Self-Interference Measurements and Analysis of Co-time Co-frequency Full Duplex Arrays in U6G Frequency Band

SHI Chengzhe; LI Weishi; LI Tong; PAN Wensheng; SHEN Ying; SHAO Shihai

doi:10.11999/JEIT241086

Volume 47 Issue 7

Jul. 2025

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Article Navigation > Journal of Electronics & Information Technology > 2025 > 47(7): 2036-2049

SHI Chengzhe, LI Weishi, LI Tong, PAN Wensheng, SHEN Ying, SHAO Shihai. Self-Interference Measurements and Analysis of Co-time Co-frequency Full Duplex Arrays in U6G Frequency Band[J]. Journal of Electronics & Information Technology, 2025, 47(7): 2036-2049. doi: 10.11999/JEIT241086

Citation:

SHI Chengzhe, LI Weishi, LI Tong, PAN Wensheng, SHEN Ying, SHAO Shihai. Self-Interference Measurements and Analysis of Co-time Co-frequency Full Duplex Arrays in U6G Frequency Band[J]. Journal of Electronics & Information Technology, 2025, 47(7): 2036-2049. doi: 10.11999/JEIT241086

Citation:

SHI Chengzhe, LI Weishi, LI Tong, PAN Wensheng, SHEN Ying, SHAO Shihai. Self-Interference Measurements and Analysis of Co-time Co-frequency Full Duplex Arrays in U6G Frequency Band[J]. Journal of Electronics & Information Technology, 2025, 47(7): 2036-2049. doi: 10.11999/JEIT241086

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Self-Interference Measurements and Analysis of Co-time Co-frequency Full Duplex Arrays in U6G Frequency Band

doi: 10.11999/JEIT241086 cstr: 32379.14.JEIT241086

National Key Laboratory of Wireless Communications, University of Electronic Science and Technology of China, Chengdu 611731, China

Funds: The National Natural Science Foundation of China (62071094), The National Key Laboratory of Wireless Communications Foundation (IFN202402), The Postdoctoral Fellowship Program (Grade C) of China Postdoctoral Science Foundation (GZC20240217)

Received Date: 2024-12-08
Rev Recd Date: 2025-05-07

Available Online: 2025-05-22

Publish Date: 2025-07-22

Abstract

Abstract

Objective The U6G frequency band spans a continuous 700 MHz bandwidth, aligning closely with the Sub-6GHz range. It offers a balance between low-frequency coverage capabilities and high-frequency capacity advantages, making it suitable for the deployment of future 5G-A and 6G systems. With the growing demand for wireless communication services and the limited availability of spectrum resources in future networks, the need for full-duplex technology has emerged. A U6G full-duplex transceiver, with sufficient transmit-receive isolation, can transmit and receive simultaneously within the same frequency band, effectively doubling spectral efficiency compared to Time-Division Duplex (TDD) or Frequency-Division Duplex (FDD) systems. However, full-duplex systems with large-scale array antennas face the challenge of complex multi-dimensional cross-coupling strong self-interference. Near-field coupling self-interference can degrade reception sensitivity, potentially leading to the saturation of low-noise amplifiers. Understanding the near-field coupling characteristics of self-interference between arrays is crucial for evaluating the proposed full-duplex industrial standards and protocols. Currently, self-interference measurements for array systems primarily focus on the millimeter-wave band, with research on array-to-array self-interference in the U6G band being relatively scarce, mostly limited to single-antenna configurations. This work utilizes an analog beamforming phased array platform capable of precise beam steering to conduct large-scale full-duplex array self-interference coupling channel measurements in the U6G band, completing nearly 3.6 million measurements. Through these self-interference coupling channel measurements between beams as well as between array elements, an in-depth analysis is provided on the angular and physical spatial distribution characteristics of transmit-receive isolation, and the inherent connection between element-to-element coupling and beam-to-beam coupling is revealed. Methods In this work, a 128T-128R phased array platform with analog beamforming capability is deployed in an outdoor environment. Frequency-domain measurement techniques are employed to acquire the frequency response of the self-interference coupling channels between different transmit and receive beams, as well as between array elements. The spatial and numerical distribution characteristics of the coupling self-interference are analyzed using transmit-receive isolation as the evaluation criterion. The measurement process utilizes a dual-port vector network analyzer, with stepwise frequency scanning conducted across the 6675～6875 MHz band (with a total measurement bandwidth of 200 MHz) to measure the frequency response of the self-interference channels. For beam-to-beam coupling channels, the azimuth sweep range is set from –60° to +60°, and the elevation sweep range is from –30° to +30°, with a step interval of 2°, resulting in a total of 3,575,881 sets of beam-to-beam coupling channel data. For element-to-element coupling channels, only one pair of transmit-receive elements is excited at a time, while all other transmit and receive elements are turned off. This measurement process covers all possible transmit-receive element pairs, yielding a total of 16,384 sets of element-to-element coupling channel data. Results and Discussions The analysis of the transmit-receive isolation between beams reveals that the maximum and minimum isolation between the transmit and receive beams are 52.17 dB and –6.25 dB, respectively. Approximately 95% of the isolation values fall between 10 dB and 40 dB, with a median isolation of 26.66 dB (Fig. 6). The isolation distribution between beams exhibits strong spatial symmetry and directionality (Fig. 7, Fig. 8, Fig. 9, Fig. 10). Specifically, steering the transmit and receive beams along the direction of the array causes significant variations in the self-interference coupling, with no transmit and receive beams consistently providing high or low isolation (Fig. 7). Moreover, in the U6G frequency band, the sensitivity of self-interference coupling to beam steering is much weaker than in the millimeter-wave frequency band (Fig. 9). Therefore, relying on beam steering to reduce self-interference in the U6G frequency band may be inefficient and result in suboptimal performance.The analysis of the transmit-receive isolation between array elements indicates that the maximum and minimum isolation between transmit and receive elements are 88.08 dB and 54.48 dB, respectively. Approximately 95% of the isolation values fall between 63 dB and 76 dB, with a median isolation of 69.43 dB (Fig. 11). Even with the same element spacing, the isolation between elements is not necessarily the same; multiple isolation mappings exist for the same distance (Fig. 12). This many-to-one mapping relationship is likely due to differences in multipath propagation between the positions of the transmit and receive elements, as well as amplitude-phase inconsistencies in the transmit and receive chains. Furthermore, by assigning beamforming weights to the non-directional element-to-element coupling channels, the transmit-receive isolation between beams can be reliably predicted. This approach accurately reproduces the self-interference coupling between the transmit and receive beams and, compared to the spherical wave model, better captures the realistic characteristics of self-interference in both spatial and numerical distributions (Fig. 13, Fig. 14). Conclusions This study examines the near-field self-interference coupling characteristics of U6G full-duplex array systems through nearly 3.6 million measurements. The measurement and analysis results demonstrate that the isolation distribution between transmit and receive beams exhibits strong spatial symmetry and directionality. In contrast to the millimeter-wave frequency band, self-interference coupling in the U6G band shows weaker sensitivity to beam steering. Therefore, relying solely on beam steering to reduce self-interference is insufficient to achieve the required receiver sensitivity, necessitating the adoption of additional active or passive spatial self-interference suppression techniques. In some cases, a combination of RF and digital-domain self-interference suppression techniques may also be necessary.Furthermore, measurements of the self-interference coupling channels between transmit and receive array elements reveal that multiple isolation mappings exist for the same element spacing, which cannot be accurately described by traditional spherical wave models. In particular, by assigning beamforming weights to the non-directional element-to-element coupling channels, the self-interference coupling characteristics between beams can be replicated, and the array isolation can be accurately predicted. These measurement and analysis results provide essential insights for the design of U6G full-duplex communication systems and lay the foundation for future work on self-interference channel modeling, beamforming optimization, and self-interference suppression.
- Co-time co-frequency full duplex,
- Self-interference,
- Phased array,
- Channel measurement,
- U6G frequency band

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References(17)

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