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Optomechanical realization of the bosonic Kitaev chain
The fermionic Kitaev chain is a canonical model featuring topological Majorana zero modes
1 . We report the experimental realization of its bosonic...
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Background: Quadratic Bosonic Hamiltonians
We present the foundational aspects of time-independent, quadratic bosonic systems. Following a brief description of the multimode bosonic landscape...
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Non-Lorentzian IIB supergravity from a polynomial realization of SL(2, ℝ)
We derive the action and symmetries of the bosonic sector of non-Lorentzian IIB supergravity by taking the non-relativistic string limit. We find...
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Efficient bosonic nonlinear phase gates
Continuous-variable (CV) quantum information processing harnesses versatile experimental tools that leverage the power of infinite-dimensional...
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Nonlinear bosonic Maxwell’s demon by coupling to qubits
The concept of Maxwell’s demon, proposed in classical physics as a means to extract work from a thermodynamics system beyond the constraints set by...
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Quantum simulation of the bosonic Kitaev chain
Superconducting quantum circuits are a natural platform for quantum simulations of a wide variety of important lattice models describing topological...
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Realization of a bosonic antiferromagnet
Quantum antiferromagnets are of broad interest in condensed-matter physics as they provide a platform for studying exotic many-body states
1 including...
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Collisionally stable gas of bosonic dipolar ground-state molecules
Stable ultracold ensembles of dipolar molecules hold great promise for studies of many-body quantum physics, but high inelastic loss rates have been...
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Bosonic near-CFT1 models from Fock-space fluxes
We construct a family of near-CFT 1 models with a conserved U(1) charge, whose basic degrees of freedom are canonical bosons. The Sachdev-Ye-Kitaev...
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Universal control of a bosonic mode via drive-activated native cubic interactions
Linear bosonic modes offer a hardware-efficient alternative for quantum information processing but require access to some nonlinearity for universal...
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Nearly degenerate ground states of a checkerboard antiferromagnet and their bosonic interpretation
The spin-1/2 model system with antiferromagnetic (AF) couplings on a J 1 - J 2 checkerboard lattice, known as the planar pyrochlore model, is strongly...
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Effective interactions of the open bosonic string via field theory
We describe a method to extract an effective Lagrangian description for open bosonic strings, at zero transcendentality. The method relies on a...
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Background: Quadratic Bosonic Lindbladians
This chapter provides an extension of Chap. 2 to the Markovian setting. We first introduce the basic...
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Collective Excitation of Bosonic Quantum Hall State
The recent developments in the theory of rapidly rotating Bose atoms have been reviewed in this article. Rotation leads to the development of...
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Many-body bound states and induced interactions of charged impurities in a bosonic bath
Induced interactions and bound states of charge carriers immersed in a quantum medium are crucial for the investigation of quantum transport....
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Acoustic realization of projective mirror Chern insulators
Symmetry plays a key role in classifying topological phases. Recent theory shows that in the presence of gauge fields, the algebraic structure of...
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Empowering a qudit-based quantum processor by traversing the dual bosonic ladder
High-dimensional quantum information processing has emerged as a promising avenue to transcend hardware limitations and advance the frontiers of...
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Nonlinear Realization of Spacetime Symmetry
The first step towards an effective field theory for spontaneously broken spacetime symmetry is the construction of the nonlinear realization of the...
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Realization of a fractional quantum Hall state with ultracold atoms
Strongly interacting topological matter
1 exhibits fundamentally new phenomena with potential applications in quantum information technology2 ,3 ....
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Quantum Speed Limit Time of Topological Qubits Influenced by the Fermionic and Bosonic Environments
Quantum theory sets a bound on the minimum time required to transform from an initial state to a target state. The bound is known as quantum speed...
