Home Productsgroup the following into metal semi metal and in pakistan

group the following into metal semi metal and in pakistan

Semiconductive metal chalcogenides of the type Cu3 VS4 and

Novel semiconductive tertiary and higher order type copper-Group V transition metal chalcogenides having useful broad-band photoconductive properties are

of three-component fermions in the topological semimetal

2017629-characterized by the symmorphic space group (the bands along Γ–A reconstruct into two non-Dirac semimetal and topological phase tran

for Weyl fermions in a canonical heavy-fermion semimetal

2018115-We report evidence for Weyl fermions in the heavy fermion semimetal YbPtBiwhich will each split into a Weyl node and a trivial crossing i

Topological semimetal in honeycomb lattice LnSI-

2017922-(TI), nodal-line semimetal, and a novel semimetal phase consisting of WNs and nodal lines, which is discussed for the first time in condense

and dynamical mass generation in Dirac semimetal ZrTe5 |

2016812-dynamical mass generation in Dirac semimetal ZrTe5the system into the ultra-quantum limit, where c=1.37 nm and a space group of Cmcm

Group News – Nanomaterials and Device Labora-

At the critical field of this band inversion, the material becomes a Dirac semimetal with anisotropic dispersion, linear in armchair and quadratic in

fermion and nodal line semimetal states in half-metallic

20161215-semimetal states in the ferromagnetic half-metal into 2D (monolayer), the anomalous Hall (FCC) lattice with the space group Fm−3m (

of negative longitudinal magnetoresistance in semimetal-

Recent observations of negative longitudinal magnetoresistance in semimetal,chiral anomaly;;magnetoresi stance;;Weyl semimetal;;Dirac semimetal,The discovery

Carbon‐Tailored Semimetal MoP as an Efficient Hydrogen

201152-We investigate novel phases that emerge from the interplay of electron correlations and strong spin-orbit interactions. We focus on describi

Dirac semimetal in β-CuI without surface Fermi arcs | PNAS

2018814-In such a fermiological Dirac semimetal, the into closed Fermi surfaces, yielding a state we with the space group R3¯m is shown in Fig

Double Andreev Reflections in Type-II Weyl Semimetal-

in the Weyl semimetalband tilting direction, which is similar to the one specular AR and one retro-AR, into one retro AR and one normal ref

A stable three-dimensional topological Dirac semimetal Cd3As2

2014525-Conventionally, band theory classifies materials into insulators and metals the non-trivial topology of the band structure in semimetal a

LaO$_{1-x}$F$_x$FeAs an antiferromagnetic semimetal_

2018223-group Fmm and experiences an antiferromagnetic phase transition at 23.4 K. and compensated semimetal, in which the total carrier concentr

Chiral magnetoresistance in the Weyl semimetal NbP |

201736-The band touching points in a Weyl semimetal –in a tetragonal lattice (space group I41md) ofinto account, and a breakdown of chiral s

of Weyl orbit and quantum Hall effect in Dirac semimetal

2017112-Evolution of Weyl orbit and quantum Hall effect in Dirac semimetal CdOur results call for further investigations into the exotic quantum

Prediction of Weyl semimetal and antiferromagnetic

201937-To obtain the best experience, we recommend you use a more up to date of Weyl semimetal and antiferromagnetic topological insulator phase

Tunable double-Weyl Fermion semimetal state in the SrSi 2

2018712-Weyl node, WSMs are classified into two types. The transitional-metal monophosphides (TaAs, TaP,a topological semimetal and a fully ga

[1708.04080] Robustness of the semimetal state of Na3Bi and

Abstract: We study the excitonic semimetal-insulator quantum phase transition in three-dimensional Dirac semimetal in which the fermion dispersion is strongly

Singular Berry Curvature in a Weyl Semimetal.pdf_

2016129-symmetry breaking and structural phase transition in type-II Weyl semimetal predicted in the orthorhombic (Td) phase of WTe2 with space g

Dirac Semimetal and Quantum Transports in Cd3As2_

2015924-Dirac and Weyl Semimetal in XYBi (X = split the Dirac point into pairs of Weyl pointshexagonal ZrBeSi type structure with space grou

Weyl–Kondo semimetal in heavy-fermion systems | PNAS

201812-the local moments into quasiparticles that can The Weyl semimetal in three dimensions (3D) wasis enforced by its space-group symmetry (25)

Structural semiconductor-to-semimetal phase transition in two

2016212-in group V TMDs (TaSe2 and TaS2) utilizing anthe semiconductor-to-semimetal phase transition inThe phase change does not enter into th


20181022-Chern semi-metal and Quantized Anomalous Hall Effect in HgCr2Se4where the gap must be closed, resulting in a Chern semi-metal state

and structure transition in Weyl semimetal TaP under

2017121-superconductivity and Majorana fermions in Weyl 4,5 When the Weyl semimetal falls into TaP adopts I41 md space group at ambient

Symmetry-protected ideal Weyl semimetal in HgTe-class

201641-and they always appear in pairs of opposite HgTe turns into the ideal Weyl semimetal phase.zinc-blende structure with the space group (Fig

CaTe: a new topological node-line and Dirac semimetal

2017123-Combining first-principles calculations and effective model analysis, we predict that CaTe is a topological node-line semimetal in the absen