Author/Authors :
Wakasa، نويسنده , , T and Hatanaka، نويسنده , , K and Fujita، نويسنده , , Y and Berg، نويسنده , , G.P.A and Fujimura، نويسنده , , H and Fujita، نويسنده , , H and Itoh، نويسنده , , M and Kamiya، نويسنده , , J and Kawabata، نويسنده , , T and Nagayama، نويسنده , , K and Noro، نويسنده , , T and Sakaguchi، نويسنده , , H and Shimbara، نويسنده , , Y and Takeda، نويسنده , , H and Tamura، نويسنده , , K and Ueno، نويسنده , , H and Uchida، نويسنده , , M and Uraki، نويسنده , , M، نويسنده ,
Abstract :
We have designed and constructed a new beam line which can accomplish both lateral and angular dispersion matching with the Grand Raiden spectrometer. In dispersive mode, lateral and angular dispersions of the beam line are b16=37.1 m and b26=−20.0 rad, respectively, to satisfy matching conditions for Grand Raiden. In achromatic mode, the beam line satisfies the double achromatic condition of b16=b26=0. The magnifications of the beam line are (Mx,My)=(−0.98,0.89) and (−1.00,−0.99) for dispersive and achromatic modes, respectively. In the commissioning experiments, we have succeeded to separate the first excited 2+ state of 168Er with Ex=79.8 keV clearly from the ground state in the (p,p′) reaction. We achieved energy resolutions of ΔE=13.0±0.3 and 16.7±0.3 keV in full width at half-maximum for 295 and 392 MeV protons, respectively. These energy resolutions agree with the resolving power of Grand Raiden for an object size of about 1 mm.
Keywords :
Beam transport , (p , p?) Reaction , Dispersion matching , Magnetic spectrometer