# Accelerated Detector Response Function in Squeezed Vacuum

## Abstract

**:**

## 1. Introduction

## 2. Simple Quantum Field Theory in Squeezed Vacuum

## 3. Accelerated Frames

## 4. Detector Response Function

- When the detector’s acceleration is ($a\le {\xi}^{\prime}$) The poles all lie in the upper half, therefore the integral vanishes and thereby the transition probability is vanishing . Hence, particle creation is not observed.
- Moreover, for ($a>{\xi}^{\prime}$ ) The poles lie in the lower half, therefore we can sum the resides and have the following transition probability:$$P={g}^{2}\sum _{E}\left(\right)open="("\; close=")">\frac{|\langle E|\widehat{\mu}|{E}_{0}{\rangle |}^{2}}{{e}^{2\pi \varpi (E-{E}_{0})}-1}$$

## 5. Discussion

## 6. Conclusions

## Acknowledgments

## Conflicts of Interest

## References

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**Figure 1.**Rindler wedge with the dashed lines resembles the “modifeid” horizons due to modifying the vacuum, and immersing the new geometry in flat spacetime. The new horizons are spread by an angle ${tan}^{-1}\frac{b}{3}$ each, corresponding to a superluminal photon propagation.

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Alsaleh, S.
Accelerated Detector Response Function in Squeezed Vacuum. *Technologies* **2017**, *5*, 17.
https://doi.org/10.3390/technologies5020017

**AMA Style**

Alsaleh S.
Accelerated Detector Response Function in Squeezed Vacuum. *Technologies*. 2017; 5(2):17.
https://doi.org/10.3390/technologies5020017

**Chicago/Turabian Style**

Alsaleh, Salwa.
2017. "Accelerated Detector Response Function in Squeezed Vacuum" *Technologies* 5, no. 2: 17.
https://doi.org/10.3390/technologies5020017