Hybrid transceiver and repeater using a PANDA ring resonator for nanocommunication

Jukgoljun, B.; Suwanpayak, N.; Teeka, C.; Yupapin, P.P.

doi:10.1117/1.3526332

Cited by 15 publications

(8 citation statements)

References 19 publications

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“…Explosive growth in wireless communications requires filters with wide pass band characteristics for ultra wide band (UWB) systems and high data rate wireless transceivers. Design of a compact broadband filter is still a key issue in many system designs [1][2][3][4][5]. Multilayer structures incorporating low temperature co-fired ceramic (LTCC) or stacking several layers of microwave laminates are some of the useful technologies for realizing miniaturized filters for wide band operation.…”

Section: Discussionmentioning

confidence: 99%

Novel optical cryptography using LIP signals generated by a PANDA ring resonator

Pongsanam

Juleang

Mitatha

et al. 2011

Micro & Optical Tech Letters

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matched case (Fig. 4) at the same fiber separation the power coupling efficency is lower.In the last study, the power variation as a function of the fiber separation in the multimode-to-multimode fiber design is investigated for the red LED and laser sources. As can be seen in Figure 6, since the launching power for the laser is considerably higher than that of the LED thus the output power for the laser is much higher. For the LED light, the power decreases from 496 to 61 nW for the gap range of 0.1-5 mm. For the laser illumination, the output power decreases from the 2036 to 110 nW for the same range. For both light sources, the related output powers are decreased by increasing the axial fiber separation. As can be noted in Figure 6, the sensitivity, in particular for the laser illumination, is higher for the range of 0.1-5-mm displacement, which can be a good range for the effective sensing operation based on the fiberto-fiber principle.

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Section: Discussionmentioning

confidence: 99%

Novel optical cryptography using LIP signals generated by a PANDA ring resonator

Pongsanam

Juleang

Mitatha

et al. 2011

Micro & Optical Tech Letters

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“…This is given in the following details. The optical circuits of ring resonant add/drop filter for the though port and drop port are defmed in by the authors in [8]. ICj and 10 are the coupling coefficients of the add/drop filters, kn=21l1.?…”

Section: Theoretical Backgroundmentioning

confidence: 99%

Molecular transistor manipulation controlled by light within a PANDA microring resonator

Panruansan

Mitatha

Yupapin

2011

2011 International Symposium on Intelligent Signal Processing and Communications Systems (ISPACS)

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A novel design of Molecular Transistor using a microring resonator called a PANDA microring resonator is proposed. A molecular transistor can control its output in proportion to the input signal; that is, it can act as an amplifier.Alternatively, it can be used to turn current on or off in a circuit as an electrically controlled switch. By using the optic tweezers, the trapped molecule can be used to form in the same way of photonic transistor, in which the increasing in magnitude of force can increase the trapped molecules. The trapping probe can be adjusted to fit for the molecules size of 10 nm to 15 nm by control ring's parameters. The molecules can be transport at the through port and storage at the drop port. In application, the number of molecules can be controlled to perform the constant and amplification characteristics, which will be suitable for molecular transistor performance.

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“…It remains as an interesting aspect of investigations, for instance, the studies of spin coupling and orbital motion of electrons in carbon nanotubes, magnetic manipulations, sidewall oxide effects on spin torque and magnetic field induced reversal characteristics of thin film nanomagnets, magnetic vortex oscillator driven by d.c. spin polarized current and measurement of the spin transfer torque vector in magnetic tunnel junctions have been reported. Recently, Yupapin et al [7–12] have shown the promising application of all optical devices, which consists of an add‐drop optical filter known as a PANDA ring resonator using optical dark‐bright soliton control within a semiconductor add‐drop multiplexer. It has been investigated clearly by the authors in references [13, 14], that one of the advantages of such a system is that the dark soliton peak signal is always at a low level, which is useful for secured signal communication in the transmission link.…”

Section: Introductionmentioning

confidence: 99%

Optical spin manipulation using dark‐bright soliton behaviors in a panda ring resonator

Muhammad

Teeka

Ali

et al. 2012

Micro & Optical Tech Letters

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A new concept of an optoelectronic spin generation using bright and dark soliton conversion behaviors within a modified optical add‐drop filters known as a PANDA ring resonator is proposed. The orthogonal solitons can be formed randomly within the system and detected simultaneously at the output ports. Under the resonant condition, the random transverse electric and magnetic fields of the solitons corresponding to the left‐hand and right‐hand photons can be generated. Whenever a photon is absorbed by an object, an angular momentum of either + ħ or –ħ is imparted to the object, in which two possible spin states known as optoelectronic spins are exhibited. Furthermore, the array of optoelectronic spins, i.e., many particles can be generated and controlled by using the proposed system, which can be used to form large scale spintronics applications. © 2012 Wiley Periodicals, Inc. Microwave Opt Technol Lett 54:987–990, 2012; View this article online at wileyonlinelibrary.com. DOI 10.1002/mop.26708

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Hybrid transceiver and repeater using a PANDA ring resonator for nanocommunication

Cited by 15 publications

References 19 publications

Novel optical cryptography using LIP signals generated by a PANDA ring resonator

Novel optical cryptography using LIP signals generated by a PANDA ring resonator

Molecular transistor manipulation controlled by light within a PANDA microring resonator

Optical spin manipulation using dark‐bright soliton behaviors in a panda ring resonator

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