๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Exploration of the integration of a passive coplanar isolator based on thin magnetic films

โœ Scribed by S. Capraro; T. Rouiller; M. Le Berre; J. P. Chatelon; B. Bayard; D. Barbier; J. J. Rousseau


Publisher
John Wiley and Sons
Year
2005
Tongue
English
Weight
141 KB
Volume
46
Category
Article
ISSN
0895-2477

No coin nor oath required. For personal study only.

โœฆ Synopsis


As an example, the helix-pitch profile of the considered tube was modified for improving the yield (Table 1), maintaining similar small-signal gain (62.6-dB average gain and 5% flatness). In particularly, according to the previously exposed theory, the helix pitch in the lower helix-pitch section (section 4) was incremented to 0.064 cm. The yield for the original and improved tubes was compared for both the cases of random (independent random variation of the helix pitch of each section) error and systematic (same helix-pitch variation for all the sections) error [5]. A maximum helix-pitch tolerance of 3% was considered. Three hundred different tubes were simulated for each value of helix-pitch error.

For the purpose of this study, a tube was considered acceptable if the average gain was included in the ฯฎ1.5% range with respect to the nominal value and the flatness was lower than 6%. A remarkable yield improvement is obtained for both random (Fig. 2) and systematic (Fig. 3) errors. The small histograms included in the figures show that the percentage increment of the yield obtained for the different helix-pitch error values is, in some cases, higher than 25%.

CONCLUSION

TWT yield degradation in case of small-signal gain, caused by the tube sections with lower helix pitch, has been studied. The analysis of the small-signal gain per unit length of a helix slow-wave structure provides useful information for predicting the yield behaviour. It was demonstrated that a suitable adjustment of the helix-pitch profile, hence maintaining similar small-signal gain performance, significantly improves the yield.


๐Ÿ“œ SIMILAR VOLUMES


Exploration of a thin YIG film-based cop
โœ S. Capraro; T. Boudiar; T. Rouiller; J. P. Chatelon; B. Bayard; M. Le Berre; B. ๐Ÿ“‚ Article ๐Ÿ“… 2004 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 78 KB

## Abstract In this paper, we present the experimental results of a coplanar isolator made on both bulk YIG and thinโ€film YIG. An external field has been applied on this device and we observe the amplitude of the nonreciprocal effect, which is between 1.8 and 6.2 dB for a resonance frequency of 3.3

Isolated Single-Molecule Magnets on the
โœ D. Ruiz-Molina; M. Mas-Torrent; J. Gรณmez; A.I. Balana; N. Domingo; J. Tejada; M. ๐Ÿ“‚ Article ๐Ÿ“… 2003 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 229 KB ๐Ÿ‘ 2 views

**Individual Mn~12~ singleโ€molecule magnets** are arranged onto a polymeric film surface using a new, soft, reliable and simple chemical methodology. Polymeric thin films, prepared from a polycarbonate matrix and Mn~12~ molecules, are subsequently treated with an organic solvent vapor, resulting in

The influence of passivation on the kine
โœ A.M. Sukhotin; M.S. Grilikhes; E.V. Lisovaya ๐Ÿ“‚ Article ๐Ÿ“… 1989 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 348 KB

By the Poisson equation solution using Fermi-Dirac statistics for a degenerate electron gas a formula for calculation of doping density N z lOi cnm3 and flat band potential E, at 300 K is derived according to the Mott-Schottky equation. The relationships for estimation of the depletion band bending