23.11.11

Paper-Direction Dependent Modulation of an RFID Tag




Abstract— In this contribution we introduce a simple radio frequency (RF) tag that can be configured to exhibit direction dependent modulation properties. The tag consists of a two-by-two array of pin diode loaded dipole elements that can be controlled by an external signal to modulate the RF scattering characteristics of the tag. The design of the tag allows for multilevel in-phase and quadrature modulation schemes to be implemented. It will also be shown that the form of the modulation generated by the tag is direction dependent and that this property can be exploited to provide an additional degree of system security.

Keywords-PSS; Secure Communication; Directional Phase Modulation; RFID; Antennas

The concept of directional modulation was recently proposed as a means for enhancing the security of wireless data transmission [1]. The idea was originally applied to a transmitting array antenna and involves imparting baseband data on to the transmitted signal by directly modulating the elements of the array.  If this process is performed correctly, the form of the modulated signal transmitted by the antenna changes with observation angle. So, for example, the antenna may configured to radiated a 16 level QAM signal on boresight, but at angles away from boresight the modulation scheme will be corrupted. This property has been proposed as means of enhancing the security of data transmission as it makes interception and decoding by an eavesdropper a difficult task.  Recently we have investigated applying directional modulation to the scattering properties of an RFID tag. The general concept of directional modulation may be explained by referring to Figure 1 which shows an RF tag which is illuminated at boresight by a cw RF signal. The tag is assumed to be configured to impart symmetrical QPSK modulation on to directly reflected signals (boresight direction). At angles away from boresight however, the form of the constellation diagram changes and it no longer exhibits the original symmetrical form of QPSK. Indeed in can be shown that in certain situations the distortion of the original constellation diagram with angle can result in the complete elimination of certain constellation points making successful detection and demodulation an almost impossible task [2]. 


The RF tag we are investigating is based on the concept of an active phase modulating surface or phase-switched screen (PSS) and consists of a two-by-two array of pin diode loaded dipole elements placed above a conducting ground plane. By applying a bias voltage to the pin diodes, the dipoles can be switched between resonant and non-resonant impedances. Hence, to a first order approximation, the diodes may be considered opaque (when resonant) or transparent (when non-resonant) in which case the primary scattering will occur from either the dipole surface or the conducting back-plane. To model the basic scattering behaviour of the tag we introduce a very simplified analytic model in which the tag is represented by two four element arrays of isotropic scattering sources as show in Figure 2. The elements of the upper array represent scattering from the resonant dipoles and those of the lower array represent scattering from the ground plane when the dipoles are non-resonant.  For the results presented here, both arrays are assumed to have x-y element separation distances of a quarter of a wavelength at the illumination frequency. In addition, the vertical (z) spacing between the upper and lower arrays is also a quarter of wavelength.  

For this configuration scattering can occur either from an upper element or the one directly below it – but not from both simultaneously - so that we have a total of 16 possible scattering state combinations. However for boresight scattering, symmetry dictates that nine of these combinations produce identical solutions and so only five distinct scattering states exist. These points are shown in the constellation diagram of Figure 3 and exhibit the characteristics of multi-level BPSK modulation. Also shown in Figure 3 is the constellation diagram produced at a scattering angle of 450 and generated by the same set of tag modulation parameters that generated the 5 boresight points. From the constellation diagram it is clear that the modulation function has changed significantly with scattering angle, as the form of the modulation pattern at 450 has the characteristics of a multi-level QAM scheme.  This property of angle dependent modulation can be exploited to increase the security of data transmission and this will be examined and reported in the final paper. Simulated results are reported in Figure 4. The measured data from a prototype experimental system will be shown later.

Fig. 5 shows a animation of both ideal and measured constellation digram changing w.r.t. the scattering angle. It is very clear that the scattered signals away from boresight are identical to boresight. Thus it is hard for a listener at other directions to demodulate the original information even with the right demodulation scheme. 

A simple short-distance demodulation scheme are employed to test the reliability of the system. Fig. 6 shows the symbol error rate (SER) with respect to scattering angles. SER stays very low at boresight and near angle and rise up from 30 degree. The beam of the operating angle is about 50 degree.


Figure 3. Ideal constellation diagram

Figure 4. Simulated constellation diagram




Figure 5. Animation of Ideal  and Simulated constellation diagram w.r.t. scattering angle
Figure 6. demodulation error rate w.r.t sacttering angle


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[1] M. Daly and J. Bernhard, “Directional modulation technique for phased arrays,” IEEE Trans. on Antenna and Propagation, vol. 57, pp. 2633–2640, Sep. 2009



[2] H. Shi and A. Tennant, "Directional dependent antenna modulation using a two element array", Proc. of the 5th EUCAP, pp. 812-815, Apr. 2011






19.11.11

Basics-Microstrip Patch Antenna-1.Fundametals




all right reserved, docs for education uses only;
feel free to contact me: elq10yw@sheffield.ac.uk


PAPER- A Phase modulated RF tag

Introduction


A new form of RFID tag based on the concept of a phase-modulating surface is presented. The tag consists of a two by two array of pin diode controlled dipole elements. By applying individual d.c. control signals to each of the diodes, it is possible to modulate RF energy scattered from the tag. An experimental system is described and measurements made at 10GHz are presented to show that the tag can impart binary phase modulation onto interrogating signals.

Experimental system
The RF tag consists of an active surface placed in front of a conducting back-plane. The active surface is a 2 by 2 grid of pin-diode loaded dipoles and is separated from an Aluminium back-plane by a quarter-wavelength thick Rhoacell 51 foam spacer.
Independent switching of each element of the array provides a total of 16 possible scattering states. However if we consider normal incidence illumination of the tag and the mono-static scattered field, then the number of scattering state combinations reduces to five (Fig.4) .

Measurements
The experimental PMRF tag was tested in a NRL arch configured to measure mono-static back-scatter reflectivity using a Hewlett-Packard 8720B network analyser.

Conclusion
An experimental RF tag designed to operate at 10GHz has been designed and tested. Measured data shows that the tag behaves in a similar manner to that predicted by a simplified model, and that the tag can impart BPSK modulation onto a continuous wave incident signal.

This contribution has been published on Loughborough Antenna and Propagation Conference 2011. For further information, please contact elq10yw@sheffield.ac.uk 


Other authors are Dr. A. Tennant and Prof. R.J. Langley;


all rights reserved.