REVIEW ARTICLE

Broadband linearization for 5G fronthaul transmission

  • Xiupu ZHANG
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  • iPhotonics Labs, Department of Electrical and Computer Engineering, Concordia University, Montreal, Quebec, H3G1M8, Canada

Received date: 12 Jan 2018

Accepted date: 15 Mar 2018

Published date: 04 Jul 2018

Copyright

2018 Higher Education Press and Springer-Verlag GmbH Germany, part of Springer Nature

Abstract

5G is emerging, but the current fronthaul transmission technologies used for 3G and 4G may not be efficient and appropriate for 5G. It has been found that frequency division multiple access (FDMA) and time-division multiple access (TDMA) based radio over fiber (RoF) may be considered the most appropriate for 5G fronthaul transmission technology. Due to analog RoF transmission, broadband linearization is required. In this work, both electrical and optical broadband linearization techniques are reviewed.

Cite this article

Xiupu ZHANG . Broadband linearization for 5G fronthaul transmission[J]. Frontiers of Optoelectronics, 2018 , 11(2) : 107 -115 . DOI: 10.1007/s12200-018-0802-4

Introduction

Broadband mobile services have been emerging very rapidly. To address the broadband, long-term evolution (LTE) and LTE Advanced (LTE-A) have been standardized and commercially deployed as 4th generation mobile technology, i.e., 4G. The 4G with LTE and LTE-A supports data rate of 300 Mb/s and 4 Gb/s, respectively [1]. It is known that the 5th generation mobile technology, i.e., 5G, is being developed to realize access speed of 10 Gb/s and above [1,2].
Optical fiber access networks have been used for supporting mobile fronthaul and mobile backhaul to realize cloud radio access networks (C-RAN). The fronthaul is the key element in the C-RAN architecture, as it connects centralized baseband units (BBUs) with remote radio units (RRUs). In the near future, the fronthaul is required to support massive multiple-input multiple-output (MIMO) for 5G [3]. Moreover, common public radio interface (CPRI) for fronthaul has been used, and Ethernet CPRI, i.e., eCPRI, could be used for 5G, which is digitized in-phase (I) and quadrature (Q) waveforms of wireless signals [1]. When binary on-off keying (OOK) optical fiber transmission is used for fronthaul, CPRI introduces inefficient utilization of optical bandwidth. For current 3G and 4G with LTE, cost-effect digital fiber optic transmission meets requirement of CPRI supported fronthaul as wireless data rate is not high; however, for LTE-A and 5G this may not be true. For an example, carrier aggregated five of 20 MHz LTE-A wireless signals with 8×8 MIMO and three directional sector antennas give 147.5 Gb/s CPRI data rate [4]. For the future 5G, carrier aggregation from 5 to 32 wireless signals may be required, and thus the CPRI and even eCPRI data rate becomes very high. To support this high data rate fronthaul, a large number of high speed optical fiber OOK transmission systems are required, making optical/wireless access networks very complicated and cost ineffective.
To achieve bandwidth-efficient mobile fronthaul transmission, several transmission techniques have been proposed and demonstrated, including frequency division multiple access (FDMA) based radio over fiber (RoF) transmission [4,5], time-division multiple access (TDMA) based RoF transmission [6], and the others [5], in which both FDMA and TDMA RoF, called digital signal processing (DSP) assisted RoF [7], are considered the most popular fronthaul transmission techniques [6]. Recently, real-time CPRI compatible TDMA RoF fronthaul transmission of 256 Gb/s was achieved using 10-GHz optics [8]. Therefore, RoF has very strong potential adoption for 5G fronthaul transmission.
Not like digital optical transmission, RoF is based on optical subcarrier modulation (SCM) and it is an analog transmission. Accompanying optical SCM, nonlinear distortion, such as harmonic and intermodulation distortion, is introduced, which induces crosstalk between wireless carriers. The nonlinearities that induce the nonlinear distortion stem from mainly optical transmitters and receivers. For example, a semiconductor laser, which is used for optical transmitters and has a nonlinear relation between driving the bias current and output optical power, will induce various harmonic and intermodulation distortion between aggregated wireless carriers, and also the distortion may overlap with the wireless signals, inducing crosstalk. Consequently, broadband linearization techniques are required for RoF transmission [9]. The linearization means that the nonlinear distortion is suppressed and thus spurious free dynamic range (SFDR) is improved, which is used to represent the distance between signal and nonlinear distortion radio frequency (RF) power.
In this paper, we review the recent progress of broadband linearization techniques for broadband RoF transmission that has potential to be used for emerging 5G fronthaul transmission.

Broadband linearization techniques

Figure 1 shows the linearization techniques recently developed, including optical and electrical linearization. The optical and electrical linearization mean the implementation in optical and electrical domain, respectively. Next, we briefly review some techniques given in Fig. 1.
Fig.1 Linearization techniques [9]

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Electrical linearization

The electrical linearization includes analog and digital predistortion and postdistortion. The pre-/post-distortion means that distortion circuits are located in before/after RoF transmission. As a rule of thumb, predistortion is much more efficient than postdistortion, and therefore the predistortion techniques are only reviewed here. In the following, we review the recent accomplishments in analog predistortion and digital predistortion.

Analog predistortion

An RoF transmission system can be considered a black box, thus a function between input and output RF can be obtained, and the function is usually nonlinear and it can be expanded into a Taylor series. The Taylor series will include 1st, 2nd, 3rd, 4th and 5th order, and further higher orders are usually negligible. The 1st order contains transmitted wireless signals, and the others are called nonlinearities that can induce nonlinear distortion, such as harmonic distortion (HD) and intermodulation distortion (IMD). When the wireless signal bands are not very broad, nonlinear distortion generated by 2nd and 4th order nonlinearities is usually out of the signal bands, thus no degradation is induced by these nonlinearities. This suggests that only 3rd and 5th order nonlinearity induce nonlinear distortion. However, when the wireless signal bands are broad, 2nd and 4th order nonlinearities may generate nonlinear distortion components that are located inside the signal bands in addition to 3rd and 5th order nonlinearity. For example, the wireless signal is ranged from −1.5 to 1.5 GHz in relative frequency [4], some HD and IMD components generated by 2nd order nonlinearity are inside of the signal bands. However, analog predistortion circuits have been designed only for suppressing nonlinear distortion generated by 3rd and 5th order nonlinearity [1013].
To illustrate the operation principle of analog predistortion, we consider a case of wireless signals having two frequency bands with carriers f1 and f2, as shown in Fig. 2. For simplicity, we only consider 3rd order nonlinearity of RoF transmission. Due to the 3rd nonlinearity of RoF transmission, two IMD components at 2f1−f2 and 2f2−f1 are generated at the output when the wireless signals at f1 and f2 are transmitted over the RoF, the two red/solid arrows as shown in Fig. 2. Note these two IMD components have the opposite phase to the wireless signals. When an analog predistortion circuit is inserted before the RoF, opposite 3rd and/or 5th order nonlinearity are introduced to the RoF. In other words, when the two wireless signals at f1 and f2 are transmitted to the analog predistortion circuit and then RoF, two IMD components at 2f1−f2 and 2f2−f1, indicated by the green/dashed arrows in Fig. 2, are also generated, but they have the opposite phase to the two IMD components generated by the RoF itself. Thus, the IMD components at 2f1−f2 and 2f2−f1, generated by the RoF and analog predistortion circuit, are cancelled out by each other through tuning the bias current of the analog predistortion circuit (APDC). As a rule of thumb, all other components that are generated by 3rd order nonlinearity can be suppressed by the same principle.
Fig.2 Working principle of APDC [12]

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Fig.3 Mathematic model for APDC to be used for suppression of 3rd order nonlinearity [9]

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As shown in Fig. 3, when 3rd order nonlinearity is only considered, the relation between the input and output of APDC is given by Vin=a 1 VRF+a3 VRF3, where the coefficients ak, k = 1 and 3, are related to the circuit and bias voltage. Similarly, the relation between the input and output of RoF transmission is given by Vout=b 1 Vin+ b2V in2+b3Vin3, where the coefficients bk, k = 1, 2 and 3, are determined by the RoF transmission, where further higher orders are not considered. Thus, the output of the RoF is given by
Vout=a 1 b1V RF+a12b 2 VRF2+(a3 b1 +a13 b3 )V RF3.
To remove the 3rd term means a3 b1 +a13 b3 =0. If the coefficients of analog predistortion circuit can meet the above condition, the 3rd order nonlinearity of RoF transmission can be removed completely.
It is found that Schottky diodes have opposite nonlinear characteristics to RoF transmission. We have designed a simple analog predistortion circuit that has bandwidth from 3.1 to 4.8 GHz and resulted in SFDR improvement of 11 dB [10]. Later, the circuit was further improved in design. The first improved design is shown in Fig. 4 [11]. Two zero bias GaAs beam lead detector diodes and capacitors were used in the APDC. The diodes can be biased at lower than 3 mA due to zero bias characteristic so that power consumption is very small. No broadband matching network is required because of high series resistance of the zero bias diodes. The anti-parallel structure of the circuit eliminates even order nonlinearity generated by the two diodes. As shown in Fig. 5 that is measured S21 versus input RF power to the APDC, it is seen that the S21 is increased with the increase of input RF power. It is well known that RoF S21 is decreased with the increase of input RF power, a common behavior as almost all RF functional components such as RF amplifiers. This suggests that the APDC has almost opposite response to RoF transmission in S21. Further, the 3rd order nonlinearity, which can induce RoF S21 decrease, will be suppressed by the APDC. The circuit has 3-dB bandwidth from 7 to 18 GHz. Using this APDC in an RoF transmission, measured SFDR was improved by more than ~10 dB from 7 to 14 GHz and ~6 dB from 15 to 18 GHz, limited by 5th order nonlinear distortion [11].
Fig.4 (a) Schematic of APDC, WPD: Wilkinson power divider; and (b) fabricated APDC [11]

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Fig.5 Measured amplitude modulation/amplitude modulation characteristic of APDC [11]

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The APDC was further improved as shown in Fig. 6 [12], where the dual diode is a three-port chip and the two diodes are connected in anti-parallel. The two diodes are in an anti-parallel structure, so even order nonlinear distortion terms are suppressed at the output of the APDC. The APDC has a 3-dB bandwidth from 10 MHz to 33 GHz. Using this circuit in an RoF transmission system, 3rd order IMD (IMD3) power versus frequency spacing was measured using two RF signals for two cases, as shown in Fig. 7 [12]. By comparison of the two cases, it is seen that the IMD3 is suppressed by more than 10 dB, and the frequency location of the IMD3 does not affect the suppression seriously. It was found that this APDC resulted in a SFDR improvement of ~12 dB for linearizing a directly modulated RoF transmission. To linearize an externally modulated RoF transmission, SFDR was improved by 5−12 dB. For a 20-MHz orthogonal frequency division multiplexing (OFDM) WiFi wireless signal at 2.4 GHz, error vector magnitude (EVM) was improved by 3.5 dB for an RoF over 20 km standard single mode fiber (SMF).
Fig.6 (a) Schematic of APDC; and (b) photo of APDC [12]

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Fig.7 Measured RF power of IMD3 versus frequency spacing between two RF signals [12]

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The above two analog predistortion circuits only enable to suppress 3rd order nonlinearity, and thus the SFDR of RoF transmission is usually limited by 5th order nonlinearity. Intuitively, further improvement of SFDR requires to suppress 5th order nonlinearity. For this case, similar to Fig. 3 the predistortion circuit output is given by
Vin=a 1 VRF+a3 VRF3+a5 VRF5.
When a RoF system up to fifth order nonlinearity is considered, i.e.,
Vout=b 1 Vin+b2Vin2+b 3Vin3+b 4Vin4+b 5Vin5,
the output of RoF transmission is given by
Vout=a1 b1V RF+a12b 2 VRF2+(a3 b1+a1 3 b3) VRF3
+ (a14b 4+2a1a3b2)VRF 4
+ (a5b1+3 a12a3b3+a 15b5)VRF 5.
Thus, to suppress both 3rd and 5th order nonlinearity, these conditions must be satisfied, a3b1+ a13b3=0, and a5b1+3a 12a3b3+ a15b5=0. Since the coefficients b1, b2, b3, b4, and b5 are fixed for a given RoF transmission, the analog predistortion circuit coefficients a1, a3 and a5 can be tuned to meet the above two conditions. Figure 8 shows our designed analog predistortion circuit for suppression of both 3rd and 5th order nonlinearity [13]. The circuit has a 3-dB bandwidth of 6 GHz. For the above WiFi wireless signal, measured EVM improvement is shown in Fig. 9 for an RoF transmission without fiber and with 10 km SMF transmission.
Fig.8 (a) Schematic of analog predistortion circuit; and (b) photo of designed circuit [13]

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Fig.9 Measured EVM improvement for WiFi signal with wireless carrier from 2 to 5 GHz over RoF [13]

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Digital predistortion

Digital predistortion (DPD) for RF power amplifiers has been investigated for decades [14]. Basically, the DPD has been realized in baseband, and also the DPD models become extremely complicated when the wireless bands are more than three or broadband. We have proposed and demonstrated a simple DPD model that is envelope assisted RF DPD [15]. When the carrier aggregation is enabled, the signal bandwidth can reach 100 MHz or more, which means that the baseband sampling rate of the analog to digital converter (ADC) can be 500 MHz or more. When the memory polynomial works at such a high sampling rate, the memory depth of the DPD might be too long, and thus the number of the polynomial coefficients becomes much higher, in particular when there is a strong long-term memory effect in RoF systems [14]. To tackle this problem, an envelope-assisted RF memory polynomial was proposed, which can be described by
z (n)= Σ j=1 JΣp=0Paj px( np) |x(np)|j1+Σk=1KΣq=1 Qbkqx(n) |w(nq)|k1,
where x(n) is the value of wireless signals in RF domain, w(n) is the value of the baseband wireless signal envelopes, J and P are the nonlinear order and memory depth for the wireless signals in RF domain, respectively, K and Q are the nonlinear order and memory depth for the wireless signals in baseband domain, respectively, and ajp and bkq are the model coefficients for the RF and baseband wireless signals, respectively. The first part of the above equation is aimed to eliminate the out-of-band nonlinearities, in-band nonlinearities and short-term memory effect, which are owing to the RF wireless signals, while the second part is aimed to eliminate the in-band nonlinearities and long-term memory effect, which are owing to the baseband wireless signals. The more details of the model can be found in Ref. [15], and the model was verified by two-band and three bands of wireless signals over RoF transmission [15].
When two bands at 800 and 840 MHz, and each band with 20 MHz LTE signal are considered, the RF spectrum after an RoF transmission with 8-km SMF, in which the envelope assisted RF DPD was used, is shown in Fig. 10. For comparison, the conventional two-dimensional DPD (2D-DPD) [16] was also used in the same RoF transmission. It is seen that both in-band and out-of-band performance are better for using the envelope assisted RF DPD than that for using the conventional 2D-DPD. Measured EVM shows more improvement of 1.9 dB using the envelope assisted RF DPD than the 2D-DPD.
Fig.10 Measured RF spectrum for two wireless bands at 800 and 840 MHz over RoF [15]

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When the model is used for more than two-bands, such as three bands of wireless signals, baseband DPD models as given in Ref. [14] become very complicated and are difficult to be used. However, the envelope assisted RF DPD model is still very simple. Figure 11 shows measured RF spectrum for three wireless bands at 800, 850 and 900 MHz with LTE signal over RoF transmission [15]. It is seen that the envelope assisted RF DPD is very effective in improvement of in-band and out-of-band performance.
Fig.11 Measured RF spectrum for three bands of wireless signals at 800, 850 and 900 MHz over RoF transmission [15]

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To decrease the sampling bandwidth, the RF wireless signals are down-converted to intermediate frequency (IF) signals, which contain all the bands in frequency domain. Then, the down-converted IF signals can be sampled with a much lower sampling rate. Figure 12 shows the measured output spectrum for envelope assisted IF DPD implemented with a sampling bandwidth of 600 MHz, from 550 to 1150 MHz. For comparison, the performance of the RoF linearized by envelope assisted RF DPD is also shown in Fig. 12. It is seen that the envelope assisted IF DPD results in a better performance.
Fig.12 Measured RF spectrum for two wireless signals at 800 and 900 MHz over RoF [15]

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Moreover, the complexity of the envelope assisted DPD model in terms of model coefficients is compared to the conventional 2D-DPD and given in Table 1. It is seen that the envelope assisted DPD has about a half of the coefficients compared with the conventional 2D-DPD.
Tab.1 Number of coefficients vs memory depth
memory depth* 1 2 3 4 5 6 7 8
envelope DPD** 14 23 32 41 50 59 68 77
2D DPD [16] 30 45 60 75 90 105 120 135

* Suppose nonlinearity order is 5.

** Suppose lengths of RF memory effect and baseband memory effect are equal.

The APDC has features: simple and compact structure, low power consumption and much more broadband, in comparison with the DPD that has features: high complex structure, high power consumption and much narrower band. Moreover, the DPD is highly efficient in in-band distortion suppression, and is difficult in out-of-band distortion suppression. In contrast, the APDC is broadband and thus is able to suppress both in-band and out-of-band distortion. In addition, the memory effect that induces signal distortion can be suppressed only by the DPD, which is very important for broadband signals. In brief, the APDC and DPD are complementary in nonlinear distortion suppression. We have also studied analog and digital predistortion combined linearization for RoF transmission, to utilize the complementary advantages of APDC and DPD, i.e., hybrid APDC and DPD [17]. For two bands of 20 MHz LTE signals transmission over RoF for the cases of without linearization, 2D-DPD [16], APDC, and combined of APDC and 2D-DPD, i.e., hybrid, Fig. 13 shows the output RF spectrum. It is seen that the combined linearization suppresses both in-band and out-of-band distortion, better than either APDC or 2D-DPD.
Fig.13 Measured RF spectrum at the output of RoF transmission that is linearized by either non linearization, 2D-DPD [16], APDC, and hybrid APDC and 2D-DPD. Two RF signals are located at 800 and 840 MHz [17]

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Table 2 summarizes comparison of three linearization techniques for three scenarios experimentally in improvement of EVM, adjacent channel power ratio (ACPR) and IMD3 [17]. Scenario 2 is the same as for Fig. 13. For Scenario 1, two wireless RF signals are located in 800 and 900 MHz. For Scenario 2, two wireless RF signals are located in 800 and 840 MHz. For Scenario 3, three wireless RF signals are located in 800, 850 and 900 MHz. Each band of wireless RF signals is 64 quadrature amplitude modulation (QAM)-OFDM 20 MHz LTE.
Tab.2 Comparison of improvements by three linearization techniques
Scenario linearization method improvement
EVM ACPR IMD3
800 and 900 MHz APDC only 2.0 dB 1.8 dB 14.9 dB
2D-DPD only 9.9 dB 17.5 dB 0.3 dB
hybrid 11.0 dB 19.4 dB 15.0 dB
800 and 840 MHz APDC only 2.2 dB 4.7 dB 17.0 dB
2D-DPD only 7.0 dB -0.3dB -1.1 dB
hybrid 8.2 dB 4.6 dB 16.8 dB
800, 850 and 900 MHz APDC only 2.4 dB 3.3 dB 3.7 dB
RF DPD only 9.3 dB 8.2 dB 16.5 dB
hybrid 10.1 dB 8.6 dB 16.9 dB

Optical linearization

As a rule of thumb, optical linearization is mainly used to linearize optical components, such as lasers, and optical modulators etc. As shown in Fig. 1, various optical linearization techniques have been investigated. However, mixed polarization and dual-wavelength linearization are considered to have a simple configuration. The principle of the optical linearization is almost similar, namely the nonlinear distortion generated by an optical component at two operation points can cancel each other. Therefore, optical linearization can be used to suppress both second- and third-order nonlinearity as well as further higher order [9].

Mixed polarization linearization

The mixed-polarization linearization means that the nonlinear distortion generated by TE and TM transmission of an optical component is cancelled by each other, when the TE and TM components are mixed to a certain degree and the nonlinear distortion from the TE and TM transmission is out of phase. Therefore, the TE and TM transmission characteristics must be different, which means that the optical component must be polarization dependent, such as polarization dependent Mach-Zehnder modulator (MZM) [1820] or electro-absorption modulator (EAM) [21,22]. To illustrate the principle, we consider to linearize an MZM that is usually biased at quadrature and has nonlinear transmission, as shown in Fig. 14. The linearized MZM consists of a front and rear polarization linearizer located at its input and output, respectively. The two polarization angles a and b are dependent on TE and TM transmission characteristics of the MZM. The rear polarization linearizer can be replaced by a saturated semiconductor optical amplifier (SOA) [23]. The nonlinear distortion can be significantly suppressed by appropriately adjusting two polarization angles, and the suppression is strongly dependent on the TE and TM transmission characteristics of the MZM or EAM. For example, when GaAs MZM is used, the TE and TM transmission characteristics, which have opposite phase modulation indices, result in much better suppression [24,25]. When an LiNbO3 MZM is linearized by the mixed polarization, Fig. 15 shows the transmission characteristics, in which three cases are given: conventional MZM, MZM linearized by the mixed polarization only, and MZM linearized by the mixed polarization and also saturated SOA. It is seen that the MZM transmission is not sinusoidal anymore and becomes linear with driving voltage. Typically speaking, SFDR improvement by mixed-polarization is more than 10 dB [1820]. Because of linearization implemented in optical domain, the linearization bandwidth is only limited by optical modulator modulation bandwidth.
Applying for the above mixed polarization linearization, integrated linear optical modulators can be obtained.
Fig.14 Schematic of mixed polarization that is used to linearize an MZM. LP: linear polarizer [18]

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Fig.15 Measured transmission characteristics for three cases: conventional MZM without linearization (TE only), MZM linearized by mixed-polarization (MP), and MZM linearized by MP combined with a saturated SOA (MP+SOA) [23]

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Dual-wavelength linearization

The principle of dual-wavelength linearization (DWL) means that the nonlinear distortion generated at two wavelengths λA and λB can cancel each other [26]. This suggests that an optical component, such as an EAM, must have wavelength dependent transmission characteristics. The nonlinear distortion generated at λA and λB can be suppressed if they are anti-phase each other. Figure 16 shows a schematic of dual-wavelength RoF transmission, where EAM has nonlinear transmission characteristic and also wavelength dependent. It was found that the suppression of nth order nonlinear distortion must satisfy
PA×mnA PB×mnB=cos[nωR F(DLΔ λ+Δ t)],
where PA and PB are optical power of λA and λB, respectively, mnA and mnB are the nth order coefficient of Taylor series expansion of the EAM transmission characteristics at λA and λB, respectively, DL is product of fiber chromatic dispersion and fiber length, Δλ = λBλA, and Δt is the delay induced by chirp of the EAM [26]. It is seen that the suppression of any order nonlinear distortion is dependent on the power ratio of the two wavelengths and the phase of D LΔλ +Δt. The linearization was verified using WiFi signals at 2.4 and 5 GHz, 3.5 dB at 2.4 GHz and 2.8 dB at 5 GHz improvements obtained with λA = 1510 nm and λB = 1552.6 nm [26].
Fig.16 Schematic of dual-wavelength RoF transmission system. oRx: optical receiver [26]

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Conclusion

We have reviewed our very recent accomplishments of broadband linearization for broadband RoF transmission, including analog predistortion circuit, digital predistortion, mixed polarization and dual-wavelength linearization techniques. Optical linearization is broadband and much desired for linearizing optical components, and also optical linearization can be integrated with the optical components. Analog predistortion circuit can be broadband, but it is less efficient. Digital predistortion is difficult for broadband, but it is efficient for 20 MHz band or less wireless signals. Consequently, electrical and optical linearization can be combined to be used for enhancing linearization in the future.
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