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Research on Modern science and Utilizing Technological Innovation Journal (RMUTI Journal)

การเปลยนสญญาณแสงแบบโซลตรอนแสงมดและแสงสวางโดยใชหลกการของโพรงสนพองระดบนาโนเมตรดวยระบบกรองสญญาณแสงแอด/ดรอป

ปรีชา ยุพาพิน, สุขุม จุฬาจัตตุรศิระรัตน์

Published Aug 29, 2014• 0 citations
OpenAlex

Abstract

We propose a novel system of a dark-bright soliton pulse conversion that can be dynamically controlled by the desired input signal within an add/drop optical filter, where the dark solition signals are controlled, tuned and amplified by the input bright soliton. In this paper, the dynamic behavior of dark-bright soliton interaction is analyzed and described. The optical storages are embedded within the add/drop optical filter system, whereas the generated optical signals can be stored and amplified. In application, the storage signals can be configured to be an optical trapping tool/potential well which is known as optical tweezers, where the high field peak signal or well can be formed the trapping tool.

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Procedia Engineering•Jan 1, 2011•5 citations
We propose a novel system of a dark-bright soliton pulse conversion that can be dynamically controlled by the desired input signal within an add/drop optical filter, where the dark solition signals are controlled, tuned and amplified by the input bright soliton. In this paper, the dynamic behavior of dark-bright soliton interaction is analyzed and described. The optical storages are embedded within the add/drop optical filter system, whereas the generated optical signals can be stored and amplified. In application, the storage signals can be configured to be an optical trapping tool/potential well which is known as optical tweezers, where the high field peak signal or well can be formed the trapping tool.
We propose a novel system of the dynamic potential well generation and control using light pulse control within an add/drop optical filter. The multiplexing signals of the dark solition with bright/Gaussian pulses are controlled, tuned and amplified within the system. The optical storage rings are embedded within the add/drop optical filter system, whereas the generated optical signals can be stored and amplified within the design system. In application, the storage signals can be configured to be an optical trapping tool which is known as optical tweezers, where the high field peak or well can be formed. The advantages are that the dynamic well can be stored and the array of well can be generated for multiple well applications. The difference in time of the first two dynamic wells of 1 ns is noted.
We propose a novel system of an optical trapping tool using a dark-bright soliton pulse-propagating within an add/drop optical filter. The multiplexing signals with different wavelengths of the dark soliton are controlled and amplified within the system. The dynamic behavior of dark bright soliton interaction is analyzed and described. The storage signal is controlled and tuned to be an optical probe which can be configured as the optical tweezer. The optical tweezer storage is embedded within the add/drop optical filter system. By using some suitable parameters, we found that the tweezers storage time of 1.2 ns is achieved. Therefore, the generated optical tweezers can be stored and amplified within the design system. In application, the optical tweezers can be stored and trapped light/atom, which can be transmitted and recovered by using the proposed system.
We propose a novel system of dynamic potential well generation and control using light pulse control within an add/drop optical filter. The multiplexing signals of the dark solition with bright/Gaussian pulses are controlled, tuned, and amplified within the system. The optical storage rings are embedded within the add/drop optical filter system, whereas the generated optical signals can be stored and amplified within the design system. In application, the storage signals can be configured to be an optical trapping tool, which is known as an optical tweezer, where the high field peak or well can be formed. The advantages are that the dynamic well can be stored and the array of wells can be generated for multiple wells applications. The different in time of the first two dynamic wells of 1 ns is noted.
We propose a novel system of multi optical trapping tool using a bright soliton pulses propagating within the add/drop optical filter system. The multiplexing signals with different wavelengths of the bright solition are controlled and amplified within the system. The dynamic behavior of bright soliton interaction is analyzed and described. The signal is controlled and tuned to be an optical probe which can be configured as the multi optical tweezers. By using some suitable parameters, we found that the tweezers widths in add/drop at the drop ports are about 18 nm is achieved. Therefore, the generated multi optical tweezers can be amplified within the design system. In application, the optical tweezers train can be trapped light/atom, which can be transmitted and recovered by using the proposed system.
Abstract We propose a novel system of the optical tweezers array generation using dark soliton control within and add/drop filter control light by light. The dynamic tweezers are generated within an add/drop filter, where the number of tweezers within the add/drop filter can be tuned and amplified. The smallest tuned tweezers width are 0.02-0.05 nm are achieved, where the number of tweezers are 10-20 in an array. We have also theoretically shown that the dynamic tweezers can be controlled and tuned by varies the couple coefficient (k) between 0.1-0.9 and the radius of ring resonator between 10-20 |j.m, which is available for trapping and transportation in the communication up­link system via a add/drop filter. In application, the transmission of tweezers with different molecules and wavelengths can be performed within the transmission link, which is available for high density molecular transportation for wireless communication in near future. Keywords : Atom transmission; Molecule transmission; Molecular communication
We propose a new system of an all optical switching system using an optical add/drop filter consisting of two nano ring resonators. The dynamic behavior of dark-bright soliton collision within the modified add/drop optical filter device, which it is known as PANDA ring resonator. By using the dark-bright soliton conversion control within the PANDA ring, the obtained output signals can be attenuated and used to perform the single photon switching, which is capable for security code application. Results obtained have shown that the random binary codes based on a single photon switching can be formed by using the polarized light components, dark and bright solitons, whereas the single photon switching codes can be obtained by using the attenuated dark-bright soliton conversion signals output signals.