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The Fascinating SSH Model and Zero Energy States

Discover the SSH model's role in zero energy states and quantum computing.

Surajit Mandal

― 6 min read


SSH Model and Zero Energy SSH Model and Zero Energy States through zero energy states. Exploring quantum computing potential
Table of Contents

The SSH Model is a fascinating concept in physics that originated in the study of a special kind of plastic known as polyacetylene. Imagine a row of atoms that are linked like a chain, but some links are stronger than others, almost like a seesaw. This creates a situation where there can be different energy states, depending on how the atoms are arranged.

Now, if you take a closer look at this chain and create a smaller section, you end up with two different setups. One setup has strong links (bonds) at the ends, while the other has weaker links. These setups are important because they can lead to what are called "zero energy states," which are special energy levels that occur at the boundaries of this chain.

What Are Zero Energy States?

Zero energy states, or ZES for short, are like secret hiding spots for energy in a system. They are often found at the edges of special types of materials and can be thought of as excitations within the material. These states occur when part of the chain is changed-imagine a little bump or a twist in our seesaw of atoms.

When this happens, ZESs can form at the ends of the chain or at the location of that twist or bump. These ZESs might carry a fractional charge, which means they have a bit of an unusual behavior when it comes to electricity.

The Domain Wall: A Special Feature

Now, let’s introduce the concept of a domain wall, which is like a line that divides two different regions within our atomic chain. This wall can change how the energy states behave. Picture a wall between two rooms: one is cozy and warm, and the other is cold and drafty. When you cross the wall (or in this case, the domain wall), you feel the difference immediately.

In our atomic chain, when a domain wall is placed between two different types of arrangements (or "phases"), special states called "domain wall states" appear. These are ZESs that are localized at the domain wall itself, meaning they are stuck right at the wall instead of spreading out.

Effects of Hopping Modulation

Now, if you start to mix things up a bit by changing how the atoms interact with each other (a process called "hopping modulation"), it can lead to even more interesting behavior. Hopping modulation is like adjusting how much the seesaw rocks back and forth.

Researchers discovered that when they periodically change the strength of the links between atoms, it affects the ZESs. Some states will only be found at the ends of the chain, while others will be stuck right at the domain wall. The interaction with the wall also changes depending on how smooth or sharp the wall is.

The Role of Commensurate Frequencies

When we talk about commensurate frequencies, we mean that the changes in hopping strength happen in a regular pattern. Think of it like a dance: everyone is moving in sync, making the dance look good.

By carefully choosing these patterns, researchers can create different configurations of the chain that yield different energy states. They found that with certain frequencies, one ZES would remain near the domain wall, while others would be at the endpoints of the chain.

Numerical Studies

To study these zero energy states, researchers use numerical models. This is like using a computer to simulate how the atomic chain behaves when you change certain parameters. The results often show how the ZESs shift in response to different configurations.

For instance, studies have shown that when the wall is introduced, ZESs can form at various locations depending on the frequency of hopping. It turns out that the physical setup of the wall-how sharp or smooth it is-also plays a big role in determining where these ZESs end up.

Analytical Techniques

Beyond numerical studies, researchers also use analytical methods to understand what’s happening. This involves using mathematical models to predict outcomes. It’s similar to how you might use a recipe to predict how a cake will turn out.

Using these techniques, they can analyze the properties of the ZESs and how they react to Domain Walls. By considering factors like the mass associated with the defects in the system, researchers can gain insights into how these zero-energy modes behave.

The Connection to Topological Quantum Computing

One of the most exciting aspects of these zero energy states is their potential role in the field of quantum computing. Imagine if you could build a super-fast computer that uses these special energy states to process information. Researchers believe that ZESs could be useful for creating qubits that are robust against errors, making them a great candidate for advancing quantum computing.

The fractional charges associated with these zero energy states also add a layer of complexity, opening new potential avenues for research in this field.

Observing Zero Energy States

In practice, observing ZESs can be done using advanced experimental techniques. Researchers can create environments that mimic the conditions necessary for these states to occur, allowing them to see how ZESs behave in real time.

For example, scientists could use lasers to cool down materials to very low temperatures. This creates a perfect playground to observe the peculiar behaviors of zero energy states and domain walls. By using these techniques, researchers can confirm their theoretical predictions.

Summary of Findings

The presence of domain walls, hopping modulation, and commensurate frequencies greatly influence the behavior of zero energy states in the SSH model. When researchers looked at the interactions and configurations, interesting patterns emerged:

  • ZESs can be localized at either the domain wall or the edges, depending on certain conditions.
  • The nature of the domain wall-sharp or smooth-changes the localization of these states.
  • The hopping modulation and commensurate frequencies used can drastically alter how these states are distributed within the chain.

Future Directions

Looking ahead, researchers plan to further explore how zero energy states behave under different conditions. They may investigate their properties in systems that are not yet fully understood or work on improving our ability to manipulate these states for better quantum computing applications.

The SSH model has opened the door to a range of exotic phenomena in solid-state physics, and each new discovery provides a fresh perspective on how we can use the strange behaviors of matter to our advantage.

So, who knew that a simple chain of atoms could lead to such thrilling possibilities? It seems that even at the quantum level, there’s always room for a twist!

Original Source

Title: Zero Energy States for Commensurate Hopping Modulation of a Generalized Su-Schrieffer-Heeger Chain in the Presence of a Domain Wall

Abstract: We study the effect of domain wall (DW) on zero-energy states (ZESs) in the Su-Schrieffer-Heeger (SSH) chain. The chain features two fractional ZESs in the presence of such DW, one of which is localized at the edge and the other bound at the location of DW. This zero-energy DW state exhibits interesting modifications when hopping modulation is tuned periodically. We studied the energy spectra for commensurate frequencies $\theta=\pi,\pi/2,\pi/3$ and $\pi/4$. Following the recent study by the author of this paper [S. Mandal, S. Kar, Phys. Rev. B 109, 195124 (2024)], we showed numerically, along with physical intuition, that one ZES can bound at the DW position only for commensurate frequency $\theta=\frac{\pi}{2s+1}$ for zero or an integer $s$ values, while for $\theta=\frac{\pi}{2s}$ with nonzero or an integer $s$ value they appear only at the edges of the chain. We verify our numerical results by using exact analytical techniques. Both analyses indicate the realization of the Jackiw-Rebbi modes for our model only with $\theta=\frac{\pi}{2s+1}$. Moreover, the localization of zero-energy edge and DW states are investigated which reveals their localized (extended) nature for smaller (larger) $\Delta_{0}$ (amplitude of DW). The localization of topological DW states is suppressed as the width of DW ($\xi$) increases (typically scaled as $\sim 1/\xi$) while the edge state shows an extended behavior only for the large $\xi$ limit.

Authors: Surajit Mandal

Last Update: Dec 19, 2024

Language: English

Source URL: https://arxiv.org/abs/2412.16239

Source PDF: https://arxiv.org/pdf/2412.16239

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.

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