Optical transmission characteristics of fiber ring resonators

Heebner, John E.; Wong, Vincent; Schweinsberg, Aaron; Boyd, Robert W.; Jackson, Deborah J.

doi:10.1109/jqe.2004.828232

Cited by 218 publications

(104 citation statements)

References 17 publications

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“…3(b)] has a Lorentzian shape [ Fig. 3(c)] and its maximum GD is proportional to [12]. Note that due to absence of the drop port, in this configuration, .…”

Section: Microring-based Dispersion-compensating Stagesmentioning

confidence: 97%

Importance of Intrinsic-$Q$ in Microring-Based Optical Filters and Dispersion-Compensation Devices

Hossein‐Zadeh

Vahala

2007

IEEE Photon. Technol. Lett.

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“…3(b)] has a Lorentzian shape [ Fig. 3(c)] and its maximum GD is proportional to [12]. Note that due to absence of the drop port, in this configuration, .…”

Section: Microring-based Dispersion-compensating Stagesmentioning

confidence: 97%

Importance of Intrinsic-$Q$ in Microring-Based Optical Filters and Dispersion-Compensation Devices

Hossein‐Zadeh

Vahala

2007

IEEE Photon. Technol. Lett.

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“…The external phase shift of OFRRs can be achieved from the argument on ratio output field and input field as [3]:…”

Section: Analysis Of Optical Fiber Ring Resonator (Ofrr)mentioning

confidence: 99%

“…There are many proposed applications of optical ring resonators [1][2][3][4][5]. These devices can be constructed in a variety of sizes from micrometers to nanometers, with spectral characteristics that scale.…”

Section: Introductionmentioning

confidence: 99%

“…In this paper, we describe our studies of the optical transmission, intensity, shift phase and group delay characteristics of a family of such devices. Optical ring resonators hold great promise for a variety of applications, including optical switching [9,10], optical time delay [10][11][12], photonic biosensors [3,13,14], laser resonators [1] and add-drop filters [15,16].…”

Section: Introductionmentioning

confidence: 99%

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Modification of surface properties of bell metal by radiofrequency plasma polymerization

Chutia

Choudhury

Pal

et al. 2012

Journal of Theoretical and Applied Physics

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This study has been focused on the linear and nonlinear behavior and investigative in single-ring resonator. Optical fiber ring resonators have great interest due to different applications, especially in communication, secured communication, slow light, fast light and light storage in optical buffers. There are many proposed applications of optical ring resonators. Optical fiber ring resonators can be readily constructed from standard optical fiber components, which allow their properties to be studied in a systematic manner. In this paper, we describe our studies of the optical transmission, intensity, shift phase and group delay characteristics of a family of such devices. In this case, Gaussian beam has been used as an input pulse inside to microring resonators. In this paper, transmission, intensity, shift phase and group delay characteristics of device have been investigated. It has been compared together in different coupling coefficients in frame of linear and nonlinear.

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“…However, the method in Refs. [5][6][7] may gives the lineshape for any frequency detuning (for example, the periodic structure when the frequency range exceeds one FSR). Figures 1(a) and (d) show the lineshape of amplitude and phase shift with respect to the detuning ∆ for the under-coupled cavity (γ a in < ρ).…”

mentioning

confidence: 99%

Phase-sensitive reflection of squeezed vacuum field in optical cavity

Di¹,

Yu²,

Fang³

et al. 2012

中国光学快报

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We experimentally investigate the optical cavity for various coupled regimes with an injected squeezed vacuum state. We measure the quantum fluctuation spectra of the reflected field of an optical cavity using the homodyne detection and present the spectral dependence on the absorption and dispersion properties of the cavity in the under-coupled, critically-coupled, and over-coupled regimes. The spectra lineshape is phase sensitive with the phase shift induced by the cavity. Moreover, we find that the over-coupled optical cavity has obvious advantage in the manipulation of quantum fluctuation.OCIS codes: 190.4360, 230.1150, 270.1670. doi: 10.3788/COL201210.091901.The optical cavity has a wide range of applications in scientific and commercial instruments, such as laser, spectroscopy, frequency stabilization, etc. An important property of optical cavity is its dispersive and absorptive response. A cavity can be over-coupled, criticallycoupled (impedance matched) [1] , or under-coupled. The phase of the field reflected from the cavity is also important for frequency lock acquisition [2−4] and optical pulse transmission. More specifically, on-resonance, over-coupled cavity results in slow light, whereas undercoupled cavity results in fast light, and critically-coupled cavity results in zero reflection [5−7] . The quantum noise of light can be manipulated by employing the optical cavity. Quantum sidebands of bright light beam are modified by the optical cavity, in which original quantum phase fluctuations of the incident bright beam are converted into amplitude fluctuations [3,8−13] (note that only amplitude fluctuations of bright light beam can be detected directly by the photodiode). The tomography of quantum states of bright light beam can be performed using this method [10,11] . The quantum fluctuation spectra of the subharmonic reflected field of a degenerate optical parametric amplifier (OPA) inside an optical cavity have been studied theoretically [14] and experimentally [15] , which is driven by the squeezed vacuum state. The quantum fluctuation spectra for an optical empty cavity and the two-coupled cavities with an injected squeezed vacuum state have also been investigated in Refs. [15] and [16]. In these works, only over-coupled cavity is considered since its phase response undergoes a 2π phase shift. In this letter, we experimentally study the quantum fluctuation spectra of the reflected field from an optical cavity with various coupled regimes when injecting the squeezed vacuum state systematically. The squeezed quadrature components of the reflected beam of the optical cavity are measured by choosing the phase of the local beam relative to the input squeezed vacuum state. We demonstrate how the absorption and dispersion properties of the cavity determine the quantum fluctuation spectra of the reflected field. To the best of our knowledge, this work is completely different from the most previous studies for bright light injecting an optical cavity [3,8−13] . An optical cavity is assumed to be a st...

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Optical transmission characteristics of fiber ring resonators

Cited by 218 publications

References 17 publications

Importance of Intrinsic-$Q$ in Microring-Based Optical Filters and Dispersion-Compensation Devices

Importance of Intrinsic-$Q$ in Microring-Based Optical Filters and Dispersion-Compensation Devices

Modification of surface properties of bell metal by radiofrequency plasma polymerization

Phase-sensitive reflection of squeezed vacuum field in optical cavity

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