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Development of an Ultrafast Accumulative X-ray Streak Camera. Mahendra Shakya , Jinyuan Liu, Bing Shan And Zenghu Chang. J.R.Macdonald Laboratory Kansas State University, KS. OBJECTIVE. To Design Camera With Resolution 100fs. Motivation.
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Development of an Ultrafast Accumulative X-ray Streak Camera Mahendra Shakya , Jinyuan Liu, Bing Shan And Zenghu Chang J.R.Macdonald Laboratory Kansas State University, KS
OBJECTIVE To Design Camera With Resolution 100fs
Motivation • Study of physical process requires fast detector • Auto correlation and Cross correlation require material with efficient non-linear effect.Not applicable for X-ray • X-ray Streak Camera Provides Intensity, Time and Space information
Streak Camera Convert time into space Dt =Dx/v Dx v Dt Film Mirror Slit
Streak Tube Electrostatic Lens Phosphor Screen Slit1 Slit2 Deflection Plate X-ray Signal CCD MCP Anode Cathode Laser Pulse GaAs Switch
Developments 1975 first demonstration 1990 2ps resolution • 1996 0.5ps resolution in single-shot mode, Z.Chang (Appl.Phys.Lett.69,1(1996) • 2001 0.7 ps in accumulation mode (G.A.Naylor, et al.) by improving laser stability • 2002 0.8 ps (Belzile et al.) by using multiplephotoconductive switches • 2003 Jinyuang Liu 590 fs in accumulation mode Appl. Phys Lett. 82, pp. 20 (2003, )
Factors Affecting Temporal Resolution in Accumulative Mode • Transit Time Dispersion Velocity distribution,Angular distribution • Scanning Speed Dt s= Dx/v x •TimingJitter E V
Anode Collimating slit Cathode Au E Effect of E field on Transit Time Dispersion • High electric field 10.6V/mm 13.75V/mm 176fs 135fs tpsReduced By 23% • Collimating Slit x Reduced 50%
Factors Affecting Temporal Resolution in Accumulative Mode • Transit Time Dispersion Velocity distribution,Angular distribution • Scanning Speed Dt s= Dx/v x •TimingJitter E V
Reducing x by Changing Electrode Geometry x y -/2 re +/2 +/2 ro -/2 re= radius of the electrode r0= radius of the gap The best focused static image width, x = 175 m(25pixels)
Static Image Vb=0V , Vf = 85V, Laser energy = 60 J , 6600 Shots, Exposure time = 6s
Images with re/r0 = 1.9 FWHM, x = 560m
Factors Affecting Temporal Resolution in Accumulative Mode • Transit Time Dispersion Velocity distribution,Angular distribution • Scanning Speed Dt s= Dx/vx •TimingJitter E V
Effect Of Cables and Switch on Scanning Speed +V0 -V0 Es DP arm 1 Rb DF arm 2 Rb RL RL GaAs switch 2GHz cable, t = 90ps, 18GHz cable , t =60 ps
Deflection Plate Output With 18GHz Cables +V0 -V0 Es DP arm 1 Rb Rb DP arm 2 RL RL GaAs switch t1/
Factors Affecting Temporal Resolution in Accumulative Mode • Transit Time Dispersion Velocity distribution,Angular distribution • Scanning Speed Dt s= Dx/v x •TimingJitter E V
Photoconductive Switch The pulse amplitude of GaAs switch changes with trigger laser energy
Streak Camera Calibration Setup CCD GaAs STREAK CAMERA STREAK CAMERA 267nm L2 L1 f=150mm f=100mm 800nm ,25 fs
Bias Voltage Vs Scanning Speed Vf = 85V, Vc=8.5 kV, Laser Energy = 60 J
Cathode Voltage Vs Temporal Resolution Temporal resolution 470fs at –8.5kV Vb= 68.3V, Vf= 85V , Laser Energy = 60J, 6600 shots, Exposure time = 6.6sec
Electron Sweep Speed Vb= 68.5V, Vc= -8.5kV, Vf= 8.5V, Laser Energy = 60J
Time Resolution with Variable Slit Vc= -8.5kV, Vb= 68.3V, Vf= 85V,Exposure time = 6s, 6600 Shots.Laser energy = 60J
Intensity Vs Time at -11KV Cathode Voltage 6600 Shots average sub-picosecond pulse width streak image, Exposition time= 6.6 sec, Vb= 68.3v,Vc=-11kV, Vf= 90 Laser Energy=60J
Modification Made • Introducing variable slit to collimate electron beam • Qudrupolens Geometry. Changed re /r0 from 1.9 to 1.147
Summary • High deflection sensitivity: • 20 cm/kV • Photoconductive Switch: • 60ps rise and fall time • Fast response time: • 120 ps rise and fall time • High scanning speed: • 2c • Current Status • 470fs • Camera Potential • 200fs