# Innovative Radiating Systems for Train Localization in Interference Conditions

Authors: C. Vegni; M. Tosti; A. M. Vegni
Journal: International Journal of Antennas and Propagation
 (2013)

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## Abstract

The design of innovative radiating systems based on the metamaterial technology for GNSS (Global Navigation Satellite System) applications in radio frequency (RF) interference conditions is proposed. To this aim, firstly two typical adaptive array techniques (i.e.,nulling and beam-forming) are discussed and tradeed off. Secondly, FRPA (Fixed Radiation Pattern Antenna) and CRPA (Controlled Radiation Pattern Antenna) phased array configurations of miniaturized patch antennas are studied by means of electromagnetic commercial tools and phased array optimization algorithms. This process leads to the identification of a phased array design. Benefits and drawbacks for GNSS applications are highlighted. Finally, the design of the phased array is applied to a GNSS user receiver in a navigation realistic environment.
Simulation results are obtained in a realistic scenario for railway applications, comprising of a GNSS satellite constellation, a GNSS user receiver (i.e., on-board train equipment) running along a track in Western Australia, and a constellation of interfering satellites. Navigation service performances (i.e., user location accuracy and service availability) are computed taking into account the adaptive array radiation pattern in two different modes (i.e., FRPA or CRPA) and band-limited white noise interference.


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## Body

## 1. Introduction

Concern about GPS (Global Positioning System) vulnerability has received a great deal of attention recently [1, 2]. GNSS receivers are highly susceptible to interference caused by jamming and spoofing. Historically, signal jamming and the design have been primarily considered as a military problem. Now, signal interference threatens all the GNSS receivers, military and civilian.GPS signal typical level on Earth surface is around −163 dB W, that is, below the noise floor of the receiver (i.e.,N=K·TSYS·B, e.g., −228.6 + 27 + 63 dB-Hz = −138 dB for 20 MHz bandwidth L band signal).The reason why GPS signals can survive to degradation effects like interference is due to the spread-spectrum nature of the transmission, allowing receivers to correlate the satellite signal out from below the background noise [2, 3]. However, each receiver exhibits a limitation to the amount of non-GNSS interference it can cope with, whilst still acquiring or tracking the desired signals. In other words, each receiver has a maximum Jammer-to-Signal ratio (i.e., J/S) that is able to tolerate.Recent studies [1, 2] demonstrated that a 10 mW jammer at a distance less than 10 km can seriously disturb the acquisition process of a GPS receiver. Jamming is not the only form of GNSS interference; spoofing is a more recent one. Spoofing (i.e., data level interference) can be considered as a more dangerous form of interference than jamming, because it is not obvious that the GNSS receiver is being spoofed, while jamming constitutes a denial of service and it is easily detectable.In this paper a band-limited white noise interference is considered. When the interference has flat spectrum centred inf frequency and extending in the range (fi-βi/2)≤f≤(fi+βi/2), its spectrum is expressed as follows [2]:
(1)Si(f)={1βi,(fi-βi2)≤f≤(fi+βi2),0,elsewhere.
RF interference and multipath effects can be mitigated or eliminated by an appropriate GNSS antenna and receiver design [1]. In particular, we focus on antenna solutions as adaptive arrays. They are considered the single most powerful antijamming tool in the GNSS systems engineer’s toolkit. They provide jamming rejection from 15 to 90 dB depending on the specific architecture used. Their main drawback is that they require an array of antenna elements, each spaced about ten centimetres (center-to-center) in S band, and thus their physical envelope cannot meet the antenna room constraints.Therefore, the paper will be organized according to three following steps.(1)
Adaptive array typology trade-off: two typical techniques (i)nulling and (ii) beam-forming are discussed and compared in Section 2.(2)
Adaptive array antenna design: in Section3 the RF design of a phased array antenna is presented in terms of array geometric layout and single radiator element in metamaterial technology.(3)
GNSS study case: a realistic navigation case is investigated in Section4. Specifically, the train localization problem by GPS satellites is studied in conditions of RF interfering satellites.FRPA and CRPA solutions are considered, and for each one GPS service performances (i.e., train accuracy and service availability) are computed. In other words, the RF design is validated in terms of GNSS system performances in a realistic scenario. Conclusions are finally drawn.


## 2. Adaptive Array Typology Trade-Off

Two types of adaptive array antenna are used with GNSS receivers, that is, (i)single-output nulling (Figure 1) antennas, and (ii) multiple-output beam-steering (Figure 2) antennas [4].Figure 1
Single-output nulling antenna block diagram.Figure 2
Multiple-output beam-steering antenna block diagram.Most of deployed systems are single-output adaptivenulling antennas that operate as an antijamming appliqué. In this way the GNSS receiver does not need to know what type of antenna is connected to, that is, FRPA or CRPA.Some development systems [6] tend to emphasize multiple-output beam-steering antennas because of their better performance. However, in order to handle the multiple-output channels, a new receiver is required too. The trend is to integrate the array processing with the GNSS receiver in a single unit.On the other side, asingle-output nulling antenna uses a common set of weights for all GNSS signals. The objective is to minimize the output power subject to the constraint that one element is turned on. Remaining channels have their output phase and amplitude dynamically adjusted, so as to cancel out jammers in the summation process. The result consists in very sharp spatial nulls in the directions of the jammers but, because the GNSS signal direction of arrival is not taken into account, a significant possibility arises for low gain in some signal directions.However, in GNSS applications, the antenna has to receive navigation signal from as many satellites as possible.On the other side, GNSS antenna is requested to reject as many interfering satellites as possible along single or multiple directions.In principle, anN-element array can independently steer N-1 spatial nulls in the direction of jammers. Moreover, in the multiple-output beam-forming array configuration, a unique set of weights is generated and optimized for each signal. The weight information process takes into account the desired signal direction of arrival, and, in absence of jamming, it will phase the input channels so they coherently add together to create a beam in the direction of the satellite.In addition, to enable an adaptive antenna array to steer minimal antenna gain towards jammers,beam-forming simultaneously ensures that the antenna steers maximum gain towards GNSS satellites.In other words, instead of minimizing the interference-to-noise ratio (INR), the aim is to maximize the signal-to-interference-plus-noise ratio (SINR).Like thenuller, the beam-former can independently steer N-1 spatial nulls.Both thenuller and the beam-former perform much better (i.e., >20 dB) against narrow-band jammers.The advantages ofnulling and beam-forming antennas can be reported as follows.(i)
Nulling solution appears less complex than beam-former one.(ii)
Nullers synthetize sympathetic nulls in directions other than those of jammers. Sometimes, this happens in the direction of a desired signal and the signal is lost. It corresponds to a decrease of the number of visible satellites and consequently to a degradation of GNSS performance parameters (e.g., accuracy, continuity).(iii)
Beam-formers provide a broad-beam in the direction of the desired signal and lower gain in other directions. Multipath arriving from low gain directions is more strongly attenuated and has less ability to corrupt code and carrier phase observables.(iv)
Nullers do not provide this performance gain as they do not seek to generate directional beam.In general, adaptive arrays improve signal-to-noise ratio in presence of jamming and thus permit signal tracking in environments that otherwise would lack code and carrier phase observables (lack of pseudorange measurement). However, this benefit is not without cost: adaptive arrays can bias code and carrier phase observables. The array antenna is a spatial filter, and its distortion effects are also direction dependent. The distortion is unique for each desired signal and does not necessarilycommon-mode out in subsequent processing.In absence of jamming, the biases are fairly benign, while in jamming conditions the biases can become large and sustained.Beam-formers can show 100-degree carrier phase biases and upwards of 1-meter code phase biases.Nullers do even worse. For high precision systems, these errors can be a significant component of the overall error budget. Table 1 summarizes the previous considerations.Table 1
Adaptive antennanulling versus beam-forming techniques.
N-elements antenna feature
Nulling
Beam-forming
Robustness to interference
Low (low gain along not IF directions)
Medium (adequate gain roll-off shown)
Maximum number of spatial nulls
N
-
1
N
-
1
Null depth
<−20 dB
<−20 dB
Directional beam capability
No
Yes
Impact on accuracy measurement
Not compatible with high precision applications
More than 100° on carrier phase meas.;1 meter on code phase meas.In this paper, the synthesis algorithm MVDR (Minimum Variance Distortionless Response) is applied [4, 6]. It falls into the category of beam-forming adaptive array. This algorithm allows the synthesis of up to N-1 nulls and the pointing of the main beam along one single direction. The considered direction is the broad-side one (θ=90° with respect to horizon).In case interfering direction is close to or coincides with the broad-side one, the algorithm shall show convergence problems.However, this satellite geometric configuration is highly unlikely. In that case the antenna beam shall point to a direction computed as the mean value among all the interfering directions.


## 3. Adaptive Array Antenna Design

In this section, firstly, we show the basic concepts to be followed to design a GNSS antenna. Secondly, the phased array element innovative design is illustrated by VSWR, axial ratio (AR), and radiation pattern curves. Finally, the adaptivebeam-forming phased array design is shown, in terms of array layout and radiation patterns.


### 3.1. GNSS Antenna Guidelines

The guidelines consider four typical specific antenna parameters, that is, (i) pattern, (ii) roll-off, (iii) polarization purity, and (iv) phase centre.(i)
Antenna pattern: the GNSS antenna has to receive all the navigation signals transmitted by the GNSS satellites in visibility. Ideally, it should show an omnidirectional radiation pattern. The GPS receiver operates best with only a small difference in power among the signals from the various satellites, and, ideally, the antenna covers the entire hemisphere with no variation in gain. This has to do with potential cross-correlation problems in the receiver and the fact that excessive gain roll-off may cause signals from satellites at low elevations to drop well below the noise floor of the receiver. On the other hand, optimization for multipath rejection and antenna noise temperature require some gain roll-off.
(ii)
Antenna roll-off: antenna should show perfect hemispherical radiation pattern. However, such an antenna cannot be practically built, and real-world GNSS antennas experience a gain roll-off of 10 to 20 dB from broad-side to the horizon.
(iii)
Antenna polarization purity: a right hand circular polarization (RHCP) antenna will pick up some left hand circular polarization (LHCP) energy. For high-end (geodetic/choke ring) GNSS antennas, the typical AR in broad-side should be around 1 dB. AR increases toward the lower elevations (less than 3 to 6 dB at 10° elevation for a high-performance antenna). Maintaining a good AR (i.e., 1-2 dB) over the entire hemisphere and at all the frequencies is a challenge for the antenna RF designer. Good polarization purity represents a valid rejection to multipath/interference effect. In fact, reflected signals are LHCP (single reflection). Consequently, multipath signals from reflections against vertical objects such as buildings can be deeply attenuated or even suppressed.
(iv)
Antenna phase centre: in GNSS applications, the user position is relative to the phase centre of the GNSS receiving antenna. The phase centre is the point in space from which all the rays appear to emanate (or converge on) the antenna. Put in another way, it is the point where the fields from all the incident rays appear to add up in phase. Determining the phase centre is important in GNSS systems, particularly when millimetre positioning resolution is desired. Ideally, the phase centre is a single point in space for all directions at all frequencies. A real-world antenna often will possess multiple phase centre points or a phase centre that appears “smeared out” as frequency and viewing angle vary. For well-designed high-end (geodetic/choke ring) GNSS antennas, phase centre variations in azimuth are small and in the order of a couple of millimetres. The vertical phase offsets are typically 10 mm or less.The above-discussed guidelines can be summarized in Table2.Table 2
GNSS antenna design guidelines.
Antenna parameter
Guidelines for GNSS applications
Radiation pattern
Hemispherical
Roll-off
11–13 dB (from broad-side to 10° elevation direction)
Polarization purity
(i) 1 dB at broad-side(ii) <6 dB at 10° elevation
Phase centre
(i) Stable versus frequency(ii) Stable versus Az, El angles


### 3.2. Element Design

The single radiator configuration is shown in the top view (Figure3), in the cross-view (Figure 4), and in 3D view (Figure 5). This is a dual probe miniaturized monolayer patch in L1 band, at 1.55 GHz central frequency. The circular polarization is obtained by two inputs (probes). Each probe is electromagnetically coupled to the radiating patch by a parasitic disk. Moreover, four mushrooms (depicted in yellow in Figure 3) are introduced to reduce the envelope of the squared ring. In particular, mushrooms are folded (dotted lines) in order to improve capacitive effects.Figure 3
Single element—top view.Figure 4
Single element—cross view (V-port not shown).Figure 5
Single element 3D view.Balanced feeds tend to have superior scanning performance as the higher order modes are naturally suppressed by the symmetrical feeding arrangement. Moreover, polarization purity is improved using two inputs instead of a single port. A dual-probe interconnect is chosen as a result of these performance advantages.The miniaturized monolayer patch can be easily obtained by using the metamaterial technology. It is well known that this technology allows several advantages in the realization of antennas, namely, the printed ones. One of these advantages (miniaturization) is obtained by using “metamaterial-based” antennas or “metamaterial-inspired” ones.The difference among “metamaterial-based” antennas and “metamaterial-inspired” ones stands either using unconventional dielectric slabs (for “metamaterial-based” antennas) or parasitic elements/cuts nearby/inside the radiating patch (for “metamaterial-inspired” antennas) [7–12].This means that major dimension of metamaterial antenna elements used in array configuration is smaller than usual ones (fromλg/2 to λg/20 or more, corresponding to an area reduction of 90% or more). Consequently, the dimensions of the whole antenna (e.g., the array) can be drastically reduced [13, 14].The patch ground-plane separation is about 5 mm, and the underlying substrate permittivity is 2.2. The envelope area is 3.38 cm2 (i.e., 1.84 × 1.84 cm ≈ 3.38). It is noted that, at the same working frequency (1.55 GHz) in case of standard monolayer (i.e., εr=2.2) patch (typical λg/2), the single element envelope would be 6.41×6.41=41.08 cm2. Metamaterial radiator technology area is the 3.38/41.08 = 8.22% of a standard monolayer patch.A Cartesian reference system adopted to define the field quantities is introduced in Figure3. Its origin is coincident to the left-side angle of the squared ring as shown in the figure.Table3 reports the single element physical parameters (distances expressed in mm).Table 3
Single element physical parameters.
Parameter
Value
Note
ε
r
2.2
Dielectric constant
t
4
Substrate thickness
a
2.8
Patch arm width
b
2.8
Patch arm length
M
x
6.1
Mushroom width
M
y
6.1
Mushroom length
mt
0.1
Mushroom thickness
dp
1.8
Probe plate diameter
s
0.15
Gap probe-patch
Vd
0.7
Via diameter
Ph
2
Parallel plates capacitors height
dh
3.85
Parasitic element height (t-s)
g
0.2
Gap between metals
o
1.9
Feed offset
L
x
18.4
Square ringx-size
L
y
18.4
Square ringy-size
H-portx
1.9
Feed offset
H-porty
9.2
L
y/2
V-portx
9.2
L
x/2
V-port y
1.9
Feed offsetFinally, the −15 dB return loss (Figure6) bandwidth is 25.2 MHz (1.6%).Figure 6
Single element return loss versus frequency.On the other side, the reduction of the antenna aperture generally corresponds to a decrease of the single element antenna gain. This effect has been taken into account in the design of the phased array antenna. The radiation pattern is shown in Figure7, where it can be noted the peak gain around 5.7 dBi.Figure 7
Single element gain versus elevation angle.The axial ratio value is about 2 dB and shows a flat trend (Figure8). It is in line with the guidelines described in the previous paragraph which are low AR values for low elevation angles.Figure 8
Single element axial ratio versus elevation angle.


### 3.3. Array Layout Optimization

The antenna aperture is a design driver. The layout definition process is addressed considering the following aspects.(i)
The envelope diameter shall be compatible to train roof accommodation, that is, 80 cm (goal) and 30 cm (nice-to-have).(ii)
The guidelines are those described in Section3.1.Two layouts have been identified, that is, (i) the 13 elements, and (ii) the 7 elements configuration, as depicted in Figures9 and 10, respectively. The first configuration is compliant to the 80 cm envelope constraint, while the second one to the nice-to-have constraint (i.e., 30 cm). The geometry proposed in the 7 elements configuration has been already studied in the frame of GNSS studies [15]. Both layouts show physical symmetry along three symmetry axes, as depicted in Figures 9 and 10. As a consequence, a symmetrical pattern shall derive. It will optimize the GNSS satellites visibility.Figure 9
13 elements array configuration—3D view.Figure 10
7 elements array configuration—3D view.In both layouts the radiating elements are 0.73λg spaced. This value derives from a trade-off between accommodation issues (d/λg>0.5) and grating lobes effect (d/λg<1).Assuming 0.73λg, for the 7 elements configuration and radiator in metamaterial technology, the antenna diameter is 20.57 cm. The total envelope is obtained by adding the 25% of antenna diameter value. The value is compliant to the accommodation constraint (<30 cm).It is noted that considering standard antenna technology the overall envelope of the antenna would have exceeded the above-mentioned constraint.The excitation coefficients for elements of the configurations at 13 and at 7 elements have been optimized by MVDR algorithm in order to synthesize nulls (up to 6) keeping the main lobe pointingθ=0° (zenith direction).Figure11 shows an example of synthesis of two nulls for 7 elements antenna, along θ1=60°, Φ1=60° and θ2=70°, Φ2=180° directions. They are marked in white. On the other side, main beam-steering direction is set to θ0=0° (zenith direction, Φ0=0°). (Note that θ angle defined in antenna reference system (par. 3) and θ elevation angle defined in GNSS user reference system (par. 4) are 90° offsets: zenith direction is θ=0° at par. 3, it is θ=90° at par. 4.) It is noted that antenna diagram shows nulls also in noninterfering directions (e.g., at θ1=70°, Φ1=300°, marked in red). This can limit the visibility of GNSS (useful) satellites. The decrease of the number of tracked satellites can lead to a reduction of the service accuracy/time availability. This impact shall be evaluated in the next paragraph in the frame of the study of the navigation realistic scenario.Figure 11
7 elements array adaptive beam-forming antenna pattern—two nulls synthesis.The 13 elements configuration design does not meet the 30 cm constraint. It is considered as a back-up design. However, as a title of example, Figure12 shows a radiation pattern for a 13 elements array configuration in case of two nulls synthesis.Figure 12
13 elements array adaptive beam-forming antenna pattern—two nulls synthesis.Phased array electromagnetic analysis has been addressed by electromagnetic commercial tool (i.e., CST Studio Suite) in order to take into account RF mutual coupling effects: in Figure13, another example of radiation pattern optimization is provided. It represents a null synthesis along broad-side (zenith) direction. The diagram appears balanced, symmetrical with respect to zenith direction. The antenna RF design allows the rejection to the interference signal (supposed along zenith direction in this case) and, on the other side, the maximization of the gain in order to receive the maximum number of GNSS useful signals with a signal-to-noise ratio adequate to ensure the tracking of the GNSS receiver [16].Figure 13
7 elements array: adaptive beam-forming antenna pattern—single null synthesis.It is important to note that the symmetry of the radiation pattern and the depth of the null (about −30 dB in Figures11 and 13) demonstrate that degradation effects like RF coupling among elements and beam-forming network effects (i.e., excitation coefficients truncation) are well taken into account in the antenna RF design.In the current paper, focus is given to the innovative radiating part of the antenna. Contribution of the antenna feeding network (i.e., typical values of excitation coefficients stability over frequency/temperature, truncation of excitation coefficients) is taken into account in the design.The excitation synthesized coefficients are shown in the following Table4 (see also Figure 10).Table 4
Excitation synthesized coefficients of pattern shown in Figure13.
Element Id.
Amplitude [dB]
Phase [deg]
1
0
0
2
0
+60
3
0
+120
4
0
+180
5
0
+240
6
0
+300
7
−30
0Finally, it is worth to note that antenna centre of phase has not been considered due to negligible contribution to accuracy error (order of millimetres).


## 3.1. GNSS Antenna Guidelines

The guidelines consider four typical specific antenna parameters, that is, (i) pattern, (ii) roll-off, (iii) polarization purity, and (iv) phase centre.(i)
Antenna pattern: the GNSS antenna has to receive all the navigation signals transmitted by the GNSS satellites in visibility. Ideally, it should show an omnidirectional radiation pattern. The GPS receiver operates best with only a small difference in power among the signals from the various satellites, and, ideally, the antenna covers the entire hemisphere with no variation in gain. This has to do with potential cross-correlation problems in the receiver and the fact that excessive gain roll-off may cause signals from satellites at low elevations to drop well below the noise floor of the receiver. On the other hand, optimization for multipath rejection and antenna noise temperature require some gain roll-off.
(ii)
Antenna roll-off: antenna should show perfect hemispherical radiation pattern. However, such an antenna cannot be practically built, and real-world GNSS antennas experience a gain roll-off of 10 to 20 dB from broad-side to the horizon.
(iii)
Antenna polarization purity: a right hand circular polarization (RHCP) antenna will pick up some left hand circular polarization (LHCP) energy. For high-end (geodetic/choke ring) GNSS antennas, the typical AR in broad-side should be around 1 dB. AR increases toward the lower elevations (less than 3 to 6 dB at 10° elevation for a high-performance antenna). Maintaining a good AR (i.e., 1-2 dB) over the entire hemisphere and at all the frequencies is a challenge for the antenna RF designer. Good polarization purity represents a valid rejection to multipath/interference effect. In fact, reflected signals are LHCP (single reflection). Consequently, multipath signals from reflections against vertical objects such as buildings can be deeply attenuated or even suppressed.
(iv)
Antenna phase centre: in GNSS applications, the user position is relative to the phase centre of the GNSS receiving antenna. The phase centre is the point in space from which all the rays appear to emanate (or converge on) the antenna. Put in another way, it is the point where the fields from all the incident rays appear to add up in phase. Determining the phase centre is important in GNSS systems, particularly when millimetre positioning resolution is desired. Ideally, the phase centre is a single point in space for all directions at all frequencies. A real-world antenna often will possess multiple phase centre points or a phase centre that appears “smeared out” as frequency and viewing angle vary. For well-designed high-end (geodetic/choke ring) GNSS antennas, phase centre variations in azimuth are small and in the order of a couple of millimetres. The vertical phase offsets are typically 10 mm or less.The above-discussed guidelines can be summarized in Table2.Table 2
GNSS antenna design guidelines.
Antenna parameter
Guidelines for GNSS applications
Radiation pattern
Hemispherical
Roll-off
11–13 dB (from broad-side to 10° elevation direction)
Polarization purity
(i) 1 dB at broad-side(ii) <6 dB at 10° elevation
Phase centre
(i) Stable versus frequency(ii) Stable versus Az, El angles


## 3.2. Element Design

The single radiator configuration is shown in the top view (Figure3), in the cross-view (Figure 4), and in 3D view (Figure 5). This is a dual probe miniaturized monolayer patch in L1 band, at 1.55 GHz central frequency. The circular polarization is obtained by two inputs (probes). Each probe is electromagnetically coupled to the radiating patch by a parasitic disk. Moreover, four mushrooms (depicted in yellow in Figure 3) are introduced to reduce the envelope of the squared ring. In particular, mushrooms are folded (dotted lines) in order to improve capacitive effects.Figure 3
Single element—top view.Figure 4
Single element—cross view (V-port not shown).Figure 5
Single element 3D view.Balanced feeds tend to have superior scanning performance as the higher order modes are naturally suppressed by the symmetrical feeding arrangement. Moreover, polarization purity is improved using two inputs instead of a single port. A dual-probe interconnect is chosen as a result of these performance advantages.The miniaturized monolayer patch can be easily obtained by using the metamaterial technology. It is well known that this technology allows several advantages in the realization of antennas, namely, the printed ones. One of these advantages (miniaturization) is obtained by using “metamaterial-based” antennas or “metamaterial-inspired” ones.The difference among “metamaterial-based” antennas and “metamaterial-inspired” ones stands either using unconventional dielectric slabs (for “metamaterial-based” antennas) or parasitic elements/cuts nearby/inside the radiating patch (for “metamaterial-inspired” antennas) [7–12].This means that major dimension of metamaterial antenna elements used in array configuration is smaller than usual ones (fromλg/2 to λg/20 or more, corresponding to an area reduction of 90% or more). Consequently, the dimensions of the whole antenna (e.g., the array) can be drastically reduced [13, 14].The patch ground-plane separation is about 5 mm, and the underlying substrate permittivity is 2.2. The envelope area is 3.38 cm2 (i.e., 1.84 × 1.84 cm ≈ 3.38). It is noted that, at the same working frequency (1.55 GHz) in case of standard monolayer (i.e., εr=2.2) patch (typical λg/2), the single element envelope would be 6.41×6.41=41.08 cm2. Metamaterial radiator technology area is the 3.38/41.08 = 8.22% of a standard monolayer patch.A Cartesian reference system adopted to define the field quantities is introduced in Figure3. Its origin is coincident to the left-side angle of the squared ring as shown in the figure.Table3 reports the single element physical parameters (distances expressed in mm).Table 3
Single element physical parameters.
Parameter
Value
Note
ε
r
2.2
Dielectric constant
t
4
Substrate thickness
a
2.8
Patch arm width
b
2.8
Patch arm length
M
x
6.1
Mushroom width
M
y
6.1
Mushroom length
mt
0.1
Mushroom thickness
dp
1.8
Probe plate diameter
s
0.15
Gap probe-patch
Vd
0.7
Via diameter
Ph
2
Parallel plates capacitors height
dh
3.85
Parasitic element height (t-s)
g
0.2
Gap between metals
o
1.9
Feed offset
L
x
18.4
Square ringx-size
L
y
18.4
Square ringy-size
H-portx
1.9
Feed offset
H-porty
9.2
L
y/2
V-portx
9.2
L
x/2
V-port y
1.9
Feed offsetFinally, the −15 dB return loss (Figure6) bandwidth is 25.2 MHz (1.6%).Figure 6
Single element return loss versus frequency.On the other side, the reduction of the antenna aperture generally corresponds to a decrease of the single element antenna gain. This effect has been taken into account in the design of the phased array antenna. The radiation pattern is shown in Figure7, where it can be noted the peak gain around 5.7 dBi.Figure 7
Single element gain versus elevation angle.The axial ratio value is about 2 dB and shows a flat trend (Figure8). It is in line with the guidelines described in the previous paragraph which are low AR values for low elevation angles.Figure 8
Single element axial ratio versus elevation angle.


## 3.3. Array Layout Optimization

The antenna aperture is a design driver. The layout definition process is addressed considering the following aspects.(i)
The envelope diameter shall be compatible to train roof accommodation, that is, 80 cm (goal) and 30 cm (nice-to-have).(ii)
The guidelines are those described in Section3.1.Two layouts have been identified, that is, (i) the 13 elements, and (ii) the 7 elements configuration, as depicted in Figures9 and 10, respectively. The first configuration is compliant to the 80 cm envelope constraint, while the second one to the nice-to-have constraint (i.e., 30 cm). The geometry proposed in the 7 elements configuration has been already studied in the frame of GNSS studies [15]. Both layouts show physical symmetry along three symmetry axes, as depicted in Figures 9 and 10. As a consequence, a symmetrical pattern shall derive. It will optimize the GNSS satellites visibility.Figure 9
13 elements array configuration—3D view.Figure 10
7 elements array configuration—3D view.In both layouts the radiating elements are 0.73λg spaced. This value derives from a trade-off between accommodation issues (d/λg>0.5) and grating lobes effect (d/λg<1).Assuming 0.73λg, for the 7 elements configuration and radiator in metamaterial technology, the antenna diameter is 20.57 cm. The total envelope is obtained by adding the 25% of antenna diameter value. The value is compliant to the accommodation constraint (<30 cm).It is noted that considering standard antenna technology the overall envelope of the antenna would have exceeded the above-mentioned constraint.The excitation coefficients for elements of the configurations at 13 and at 7 elements have been optimized by MVDR algorithm in order to synthesize nulls (up to 6) keeping the main lobe pointingθ=0° (zenith direction).Figure11 shows an example of synthesis of two nulls for 7 elements antenna, along θ1=60°, Φ1=60° and θ2=70°, Φ2=180° directions. They are marked in white. On the other side, main beam-steering direction is set to θ0=0° (zenith direction, Φ0=0°). (Note that θ angle defined in antenna reference system (par. 3) and θ elevation angle defined in GNSS user reference system (par. 4) are 90° offsets: zenith direction is θ=0° at par. 3, it is θ=90° at par. 4.) It is noted that antenna diagram shows nulls also in noninterfering directions (e.g., at θ1=70°, Φ1=300°, marked in red). This can limit the visibility of GNSS (useful) satellites. The decrease of the number of tracked satellites can lead to a reduction of the service accuracy/time availability. This impact shall be evaluated in the next paragraph in the frame of the study of the navigation realistic scenario.Figure 11
7 elements array adaptive beam-forming antenna pattern—two nulls synthesis.The 13 elements configuration design does not meet the 30 cm constraint. It is considered as a back-up design. However, as a title of example, Figure12 shows a radiation pattern for a 13 elements array configuration in case of two nulls synthesis.Figure 12
13 elements array adaptive beam-forming antenna pattern—two nulls synthesis.Phased array electromagnetic analysis has been addressed by electromagnetic commercial tool (i.e., CST Studio Suite) in order to take into account RF mutual coupling effects: in Figure13, another example of radiation pattern optimization is provided. It represents a null synthesis along broad-side (zenith) direction. The diagram appears balanced, symmetrical with respect to zenith direction. The antenna RF design allows the rejection to the interference signal (supposed along zenith direction in this case) and, on the other side, the maximization of the gain in order to receive the maximum number of GNSS useful signals with a signal-to-noise ratio adequate to ensure the tracking of the GNSS receiver [16].Figure 13
7 elements array: adaptive beam-forming antenna pattern—single null synthesis.It is important to note that the symmetry of the radiation pattern and the depth of the null (about −30 dB in Figures11 and 13) demonstrate that degradation effects like RF coupling among elements and beam-forming network effects (i.e., excitation coefficients truncation) are well taken into account in the antenna RF design.In the current paper, focus is given to the innovative radiating part of the antenna. Contribution of the antenna feeding network (i.e., typical values of excitation coefficients stability over frequency/temperature, truncation of excitation coefficients) is taken into account in the design.The excitation synthesized coefficients are shown in the following Table4 (see also Figure 10).Table 4
Excitation synthesized coefficients of pattern shown in Figure13.
Element Id.
Amplitude [dB]
Phase [deg]
1
0
0
2
0
+60
3
0
+120
4
0
+180
5
0
+240
6
0
+300
7
−30
0Finally, it is worth to note that antenna centre of phase has not been considered due to negligible contribution to accuracy error (order of millimetres).


## 4. GNSS Study Case

In the current paragraph, the design of the phased array shown in the previous part is applied to a GNSS user receiver antenna in a navigation realistic environment consisting of(i)
GNSS satellite constellation (e.g., GPS, Galileo, GLONASS, and Compass);(ii)
SBAS satellite constellation (e.g., QZSS for Japan and Australia, EGNOS for Europe, and WAAS for U.S.);(iii)
GNSS user receiver antenna accommodated on the train roof. The train is travelling along a more than 200 km long route from a mines area to “Port Headland” (and back) in Western Australia region, rural rail environment at an average speed of 80 km/h (Figure14);(iv)
Satellite constellation of interfering satellites (from 1 to 6, randomly selected) transmitting 20 dBW over the GPS EIRP nominal value on L1 bandwidth;(v)
Train running in adverse conditions (totally disconnected scenario, no ground infrastructures).Figure 14
GNSS scenario under study—train path trajectory.In particular, the GNSS antenna (7 elements array discussed at par. 3.1, 3.2) is supposed to work in FRPA or CRPA modes. Consequently, five cases are taken into account (Table5).Table 5
7 elements array: cases considered in the navigation realistic scenario.
Case
Meaning
FRPA cosine-like
The radiation pattern of the user antenna is a fixed beam approximated by acosinep function (p: integer). No interfering satellite is considered in the analysis.
FRPA simulated
The radiation pattern of the user antenna is a fixed beam (Figure15) designed and simulated by electromagnetic commercial tool (i.e., “CST studio suite”). No interfering satellite is considered in the analysis.
FRPA cosine-like with IF
The radiation pattern of the user antenna is a fixed beam approximated by acosinep function (p: integer). Interfering satellite is considered in the analysis.
FRPA simulated with IF
The radiation pattern of the user antenna is a fixed beam (Figure15) designed and simulated by electromagnetic commercial tool. Interfering satellite is considered in the analysis.
CRPA
The radiation pattern of the user antenna is synthesised by MVDR algorithm (beam-forming) implemented by “MatLab” software tool. In other words, the antenna dynamically synthesizes null/s along direction of interferer/s. Interfering satellite is considered in the analysis.Figure15 shows the FRPA simulated pattern (three Φ cuts) and the FRPA “cosine-like” pattern (pink dotted line).Figure 15
Ground planar array antenna. FRPA simulated and “cosine-like” pattern.The assumptions followed in the realistic scenario simulation are the following.(i)
The observation period is 10 days, 5 minutes sampling: the train is running from mines area point to “Port Headland” and back; the total number of points described by the trajectory is 2881;(ii)
the accuracy value is computed with 95% confidence level;(iii)
GPS signal on-ground power level as defined in [16];(iv)
the attenuation by atmospheric gases is computed byITU-R P.676-2 model [17];(v)
the rainfall attenuation is modelled as described in [17];(vi)
masked areas as those pertaining to a tunnel and bridges are neglected;(vii)
no GNSS satellite failure (i.e., on-board clocks) is assumed;(viii)
GNSS receiver mask angle >10° with respect to horizon (as shown in Figure15);(ix)
GPS receiver acquisition threshold: 30 dB-Hz (typical value);(x)
GNSS user receiver antenna given by a 7 elements phased array working in FRPA mode (cosine-like pattern or simulated in Figure15) or CRPA mode;(xi)
user equivalent ranging error (UERE) figure is considered common to each GPS satellite. The value is equal to 4.87 meters (at1σ) computed at θ=15° (conservative approach). Source error typical standard deviations in L1 band only are reported in  Table 6.Table 6
UERE figure for GPS L1 receiver.
It.
Error source
Value (rms-m)
1
Satellite clock synchronization
01
2
Satellite perturbations
02
3
Ephemeris prediction error
01
4
Ionosphere delay
4.873
5
Troposphere delay
0.14
6
Multipath
0.25
7
Receiver noise and resolution thermal noise
0.206
8
UERE
4.87

1GNSS receiver augmented by SBAS satellites (e.g., QZSS for Australia) from direct signal in space (SIS).
2GNSS receiver augmented by SBAS satellites.
3Single frequency GNSS receiver, no corrections applied.
4Value obtained by “Ifadis” model [5].
5Assuming signal-to-multipath ratio: 27.5 dB, path delay: 26 m, E-L narrow spacing: 0.1 chip, signal bandwidth = 24 MHz.
6Assuming noncoherent discriminator DLL with early-late spacing: 0.1; C/No: 40 dB-Hz; code loop noise bandwidth: 0.1 Hz integration time: 20 msec; chip length of code: 293.2551 m.The UERE budget driver is the ionosphere residual error.For each case of the described navigation scenario, user location 2D accuracy versus time and service availability figures are computed, and the results are compared in order to have evidence of the impact of user antenna pattern on the GNSS service performance.In particular, a constellation of 24/24 GPS satellites disposed over 6 orbital planes (4 satellites per plane) is studied. RF interferers are gradually introduced (from 1 to 6) in the scenario. Figures16–24 show the horizontal accuracy cumulative distribution function (CDF) for the cases described in Table 5.Figure 16
Horizontal accuracy CDF curve −24/24 GPS constellation and 1 RF interfering satellite.Number of visible satellites −24/24 GPS constellation and 1 RF interfering satellite.
(a)
(b)Figure 18
Horizontal accuracy CDF curve −24/24 GPS constellation and 2 RF interfering satellites.Figure 19
Horizontal accuracy CDF curve −24/24 GPS constellation and 3 RF interfering satellites.Figure 20
Horizontal accuracy CDF curve −24/24 GPS constellation and 4 RF interfering satellites.Figure 21
Horizontal accuracy mapping −24/24 GPS constellation and 4 RF interfering satellites.Figure 22
Horizontal accuracy CDF curve −24/24 GPS constellation and 5 RF interfering satellites.Figure 23
Horizontal accuracy CDF curve −24/24 GPS constellation and 6 RF interfering satellites.Figure 24
Horizontal accuracy mapping (“zoomed” view) −24/24 GPS constellation and 6 RF interfering satellites.In Figure16, in absence of interference, the horizontal accuracy at a time availability of 95% is about 12 meters both for FRPA cosine and simulated pattern antenna. In interference conditions, the GPS receiver ‘‘sees’’ a useful link with the GPS satellite, whose C/N0 is between 35 and 50 dB-Hz (according to user elevation angle) and noise contribution I0 due to RF interference.Consequently, total GPS satelliteC/(N0+I0) figure is degraded; the signal-to-noise ratio starts to decrease as soon as the interfering satellite is in visibility of the GPS user receiver. If the GPS satellite signal-to-noise ratio is less than the receiver acquisition threshold, satellite signal cannot be acquired and satellite cannot be tracked by the receiver, so the number of useful (necessary to compute user position) satellites starts to decrease.This concept is illustrated in Figure17. It represents the number of GNSS satellites geometrically visible (in light blue), electrically visible (in red) to the train along its route (versus observation time). In absence of interference, satellites that are visible geometrically are also electrically (even with a 0 dBi gain antenna) visible. In case of interference, as mentioned before, the useful signal power shall be below the noise (thermal and interference nature) more than 30 dB-Hz leading to the loss of satellite track. In addition, the DOC4 figure (Depth of Coverage 4: time percentage to have at least four satellites in visibility to the GPS receiver) shall pass from 100% to 70.53% as shown in Figure 16. (Note that 4 is the minimum number of GNSS satellite to compute the user 3D location.) The threshold of 4 satellites (minimum number to compute GNSS user position) is highlighted in Figure 17 by dotted green line.Consequently, the user accuracy is computed by a reduced number of satellites. It is degraded (about 18 meters) with a reduced availability (about 70%) both for cosine and simulated FRPA antennas. Adopting the CRPA solution, a null is synthesized along interfering direction and the antenna main beam points the broad-side direction. It mitigates the effects of the interference; however, the synthesized radiation pattern can show undesired nulls that can limit the GPS satellite visibility (Figure11). Consequently, the service can be provided with a maximum 2D accuracy of 30 meters with a time availability of about 75%.In Figure18 two interfering satellites are considered. The 2D accuracy figure is reduced to 18 m with 52% time availability both for FRPA cosine and FRPA simulated. CRPA antenna solution mitigates the interference effect (30 meters accuracy with about 74% time availability). This value is very similar to the one obtained for one single interfering satellite case. It is noted that CRPA provides robustness to interference without affecting the GPS satellite visibility.For the 3 interfering satellites option (Figure19), the horizontal accuracy of the train is degraded to 18 meters at 52% of the time for FRPA patterns. Adopting CRPA solution it is 30 meters at 68% of the time (10 days).On each curve, a reference value of 5 meters has been considered (green dotted line). An horizontal accuracy of 5 meters represents a typical value for train applications (this is why user antenna phase centre error contribution is not taken into account). This value can be even lower when additional capabilities, like parallel track discrimination is required [18].The multiconstellation capabilities relying on GPS, GLONASS, and in perspective Galileo and Compass offer a higher degree of flexibility to reach better performance.For the 4 interfering satellites option (Figures20 and 21), the horizontal accuracy is degraded to 18 meters at about 15% of the observation time for FRPA patterns. Adopting CRPA solution it is 30 meters at 55% of the time.More specifically, it means that, in conditions of interference, the train position can be computed by the GPS receiver in 15% of the total time (in other words, for the 15% of the points of the train route shown at Figure14) with a minimum 2D accuracy of 8.63 m and a maximum 2D accuracy of 18.38 m (Figure 21).For the 5 interfering satellites option (Figure22), the horizontal accuracy is degraded to 18 meters at 5% of the time for FRPA patterns. Adopting CRPA solution it is 30 meters at 68% of the time (10 days).For the 6 interfering satellites option (Figures23 and 24), the horizontal accuracy is degraded to 18 meters at 5% of the time for FRPA patterns. It is noted that CRPA antenna solution strongly mitigates the interference effects. In other words, the train position can be located along the route with a 2D maximum accuracy of 30 meters at 60% of the time (10 days).By adopting an FRPA antenna, the 2D position of the train is known with an accuracy of 18.3 meters (Figure23) at about the 5% of the train route (Figure 14). Comparing Figures 24 and 13, it is noted that the points (user positions computed by the receiver—128) do not encompass the whole rail path (2881 points). It is due to the lack of GPS visible satellites (caused by RF interference) to the receiver. If the number of GPS satellites visible is less than 4, the receiver cannot compute the user position; consequently, the marker is, respectively, blank in Figures 21 and 24.


## 5. Conclusions

In this paper an innovative radiating system for train localization in interference conditions is presented. This system consists of abeam-forming adaptive antenna, a phased array of miniaturized (metamaterial technology) patch radiators. The design of the beam-forming antenna is presented (working in FRPA or CRPA mode).Phased array antenna is embedded into a navigation realistic scenario in interference conditions, and the problem of localization-by-GNSS-satellite of a train travelling along a route in Australia is approached.Service performance figures (i.e., accuracy, time availability) are evaluated, and emphasis is given to the capability of the GNSS-designed array to mitigate RF interference effects (reduction of service availability, increase of location accuracy).



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*Source: 623950-2013-07-30.xml*