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Qmechanic
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I know very simple example of anomaly inflow. See section 4.4 in David Tong: Lectures on Gauge Theory. As I read, such mechanism have some applications in condensed matter and in quantum field theory, but I haven't face with some concrete applications. What is this application?

Essence of example:

  1. One consider 5d fermion with mass term, which depends on fifth coordinate (y): $$ i\not\partial \psi + i \gamma^5 \partial_y \psi - m(y) \psi = 0 $$

  2. Exist special solution of this equation, after rewriting Dirac spinor $\psi$ as two Weyl spionors $\psi_+$ and $\psi_-$: $$ \psi_+ = \exp\left(- \int^y dy^\prime m(y^\prime) \right) \chi_+ (x) \;\;\;\;\;\;\;\;\;\; \psi_- = 0 $$ $$ \partial_0\chi_+ - \sigma^i \partial_i \chi_+ = 0 $$ The profile is supported only in the vicinity of the domain wall; it dies off exponentially $∼ e^{−M|y|}$ as $y → ±\infty$. Importantly, there is no corresponding solution for $\psi_−$, since the profile must be of the form $exp(+\int dy^\prime m(y^\prime))$which now diverges exponentially in both directions. So we obtain chiral fermion zero mode that lives on domain wall.

  3. Chiral anomaly of this zero mode cancel with 5d Chern-Simons term. So theory $$ S = S^{5d}_{CS} + S^{4d}_{chiral fermion} $$ is gauge invariant. This known as anomaly inflow.

    One consider 5d fermion with mass term, which depends on fifth coordinate (y): $$ i\not\partial \psi + i \gamma^5 \partial_y \psi - m(y) \psi = 0 $$

  1. Exist special solution of this equation, after rewriting Dirac spinor $\psi$ as two Weyl spinors $\psi_+$ and $\psi_-$: $$ \psi_+ = \exp\left(- \int^y dy^\prime m(y^\prime) \right) \chi_+ (x) \;\;\;\;\;\;\;\;\;\; \psi_- = 0 $$ $$ \partial_0\chi_+ - \sigma^i \partial_i \chi_+ = 0 $$ The profile is supported only in the vicinity of the domain wall; it dies off exponentially $∼ e^{−M|y|}$ as $y → ±\infty$. Importantly, there is no corresponding solution for $\psi_−$, since the profile must be of the form $exp(+\int dy^\prime m(y^\prime))$which now diverges exponentially in both directions. So we obtain chiral fermion zero mode that lives on domain wall.

  2. Chiral anomaly of this zero mode cancel with 5d Chern-Simons term. So theory $$ S = S^{5d}_{CS} + S^{4d}_{chiral fermion} $$ is gauge invariant. This known as anomaly inflow.

I wanna to understand more examples of such phenomena.

What kind of useful information can be extracted from such mechanism?

Could we consider more exotic gauge symmetries, what kind of generalisation allow such mechanism?

Also it is related to thisthis question. As I understand, appearing of topological theory on domain walls are related to anomaly inflow in discrete symmetry. Some explanations of this phenomenona will be also appreciated!

I know very simple example of anomaly inflow. See section 4.4 in David Tong: Lectures on Gauge Theory. As I read, such mechanism have some applications in condensed matter and in quantum field theory, but I haven't face with some concrete applications. What is this application?

Essence of example:

  1. One consider 5d fermion with mass term, which depends on fifth coordinate (y): $$ i\not\partial \psi + i \gamma^5 \partial_y \psi - m(y) \psi = 0 $$

  2. Exist special solution of this equation, after rewriting Dirac spinor $\psi$ as two Weyl spionors $\psi_+$ and $\psi_-$: $$ \psi_+ = \exp\left(- \int^y dy^\prime m(y^\prime) \right) \chi_+ (x) \;\;\;\;\;\;\;\;\;\; \psi_- = 0 $$ $$ \partial_0\chi_+ - \sigma^i \partial_i \chi_+ = 0 $$ The profile is supported only in the vicinity of the domain wall; it dies off exponentially $∼ e^{−M|y|}$ as $y → ±\infty$. Importantly, there is no corresponding solution for $\psi_−$, since the profile must be of the form $exp(+\int dy^\prime m(y^\prime))$which now diverges exponentially in both directions. So we obtain chiral fermion zero mode that lives on domain wall.

  3. Chiral anomaly of this zero mode cancel with 5d Chern-Simons term. So theory $$ S = S^{5d}_{CS} + S^{4d}_{chiral fermion} $$ is gauge invariant. This known as anomaly inflow.

I wanna to understand more examples of such phenomena.

What kind of useful information can be extracted from such mechanism?

Could we consider more exotic gauge symmetries, what kind of generalisation allow such mechanism?

Also it is related to this question. As I understand, appearing of topological theory on domain walls are related to anomaly inflow in discrete symmetry. Some explanations of this phenomenona will be also appreciated!

I know very simple example of anomaly inflow. See section 4.4 in David Tong: Lectures on Gauge Theory. As I read, such mechanism have some applications in condensed matter and in quantum field theory, but I haven't face with some concrete applications. What is this application?

Essence of example:

  1. One consider 5d fermion with mass term, which depends on fifth coordinate (y): $$ i\not\partial \psi + i \gamma^5 \partial_y \psi - m(y) \psi = 0 $$

  1. Exist special solution of this equation, after rewriting Dirac spinor $\psi$ as two Weyl spinors $\psi_+$ and $\psi_-$: $$ \psi_+ = \exp\left(- \int^y dy^\prime m(y^\prime) \right) \chi_+ (x) \;\;\;\;\;\;\;\;\;\; \psi_- = 0 $$ $$ \partial_0\chi_+ - \sigma^i \partial_i \chi_+ = 0 $$ The profile is supported only in the vicinity of the domain wall; it dies off exponentially $∼ e^{−M|y|}$ as $y → ±\infty$. Importantly, there is no corresponding solution for $\psi_−$, since the profile must be of the form $exp(+\int dy^\prime m(y^\prime))$which now diverges exponentially in both directions. So we obtain chiral fermion zero mode that lives on domain wall.

  2. Chiral anomaly of this zero mode cancel with 5d Chern-Simons term. So theory $$ S = S^{5d}_{CS} + S^{4d}_{chiral fermion} $$ is gauge invariant. This known as anomaly inflow.

I wanna to understand more examples of such phenomena.

What kind of useful information can be extracted from such mechanism?

Could we consider more exotic gauge symmetries, what kind of generalisation allow such mechanism?

Also it is related to this question. As I understand, appearing of topological theory on domain walls are related to anomaly inflow in discrete symmetry. Some explanations of this phenomenona will be also appreciated!

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Nikita
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Anomaly inflow mechanism

I know very simple example of anomaly inflow. See section 4.4 in David Tong: Lectures on Gauge Theory. As I read, such mechanism have some applications in condensed matter and in quantum field theory, but I haven't face with some concrete applications. What is this application?

Essence of example:

  1. One consider 5d fermion with mass term, which depends on fifth coordinate (y): $$ i\not\partial \psi + i \gamma^5 \partial_y \psi - m(y) \psi = 0 $$

  2. Exist special solution of this equation, after rewriting Dirac spinor $\psi$ as two Weyl spionors $\psi_+$ and $\psi_-$: $$ \psi_+ = \exp\left(- \int^y dy^\prime m(y^\prime) \right) \chi_+ (x) \;\;\;\;\;\;\;\;\;\; \psi_- = 0 $$ $$ \partial_0\chi_+ - \sigma^i \partial_i \chi_+ = 0 $$ The profile is supported only in the vicinity of the domain wall; it dies off exponentially $∼ e^{−M|y|}$ as $y → ±\infty$. Importantly, there is no corresponding solution for $\psi_−$, since the profile must be of the form $exp(+\int dy^\prime m(y^\prime))$which now diverges exponentially in both directions. So we obtain chiral fermion zero mode that lives on domain wall.

  3. Chiral anomaly of this zero mode cancel with 5d Chern-Simons term. So theory $$ S = S^{5d}_{CS} + S^{4d}_{chiral fermion} $$ is gauge invariant. This known as anomaly inflow.

I wanna to understand more examples of such phenomena.

What kind of useful information can be extracted from such mechanism?

Could we consider more exotic gauge symmetries, what kind of generalisation allow such mechanism?

Also it is related to this question. As I understand, appearing of topological theory on domain walls are related to anomaly inflow in discrete symmetry. Some explanations of this phenomenona will be also appreciated!