Interactions in Quantum Lifshitz Criticality
Examining how particle interactions affect topological chains at critical points.
― 5 min read
Table of Contents
- The Importance of Interactions
- Theoretical Background
- The Lifshitz Critical Point
- Lattice Models and Theoretical Approaches
- Renormalization Group Analysis
- Numerical Simulations and Predictions
- Phenomena of Entanglement
- Collective Modes and Energy Spectrum
- Conclusion and Future Directions
- Original Source
- Reference Links
Quantum Lifshitz criticality is a concept in physics that deals with how certain materials behave near a transition point where they change from one state to another. This article explores the effects of Interactions in topological chains, which are special arrangements of particles that have unique surface properties. We look at how these interactions can significantly influence the critical points of these systems.
The Importance of Interactions
Interactions between particles play a crucial role in determining the behavior of materials at low temperatures. In our study, we find that when particles in a topological chain repel each other, they lead to a new state where the system behaves like a conformal invariant. In this state, low-energy excitations, or disturbances, do not have a gap, allowing them to move freely.
Conversely, when particles attract each other, they stabilize the state of the system, creating low-energy excitations that act almost like free particles. The balance between these interactions is vital for maintaining the stability of the system, which is affected by strong quantum fluctuations.
Theoretical Background
In physics, we often study the behavior of materials in terms of field theories. In lower dimensions, such theories can display complex behaviors due to the limitations in how particles can interact. For example, in two-dimensional systems, certain fluctuations can destroy long-range order, which is why understanding these fluctuations is essential.
A significant part of the work on quantum criticality is based on conformal field theories, which are effective in explaining many phenomena. However, Lifshitz criticalities represent a different situation since they do not follow the same symmetry rules.
The Lifshitz Critical Point
The Lifshitz critical point is characterized by specific scaling behaviors and is particularly relevant in systems like topological chains or atom arrangements. At this point, the behavior of the material can change dramatically based on how particles interact.
We address a fundamental question: what is the low-energy description of these interacting systems? We find that repulsive interactions lead to one type of critical behavior, while attractive interactions lead to another.
Lattice Models and Theoretical Approaches
To study the Lifshitz criticality, we use models based on the Su–Schrieffer–Heeger (SSH) framework. This model helps us simplify complex interactions and allows for a better understanding of how particles behave at the critical point.
The equations involved help express how these interactions function, focusing on the energy levels of the system. By analyzing these levels, we can gain insights into the collective behaviors of particles when they interact.
Renormalization Group Analysis
The renormalization group (RG) approach is a tool used to study how a system's properties change at different energy scales. In this analysis, we look at how interactions evolve as energy scales change, which is crucial for understanding the stability of the state near the Lifshitz critical point.
By employing this technique, we can track how the effective interactions vary, determine how close the system is to the critical point, and what behaviors emerge as we change the interactions.
Numerical Simulations and Predictions
To validate our theoretical predictions, we conduct numerical simulations. These simulations provide insights into how the interactions affect the system. They confirm that positive interactions lure the system into a different universality class while negative interactions can maintain stability.
The results highlight distinct behaviors based on the type of interaction. For example, when observing the Entanglement Entropy, we notice that positive interactions lead to rapid changes, signaling a phase transition, while negative interactions indicate a more stable state.
Phenomena of Entanglement
Entanglement entropy plays a significant role in understanding the behavior of quantum systems. It reflects the amount of information that is shared between different parts of the system. Our findings indicate that entanglement behaves differently depending on whether the interactions are positive or negative.
For positive interactions, we observe a quick increase in entropy, signifying complex changes in the system's state. In contrast, for negative interactions, the entropy remains more stable, suggesting that the system's excitations do not undergo as much change.
Collective Modes and Energy Spectrum
We explore the energy levels of collective modes, which describe how groups of particles behave together. The analysis reveals that these modes can exhibit a range of behaviors based on the interactions present.
Near the Lifshitz critical point, we find that the spectrum remains gapless, indicating that there are still available energy states for excitations. This characteristic is essential for understanding the low-energy physics of the system, particularly as the system's size varies.
Conclusion and Future Directions
The study of quantum Lifshitz criticality in interacting topological chains reveals that interactions are fundamental to the stability and behavior of these systems. Repulsive interactions can lead to new quantum states, while attractive interactions help maintain stability.
Looking ahead, additional research could explore how these systems behave in more dimensions or under different types of interactions. Investigating the role of long-range interactions or other perturbations may also provide further insights into the complex world of quantum criticality.
In summary, understanding how interactions influence Lifshitz criticality not only deepens our knowledge of condensed matter physics but also opens doors to exploring new materials and their potential applications in technology.
Title: Quantum $z=2$ Lifshitz criticality in one-dimensional interacting fermions
Abstract: We consider Lifshitz criticality (LC) with the dynamical critical exponent $z=2$ in one-dimensional interacting fermions with a filled Dirac Sea. We report that interactions have crucial effects on Lifshitz criticality. Single particle excitations are destabilized by interaction and decay into the particle-hole continuum, which is reflected in the logarithmic divergence in the imaginary part of one-loop self-energy. We show that the system is sensitive to the sign of interaction. Random-phase approximation (RPA) shows that the collective particle-hole excitations emerge only when the interaction is repulsive. The dispersion of collective modes is gapless and linear. If the interaction is attractive, the one-loop renormalization group (RG) shows that there may exist a stable RG fixed point described by two coupling constants. We also show that the on-site interaction (without any other perturbations at the UV scale) would always turn on the relevant velocity perturbation to the quadratic Lagrangian in the RG flow, driving the system flow to the conformal-invariant criticality. In the numerical simulations of the lattice model at the half-filling, we find that, for either on-site positive or negative interactions, the dynamical critical exponent becomes $z=1$ in the infrared (IR) limit and the entanglement entropy is a logarithmic function of the system size $L$. The work paves the way to study one-dimensional interacting LCs.
Authors: Ke Wang
Last Update: 2023-07-29 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2302.13243
Source PDF: https://arxiv.org/pdf/2302.13243
Licence: https://creativecommons.org/licenses/by/4.0/
Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.
Thank you to arxiv for use of its open access interoperability.