Issue 
EPJ Applied Metamaterials
Volume 3, 2016
MetamaterialbyDesign: Theory, Methods, and Applications



Article Number  1  
Number of page(s)  6  
DOI  https://doi.org/10.1051/epjam/2016002  
Published online  07 June 2016 
https://doi.org/10.1051/epjam/2016002
Research Article
Spectral signature barcodes based on Sshaped Split Ring Resonators (SSRRs)
CIMITEC, Departament d’Enginyeria Electrònica, Universitat Autònoma de Barcelona, 08193
Bellaterra, Spain
^{*} email: cristian.herrojo@uab.cat
Received:
26
February
2016
Accepted:
26
April
2016
Published online: 7 June 2016
In this paper, it is shown that Sshaped split ring resonators (SSRRs) are useful particles for the implementation of spectral signature (i.e., a class of radiofrequency) barcodes based on coplanar waveguide (CPW) transmission lines loaded with such resonant elements. By virtue of its S shape, these resonators are electrically small. Hence SSRRs are of interest for the miniaturization of the barcodes, since multiple resonators, each tuned at a different frequency, are used for encoding purposes. In particular, a 10bit barcode occupying 1 GHz spectral bandwidth centered at 2.5 GHz, with dimensions of 9 cm^{2}, is presented in this paper.
Key words: Split ring resonators (SRRs) / Radiofrequency barcodes / Chipless RFID
© C. Herrojo et al., Published by EDP Sciences, 2016
This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1 Introduction
Metamaterial transmission lines can be implemented by loading a host line with electrically small resonant elements, such as split ring resonators (SRRs) [1], or complementary split ring resonators (CSRRs) [2], among others. Many microwave devices based on these artificial lines have been designed on the basis of the further controllability, as compared to ordinary lines, of line impedance and dispersion [3], achieved by virtue of the loading elements (which provide more degrees of freedom for device design). The key aspect in these designs is thus impedance and dispersion engineering. However, in other applications, the resonance phenomenon is the key aspect. In this case, where the functionality is based on particle resonance (rather than on impedance and dispersion engineering), the lines are usually referred to as transmission lines with metamaterial loading [3]. These structures have been applied to the design of planar bandstop and notch filters [4, 5], multiband printed dipole and monopole antennas [6–8], commonmode suppressed differential lines and filters [9, 10], microwave sensors [11–18], and radiofrequency barcodes [19–21], among others.
In this work, radiofrequency barcodes implemented by means of Sshaped SRRs (SSRRs), previously used for the implementation of metamaterials [22–24], are presented in a journal paper for the first time. SSRRs are electrically smaller than electricLC resonators (ELC) and even smaller than split ring resonators (SRRs) [15]. Thus, high miniaturization levels can be obtained by using SSRRs, with direct impact on the achievable number of bits per cm^{2}, superior in SSRRbased barcodes.
SSRRs have been successfully applied to the design of microwave filters [25] and sensors [26] as well. Coupled to CPW transmission lines, SSRRs generate notches (transmission zeros) in the transmission coefficient at their resonance frequency. However, through a proper orientation, line to resonator coupling can be prevented, and hence the presence or absence of the transmission zero can be controlled, and this is used for encoding, as will be later shown.
2 Topology and working principle
The typical topology of this particle is depicted in Figure 1. This particle cannot be excited by means of an uniform timevarying magnetic field applied in the direction orthogonal to the plane of the particle, contrary to SRRs [1, 27], but it can be driven by means of counter magnetic fields, as depicted in the figure, and similar to the excitation of electric LC (ELC) resonant particles [28]. According to this, it follows that by etching these SSRRs on the back substrate side of a coplanar waveguide (CPW), the fundamental resonance can be excited as long as each loop of the particle lies on bottom of one of the slots of the CPW, as indicated in Figure 2. However, by rotating the particle 90° (0° orientation in Figure 2), no significant excitation is expected since there is not a net magnetic field in each loop, able to induce a current. According to this, SSRRs are useful for the implementation of multiresonator [19, 20] spectral signature barcodes for chipless RFID, where each resonator corresponds to a bit and the “0” or “1” logic states are simply set by the orientation of the SSRRs.
Figure 1. Typical topology of an SSRR and indication of the driving mechanism by means of countermagnetic fields. 
Figure 2. Response of the CPW loaded with a single SSRR for the two considered states: “1” (90°) and “0” (0°). 
3 Circuit model and design
The typical topology (including relevant dimensions) and circuit model of a CPW loaded with a square SSRR, etched on the back substrate side, are depicted in Figure 3 [26]. The line is modeled by the inductance L and the capacitance C, the SSRR is described by the capacitance C_{s} and by the inductance of each loop, L_{s}. Finally, the coupling between the line and the resonator is accounted for by the mutual inductance 2M. Note that this model is formally identical to the one describing a SRRloaded CPW transmission line [1, 3]. As discussed in [26], the mutual coupling depends on the relative orientation between the line and the resonator, it being maximum for the 90° orientation, i.e., the one indicated in Figure 3a. In the circuit of Figure 3b, losses have been excluded. This circuit can be transformed to the one indicated in Figure 3c, where the reactive elements of both models are related by [3]:(1) (2) (3)and the notch (angular) frequency is given by(4)
Figure 3. Topology of a SSRRloaded CPW (a), lumped element equivalent circuit model (b), and transformed model (c). 
This model has been validated by parameter extraction, following the procedure reported in [29]. Figure 4 shows the frequency response of a particular SSRRloaded CPW, where both the lossless electromagnetic (inferred from Keysight Momentum) and circuit simulations are compared. The considered substrate is Rogers RO4003C with dielectric constant ε_{r} = 3.55 and thickness h = 0.81 mm (dimensions as well as circuit element values are indicated in the caption). As can be appreciated, there is very good agreement between the circuit and electromagnetic simulations in the frequency range of interest, pointing out the validity of the lumped element equivalent circuit model.
Figure 4. Frequency response of a CPW loaded with a square SSRR. (a) Magnitude response; (b) phase response. Dimensions are: l_{r} = w_{r} = 5.6 mm, w_{l} = s = 0.2 mm, w_{c} = 2.87 mm, and l_{c} = 0.47 mm. Line dimensions are: W = 2.1 mm, g = 0.2 mm corresponding to a 50 Ω transmission line. The extracted element values are: C = 0.92 pF, L′ = 1.69 nH, C_{s}′ = 58.6 pF, and L_{s}′ = 69.8 pH. 
For design purposes, there are two important parameters: the notch depth, and the −3 dB notch bandwidth. In order to accommodate the largest number of bits in a given spectral bandwidth, it is convenient to reduce the notch bandwidth of each individual resonator as much as possible, but, due to losses, this affects the notch depth, reducing its magnitude and consequently jeopardizing the correct reading of the written code. Therefore, a tradeoff results. To gain insight into this important aspect, let us now consider the presence of losses in the circuit models (Figure 5). The notch magnitude in the circuit of Figure 5b can be expressed as [26]: (5)where Z_{s} is the impedance of the series branch, Y_{p} is the admittance of the shunt branch, and Z_{0} is the port impedance. The previous expression, evaluated at resonance, can be written as:(6)where Z_{L′} is the impedance of the line inductance. To the light of equation (6), M tends to increase the notch depth, whereas an increase in R_{s} reduces the magnitude of the notch, as expected. Nevertheless, R_{s} is not a design parameter, contrary to M, which depends on SSRR orientation and also on substrate thickness. Note that, according to expressions (1) and (2), if M increases, L_{s}′ also increases, whereas C_{s}′ decreases, thereby enhancing the bandwidth (related to the ratio L_{s}′/C_{s}′).
Figure 5. Lossy equivalent circuit model of an SSRRloaded CPW. (a) Simplified model and (b) equivalent transformed model. 
By considering the substrate permittivity and thickness indicated before (ε_{r} = 3.55, and h = 0.81 mm) and a loss tangent of tan δ = 0.0021, we have obtained the frequency response of the SSRRloaded CPW of Figure 2, inferred from electromagnetic simulation with losses (the conductivity of copper for the metallic layers has been assumed). Then we have repeated these electromagnetic simulations by considering different substrate thicknesses, in order to infer the effect of M on bandwidth and notch depth. The results are depicted in Figure 6, where we have also included the dependence of L_{s}′/C_{s}′ on substrate thickness. In order to accommodate 10 bits (and hence 10 resonators) in a 1 GHz spectral bandwidth between 2 GHz and 3 GHz, it is necessary to limit the resonator bandwidths to less than 100 MHz. In view of Figure 6, for the thickness of h = 0.81 mm, the notch depth is found to be larger than 10 dB, which is a reasonable value to adequately read the “1” logic states, whereas this thickness clearly gives a bandwidth much smaller than 100 MHz. Therefore, this has been the considered thickness value, which corresponds to a commercially available microwave substrate. From the considered resonator (with a frequency of 2.5 GHz), the other resonant elements have been obtained by merely scaling the length of the loops.
Figure 6. Dependence of the notch bandwidth (a), L_{s}′/C_{s}′ (b), and notch depth (c) with substrate thickness. 
4 Results
The topology of the SSRR with reference frequency has been determined with a relatively small value of L_{s} and large value of C_{s} (significant L_{s}′/C_{s}′ ratio) in order to achieve a notch depth of at least 10 dB. The dimensions are l_{r} = w_{r} = 6.4 mm, w_{l} = 0.5 mm, s = 0.2 mm, w_{c} = 2.9 mm, and l_{c} = 0.5 mm. After scaling, in order to generate notch frequencies equally distributed within the bandwidth 2–3 GHz, we have implemented several codes by loading the CPW with such resonant elements, where the “1” and “0’ logic states have been simply achieved by properly orienting the SSRRs. The four considered codes and the corresponding frequency responses (inferred from lossy electromagnetic simulations and measurements) are depicted in Figure 7. Note that the ground plane regions of the CPW are connected by means of backside strips and vias in order to avoid the generation of the parasitic slot mode. The measured responses have been achieved by means of the Agilent N5221A vector network analyzer. According to Figure 7, there is good agreement between the electromagnetic simulation and measurement, and the different code responses reveal that a threshold of 5 dB suffices to distinguish between the “0” and “1” logic states. The area of the codes is as small as 9 cm^{2}. Moreover, the fact that by rotating the SSRR the coupling can be controlled opens the possibility of increasing the number of states per resonator, and thus increase the information density per GHz (work is in progress).
Figure 7. Simulated and measured transmission coefficient of the corresponding indicated codes. 
5 Conclusions
In summary, novel spectral signature barcodes implemented by loading a CPW with SSRRs have been proposed. On the basis of the lumped element equivalent circuit model, which has been validated through parameter extraction, we have analyzed the effects of line to resonator coupling and losses on the response of the SSRR loaded CPW. Particularly, it has been found that by increasing the mutual coupling, the notch magnitude of the structure is enhanced but at the expense of a broader bandwidth. Hence, it has been concluded that a tradeoff for design purposes is necessary, and with this in mind we have designed the SSRRs in order to accommodate 10 notches (corresponding to 10 bits) in a 1 GHz spectral bandwidth between 2 GHz and 3 GHz. The resulting codes, smaller than 9 cm^{2}, exhibit responses that can be easily read, with equidistant notches for the extreme case where all the bits are set to the “1” state.
Acknowledgments
This work was supported by MINECOSpain (projects TEC201340600R and RTC201425507 ChiplessRFID), by Generalitat de Catalunya (project 2014SGR157), by Institució Catalana de Recerca i Estudis Avançats (who awarded Ferran Martín), and by FEDER funds. Cristian Herrojo has been granted by MINECO with the grant number BES2014068164.
References
 F. Martín, F. Falcone, J. Bonache, R. Marqués, M. Sorolla, Split ring resonator based left handed coplanar waveguide, Appl. Phys. Lett. 83 (2003) 4652–4654. [CrossRef] [Google Scholar]
 F. Falcone, T. Lopetegi, J.D. Baena, R. Marqués, F. Martín, M. Sorolla, Effective negativeepsilon stopband microstrip lines based on complementary split ring resonators, IEEE Microw. Wirel. Compon. Lett. 14 (2004) 280–282. [CrossRef] [Google Scholar]
 F. Martín, Artificial Transmission Lines for RF and Microwave Applications, John Wiley, Hoboken, NJ, 2015. [CrossRef] [Google Scholar]
 F. Martín, F. Falcone, J. Bonache, R. Marqués, M. Sorolla, Miniaturized CPW stop band filters based on multiple tuned split ring resonators, IEEE Microw. Wirel. Compon. Lett. 13 (2003) 511–513. [CrossRef] [Google Scholar]
 J. GarcíaGarcía, J. Bonache, I. Gil, F. Martín, R. Marqués, F. Falcone, T. Lopetegi, M.A.G. Laso, M. Sorolla, Comparison of electromagnetic bandgap and split rings resonator microstrip lines as stop band structures, Microw. Opt. Technol. Lett. 44 (2005) 376–379. [CrossRef] [Google Scholar]
 F.J. HerraizMartínez, L.E. GarcíaMuñoz, D. GonzálezOvejero, V. GonzálezPosadas, D. SegoviaVargas, Dualfrequency printed dipole loaded with split ring resonators, IEEE Antennas Wirel. Propag. Lett. 8 (2009) 137–140. [CrossRef] [Google Scholar]
 F.J. HerraizMartínez, G. Zamora, F. Paredes, F. Martín, J. Bonache, Multiband printed monopole antennas loaded with open complementary split ring resonators for PANs and WLANs, IEEE Antennas Wirel. Propag. Lett. 10 (2011) 1528–1531. [CrossRef] [Google Scholar]
 F.J. HerraizMartínez, F. Paredes, G. Zamora, F. Martín, J. Bonache, Dualband printed dipole antenna loaded with open complementary splitring resonators (OCSRRs) for wireless applications, Microw. Opt. Technol. Lett. 54 (2012) 1014–1017. [CrossRef] [Google Scholar]
 J. Naqui, A. FernándezPrieto, M. DuránSindreu, F. Mesa, J. Martel, F. Medina, F. Martín, Common mode suppression in microstrip differential lines by means of complementary split ring resonators: theory and applications, IEEE Trans. Microwave Theor. Tech. 60 (2012) 3023–3034. [CrossRef] [Google Scholar]
 P. Vélez, J. Naqui, A. FernándezPrieto, M. DuránSindreu, J. Bonache, J. Martel, F. Medina, F. Martín, Differential bandpass filter with common mode suppression based on open split ring resonators and open complementary split ring resonators, IEEE Microw. Wirel. Compon. Lett. 23 (1) (2013) 22–24. [CrossRef] [Google Scholar]
 M. Puentes, C. Weiss, M. Schüßler, R. Jakoby, Sensor array based on split ring resonators for analysis of organic tissues, IEEE MTTS International Microwave Symposium Digest, Baltimore, MD, USA, 2011, pp. 5–10. [Google Scholar]
 J. Naqui, M. DuránSindreu, F. Martín, Novel sensors based on the symmetry properties of Split Ring Resonators (SRRs), Sensors 11 (2011) 7545–7553. [CrossRef] [Google Scholar]
 M.S. Boybay, O.M. Ramahi, Material characterization using complementary splitring resonators, IEEE Trans. Instrum. Meas. 61 (2012) 3039–3046. [CrossRef] [Google Scholar]
 J. Naqui, M. DuránSindreu, F. Martín, Alignment and position sensors based on split ring resonators, Sensors 12 (2012) 11790–11797. [CrossRef] [Google Scholar]
 J. Naqui, F. Martín, Transmission lines loaded with bisymmetric resonators and their application to angular displacement and velocity sensors, IEEE Trans. Microwave Theor. Tech. 61 (2013) 4700–4713. [CrossRef] [Google Scholar]
 A. Abduljabar, D. Rowe, A. Porch, D. Barrow, Novel microwave microfluidic sensor using a microstrip splitring resonator, IEEE Trans. Microwave Theor. Tech. 62 (2014) 679–688. [CrossRef] [Google Scholar]
 A. Ebrahimi, W. Withayachumnankul, S. AlSarawi, D. Abbott, Highsensitivity metamaterialinspired sensor for microfluidic dielectric characterization, IEEE Sens. J. 14 (2014) 1345–1351. [CrossRef] [Google Scholar]
 A. Ebrahimi, W. Withayachumnankul, S.F. AlSarawi, D. Abbott, Metamaterialinspired rotation sensor with wide dynamic range, IEEE Sens. J. 14 (2014) 2609–2614. [CrossRef] [Google Scholar]
 S. Preradovic, N.C. Karmakar, Chipless RFID: bar code of the future, IEEE Microw. Mag. 11 (2010) 87–97. [CrossRef] [Google Scholar]
 S. Preradovic, I. Balbin, N.C. Karmakar, G.F. Swiegers, Multiresonatorbased chipless RFID system for lowcost item tracking, IEEE Trans. Microwave Theor. Tech. 57 (2009) 1411–1419. [CrossRef] [Google Scholar]
 J. Naqui, M. DuránSindreu, F. Martín, On the symmetry properties of coplanar waveguides loaded with symmetric resonators: analysis and potential applications, IEEE MTTS Int. Microwave Symp. Dig, Montreal (Canada), 2012. [Google Scholar]
 H. Chen, L. Ran, J. Huangfu, X. Zhang, K. Chen, T.M. Grzegorczyk, J.A. Kong, Lefthanded materials composed of only Sshaped resonators, Phys. Rev. E 70 (2004) 057605. [CrossRef] [Google Scholar]
 H. Chen, L. Ran, J. Huangfu, X. Zhang, K. Chen, T.M. Grzegorczyk, J.A. Kong, Negative refraction of a combined double Sshaped metamaterial, Appl. Phys. Lett. 86 (2005) 151909. [CrossRef] [Google Scholar]
 H. Chen, L.X. Ran, J.T. HuangFu, X.M. Zhang, K.S. Cheng, T.M. Grzegorczyk, J.A. Kong, Magnetic properties of Sshaped split ring resonators, Progress Electromagn. Res. 51 (2005) 231–247. [CrossRef] [Google Scholar]
 A.K. Horestani, M. DuránSindreu, J. Naqui, C. Fumeaux, F. Martín, Compact coplanar waveguide bandpass filter based on coupled Sshaped split ring resonators, Microw. Opt. Technol. Lett. 57 (2015) 1113–1116. [CrossRef] [Google Scholar]
 J. Naqui, J. Coromina, A. KaramiHorestani, C. Fumeaux, F. Martín, Angular displacement and velocity sensors based on coplanar waveguides (CPWs) loaded with Sshaped split ring resonator (SSRR), Sensors 15 (2015) 9628–9650. [CrossRef] [Google Scholar]
 J.B. Pendry, A.J. Holden, D.J. Robbins, W.J. Stewart, Magnetism from conductors and enhanced nonlinear phenomena, IEEE Trans. Microwave Theor. Tech. 47 (1999) 2075–2084. [CrossRef] [Google Scholar]
 D. Schurig, J.J. Mock, D.R. Smith, Electricfieldcoupled resonators for negative permittivity metamaterials, Appl. Phys. Lett. 88 (2006) 041109. [CrossRef] [Google Scholar]
 F. Aznar, M. Gil, J. Bonache, J.D. Baena, L. Jelinek, R. Marqués, F. Martín, Characterization of miniaturized metamaterial resonators coupled to planar transmission lines, J. Appl. Phys. 104 (2008) 11450118. [CrossRef] [Google Scholar]
Cite this article as: Herrojo C, Naqui J, Paredes F & Martín F: Spectral signature barcodes based on Sshaped Split Ring Resonators (S64 SRRs). EPJ Appl. Metamat. 2016, 3, 1.
All Figures
Figure 1. Typical topology of an SSRR and indication of the driving mechanism by means of countermagnetic fields. 

In the text 
Figure 2. Response of the CPW loaded with a single SSRR for the two considered states: “1” (90°) and “0” (0°). 

In the text 
Figure 3. Topology of a SSRRloaded CPW (a), lumped element equivalent circuit model (b), and transformed model (c). 

In the text 
Figure 4. Frequency response of a CPW loaded with a square SSRR. (a) Magnitude response; (b) phase response. Dimensions are: l_{r} = w_{r} = 5.6 mm, w_{l} = s = 0.2 mm, w_{c} = 2.87 mm, and l_{c} = 0.47 mm. Line dimensions are: W = 2.1 mm, g = 0.2 mm corresponding to a 50 Ω transmission line. The extracted element values are: C = 0.92 pF, L′ = 1.69 nH, C_{s}′ = 58.6 pF, and L_{s}′ = 69.8 pH. 

In the text 
Figure 5. Lossy equivalent circuit model of an SSRRloaded CPW. (a) Simplified model and (b) equivalent transformed model. 

In the text 
Figure 6. Dependence of the notch bandwidth (a), L_{s}′/C_{s}′ (b), and notch depth (c) with substrate thickness. 

In the text 
Figure 7. Simulated and measured transmission coefficient of the corresponding indicated codes. 

In the text 
Current usage metrics show cumulative count of Article Views (fulltext article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 4896 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.