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 249
Optimum sensitivity
If measurements are made such that the offset frequency of interest ( ) is
<1/2 the sin(x)/x term can be ignored and the transfer response can be
reduced to
where is the discriminator constant.
The reduced transfer equation implies that a frequency discriminator’s system
sensitivity can be increased simply by increasing the delay or by increasing
the phase detector constant . This assumption is not completely correct.
is dependent on the signal level provided by the delay line and cannot exceed a
device dependent maximum. This maximum is achieved when the phase
detector is operating in compression
1
. Increasing the delay will reduce the
signal level out of the delay line often reducing the sensitivity of the phase
detector. Optimum system sensitivity is obtained in a trade-off between delay
and attenuation.
Sensitivity = K
L
V
in
LX(10)
−LZ/20
Where K
L
is the phase detector efficiency, V
in
is the signal voltage into the
delay line, LX (dB) is the sensitivity provided by the delay line and LZ is the
attenuation of the delay line. Taking the derivative with respect to the length L
to find the maximum of this equation results in
LZ = 8.7 dB of attenuation
The optimum sensitivity of a system with the phase detector operating out of
results from using a length of coaxial line that has 8.7 dB of attenuation.
One way to increase the sensitivity of the discriminator when the phase
detector is out of compression is to increase the signal into the delay line. This
can be accomplished with an RF amplifier before the signal splitter. The noise
of the RF amplifier will not degrade the measurement if the two-port noise of
the amplifier is much less than the noise of the DUT. However, some
attenuation may be needed in the signal path to the reference input to the
double-balanced mixer (phase detector) to protect it from excessive power
levels.
If the amplifier signal puts the phase detector into compression, is at its
maximum and system sensitivity is now dependent on the length of the delay
. For maximum sensitivity more delay can be added until the signal level out
of the delay line is 8.7 dB below the phase detector compression point.
The following example illustrates how to choose a delay line that provided the
optimum sensitivity given certain system parameters. (See Table 39 on
page 250).
1 Compression: The level of the output signal at which the gain of a device is reduced by a specific amount,
usually expressed in decibels (dB), as in the 1 dB compression point.
f
m
πτ
d
ΔVf
m
() K
d
Δff
m
() K
φ
πτ
d
Δff
m
(==
K
d
τ
d
K
φ
K
φ
τ
d
K
φ
τ
d