Measurement of microwave magnetic field in free space using the Rabi frequency

Author(s):  
Moto Kinoshita ◽  
Masanori Ishii
2018 ◽  
Vol 89 (6) ◽  
pp. 063104 ◽  
Author(s):  
Xiaochi Liu ◽  
Zhiyuan Jiang ◽  
Jifeng Qu ◽  
Dong Hou ◽  
Xianhe Huang ◽  
...  

Sensors ◽  
2018 ◽  
Vol 18 (10) ◽  
pp. 3288 ◽  
Author(s):  
Hao Shi ◽  
Jie Ma ◽  
Xiaofeng Li ◽  
Jie Liu ◽  
Chao Li ◽  
...  

In this paper, a quantum-based method for measuring the microwave magnetic field in free space is presented by exploring atomic Rabi resonance in the clock transition of 133Cs. A compact cesium glass cell serving as the microwave magnetic field sensing head was used to measure the spatial distribution of microwave radiation from an open-ended waveguide antenna. The measured microwave magnetic field was not restricted by other microwave devices. The longitudinal distribution of the magnetic field was measured. The experimental results measured by the sensor were in agreement with the simulation. In addition, a slightly electromagnetic perturbation caused by the glass cell was investigated through simulation calculations.


2000 ◽  
Vol 28 (3) ◽  
pp. 472-477 ◽  
Author(s):  
M. Kristiansen ◽  
L.L. Hatfield ◽  
H. Krompholz ◽  
J. Dickens ◽  
A.A. Neuber ◽  
...  

2018 ◽  
Vol 113 (16) ◽  
pp. 164101 ◽  
Author(s):  
Fuyu Sun ◽  
Zhiyuan Jiang ◽  
Jifeng Qu ◽  
Zhenfei Song ◽  
Jie Ma ◽  
...  

1994 ◽  
Vol 16 (10-11) ◽  
pp. 1889-1894
Author(s):  
A. Agliolo Gallitto ◽  
I. Ciccarello ◽  
M. Guccione ◽  
M. Li Vigni ◽  
M. R. Trunin

2015 ◽  
Vol 735 ◽  
pp. 278-281
Author(s):  
Yi Lung Then ◽  
Kok Yeow You ◽  
Mohamad Ngasri Dimon ◽  
Wei Ying Lai

Microstrip ring resonator (MRR) sensor was modeled by simple equivalent lumped element circuits in free space based on simulation data obtained from Microwave Office (AWR) simulator and comparison was made with the measurements using the E5071C Network Analyzer. The calculated reflection coefficient, |G| and complex input impedanceZinusing lumped element model were compared with the measurements results. Both results showed well agreement with a little discrepancy, basically due to imperfect soldering. The MRR was designed to have operating frequencies between 0.5 GHz and 4.5 GHz. The maximum surrounding of magnetic field,Hϕis within 15 A/m in free space.


Author(s):  
Subhajit Karmakar ◽  
Ravi Varshney ◽  
Dibakar Roy Chowdhury

Abstract Optically thin metasurfaces operating at sub-skin depth thicknesses are intriguing because of its associated low plasmonic losses (compared to optically thick, beyond skin-depth metasurfaces). However, their applicability has been restricted largely because of reduced free space coupling with incident radiations resulting in limited electromagnetic responses. To overcome such limitations, we propose enhancement of effective responses (resonances) in sub-skin depth metasurfaces through incorporation of magneto-transport (Giant Magneto Resistance, GMR) concept. Here, we experimentally demonstrate dynamic magnetic modulation of structurally asymmetric metasurfaces (consisting of superlattice arrangement of thin (~ 10 nm each) magnetic (Ni)/ nonmagnetic (Al) layers) operating at terahertz (THz) domain. With increasing magnetic field (applied from 0 to 30 mT approximately, implies increasing superlattice conductivity), we observe stronger confinement of electromagnetic energy at the resonances (both in dipole and Fano modes). Therefore, this study introduces unique magnetically reconfigurable ability in Fano resonant THz metamaterials, which directly improves its performances operating in the sub-skin depth regime. Our study can be explained by spin-dependent terahertz magneto-transport phenomena in metals and can stimulate the paradigm for on-chip spin-based photonic technology enabling dynamic magnetic control over compact, sub-wavelength, sub-skin depth metadevices.


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