AM-PM conversion and related pump noise effects on parametric amplifiers and converters by S.I Ghobrial

Cover of: AM-PM conversion and related pump noise effects on parametric amplifiers and converters | S.I Ghobrial

Published by University of Bradford.Postgraduate School of Electrical and Electronic Engineering in Bradford .

Written in English

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Edition Notes

Book details

Statementby S.I.Ghobrial and J.G.Gardiner.
Seriesreports -- No.148.
ContributionsGardiner, J.G.
The Physical Object
Pagination18p.
Number of Pages18
ID Numbers
Open LibraryOL21532289M

Download AM-PM conversion and related pump noise effects on parametric amplifiers and converters

We demonstrate the suitability of the Raman-amplified pump for parametric amplification by characterizing its optical signal to noise ratio and relative intensity noise (RIN). The amplified pump is subsequently employed within a FOPA obtaining net gain of Cited by: 1.

Transfer of intensity noise from pumps to signal in dual-pump fiber-optic parametric amplifiers is simulated numerically for a realistic configuration in which both pumps are amplified and. In this paper, the effect of parametric amplifier pump phase noise on the cooling of a micromirror in an optomechanical system with an optical parametric amplifier inside the optical cavity is investigated theoretically.

It has been demonstrated that the photon number distribution of a parametric amplifier near the threshold of instability leads to improved cooling of the micromirror.

AM-PM conversion usually results due to nonlinear capacitors in power amplifier circuit. Fig.1 AM-AM/AM-PM conversion Equation Unit of AM-PM conversion is deg/dB QPSK constellation changes as shown in the fig.

2 due to AM-PM-conversion, but due to other impairments in the system such as AM-AM distortion, I-Q mismatch, phase noise etc. one cannot distinct whether the effect (constellation. Fig.1 AM-AM/AM-PM conversion Equation Unit of AM-AM conversion is dB/dB QPSK constellation changes as shown in the fig.

2 due to AM-AM-conversion, but due to other impairments in the system such as AM-PM distortion, I-Q mismatch, phase noise etc. one cannot distinct whether the effect (constellation change) is due to which of the impairments.

struggling with AM-PM conversion. Few discussions are available on the AM noise of different microwave components. In this paper we report the AM noise of different commercial amplifiers and oscillators at 10 GHz.

To adequately characterize the AM noise of high performance amplifiers, we design and investigate an. Raman-effect induced noise limits on (3) parametric amplifiers and wavelength converters Article (PDF Available) in Journal of Optics B Quantum and Semiclassical Optics 6(8) Noise Figure The noise in a parametric amplifler is generated by the circuit conductance Gs;G1 and G2.

The noise generated by the pump circuit conductance G3 can be normally neglected because the pump current iP(t) is usually very large and well approximated as a noise-free sinusoidal wave. The noise from the load conductance GL is.

Contrast limitation due to pump noise in an optical parametric chirped pulse amplification system. the restriction on the signal-to-noise ratio of the recompressed pulse arising from temporal noise on the pump.

The effect of pump noise has been studied experimentally by Forget et al Also shown is the pump to signal conversion efficiency.

Figure 1 – The intersection of 1/f noise and wideband noise lines form the 1/f corner commonly found in most amplifiers. The low-frequency noise grows inversely with frequency and is problematic in high-precision systems. In an effort to combat this noise source, a new class of devices has arrived that has solved the 1/f noise issue.

The effects of nonlinear distortion and amplifier noise on the scale of a WDM link are analyzed in [TO98]. Advances in tunable lasers and filters are described in [CM98b].

Wavelength converters are reviewed in [So96]. Issues in the design and performance of optical networks using wavelength conversion are reviewed in [RM98].

The noise performance of an erbium-doped fiber amplifier (EDFA) is characterized by modeling optical amplifiers as four-level or three-level systems. The gain and noise performance are then examined under forward and reverse pumping. It is found that a four-level system displays.

For laser amplifiers (based on stimulated emission, e.g. fiber amplifiers), the unavoidable excess noise can be regarded as arising from spontaneous emission of the gain medium into the amplified mode. For a four-level gain medium with a low-noise pump, the excess noise can approach the minimum quantum-mechanically allowed level.

(Note that the gain medium acts as an energy reservoir. The importance of large-signal converters becomes evident from a discussion of up-converters as well as of harmonic multipliers. “AM-PM Conversion and Related Pump Noise Effects in Parametric Amplifiers and Converters”; Tech.

Rpt., Univ. Bradford L.A. Blackwell, K.L. Kotzebue: Semiconductor-Diode Parametric Amplifiers (Prentice-Hall. The bandwidth of a single-pump fiber optical parametric amplifier is governed by the even orders of fiber dispersion at the pump wavelength.

The amplifier can exhibit gain over a wide wavelength. - Fiber Optical Parametric Amplifiers, Oscillators and Related Devices - by MICHEL E. MARHIC Excerpt. Introduction. Fiber optical parametric amplifiers (OPAs) exploit nonlinear optical properties of optical fibers.

Their operation is based on the third-order susceptibility χ (3) of the glasses making up the fiber core. While this. I will present recent results demonstrating frequency conversion with high gain and low noise figure in a fiber parametric amplifier.

Four-wave-mixing in these devices can also be used to realize. Nonlinear-optical (NLO) effects make possible devices that perform many functions, such as wavelength conversion and signal processing, while waveguides enable the devices to be both efficient and compact. This book presents a systematic description of the NLO field, with an emphasis on devices that use ferroelectric waveguides.

The earlier chapters provide an introduction to the concepts. How to Measure AM-PM Conversion. Preset the analyzer. Select an S21 measurement in the power-sweep mode.

Enter the start and stop power levels for the analyzer's power sweep. The start power level should be in the linear region of the amplifier's response.

Ultralow-Noise Parametric Amplifiers in Communication Satellite Earth Terminals. Author links open overlay panel C. Louis Cuccia. Show more. The parametric gain is used in optical parametric amplifiers. In optical parametric generators (OPG), on the other hand, the DFG process is seeded by quantum noise, so only a single pump wave is present at the input of a crystal.

An optical parametric oscillator (OPO) is essentially an OPG process realized inside a resonant cavity. power amplifier (PA) with baseband samples and then observes the result of that stimulus at the PA output.

Then, the amplitude-to- amplitude modulation (AM/AM) and amplitude-to-phase modulation (AM/PM) effects of the PA are estimat-ed distortions are then removed from the PA by pre-distorting the input stimulus with.

Locherer and R. Maurer, “ Nonreciprocal parametric amplifier converter with internal pump,” Patent USA (). We renewed the idea by replacing the tunnel diode with an SIS junction.

Our concept utilizes positive conversion gain by the quantum effect in. (Last Updated On: Ma ) This is the Multiple Choice Questions in Chapter 6: Receivers from the book Electronic Communication Systems by Roy you are looking for a reviewer in Communications Engineering this will definitely help.

Video shows what parametric amplifier means. a sensitive, low-noise amplifier of high-frequency or microwave radio waves that utilizes an inductor or.

Dealing with low amplitude signals can be challenging. In order to differentiate between the low level signal and the noise contributed by surrounding circuitry, we typically use gain to amplify the signal above the noise floor.

However, a standard amplifier configuration multiplies the input signal, the input noise, and the noise contribution of t. Effects of Nonlinearity 14 Harmonic Distortion 14 Gain Compression 16 Cross Modulation 20 Intermodulation 21 Cascaded Nonlinear Stages 29 AM/PM Conversion 33 Noise 35 Noise as a Random Process 36 Noise Spectrum 37 vii.

MT 1/f Corner Frequency is a figure of merit for op amp noise performance (the lower the better) Typical Ranges: 2Hz to 2kHz Voltage Noise and Current Noise do not necessarily have the same 1/f corner frequency.

3dB/Octave WHITE NOISE LOG f CORNER 1 f NOISE nV. Furthermore, the estimated SH-conversion efficiency of % W −1 is consistent with the obtained value of % W −1, which was estimated from the measurement of SH-conversion efficiency with a 3-mW μm-wavelength pump light shown in Fig.

1(d). These results indicate that our waveguide provides a highly efficient optical parametric. (FM) noise or rms frequency deviation can also be measured with an am- plitude (AM) detection system after the FM variations are converted to AM variations, as shown in Fig.

The FM-AM conversion is obtained by applying two signals in phase quadrature (90”) at the inputs to a balanced mixer (detector). Analog Devices' Selection Table for Low Noise Amplifiers lets you add, remove, and configure parameters to display; compare parts and choose the best part for your design.

Particularly, this introductory work attempts to make a connection between the nonlinearity characteristics (i.e., both joint and individual AM-AM and AM-PM conversion) of a high power amplifier (HPA) chain and the simulated EVM-SNR characteristics of specific digital communication signals (i.e., QPSK, 8-PSK and QAM) on this chain.

Fiber Optic Parametric Amplifiers - Free ebook download as PDF File .pdf), Text File .txt) or read book online for free. I investigated the impact of pump noise on the amplified signal in the context of intensity noise transfer. It is shown that the group-velocity dif- ference between the signal and pumps play an important role and.

Click here to go to our main amplifier page. New for June. Also known as paramps, parametric amplifiers use non-linear elements. While we wait for some IEEE MTT-S help on this topic, here is a book chapter on paramps.

Noise Performance of Single-Varactor Diode Parametric Circuits.- Noise Sources in Parametric Circuits.- Converters.- The Three-Frequency Converter.- The Four-Frequency Converter with Resistive Image Termination.- The Amplifier.- The Amplifier Without Circulator.- The Amplifier with Circulator.- power amplifiers with more than five times.

The measurement system is used for sampled input – output measurements of power amplifiers and the obtained data are fitted to different behavioral power amplifier models including memory.

Some different behavioral models are evaluated and compared for different kinds of power amplifiers. A neural.

pump energy savings with frequency converters Applying a frequency converter to a pump to reduce speed and therefore flow, causes the pump curve to shift down as shown in figure 4. Since the operating point is still the new reduced pump curve and the system curve, the same reduced flow (note GPM from GPM in figures) is achieved as with.

We find the use of amplifiers in medical devices, scientific equipment, automation, military tools, communication devices, and even in household equipment. In this tutorial, we will discuss all the important concepts from the introduction of transistors along with the amplifier action of transistor.

Amplifiers from Analog Devices deliver both high performance and high value. These amplifier ICs combine circuit design, manufacturing process innovation, and applications expertise to create products that simplify signal conditioning design.

We offer a variety of online and downloadable tools to help engineers quickly select the right amplifier. Abstract: This article examines key parameters that contribute to amplifier noise. It explains how amplifier design, specifically the choice of bipolar, JFET-input, or CMOS-input design, affects noise.

The note also explains how to select a low-noise amplifier for low-frequency analog applications such as buffering data converters, amplifying strain-gauge signals, and preamplifying microphone. Increased input capacitance requires a lower impedance virtual ground and lower feedback resistor to drive the input, thus increasing the noise (in addition to the voltage noise related effect discussed earlier).

How to Measure Noise of VOLTAGE AMPLIFIERS. To measure the noise of a voltage amplifier, the input is short‑circuited.Exercise 1: Find the bias point and the amplifier parameters of the circuit below.

(Si BJT with β =V A = V, ignore Early effect in bias calculations). This is a common collector amplifier (emitter follower). o Input at the base, output at the emitter. It has a .P. L. Voss and P. Kumar, ―Raman-effect induced noise-figure limit for c(3) parametric amplifiers and wavelength converters,‖ presented at the Optical Fiber Communications Conference (OFC‘), Los Angeles Convention Center, Los Angeles, CA, February 22–27, ; paper TuK4.

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