sagnac phase
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2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Yehoshua Winsten ◽  
Doron Cohen

AbstractQuasi-static protocols for systems that feature a mixed phase-space with both chaos and quasi-regular regions are beyond the standard paradigm of adiabatic processes. We focus on many-body system of atoms that are described by the Bose–Hubbard Hamiltonian, specifically a circuit that consists of bosonic sites. We consider a sweep process: slow variation of the rotation frequency of the device (time dependent Sagnac phase). The parametric variation of phase-space topology implies that the quasi-static limit is not compatible with linear response theory. Detailed analysis is essential in order to determine the outcome of such transfer protocol, and its efficiency.


2020 ◽  
Vol 17 (09) ◽  
pp. 2050128
Author(s):  
E. Benedetto ◽  
F. Feleppa ◽  
G. Iovane ◽  
E. Laserra

In this paper, some analogies between the Shapiro effect in the solar gravitational field and the Sagnac phase shift have been found. Starting from Einstein equivalence principle (EEP), which states the equivalence between the gravitational force and the pseudo-force experienced by an observer in a noninertial frame of reference, we imagine an observer on a rotating platform immersed in a gravitational field. In the Shapiro effect, for example, we know that the speed of an electromagnetic signal, calculated from the Earth, is less than [Formula: see text], but, if we calculate the speed using a clock at rest in the solar gravitational field, where the photon is passing, we get that the speed of light is [Formula: see text]. Similarly, by considering the fictitious gravitational field of the rotating platform, if we look for a clock with respect to which the signal speed is [Formula: see text], we can interpret the time delay as a gravitational effect.


Sensors ◽  
2019 ◽  
Vol 19 (7) ◽  
pp. 1710 ◽  
Author(s):  
Michal Skalský ◽  
Zdeněk Havránek ◽  
Jiří Fialka

This paper presents a simple method for compensating the Sagnac phase shift in an interferometric fiber-optic gyroscope (I-FOG) with a piezoelectric modulator. The common advantages of I-FOGs with closed-loop compensation are linearized output characteristics and insensitivity to the light source power, including its time and thermal-induced fluctuations. Whereas closed-loop operation is normally achieved via ramp modulation requiring an electro-optic modulator, all-fiber architectures with a piezoelectric modulator are mostly limited to open loop. Nevertheless, such setups can more conveniently utilize a less expensive single-mode fiber with depolarized light and do not require any custom-made components. The proposed method allows us to combine the advantages of both approaches. Closed-loop compensation is ensured by adding further sinusoidal modulation to the common biasing modulation, such that the Sagnac phase shift is compensated solely at the sampling instants. We describe and experimentally demonstrate the proposed approach, utilizing a test setup to compare our closed-loop solution with open-loop operation. The results denote that the method provides a cost-efficient manner of performance improvement compared to the open-loop I-FOGs based on a piezoelectric modulator.


2009 ◽  
Vol 95 (14) ◽  
pp. 141104 ◽  
Author(s):  
Lu Yan ◽  
Zhisong Xiao ◽  
Xiaoqian Guo ◽  
Anping Huang

2008 ◽  
Vol 78 (1) ◽  
Author(s):  
Marion Jacquey ◽  
Alain Miffre ◽  
Gérard Trénec ◽  
Matthias Büchner ◽  
Jacques Vigué ◽  
...  

2000 ◽  
Vol 336 (1-2) ◽  
pp. 27-32
Author(s):  
D. Fargion ◽  
L. Chiatti ◽  
A. Aiello

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