scholarly journals Erratum to: Scaling of the Temperature Dependent Resistivity and Hall Effect in Ba(Fe1−x Co x )2As2

2011 ◽  
Vol 24 (7) ◽  
pp. 2181-2181
Author(s):  
E. Arushanov ◽  
S. Levcenko ◽  
G. Fuchs ◽  
B. Holzapfel ◽  
S. L. Drechsler ◽  
...  
2019 ◽  
Vol 99 (17) ◽  
Author(s):  
David Wagenknecht ◽  
Libor Šmejkal ◽  
Zdeněk Kašpar ◽  
Jairo Sinova ◽  
Tomáš Jungwirth ◽  
...  

2011 ◽  
Vol 24 (8) ◽  
pp. 2285-2292 ◽  
Author(s):  
E. Arushanov ◽  
S. Levcenko ◽  
G. Fuchs ◽  
B. Holzapfel ◽  
S. L. Drechsler ◽  
...  

2011 ◽  
Author(s):  
B. Guster ◽  
V. Ghenescu ◽  
L. Ion ◽  
A. Radu ◽  
O. Porumb ◽  
...  

2006 ◽  
Vol 23 (6) ◽  
pp. 1551-1553 ◽  
Author(s):  
Cao Shuo ◽  
Zhou Qing-Li ◽  
Guan Dong-Yi ◽  
Lu Hui-Bin ◽  
Yang Guo-Zhen

2012 ◽  
Vol 05 (03) ◽  
pp. 1250026 ◽  
Author(s):  
FAHAD ALAM ◽  
SAJID ALI ANSARI ◽  
WASI KHAN ◽  
M. EHTISHAM KHAN ◽  
A. H. NAQVI

Polyaniline (PANI) is recognized as one of the most important conducting polymers due to its high conductivity and good stability. In this paper, polyaniline/silver (PANI/Ag) nanocomposites were synthesized by in-situ polymerization of aniline using ammonium peroxydisulphate (APS) as oxidizing agent with varying concentration of Ag nanoparticles colloids (0 ml, 25 ml and 50 ml). Silver nanoparticles were synthesized separately in colloidal form from silver nitrate (Ag2NO3) with the help of reducing agent sodium borohydride (NaBH4). The PANI/ Ag nanocomposites were characterized by XRD, SEM, AFM, UV-visible, temperature dependent resistivity and dielectric measurements. All samples show a single phase nature of the nanoparticles. The electrical resistivity as function of temperature was measured in the temperature range 298–383 K, which indicates a semiconducting to metallic transition at 373 K and 368 K for 25 ml and 50 ml silver colloid samples, respectively.


2020 ◽  
Vol 1004 ◽  
pp. 620-626
Author(s):  
Hironori Takeda ◽  
Mitsuru Sometani ◽  
Takuji Hosoi ◽  
Takayoshi Shimura ◽  
Hiroshi Yano ◽  
...  

Temperature-dependent Hall effect measurements were conducted to investigate the channel conduction mechanisms of 4H-SiC metal-oxide-semiconductor field-effect transistors (MOSFETs). This method allows us to discriminate the impact of the density of mobile (free) carriers in the inversion channels and their net mobility on the performance of SiC MOSFETs. It was found that, while the free carrier ratio of SiC MOSFETs with conventional gate oxides formed by dry oxidation is below 4% at 300 K, increasing the free carrier ratio due to thermal excitation of trapped electrons from SiO2/SiC interfaces leads to an unusual improvement in the field-effect mobility of SiC MOSFETs at elevated temperatures. Specifically, a significant increase in free carrier density surpasses the mobility degradation caused by phonon scattering for thermally grown SiO2/SiC interfaces. It was also found that, although nitrogen incorporation in SiO2/SiC interfaces increases the free carrier ratio typically up to around 30%, introduction of an additional scattering factor associated with interface nitridation compensates for the moderate amount of thermally generated mobile carriers at high temperatures, indicating a fundamental drawback of nitridation of SiO2/SiC interfaces. On the basis of these findings, we discuss the channel conduction mechanisms of SiC MOSFETs.


2013 ◽  
Vol 1517 ◽  
Author(s):  
P. Koželj ◽  
S. Jazbec ◽  
J. Dolinšek

ABSTRACTThe δ-FeZn10 phase possesses high structural complexity typical of complex metallic alloys: a giant unit cell comprising 556 atoms, polyhedral atomic order with icosahedrally-coordinated environments, fractionally occupied lattice sites and statistically disordered atomic clusters that introduce intrinsic disorder into the structure. The electrical resistivity is large and exhibits a maximum at about 220 K. The magnetoresistance is sizeable, amounting to 1.5 % at 2 K in 9 T field. The temperature–dependent resistivity is discussed within the frame of the theory of slow charge carriers, applicable to metallic systems with weak dispersion of the electronic bands, where the electron motion changes from ballistic to diffusive upon heating. A comparison to the theory of weak localization is also made.


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