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This system is intended to promote experimental research on fundamental technologies in private sector, with The Japan Key Technology Center(70 %) and participating private companies (30 %) financing the capital requiring for this purpose.
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| Research Organization | Electron Accelerator | Electron Gun | First Lasing (Year of Building) | FEL Wavelength Range (ƒÊm) | Peak Power (Average Power) | Research Theme |
| Stanford Univ (USA) | Superconductive Linea Accelerator 66MeV, 5.6A | Hot Cathode | 1977 | 3 - 15 20 - 60 | 1.2MW (1W) | solid state physics Solid state physics, bioscience, medicine |
| UCSB (USA) | Van de Greaf
6MeV | Hot Cathode | 1985 | 350 - 2500 60 - 350 30 - 90 | ( - 10kW) | Semiconductor solid state |
| Duke Univ. (USA)(Mark III) | Normal Conductive Linea Accelerator 45MeV, 40A | Hot Cathode RF Gun | 1986 | 1.8 - 9.5 | 2MW (3W) | Solid state physics |
| Vanderbilt Univ. (USA)(Mark III) | Normal Conductive Linea Accelerator 45MeV, 40A | Hot Cathode RF Gun | 1991 (1987) | 2 - 8 | 3MW (6W) | Bioscience, medicine, solid state physics Solid state physics |
| FOM FELIX (Netherlands) | Normal Conductive Linea Accelerator 45MeV, 70A | Hot Cathode | 1991 | 5 - 30 16 - 110 |
5MW (0.5W) | Nuclear/ molecular physics, bioscience, medicine |
| LURE CLIO (France) | Normal Conductive Linea Accelerator 70MeV, 75A | Hot Cathode | 1992 | 1.8 - 17.5 | 10MW (9W) | Solid state physics |
| LANL AFEL (USA) | Normal Conductive Linea Accelerator 15MeV, 100A | Optical Cathode | 1993 | 4 - 6 | 10MW (1.5W) | Medical applications |
| FELI (Japan) | Normal Conductive Linea Accelerator
33MeV, 42A 75MeV, 50A 160MeV, 60A 20MeV, 40A 20MeV, 40A | Hot Cathode |
(1993) 1994 1995 1995 1996 1996 | 5 - 22 1 - 6 0.23 - 1.2 20 - 60 50 - 100 | 5MW (2W) 15MW(3W) 10MW(2W) 5MW(1W) 5 MW(1W) | Semiconductor solid state, isotope separation Medical applications Bioscience New material Catalyst development |
We are developing a wavelength-independent method for the simultaneous sharing of FEL beams. The FEL beams pass through the 1 mm diameter exit hole in the output mirror which forms a part of the optical resonator in the free electron laser device. These FEL beams broaden by diffraction are transported to nearby experimental stations over a distance of several tens of meters; the beam radius involved is on the order of several centimeters. The simultaneous FEL beam sharing method we developed uses a series of specially-shaped fan-shaped mirrors (installed in each stations) to split and distribute the beams into roughly triangular, fan-shaped pieces. These mirrors are positioned such that the reflected beams do not overlap, and therefore interfere with each other. In this manner, as multiple sites may use FEL simultaneously, the rate of FEL use would be improved.
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So therefore, as conventional lasers use only certain restricted portions of the spectrum for their operation, it follows from this that new applications may be found for lasers using these currently-unexploited wavelengths. Given the FEL laser's broad spectral coverage from the far-infrared through the ultra-violet region, including these currently-unexploited wavelengths, it is a natural candidate for the exploration and development of new applications using these portions of the spectrum.
These applications may include: polishing and surface hardening of the teeth using a wavelength of 9.4ƒÊm taking advantage of the resonance of the PO4 coupling bond of hydroxyapatite which forms an enamel-like substance as mentioned above. Other applications include the evaluation of characteristics of TeraHertz band semiconductor super-grid structure as a super high-speed device; and creation of new materials using lattice vibration phenomena as the vibrating/exciting Si compounds using a 12.6ƒÊm free electron laser.
Expected Cost:
Annual Budget(Unit: billion yen)
| Fiscal Year | Budget |
| FY1990 | 0.2134 |
| FY 1991 | 0.2828 |
| FY 1992 | 1.1006 |
| FY 1993 | 2.0260 |
| FY 1994 | 2.5830 |
| FY 1995 | 1.7354 |
| FY 1996 | 0.6890 |
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