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[PDF] Top 20 Spin dependent electron transport in semiconductors due to the Pauli principle

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Spin dependent electron transport in semiconductors due to the Pauli principle

Spin dependent electron transport in semiconductors due to the Pauli principle

... us to explore a novel charge-spin coupling mechanism which modifies electron ...of the electron gas (high concentration, low temperature), a dip at the centre of the ... Voir le document complet

172

Ab initio calculation of spin-dependent electron-phonon coupling and transport in iron and cobalt

Ab initio calculation of spin-dependent electron-phonon coupling and transport in iron and cobalt

... Introduction The coupling of electron spin and vibrations in solids has garnered renewed interest in the past decade, after a lull since the 60s and ...from the ... Voir le document complet

16

Spin-dependent transport in antiferro and ferrimagnetic nanostructures

Spin-dependent transport in antiferro and ferrimagnetic nanostructures

... ]. The working principle is explained in the text. The free layer of the magnetic element to write can be reversed by the Oersted elds generated by current pulses ... Voir le document complet

176

Spin dependent transport in antiferro and ferrimagnetic nanostructures

Spin dependent transport in antiferro and ferrimagnetic nanostructures

... ]. The working principle is explained in the text. The free layer of the magnetic element to write can be reversed by the Oersted elds generated by current pulses ... Voir le document complet

177

Spin-dependent transport in antiferromagnetic tunnel junctions

Spin-dependent transport in antiferromagnetic tunnel junctions

... the total torque of Fig. 3 gave the non-equilibrium torque represented in .... The former accounts for the Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction and is not associated with ... Voir le document complet

6

Spin-dependent diffraction at ferromagnetic/spin spiral interface

Spin-dependent diffraction at ferromagnetic/spin spiral interface

... For the numerical simulations, we took parameters corresponding to spin transport in Co: the Fermi wavevectors for majority and minority spins are respectively k ↑ F = ...; ... Voir le document complet

9

Mapping spin–charge conversion to the band structure in a topological oxide two-dimensional electron gas

Mapping spin–charge conversion to the band structure in a topological oxide two-dimensional electron gas

... for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or ...not. The documents may come from teaching and research institutions in France or abroad, or ... Voir le document complet

22

Time-dependent upregulation of electron transport with concomitant induction of regulated excitation dissipation in Haslea diatoms

Time-dependent upregulation of electron transport with concomitant induction of regulated excitation dissipation in Haslea diatoms

... grown to exponential phase under 50 µmol m −2 s −1 photosynthetic available radiation (PAR) and then exposed to non-sequential rapid light curves where, once electron transport rate (ETR) had ... Voir le document complet

13

Precision Measurement of the Neutron Spin Asymmetries and Spin-dependent Structure Functions in the Valence Quark Region

Precision Measurement of the Neutron Spin Asymmetries and Spin-dependent Structure Functions in the Valence Quark Region

... Conservation In the early 1970’s, in one of the first applications of per- turbative QCD (pQCD), it was noted that as x → 1, the scat- tering is from a high-energy quark and thus ... Voir le document complet

25

Transmission electron microscopy in situ investigation of dislocation behaviour in semiconductors and the influence of electronic excitation

Transmission electron microscopy in situ investigation of dislocation behaviour in semiconductors and the influence of electronic excitation

... of the triangle being located close to the interface; it is noteworthy that they are present only in two {111} planes with the same polarity: (111) and (1 - 1 - ...similar to ... Voir le document complet

36

Classical and quantum systems: transport due to rare events

Classical and quantum systems: transport due to rare events

... legitimate, to take for κ the conductivity computed in equilibrium as in ...polynomial in ρ, then the spreading of the wave packet must itself be slower than any power law ... Voir le document complet

24

DDFV Schemes for semiconductors energy-transport models

DDFV Schemes for semiconductors energy-transport models

... symmetrize the problem and allow to prove a priori estimates by using an entropy ...is to extend the work done in [2] to the case of general ...meshes. In order ... Voir le document complet

11

The Detectability Of Transit Depth Variations Due To Exoplanetary Oblateness And Spin Precession

The Detectability Of Transit Depth Variations Due To Exoplanetary Oblateness And Spin Precession

... course the identification of a single optimal period is a simplification. The existence and observability of T δVs and TDVs depends on the particular mass and radius of the planet under ... Voir le document complet

9

Numerical schemes for semiconductors energy- transport models

Numerical schemes for semiconductors energy- transport models

... Schemes in primal and dual entropy variables Our aim is to design a scheme for the energy transport model in the primal entropy variables ...lead to an equivalent scheme ... Voir le document complet

16

Impact of electron-electron interactions induced by disorder at interfaces on spin-dependent tunneling in Co-Fe-B/MgO/Co-Fe-B magnetic tunnel junctions

Impact of electron-electron interactions induced by disorder at interfaces on spin-dependent tunneling in Co-Fe-B/MgO/Co-Fe-B magnetic tunnel junctions

... presence in our tunnel barrier. This analysis based on transport measurements is supported by x-ray pho- toemission spectroscopy 共XPS兲 analysis made on our samples in order to determine their ... Voir le document complet

5

About the Dedekind psi function in Pauli graphs

About the Dedekind psi function in Pauli graphs

... on the projective line P 1 (Z q ) (in the Dedekind finction ψ(q), the product is taken over all primes p dividing q) and the remaining σ(q) − ψ(q) 6= 0 independent points (with σ(q) ... Voir le document complet

13

Off-line algorithm for calculation of vertical tracer transport in the troposphere due to deep convection

Off-line algorithm for calculation of vertical tracer transport in the troposphere due to deep convection

... itations in this approach: (1) tracer transport cannot proceed unmixed through more than one vertical grid cell per time step in penetrative cumulus; (2) the fluxes in opposite di- ... Voir le document complet

23

Gate control of the electron spin-diffusion length in semiconductor quantum wells

Gate control of the electron spin-diffusion length in semiconductor quantum wells

... of the Dresselhaus and Rashba coefficients in GaAs vary strongly, ranging from |g| ¼ 3 to 35 eV Å 3 for Dresselhaus 29,31–35 and r 41 from 5–10 e Å 2 for Rashba 13,29,36 ...of the techniques ... Voir le document complet

6

Response functions of semiconductors and insulators : from the Bethe-Salpeter equation to time-dependent density functional theory

Response functions of semiconductors and insulators : from the Bethe-Salpeter equation to time-dependent density functional theory

... Introduction The electronic structure of semiconductors and insulators is well described by reliable ab inito methods [41, 42, 159, ...compared to ex- periment ...example in Fig. 3.V, where ... Voir le document complet

198

Quantitative Transmission Electron Microscopy Study of III-Nitrides Semiconductors Nanostructures

Quantitative Transmission Electron Microscopy Study of III-Nitrides Semiconductors Nanostructures

... In fact, if specimen thicknesses or microscope defocuses slightly differ from the approved values (Table III-2 and Table III-3), the HRTEM images do not immediately become inappropriate for ... Voir le document complet

191

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