Carrollian Conformal Scalar Theories in Physics
Study of Carrollian symmetries and their implications in modern physics.
― 6 min read
Table of Contents
- What are Carrollian Symmetries?
- Why Study Carrollian Theories?
- The Basics of Quantization
- Carrollian Theories and Their Quantization
- Understanding Correlation Functions
- Carrollian Magnetic Scalar Theory
- The Role of the Rigged Hilbert Space
- Non-Unitary Quantization Approaches
- Exploring Electric Scalars in 3D
- Conclusion: The Future of Carrollian Conformal Scalar Theories
- Original Source
Carrollian conformal scalar theories are a fascinating area of study in physics. They explore the behavior of certain fields under specific symmetry transformations known as Carrollian Symmetries. These theories have connections to both classical and modern physics concepts and can be studied in various dimensions, such as two-dimensional (2D) and three-dimensional (3D).
What are Carrollian Symmetries?
Carrollian symmetry is derived from the concept of relativity, similar to Poincaré symmetry but in a different limit. It describes how objects behave when speeds approach that of light. While Poincaré symmetry includes time and space in a particular way, Carrollian symmetry involves a unique structure where time behaves differently from space, creating a distinct framework for understanding particle dynamics.
This symmetry was explored in the 1960s by physicists seeking to understand how special relativity could lead to different behaviors under certain conditions. It allows for translations and rotations among spatial dimensions and introduces a special type of transformation called Carrollian boosts.
Why Study Carrollian Theories?
Researchers are interested in Carrollian theories because they provide insight into various fields, including gravity, cosmology, and even quantum mechanics. They offer a new way to look at complex systems and help to answer significant questions about the nature of space, time, and matter.
Carrollian symmetries can appear in various scenarios, such as when dealing with gravitational waves, fluid dynamics, and certain theoretical models involving particles that behave in non-standard ways. By studying these theories, scientists hope to uncover deeper connections between classical physics and quantum theories.
Quantization
The Basics ofIn physics, quantization is the process of turning classical fields and particles into quantum objects. This involves defining a mathematically rigorous framework through which we can describe the behavior of particles at extremely small scales. The key aspect of quantization is the creation of a Hilbert space, a mathematical space where all possible states of a system can be represented.
There are different ways to approach quantization. The best-known methods include the canonical quantization approach, which uses classical equations of motion to derive quantum mechanical rules, and path integral quantization, which involves summing over all possible paths a particle can take.
Carrollian Theories and Their Quantization
When we apply quantization to Carrollian conformal scalar theories, things can get quite interesting. These theories exist in different dimensions and can exhibit very different behaviors depending on the chosen vacuum state. The vacuum state is the lowest energy state of a quantum system and serves as the foundation for building all other states.
For Carrollian scalar theories, researchers have identified two main quantization schemes based on different vacuum states. The first involves what is known as the induced vacuum, which provides a Unitary Hilbert space, meaning that probabilities can be calculated consistently. The second scheme involves the highest-weight vacuum, which breaks this unitarity, leading to different behaviors and properties in the correlations between various states.
Correlation Functions
UnderstandingCorrelation functions serve as a crucial tool in quantum field theory. They describe how different points in a quantum field are related to one another and can be used to infer physical properties about the system being studied. In Carrollian theories, correlation functions can take on different forms depending on the quantization approach used.
In the induced vacuum scenario, correlation functions often resemble those observed in classical conformal field theories (CFT), where power laws appear in time and delta functions appear in space. On the other hand, when working with the highest-weight vacuum, correlation functions exhibit power-law forms across spatial dimensions, which can be traced back to certain limits applied to CFTs.
This distinction illuminates how different foundational choices in quantization can lead to varied physical interpretations and mathematical outcomes.
Carrollian Magnetic Scalar Theory
Focusing on the magnetic scalar theory, consider a massless Carrollian magnetic scalar field existing on a cylinder. The dynamics of this field can be described using the mathematical framework of Carrollian symmetries and quantization methods discussed previously.
The first step is to examine the BMS symmetry relevant to this theory, which involves specific transformations that preserve the symmetry of the metric and time-like vectors. These transformations can be grouped into different classes based on their properties and the equations they generate.
When we perform canonical quantization on the magnetic scalar theory, we can derive correlation functions that align with those computed through path integral techniques. This coherence among different methods strengthens our understanding and provides confidence in the mathematical foundations of Carrollian theories.
The Role of the Rigged Hilbert Space
The concept of the rigged Hilbert space plays an essential role in the quantization of Carrollian theories. This mathematical structure allows for the inclusion of states that are not strictly confined to the traditional Hilbert space. The rigged Hilbert space is composed of three spaces: the Hilbert space itself, a physical space containing states with finite expectation values, and a dual space representing generalized states.
This triplet structure is useful in dealing with the non-normalizable states found in Carrollian theories. It provides a way to discuss the canonical quantization of massless scalar fields without the restrictions imposed by conventional Hilbert spaces.
Non-Unitary Quantization Approaches
While unitary quantization ensures that probabilities remain consistent and applicable, non-unitary quantization approaches can introduce complexities that lead to interesting results. The highest-weight vacuum scheme, for example, can result in a Hilbert space that lacks unitarity, leading to states that do not adhere to conventional rules of probability.
In this setup, certain correlations may exhibit anomalous behavior, mirroring findings from 2D conformal field theory. This aspect is particularly intriguing as it challenges our understanding of how different frameworks can yield similar results under specific conditions.
Exploring Electric Scalars in 3D
Just as with the magnetic scalar theory, we can analyze electric scalar theories in a Carrollian context. Like magnetic scalars, electric scalars also exhibit interesting symmetry properties and quantization behaviors. The primary difference lies in their action and how they transform under symmetry groups.
Quantizing electric scalar theories follows a similar structure to the magnetic case, resulting in a wealth of insights into the nature of the fields involved and their interactions. The connection to the BMS symmetry remains crucial, as it informs the behavior of these fields in a Carrollian framework.
Conclusion: The Future of Carrollian Conformal Scalar Theories
The exploration of Carrollian conformal scalar theories offers a unique perspective on the nature of spacetime, symmetries, and fundamental forces. By delving into quantization approaches, correlation functions, and the intricacies of vacuum states, researchers can piece together the broader tapestry of modern physics.
As our understanding deepens, the insights gained from Carrollian theories could lead to new discoveries in gravitational physics, quantum mechanics, and potentially even cosmological models. The interplay between classical and quantum realms continues to captivate scientists, and Carrollian symmetries hold promise for future advancements in our quest to comprehend the universe.
Title: Quantization of Carrollian conformal scalar theories
Abstract: In this work, we study the quantization of Carrollian conformal scalar theories, including two-dimensional(2D) magnetic scalar and three-dimensional(3D) electric and magnetic scalars. We discuss two different quantization schemes, depending on the choice of the vacuum. We show that the standard canonical quantization corresponding to the induced vacuum yields a unitary Hilbert space and the 2-point correlation functions in this scheme match exactly with the ones computed from the path integral. In the canonical quantization, the BMS symmetry can be realized without anomaly. On the other hand, for the quantization based on the highest-weight vacuum, it does not have a unitary Hilbert space. In 2D, the correlators in the highest-weight vacuum agree with the ones obtained by taking the $c\to 0$ limit of the 2D CFT, and there is an anomalous term in the commutation relations between the Virasoso generators, whose form is similar to the one in 2D CFT. In 3D, there is no good definition of the highest-weight vacuum without breaking the rotational symmetry. In our study, we find that the usual state-operator correspondence in CFT does not hold in the Carrollian case.
Authors: Bin Chen, Haowei Sun, Yu-fan Zheng
Last Update: 2024-12-17 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2406.17451
Source PDF: https://arxiv.org/pdf/2406.17451
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.