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A concrete and experimentally feasible example for testing the putative Majorana zero energy state bound in a vortex is theoretically proposed for a parallel plate geometry of superfluid $^3$He-A phase.
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The following GL parameters are used: α 0 = 3.81 × 10 50 [ J − 1 m − 3 ] \alpha_{0}=3.81\times 10^{50}[J^{-1}m^{-3}] , β 1 = − 3.75 × 10 99 [ J − 3 m − 3 ] \beta_{1}=-3.75\times 10^{99}[J^{-3}m^{-3}] , β 2 = 6.65 × 10 99 [ J − 3 m − 3 ] \beta_{2}=6.65\times 10^{99}[J^{-3}m^{-3}] , β 3 = 6.56 × 10 99 [ J − 3 m − 3 ] \beta_{3}=6.56\times 10^{99}[J^{-3}m^{-3}] , β 4 = 5.99 × 10 99 [ J − 3 m − 3 ] \beta_{4}=5.99\times 10^{99}[J^{-3}m^{-3}] , β 5 = − 8.53 × 10 99 [ J − 3 m − 3 ] \beta_{5}=-8.53\times 10^{99}[J^{-3}m^{-3}] , 2 m 3 / ℏ = 9.51 × 10 7 [ m − 2 s ] . 2m_{3}/\hbar=9.51\times 10^{7}[m^{-2}s]
Cited in the paper.
T. Mizushima et al
Cited in the paper.
“Ettore Majorana”
2006
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N.B. Kopnin and M.M. Salomaa, Phys. Rev. B 44
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Sr 2 RuO 4 , often refereed to as a chiral p p -wave superconductor, is re-examined critically in K. Machida and M. Ichioka, Phys. Rev. B 77
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Closest in time.
M. Yamashita, K. Izumina, A. Matsubara, Y. Sasaki, O. Ishikawa, T. Takagi, M. Kubota, and T. Mizusaki, Phys. Rev. Lett. 101
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