Abstract:Based on a phenomenological model with competing spin-density-wave (SDW) and extended s-wave superconductivity, the vortex states in Ba(1-x)K(x)Fe2As2 are investigated by solving Bogoliubov-de Gennes equations. Our result for the optimally doped compound without induced SDW is in qualitative agreement with recent scanning tunneling microscopy experiment. We also propose that the main effect of the SDW on the vortex states is to reduce the intensity of the in-gap peak in the local density of states and transfer… Show more
“…In the presence of an applied magnetic field, our calculations show that the spatial variation of the s ± order parameter is similar to that obtained in Ref. 15 (not shown here). Figure 1(a) shows the zero-energy (ZE) LDOS in real space and the position of the sites [V: (16,16), S: (32, 16), C: (32, 0)] where we calculate ρ i (ω) and T −1 1 (i).…”
Section: Resultssupporting
confidence: 89%
“…15, we conclude that the existence of this peak is robust since the magnetic field is about B = 23 Tesla in Ref. 15. The robustness of the peak has also been verified by STM experiment conducted at magnetic fields of 4 and 9 Tesla.…”
Section: Resultssupporting
confidence: 69%
“…By comparing with Ref. 15, we conclude that the existence of this peak is robust since the magnetic field is about B = 23 Tesla in Ref. 15.…”
Section: Resultssupporting
confidence: 50%
“…The reason we adopt this model is its ability 12 to qualitatively account for the doping evolution of the FS as observed by ARPES 13 on the K-and Co-doped 122-family of the iron pnictides. More importantly, based on this model, the existence of the negative-energy (NE) ingap peak in the local density of states (LDOS) at the vortex core center observed by scanning tunneling spectroscopy (STM) 14 has been successfully explained, 15 all justifying the validity of this model. In the presence of a magnetic field B perpendicular to the plane, the hopping integral can be expressed as t …”
Based on a phenomenological model with s± or s-wave pairing symmetry, the spatially resolved nuclear magnetic resonance (NMR) relaxation rate in the iron pnictides is investigated by solving Bogoliubov-de Gennes equations. Taking into account the presence of a magnetic field, our result for the s± pairing is in qualitative agreement with recent NMR experiments, while for the s-wave pairing, a coherence peak shows up right below Tc in apparent contradiction with experimental observations, thus excluding the s-wave pairing. We also propose that the spin-lattice relaxation rate (SLRR) should follow an exponential relation when the temperature is lowered below T /Tc ≈ 0.1 down to 0.01. It is noted that the SLRR cannot be entirely determined by the local density of states; the mixed state effect and multiorbital physics must be considered.
“…In the presence of an applied magnetic field, our calculations show that the spatial variation of the s ± order parameter is similar to that obtained in Ref. 15 (not shown here). Figure 1(a) shows the zero-energy (ZE) LDOS in real space and the position of the sites [V: (16,16), S: (32, 16), C: (32, 0)] where we calculate ρ i (ω) and T −1 1 (i).…”
Section: Resultssupporting
confidence: 89%
“…15, we conclude that the existence of this peak is robust since the magnetic field is about B = 23 Tesla in Ref. 15. The robustness of the peak has also been verified by STM experiment conducted at magnetic fields of 4 and 9 Tesla.…”
Section: Resultssupporting
confidence: 69%
“…By comparing with Ref. 15, we conclude that the existence of this peak is robust since the magnetic field is about B = 23 Tesla in Ref. 15.…”
Section: Resultssupporting
confidence: 50%
“…The reason we adopt this model is its ability 12 to qualitatively account for the doping evolution of the FS as observed by ARPES 13 on the K-and Co-doped 122-family of the iron pnictides. More importantly, based on this model, the existence of the negative-energy (NE) ingap peak in the local density of states (LDOS) at the vortex core center observed by scanning tunneling spectroscopy (STM) 14 has been successfully explained, 15 all justifying the validity of this model. In the presence of a magnetic field B perpendicular to the plane, the hopping integral can be expressed as t …”
Based on a phenomenological model with s± or s-wave pairing symmetry, the spatially resolved nuclear magnetic resonance (NMR) relaxation rate in the iron pnictides is investigated by solving Bogoliubov-de Gennes equations. Taking into account the presence of a magnetic field, our result for the s± pairing is in qualitative agreement with recent NMR experiments, while for the s-wave pairing, a coherence peak shows up right below Tc in apparent contradiction with experimental observations, thus excluding the s-wave pairing. We also propose that the spin-lattice relaxation rate (SLRR) should follow an exponential relation when the temperature is lowered below T /Tc ≈ 0.1 down to 0.01. It is noted that the SLRR cannot be entirely determined by the local density of states; the mixed state effect and multiorbital physics must be considered.
“…We use a two-orbital four-band phenomenological model [15,24,25,26,27,28,29,30] [31,32,33,34,35,36]. The obtained results are consistent with the ARPES [37], neutron scattering [38] experiments.…”
Effects of disorder on electron-doped iron pnictides are investigated systematically based on self-consistent Bogoliubov-de Gennes equations. Multiply impurities with same scattering potential (SP) are randomly distributed in a square lattice. Probability distribution functions of normalized order parameters for different impurity concentrations δ imp , different electron doping concentrations δ are investigated for given SPs. Samples are found to be very robust against weak SP, in which order parameters do not have qualitative change even at very large δ imp . While strong SP is able to easily break down the order parameters. For moderate SP, variations of order parameters on and around impurities strongly depend on δ, however the distribution functions of normalized order parameters have similar behavior as δ imp increases. Compared with superconducting (SC) order, the magnetic order is more sensitive to multi-impurity effect. The spatial spin density wave pattern has already been destroyed before the system loses its superconductivity. Dependence of SC order on temperature is similar to that of impurity-free case, with the critical temperature being remarkably suppressed for high δ imp .
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