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Dive into the research topics where Kyriacos Kalli is active.

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Featured researches published by Kyriacos Kalli.


Optics Letters | 2005

Continuous-wave ultraviolet light induced fiber Bragg gratings in few- and single-mode microstructured polymer optical fibers

Helen L. Dobb; David J. Webb; Kyriacos Kalli; Alexander Argyros; Maryanne C. J. Large; Martijn A. van Eijkelenborg

We report observations and measurements of the inscription of fiber Bragg gratings (FBGs) in two different types of microstructured polymer optical fiber: few-mode and an endlessly single mode. Contrary to the FBG inscription in silica microstructured fiber, where high-energy laser pulses are a prerequisite, we have successfully used a low-power cw laser source operating at 325 nm to produce 1 cm long gratings with a reflection peak at 1570 nm. Peak reflectivities of more than 10% have been observed.


Optics Express | 2007

Thermal response of Bragg gratings in PMMA microstructured optical fibers.

Karen Carroll; Chi Zhang; David J. Webb; Kyriacos Kalli; Alexander Argyros; Maryanne C. J. Large

We report on the thermal characteristics of Bragg gratings fabricated in polymer optical fibers. We have observed a permanent shift in the grating wavelength at room temperature which occurs when the grating has been heated above a threshold temperature. This threshold temperature is dependent on the thermal history of the grating, and we attribute the effect to a shrinking of the fiber. This effect can be avoided by annealing the fiber before grating inscription, resulting in a linear response with temperature and an increased linear operating temperature range of the grating.


photonics north | 2004

Temperature insensitive long-period grating sensors in photonic crystal fiber

Helen L. Dobb; Kyriacos Kalli; David J. Webb

Presented are long-period gratings (LPGs) fabricated in pure silica photonic crystal fibre (PCF) using an electric arc. Two different varieties of PCF have been investigated, an endlessly single mode PCF and a large-mode area PCF. The LPGs have been characterised for their sensitivity to a variety of external measurands. The LPGs in both fibres have been found to have negligible temperature sensitivity whilst exhibiting good sensitivity to bending and strain.


Journal of Applied Physics | 2002

Characterization of reflectivity inversion, α- and β-phase transitions and nanostructure formation in hydrogen activated thin Pd films on silicon based substrates

Kyriacos Kalli; Andreas Othonos; Constantinos Christofides

Optically thin palladium metal films evaporated on different silicon based substrates are investigated following exposure to different concentrations of hydrogen gas in air. Laser modulated reflectance off the palladium surface of silicon oxide and silicon nitride substrates is used to recover information regarding the reflectivity inversion and α/β-phases of the palladium complex after both first and multiple gas cycling. Atomic force microscopy confirms the formation of metal nanostructures following exposure to hydrogen of the optically thin palladium films.


Optics Letters | 1992

Ring Resonator Optical-Spectrum Analyzer with 20-Khz Resolution

Kyriacos Kalli; David A. Jackson

We demonstrate a fiber-optic ring resonator operated as a high-resolution spectrum analyzer. An optical resolution of 20 +/- 3 kHz is demonstrated.


Measurement Science and Technology | 2007

Development of an electrically tuneable Bragg grating filter in polymer optical fibre operating at 1.55 µm

Kyriacos Kalli; Helen L. Dobb; David J. Webb; Karen Carroll; Christos Themistos; Michalis Komodromos; Gang-Ding Peng; Q. Fang; Ian W. Boyd

We present a thorough study on the development of a polymer optical fibre-based tuneable filter utilizing an intra-core Bragg grating that is electrically tuneable, operating at 1.55 νm. The Bragg grating is made tuneable using a thin-film resistive heater deposited on the surface of the fibre. The polymer fibre was coated via the photochemical deposition of a Pd/Cu metallic layer with the procedure induced by VUV radiation at room temperature. The resulting device, when wavelength tuned via Joule heating, underwent a wavelength shift of 2 nm for a moderate input power of 160 mW, a wavelength to input power coefficient of -13.4 pm mW-1 and time constant of 1.7 s-1. A basic theoretical study verified that for this fibre type one can treat the device as a one-dimensional system. The model was extended to include the effect of input electrical power changes on the refractive index of the fibre and subsequently to changes in the Bragg wavelength of the grating, showing excellent agreement with the experimental measurements.


Measurement Science and Technology | 2004

Blank beam fabrication of regenerated type IA gratings

George Simpson; Kyriacos Kalli; Kaiming Zhou; Lin Zhang; Ian Bennion

We demonstrate an idealized method for the fabrication of regenerated type IA fibre Bragg gratings using commonly available apparatus. We use this technique to show that gratings written in the same fibre with the same period may have central wavelengths which are 14.4 nm apart and have an + 11.5% and - 1.2% difference in temperature and strain coefficients, respectively. We use these results to show that temperature compensated dual grating sensor heads, of an arbitrary length, may be quickly and consistently manufactured.


SPIE's 1996 International Symposium on Optical Science, Engineering, and Instrumentation | 1996

Recent developments in optical fiber sensing using fiber Bragg gratings

G.P. Brady; Kyriacos Kalli; David J. Webb; David A. Jackson; Lin Zhang; Ian Bennion

We report on recent work on sensing using in-fiber Bragg gratings carried out in our laboratory. First, an alternative method of discriminating between temperature and strain effects using a conventionally written, in-fiber Bragg grating is presented. The technique uses wavelength information from the first and second diffraction orders of the grating element to determine the wavelength dependent strain and temperature coefficients, from which independent temperature and strain measurements can be made. Secondly, we describe an all-fiber, passive scheme for making extended range interferometric measurements based on the dual wavelength technique. A coherence turned interferometer network is illuminated with a single superfluorescent fiber source at 1.55 mm and the two wavelengths are synthesized at the output by means of chirped fiber Bragg gratings.


Optics Letters | 2007

Electrically tunable Bragg gratings in single-mode polymer optical fiber

Kyriacos Kalli; Helen L. Dobb; David J. Webb; Karen Carroll; Michael Komodromos; C. Themistos; Gang-Ding Peng; Q. Fang; Ian W. Boyd

We present what is to our knowledge the first demonstration of a tunable fiber Bragg grating device in polymer optical fiber that utilizes a thin-film resistive heater deposited on the surface of the fiber. The polymer fiber was coated via photochemical deposition of a Pd/Cu metallic layer with a procedure induced by vacuum-ultraviolet radiation at room temperature. The resulting device, when wavelength tuned via joule heating, underwent a wavelength shift of 2 nm for a moderate input power of 160 mW, a wavelength to input power coefficient of -13.4 pm/mW, and a time constant of 1.7 s(-1).


Optics Letters | 1995

Simultaneous interrogation of interferometric and Bragg grating sensors

G.P. Brady; Kyriacos Kalli; David J. Webb; David A. Jackson; L. Reekie; J.L. Archambault

We propose a new method for the simultaneous interrogation of conventional two-beam interferometers and Bragg grating sensors. The technique employs an unbalanced Mach-Zehnder interferometer illuminated by a single low coherence source, which acts as a wavelength-tunable source for the grating and as a path-matched filter for the Fizeau interferometer, thus providing a high phase resolution output for each sensor. The grating sensor demonstrates a dynamic strain resolution of ~0.05 µ.epsilon/√Hz at 20 Hz, while the interferometric phase resolution is better than 1 mrad/√Hz at 20 Hz, corresponding to an rms mirror displacement of 0.08 nm.

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Christos Themistos

Frederick Institute of Technology

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