This study demonstrates how p-brane propagation in effective field theory reveals intricate phase structures and implications of higher-form global symmetries.
A bstract We study phases and propagation of closed p -brane within the framework of effective field theory with higher-form global symmetries, i.e., brane-field theory . We extend our previous studies by including the kinetic term of the center-of-mass motion as well as the kinetic term for the relative motions constructed by the area derivatives. This inclusion gives rise to another scalar Nambu-Goldstone mode in the broken phase, enriching the phase structures of p -brane. For example, when the higher-form global symmetries are discrete ones, we show that the low-energy effective theory in the broken phase is described by a topological field theory of the axion φ ( X ) and p -form field A p ( X ) with multiple (emergent) higher-form global symmetries. After the mean-field analysis, we investigate the propagation of p -brane in the present framework. We find the (functional) plane-wave solutions for the kinetic terms and derive a path-integral representation of the brane propagator. This representation motivates us to study the brane propagation within the Born-Oppenheimer approximation, where the volume of p -brane is treated as constant. In the volume-less limit (i.e. point-particle limit), the propagator reduces to the ordinary propagator of relativistic particle, whereas it describes the propagation of the area elements in the large-volume limit. Correspondingly, it is shown that the Hausdorff dimension of p -brane varies from 2 to 2( p + 1) as we increase the p -brane volume within the Born-Oppenheimer approximation. Although these results are quite intriguing, we also point out that the Born-Oppenheimer approximation is invalid in the point-particle limit, highlighting the quantum nature of p -brane as an extended object in spacetime.
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Kiyoharu Kawana (2025) studied this question.
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