paint-brush
Exploring Gauge-Higgs Inflation with Extra Dimensions: U(1) Gauge Theory on a Warped Backgroundby@phenomenology

Exploring Gauge-Higgs Inflation with Extra Dimensions: U(1) Gauge Theory on a Warped Background

by Phenomenology Technology
Phenomenology Technology HackerNoon profile picture

Phenomenology Technology

@phenomenology

Phenomenology explores the depths of consciousness, fostering a deeper understanding...

June 5th, 2024
Read on Terminal Reader
Read this story in a terminal
Print this story
Read this story w/o Javascript
Read this story w/o Javascript
tldt arrow

Too Long; Didn't Read

This paper is available on arxiv.org/abs/2403.01705 under CC BY 4.0 DEED license. We introduce both M and c in a general standpoint, and we will see that c. (y) is forbidden by imposing specific boundary conditions on fields.
featured image - Exploring Gauge-Higgs Inflation with Extra Dimensions: U(1) Gauge Theory on a Warped Background
1x
Read by Dr. One voice-avatar

Listen to this story

Phenomenology Technology HackerNoon profile picture
Phenomenology Technology

Phenomenology Technology

@phenomenology

Phenomenology explores the depths of consciousness, fostering a deeper understanding of the world.

Learn More
LEARN MORE ABOUT @PHENOMENOLOGY'S
EXPERTISE AND PLACE ON THE INTERNET.
0-item

STORY’S CREDIBILITY

Academic Research Paper

Academic Research Paper

Part of HackerNoon's growing list of open-source research papers, promoting free access to academic material.

Authors:

(1) Toshiki Kawai, Department of Physics, Hokkaido University, Sapporo 060-0810, Japan (E-mail: t-kawai@higgs3.sci.hokudai.ac.jp);

(2) Yoshiharu Kawamura, Department of Physics, Shinshu University, Matsumoto 390-8621, Japan (E-mail: haru@azusa.shinshu-u.ac.jp).

Abstract and 1 Introduction

2 U(1) gauge theory on a warped background

3 Gauge-Higgs inflation on a warped background

4 Conclusions and discussions, Acknowledgements, and References

2 U(1) gauge theory on a warped background

2.1 Randall-Sundrum metric and action integral

The spacetime is assumed to be 5d one with the RS metric given by [8, 9]


image

2.2 Conjugate boundary conditions

image


where β is a constant called a twisted phase, the superscript C denotes a 4d charge conjugation, θC is a real number, and the asterisk means the complex conjugation. Then, the covariant derivatives obey the relations:


image

2.3 Mass spectrum

image


Then, the action integral is rewritten as


image


image


image

2.4 Effective potential

Let us derive the effective potential for the Wilson line phase θ(= θ(x)). Taking the standard procedure, a d-dimensional effective potential involving one degree of freedom at the one-loop level is given b


image


image


This paper is available on arxiv under CC BY 4.0 DEED license.


[3] We introduce both Mψ and cσ′ (y) in a general standpoint, and we will see that cσ′ (y) is forbidden by imposing specific boundary conditions on fields in the next subsection.

L O A D I N G
. . . comments & more!

About Author

Phenomenology Technology HackerNoon profile picture
Phenomenology Technology@phenomenology
Phenomenology explores the depths of consciousness, fostering a deeper understanding of the world.

TOPICS

THIS ARTICLE WAS FEATURED IN...

Permanent on Arweave
Read on Terminal Reader
Read this story in a terminal
 Terminal
Read this story w/o Javascript
Read this story w/o Javascript
 Lite
X REMOVE AD