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| author | Philipp Le <philipp-le-prviat@freenet.de> | 2020-05-27 00:59:00 +0200 |
|---|---|---|
| committer | Philipp Le <philipp-le-prviat@freenet.de> | 2021-03-04 01:31:57 +0100 |
| commit | f6a45ff2a7bf405da58872611c74fd6bab1d6994 (patch) | |
| tree | 0a571e1d42defbfbefee4ebc4906a005b88f81c9 /chapter04/content_ch04.tex | |
| parent | 7006abf6dbac4d18172786140e81431a1b237c9a (diff) | |
| download | dcs-lecture-notes-f6a45ff2a7bf405da58872611c74fd6bab1d6994.zip dcs-lecture-notes-f6a45ff2a7bf405da58872611c74fd6bab1d6994.tar.gz dcs-lecture-notes-f6a45ff2a7bf405da58872611c74fd6bab1d6994.tar.bz2 | |
WIP: Chapter 5
Diffstat (limited to 'chapter04/content_ch04.tex')
| -rw-r--r-- | chapter04/content_ch04.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/chapter04/content_ch04.tex b/chapter04/content_ch04.tex index e93f287..6cd3635 100644 --- a/chapter04/content_ch04.tex +++ b/chapter04/content_ch04.tex @@ -2146,7 +2146,7 @@ The dynamic range increases, when more bits $B$ are added. However, the number o % %Analogous to the thermal noise floor, -\subsection{Time Recovery} +\subsection{Synchronization 1: Time Recovery} For wideband \ac{RF} applications, the sampling rate is chosen close to the maximum frequency of the signal, so that the Shannon-Nyquist sampling theorem can be fulfilled. |