Grating Length

14,000,000 Leading Edge Experts on the ideXlab platform

Scan Science and Technology

Contact Leading Edge Experts & Companies

Scan Science and Technology

Contact Leading Edge Experts & Companies

The Experts below are selected from a list of 7728 Experts worldwide ranked by ideXlab platform

Sourangsu Banerji - One of the best experts on this subject based on the ideXlab platform.

  • To Study the Effect of Grating Length on Propagating Modes in Bragg Filters with AlXGa1-XN/GaN Material Composition
    International Journal of Advanced Science and Technology, 2014
    Co-Authors: Sourangsu Banerji
    Abstract:

    In this paper, the forward and backward propagating modes in an optical waveguide structure namely the fiber Bragg filter also considered as a one dimensional photonic crystal, is analytically computed as a function of Grating Length for coupled optical modes. AlxGa1xN/GaN material composition is considered as a unit block of the periodic organization, and refractive index of AlxGa1-xN/GaN is taken to be dependent on material composition, bandgap and operating waveLength following Adachi’s model. Expressions for propagating wave have been derived using coupled mode theory. Simulated results help us to study the propagation of forward and backward wave propagating modes inside fiber and waveguide devices.

  • To Study the Effect of Grating Length on Propagating Modes in Bragg Filters with AlxGa1-xN/GaN Material Composition
    arXiv: General Physics, 2013
    Co-Authors: Sourangsu Banerji
    Abstract:

    In this paper, the forward and backward propagating modes in an optical waveguide structure namely the fiber Bragg filter also considered as a one dimensional photonic crystal, are analytically computed as a function of Grating Length for coupled optical modes. AlxGa1-xN/GaN material composition is considered as a unit block of the periodic organization, and refractive index of AlxGa1-xN/GaN is taken to be dependent on material composition, bandgap and operating waveLength following Adachi's model. Expressions of propagating wave are derived using coupled mode theory. Simulated results help us to study the propagation of forward and backward wave propagating modes inside fiber and waveguide devices.

  • Study of Propagating Modes and Reflectivity in Bragg Filters with AlxGa1-xN/GaN Material Composition
    arXiv: General Physics, 2013
    Co-Authors: Sourangsu Banerji
    Abstract:

    In this paper, forward and backward propagating waves and reflectivity in an optical waveguide structure namely the fiber Bragg reflector also considered as a one dimensional photonic crystal, are analytically computed using coupled mode theory for different Grating Lengths and coupling conditions. AlxGa1-xN/GaN material composition is considered as unit block of the periodic organization, and refractive index of AlxGa1-xN is taken to be dependent on material composition, bandgap and operating waveLength following Adachis' model. The structure being considered is the Bragg Grating where increase in Grating Length enhances the reflection of electromagnetic wave, and strong coupling provides larger bandgap spectral width. Input waveLength is made different from Bragg waveLength to study the characteristics of propagating waves. A suitable combination of Grating Length and coupling coefficient is helpful in designing the photonic bandgap at 1550 nm waveLength. These characteristic curves can be utilized to study how waves propagate through the optical waveguides which have a special place in optical communications

Hsu-chih Cheng - One of the best experts on this subject based on the ideXlab platform.

Jose Azana - One of the best experts on this subject based on the ideXlab platform.

  • Terahertz bandwidth all-optical Hilbert transformers based on long-period Gratings.
    Optics Letters, 2012
    Co-Authors: Reza Ashrafi, Jose Azana
    Abstract:

    A novel, all-optical design for implementing terahertz (THz) bandwidth real-time Hilbert transformers is proposed and numerically demonstrated. An all-optical Hilbert transformer can be implemented using a uniform-period long-period Grating (LPG) with a properly designed amplitude-only Grating apodization profile, incorporating a single π-phase shift in the middle of the Grating Length. The designed LPG-based Hilbert transformers can be practically implemented using either fiber-optic or integrated-waveguide technologies. As a generalization, photonic fractional Hilbert transformers are also designed based on the same optical platform. In this general case, the resulting LPGs have multiple π-phase shifts along the Grating Length. Our numerical simulations confirm that all-optical Hilbert transformers capable of processing arbitrary optical signals with bandwidths well in the THz range can be implemented using feasible fiber/waveguide LPG designs.

  • all optical hilbert transformer based on a single phase shifted fiber bragg Grating design and analysis
    Optics Letters, 2009
    Co-Authors: Mohammad H Asghari, Jose Azana
    Abstract:

    A simple all-fiber design for implementing an all-optical temporal Hilbert transformer is proposed and numerically demonstrated. We show that an all-optical Hilbert transformer can be implemented using a uniform-period fiber Bragg Grating (FBG) with a properly designed amplitude-only Grating apodization profile incorporating a single π phase shift in the middle of the Grating Length. All-optical Hilbert transformers capable of processing arbitrary optical waveforms with bandwidths up to a few hundreds of gigahertz can be implemented using feasible FBGs.

Shivendu Prashar - One of the best experts on this subject based on the ideXlab platform.

  • Investigation of Grating Parameters Impact on Spectral Characteristics of LPFG using Two-Layer Fiber Geometry
    2018 6th Edition of International Conference on Wireless Networks & Embedded Systems (WECON), 2018
    Co-Authors: Shivendu Prashar
    Abstract:

    The study on spectral characteristics of long period fiber Grating (LPFG) explores its usefulness in many applications. This scenario insists the researchers to calculate the impact of LPFG's parameters on its characteristics. The paper presents the effect of Grating Length and Grating period on the spectral characteristics of LPFG. Their impact is calculated in terms of variation in position of resonant waveLength and attenuation band depth. For this, the transmission profiles of LP03 and LP05 cladding modes are kept under observation here. The spectral profiles are calculated using analytical expressions obtained through coupled mode theory. The two layer fiber geometrical model is implemented on SMF28 optical fiber parameters to evaluate propagation constants of fiber's core region's and cladding region's modes. The results show linear increase in attenuation depth of spectrum with increase in Grating Length. On the other hand, with the rise in periodicity the shift in resonant waveLength is towards longer waveLengths.

  • Investigative Study of Transmission Spectra of FBG at Varying Induced Index & Grating Length
    Procedia Engineering, 2012
    Co-Authors: Shivendu Prashar, Derick Engles, Sham S. Malik, Rajan Vohra
    Abstract:

    Abstract The waveLength tuning capacities of Fiber Bragg Gratings (FBG) are related with the change in reflectivity of FBG at Bragg's waveLength. There are two main methods to obtain such effect: by modifying the fiber refractive index or by changing the Grating period. In our work, we have simulated a uniform FBG in MATLAB and studied its transmission spectra for different refractive index modulation values at 0.5x10-4, 1.5x10-4and 2x10-4. The numerical integration of the coupled mode equation was used to solve the properties of FBG. Then a fast and accurate technique that based on T-matrix formalism was used for calculating the input and output fields. Reflectivity shown by FBG of Grating Length 7mm for different induced index values (Δn) = 0.5x10-4, 1.5x10-4and 2x10-4is 27.95%, 88.94% and 96.45% respectively. Reflectivity is also investigated for 10mm & 15mm Grating Lengths for the same values of Δn.

  • investigative study of transmission spectra of fbg at varying induced index Grating Length
    Procedia Engineering, 2012
    Co-Authors: Shivendu Prashar, Derick Engles, Sham S. Malik, Rajan Vohra
    Abstract:

    Abstract The waveLength tuning capacities of Fiber Bragg Gratings (FBG) are related with the change in reflectivity of FBG at Bragg's waveLength. There are two main methods to obtain such effect: by modifying the fiber refractive index or by changing the Grating period. In our work, we have simulated a uniform FBG in MATLAB and studied its transmission spectra for different refractive index modulation values at 0.5x10-4, 1.5x10-4and 2x10-4. The numerical integration of the coupled mode equation was used to solve the properties of FBG. Then a fast and accurate technique that based on T-matrix formalism was used for calculating the input and output fields. Reflectivity shown by FBG of Grating Length 7mm for different induced index values (Δn) = 0.5x10-4, 1.5x10-4and 2x10-4is 27.95%, 88.94% and 96.45% respectively. Reflectivity is also investigated for 10mm & 15mm Grating Lengths for the same values of Δn.

Kristjan Leosson - One of the best experts on this subject based on the ideXlab platform.

  • compact z add drop waveLength filters for long range surface plasmon polaritons
    Optics Express, 2005
    Co-Authors: Alexandra Boltasseva, Sergey I Bozhevolnyi, Thomas Sondergaard, Thomas Nikolajsen, Kristjan Leosson
    Abstract:

    We design, fabricate and investigate compact Z-add-drop (ZAD) filters for long-range surface plasmon polaritons (LR-SPPs) at telecom waveLengths. The ZAD filter for LR-SPPs consists of two ridge Gratings formed by periodic gold thickness modulation at the intersections of three zigzag-crossed gold stripes embedded in polymer. We investigate influence of the Grating Length and crossing angle on the filter characteristics and demonstrate a 10°-ZAD filter based on 80-µm-long Gratings that exhibit a 15-dB dip (centered at ~1.55 µm) in transmission of the direct arm along with the corresponding ~13-nm-wide transmission peak in the drop arm.