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@@ -21,7 +21,7 @@
\contentsline {figure}{\numberline {3.7}{\ignorespaces Demodulation of the L1 GPS signal.\relax }}{25}{figure.caption.25}
\contentsline {figure}{\numberline {3.8}{\ignorespaces Comparison between the original C/A code generated on the GPS satellite with two synthesized PRN codes with a different phase shift on the receiver. Image courtesy of \citep {understandGPS}.\relax }}{26}{figure.caption.26}
\contentsline {figure}{\numberline {3.9}{\ignorespaces Segment of the frequency/code delay search space for a single GPS satellite. Image courtesy of \citep {diggelen2009a-gps}.\relax }}{28}{figure.caption.27}
-\contentsline {figure}{\numberline {3.10}{\ignorespaces Basic AGPS principle\relax }}{29}{figure.caption.28}
+\contentsline {figure}{\numberline {3.10}{\ignorespaces Basic AGPS principle.\relax }}{29}{figure.caption.28}
\addvspace {10\p@ }
\contentsline {figure}{\numberline {4.1}{\ignorespaces RRLP Request protocol. Assistance data can be sent before the request is made. If the assistance data are sent, their reception acknowledgement is sent as a response from the MS. Image courtesy of \citep {harper2010server-side} and \citep {04.31V8.18.0}.\relax }}{32}{figure.caption.29}
\contentsline {figure}{\numberline {4.2}{\ignorespaces An example of constructing an RRLP request. Image courtesy of \citep {harper2010server-side}.\relax }}{37}{figure.caption.30}
@@ -36,8 +36,8 @@
\contentsline {figure}{\numberline {6.1}{\ignorespaces Test rooms as well as the results delivered by the smart phones. Image courtesy of Google Maps.\relax }}{59}{figure.caption.39}
\contentsline {figure}{\numberline {6.2}{\ignorespaces Test room 2 with the positions of the smart phones.\relax }}{60}{figure.caption.40}
\addvspace {10\p@ }
-\contentsline {figure}{\numberline {C.1}{\ignorespaces Effects of the low frequency term on the demodulated output C/A wave on the GPS receiver (the explanations and figures are from top to bottom). If the synthesized frequency is correct, $f_{1}=f_{2}$, the low frequency term becomes a DC term and does not modify the output $d_{C/A}$ wave (first figure). If the frequency matches but the phase not, in this case the phase is shifted for $\pi $, then $d_{C/A}$ is inverted (second figure). If the phase shifts with time, then the amplitude and phase of $d_{C/A}$ will vary as well (third figure). Image courtesy of \citep {diggelen2009a-gps}.\relax }}{86}{figure.caption.48}
-\contentsline {figure}{\numberline {D.1}{\ignorespaces Cross-correlation on three different signals. Image courtesy of \citep {understandGPS}.\relax }}{87}{figure.caption.49}
-\contentsline {figure}{\numberline {F.1}{\ignorespaces Basic distance estimation principle for one satellite. Image courtesy of \citep {understandGPS}.\relax }}{91}{figure.caption.53}
-\contentsline {figure}{\numberline {F.2}{\ignorespaces Estimating the distance by phase shift $\Delta t =t_2 - t_1 =\tau $. Image courtesy of \citep {understandGPS}.\relax }}{92}{figure.caption.54}
-\contentsline {figure}{\numberline {F.3}{\ignorespaces Taylor series approximation for a point $a=0.5$ where $n$ is the Taylor polynomial degree.\relax }}{94}{figure.caption.55}
+\contentsline {figure}{\numberline {C.1}{\ignorespaces Effects of the low frequency term on the demodulated output C/A wave on the GPS receiver (the explanations and figures are from top to bottom). If the synthesized frequency is correct, $f_{1}=f_{2}$, the low frequency term becomes a DC term and does not modify the output $d_{C/A}$ wave (first figure). If the frequency matches but the phase not, in this case the phase is shifted for $\pi $, then $d_{C/A}$ is inverted (second figure). If the phase shifts with time, then the amplitude and phase of $d_{C/A}$ will vary as well (third figure). Image courtesy of \citep {diggelen2009a-gps}.\relax }}{88}{figure.caption.51}
+\contentsline {figure}{\numberline {D.1}{\ignorespaces Cross-correlation on three different signals. Image courtesy of \citep {understandGPS}.\relax }}{89}{figure.caption.52}
+\contentsline {figure}{\numberline {F.1}{\ignorespaces Basic distance estimation principle for one satellite. Image courtesy of \citep {understandGPS}.\relax }}{93}{figure.caption.56}
+\contentsline {figure}{\numberline {F.2}{\ignorespaces Estimating the distance by phase shift $\Delta t =t_2 - t_1 =\tau $. Image courtesy of \citep {understandGPS}.\relax }}{94}{figure.caption.57}
+\contentsline {figure}{\numberline {F.3}{\ignorespaces Taylor series approximation for a point $a=0.5$ where $n$ is the Taylor polynomial degree.\relax }}{96}{figure.caption.58}