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On-Surface Synthesis of Variable Bandgap Nanoporous Graphene
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Tuning the bandgap of nanoporous graphene
is desirable for applications such as the charge transport layer in
organic-hybrid devices. The holy grail in the field is the ability to
synthesize 2D nanoporous graphene with variable pore sizes, and hence tuneable band
gaps. Herein, we demonstrate the on-surface synthesis of nanoporous graphene
with variable bandgaps. Two types of nanoporous graphene were synthesized via
hierarchical C-C coupling, and verified by low-temperature scanning tunneling
microscopy and non-contact atomic force microscopy with CO-terminated tip. Nanoporous
graphene-1 is non-planar, and nanoporous graphene-2 is a single-atom thick
planar sheet. Scanning tunneling spectroscopy measurements reveal that nanoporous
graphene-2 has a bandgap of 3.8 eV, while nanoporous graphene-1 has a larger
bandgap of 5.0 eV. Corroborated by first-principles calculations, we propose
that the large bandgap opening is governed by the confinement of π-electrons
induced by pore generation or the non-planar structure, and can be explained by
Clar sextet theory. Our finding shows that by introducing nanopores, semimetallic
graphene is converted into semiconducting nanoporous graphene-2 or insulating
wide-bandgap nanoporous graphene-1.
American Chemical Society (ACS)
Title: On-Surface Synthesis of Variable Bandgap Nanoporous Graphene
Description:
Tuning the bandgap of nanoporous graphene
is desirable for applications such as the charge transport layer in
organic-hybrid devices.
The holy grail in the field is the ability to
synthesize 2D nanoporous graphene with variable pore sizes, and hence tuneable band
gaps.
Herein, we demonstrate the on-surface synthesis of nanoporous graphene
with variable bandgaps.
Two types of nanoporous graphene were synthesized via
hierarchical C-C coupling, and verified by low-temperature scanning tunneling
microscopy and non-contact atomic force microscopy with CO-terminated tip.
Nanoporous
graphene-1 is non-planar, and nanoporous graphene-2 is a single-atom thick
planar sheet.
Scanning tunneling spectroscopy measurements reveal that nanoporous
graphene-2 has a bandgap of 3.
8 eV, while nanoporous graphene-1 has a larger
bandgap of 5.
0 eV.
Corroborated by first-principles calculations, we propose
that the large bandgap opening is governed by the confinement of π-electrons
induced by pore generation or the non-planar structure, and can be explained by
Clar sextet theory.
Our finding shows that by introducing nanopores, semimetallic
graphene is converted into semiconducting nanoporous graphene-2 or insulating
wide-bandgap nanoporous graphene-1.
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