Towards high energy, minimum duration pulse in Yb-doped fiber CPA system by spectral shaping technique

Optik ◽  
2021 ◽  
pp. 168006
Author(s):  
Kun Chang ◽  
Longfei Zhu ◽  
Baoluo Yan ◽  
Guangke Jiang ◽  
Dengke Xing ◽  
...  
2016 ◽  
Vol 24 (9) ◽  
pp. 9905 ◽  
Author(s):  
Peter Kroetz ◽  
Axel Ruehl ◽  
Krishna Murari ◽  
Huseyin Cankaya ◽  
Franz X. Kärtner ◽  
...  

Author(s):  
Khmaies Ouahada ◽  
Theo G. Swart ◽  
Hendrik C. Ferreira ◽  
Ling Cheng

2020 ◽  
Vol 38 (2) ◽  
pp. 466-474 ◽  
Author(s):  
Shuto Yamamoto ◽  
Hiroki Taniguchi ◽  
Asuka Matsushita ◽  
Masanori Nakamura ◽  
Seiji Okamoto ◽  
...  

2011 ◽  
Vol 1 (03) ◽  
Author(s):  
Nguyen Quang Tuan ◽  
Do Quoc Trinh ◽  
Tran Xuan Nam ◽  
Dinh The Cuong

A new method of reusing a subset of an M-QAM signal constellation is presented for Bit-Interleaved Coded Modulation systems with Iterative Decoding (BICM-ID). In addition to the remapping of high-energy signals to low-energy signals in order to save the average signal energy as a shaping technique known so far, a new scheme of remapping low-energy signals to high-energy signals is proposed in order to gain the equivalent distance when decoding bits, often called the Squared Euclidean Weights (SEW). Numerical analysis and simulation results show that the partial reuse of the signals in the BICM-ID system with 16-QAM can improve the system performance in terms of lowering the bit error rate in the error floor region.


1984 ◽  
Vol 75 ◽  
pp. 599-602
Author(s):  
T.V. Johnson ◽  
G.E. Morfill ◽  
E. Grun

A number of lines of evidence suggest that the particles making up the E-ring are small, on the order of a few microns or less in size (Terrile and Tokunaga, 1980, BAAS; Pang et al., 1982 Saturn meeting; Tucson, AZ). This suggests that a variety of electromagnetic and plasma affects may be important in considering the history of such particles. We have shown (Morfill et al., 1982, J. Geophys. Res., in press) that plasma drags forces from the corotating plasma will rapidly evolve E-ring particle orbits to increasing distance from Saturn until a point is reached where radiation drag forces acting to decrease orbital radius balance this outward acceleration. This occurs at approximately Rhea's orbit, although the exact value is subject to many uncertainties. The time scale for plasma drag to move particles from Enceladus' orbit to the outer E-ring is ~104yr. A variety of effects also act to remove particles, primarily sputtering by both high energy charged particles (Cheng et al., 1982, J. Geophys. Res., in press) and corotating plasma (Morfill et al., 1982). The time scale for sputtering away one micron particles is also short, 102 - 10 yrs. Thus the detailed particle density profile in the E-ring is set by a competition between orbit evolution and particle removal. The high density region near Enceladus' orbit may result from the sputtering yeild of corotating ions being less than unity at this radius (e.g. Eviatar et al., 1982, Saturn meeting). In any case, an active source of E-ring material is required if the feature is not very ephemeral - Enceladus itself, with its geologically recent surface, appears still to be the best candidate for the ultimate source of E-ring material.


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