Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients
Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients are investigated by using the split-step Fourier method. The soliton pulse still maintains soliton characteristics after propagation in the system. The shape of output spectrum is...
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Veröffentlicht in: | Optik (Stuttgart) 2012-05, Vol.123 (9), p.818-822 |
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description | Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients are investigated by using the split-step Fourier method. The soliton pulse still maintains soliton characteristics after propagation in the system. The shape of output spectrum is still with a single peak. The temporal FWHM of an unchirped soliton performs a slight oscillation with the increase of propagation distance. The oscillation amplitude is slightly increased with the increase of the gain or loss parameter σ. The chirped soliton is obviously and periodically compressed and broadened with the increase of propagation distance in the system. The lager the value of chirp parameter |C| and σ is, the greater the variation of temporal width with the distance is. The effect of chirp on temporal width of soliton in a amplification system is greater than that in a loss system. Three types of numerical experiments show that the soliton with different perturbations can stably propagate along the fiber. In practical applications, one can obtain a suitable soliton pulse by controlling the parameters of the fiber system. |
doi_str_mv | 10.1016/j.ijleo.2011.06.045 |
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The soliton pulse still maintains soliton characteristics after propagation in the system. The shape of output spectrum is still with a single peak. The temporal FWHM of an unchirped soliton performs a slight oscillation with the increase of propagation distance. The oscillation amplitude is slightly increased with the increase of the gain or loss parameter σ. The chirped soliton is obviously and periodically compressed and broadened with the increase of propagation distance in the system. The lager the value of chirp parameter |C| and σ is, the greater the variation of temporal width with the distance is. The effect of chirp on temporal width of soliton in a amplification system is greater than that in a loss system. Three types of numerical experiments show that the soliton with different perturbations can stably propagate along the fiber. 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The soliton pulse still maintains soliton characteristics after propagation in the system. The shape of output spectrum is still with a single peak. The temporal FWHM of an unchirped soliton performs a slight oscillation with the increase of propagation distance. The oscillation amplitude is slightly increased with the increase of the gain or loss parameter σ. The chirped soliton is obviously and periodically compressed and broadened with the increase of propagation distance in the system. The lager the value of chirp parameter |C| and σ is, the greater the variation of temporal width with the distance is. The effect of chirp on temporal width of soliton in a amplification system is greater than that in a loss system. Three types of numerical experiments show that the soliton with different perturbations can stably propagate along the fiber. In practical applications, one can obtain a suitable soliton pulse by controlling the parameters of the fiber system.</description><subject>Amplification</subject><subject>Chirp</subject><subject>Chirped soliton</subject><subject>Fibers</subject><subject>Fourier analysis</subject><subject>Mathematical models</subject><subject>Nonlinear optics</subject><subject>Oscillations</subject><subject>Periodic distributed amplification systems</subject><subject>Solitons</subject><subject>Temporal logic</subject><subject>Temporal waveform</subject><issn>0030-4026</issn><issn>1618-1336</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNp9kD9PwzAQxS0EEqXwCVgysiSc48RJBwZU8U-qBAPMlmNf6FVpHWy3Fd8elzIznXT3e0_3HmPXHAoOXN6uCloN6IoSOC9AFlDVJ2zCJW9zLoQ8ZRMAAXkFpTxnFyGsAKBpoJmw_Zt3o_7UkdwmM0vttYnoKUQyIXN9WpEf0WbBDRQTQptsTHdnyWQ2YZ66bUx3vR4H6skcjcJ3iLgO2Z7iMttpT7obMDMO-4QQbmK4ZGe9HgJe_c0p-3h8eJ8_54vXp5f5_SI36e-YW9GIagadrlGIEupZ27X9TFrbVk1puJayNp1oADRHgaJvdWKs7GxTd71sOzFlN0ff0buvLYao1hQMDoPeoNsGxaEs27YCKRIqjqjxLgSPvRo9rbX_TpA61KxW6rdmdahZgVSp5qS6O6owpdgRehUOCQ1a8miiso7-1f8A21KKgg</recordid><startdate>201205</startdate><enddate>201205</enddate><creator>Zheng, Hongjun</creator><creator>Wu, Chongqing</creator><creator>Wang, Zhi</creator><creator>Yu, Huishan</creator><creator>Liu, Shanliang</creator><creator>Li, Xin</creator><general>Elsevier GmbH</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>201205</creationdate><title>Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients</title><author>Zheng, Hongjun ; Wu, Chongqing ; Wang, Zhi ; Yu, Huishan ; Liu, Shanliang ; Li, Xin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c336t-d373490ba5e3320598b8f96dd8472c1a665cb3700a1e3e3f8a059d6bd75bf68b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Amplification</topic><topic>Chirp</topic><topic>Chirped soliton</topic><topic>Fibers</topic><topic>Fourier analysis</topic><topic>Mathematical models</topic><topic>Nonlinear optics</topic><topic>Oscillations</topic><topic>Periodic distributed amplification systems</topic><topic>Solitons</topic><topic>Temporal logic</topic><topic>Temporal waveform</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zheng, Hongjun</creatorcontrib><creatorcontrib>Wu, Chongqing</creatorcontrib><creatorcontrib>Wang, Zhi</creatorcontrib><creatorcontrib>Yu, Huishan</creatorcontrib><creatorcontrib>Liu, Shanliang</creatorcontrib><creatorcontrib>Li, Xin</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Optik (Stuttgart)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zheng, Hongjun</au><au>Wu, Chongqing</au><au>Wang, Zhi</au><au>Yu, Huishan</au><au>Liu, Shanliang</au><au>Li, Xin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients</atitle><jtitle>Optik (Stuttgart)</jtitle><date>2012-05</date><risdate>2012</risdate><volume>123</volume><issue>9</issue><spage>818</spage><epage>822</epage><pages>818-822</pages><issn>0030-4026</issn><eissn>1618-1336</eissn><abstract>Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients are investigated by using the split-step Fourier method. The soliton pulse still maintains soliton characteristics after propagation in the system. The shape of output spectrum is still with a single peak. The temporal FWHM of an unchirped soliton performs a slight oscillation with the increase of propagation distance. The oscillation amplitude is slightly increased with the increase of the gain or loss parameter σ. The chirped soliton is obviously and periodically compressed and broadened with the increase of propagation distance in the system. The lager the value of chirp parameter |C| and σ is, the greater the variation of temporal width with the distance is. The effect of chirp on temporal width of soliton in a amplification system is greater than that in a loss system. Three types of numerical experiments show that the soliton with different perturbations can stably propagate along the fiber. In practical applications, one can obtain a suitable soliton pulse by controlling the parameters of the fiber system.</abstract><pub>Elsevier GmbH</pub><doi>10.1016/j.ijleo.2011.06.045</doi><tpages>5</tpages></addata></record> |
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subjects | Amplification Chirp Chirped soliton Fibers Fourier analysis Mathematical models Nonlinear optics Oscillations Periodic distributed amplification systems Solitons Temporal logic Temporal waveform |
title | Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients |
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