This week

In this talk, I will briefly describe two of our recent pieces of work on the physics of the J1-J2 Heisenberg spin chain, a one-dimensional array of quantum spins coupled by first- and second-neighbour exchange interactions. The first piece of work [1] concerns the case where J1 and J2 are both antiferromagnetic: in this case there is a phase transition from a Luttinger liquid to a valence bond solid as In this talk, I will briefly describe two of our recent pieces of work on the physics of the J1-J2 Heisenberg spin chain, a one-dimensional array of quantum spins coupled by first- and second-neighbour exchange interactions. The first piece of work [1] concerns the case where J1 and J2 are both antiferromagnetic: in this case there is a phase transition from a Luttinger liquid to a valence bond solid as J2/J1 In this talk, I will briefly describe two of our recent pieces of work on the physics of the J1-J2 Heisenberg spin chain, a one-dimensional array of quantum spins coupled by fi rst- and second-neighbour exchange interactions. The first piece of work [1] concerns the case where J1 and J2 are both antiferromagnetic: in this case there is a phase transition from a Luttinger liquid to a valence bond solid as J2/J1 is increased, and we provide a novel direct method to derive the field theory that describes the critical point between these two phases. The second piece [2] concerns the case where J1 is antiferromagnetic but J2 is strongly ferromagnetic: counter-intuitively, there is a transition in this case as well, but this time of a "liquid-to-liquid" type. We present a field-theory description of it, and an analogue system of three coupled chains that helps to illustrate the physics. [1] F. Azad, A. J. McRoberts, CAH, and A. G. Green, "Generalized Haldane map from the matrix product state path integral to the critical theory of the J1-J2 chain," Phys. Rev. Research 7, L012037 (2025). [2] A. J. McRoberts, CAH, and A. G. Green, "Transition between critical antiferromagnetic phases in the J1-J2 spin chain," arXiv:2411.08095v2 (2025).

I will review the basic story behind the black hole/string correspondence, its advantages, and its limits. I will then summarize some recent progress on this topic and go over several possible open directions.