2006
DOI: 10.1109/jlt.2006.874652
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Photonic microwave tunable single-bandpass filter based on a Mach-Zehnder interferometer

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Cited by 269 publications
(117 citation statements)
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“…3. In this case, note that the fundamental electrical transfer function has a single bandpass centered at the designed frequency f o = 4.56 GHz since the optical source has a gaussian profile sliced with a sinusoidal pattern [12]. Note that this filter is more selective as compared to the previous case and, therefore, it is expected that the nonlinear electrical responses have a different behaviour.…”
Section: Resultsmentioning
confidence: 93%
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“…3. In this case, note that the fundamental electrical transfer function has a single bandpass centered at the designed frequency f o = 4.56 GHz since the optical source has a gaussian profile sliced with a sinusoidal pattern [12]. Note that this filter is more selective as compared to the previous case and, therefore, it is expected that the nonlinear electrical responses have a different behaviour.…”
Section: Resultsmentioning
confidence: 93%
“…Also, we experimentally show the harmonic distortion of two different microwave photonic filtering structures which are based on the slicing of a broadband source (BBS) combined with a dispersive single mode fiber (SMF) link. We consider a discrete slicing achieved by a structure of AWGs obtaining a periodical electrical response [9] and a quasi-continuous slicing by means of a Mach-Zenhder Interferometer (MZI) yielding a non-periodic response [12]. The experimental and theoretical analysis of these electrical responses yield an excellent agreement revealing the interest of considering this harmonic distortion model on the design of advanced microwave photonic filters to exploit the MWP benefits.…”
Section: Introductionmentioning
confidence: 94%
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“…Phase dependence can be developed by means of a Taylor expansion around the central frequency of the optical source ω 0 [16]:…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…To satisfy the requirement of incoherent summing, either the laser coherence time must be shorter than the optical delay time, or the state of polarization ͑SOP͒ of the optical signals must be orthogonal. For the first approach, a laser array 3 or a sliced wideband source 4 is used, but these increase the complexity of the system. If a single-wavelength laser source is used, either a long time delay line is required, 5 which restricts the free spectral range ͑FSR͒, or the optical mixing effect is used, 6 which increases the system cost.…”
Section: Introductionmentioning
confidence: 99%