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Journal ArticleDOI

Advanced topics on RF amplitude and phase detection for low-level RF systems

01 Oct 2019-Nuclear Science and Techniques (Springer Singapore)-Vol. 30, Iss: 10, pp 1-12
TL;DR: In this paper, different sampling strategies and demodulation algorithms have been developed for low-level radio frequency (LLRF) systems, including accurate RF transient measurement, wideband RF detection, and detection with an asynchronous trigger, local oscillator, or clock.
About: This article is published in Nuclear Science and Techniques.The article was published on 2019-10-01 and is currently open access. It has received 8 citations till now. The article focuses on the topics: Radio frequency & Local oscillator.

Summary (2 min read)

1 Introduction

  • The asynchronous sampling scheme does not require deterministic phase relations between the trigger, LO, clock and RF signals but places difficulties in the design of demodulation algorithms.
  • There are already quite a few articles to discuss the RF signal detection focusing on the accuracy, precision and latency requirements described above [24] [25] [26] [27] [28] .
  • For these special requirements, different demodulation algorithms are needed based on the common RF detector architecture in Fig. 1 .The following topics will be discussed: 1) RF transient detection with non-IQ: some RF signals may have transients with fast changing amplitude or phase which need to be measured accurately by the RF detector.

2.1 RF Transient Detection with non-IQ

  • If the kth sample of the IF signal is denoted as xk, the in-phase (I) and quadrature (Q) components of the RF envelop vector can be calculated with the last n samples as EQUATION where the phase step.
  • The non-IQ demodulation algorithm (2) can filter out the harmonics and DC offset in the IF samples [21] , [22] with a reasonable latency if n is not too large.
  • When the IF amplitude or phase change fast like in the transients of an RF pulse, the second term will not vanish and appear as a systematic error with its spectrum centered at twice the IF frequency.
  • Due to the fact that the clock frequency is synchronized with the IF frequency, a moving-average Finite Impulse Response (FIR) filter can also provide an accurate notch at double of the IF frequency.
  • The moving-average FIR filter with 3 taps has been applied to SwissFEL LLRF system and resulted RF pulse baseband signal and spectrum have been shown as dotted-line plots in Fig. 2 and Fig. 3(a) .

2.2 Wideband RF Detection

  • The non-IQ demodulation algorithm requires n samples of the IF signal to do the demodulation which reduces the bandwidth of the sampling.
  • Let's assume that the ADC data is collected after a trigger and the first sample corresponds to a phase φ0 of the IF signal, see Fig. 4 below.
  • This situation can happen if the phases of the IF and clock signals are aligned at some time point, when the clock samples a point close to the zero-crossing of the IF signal.
  • The frequency responses of the non-IQ demodulation algorithm with n = 6 and the wideband detection algorithm (9) are compared in Fig. 6(b ).
  • It can be seen that the wideband detection algorithm has larger bandwidth without notches at the IF frequency and double of the IF frequency.

2.3 RF Detection Regardless of Trigger

  • The phase of the first sample after the trigger is defined as the reference phase of the demodulation and the phase variations of the later samples are detected by removing the expected phase lags compared to the reference phase.
  • If the rising edges of the trigger and clock signals are very closely aligned in time, the trigger may fall randomly into two adjacent clock cycles and select different ADC samples.
  • Fig. 8 . Reference IF signal derived quadrature signal with synchronous sampling at SwissFEL.
  • Because the RF detection strategy in Fig. 7 always compares the RF phase and the MO phase regardless to the trigger, the phase jumps caused by the racing between trigger and clock can be avoided.
  • The low-frequency noises, which are the drifts in the amplitudes and phases of the reference and RF signals, are mostly correlated while the high-frequency noises are mostly uncorrelated.

2.4 RF Detection with Asynchronous LO or Clock

  • Instead, it might be easier to get separate oscillators to provide the LO and clock signals, which are not synchronized with the RF signal to be detected.
  • The major differences are the implementations of the 0º/90º splitter and the LPF due to asynchronous sampling.
  • With asynchronous sampling, the IF phase lag   between two adjacent ADC samples is unknown so the authors cannot use the simple algorithm in (12) to calculate the quadrature signal of the reference signal.
  • Practically the authors can use an FIR filter to approximately implement the Hilbert transform.
  • Fig. 13 shows the frequency response of a 16-tap Hilbert transform FIR filter designed with the "Filter Designer" of Matlab.

4 Conclusions and Outlook

  • The digital RF amplitude and phase detector is one of the key components in LLRF systems.
  • Based on the same hardware, different digital demodulation algorithms should be implemented to address different requirements on the RF detection.
  • This paper describes several RF detection algorithms to satisfy different requirements that the author has met when working on different LLRF systems, which can be used in other machines with similar conditions.
  • New algorithms will be developed for newly emerging requirements on the performance, reliability and robustness of RF detectors.
  • If the requirements (e.g. bandwidth requirements) exceed the limits of the existing hardware, a modification of the RF detector hardware could be also needed together with the demodulation development.

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Citations
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Journal ArticleDOI
Qi Chen1, Zheng Gao1, Z. A. Zhu1, Zongheng Xue1, Yuan He1, Xian-Wu Wang1 
TL;DR: In this article, a general-purpose design front-end prototype has been developed to evaluate the multi-frequency point supported design feasibility, with a carefully selected low-noise wide-band RF mixer and amplifier to balance the performance of multichannel supported downconversion, specially designed local oscillator (LO) distribution net to increase isolation between adjacent channels, and external band-pass filter to realize expected up-conversion frequencies.
Abstract: The China initiative Accelerator Driven System, CiADS, physics design adopts $162.5 \,\mathrm{MHz}$, $325 \,\mathrm{MHz}$, and $650 \,\mathrm{MHz}$ cavities, which are driven by the corresponding radio frequency (RF) power system, requiring frequency translation front-end for the RF station. For that application, a general-purpose design front-end prototype has been developed to evaluate the multi-frequency point supported design feasibility. The difficult parts to achieve the requirements of the general-purpose design are reasonable device selection and balanced design. With a carefully selected low-noise wide-band RF mixer and amplifier to balance the performance of multi-frequency supported down-conversion, specially designed local oscillator (LO) distribution net to increase isolation between adjacent channels, and external band-pass filter to realize expected up-conversion frequencies, high maintenance and modular front-end general-purpose design has been implemented. Results of standard parameters show an $R^2$ value of at least $99.991\%$ in the range of $-60 \sim 10\,\mathrm{dBm}$ for linearity, up to $18\,\mathrm{dBm}$ for P1dB, and up to $89\,\mathrm{dBc}$ for crosstalk between adjacent channels. The phase noise spectrum is lower than $80\,\mathrm{dBc}$ in the range of $0 \sim 1\,\mathrm{MHz}$, and cumulative phase noise is $0.006^\circ$; amplitude and phase stability are $0.022\%$ and $0.034^\circ$, respectively.

10 citations

Journal ArticleDOI
TL;DR: The development of iterative learning control combined with disturbance-observer-based (DOB) control for the digital low-level radio frequency (LLRF) system of the International Linear Collider project is presented and the performance of the LLRF system was improved, as expected by this combined control approach.

10 citations

Journal ArticleDOI
Qi Chen1, Zheng Gao1, Z. A. Zhu1, Zongheng Xue1, Yuan He1, Xian-Wu Wang1 
TL;DR: A carefully selected low-noise wide-band RF mixer and amplifier to balance the performance of multi-frequency supported down-conversion, specially designed LO distribution net to increase isolation between adjacent channels, and external band-pass filter to realize expected up-converting frequencies, high maintenance and modular front-end general-purpose design has been implemented.

5 citations


Additional excerpts

  • ...LINAC, 568–570 (2006), [23] Z....

    [...]

01 Jan 2009
TL;DR: The new generation particle accelerator requires a highly stable radio frequency(RF) system and the Low Level RF(LLRF) subsystem which controls the amplitude and phase of the RF signal.
Abstract: The new generation particle accelerator requires a highly stable radio frequency(RF) system. The stability of the RF system is realized by the Low Level RF(LLRF) subsystem which controls the amplitude and phase of the RF signal. The detection of the RF signal's amplitude and phase is fundamental to ...

4 citations

Journal ArticleDOI
TL;DR: In this article, the robustness of the timing and synchronization systems, such as the time uncertainty of the RF pulse related with the trigger, the phase uncertainty of frequency dividers after power cycles and the race condition between the trigger and clock are discussed.
Abstract: Free electron lasers (FEL) require strict time relations for the electron bunch and RF field interaction, which must be precise and deterministic in time. This is guaranteed by the timing and synchronization systems that should be robust under the situations like a power cycle in the master oscillator, timing master, reference frequency distribution devices or low-level radio frequency (LLRF) devices. After the power cycles, the time relations should be kept or be capable to recover quickly to improve the availability of the FEL machine. This article focuses on the robustness of the timing and synchronization systems, such as the time uncertainty of the RF pulse related with the trigger, the phase uncertainty of frequency dividers after power cycles and the race condition between the trigger and clock. The possible solutions to achieve a robust design of the timing and synchronization systems are also discussed.

2 citations

References
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Abstract: From the Publisher: This is a book on practical feedback control and not on system theory in general. Feedback is used in control systems to change the dynamics of the system and to reduce the sensitivity of the system to both signal and model uncertainty. The book presents a rigorous, yet easily readable, introduction to the analysis and design of robust multivariable control systems. It provides the reader with insights into the opportunities and limitations of feedback control. Its objective is to enable the engineer to design real control systems. Important topics are: extensions and classical frequency-domain methods to multivariable systems, analysis of directions using the singular value decomposition, performance limitations and input-output controllability analysis, model uncertainty and robustness including the structured singular value, control structure design, and methods for controller synthesis and model reduction. Numerous worked examples, exercises and case studies, which make frequent use of MATLAB, are included. MATLAB files for examples and figures, solutions to selected exercises, extra problems and linear state-space models for the case studies are available on the Internet.

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"Advanced topics on RF amplitude and..." refers background in this paper

  • ...The latency of the RF detector is critical when using in an RF feedback loop for which the overall loop delay will limit the closed-loop bandwidth that the feedback loop can achieve [15],[16]....

    [...]

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TL;DR: This book presents a control engineering methodology that, while based on mathematical fundamentals, stresses physical system modeling and practical control system designs with realistic system specifications.
Abstract: From the Publisher: For more than twenty years, Modern Control Systems has set the standard of excellence for undergraduate control systems textbooks. It has remained a bestseller because Richard Dorf and Robert Bishop have been able to take complex control theory and make it exciting and accessible to students. The book presents a control engineering methodology that, while based on mathematical fundamentals, stresses physical system modeling and practical control system designs with realistic system specifications.

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"Advanced topics on RF amplitude and..." refers background in this paper

  • ...The latency of the RF detector is critical when using in an RF feedback loop for which the overall loop delay will limit the closed-loop bandwidth that the feedback loop can achieve [15],[16]....

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TL;DR: This paper presents a meta-analysis of non-Parametric Spectral methods for Singular Spectrum Analysis (SSA) of Deterministic Discrete-Time Signals and discusses their applications in filters and noise reduction.
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"Advanced topics on RF amplitude and..." refers background in this paper

  • ...The low-pass filter design is out of the scope of this paper and can be referred to the digital signal processing books [38]....

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01 May 2012
TL;DR: The complete LLRF system design is now in its final phase and the designed hardware was installed and commissioned at FLASH and the MTCA.4 LLRF architecture and system results will be shown.
Abstract: The European X-Ray free electron laser accelerator con- sists of 808 superconducting cavities grouped in 25 RF sta- tions. The challenges associated with the size and com- plexity of this accelerator require a high-precision, mod- ular and scalable low level RF (LLRF) system. The Mi- cro TCA technology (MTCA.4) was chosen to support this system and adapted for RF standards. State-of-the-art hard- ware development in close collaboration with the industry allowed for the system continuity and maintainability. The complete LLRF system design is now in its final phase and the designed hardware was installed and commissioned at FLASH. The MTCA.4 LLRF architecture and system per- formance results will be shown. Operation strategies and future automation algorithms for performance optimization will also be presented in this paper.

56 citations

Frequently Asked Questions (19)
Q1. What have the authors contributed in "Advanced topics on rf amplitude and phase detection for low-level rf systems" ?

Low-Level RF ( LLRF ) systems stabilize the electromagnetic field in the RF cavities for beam acceleration in particle accelerators. Different sampling strategies and demodulation algorithms have been developed and will be introduced in this paper. This article will focus on some advanced topics for RF detection like the accurate RF transient measurement, wideband RF detection and the RF detection with asynchronous trigger, Local Oscillator ( LO ) or clock. The analysis will be based on the measurement from SwissFEL but the introduced algorithms are general for the RF signal detection in particle accelerators. 

In order to generate the quadrature signal from the time series of the reference IF signal, the last two ADC samples denoted as xref,k-1 and xref,k can be used. 

The latency of the RF detector is critical when using in an RF feedback loop for which the overall loop delay will limit the closed-loop bandwidth that the feedback loop can achieve [15],[16]. 

The LPFs in the The authorand Q output paths are used to remove the leakage of the IF frequency and the higher-order (especially the second-order) harmonics of the IF frequency. 

The wideband detection algorithm can detect faster transients in the RF pulse with a cost of keepingall unwanted frequency components introduced in the down-conversion mixing and ADC sampling processes, such as the DC offset in ADC samples, leakage of IF frequency in demodulation and all higher-order harmonics of the IF frequency due to the non-linearity in the RF detector. 

4. The phase of the first sample after the trigger is defined as the reference phase of the demodulation and the phase variations of the later samples are detected by removing the expected phase lags compared to the reference phase. 

Due to the asynchronous sampling, the phase lag ̂ between two samplesis unknown, but it can be estimated with the phase slope of the complex signal in equation (18)calculated with linear fitting of the phases of each sample. 

A precise RF detector will be able to detect small changes in the RF field or in other words, with high resolution in RF measurements. 

With asynchronous sampling, the IF phase lag ̂ between two adjacent ADC samples isunknown so the authors cannot use the simple algorithm in (12) to calculate the quadrature signal of the reference signal. 

2.1 RF Transient Detection with non-IQThe non-IQ algorithm is a popular demodulation algorithm for RF detection based on synchronoussampling of IF signal. 

In LLRF systems, the RF detector is one of the key devices to diagnose and control the RF fields in cavities used for beam acceleration. 

Due to the asynchronous sampling, the moving-average FIR filter is no longer suitable toimplement the LPFs at the firmware or software side in Fig. 11. 

Counting from the first sample after the trigger, the kth and (k+1)th sample of an ideal IF signal (single-tone without amplitude or phase noises) can be written as 0 01 0 0sin 1sinkkx A kx A k . 

4) RF detection with asynchronous LO or clock: in some applications, the phase locked LO andclock generator are not available, and this demodulation algorithm should allow using asynchronous LO or clock sources to perform RF amplitude and phase measurement. 

The The authorand Q components of the IF samples in Fig. 4 are represented by the amplitude A0 and initialphase φ0 of the IF signal:0 0 0 0cos , sinI A Q A . (7)In order to get the The authorand Q components, at least two samples are needed, resulting in the possible maximum RF detection bandwidth. 

To overcome this problem, someLLRF systems use asynchronous trigger, LO and clock signals generated by separate oscillators, resulting in the asynchronous sampling scheme. 

(12) Similar as the discussion for equation (9), the phase-lag Δφ between two ADC samples shouldn’t be close to integer times of π. 

2.3 RF Detection Regardless of TriggerFor RF systems working in pulsed mode, the measurement of an RF pulse is usually started with atrigger as shown in Fig. 

With an accurate measurement of the RF amplitude and phase, the authors will be able to capture the exact changes in the RF field really felt by the beam.