BEPCII Transverse Feedback System Yue Junhui IHEP , Beijing Sep 17 th, 08IMAC.

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Presentation transcript:

BEPCII Transverse Feedback System Yue Junhui IHEP , Beijing Sep 17 th, 08IMAC

Including three parts: The main parameters of BEPCII The coupled bunch instability The bunch by bunch feedback system Outline

I : Some Parameters of BEPCII Beam Energy, E GeV 1.89 Circumference, C m Total beam current, A 0.91 Bunch current, mA 9.8 Revolution frequency, MHz RF frequency, MHz Harmonic Number, h 396 Tunes, 6.57/7.61/0.034 Radiation damping times, ms 25/25/12.5 Number of Bunches, B 93 Bunch spacing, m 2.4 Bunch frequency, MHz 125

The high beam current (0.9 A) and the large number of bunches (93 bunches) will cause the coupled bunch instabilities (CBI) in BEPCII Two source  The higher order modes (HOMs) of RF cavities  The resistive wall impedance Active feedback systems are required to suppress CBI II :The Coupled Bunch Instability

BEPCII will operate on colliding mode and synchrotron mode. So our transverse feedback will have three sets: electron ring, positron ring, and synchrotron ring. The electronics bandwidth should be at least half of the bunch frequency colliding mode 62.5MHz Synchrotron radiation mode 250MHz The design damping time of transverse feedback system is 0.5ms III: Bunch by bunch Transverse Feedback System

Transverse feedback system located in the storage ring

The Transverse Feedback System Schematic diagram Front-end electronics Signal processing system Kicker and power amplifier Parameters of Transverse Feedback System The experiments of BEPCII TFB

The Schematic Diagram of TFB System

The local station of the Transverse Feedback System

Transfer the signal whose bandwidth is 500MHz at the center frequency of 1.5GHz to base band. Detection frequency is 1.5GHz , triple of RF The local DC rejection circuit in fixed-voltage mode Front-end electronics

Signal processing system Full analog system simply using the cable line Three functions  Making the 90 phase shift  Rejection the closed orbit signal  One turn delay Realization  Two manual attenuators for 90 phase shift control  Notch filter rejection the revolution frequency  The time delay by cable

Signal processing system – Phase shift and Notch Filter

Kicker and Power Amplifier Four strip line electrode as kicker (considering it is easy to realize, so the kicker length is 600mm just for every other bunches) One kicker per ring because the limited space Model 75A250A power amplifier is selected. Two 75A250A are connected in the differential style

Kicker and Power Amplifier

Specifications of the TFB system RF frequency MHz Bunch spacing ns 8 Feedback damping time ms 0.5 Detection frequency GHz 1.5 Number of kickers per plane per ring 1 Kicker shunt impedance (at 125MHz) k  4.0 Total damping voltage per turn V 800 Kicker power for 800 V w 106 Number of power amplifiers per plane per ring 2 Bandwidth of power amplifier MHz 250

Beam profiles with TFB turning off and on 两个方向都未加反馈 两个方向都加 只加 y 方向 只加 x 方向 TFB off TFB on

Sidebands suppressed by TFB system Transverse instabilities in full bandwidth of 125MHz suppressed by TFB system with beam current 243mA with 99 bunches in positron ring. The background frequency lines are revolution frequency harmonics and the dark-coloured lines are instability sidebands. We can see that the magnitude of instability sidebands is attenuated more than 30dB when the feedback is on. TFB off TFB on

Measurement of damping time of TFB FB OFF FB ON

Single bunch 3mA ; Damping time is 2.43ms with TFB off; Damping time is 0.4ms with TFB on So tao_FB = 2.43*0.4/( )=0.4788ms. Measurement of damping time of TFB (cont’)

Summary The transverse feedback systems of BEPCII have been installed and played an important role during the commissioning of BEPCII double rings. It can suppress the strong multi-bunch instabilities at the higher beam current of over 500mA. In the next stage, we need careful tuning the system and make sure of suppressing the transverse instabilities at higher current. In addition, remote control and damping time measurement will be completed.

Acknowledgement I would like to express my sincere appreciations to M.Tobiyama, E.Kikutani and John Byrd for helpful suggestions and thoughtful discussion.

Thank you very much for your attention!