Regulation of the thermopower and ultrasound by magnetic field in manganese sulfide doped with variable-valence ions

[1]  L. Udod,et al.  Phase transitions in a polycrystalline compound Ho0.1Mn0·9S , 2023, Solid State Communications.

[2]  C. Felser,et al.  Ultrahigh transverse thermoelectric power factor in flexible Weyl semimetal WTe2 , 2022, Nature Communications.

[3]  O. Tschauner.  An Observation Related to the Pressure Dependence of Ionic Radii , 2022, Geosciences.

[4]  O. Romanova,et al.  Electrosound and asymmetry of the I‒V characteristic induced by ultrasound in the RexMn1−xS (Re = Tm, Yb) , 2022, The European Physical Journal Plus.

[5]  Farheen F Jaldurgam,et al.  Low-Toxic, Earth-Abundant Nanostructured Materials for Thermoelectric Applications , 2021, Nanomaterials.

[6]  W. Ernst,et al.  Origin of the Electron–Phonon Interaction of Topological Semimetal Surfaces Measured with Helium Atom Scattering , 2020, The journal of physical chemistry letters.

[7]  L. Udod,et al.  Phase transitions in bismuth pyrostannate upon substitution of tin by iron ions , 2019, Journal of Alloys and Compounds.

[8]  A. Powell.  Recent developments in Earth-abundant copper-sulfide thermoelectric materials , 2019, Journal of Applied Physics.

[9]  Y. Okamoto,et al.  Giant isotropic negative thermal expansion in Y-doped samarium monosulfides by intra-atomic charge transfer , 2019, Scientific Reports.

[10]  Masaaki Tanaka,et al.  Giant gate-controlled proximity magnetoresistance in semiconductor-based ferromagnetic–non-magnetic bilayers , 2018, Nature Physics.

[11]  P. Smet,et al.  Samarium Monosulfide (SmS): Reviewing Properties and Applications , 2017, Materials.

[12]  Y. Okamoto,et al.  Colossal negative thermal expansion in reduced layered ruthenate , 2017, Nature Communications.

[13]  A. Szczerbakow,et al.  Nernst-Ettingshausen effect at the trivial-nontrivial band ordering in topological crystalline insulator Pb1−xSnxSe , 2015, 1509.07052.

[14]  G. J. Snyder,et al.  High thermoelectric and mechanical performance in highly dense Cu2−xS bulks prepared by a melt-solidification technique , 2015 .

[15]  A. Nenashev,et al.  Large positive magnetoresistance effects in the dilute magnetic semiconductor (Zn,Mn)Se in the regime of electron hopping , 2014 .

[16]  Dezheng Yang,et al.  A Large Magnetoresistance Effect in p–n Junction Devices by the Space‐Charge Effect , 2013 .

[17]  M. Gorev,et al.  Magnetic and thermophysical properties of GdXMn1−XS solid solutions , 2013, Journal of physics. Condensed matter : an Institute of Physics journal.

[18]  Z. Ren,et al.  Experimental realization of a topological crystalline insulator in SnTe , 2012, Nature Physics.

[19]  Xili Gao,et al.  Geometrical enhancement of low-field magnetoresistance in silicon , 2011, Nature.

[20]  K. Yanushkevich,et al.  Magnetic properties of SmxMn1−xS solid solutions , 2011 .

[21]  Y. Ihm,et al.  Magnetism in Si1 − xMnx diluted magnetic semiconductor thin films , 2009 .

[22]  M. Salamon,et al.  Magnetothermopower in La0.67Ca0.33MnO3 thin films , 1996 .

[23]  P. N. Gorley,et al.  Transverse and Longitudinal Nernst-Ettingshausen Effect in p-Te , 1978 .

[24]  J. L. Feldman.  Abstracts of articles to be published in The Journal of Physics and Chemistry of SolidsElastic constants of 2H-MoS2 and 2H-NbSe2 extracted from measured dispersion curves and linear compressibilities , 1976 .

[25]  M. A. Khan,et al.  Insight into the structural, vibrational and thermodynamic properties of SmX (X = S, Se, Te) chalcogenides: First-principles investigations , 2020 .

[26]  Maksim Yu Kagan,et al.  Inhomogeneous charge distributions and phase separation in manganites , 2001 .

[27]  R. N. Hampton,et al.  Samarium-ion valence instability in a glassy matrix , 1988 .

[28]  E. Kaldis,et al.  Valence and phase instabilities in TmSe crystals , 1982 .