User`s guide
Table Of Contents
- Title Page
- Contents
- Getting Started
- Introduction and Measurement
- Phase Noise Basics
- Expanding Your Measurement Experience
- Starting the Measurement Software
- Using the Asset Manager
- Using the Server Hardware Connections to Specify the Source
- Setting GPIB Addresses
- Testing the 8663A Internal/External 10 MHz
- Testing the 8644B Internal/External 10 MHz
- Viewing Markers
- Omitting Spurs
- Displaying the Parameter Summary
- Exporting Measurement Results
- Absolute Measurement Fundamentals
- Absolute Measurement Examples
- Residual Measurement Fundamentals
- What is Residual Noise?
- Assumptions about Residual Phase Noise Measurements
- Calibrating the Measurement
- Measurement Difficulties
- Residual Measurement Examples
- FM Discriminator Fundamentals
- FM Discriminator Measurement Examples
- AM Noise Measurement Fundamentals
- AM Noise Measurement Examples
- Baseband Noise Measurement Examples
- Evaluating Your Measurement Results
- Advanced Software Features
- Reference Graphs and Tables
- Approximate System Noise Floor vs. R Port Signal Level
- Phase Noise Floor and Region of Validity
- Phase Noise Level of Various Agilent Sources
- Increase in Measured Noise as Ref Source Approaches DUT Noise
- Approximate Sensitivity of Delay Line Discriminator
- AM Calibration
- Voltage Controlled Source Tuning Requirements
- Tune Range of VCO for Center Voltage
- Peak Tuning Range Required by Noise Level
- Phase Lock Loop Bandwidth vs. Peak Tuning Range
- Noise Floor Limits Due to Peak Tuning Range
- Tuning Characteristics of Various VCO Source Options
- 8643A Frequency Limits
- 8644B Frequency Limits
- 8664A Frequency Limits
- 8665A Frequency Limits
- 8665B Frequency Limits
- System Specifications
- System Interconnections
- PC Components Installation
- Overview
- Step 1: Uninstall the current version of Agilent Technologies IO libraries
- Step 2: Uninstall all National Instruments products.
- Step 3: Install the National Instruments VXI software.
- Step 4: Install the National Instruments VISA runtime.
- Step 5: Install software for the NI Data Acquisition Software.
- Step 6: Hardware Installation
- Step 7. Finalize National Instruments Software Installation.
- Step 8: System Interconnections
- Step 9: Install Microsoft Visual C++ 2008 Redistributable Package use default settings
- Step 10: Install the Agilent I/O Libraries
- Step 11: Install the E5500 Phase Noise Measurement software.
- Step 12: Asset Configuration
- Step 13: License Key for the Phase Noise Test Set
- Overview
- PC Digitizer Performance Verification
- Preventive Maintenance
- Service, Support, and Safety Information
- Safety and Regulatory Information
- Safety summary
- Equipment Installation
- Environmental conditions
- Before applying power
- Ground the instrument or system
- Fuses and Circuit Breakers
- Maintenance
- Safety symbols and instrument markings
- Regulatory Compliance
- Declaration of Conformity
- Compliance with German noise requirements
- Compliance with Canadian EMC requirements
- Service and Support
- Return Procedure
- Safety and Regulatory Information

FM Discriminator Fundamentals
9
Agilent E5505A User’s Guide 247
The double-balanced mixer, acting as a phase detector, transforms the
instantaneous phase fluctuations into voltage fluctuations ( ). With the
two input signals 90° out of phase (phase quadrature), the voltage out is
proportional to the input phase fluctuations. The voltage fluctuations can then
be measured by the baseband analyzer and converted to phase noise units.
The discriminator transfer response
The important equation is the final magnitude of the transfer response.
Where represents the voltage fluctuations out of the discriminator and
represents the frequency fluctuations of the DUT. is the phase
detector constant (phase to voltage translation). is the amount of delay
provided by the delay line and is the frequency offset from the carrier that
the phase noise measurement is made.
System sensitivity
A frequency discriminator’s system sensitivity is determined by the transfer
response. As shown below, it is desirable to make both the phase detector
constant and the amount of delay large so that the voltage fluctuations
out of a frequency discriminator will be measurable for even small
fluctuations .
The magnitude of the sinusoidal output term or the frequency discriminator is
proportional to . This implies that the output response will have
peaks and nulls, with the first null occurring at . Increasing the rate of
a modulation signal applied to the system will cause nulls to appear at
frequency multiples of (Figure 179).
Δφ ΔV→
ΔVf
m
() K
φ
2πτ
d
Δff
m
()
πf
m
τ
d
()sin
πf
m
τ
d
()
-----------------------------
=
ΔVf
m
()
Δffm()
Kφ
τd
f
m
Kφ
τd
ΔV
Δf
ΔVf
m
() K
φ
2πτ
d
πf
m
τ
d
()sin
πf
m
τ
d
()
-----------------------------
Δffm()()=
NOTE
The system sensitivity is independent of carrier frequency .
f
o
πf
m
τ
d
()πf
m
τ(⁄n
m 1 τd⁄=
1 τd⁄