Reconstruction for the brilliance-upgrading project of the Photon Factory storage ring

1998 ◽  
Vol 5 (3) ◽  
pp. 366-368 ◽  
Author(s):  
M. Katoh ◽  
Y. Hori ◽  
Y. Kobayashi ◽  
S. Sakanaka ◽  
M. Izawa ◽  
...  

Reconstruction of the Photon Factory storage ring (PF ring; 2.5 GeV) is now in progress to provide very brilliant synchrotron radiation to users, i.e. the emittance is being reduced by a factor of five. Components, such as the quadrupole and sextupole magnets, vacuum chambers, beamlines and beam-position monitors, are being replaced by new ones in 16 normal-cell sections of the PF ring. The accelerating cavities, injection systems and control systems are also being replaced. Operation will commence when the improvements are completed on 1 October 1997.

2010 ◽  
Vol 1 (MEDSI-6) ◽  
Author(s):  
B. Kosciuk ◽  
V. Ravindranath ◽  
O. Singh ◽  
S. Sharma

The National Synchrotron Light Source II currently under construction at the Brookhaven National Laboratory is expected to provide unprecedented orbit stability in the storage ring in order to fully utilize the very small emittance of the electron beam. The desire to measure the position of such small beams to high resolution imposes stringent requirements on the thermal and structural stability of the supports for the beam postion monitor (BPM) pick-up electrodes located on multi-pole vacuum chambers and more so on those located upstream and downstream of insertion device sources where the beam size is the smallest. Even with tunnel air temperature expected to be controlled to ±0.1°C, low coefficient of thermal expansion materials is required to meet this level of thermal stability. Here, we present the application of these materials to the design of stable supports for radio frequency (RF)-BPMs as well as the methods of testing their performance.


1998 ◽  
Vol 5 (3) ◽  
pp. 627-629 ◽  
Author(s):  
U. Hahn ◽  
W. Brefeld ◽  
M. Hesse ◽  
J. R. Schneider ◽  
H. Schulte-Schrepping ◽  
...  

At the 12 GeV storage ring PETRA, the first synchrotron radiation beamline uses a 4 m-long undulator. The beamline, with a length of 130 m between source and sample, delivers hard X-ray photons usable up to 300 keV. The photon beam has a total power of 7 kW. Combined with the high brilliance, the powerful beam is very critical for all beamline components. Copper, located at a distance of 26 m, hit by the full undulator beam, melts within 20 ms. Different monitors are described for stable, safe and reliable operation of beam and experiments.


2013 ◽  
Vol 198 ◽  
pp. 507-512
Author(s):  
Florian Quantmeyer ◽  
Xiao Bo Liu-Henke

Political pressure on the automotive industry will lead in future to an increasing electrification of the powertrain. The new components require the development of new vehicle control systems and control functions. Due to the high complexity of such systems the mechatronical development process including Model in the Loop (MIL), Software in the Loop (SIL) and Hardware in the Loop (HIL) simulation has been established. In this paper, a HiL test rig is presented, which has high flexibility and supports the model based development of control systems for battery electric vehicles at all levels.


Author(s):  
P. Wang ◽  
N. Hower ◽  
V. Litvinenko ◽  
M. Moallem ◽  
O. Oakeley ◽  
...  

1998 ◽  
Vol 5 (3) ◽  
pp. 618-620 ◽  
Author(s):  
T. Honda ◽  
M. Katoh ◽  
T. Mitsuhashi ◽  
A. Ueda ◽  
M. Tadano ◽  
...  

At the 2.5 GeV ring of the Photon Factory, a single-pass beam-position monitor (BPM) system is being prepared for the storage ring and the beam transport line. In the storage ring, the injected beam position during the first several turns can be measured with a single injection pulse. The BPM system has an adequate performance, useful for the commissioning of the new low-emittance lattice. Several stripline BPMs are being installed in the beam transport line. The continuous monitoring of the orbit in the beam transport line will be useful for the stabilization of the injection energy as well as the injection beam orbit.


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