Correct troff usage; typo fixes.
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@ -99,7 +99,7 @@ atomic Quantum-state transitions in atoms.
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We can therefore with good fidelity define ``a clock'' to be the
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combination of an oscillator and a counting mechanism:
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.LP
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.PSPIC fig3.eps
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.if t .PSPIC fig3.eps
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.LP
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The standard second is currently defined as
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.QP
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@ -110,7 +110,7 @@ such seconds
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with an error less than ø2 cdot 10 sup{-15}ø [DMK2001] with commercially
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available products doing better than ø1 cdot 10 sup{-14}ø [AG2002].
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.LP
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Unlike other physical units with a conventionally defined origo,
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Unlike other physical units with a conventionally defined origin,
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longitude for instance, the ephemeral nature of time prevents us
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from putting a stake in the ground, so to speak, and measure from
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there. For measuring time we have to rely on ``dead reckoning'',
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@ -251,7 +251,7 @@ valuable property than precision, this is probably best explained
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using a graphic illustration of the difference between the two
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concepts:
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.LP
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.PSPIC fig1.eps
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.if t .PSPIC fig1.eps
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.LP
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In the top row we have instability, the bullet holes are spread over
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a large fraction of the target area.
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@ -272,7 +272,7 @@ gets too quantum-mechanical-oid to serve the instructional purpose.
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Transposing these four targets to actual clocks, the situation
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could look like the following plots:
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.LP
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.PSPIC fig2.eps
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.if t .PSPIC fig2.eps
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.LP
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On the x-axis we have time and on the y-axis how wrong the clock
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was at a given point in time.
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@ -712,7 +712,7 @@ suffered an interrupt which resulted in the above periodic processing
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can continue unaware of this afterwards and not suffer corruption
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or miscalculation even though it holds no locks on the shared
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meta-data.
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.PSPIC fig4.eps
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.if t .PSPIC fig4.eps
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.LP
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This scheme has an inherent risk that a process may be de-scheduled for
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so long time that it will not manage to complete the timestamping
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@ -901,7 +901,7 @@ Using a COTS product, ``HOT1'', from Virtual Computers Corporation
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[VCC2002] containing a FPGA chip on a PCI form factor card, a 26
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bit timecounter running at 100MHz was successfully implemented.
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.LP
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.PSPIC fig5.eps
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.if t .PSPIC fig5.eps
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.LP
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.LP
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In order to show that timestamping does not necessarily have to
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@ -925,7 +925,7 @@ This plot shows the timestamps corrected for this ``negative
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sawtooth correction''.
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.FE
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.LP
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.PSPIC gps.ps
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.if t .PSPIC gps.ps
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.LP
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It shold be noted that the author is no hardware wizard and
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a number of issues in the implementation results in less than
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@ -943,7 +943,7 @@ The average quality of crystals used for computers would
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totally obscure the curves due to their temperature coefficient.
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.FE
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.LP
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.PSPIC intr.ps
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.if t .PSPIC intr.ps
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.LP
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It is painfully obvious that the interrupt latency is the
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dominant noise factor in PPS timestamping in the second case.
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@ -1065,7 +1065,7 @@ Genius Who Solved the Greatest Scientific Problem of His
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Time" Penguin USA (Paper); ISBN: 0140258795.
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.LP
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[SAGE]
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This ``gee-wiz'' kind of article in Dr. Jobbs Journal is a goot place to
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This ``gee-wiz'' kind of article in Dr. Jobbs Journal is a good place to
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start:
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.br
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http://www.ddj.com/documents/s=1493/ddj0001hc/0085a.htm
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