Related Experiment Video
Updated: Feb 23, 2026

06:42
Generation and Coherent Control of Pulsed Quantum Frequency Combs
Published on: June 8, 2018
9.8K
Power Spectrum Computation for an Arbitrary Phase Noise Using Middleton's Convolution Series: Implementation
IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control
|September 8, 2017
Summary
This study simplifies calculating the power spectrum of periodic signals using phase noise power spectral density. The new method offers intuitive understanding and accurate results for lasers and oscillators.
Area of Science:
- Physics
- Signal Processing
- Optical Engineering
Background:
- Phase noise power spectral density is crucial for understanding periodic signals in systems like lasers and oscillators.
- Existing methods for power spectrum calculation can be complex.
Purpose of the Study:
- To revisit and simplify the calculation of power spectrum from phase noise power spectral density.
- To provide a straightforward guideline for computing power spectra for arbitrary phase noise.
- To offer intuitive understanding of phase noise effects on spectral line shape.
Main Methods:
- Revisiting Middleton's convolution series for power spectrum analysis.
- Developing a simplified computational guideline for arbitrary phase noise.
- Applying the method to experimental signals with varying phase noise levels.
Main Results:
- A straightforward method for computing the power spectrum from phase noise power spectral density was introduced.
- The approach demonstrated computational benefits.
- Excellent agreement was observed between computed and experimental spectra across different phase noise regimes.
Conclusions:
- The revisited convolution series offers an intuitive and computationally efficient way to determine the power spectrum of periodic signals.
- This method is broadly applicable to scientific areas involving lasers and oscillators.
- The approach enhances understanding of phase noise impacts on spectral characteristics.
Related Concept Videos
Convergence of Fourier Series
462
The Fourier series is a powerful mathematical tool for representing periodic signals as an infinite sum of complex exponentials. In practice, this infinite series is truncated to a finite number of terms, yielding a partial sum. This truncation makes the approximation of the signal feasible but introduces certain challenges, particularly near discontinuities, known as the Gibbs phenomenon.
The Gibbs phenomenon refers to the persistent oscillations and overshoots that occur near discontinuities...
The Gibbs phenomenon refers to the persistent oscillations and overshoots that occur near discontinuities...
462
Parseval's Theorem
1.2K
Parseval's theorem is a fundamental concept in signal processing and harmonic analysis. It asserts that for a periodic function, the average power of the signal over one period equals the sum of the squared magnitudes of all its complex Fourier coefficients. This theorem, named after Marc-Antoine Parseval, provides a powerful tool for analyzing the energy distribution in signals.
Interestingly, Parseval's theorem also holds for the trigonometric form of the Fourier series, which expresses a...
Interestingly, Parseval's theorem also holds for the trigonometric form of the Fourier series, which expresses a...
1.2K
Graphical and Analytic Representation of Sinusoids
1.0K
Analyzing two sinusoidal voltages with equal amplitude and period but different phases on an oscilloscope, an instrument used to display and analyze waveforms, involves a three-step process.
The first step is measuring the peak-to-peak value, which is twice the amplitude of the sinusoid. This provides information about the maximum voltage swing of the waveform.
Secondly, the period and angular frequency are determined. The period is the time taken for one complete cycle of the waveform, while...
The first step is measuring the peak-to-peak value, which is twice the amplitude of the sinusoid. This provides information about the maximum voltage swing of the waveform.
Secondly, the period and angular frequency are determined. The period is the time taken for one complete cycle of the waveform, while...
1.0K
Time and frequency -Domain Interpretation of Phase-lead Control
487
Phase-lead controllers are commonly used in various control systems to enhance response speed and stability. Adjusting the brightness on a television screen offers a practical example of phase-lead control. When contrast is enhanced, a phase-lead controller is employed. Mathematically, phase-lead control is identified when the first parameter is smaller than the second.
The design of phase-lead control involves the strategic placement of poles and zeros to balance steady-state error and system...
The design of phase-lead control involves the strategic placement of poles and zeros to balance steady-state error and system...
487
Phasors
1.3K
Phasors are a powerful mathematical tool used to analyze alternating current (AC) circuits. They provide a complex number representation of sinusoids, with the magnitude of the phasor equating to the amplitude of the sinusoid and the angle of the phasor representing the phase measured from the positive x-axis.
One of the significant benefits of using phasors is that they simplify the analysis of AC circuits by eliminating the time dependence of the current and voltage. This transformation...
One of the significant benefits of using phasors is that they simplify the analysis of AC circuits by eliminating the time dependence of the current and voltage. This transformation...
1.3K
Phasor Arithmetics
887
Phasors and their corresponding sinusoids are interrelated, offering unique insights into the behavior of alternating current (AC) circuits. One way to understand this relationship is through the operations of differentiation and integration in both the time and phasor domains.
When the derivative of a sinusoid is taken in the time domain, it transforms into its corresponding phasor multiplied by j-omega (jω) in the phasor domain, where j is the imaginary unit, and ω is the angular...
When the derivative of a sinusoid is taken in the time domain, it transforms into its corresponding phasor multiplied by j-omega (jω) in the phasor domain, where j is the imaginary unit, and ω is the angular...
887

