Full-band continuum model for spin- and valley-dependent electron transport through a magnetic barrier; analytical matching of eigenspinors across regions and numerical evaluation of transmission and conductance.
Settings
systemmonolayer MoS₂
regions3
valleysK, K'
band gap eV1.8
spin channelsup, down
barrier width nm10, 15, 20, 30
magnetic barriertwo closely spaced delta-function-like magnetic fields
magnetic field T0.1, 0.2, 0.3, 0.4
incident energy eV2, 2.5
fermi velocity m per s530,000
conductance calculationangular integration over transmission probability
spin orbit splitting eV0.082
incident angle range deg-60, 60
transverse momentum ky nm inv0.5
Conditions
model parameters:{"mass_term_eV":1.8,"fermi_velocity_m_per_s":530000,"spin_orbit_coupling_eV":0.082}
magnetic barrier geometry:{"width_L_nm":"variable","field_profile":"B(x)=BlB[delta(x)-delta(x-L)]"}
Full-band continuum model for spin- and valley-dependent electron transport through a magnetic barrier; analytical matching of eigenspinors across regions and numerical evaluation of transmission and conductance.
Settings
systemmonolayer MoS₂
regions3
valleysK, K'
band gap eV1.8
spin channelsup, down
barrier width nm10, 15, 20, 30
magnetic barriertwo closely spaced delta-function-like magnetic fields
magnetic field T0.1, 0.2, 0.3, 0.4
incident energy eV2, 2.5
fermi velocity m per s530,000
conductance calculationangular integration over transmission probability
spin orbit splitting eV0.082
incident angle range deg-60, 60
transverse momentum ky nm inv0.5
Conditions
model parameters:{"mass_term_eV":1.8,"fermi_velocity_m_per_s":530000,"spin_orbit_coupling_eV":0.082}
magnetic barrier geometry:{"width_L_nm":"variable","field_profile":"B(x)=BlB[delta(x)-delta(x-L)]"}
Full-band continuum model for spin- and valley-dependent electron transport through a magnetic barrier; analytical matching of eigenspinors across regions and numerical evaluation of transmission and conductance.
Settings
systemmonolayer MoS₂
regions3
valleysK, K'
band gap eV1.8
spin channelsup, down
barrier width nm10, 15, 20, 30
magnetic barriertwo closely spaced delta-function-like magnetic fields
magnetic field T0.1, 0.2, 0.3, 0.4
incident energy eV2, 2.5
fermi velocity m per s530,000
conductance calculationangular integration over transmission probability
spin orbit splitting eV0.082
incident angle range deg-60, 60
transverse momentum ky nm inv0.5
Conditions
model parameters:{"mass_term_eV":1.8,"fermi_velocity_m_per_s":530000,"spin_orbit_coupling_eV":0.082}
magnetic barrier geometry:{"width_L_nm":"variable","field_profile":"B(x)=BlB[delta(x)-delta(x-L)]"}
Full-band continuum model for spin- and valley-dependent electron transport through a magnetic barrier; analytical matching of eigenspinors across regions and numerical evaluation of transmission and conductance.
Settings
systemmonolayer MoS₂
regions3
valleysK, K'
band gap eV1.8
spin channelsup, down
barrier width nm10, 15, 20, 30
magnetic barriertwo closely spaced delta-function-like magnetic fields
magnetic field T0.1, 0.2, 0.3, 0.4
incident energy eV2, 2.5
fermi velocity m per s530,000
conductance calculationangular integration over transmission probability
spin orbit splitting eV0.082
incident angle range deg-60, 60
transverse momentum ky nm inv0.5
Conditions
model parameters:{"mass_term_eV":1.8,"fermi_velocity_m_per_s":530000,"spin_orbit_coupling_eV":0.082}
magnetic barrier geometry:{"width_L_nm":"variable","field_profile":"B(x)=BlB[delta(x)-delta(x-L)]"}