microwave spectrometer
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2021 ◽  
Vol 16 (12) ◽  
pp. P12037
Author(s):  
P. Alonso-Arias ◽  
P.A. Fuerte-Rodríguez ◽  
R.J. Hoyland ◽  
J.A. Rubiño-Martín

Abstract The TMS optical system is based on a decentered dual-reflector system in a Gregorian configuration to observe with an angular resolution of less than 2°. The primary goal of the present study is to evaluate the final design and verify that it satisfies the design requirements. We aim for low cross-polarization (-30 dB), low sidelobe (-25 dB) levels, and a stable beam in terms of shape (low ellipticity) and size over a full octave bandwidth (10–20 GHz). We performed both ray-tracing and full-wave simulations using the CST Studio software in order to investigate the system behaviour. We gave special attention to the beam frequency variation and polarization leakage. We have characterized the effects on the radiation pattern produced by the cryostat window. We present the final design of the TMS optical system, as well as a complete study of the system's performance in terms of cross-polarization, sidelobes, ellipticity and beamwidth. We discuss the effects of sidelobes and study the need for a baffle.


2021 ◽  
Vol 7 (9) ◽  
pp. 126
Author(s):  
David S. Schmool ◽  
Daniel Markó ◽  
Ko-Wei Lin ◽  
Aurelio Hierro-Rodríguez ◽  
Carlos Quirós ◽  
...  

Ferromagnetic resonance is a powerful method for the study of all classes of magnetic materials. The experimental technique has been used for many decades and is based on the excitation of a magnetic spin system via a microwave (or rf) field. While earlier methods were based on the use of a microwave spectrometer, more recent developments have seen the widespread use of the vector network analyzer (VNA), which provides a more versatile measurement system at almost comparable sensitivity. While the former is based on a fixed frequency of excitation, the VNA enables frequency-dependent measurements, allowing more in-depth analysis. We have applied this technique to the study of nanostructured thin films or nanodots and coupled magnetic layer systems comprised of exchange-coupled ferromagnetic layers with in-plane and perpendicular magnetic anisotropies. In the first system, we have investigated the magnetization dynamics in Co/Ag bilayers and nanodots. In the second system, we have studied Permalloy (Ni80Fe20, hereafter Py) thin films coupled via an intervening Al layer of varying thickness to a NdCo film which has perpendicular magnetic anisotropy.


2021 ◽  
Author(s):  
Amanda Duerden ◽  
G. Grubbs II ◽  
Kristen Donnell ◽  
Joshua Isert ◽  
Frank Marshall ◽  
...  

Author(s):  
Arsh Singh Hazrah ◽  
Mohamad al-Jabiri ◽  
Raiden Speelman ◽  
Wolfgang Jaeger

Broadband rotational spectra of cis- and trans- (-) carveol were recorded using a chirped pulse Fourier transform microwave spectrometer in the 2-6 GHz region. To aid in spectroscopic assignments a...


Author(s):  
Jose A. Rubiño Martín ◽  
Paz Alonso Arias ◽  
Roger J. Hoyland ◽  
Marta Aguiar-Gonzalez ◽  
Javier De Miguel Hernandez ◽  
...  

Author(s):  
Paz Alonso-Arias ◽  
José Alberto Rubiño-Martín ◽  
Roger J. Hoyland ◽  
Marta Aguiar-González ◽  
Javier De Miguel-Hernández ◽  
...  

2020 ◽  
pp. 111396
Author(s):  
Amanda Duerden ◽  
Frank E. Marshall ◽  
Nicole Moon ◽  
Christian Swanson ◽  
Kristen M. Donnell ◽  
...  

2020 ◽  
Vol 10 (23) ◽  
pp. 8471
Author(s):  
Haoyang Tan ◽  
Miaoling Yang ◽  
Chenbo Huang ◽  
Shengwen Duan ◽  
Ming Sun ◽  
...  

The investigation on microwave spectrum of benzophenone was conducted with a recently constructed broadband chirped-pulse Fourier transform microwave spectrometer with a heating nozzle in the 2–8 GHz range. In this work, 138 b-type pure rotational transitions were assigned to bridge the measuring gap in the microwave region. The rotational constants for benzophenone were accurately determined by a combined microwave data fitting with frequency coverage between 2–14 GHz and have the following values: A = 1692.8892190(119) MHz, B = 412.6446602(43) MHz and C = 353.8745644(43) MHz.


Author(s):  
Stanislav Dyubko ◽  
Mykola Pogrebnyak ◽  
Eugene Alekseev ◽  
Michail Perepechaj

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