1 Introduction

Reconfigurable intelligent surface (RIS) is a revolutionizing technology which can configure wireless propagation environment by using a large number of low-cost passive reflecting elements where each passive element can induce amplitude and phase shifts thus beamforming and nulling the signal in an area of the interest (Kaina et al., 2014b; Basar et al., 2019; Tang et al., 2020a). RIS can be used to coat planar or conformal objects in the environment that constitute a radio channel such as walls, ceilings, building facades, furniture. Therefore, RIS can address the core problems of energy-efficiency, spectral-efficiency, co-channel interference, PHY layer security (Cui et al., 2019; Xu et al., 2021). Hence, RIS shall be central to 6G wireless communication Calvanese Strinati et al. (2021). Received power in RIS-assisted communication system is proportional to the number of elements used in the RIS, reflection coefficient and reflection-efficiency of the elements. Therefore, a large RIS with higher number of passive reflecting elements can optimize BLE link effectively. RIS do not use amplifiers, analog to digital converter/ digital to analog converter (ADC/DAC) and active RF chains therefore it consumes significantly less energy than the contemporary massive MIMO, active amplify and forward relaying technique Björnson et al. (2019). However, there are works which suggest usage of active sensor components in addition to passive elements for both pilot-based channel estimation and passive beamforming. A detailed assessment and performance analysis of reconfigurable intelligent surface and relaying in terms of diversity gain and end-to-end SNR is given in Boulogeorgos and Alexiou (2020). Authors in Hu et al. (2020) have developed experimental framework for RF sensing of RIS-assisted posture recognition. Authors in Dai et al. (2020), Tang et al. (2020b) have demonstrated RIS-based experimental prototypes for demonstration of wireless communication system. Authors in Dai et al. (2020) developed 256 element RIS prototype and demonstrated wireless communication systems with antenna gains of 21.7 dBi and 19.1 dBi at RF frequency of 2.3 and 28.5 GHz. A framework for joint trajectory and passive beamforming using RIS unmanned aerial vehicle (UAV) communication has been presented in Li et al. (2020). RIS is a cost-effective, energy-efficient and spectral-efficient solution for sixth-generation wireless communication as it will solve key technical issue of blockage at mmWave band and THz band where enormous bandwidth can be exploited to meet the user bandwidth requirements (Wu and Zhang, 2019; Yuan et al., 2021). Authors in Tan et al. (2018) have demonstrated RIS-assisted indoor link for IEEE 802.11ad at 60 GHz. RIS application at mmWave band can be used to overcome the sparsity of mmWave channels. Energy-efficiency of RIS has been studied by authors in Huang et al. (2019). RIS can also be useful for secondary user link optimization in cognitive radio and alleviating interference to primary user link Guan et al. (2020). Authors have presented sum-rate maximization of secondary user link subject to minimizing interference to primary user. Authors in Hou et al. (2019) have studied the issue of co-located multi-RIS deployment. The applications of RISs are diverse. We take the opportunity to propose the usage of RIS for low energy Bluetooth. BLE is a key short-range data transmission technology in internet of things along with Zigbee and narrowband internet of things (NB-IoT) that is used for multimedia file sharing, home automation, and other internet-of-things applications such as medical internet of things, smart homes, indoor positioning, and localization (Montoliu et al., 2020; Spachos and Plataniotis, 2020). We believe the usage of RIS in BLE framework can increase the signal quality, PER performance and also increase the overall lifetime of already energy-constraint IoT devices. In this work, we arranged master and slave BLE nodes in NLOS in a reverberant metal enclosure, an environment that has been tackled by other investigators in wireless communication (Gagliardi et al., 2015; Micheli et al., 2016; Barazzetta et al., 2017; Primiani et al., 2020; Micheli et al., 2021), as shown in Figure 1. We have optimized the PER performance using RIS of all the BLE PHY modes. We have divided our manuscript into four sections. Section 1 is introduction and motivation of the usage of RIS technology in BLE communication. Section 2 explains BLE baseband transmitter and receiver for BLE PER measurement as well as the measurement setup. Section 3 is measurement result about PER optimization using RIS. Finally, the conclusion is presented in section 4.

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FIGURE 1. RIS-assisted BLE PER measurement sketch.

2 BLE Baseband Tx/Rx Model and Measurement Setup

2.1 BLE Baseband Transmitter and Receiver

Baseband transmitter generates link layer PDUs and generates IQ waveforms which are passed to PlutoSDR for over-the-air transmission. Link layer PDUs are modelled as advertising channel PDUs or data channel PDUs. BLE receiver performs RF impairment compensation such as RF nonlinearity effect, carrier frequency offset, carrier phase offset, and symbol timing offset. Standard-compliant BLE receivers consist of automatic gain control (AGC) stage, DC compensation stage, matched filtering, carrier frequency offset (CFO) estimation, timing synchronization stage, demodulation, de-whitening, and CRC stage. After the initial receiver operations demodulation of Gaussian minimum shift keying (GMSK) symbols is accomplished and a CRC check is performed. The AGC component in the digital receiver is vital for the correct recovery of information and for end-to-end PER performance measurement. The AGC is the first stage where a weak signal is received and stabilized for further downstream processing. The AGC can be configured in slow-attack mode or fast-attack mode to track the received signal. Previously, we have recorded our experimental experience with AGC in the metal enclosure Lodro et al. (2020). The AGC helps for coarse and fine frequency correction in the baseband receiver. AGC is configured with maximum power gain of 20 dB and desired power of 2 W. After the AGC stage, DC removal in the received waveform is performed using a notch filter. The existence of the DC component is a common problem in radio receivers, and it is particularly common in direct-conversion receivers such as software-defined-radios. The next two stages are frequency offset correction and matched filtering. Frequency offset estimation and correction must be performed before received samples are processed by a matched filter. The matched filter increases the signal-to-noise (SNR) at the receiver i.e., it limits the amount of noise that is passed down to subsequent stages Litwin (2001) in the receiver. Coarse frequency compensation uses an FFT-based or correlation-based algorithm to measure frequency offset. Fine frequency and demodulation of GMSK packets are performed. Frame timing synchronization is performed using preamble detection which measures detection metric and the threshold. After these critical design stages, data decoding and de-mapping are performed. Long series of zeros and ones such as 000000 or 1111111 may occur in the data bitstream. Data whitening is used to avoid such a long sequence of ones and zeros. Data de-whitening and CRC are performed to measure the BLE PER. For the packet error measurement, access address is checked first and then CRC is checked, If the access address or CRC is incorrect then the packet shall be rejected. The received BLE packets are considered only valid when both access address and CRC check is correct. Figure 2 shows flowchart of the BLE link PER measurement process. First BLE PHY mode specific packetized baseband waveforms are generated which are then digital upconverted for over-the-air transmission. After the NLOS channel is tuned using RIS elements, the BLE packet capture is performed using Rx PlutoSDR. The captured packets are further processed using baseband BLE receiver at host PC. BLE operates using uncoded and coded PHY modes with minimum and maximum data-rates of 125 Kbps for coded and 2 Mbps for uncoded respectively. Packet format for uncoded and coded BLE PHY modes consists of 32-bit access address, 16-bit header length, 24-bit cyclic redundancy check (CRC), and 16-bit to 2056-bit protocol data unit (PDU) with additional term1 and term2 fields for coded BLE PHY modes. Preamble field for uncoded and coded BLE PHY mode is 8/16-bit and 80-bit, respectively. We presented PER measurement of BLE in presence of WLAN interference in reverberation chamber but without reconfigurable intelligent surface Lodro et al. (2021).

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FIGURE 2. RIS-assisted BLE PER measurement flowchart.

2.2 Measurement Setup

We created BLE communication link in neighbor discovery mode in the metal enclosure. The metal enclosure used has dimensions of h × × w of 1 × 0.8 × 1 m3. We used two PlutoSDRs from Analog Devices Inc. (ADI) for BLE communication link in metal enclosure. PlutoSDR is a low-cost full-duplex transceiver with ADI 9363 integrated RFIC with operating frequency range from 325 MHz to 3.8 GHz and its RF frequency range is software upgradeable upto 6 GHz. The transmitter (Tx) and receiver (Rx) PlutoSDRs are connected with host PC for exchanging transmitted and received complex signal samples. We also connected RISs via USB-serial port with the same host PC. Each RIS plate consists of eight rows and ten columns of passive elements. Therefore, the RIS can introduce discrete phase shifts to incident signal. We also connected RIS manufactured and patented by GREENERWAVE (https://greenerwave.com/) to the same host PC through USB serial port. The same USB port is used to simultaneously power the integrated control board of the RIS and send commands that impose RIS configuration by controlling the bias voltage of a set of PIN diodes through a set of shift registers. Each surfaces consists of 76 phase-binary pixels, which are based on hybridizing two resonances Kaina et al. (2014a). Each pixel can be configured electronically to control independently, via the states of two PIN diodes, both components of the reflected electric field tangential to the pixel plane by imposing a 0 or π phase, thus leading to a total number of 152 effective pixels per RIS. The transmitter and receiver BLE baseband models run in separate MATLAB sessions. We considered RIS-assisted non-LOS (NLOS) single-input single-output (SISO) BLE communication link by using directional Tx antenna. The direction of peak radiation of transmitting antenna is pointed towards RIS. This means the multipath contribution at the receiver is largely from the RIS. There is line-of-sight (LOS) between transmitter and the RIS for leveraging maximum benefits from RIS beamforming. RIS can be deployed closer to transmitter or closer to user to fully exploit RIS passive beamforming. In our work, transmitter is located closer to RIS and there is no direct link between transmitter (Master) and receiver (Slave). Hence, PER measurement takes place using cascaded channel i.e. Master-RIS-Slave link in neighbour discovery (NDP) mode. BLE PHY mode specific waveforms are generated using MATLAB-based BLE baseband transmitter. Complex waveform samples are transferred to Tx PlutoSDR for over-the-air transmission in metal enclosure. The metal enclosure is perfectly reflecting environment and it supports rich multipath scattering. The measurements are conducted in stationary environment i.e. there is no active mode-stirrer inside metal enclosure except two PlutoSDRs, two RISs and ten pieces of standard RF absorber cones. We conducted BLE PER measurements using one RIS with Tx antenna pointing towards RIS as shown in Figure 3. Then we conducted PER optimization of BLE modes using two RISs in distributed and centralized arrangement. In distributed arrangement, the RIS 1 was located closer to Tx and the RIS 2 was located at some distance from RIS 1. Similarly, in centralized arrangement RIS 1 and RIS 2 were colocated with Tx antenna pointing towards RISs. Mode specific BLE packet waveforms are captured by Rx PlutoSDR which are digital-downconverted to complex baseband samples for processing in the BLE baseband receiver.

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FIGURE 3. Measurement setup (A) metal enclosure (B) distributed RISs (C) centralized or co-located RISs.

3 Measurement Results

The RIS manipulates impinging electromagnetic waves and increases signal power using quasi-passive beamforming at the receiver. Received signal power in RIS-assisted communication depends on transmitted signal power, transmit and receive antenna gains and their polarization, gain and size of the unit cell, and frequency of operation. More importantly, it also depends on the method of RIS-element excitation. We performed PER for 190 random configurations using one RIS and 380 random configurations using two RISs. Random samples are generated for each measurement iteration. PER optimization is performed and the RIS values are considered which gives PER equal to or less than the current PER value. BLE system parameters and radio parameters are shown in Table. 1. PER performance of BLE PHY modes (see Figure 4) shows BLE LE2M PHY mode has worst PER followed by LE1M. LE1M and LE2M are uncoded PHY modes. Coded BLE PHY modes i.e., LE500K and LE125K show better PER than the uncoded LE1M and LE2M, respectively. The reason for better PER for coded BLE PHY modes is because of the forward coding and low data rates. Similarly, among uncoded standard LE2M has higher data rate than the LE1M and because of higher data rates LE2M BLE link has higher PER. For initial RIS configuration PER for all BLE PHY modes is high as shown in Figure 5. After the RIS tunes its element properties, the PER for all BLE PHY modes improves. Figure 6 shows empirical CDF of PER of all BLE PHY modes with 99% confidence interval. The coded BLE PHY mode outperforms uncoded BLE PHY modes with lowest PER for LE125K and highest PER for LE2M. Lastly, the PER for all the BLE PHY modes is optimized using reconfigurable intelligent surface.

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TABLE 1. BLE system and radio parameters.

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FIGURE 4. PER measurement results of all the BLE PHY modes as a function of random RIS configuration. The PER measurements are performed with one RIS.

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FIGURE 5. Optimized PER results of all the BLE PHY modes as a function of optimized RIS configuration. The PER measurements are performed with one RIS.

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FIGURE 6. Empirical CDF of PER measurements of all PHY modes of BLE using one RIS.

Figure 7 shows PER of all the BLE PHY modes for 8×38 RIS configurations. Similarly, Figures 8, 9 show optimized PER and empirical CDF of PER of all the BLE PHY modes in distributed arrangement of RISs. PER measurements of all the BLE PHY modes in centralized RIS arrangement is shown in Figure 10. The average BLE PER for 2 Mbps LE2M mode is higher than rest of the BLE PHY modes both uncoded and coded. Coded LE500K and LE125K are superior in terms of PER performance. Similarly, Figures 8, 11 show optimized PER of all BLE PHY modes in presence of two RIS in distributed and centralized arrangement. Like our previous observations with one RIS, the LE2M PER using two RISs is higher than the PER of rest of PHY modes for both RISs arrangements. Optimized PER of LE1M is lower than the LE2M PER and is in accordance with the data-rate intuition. LE125K has the lowest PER of all BLE PHY modes (see Figures 9, 12). It can be noticed that the performance of centralized RISs is higher than than distributed RISs. The radiation pattern of the Tx Antenna intercepts only one RIS in the distributed scenario, while it intercepts both the RISs in the centralized scenario. Hence, the centralized scenario benefits from channel hardening.

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FIGURE 7. PER measurement results of all the BLE PHY modes using two RIS as a function of random RIS configuration. The PER measurements are performed with distributed RISs.

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FIGURE 8. PER measurement results of all the BLE PHY modes using two RIS as a function of optimized RIS configuration. The PER measurements are performed with distributed RISs.

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FIGURE 9. Empirical CDF of PER measurements of all PHY modes of BLE using distributed RISs.

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FIGURE 10. PER measurement results of all the BLE PHY modes using two RIS as a function of random RIS configuration. The PER measurements are performed with centralized RISs.

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FIGURE 11. PER measurement results of all the BLE PHY modes using two RIS as a function of optimized RIS configuration. The PER measurements done with centralized RISs.

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FIGURE 12. Empirical CDF of PER measurements of all PHY modes of BLE using centralized RISs.

From our measurements it is shown that the BLE link PER reliability increases when we increase the RIS size as shown in Figures 6, 9, 12, respectively. Additionally, the reliability of BLE link is higher for centralized arrangement than the distributed arrangement. Additionally, irrespective of RIS size the reliability of coded BLE PHY mode i.e. LE125K is highest than the rest of BLE PHY modes. Finally, it can be noticed that the uncoded BLE PHY modes LE2M reliability increases with the increase in RIS size. This suggests that the usage of RIS and increased size of RIS can sustain higher data rates. Figures 1315 shows final best configuration using one RIS, and two RISs in distributed and centralized configurations respectively. These final configurations yield the optimized PER for all BLE PHY modes using one RIS and two RISs respectively.

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FIGURE 13. Optimized binary coding matrices representing final configurations of the RIS for LE1M, LE2M, LE500K, and LE125K.

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FIGURE 14. Optimized binary coding matrices representing final configurations of the two distributed RISs for LE1M, LE2M, LE500K, and LE125K.

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FIGURE 15. Optimized binary coding matrices representing final configurations of the two centralized RISs for LE1M, LE2M, LE500K, and LE125K.

4 Conclusion

In this work, we created RIS-assisted programmable radio environment, contrary to legacy radio channels, programmable radio channel creates a degree of freedom for PER optimization. We demonstrated RIS-assisted BLE communication link in metal enclosure. We checked the PER performance of four BLE PHY layer modes and optimized the BLE PER for all the BLE PHY modes. From measurement results we conclude that the RIS successfully optimized PER of all BLE PHY modes. Out of two RISs arrangements centralized arrangement is better than the distributed arrangement. One potential reason could be the path loss between transmitter and the RIS is higher in distributed arrangement than in the centralized arrangement where the Tx antenna pointing towards RISs illuminates RISs at same length with same power. Future aspect of the research is to perform PER optimization in presence of active RF interference signals.

Data Availability Statement

The raw data supporting the conclusion of this article will be made available by the authors, without undue reservation.

Author Contributions

ML performed measurements and covered mainly the SDR aspect of the research and did data analysis. J-BG created the measurement setup and the optimization code. GG directed reverberation and metal enclosure effects related aspects of the research. SG and GL arranged measurement equipment and presented some thoughts on the results.

Funding

This work was supported by the European Commission through the H2020 RISE-6G Project under Grant 101017011, and in part by the Royal Society under Grant INFR2192066.

Conflict of Interest

Authors J-BG and GL were employed by the company Greenerwave.

The remaining author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s Note

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References


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