Abstract:Ge‐doped In2O3 thin films prepared by magnetron sputtering are studied using photoelectron spectroscopy and Hall effect measurements. Carrier conductivities of up to 8.35thinmathspace×thinmathspace103cm−1 and carrier mobilities of up to 57thinmathspacecm2thinmathspaceV−1s−1 are observed. The surface Ge concentration is enhanced by a factor of 2–3 compared to the concentration in the interior of the films. The surface Ge concentration increases with more oxidizing deposition conditions, in opposite to what has … Show more
“…All the examples given in this section so far concerned Sn doped indium oxide, as it is currently the benchmark materials for inorganic transparent electrodes. However, it has been shown that indium oxide can also be efficiently doped by other elements such as Si, Ga or Mo [34][35][36][37] .…”
Section: Figure 3 Evolution Of Resistivity Carrier Concentration and Carrier Mobility (Hall Mobility) Inmentioning
confidence: 99%
“…Gallium doped In2O3 for instance, was reported to display conductivities in the range of 10 3 to 10 4 Scm -1 and extremely high electron mobilities of 50 cm 2 V -1 s -1 [34,36,37] , whereas doping of In2O3 with molybdenum resulted in improved transmittance in the visible regime as compared to tin doped InO [35] . deposited via an aqueous sol-gel process.…”
Section: Figure 3 Evolution Of Resistivity Carrier Concentration and Carrier Mobility (Hall Mobility) Inmentioning
Nowadays, opto-electronic devices, such as displays, are omnipresent in our daily life. A crucial component of these devices is a transparent electrode, which allows the in-and out-coupling of light. With the goal of optimizing the electrode characteristics and improving device efficiencies, many approaches for the fabrication of thin, transparent conducting films have been studied. This review gives an overview of the different material classes which have been 2 used as transparent electrodes, ranging from metal oxides, such as Indium Tin Oxide, metal and carbonaceous nanostructures, to conducting polymers and composites. For every material class a brief description of the fundamental principles, processing routes and the latest achievements is given. Furthermore, the different electrodes are compared regarding their opto-electronic performance, flexibility and surface roughness. Ultimately, advantages and drawbacks of the respective electrodes are discussed. This critical comparison of fundamentally different transparent conducting materials allows, on one hand, to make a sensible choice of electrode for specific applications, and, on the other hand, to point out scientific challenges that must still be addressed.
“…All the examples given in this section so far concerned Sn doped indium oxide, as it is currently the benchmark materials for inorganic transparent electrodes. However, it has been shown that indium oxide can also be efficiently doped by other elements such as Si, Ga or Mo [34][35][36][37] .…”
Section: Figure 3 Evolution Of Resistivity Carrier Concentration and Carrier Mobility (Hall Mobility) Inmentioning
confidence: 99%
“…Gallium doped In2O3 for instance, was reported to display conductivities in the range of 10 3 to 10 4 Scm -1 and extremely high electron mobilities of 50 cm 2 V -1 s -1 [34,36,37] , whereas doping of In2O3 with molybdenum resulted in improved transmittance in the visible regime as compared to tin doped InO [35] . deposited via an aqueous sol-gel process.…”
Section: Figure 3 Evolution Of Resistivity Carrier Concentration and Carrier Mobility (Hall Mobility) Inmentioning
Nowadays, opto-electronic devices, such as displays, are omnipresent in our daily life. A crucial component of these devices is a transparent electrode, which allows the in-and out-coupling of light. With the goal of optimizing the electrode characteristics and improving device efficiencies, many approaches for the fabrication of thin, transparent conducting films have been studied. This review gives an overview of the different material classes which have been 2 used as transparent electrodes, ranging from metal oxides, such as Indium Tin Oxide, metal and carbonaceous nanostructures, to conducting polymers and composites. For every material class a brief description of the fundamental principles, processing routes and the latest achievements is given. Furthermore, the different electrodes are compared regarding their opto-electronic performance, flexibility and surface roughness. Ultimately, advantages and drawbacks of the respective electrodes are discussed. This critical comparison of fundamentally different transparent conducting materials allows, on one hand, to make a sensible choice of electrode for specific applications, and, on the other hand, to point out scientific challenges that must still be addressed.
“…Nevertheless, according to DFT calculations [28][29][30]33], one would expect some differences between [110]and [111]-oriented films, which both exhibit flat surfaces. A possible explanation for the independence on surface orientation is the segregation of the Sn dopant to the surface, which is particularly observed under reducing conditions [34][35][36]. A different surface composition will affect the surface dipole.…”
Section: Ito Surface Potentialsmentioning
confidence: 99%
“…Significant difference of the ionization potential I P , which is the difference between the valence band maximum and vacuum energy, between the [100] and [111]-surfaces of In 2 O 3 could be observed as well [29]. The situation is more complex for doped In 2 O 3 due to dopant segregation [30,[34][35][36]. Some authors [17,37] suggested that a surface treatment of the substrate may enhance the stability of the organic molecules.…”
The modification of the work function of Sn-doped In 2 O 3 (ITO) by vacuum adsorption of 4-(Dimethylamino)benzoic acid (4-DMABA) has been studied using in situ photoelectron spectroscopy. Adsorption of 4-DMABA is self-limited with an approximate thickness of a single monolayer. The lowest work function obtained is 2.82 ± 0.1 eV, enabling electron injection into many organic materials. In order to identify a potential influence of the ITO substrate surface on the final work function, different ITO surface orientations and treatments have been applied. Despite the expected differences in substrate work function and chemical bonding of 4-DMABA to the substrate, no influence of substrate surface orientation is identified. The resulting work function of ITO/4-DMABA substrates can be described by a constant ionization potential of the adsorbed 4-DMABA of 5.00 ± 0.08 eV, a constant band alignment between ITO and 4-DMABA and a varying Fermi energy in the ITO substrate. This corresponds to the behaviour of a conventional semiconductor heterostructure and deviates from the vacuum level alignment of interfaces between organic compounds. The difference is likely related to a stronger chemical bonding at the ITO/4-DMABA interface compared to the van der Waals bonding at interfaces between organic compounds.
“…The electrical conductivity can be significantly enhanced to approximately 1000 S cm −1 by alloying with Sn, which is known as indiumtin-oxide (ITO). There are also reports on the improvement of electrical conductivity by alloying with different elements, such as Ti [29], Ge [30], and Mo [31]. However, the thermal conductivity of In 2 O 3 -based materials is generally high, which is an obstacle for thermoelectric applications.…”
Thermoelectric materials are considered promising candidates for thermal energy conversion. This study presents the fabrication of Zn– and Ce–alloyed In2O3 with a porous structure. The electrical conductivity was improved by the alloying effect and an ultra–low thermal conductivity was observed owing to the porous structure, which concomitantly provide a distinct enhancement of ZT. However, SiO2 nanoparticle additives react with the matrix to form a third-phase impurity, which weakens the electrical conductivity and increases the thermal conductivity. A thermoelectric module was constructed for the purpose of thermal heat energy conversion. Our experimental results proved that both an enhancement in electrical conductivity and a suppression in thermal conductivity could be achieved through nano–engineering. This approach presents a feasible route to synthesize porous thermoelectric oxides, and provides insight into the effect of additives; moreover, this approach is a cost-effective method for the fabrication of thermoelectric oxides without traditional hot-pressing and spark–plasma–sintering processes.
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