20W GaN HPAs for Next Generation X-Band T/R-Modules

Author(s):  
P. Schuh ◽  
R. Leberer ◽  
H. Sledzik ◽  
M. Oppermann ◽  
B. Adelseck ◽  
...  
Keyword(s):  
2017 ◽  
Vol 2017 (NOR) ◽  
pp. 1-5
Author(s):  
Martin Oppermann ◽  
Ralf Rieger

Abstract Next generation RF sensor modules for multifunction active electronically steered antenna (AESA) systems will need a combination of different operating modes, such as radar, electronic warfare (EW) functionalities and communications/datalinks within the same antenna frontend. They typically operate in C-Band, X-Band and Ku-Band and imply a bandwidth requirement of more than 10 GHz. For the realisation of modern active electronically steered antennas, the transmit/receive (T/R) modules have to match strict geometry demands. A major challenge for these future multifunction RF sensor modules is dictated by the half-wavelength antenna grid spacing, that limits the physical channel width to < 12 mm or even less, depending on the highest frequency of operation with accordant beam pointing requirements. A promising solution to overcome these geometry demands is the reduction of the total monolithic microwave integrated circuit (MMIC) chip area, achieved by integrating individual RF functionalities, which are commonly achieved through individual integrated circuits (ICs), into new multifunctional (MFC) MMICs. Various concepts, some of them already implemented, towards next generation RF sensor modules will be discussed and explained in this work.


Author(s):  
S Sazonov ◽  
I Khabibullin

Abstract There is a hope that looking into the early Universe with next-generation telescopes, one will be able to observe the early accretion growth of supermassive black holes (BHs) when their masses were ∼104–106M⊙. According to the standard accretion theory, the bulk of the gravitational potential energy released by radiatively efficient accretion of matter onto a BH in this mass range is expected to be emitted in the extreme UV–ultrasoft X-ray bands. We demonstrate that such a ’miniquasar’ at z ∼ 15 should leave a specific, localized imprint on the 21 cm cosmological signal. Namely, its position on the sky will be surrounded by a region with a fairly sharp boundary of several arcmin radius, within which the 21 cm brightness temperature quickly grows inwards from the background value of ∼−250 mK to ∼+30 mK. The size of this region is only weakly sensitive to the BH mass, so that the flux density of the excess 21 cm signal is expected to be ∼0.1–0.2 mJy at z ∼ 15 and should be detectable by the Square Kilometer Array. We argue that an optimal strategy would be to search for such signals from high-z miniquasar candidates that can be found and localized with a next-generation X-ray mission such as Lynx. A detection of the predicted 21 cm signal would provide a measurement of the growing BH’s redshift to within Δz/(1 + z) ≲ 0.01.


Author(s):  
L. Lodola ◽  
G. Batignani ◽  
M.A. Benkechkache ◽  
S. Bettarini ◽  
G. Casarosa ◽  
...  
Keyword(s):  
Sar Adc ◽  

2012 ◽  
Vol 423 (3) ◽  
pp. 2503-2517 ◽  
Author(s):  
B. Sartoris ◽  
S. Borgani ◽  
P. Rosati ◽  
J. Weller

2014 ◽  
Vol 439 (1) ◽  
pp. 102-122 ◽  
Author(s):  
N. W. Slack ◽  
T. J. Ponman
Keyword(s):  

2010 ◽  
Vol 49 (21) ◽  
pp. 4077 ◽  
Author(s):  
Maxime Chauvin ◽  
Jean-Pierre Roques

2004 ◽  
Author(s):  
Hans P. Bluem ◽  
Alan M. M. Todd ◽  
Ilan Ben-Zvi ◽  
Michael D. Cole ◽  
Pat Colestock ◽  
...  
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