Science Advances

Supplementary Materials

This PDF file includes:

  • Appendix A. 3D TB model of FeTexSe1−x.
  • Appendix B. Simulation details.
  • Appendix C. Particle-hole symmetry broken by Majorana hybridization.
  • Appendix D. Simulation for a moving vortex.
  • Appendix E. STM measurement of creeping vortex and vortex relocation.
  • Appendix F. Simulation for LDOS line profiles of ZBP and non-ZBP vortices.
  • Appendix G. Inhomogeneous superconducting gaps and chemical potentials.
  • Appendix H. ZBP heights.
  • Fig. S1. The line profile of the Majorana wave function.
  • Fig. S2. The system size of the 3D TB model for the simulation.
  • Fig. S3. The TB simulation without magnet flux.
  • Fig. S4. FWHM of the tunneling peaks in the STM experiment (9).
  • Fig. S5. The angles and phases for a point near vortex.
  • Fig. S6. The LDOS changes with R¯v=46.5 nm corresponding to B = 1 T before and after the central vortex α moves 14 nm down.
  • Fig. S7. The LDOS changes with R¯v = 33 nm corresponding to B = 2 T before and after the central vortex α moves 14 nm down.
  • Fig. S8. Time dependence measurements on a creeping vortex in B = 4 T with averaged intervortex distance R¯v23nm.
  • Fig. S9. The tunneling spectra before and after the vortex relocation in the same FOV.
  • Fig. S10. (Spin) LDOS line profiles of the two selected vortices.
  • Fig. S11. Inhomogeneous superconducting gaps for triangular vortex lattice with intervortex distances.
  • Fig. S12. Inhomogeneous chemical potentials for triangular vortex lattice with intervortex distances.
  • Fig. S13. ZBP heights from the simulation and the STM experiment in different magnetic fields.
  • References (4246)

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