2012
DOI: 10.1002/adma.201203346
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Enhanced Charge Carrier Mobility in Two‐Dimensional High Dielectric Molybdenum Oxide

Abstract: We demonstrate that the energy bandgap of layered, high-dielectric α-MoO(3) can be reduced to values viable for the fabrication of 2D electronic devices. This is achieved through embedding Coulomb charges within the high dielectric media, advantageously limiting charge scattering. As a result, devices with α-MoO(3) of ∼11 nm thickness and carrier mobilities larger than 1100 cm(2) V(-1) s(-1) are obtained.

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Cited by 377 publications
(364 citation statements)
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“…Inclusion of nonlocal bonding in the computation of MoO 3 helps with the description of anisotropic bulk properties as well as supporting the use of twodimensional sheets, belts and flakes in many electronic devices. [10][11][12][13][14][15] The thermodynamically stable phase of MoO 3 is a unique orthorhombic layered structure (Figure 1), space group Pbnm, with each layer comprising two sub-layers of MoO 6 distorted octahedra, edge-sharing along the c-axis and corner-sharing along the a-axis. The layers are bound by weak, mainly van der Waals, interactions and the separation between the layers is known as the van der Waals gap.…”
Section: Introductionmentioning
confidence: 99%
“…Inclusion of nonlocal bonding in the computation of MoO 3 helps with the description of anisotropic bulk properties as well as supporting the use of twodimensional sheets, belts and flakes in many electronic devices. [10][11][12][13][14][15] The thermodynamically stable phase of MoO 3 is a unique orthorhombic layered structure (Figure 1), space group Pbnm, with each layer comprising two sub-layers of MoO 6 distorted octahedra, edge-sharing along the c-axis and corner-sharing along the a-axis. The layers are bound by weak, mainly van der Waals, interactions and the separation between the layers is known as the van der Waals gap.…”
Section: Introductionmentioning
confidence: 99%
“…[12][13][14][15][16][17][18][19][20][21][22] Owing to its high work function -up to 6.9 eV [12] and to the layered structure of α-MoO 3 , MoO x is also employed as a 2D material beyond graphene and as efficient hole contact on 2D transition metal dichalcogenides for p-type field effect transistors (p-FETs). [23][24][25] In view of a reliable device performance, the control over the chemical and physical properties of the MoO x system is mandatory. It has been recently reported 14,[26][27][28][29][30][31][32] that in MoO x with x < 3, oxygen vacancies originated from partially populated d-states, give rise to occupied energy states within the forbidden gap -∼ 3.0 eV at room temperature (RT) 12 -becoming bands above a critical concentration and driving the Fermi level close to the conduction band.…”
mentioning
confidence: 99%
“…The carrier mobility is an important device parameter in semiconductor applications which has received considerable attention [1][2][3]. The evaluation of the electron mobility in an n-type semiconductor depends on a set of parameters such as temperature and doping concentration along with some material characteristics like static dielectric permittivity, electron effective mass, deformation potential and piezoelectric constant.…”
Section: Introductionmentioning
confidence: 99%