SUBSCRIPTIONS & PRICING
GENERAL INFORMATION
chapter 9, Basic RF Definitions and IMD Effects on TV Picture
Table of Contents
- Part 1 System Overview
- 1. WDM, Fiber to the X, and HFC Systems: A Technical Review
- Part 2 Semiconductors and Passives
- 4. Introduction to Optical Fibers and Passive Optical Fiber Components
- Part 3 RF and Control Concepts
- 9. Basic RF Definitions and IMD Effects on TV Picture
- Part 4 Introduction to CATV MODEM and Transmitters
- 14. Quadrature Amplitude Modulation (QAM) in CATV Optical Transmitters
- Part 5 Digital Transceivers Performance
- 18. Introduction to Digital Data Signals and Design Constraints
- Part 6 Integration and Testing
- 20. Cross-Talk Isolation
- 21. Test Setups
Chapter Contents
- 9.1 Distortions and Dynamic Range
- 9.2 1-dB Compression Point and IP3 Relations
- 9.3 Amplifier Gain Reduction Due to Third-Order Nonlinearity
- 9.4 Cross Modulation Effects
- 9.5 AM-to-PM Effects
- 9.6 Multitone CTB Relations
- 9.7 RF Lineups, NF Calculations, and Considerations
- 9.8 RF Lineups, P1dB and IP3 Calculations, and Considerations
- 9.9 Mismatch Effects
- 9.10 CSO and CTB Distortion Effects on TV Picture
- 9.11 Main Points of this Chapter
- References
Excerpt
9.1 Distortions and Dynamic Range
Any active network can be described by the power series. This term is correct in the first approximation, when the system has no memory. Memory effects of an active system are caused by a time-varying phase response, which is, in turn, manifested in the frequency response. This phase response is referred to as the amplitude modulation (AM) to phase modulation (PM) characteristic. This phenomenon describes how the phase response is affected by input power. Under these terms of memory, the system is described by a Volterra series. The power series presentation here considers AM- to-PM effects only and the associated calculation is scalar only, which means a simple polynomial with real coefficients.
Assume an RF device such that its output voltage performance is described by power series at the operating frequency ω as follows:

Since the transfer function is not linear, intermodulation interference occurs, In fact, this power series can be referred to as a sum of transfer functions, where each one generates distortions of a different order. Presenting these arguments in a log scale would result in a linear function where its slope is the distortion order (the Y axis represents power in dBm, since 20 log of the voltage is measured, and the X axis is the input power). Thus, it can be written as

©2008 Society of Photo-Optical Instrumentation Engineers











This Publication
Google Scholar
PubMed