CAS 2005 TRIESTE APPLICATION OF THE BEAM PROFILE MONITOR FOR VEPP-4M TUNING Andrey Zhuravlev Technical parameters The BEAM profile monitor data: The beam kick and beam-beam effects Budker Institute of Nuclear Physics Beam dipole oscillations (black plot) and size Y behavior (red plot) after kick, Ie- =5.4 mA. It is the limit current for the VEPP-4M. The beam losses after a small kick and quadrupole mode instability take place. Multi-anode PMT R5900U-00-L16 HAMAMATSU Amplitude of the signal is scaled in artificial colors. MAPMT has 16 anode strips. The size of the single anode is 0.816 mm. The MAPMT Technical Parameters The Vepp-4 Facility Technical Parameters VEPP-3 circumference 75 м VEPP-4M circumference 366 м VEPP-3 maximum energy 2000 МэВ VEPP-3 Maximum current 200 мА VEPP-4M maximum energy 6000 МэВ VEPP-4M Maximum electron/positron currents 80 мА 0,2 х 0,6 VEPP-4M beam size Size 250 x 100 x 100 mm Interface 100М ethernet Internal memory ~4 М (217 beam profiles at 16 points) Discontinuity of record 1… 28 turns Beam dipole oscillations (black plot) and size Y behavior (red plot) after kick, Ie- = 220 A. мм2 Collider luminosity 1.5*10 32 VEPP-3 period of revolution 0,25 мс VEPP-4M period of revolution 1,22 мс Example of the single beam profile fitted by the Gauss function. Analyzable frequency range 10 Hz … 1 MHz Single anode size 0.8 16 mm x 64 The beam dipole oscillations (black plot) and Y behavior (red plot) during the beams convergence in the interaction point. Duration of the single turn is 1220 ns. Channel constant is 0.12 mm. Ie+= 3.4 mA, Ie- = 3.0 mA. Arrangement and principle of operation The lens. Optical magnification within limits of 320. To ADC MAPMT Phase oscillations of the beam are shown. Beam image, created by the primary optical system 64 The convergence of the beams with currents of accompanied by quadrupole instability. 16 anode strips Iе+=2.4 mA, Iе- =2.9 mA, The BEAM profile monitor data: the Beam frequencies measurement E=1777 MeV frequency Evolution of the betatron frequencies during scanning The Fourie-spectrum of the betatron fluctuations sy 100 sign/noise Start pulse E=1850 MeV 0.011 ADC triggering 80 60 40 20 0.01 The typical MAPMT signal and the operating point for the amplitude measurement Qy 120 0.012 Urf [kV] 0.009 250 Qx Qx смена 12. 05. 05. 12.05. TheНочная VEPP-4M night run. Qs s 0.013 The operating cycle of the device is as follows. MAPMT signals are recorded to the ADC after start pulse. The starting moment is either chosen by user or coincides with the beams convergence in the interaction point, “kick”, beam pass by, etc. The ADC triggering is synchronized with the beam revolution frequency. The recorded signals are stored in the internal memory and read out to the PC. Qy Time The measured low frequency oscillations of the beam (upper plot). The measured synchrotron s and betatron X, Y frequency of the beam (down plot). 0.014 amplitude frequency Layout of the optical diagnostic system. A visible part of the SR is reflected from the cooled metallic mirror and leaves the VEPP-4M vacuum Chamber through a glass window Optical layout of the diagnostics. The lens sets up a beam image on the photocathode of the MAPMT. The radial profile measurement is shown. 300 350 400 450 500 550 600 The dependence of the synchrotron frequency s with respect to the accelerating voltage Urf 0 0:00 1:00 2:00 3:00 4:00 5:00 6:00 7:00 8:00 9:00 10:00 sx Time Monitoring of parasitic phase oscillations. MAPMT data are shown. Vertical beam size depending on betatron frequencies