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@inproceedings{saha:hb2023-tua4i2, author = {P.K. Saha and H. Harada and H. Hotchi and K. Okabe and H. Okita and Y. Shobuda and F. Tamura and K. Yamamoto and M. Yoshimoto}, % author = {P.K. Saha and H. Harada and H. Hotchi and K. Okabe and H. Okita and Y. Shobuda and others}, % author = {P.K. Saha and others}, title = {{1-MW Beam Operation at J-PARC RCS with Minimum Beam Loss}}, % booktitle = {Proc. HB'23}, booktitle = {Proc. 68th Adv. Beam Dyn. Workshop High-Intensity High-Brightness Hadron Beams (HB'23)}, eventdate = {2023-10-09/2023-10-13}, pages = {147--152}, paper = {TUA4I2}, language = {english}, keywords = {injection, operation, simulation, beam-losses, scattering}, venue = {Geneva, Switzerland}, series = {ICFA Advanced Beam Dynamics Workshop on High-Intensity and High-Brightness Hadron Beams}, number = {68}, publisher = {JACoW Publishing, Geneva, Switzerland}, month = {04}, year = {2024}, issn = {2673-5571}, isbn = {978-3-95450-253-0}, doi = {10.18429/JACoW-HB2023-TUA4I2}, url = {https://jacow.org/hb2023/papers/tua4i2.pdf}, abstract = {{The 3-GeV RCS of J-PARC now operates at high-intensity to nearly the designed 1 MW beam. The beam loss and the corresponding residual radiation is one of the key limitations against beam intensity ramp up. Recently, by a series of beam studies and feedback from numerical simulations, we have well mitigated the beam loss to a minimum level and also reduced the beam emittances for beam operation to the spallation neutron source as well as to the main ring. The residual beam loss at the designed 1 MW beam power occurs mostly due to the unavoidable foil scattering beam loss during multi-turn injection, while other beam loss sources have been well mitigated to realize a stable and higher availability beam operation at a nearly 1 MW beam power.}}, }