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  1. No, if you want to have a 1D defect in $d$ spatial dimensions, you need $\pi_{d-2} (M)$ to be nontrivial.

  2. The fact that your Lagrangian has nontrivial $\pi_{1} (M)$ implies, when extended to 4 spatial dimensions, that there are 2D defects.

AMENDED to address OP's follow-up question:

  1. If you want a 1D defect in 4 spatial dimensions, you need to use a model that yields a nontrivial $\pi_{2} (M)$ (which would yield a 0D defect in 3 spatial dimensions, such as a magnetic monopole). Typically you'd use something with an internal $SU(2)$ symmetry, see for example this discussion.
  1. No, if you want to have a 1D defect in $d$ spatial dimensions, you need $\pi_{d-2} (M)$ to be nontrivial.

  2. The fact that your Lagrangian has nontrivial $\pi_{1} (M)$ implies, when extended to 4 spatial dimensions, that there are 2D defects.

  1. No, if you want to have a 1D defect in $d$ spatial dimensions, you need $\pi_{d-2} (M)$ to be nontrivial.

  2. The fact that your Lagrangian has nontrivial $\pi_{1} (M)$ implies, when extended to 4 spatial dimensions, that there are 2D defects.

AMENDED to address OP's follow-up question:

  1. If you want a 1D defect in 4 spatial dimensions, you need to use a model that yields a nontrivial $\pi_{2} (M)$ (which would yield a 0D defect in 3 spatial dimensions, such as a magnetic monopole). Typically you'd use something with an internal $SU(2)$ symmetry, see for example this discussion.
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  1. No, if you want to have a 1D defect in $d$ spatial dimensions, you need $\pi_{d-2} (M)$ to be nontrivial.

  2. The fact that your Lagrangian has nontrivial $\pi_{1} (M)$ implies, when extended to 4 spatial dimensions, that there are 2D defects.