90
Appendix B: Theory of Operation
Instead of computing the magnitude-squared of the DFT to obtain an estimate of the PSD, the
5120A computes the cross-spectrum of two identical measurement systems as shown in
. The ADC noise is highly uncorrelated and averages down, allowing improvement of the
broadband noise floor to better than –170 dBc/Hz.
Figure B-6: 5120A and 5120A-01 with external reference: The PSD is computed as the cross-spectrum of the DFTs
from two identical processing front ends.
The 5120A-01 computes the cross-spectrum of two identical measurement systems as shown in
. The ADC noise and the internal reference oscillator noise are highly uncorrelated and
average down, allowing improvement of the broadband noise floor to fall below –170 dBc/Hz with
only one instrument input.
Figure B-7: 5120A-01 with internal references: The PSD is computed as the cross-spectrum of the DFTs from two
identical processing front ends.
Sample,
Down-convert,
& Transform A
Input 1
Reference 2
S
Φ
1
Φ
2
–
Multiply
Φ
1
A
Φ
2
A
Φ
ADC1A
Φ
ADC2A
–
+
–
Sample,
Down-convert,
& Transform B
Σ
Σ
Φ∗
1
B
Φ∗
2
B
Φ∗
ADC1B
Φ∗
ADC2B
–
+
–
Uncorrelated
Sample,
Down-convert,
& Transform A
Input
S
Φ
1
Φ
1
A
Φ
2
A
Φ
ADC1A
Φ
ADC2A
–
+
–
Sample,
Down-convert,
& Transform B
Σ
Φ∗
1
B
Φ∗
2
B
Φ∗
ADC1B
Φ∗
ADC2B
–
+
–
Uncorrelated
Internal
Reference 2
2
3
1
Multiply
Internal
Reference 1
Summary of Contents for 5115A
Page 6: ...iv Contents Index 97 ...
Page 12: ...6 1 Introduction ...
Page 16: ...10 2 Setting Up a PNTS ...
Page 26: ...20 3 The Screen and Basic Concepts ...
Page 82: ...76 9 Maintaining a PNTS ...
Page 92: ...86 Appendix A Specifications ...
Page 98: ...92 Appendix B Theory of Operation ...
Page 100: ...94 ...
Page 102: ...96 ...
Page 106: ...100 ...