Thermal Noise Defies Expectations in Quantum Materials
New insights reveal thermal noise increases in certain low-temperature materials under light.
Longjun Xiang, Lei Zhang, Jun Chen, Fuming Xu, Yadong Wei, Jian Wang
― 7 min read
Table of Contents
- Thermal Noise in Electrical Currents
- The Role of Light and Photocurrents
- Quantum Materials and Their Peculiarity
- A Surprising Connection to Quantum Metrics
- The Nature of Anomalous DTN
- How Does It All Work?
- Comparing to Mesoscopic Conductors
- The Noise Spectrum
- Experimental Outlook
- Conclusion
- Original Source
- Reference Links
In the world of physics, there are many curious phenomena that scientists strive to understand. One of these peculiarities is the behavior of Thermal Noise in electric currents. Traditionally, thermal noise is believed to increase with temperature. Essentially, when things heat up, particles jiggle more, and thus create more noise. Conversely, it’s generally accepted that when you cool things down to absolute zero, the noise should vanish into thin air. But, oh boy, the universe loves to throw a curveball now and then!
Recently, researchers have stumbled upon an unexpected twist in this tale. It turns out that in specific materials, particularly those that interact with light, thermal noise doesn't just hang around at low temperatures; it actually becomes stronger. Yep, you heard that right! Instead of fading away, this peculiar thermal noise decides to party on, defying all conventional wisdom.
Thermal Noise in Electrical Currents
First off, let’s break down what thermal noise is. When things get warm, the tiny particles that make up materials-like electrons in metals-start to dance around more energetically. This frenetic activity generates what is known as Johnson-Nyquist noise, or thermal noise. It's like the sound of a lively party happening in a room full of people who can’t stop moving.
At low temperatures, one would expect this noise to die down as the energy of the particles decreases. In most scenarios, when the temperature approaches zero, the dance slows down, and the noise diminishes. But here’s where the plot thickens: in certain Quantum Materials, particularly those influenced by light, thermal noise sticks around and even grows stronger as temperatures drop. Who would have thought that noise would be so rude?
Photocurrents
The Role of Light andWhen light interacts with materials, it can excite the electrons, pushing them into a state where they can flow freely and create what we call photocurrents. Think of photocurrents as the electric signals generated when light shines on a surface-like turning on a lightbulb when you flick the switch.
Now, in some of these quantum materials, it appears that thermal noise behaves differently. Instead of fading away, it shows a wild resurgence, especially in what scientists call resonant DC thermal noise (DTN). This DTN doesn't just sit there; it actively interacts with the light, leading to a unique kind of noise that had previously gone unnoticed.
Quantum Materials and Their Peculiarity
What’s so special about the materials we’re talking about? Well, these are known as quantum materials, which exhibit unusual properties due to the quantum mechanics that govern their behavior. Imagine if your favorite superheroes had special powers; these materials have their own quirks.
Take graphene, for instance. This two-dimensional material made up of a single layer of carbon atoms has remarkable electrical properties. It's as if it has super-speed. In addition to graphene, there are three-dimensional topological insulators and Weyl semimetals, all showcasing odd behavior when it comes to electric currents and noise. The connection to quantum metrics, a fancy term for the properties that describe how these materials respond to various influences, makes them even more fascinating.
A Surprising Connection to Quantum Metrics
The intriguing behavior of this thermal noise anomaly has a strong link to something called the quantum metric. So, what in the world is that? It essentially describes how the states of electrons in these materials change when influenced by external factors like electric or magnetic fields.
Think of quantum metrics as the rules of engagement for our superhero materials. They dictate how the electrons behave under various conditions and how this behavior can lead to noise when the materials are subjected to light. This unexpected relationship opens up a whole new avenue of exploration in the field of quantum physics.
The Nature of Anomalous DTN
Now, let’s focus on the key player in our story: the anomalous DTN. This form of noise is not just an annoying background sound; it has characteristics that set it apart from the typical thermal noise seen in everyday materials. This anomalous DTN can cause greater fluctuations in the electrical signals coming from these quantum materials, which could lead to innovative applications in future technologies.
What's more, the relationship between light and the Fermi surface-the area where the electrons behave differently-further fuels the strength of this peculiar DTN. The Fermi surface acts like a dance floor for electrons, and the new types of noise are related to how they move and interact with each other once the lights come on, so to speak.
How Does It All Work?
The process behind this intriguing phenomenon is quite elaborate. When light hits these materials, it creates conditions that are very different from our usual understanding of thermal noise. The interplay between the light and the electrons near the Fermi surface creates a unique situation that allows the DTN to flourish.
The dance of the electrons, when combined with the effects of light, generates a noise that does not merely diminish at low temperatures. Instead, it exhibits peaks at certain frequencies, depending on the light and chemical properties of the materials involved. It's as if the electrons found a new rhythm that didn't exist before.
Comparing to Mesoscopic Conductors
As if things weren't busy enough, let's introduce another player: mesoscopic conductors. These materials are interesting because they exist between the macro and micro worlds, showing phenomena that are influenced by both. In mesoscopic systems, thermal noise typically takes a backseat to shot noise, which is largely driven by the quantization of charge.
However, with the emergence of this anomalous DTN in quantum materials, the balance of noise sources shifts. No longer can we say that shot noise is always the loudest sound in the room. Instead, the anomalous DTN becomes a worthy contender that works in harmony-or perhaps competition-with shot noise. Suddenly, the music at the party sounds different, and everyone is paying attention.
Noise Spectrum
TheAs the temperature dips and light continues to play its role, the impact of both the anomalous DTN and shot noise can be seen in the noise spectrum. This spectrum represents the characteristics of noise produced by various sources within the material.
Researchers have found that at low temperatures, the total noise brought on by both contributions peaks at specific frequencies. This means that the interaction between light, the quantum metric, and the unique properties of the materials all converge to produce a monumental moment in the noise game.
Experimental Outlook
So, how do researchers put these ideas to the test? One exciting avenue is through the use of advanced techniques like scanning noise microscopy, which can provide insights into these quantum phenomena without needing to introduce additional materials that could interfere with the results. It's like having a superhero who can see the invisible!
Experimental validation of these findings could lead to groundbreaking applications in electronic devices, communication technologies, and energy systems. Imagine a future where your gadgets can communicate more efficiently thanks to an understanding of these quantum noise properties!
Conclusion
The exploration of thermal noise and its unexpected behavior in quantum materials under the influence of light marks a significant leap in our comprehension of physics. This anomaly, particularly in the context of resonant DC thermal noise, challenges long-held beliefs and opens the door to numerous possibilities. The interplay between light, quantum metrics, and unique material properties presents a tantalizing puzzle waiting to be further explored.
In essence, the world of physics thrives on surprises. Just when you think you've got it all figured out, nature pulls out a little trick to keep you on your toes. As we move forward, these revelations promise to unlock new horizons in technology, reshaping how we understand and manipulate the world around us. And who knows, maybe one day, we’ll all be dancing to the rhythm of quantum noise!
Title: Light-induced thermal noise \textit{anomaly} governed by quantum metric
Abstract: Traditionally, thermal noise in electric currents, arising from thermal agitation, is expected to increase with temperature $T$ and disappear as $T$ approaches zero. Contrary to this expectation, we discover that the resonant DC thermal noise (DTN) in photocurrents not only persists at $T=0$ but also exhibits a divergence proportional to $1/T$. This thermal noise \textit{anomaly} arises from the unique electron-photon interactions near the Fermi surface, manifesting as the interplay between the inherent Fermi-surface property and the resonant optical selection rules of DTN, and thereby represents an unexplored noise regime. Notably, we reveal that this \textit{anomalous} DTN, especially in time-reversal-invariant systems, is intrinsically linked to the quantum metric. We illustrate this \textit{anomalous} DTN in massless Dirac materials, including two-dimensional graphene, the surfaces of three-dimensional topological insulators, and three-dimensional Weyl semimetals, where the quantum metric plays a pivotal role. Finally, we find that the total noise spectrum at low temperatures, which includes both the DC shot noise and the \textit{anomalous} DTN, will universally peak at $\omega_p=2|\mu|$ with $\omega_p$ the frequency of light and $\mu$ the chemical potential of the bulk crystals.
Authors: Longjun Xiang, Lei Zhang, Jun Chen, Fuming Xu, Yadong Wei, Jian Wang
Last Update: Dec 17, 2024
Language: English
Source URL: https://arxiv.org/abs/2412.12662
Source PDF: https://arxiv.org/pdf/2412.12662
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.
Reference Links
- https://doi.org/10.1016/S0370-1573
- https://doi.org/10.1063/1.1583532
- https://doi.org/10.1103/PhysRev.32.110
- https://doi.org/10.1103/PhysRevB.87.245103
- https://doi.org/10.1103/PhysRevLett.130.036202
- https://doi.org/10.1103/PhysRevLett.121.267401
- https://doi.org/10.1038/s41467-024-46264-1
- https://doi.org/10.1103/PhysRevLett.127.277201
- https://doi.org/10.1103/PhysRevLett.127.277202
- https://doi.org/10.1126/science.adf1506
- https://doi.org/10.1038/s41586-023-06363-3
- https://doi.org/10.1103/PhysRevLett.132.106601
- https://doi.org/10.1103/PhysRevB.109.075419
- https://doi.org/10.1038/s41567-024-02476-2
- https://doi.org/10.1103/PhysRevB.110.245406
- https://doi.org/10.1126/science.1102896
- https://doi.org/10.1038/nature04235
- https://doi.org/10.1038/nmat1849
- https://doi.org/10.1103/PhysRevLett.99.236809
- https://doi.org/10.1038/nphys1270
- https://doi.org/10.1103/PhysRevB.82.045122
- https://doi.org/10.1103/PhysRevLett.103.266801
- https://doi.org/10.1103/RevModPhys.82.3045
- https://doi.org/10.1103/RevModPhys.83.1057
- https://doi.org/10.1038/nature08916
- https://doi.org/10.1103/RevModPhys.90.015001
- https://doi.org/10.1103/RevModPhys.93.025002
- https://doi.org/10.1146/annurev-conmatphys-031016-025458
- https://doi.org/10.1103/PhysRevLett.93.206602
- https://doi.org/10.1103/PhysRevB.61.5337
- https://doi.org/10.1103/RevModPhys.82.1959
- https://doi.org/10.1126/sciadv.1501524
- https://doi.org/10.1146/annurev-conmatphys-031113-133841
- https://doi.org/10.1038/s41524-020-00462-9
- https://doi.org/10.1038/ncomms14176
- https://doi.org/10.1103/PhysRevLett.131.240001
- https://doi.org/10.1038/s41467-018-05137-0
- https://doi.org/10.1126/science.aam9991
- https://doi.org/10.1038/s41467-021-25094-5
- https://doi.org/10.1063/1.2221541
- https://doi.org/10.1063/5.0078917