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Note that there is a gap where the BER is so close to 10
-12
that we cannot
decide. For example, if we compared 3 × 10
12
bits and got two errors (a
measured BER of 0.667 × 10
-12
), we are in the "uncertain" white area on
the graph.
In such a case, we need to transmit more bits until the number of bits
either reaches the upper limit (6.296 × 10
12
), or until we see more errors.
If the actual BER is very close to 10
-12
, however, we are unable to apply
a lower or upper limit to the BER, no matter how many bits we transmit.
Whether such a test fails or passes depends entirely on the application.
Once we are able to decide for a measured point whether its BER is
above or below the BER threshold, we can determine the total jitter at
the intersection of the BER threshold with the bathtub curve.
Since we are unable to find a single point on the slope where the BER
is exactly 10
-12
, we search for an interval that brackets the point at which
the BER is equal to 10
-12
. This is illustrated for the left-hand slope in the
following figure.
5
Advanced Analysis
180
Agilent J-BERT N4903 High-Performance Serial BERT
The Bracketing Approach
Содержание J-BERT N4903
Страница 1: ...S Agilent J BERT N4903 High Performance Serial BERT User Guide s Agilent Technologies...
Страница 68: ...2 Setting up Patterns 68 Agilent J BERT N4903 High Performance Serial BERT...
Страница 158: ...4 Setting up the Error Detector 158 Agilent J BERT N4903 High Performance Serial BERT...
Страница 314: ...6 Evaluating Results 314 Agilent J BERT N4903 High Performance Serial BERT...
Страница 374: ...7 Jitter Tolerance Tests 374 Agilent J BERT N4903 High Performance Serial BERT...
Страница 394: ...8 Solving Problems 394 Agilent J BERT N4903 High Performance Serial BERT...
Страница 434: ...Index 434 Agilent J BERT N4903 High Performance Serial BERT...