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Quantum Coherence and Lorentz Boosts: A Key Connection

Explore how Lorentz boosts affect quantum coherence in various particles.

― 5 min read


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Table of Contents

Quantum Coherence is a unique property of quantum systems that differs from classical systems. In simple terms, coherence refers to how well the quantum state of a system can maintain its specific properties, such as phase relationships, over time. This property is important for various applications, especially in quantum information science, where coherent states can be used for tasks like quantum computing, cryptography, and more.

Understanding Quantum States

In quantum physics, a quantum state describes the full set of information about a system. It can represent various physical quantities, such as position, Momentum, and spin. One common way to represent a quantum state is using a wave function, which provides a probability distribution of finding a particle in a certain state.

What is Lorentz Boost?

Lorentz boost is a concept from the theory of relativity that describes how the measurements of time and space change for observers moving at different speeds, particularly those close to the speed of light. When an observer moves relative to another, the way they perceive events, distances, and times will differ due to the effects of relativity.

Why Combine These Concepts?

When we look at quantum systems, especially those that can be entangled (where two particles are linked in a way that the state of one can affect the state of another), it's crucial to understand how such states behave under various conditions. Specifically, how these states of quantum coherence change when viewed from different inertial frames, or when subjected to Lorentz Boosts.

Effects of Lorentz Boost on Quantum States

When a quantum state is subjected to a Lorentz boost, the properties that describe it can change. This shift can affect both the momentum and spin of the particles involved. For instance, imagine a spinning particle moving at a high speed; its properties will be perceived differently by observers who are stationary compared to those moving close to the speed of light.

The Role of Momentum

Momentum refers to the quantity of motion an object has. In quantum mechanics, studying how momentum interacts with quantum states can reveal information about how coherent states behave under boosts. Observers moving at different speeds will measure different values for momentum, affecting the overall coherence of the state.

Measuring Quantum Coherence

There are several ways to measure quantum coherence. One widely used method is the Frobenius-norm measure of coherence. This approach looks at the Density Matrix, which contains all the information about a quantum system. The measure quantifies how much a quantum state can be said to retain its coherence after undergoing various transformations, including those from Lorentz boosts.

Analysis of Quantum States with Lorentz Boosts

In studies involving quantum coherence and Lorentz boosts, researchers often focus on specific types of particles. For example, particles can be light, such as electrons, or heavier particles such as neutrons. These particles will respond differently to changes in momentum and spin when they experience Lorentz boosts.

What Happens to Coherence?

When a particle experiences a Lorentz boost, the coherence of its quantum state typically decreases. This decay in coherence can be attributed to the increased momentum of the particle. Observations show that electrons, being much lighter than neutrons, demonstrate a more significant loss of coherence when undergoing boosts.

The Mass Factor

The mass of a particle plays a crucial role in its behavior under Lorentz boosts. Lighter particles (like electrons) show a more pronounced decay in coherence compared to heavier particles (like neutrons) when exposed to similar conditions. This phenomenon is vital for understanding how different types of particles maintain coherence in various situations.

Visualizing the Results

Researchers often represent their findings using graphs and plots. By plotting coherence levels against different parameters, such as the width of the wave function and the boost parameters, one can visualize how coherence changes.

Electron vs. Neutron Coherence

In experimental results, the behavior of electrons can be contrasted with that of neutrons. While both types of particles undergo coherence loss due to Lorentz boosts, electrons typically experience a more substantial decrease. The visual representations of these findings help clarify the differences in behavior between light and heavy particles.

Implications of Quantum Coherence Loss

The loss of quantum coherence has significant implications for various fields, especially quantum information theory. When coherence is lost, the ability to perform certain quantum tasks can degrade. This has direct consequences in fields like quantum computing, where maintaining coherence is crucial for effective operation.

Importance in Real-World Applications

The effects of Lorentz boosts on quantum coherence are not just theoretical. They have practical implications for technologies that rely on quantum states. For example, in quantum teleportation or quantum cryptography, maintaining coherence is essential for the reliability of these processes.

Summary of Key Points

  1. Quantum coherence is essential for the functionality of various quantum systems.
  2. Lorentz boosts illustrate how different observers measure time and space differently, depending on their speed.
  3. The coherence of quantum states typically decreases under Lorentz boosts, especially for lighter particles like electrons.
  4. The decay in coherence can significantly affect the performance of quantum applications.
  5. Visual representation of results aids in understanding complex behaviors under different conditions.

Conclusion

Quantum coherence and Lorentz boosts are interconnected concepts that provide valuable insights into the behavior of quantum systems. Understanding how coherence changes with boosts is essential for advancing quantum technologies and unraveling the mysteries of particle behavior in relativistic physics. As research progresses, it will continue to illuminate the fascinating relationship between quantum mechanics and the effects of relativity, paving the way for future developments in both fields.

Original Source

Title: Quantum coherence measures for generalized Gaussian wave packets under a Lorentz boost

Abstract: In this paper we consider a single particle, spin-momentum entangled state and measure the effect of relativistic boost on quantum coherence. The effect of the relativistic boost on single-particle generalized Gaussian wave packets is studied. The coherence of the wave function as measured by the boosted observer is studied as a function of the momentum and the boost parameter. Using various formulations of coherence, it is shown that in general the coherence decays with the increase in momentum of the state, as well as the boost applied to it. A more prominent loss of coherence due to relativistic boost is observed for a single particle electron than that of a neutron. The analysis is carried out with generalized Gaussian wave packet of the form $\mathcal{N} p^n \exp(-\frac{p^2}{\sigma^2})$ with $n$ being the ``generalization parameter" and $\mathcal{N}$ denoting the appropriate normalization constant. We also obtain a range for parameter $n$ appearing in the wave packet. The upper bound is found to have a dependence on the mass of the particle and the width of the Gaussian wave packet. We have obtained the Frobenius-norm measure of coherence, $l_1$ and $l_2$ norm measure of coherence, and relative entropy of coherence for a (1+1) and (3+1)-dimensional analysis. Corresponding to each of the cases, we observe that the $l_1$ norm measure of coherence is equal to the Frobenius norm measure of coherence. We have analyzed the scenario for which such a beautiful coincidence can occur. Finally, we have plotted different measures of coherence for the electron as well as the neutron for different values of the width of the wave-function $\sigma$, boost parameter $\beta$, and generalization parameter $n$.

Authors: Arnab Mukherjee, Soham Sen, Sunandan Gangopadhyay

Last Update: 2024-11-13 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2407.06599

Source PDF: https://arxiv.org/pdf/2407.06599

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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