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Bulletin of the American Physical Society

Many-body physics of plane-polarized dipoles in a quasi-1D zigzag chain

Niraj Ghimire, Susanne F. Yelin

Published May 31, 2018• 0 citations
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Finding frustrations and topological phases in a quasi-1D zig-zag chain of dipoles

Niraj Ghimire, Susanne F. Yelin

Bulletin of the American Physical Society•Jun 6, 2017•0 citations

Quantum Phases of Externally In-Plane Polarized Hard-Core Dipoles on a Zig-Zag Chain

Qingyang Wang, Johanes Otterbach, Susanne F. Yelin

Bulletin of the American Physical Society•May 24, 2016•0 citations

Study of dipolar many-body system in a one-dimensional zig-zag chain

Niraj Ghimire, Susanne F. Yelin

Bulletin of the American Physical Society•May 26, 2016•0 citations

Density Matrix Renormalization Group Studies of Interacting Dipoles in a Zigzag Chain

Niraj Ghimire

In this dissertation, we study the many-body effects of dipoles in a quasi-one-dimensional zigzag optical lattice, which we call the zigzag chain. We study this system using the Density Matrix Renormalization Group (DMRG) method, which has established itself as the most powerful numerical method to simulate one-dimensional lattices. For the implementation of DMRG, we have used the open-source package Intelligent Tensor, or simply ITensor. The first part of this research focuses on dipoles polarized in the plane of the zigzag chain by an external electric field with the condition that the dipoles can hop around and interact with their first and second neighbors and the number of dipoles is exactly a half of the number of lattice sites. With the interactions much stronger than the hopping, the system comprises of frustrated and non-frustrated regimes owing to the combination of attractive and repulsive interactions in different directions. The consequence is a complex phase diagram featuring the trivial ferromagnetic and antiferromagnetic phases as well as the non-trivial dimerized and superfluid phases. The second part of the research deals with randomly oriented dipoles in the zigzag chain such that each lattice site has exactly one dipole and each dipole interacts with its first and second neighbors but in the absence of any hopping. We study the second system classically allowing many different orientations for each dipole in a lattice site as well as quantum mechanically by allowing a few quantized degrees of freedom to each dipole. The result is a phase diagram showing ferromagnetic, antiferromagnetic and paramagnetic phases.

•Jan 1, 2019•0 citations

Frustrated plane-polarized dipoles in one dimension

Niraj Ghimire, Susanne F. Yelin

We investigate the zero-temperature quantum phases of a quasi-one-dimensional zigzag chain of dipoles that are polarized in a plane by an external electric field. Since the Hamiltonian contains nearest-neighbor and next-nearest-neighbor hopping and interaction terms, this model allows frustration, which induces phases that can be interesting and unusual. By using the density matrix renormalization group algorithm, we produce a complex phase diagram. This is an extension of an earlier work by Wang et al. [Phys. Rev. A 96, 043615 (2017)].

arXiv:1810.00646•Physical review. B./Physical review. B•Sep 5, 2019•0 citations

Many-body correlations in a one-dimensional spin chain with simplified dipole-dipole interactions

A. Cidrim, Tommaso Macrì, Ana María Rey +1 more

Bulletin of the American Physical Society•May 30, 2019•0 citations
In this dissertation, we study the many-body effects of dipoles in a quasi-one-dimensional zigzag optical lattice, which we call the zigzag chain. We study this system using the Density Matrix Renormalization Group (DMRG) method, which has established itself as the most powerful numerical method to simulate one-dimensional lattices. For the implementation of DMRG, we have used the open-source package Intelligent Tensor, or simply ITensor. The first part of this research focuses on dipoles polarized in the plane of the zigzag chain by an external electric field with the condition that the dipoles can hop around and interact with their first and second neighbors and the number of dipoles is exactly a half of the number of lattice sites. With the interactions much stronger than the hopping, the system comprises of frustrated and non-frustrated regimes owing to the combination of attractive and repulsive interactions in different directions. The consequence is a complex phase diagram featuring the trivial ferromagnetic and antiferromagnetic phases as well as the non-trivial dimerized and superfluid phases. The second part of the research deals with randomly oriented dipoles in the zigzag chain such that each lattice site has exactly one dipole and each dipole interacts with its first and second neighbors but in the absence of any hopping. We study the second system classically allowing many different orientations for each dipole in a lattice site as well as quantum mechanically by allowing a few quantized degrees of freedom to each dipole. The result is a phase diagram showing ferromagnetic, antiferromagnetic and paramagnetic phases.
We investigate the zero-temperature quantum phases of a quasi-one-dimensional zigzag chain of dipoles that are polarized in a plane by an external electric field. Since the Hamiltonian contains nearest-neighbor and next-nearest-neighbor hopping and interaction terms, this model allows frustration, which induces phases that can be interesting and unusual. By using the density matrix renormalization group algorithm, we produce a complex phase diagram. This is an extension of an earlier work by Wang et al. [Phys. Rev. A 96, 043615 (2017)].