<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD v1.0 20120330//EN" "JATS-archivearticle1.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta>
      <journal-title-group>
        <journal-title>Work-in-Progress in Hardware and Software for Location Computation, June</journal-title>
      </journal-title-group>
    </journal-meta>
    <article-meta>
      <title-group>
        <article-title>GNSS Jammer Localization in Urban Areas Based on Carrier-to-Noise Ratio and Classification Methods</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Zhe Yan</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Ahmed Al-Tahmeesschi</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Titti Malmivirta</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Laura Ruotsalainen</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Department of Computer Science, University of Helsinki</institution>
          ,
          <addr-line>Helsinki</addr-line>
          ,
          <country country="FI">Finland</country>
        </aff>
      </contrib-group>
      <pub-date>
        <year>2023</year>
      </pub-date>
      <volume>0</volume>
      <fpage>6</fpage>
      <lpage>08</lpage>
      <abstract>
        <p>Global Navigation Satellite Systems (GNSS) are the primary sources of accurate Position, Navigation, and Time (PNT) information to critical infrastructures. As a result, the localization of an intentional jamming source is an important step in securing GNSS resilience as it provides the authorities with technical tools to prevent the jamming action. However, conventional jammer localization methods are all in a way limited in urban areas, and the non-line-of-sight and multipath receptions that are frequently encountered are not well addressed. So in this work, a ray-tracing method is used to simulate the jamming propagation in a real urban environment, and a receiver characterization method is provided to obtain the efective carrier-to-noise ratio measurement. Besides, diferent support-vector-machine-based methods are used to determine the jammer location as a classification problem. A preliminary result with a validation accuracy of 96.2% is provided and proves the feasibility of this method. In the end, the drawbacks and future work plan are summarized.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;GNSS</kwd>
        <kwd>jammer localization</kwd>
        <kwd>urban areas</kwd>
        <kwd>classification</kwd>
        <kwd>machine learning</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        Localization of an intentional jamming source is an important step in securing GNSS
resilience as it provides the authorities with tools to prevent the continuation of a detected
jamming action. However, the complex signal propagation in dense urban areas makes
localization a challenging problem for conventional techniques. Generally, the measurements for
jammer localization can be categorized as Received Signal Strength (RSS)/Diferential
Received Signal Strength (DRSS), Angle of Arrival (AOA)/Direction of Arrival (DOA), Time
of Arrival (TOA)/Time Diference of Arrival (TDOA), and Frequency Diference of Arrival
(FDOA) [
        <xref ref-type="bibr" rid="ref5 ref6">5, 6</xref>
        ]. The possibility of using automatic gain control (AGC) for jammer localization
has been studied in [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ], where the 2D-position of an interference source can be solved by the
AGC values from at least three monitoring stations. However, the AGC may saturate [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ] and
the localization accuracy declines rapidly for long-distance interference source [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ]. Use of DRSS
can solve the problem of unknown transmitter power [
        <xref ref-type="bibr" rid="ref5">5</xref>
        ], [
        <xref ref-type="bibr" rid="ref9">9</xref>
        ] and [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ]. However, for dense urban
environments, the none-line-of-sight (NLOS) reception and multipath [11] efect may
deteriorate the positioning accuracy significantly, because even simple ground reflections can severely
afect the RSS-based methods [12]. AOA is not as popular as other methods because it has the
highest implementation complexity. To obtain the AOA measurements, antenna arrays or the
antenna that can be precisely rotated or moved are needed [
        <xref ref-type="bibr" rid="ref4">4, 13</xref>
        ]. AOA performance is also
poor in the presence of NLOS and multipath signals [
        <xref ref-type="bibr" rid="ref5">5</xref>
        ]. TDOA has been widely used and well
developed in radio-network-based navigation systems, but it requires accurate synchronization
of the receiver clock among all the monitors to acquire range information, which brings
dififculties to implementation. The main disadvantage of TDOA is that it is only suitable for
wide-band interference localization [14]. One way to improve this is to use TDOA in
combination with some other localization techniques, for example, [15] combines it with AGC, and [14]
with AOA, while [16] suggests the jointly estimation of TDOA and FDOA. Another problem
is that GNSS signals themselves, as the in-band signals for the jamming, will cause additional
peaks in the cross-correlation for TDOA systems [17]. in order to localize moving emitters.
Mainly working well for narrow-band interference, FDOA requires the relative movement
between the jammer and monitor nodes as well as precise timing and frequency synchronization,
and is usually used together with TDOA [18, 19].
      </p>
      <p>
        Carrier-to-noise ratio (C/N0) is commonly used as an indicator for jamming detection [20],
and is receiving increasing attention to be used as the measurement for jammer localization.
Because (C/N0) requires no complex equipment, and methods using it can be easily
implemented using of-the-shelf receivers. By constructing a model that describes the variation of
C/N0 as a function of the distance between the target receiver and interference source, the
localization performance is validated without considering the NLOS and multipath reception
[
        <xref ref-type="bibr" rid="ref4">4, 21</xref>
        ]. LOS, NLOS and difraction loss models are used to simulate the jamming signals, and
a linear formula is fitted to obtain the corresponding efective C/N0 in [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ], but the simulation
details are not given.
      </p>
      <p>As a result, though using C/N0 as the measurement for jammer localization is a promising
and attractive method, the limitation in urban area remains a significant problem. The
effective C/N0 impacted by reflected and difracted jamming signals is dificult to be modeled.
Fortunately, the well-explored ray-tracing technologies in mobile-communication community
and the use of machine learning models provide good tools to solve this problem. So in this
work, ray-tracing technology is used to simulate the jamming propagation in a real-life urban
area. And the efective C/N0 outputs of a commercial GNSS receiver under jamming are
modeled. Then, the obtained efective C/N0 is used as the measurement, and the jammer
localization is described as a classification problem.</p>
      <p>Ci/N0|eff =</p>
      <p>Ci
N0 + kJ
=</p>
      <p>1
Ci
N0 · 1 + k NJ0 ,
where Ci is the received signal power of the ith satellite, N0 is the noise power spectral density,
and J is the received jamming power. k is the Spectral Separation Coeficient (SSC) which
models the filtering efect of the receiver on the jamming signal. (1) is converted to log scale
as</p>
      <p>The rest of this article is organized as follows: the efective carrier-to-noise ratio model is
given in section 2. Then, the ray-tracing propagation model is introduced in section 3. Section
4 describes the receiver characterization and modeling. Next, in section 5, a preliminary result
is provided which demonstrates the efectiveness of this method in urban jammer localization.</p>
      <sec id="sec-1-1">
        <title>At last, the work plan for the future is given.</title>
      </sec>
    </sec>
    <sec id="sec-2">
      <title>2. Efective Carrier-to-noise ratio</title>
      <p>Supposing C/N0 is the carrier-to-noise ratio without jamming, the efective</p>
      <sec id="sec-2-1">
        <title>C/N0 output of</title>
        <p>the receiver under jamming can be modeled by
where the jamming power J is expressed in dBW.</p>
        <p>
          Using the jamming resistance quality factor Q, another expression of (1) given by [
          <xref ref-type="bibr" rid="ref8">8</xref>
          ] is
Ci/N0|eff,dB - Hz = Ci/N0|dB - Hz − 10log10 1 + k
J )︃
N0
.
        </p>
        <p>After this conversion to logarithmic scale, we can obtain the commonly used C/N0 that is
expressed in dB-Hz. Assuming that the jamming power J is considered significantly larger
than noise N0, namely k NJ0 ≫</p>
      </sec>
      <sec id="sec-2-2">
        <title>1, we can obtain [4]</title>
        <p>Ci/N0|eff,dB - Hz ≈</p>
        <p>Ci/N0|dB - Hz − 10log10</p>
        <p>− J |dBW,
C/N0|eff =</p>
        <p>1
1
C/N0</p>
        <p>J
+ SQRC
where S is the satellite signal power and RC is the spreading code rate. (4) is converted to log
C/N0|eff,dB - Hz = C/N0|dB - Hz − 10log10 1 +
C/N0 J )︃ .</p>
        <sec id="sec-2-2-1">
          <title>SQRC</title>
          <p>scale as
obtain
where SQRC actually functions in the same way with k.</p>
          <p>Assuming that the jamming signal power is much greater than the satellite signal, we can
C/N0|eff,dB - Hz ≈</p>
          <p>C/N0|dB - Hz − 10log10
︃( C/N0 )︃</p>
        </sec>
        <sec id="sec-2-2-2">
          <title>SQRC</title>
          <p>− J |dBW,
︃(
︃( k )︃</p>
          <p>N0
︃(
(1)
(2)
(3)
(4)
(5)
(6)</p>
        </sec>
      </sec>
    </sec>
    <sec id="sec-3">
      <title>3. Ray-tracing propagation model</title>
      <p>
        We have experimented the method using simulated signals. A ray-tracing technique based on
real-life city model is developed to guarantee the high dfielity of signal propagation in urban
environments. Diferent from the theoretical and empirical models which provide simple formulas
for the path-loss calculation, such as, [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ], [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ], and the standards recommended by the
International Telecommunication Union-Radiocommunication Sector (ITU-R), ray-tracing is a general
propagation modeling tool that provides estimates of path loss, angle of arrival/departure, and
time delays by numerically solving Maxwell’s equations [22].
      </p>
      <p>Herein, the Shooting and Bouncing Ray (SBR) [23] provided by MATLAB and the city
model from OpenStreetMap are used to simulate the jamming signal propagation loss in Sello
shopping center area of Espoo, Finland. The layout of this area can be seen in Figure 1.</p>
      <p>
        By the ray-tracing method introduced in this section, the received jamming power J at each
monitor can be obtained.
4. Receiver characterization and modeling
Apart from the J obtained from section 3, the spectral separation coeficient k or the jamming
resistance quality factor Q needs to be modeled to obtain the efective C/N0 measurement,
according to (3) or (6). Though these two values can be learned automatically in the training,
we need to determine k first to simulate a jamming scenario. To keep the high fidelity with
the future practical real-life validation, a popular and low-cost Ublox F9P GNSS receiver is
chosen for the efective C/N0 modeling. Generally, most of the jamming devices transmit a
swept tone waveform (chirp) which can be generated from inexpensive devices and is quite
efective in rendering GNSS inoperable [
        <xref ref-type="bibr" rid="ref10 ref2">2, 10</xref>
        ]. Here, the chirp signal transmit powers ranging
from -130 ˜-35 dBm by step 5 dBm, in a 10 MHz band centered at L1 1575.42 MHz, and with
a sweep time of 10 µ s were simulated. The chirp signal can be modeled as the combination of
(7)
(8)
multiple saw-tooth functions according to the following expressions[
        <xref ref-type="bibr" rid="ref10">10</xref>
        ]
      </p>
      <p>︄(
x (t) = a sin 2π ∑+∞︂ (︃ ∫︂ t
h=0
0
f1 (︁ t′ − h · Tsw,1)︁ · dt′ + · · ·</p>
      <p>fn (︁ t′ − h · Tsw,n)︁ · dt′
+
∫︂ t</p>
      <p>0
fn (t) =
︃{ f0,n + ku,nt,
f0,n + (ku,n − kd,n) Tu,n + kd,nt, Tu,n ≤ t &lt; Tsw,n
0 ≤ t &lt; Tu,n
where fn(t) represents the nth saw-tooth function with the starting frequency of f0,n. ku,n and
kd,n are the positive and negative slope of the saw-tooth function respectively, and Tu,n and
Td,n the increasing and decreasing time duration of the saw-tooth function respectively. Tsw,n
is the sweep time.</p>
      <p>The GPS L1 C/A signal jammed by the chirp signals from an Orolia GSG-8 constellation
simulator, shown in Figure 2, was input into the F9P receiver, and the C/N0 outputs under
diferent jamming power were logged. The efective
C/N0 of GPS SVN 05, SVN 23, and SVN
29 are drawn in Figure 3.</p>
      <p>
        A linear formula was used in [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ] to fitting the linear part below -95 dBm . In this work,
to simulate the multipath impacted jamming scenario, the whole range in Figure 3 was fitted
using Fourier series. To keep the balance between the accuracy and avoiding over-fitting, 3-4
components are recommended. It is also important to make the lower-frequency component
the main part. The fitting results are shown in Figure 4.
      </p>
      <p>The efective</p>
      <p>C/N0 model provided here is established according to Ublox F9P, to obtain
the C/N0 output of the F9P given a jamming power value from the ray-tracing introduced
previously in section 3.</p>
      <p>SVN 05
SVN 23</p>
      <p>SVN 29
0
-130 -120 -110 -100 -90 -80 -70</p>
      <p>Interference Power/dBm
-60
-50
-40
-30
5. Simulation and localization experiments
5.1. Simulation settings
In our ray-tracing simulation, an urban area about 0.5 km2 around the Sello shopping center
of Espoo, Finland was chosen. 7 monitoring nodes were placed 2 m above the building roofs,
and 60 jamming emitters were randomly generated on each street out of the 4 streets around
the block. So totally 240 jammer samples and 240× 7× 3 C/N0 measurements from 7 nodes
and 3 satellites were obtained. One of the ray-tracing examples can be seen in Figure 5. The
maximum reflections for each path were set to 5, and the reflections with a relative path loss
greater than 40 dB were discarded. The materials of the building and terrain were both set as
concrete.</p>
      <p>
        It needs to be noted that the multipath efect in a GNSS receiver is totally diferent from
the multipath efect that the jammer encounters. For the fixed GNSS monitors on building
roofs in this simulation, multipath changed slowly (for hours) and could be modeled as static.
So it was unnecessary to keep GNSS multipath environment exactly the same with the one
of jammer multipath. In a more complex scenario, multipath modelling details need to be
considered.
5.2. Localization using classification methods
By modelling the variation of C/N0 as a function of the distance between the target receiver and
jamming source, the jammer may be localized by optimizing a cost function which combines
all the C/N0s of the monitoring nodes [
        <xref ref-type="bibr" rid="ref4">4, 21</xref>
        ]. However, the NLOS and multipath signals make
the relation between C/N0 and the distance ambiguous and thereby dificult to be modeled.
A possible solution is to do the modelling using machine learning, namely as a multi-class
      </p>
      <p>C/N0 from F9P
Fourier fitting</p>
      <p>C/N0 from F9P</p>
      <p>Fourier fitting
-5130 -120 -110 -100 -90 -80 -70 -60 -50 -40 -30</p>
      <p>Interference Power/dBm
-5130 -120 -110 -100 -90 -80 -70 -60 -50 -40 -30</p>
      <p>Interference Power/dBm</p>
      <p>SVN 29
classification task.</p>
      <p>
        Support vector machines (SVMs) are supervised learning models used for classification and
regression problems. SVMs have already been used for jammer localization in [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ]. Herein,
SVMs using diferent kernel functions are tested to determine which street the jammer is on.
The models include linear, quadratic, and cubic SVMs, and fine, medium, and coarse Gaussian
SVMs. The last three methods make finely detailed, medium, and coarse distinctions between
classes with kernel scale set to sqrt(P)/4, sqrt(P), and sqrt(P)*4 respectively, where P is the
number of predictors. In the validation, a 5-fold cross-validation method is used, and the
results can be seen in Figure 6 and Table 1.
      </p>
      <p>According to our experimental results, Cubic SVM achieves the best performance with 96.2%
validation accuracy, while Quadratic SVM performs similarly with an accuracy of 95.8%. This
demonstrates the potential of using the C/N0 measurements and classification to localize
jammers in an urban area with NLOS and multipath propagation. According to the results
presented with confusion matrices, the classification mistakes mainly appear between the adjacent
streets. Except for fine Gaussian SVM, rare confusions appear between the street 1 and 3, and
the street 1 and 4, as seen in Figure 5. This can be partly attributed to the 4 monitors on the
street corners because they are usually totally blocked and have no jamming reception. This
leads to a conclusion that the placement of the monitors, to a certain extent, is important for
jammer localization.</p>
    </sec>
    <sec id="sec-4">
      <title>6. Conclusion and future work</title>
      <p>Conventional jammer localization methods are all in a way limited in urban areas where the
NLOS and multipath receptions are frequent, and the models between the measurements and
the ranges between the jammer and monitors become ambiguous. Machine learning-based
methods are powerful in solving the ambiguity problem and have not been well explored yet.
In this work, SVMs and the easily available C/N0 measurements were used for jammer
localization. A preliminary result was provided, and the potential of this method was verified.
Also, a detailed jamming multipath simulation method based on receiver characterization was
provided and will serve as basis for more realistic further research.</p>
      <p>1
2
1.7%
1 98.3%
1.7%</p>
      <p>This paper described the very first phase of our ongoing research. In our future research, we
will divide the simulated area in finer blocks to get more precise location solution. Secondly,
since the C/N0 is not reliable when the jamming is extremely strong, more measurements
should be utilized, such as AGC and AOA. Thirdly, we have previously developed an
LSTMbased anomaly detection method and based on the good results we will also use LSTM models
for jammer localization. At last, real-life data from our ARFIDAAS2 project will be used for
experiment validation.</p>
    </sec>
    <sec id="sec-5">
      <title>Acknowledgments</title>
      <p>This work was funded by the Academy of Finland project 338043 Resilience and security
of geospatial data for critical infrastructures (REASON), and the Department of Computer
Science, University of Helsinki.
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