4 research outputs found
Current Saturation and Voltage Gain in Bilayer Graphene Field Effect Transistors
The emergence of graphene with its unique electrical
properties
has triggered hopes in the electronic devices community regarding
its exploitation as a channel material in field effect transistors.
Graphene is especially promising for devices working at frequencies
in the 100 GHz range. So far, graphene field effect transistors (GFETs)
have shown cutoff frequencies up to 300 GHz, while exhibiting poor
voltage gains, another important figure of merit for analog high frequency
applications. In the present work, we show that the voltage gain of
GFETs can be improved significantly by using bilayer graphene, where
a band gap is introduced through a vertical electric displacement
field. At a displacement field of −1.7 V/nm the bilayer GFETs
exhibit an intrinsic voltage gain up to 35, a factor of 6 higher than
the voltage gain in corresponding monolayer GFETs. The transconductance,
which limits the cutoff frequency of a transistor, is not degraded
by the displacement field and is similar in both monolayer and bilayer
GFETs. Using numerical simulations based on an atomistic <i>p</i><sub><i>z</i></sub> tight-binding Hamiltonian we demonstrate
that this approach can be extended to sub-100 nm gate lengths
Experimental Verification of Carrier Multiplication in Graphene
We
report on the first direct experimental observation of carrier multiplication
in graphene reaching a multiplication factor of up to 2 and persisting
on a picoseconds time scale. Exploiting multicolor pump–probe
measurement techniques, the excited nonequilibrium carrier distribution
is retrieved on an ultrafast time scale. This provides access to the
temporal evolution of the optically excited carrier density and thus
allows quantitative conclusions on possible carrier multiplication.
Microscopic time- and momentum-resolved calculations on the ultrafast
relaxation dynamics of optically excited carriers confirm the observation
of carrier multiplication under corresponding experimental conditions,
suggesting graphene as a promising material for novel high-efficiency
photodetection devices
Gate-Defined Electron–Hole Double Dots in Bilayer Graphene
We
present gate-controlled single-, double-, and triple-dot operation
in electrostatically gapped bilayer graphene. Thanks to the recent
advancements in sample fabrication, which include the encapsulation
of bilayer graphene in hexagonal boron nitride and the use of graphite
gates, it has become possible to electrostatically confine carriers
in bilayer graphene and to completely pinch-off current through quantum
dot devices. Here, we discuss the operation and characterization of
electron–hole double dots. We show a remarkable degree of control
of our device, which allows the implementation of two different gate-defined
electron–hole double-dot systems with very similar energy scales.
In the single-dot regime, we extract excited state energies and investigate
their evolution in a parallel magnetic field, which is in agreement
with a Zeeman-spin-splitting expected for a <i>g</i>-factor
of 2
Gate-Defined Electron–Hole Double Dots in Bilayer Graphene
We
present gate-controlled single-, double-, and triple-dot operation
in electrostatically gapped bilayer graphene. Thanks to the recent
advancements in sample fabrication, which include the encapsulation
of bilayer graphene in hexagonal boron nitride and the use of graphite
gates, it has become possible to electrostatically confine carriers
in bilayer graphene and to completely pinch-off current through quantum
dot devices. Here, we discuss the operation and characterization of
electron–hole double dots. We show a remarkable degree of control
of our device, which allows the implementation of two different gate-defined
electron–hole double-dot systems with very similar energy scales.
In the single-dot regime, we extract excited state energies and investigate
their evolution in a parallel magnetic field, which is in agreement
with a Zeeman-spin-splitting expected for a <i>g</i>-factor
of 2
