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We have performed a first-principles study of the p- and n-type conductivity in CuIn$_{1-x}$Ga$_x$Se$_{2}$ due to native point defects, based on the HSE06 hybrid functional. Band alignment shows that the band gap becomes larger with $x$ due…

Mesoscale and Nanoscale Physics · Physics 2015-06-22 Jonas Bekaert , Rolando Saniz , Bart Partoens , Dirk Lamoen

Semiconductor materials that can be doped both n-type and p-type are desirable for diode-based applications and transistor technology. Copper nitride (Cu3N) is a metastable semiconductor with a solar-relevant bandgap that has been reported…

Efficient doping of semiconductor nanowires remains a major challenge towards the commercialization of nanowire-based devices. In this work we investigate the growth regimes and electrical properties of MBE-grown p- and n-type gallium…

Mesoscale and Nanoscale Physics · Physics 2024-02-01 Vladislav Sharov , Kristina Novikova , Alexey Mozharov , Vladimir Fedorov , Prokhor Alekseev , Ivan Mukhin

Whether a quantum critical point (QCP) demarcates the end of the pseudogap (PG) regime in hole-doped cuprates at a singular doping level $p^* \approx 0.19$ remains an open question. A crucial part of this puzzle is how the carrier density…

Carrier-type reversal to enable the formation of semiconductor p-n junctions is a prerequisite for many electronic applications. Chalcogenide glasses are p-type semiconductors and their applications have been limited by the extraordinary…

In this paper we investigate, computationally and experimentally, the phase stability, electronic structure properties, and the propensity for n-type doping of In$_{2}$X$_{2}$O$_{7}$ (X=Si, Ge) ternary oxides. This family of materials…

The significance of p-type transparent oxide semiconductors (TOS) in the semiconductor industry is paramount, driving advancements in optoelectronic technologies for transparent electronic devices with unique properties. The recent…

Materials Science · Physics 2025-01-22 Zewen Xiao

We report a mechanical point-contact spectroscopy study on the single crystalline NbGe$_2$ with a superconducting transition temperature $T\rm_c$ = 2.0 - 2.1 K. The differential conductance curves at 0.3 K can be well fitted by a single gap…

Superconductivity · Physics 2021-06-29 Dongting Zhang , Tian Le , Baijing Lv , Lichang Yin , Chufan Chen , Zhiyong Nie , Dajun Su , Huiqiu Yuan , Zhu-An Xu , Xin Lu

The electron-doped cuprates Pr_{2-x}Ce_xCuO_4 and Nd_{2-x}Ce_xCuO_4 have been studied by electronic Raman spectroscopy across the entire region of the superconducting (SC) phase diagram. The SC pairing strength is found to be consistent…

A series of 122 phase BaFe$_{2-x}$Ni$_x$As$_2$ ($x$ = 0, 0.055, 0.096, 0.18, 0.23) single crystals were grown by self flux method and a dome-like Ni doping dependence of superconducting transition temperature is discovered. The transition…

Superconductivity · Physics 2009-02-27 L. J. Li , Q. B. Wang , Y. K. Luo , H. Chen , Q. Tao , Y. K. Li , X. Lin , M. He , Z. W. Zhu , G. H. Cao , Z. A. Xu

We systematically investigate the photoexcited (PE) quasi-particle (QP) relaxation and low-energy electronic structure in electron doped Ba(Fe_{1-x}Co_{x})_{2}As_{2} single crystals as a function of Co doping, 0<= x <=0.11. The evolution of…

Superconductivity · Physics 2012-08-07 L. Stojchevska , T. Mertelj , Jiun-Haw Chu , Ian R. Fisher , D. Mihailovic

We report persistent photoconductivity in $p$-type Sb$_2$Se$_3$ single crystals doped with Cd or Zn, where enhanced conductivity remains for hours after illumination ceases at temperatures below $\sim$25~K. Comparative transport and…

Materials Science · Physics 2025-10-17 F. Herklotz , E. V. Lavrov , T. D. C. Hobson , T. P. Shalvey , J. D. Major , K. Durose

Scalable substitutional doping of two-dimensional (2D) transition metal dichalcogenides (TMDCs) is a prerequisite to developing next-generation logic and memory devices based on 2D materials. To date, doping efforts are still nascent. Here,…

Here, we have studied the temperature dependent Seebeck coefficient (S) of the NaCo$_2$O$_4$ (NCO) by using experimental and computational methods. The range of experimentally obtained S is $\sim$55 to 103 $\mu$V/K in the temperature range…

Materials Science · Physics 2025-05-06 Rahul Raj , Sudhir K. Pandey

Cu$_3$SbSe$_4$ is a promising thermoelectric material due to high thermopower ($>400\ \mu$V/K) at 300K and higher. Although it has a simple crystal structure derived from zinc blende structure, previous work has shown that the physics of…

Materials Science · Physics 2014-09-17 Dat T. Do , S. D. Manhanti

Semiconductors with wide band gap (3.0 eV), high dielectric constant (> 10), good thermal dissipation, and capable of $n$- and $p$-type doping are highly desirable for high-energy power electronic devices. Recent studies indicate that $\rm…

Materials Science · Physics 2022-02-11 Fernando P. Sabino , Intuon Chatratin , Anderson Janotti , Gustavo M. Dalpian

Germanium single crystal having 45 mm diameter and 100 mm length of 7N+ purity has been grown by Czochralski method. Structural quality of the crystal has been characterized by Laue diffraction. Electrical conduction and Hall measurements…

Materials Science · Physics 2019-07-12 Manoranjan Ghosh , Shreyas Pitale , S. G. Singh , Shashwati Sen , S. C. Gadkari

The thermoelectric characteristics of lead selenium (PbSe) doped with gallium (Ga) are investigated in this study. When the lead sulfide (PbSe) is tuned with appropriate dopants, it exhibits satisfactory ZT values, hence making it a…

Materials Science · Physics 2025-04-01 Md. Moklesur Rahman , Md Kamal Hossain , Fateha Samad , Fysol Ibna Abbas

The effects of planar hole concentration, p, and in-plane disorder, Zn (y), on the DC resistivity, r(T), of sintered samples of Y_{1-x}Ca_xBa_2(Cu_{1-y}Zn_y)_3O_{7-d} were investigated over a wide doping range by changing both the oxygen…

Superconductivity · Physics 2015-06-24 S. H. Naqib , J. R. Cooper , J. L. Tallon , C. Panagopoulos

We report the temperature dependence of the infrared-visible conductivity of Pr(2-x)Ce(x)CuO(4) thin films. When varying the doping from a non-superconducting film (x = 0.11) to a superconducting overdoped film (x = 0.17), we observe, up to…

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