molecular interfacial films
Modifying Surface Energy of Graphene via Plasma-Based Chemical Functionalization to Tune Thermal and Electrical Transport at Metal Interfaces
The high mobility exhibited by both
supported and suspended graphene, as well as its large in-plane thermal
conductivity, has generated much excitement across a variety of applications.
As exciting as these properties are, one of the principal issues inhibiting
the development of graphene technologies pertains to difficulties
in engineering high-quality metal contacts on graphene. As device
dimensions decrease, the thermal and electrical resistance at the
metal/graphene interface plays a dominant role in degrading overall
performance. Here we demonstrate the use of a low energy, electron-beam
plasma to functionalize graphene with oxygen, fluorine, and nitrogen
groups, as a method to tune the thermal and electrical transport properties
across gold-single layer graphene (Au/SLG) interfaces. We find that
while oxygen and nitrogen groups improve the thermal boundary conductance
(<i>h</i><sub>K</sub>) at the interface, their presence
impairs electrical transport leading to increased contact resistance
(Ï<sub>C</sub>). Conversely, functionalization with fluorine
has no impact on <i>h</i><sub>K</sub>, yet Ï<sub>C</sub> decreases with increasing coverage densities. These findings indicate
exciting possibilities using plasma-based chemical functionalization
to tailor the thermal and electrical transport properties of metal/2D
material contacts
Room-Temperature Voltage Tunable Phonon Thermal Conductivity via Reconfigurable Interfaces in Ferroelectric Thin Films
Dynamic
control of thermal transport in solid-state systems is a transformative
capability with the promise to propel technologies including phononic
logic, thermal management, and energy harvesting. A solid-state solution
to rapidly manipulate phonons has escaped the scientific community.
We demonstrate active and reversible tuning of thermal conductivity
by manipulating the nanoscale ferroelastic domain structure of a PbÂ(Zr<sub>0.3</sub>Ti<sub>0.7</sub>)ÂO<sub>3</sub> film with applied electric
fields. With subsecond response times, the room-temperature thermal
conductivity was modulated by 11%
Interlayer Coupling Controlled Ordering and Phases in Polar Vortex Superlattices
The
recent discovery of polar topological structures
has opened
the door for exciting physics and emergent properties. There is, however,
little methodology to engineer stability and ordering in these systems,
properties of interest for engineering emergent functionalities. Notably,
when the surface area is extended to arbitrary thicknesses, the topological
polar texture becomes unstable. Here we show that this instability
of the phase is due to electrical coupling between successive layers.
We demonstrate that this electrical coupling is indicative of an effective
screening length in the dielectric, similar to the conductorâferroelectric
interface. Controlling the electrostatics of the superlattice interfaces,
the system can be tuned between a pure topological vortex state and
a mixed classical-topological phase. This coupling also enables engineering
coherency among the vortices, not only tuning the bulk phase diagram
but also enabling the emergence of a 3D lattice of polar textures