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C2830 Datasheet(PDF) 2 Page - Hamamatsu Corporation |
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C2830 Datasheet(HTML) 2 Page - Hamamatsu Corporation |
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2 / 4 page ![]() Plug-in Sweep Units Available: Fast Sweep Unit Slow Sweep Unit Video output (Video CCD Camera)* Output format Cooled Digital Camera C4742-95 Camera head Control unit Frame Grabber Streak Image Analysis Software Streak Image Analysis Systems for IBM ® PC/AT Lens output Personal computer (IBM PC/AT Compatible) C2830 Main body Sweep units Readout system (HPD-TA) SYSTEM CONFIGURATION OPERATING PRINCIPLE The streak camera converts incident light into electrons and performs a high-speed sweep (deflecting electrons from top to bottom), enabling detection of the time variation of the incident light intensity by converting these into different positions on the screen. The figure below shows the operating principle of the streak tube, which forms the heart of the streak camera. The light pulse to be measured is focused onto the photocath- ode of the streak tube through the slit, where the photons are converted into a number of electrons proportional to the inten- sity of the incident light. These electrons are accelerated and conducted towards the phosphor screen, and a high-speed voltage which is synchronized to the incident light is applied. The electrons are swept at high speed from top to bottom and are then multipled in the MCP (micro-channel plate), after which they are bombarded against the phosphor screen of the streak tube and converted to an optical image. The optical image which appears on the phosphor screen is called a streak image, and shows the intensity distribution of the incident light, by which the positions of the electrons can be Optical intensity Time Space Trigger signal Slit Lens Incident light Photocathode (photons → electrons) Phosphor screen (electrons → light) MCP (which multiplies electrons) Streak image on phosphor screen Time Space Sweep electrode (where electrons are swept in the direction from top to bottom) Sweep circuit Accelerating electrode (where electrons are accelerated) The intensity of the incident light can be read from the brightness of the phosphor screen, and the time and space from the position of the phosphor screen. determined in the perpendicular direction over the passage of time. Using this method, the temporal intensity distribution of the light being measured can be displayed as the spatial intensity distribution on the phosphor screen. APPLICATIONS q Research involving free electron lasers and various other types of pulsed lasers q Plasma light emission, radiation, laser ablation, com- bustion and explosions q Fluorescence lifetime measurement, transient absorp- tion measurement, time-resolved Raman spectroscopy q Lidar, Thomson scattering, laser distance measurement 5 Built in main body. [Operating Principle of the Streak Tube] |
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