Figure 2: MC Storage Ring dipole based on 4-layer block- type coil - - PDF document

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Mar 30, 2023 176 likes •219 views

SLIDE 1

✂ ✁ ✄ ☎ ✆ ✝ ✞ ✟ ✠ ✡ ☛ ✁ ☞ ✁

✌ ✍ ✎ ✏ ✞ ✟ ✡ ✂ ✁ ✂ ✁ ✑ ✎ ✒ ✏ ✞ ✓ ✏ ✞ ✟ ✡ ✔ ✁ ✂ ✁ ✕ ✆ ✓ ✏ ✆ ✖ ✡ ✗ ✌ ✘ ✙ ✞ ☎ ✎ ✝ ✡ ✚ ✎ ✛ ✎ ✖ ✞ ✎ ✡ ☞ ✜ ✢ ✣ ✤ ✥ ✣ ✡ ✦ ✁ ✧ ✁

★ ✩ ✪ ✫ ✬ ✭ ✮ ✫ ✯ ✰ ✱ ✲ ✳ ✴ ✵ ✶ ✷ ✸ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ✰ ✽ ✺ ✶ ✴ ✳ ✾ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✻ ✱ ✼ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✽ ✰ ✾ ✵ ❀ ✳ ✺ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ✰ ✽ ✷ ❁ ✶ ✰ ✱ ✯ ✰ ✸ ✸ ✻ ✹ ✳ ✾ ❂ ✻ ✵ ❀ ✷ ❃ ❄ ❅ ❆ ✳ ❇ ✲ ❄ ✰ ❄ ✿ ❄ ✳ ✱ ✳ ✾ ✼ ❈ ✷ ✱ ✹ ✷ ✱ ✷ ❉ ✳ ✾ ✷ ✼ ✳ ✸ ✶ ✿ ✻ ✱ ✰ ✺ ✻ ✵ ❈ ✰ ✽ ❃ ❊ ❋

✿ ❍ ■ ✺ ❍ ❏ ✷ ✾ ✳ ✴ ✾ ✳ ✺ ✳ ✱ ✵ ✳ ✹ ❄ ❑ ✸ ✸ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✷ ✾ ✳ ▲ ✷ ✺ ✳ ✹ ✰ ✱ ▼ ▲ ❋ ◆ ✱ ✺ ✶ ✴ ✳ ✾ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✰ ✾ ✷ ✱ ✹ ✹ ✳ ✺ ✻ ✼ ✱ ✳ ✹ ✵ ✰ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ✷ ✱ ✷ ✹ ✳ ❖ ✶ ✷ ✵ ✳ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✽ ✻ ✳ ✸ ✹ P ✽ ✻ ✳ ✸ ✹ ✼ ✾ ✷ ✹ ✻ ✳ ✱ ✵ ✻ ✱ ✵ ❀ ✳ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ❂ ✻ ✵ ❀ ✵ ❀ ✳ ✲ ✾ ✻ ✵ ✻ ✲ ✷ ✸ ✲ ✶ ✾ ✾ ✳ ✱ ✵ ✿ ✷ ✾ ✼ ✻ ✱ ✾ ✳ ❖ ✶ ✻ ✾ ✳ ✹ ✽ ✰ ✾ ✾ ✳ ✸ ✻ ✷ ▲ ✸ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✰ ✱ ✻ ✱ ✵ ❀ ✳ ✿ ✷ ✲ ❀ ✻ ✱ ✳ ❄ ❁ ✷ ✼ ✱ ✳ ✵ ✲ ✾ ✰ ✺ ✺ ◗ ✺ ✳ ✲ ✵ ✻ ✰ ✱ ✺ ❂ ✳ ✾ ✳ ✰ ✴ ✵ ✻ ✿ ✻ ❘ ✳ ✹ ✵ ✰ ✷ ✲ ❀ ✻ ✳ ❉ ✳ ✵ ❀ ✳ ✷ ✲ ✲ ✳ ✸ ✳ ✾ ✷ ✵ ✰ ✾ ✽ ✻ ✳ ✸ ✹ ❖ ✶ ✷ ✸ ✻ ✵ ❈ ✻ ✱ ✵ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✰ ✲ ✲ ✶ ✴ ✻ ✳ ✹ ❂ ✻ ✵ ❀ ▲ ✳ ✷ ✿ ✺ ❄ ❆ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✷ ✱ ✹ ✲ ✰ ✾ ✾ ✳ ✺ ✴ ✰ ✱ ✹ ✻ ✱ ✼ ✴ ✾ ✰ ✵ ✳ ✲ ✵ ✻ ❉ ✳ ✿ ✳ ✷ ✺ ✶ ✾ ✳ ✺ ✷ ✾ ✳ ✹ ✳ ✺ ✻ ✼ ✱ ✳ ✹ ✵ ✰ ❀ ✷ ✱ ✹ ✸ ✳ ✷ ▲ ✰ ✶ ✵ ❊ ❄ ❅ ❙ ❚ P ✿ ✰ ✽ ✹ ❈ ✱ ✷ ✿ ✻ ✲ ❀ ✳ ✷ ✵ ✸ ✰ ✷ ✹ ✽ ✾ ✰ ✿ ✵ ❀ ✳ ✿ ✶ ✰ ✱ ▲ ✳ ✷ ✿ ✹ ✳ ✲ ✷ ❈ ✺ ❄ ❁ ✷ ✼ ✱ ✳ ✵ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ✷ ✾ ✳ ✾ ✳ ✴ ✰ ✾ ✵ ✳ ✹ ✷ ✱ ✹ ✲ ✰ ✿ ✴ ✷ ✾ ✳ ✹ ❂ ✻ ✵ ❀ ✵ ❀ ✳ ✾ ✳ ❖ ✶ ✻ ✾ ✳ ✿ ✳ ✱ ✵ ✺ ❄ ❯ ❱ ❲ ❳ ❨ ❩ ❬ ❭ ❲ ❯ ❨ ❱

A Muon Collider is seen as a promising machine for the future of high energy physics [1]. Particle collisions in the Muon Collider will occur through the intersection of two circulating beams inside a storage ring. Requirements and

perating conditions for a Muon Collider pose significant

challenges to superconducting magnet designs and technologies [2]. For instance, contrary to proton machines, the ring dipole magnets should allow the muon decay products to escape the magnet helium volume. The IR quadrupoles must have a large aperture to accommodate the large decay deposition and large beam size at the expected *. For the IR dipoles, the required good field quality region needs to have a vertical aspect ratio of 2:1. This imposes additional challenges for the magnet design.

❆ ❀ ✻ ✺ ✴ ✷ ✴ ✳ ✾ ✺ ✶ ✿ ✿ ✷ ✾ ✻ ❘ ✳ ✺ ✵ ❀ ✳ ✾ ✳ ✺ ✶ ✸ ✵ ✺ ✰ ✽ ✲ ✰ ✱ ✲ ✳ ✴ ✵ ✶ ✷ ✸ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ✵ ✶ ✹ ✻ ✳ ✺ ✰ ✽ ✺ ✶ ✴ ✳ ✾ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✻ ✱ ✼ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✽ ✰ ✾ ✵ ❀ ✳ ✺ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ✰ ✽ ✷ ❁ ✶ ✰ ✱ ✯ ✰ ✸ ✸ ✻ ✹ ✳ ✾ ❂ ✻ ✵ ❀ ✷ ❃ ❄ ❅ ❆ ✳ ❇ ✲ ❄ ✰ ❄ ✿ ❄ ✳ ✱ ✳ ✾ ✼ ❈ ✷ ✱ ✹ ✷ ✱ ✷ ❉ ✳ ✾ ✷ ✼ ✳ ✸ ✶ ✿ ✻ ✱ ✰ ✺ ✻ ✵ ❈ ✰ ✽ ❃ ❊ ❋

✿ ❍ ■ ✺ ❍ ❏ ❄ ❆ ❀ ✳ ✺ ✳ ✺ ✵ ✶ ✹ ✻ ✳ ✺ ✻ ✱ ✲ ✸ ✶ ✹ ✳ ✹ ✵ ❀ ✳ ✲ ❀ ✰ ✻ ✲ ✳ ✰ ✽ ✺ ✶ ✴ ✳ ✾ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✰ ✾ ✷ ✱ ✹ ✿ ✷ ✼ ✱ ✳ ✵ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ✵ ✰ ✷ ✲ ❀ ✻ ✳ ❉ ✳ ✵ ❀ ✳ ✾ ✳ ❖ ✶ ✻ ✾ ✳ ✹ ✽ ✻ ✳ ✸ ✹ ✰ ✾ ✽ ✻ ✳ ✸ ✹ ✼ ✾ ✷ ✹ ✻ ✳ ✱ ✵ ✻ ✱ ❁ ✯ ◆ ✵ ✰ ✾ ✷ ✼ ✳ ❪ ✻ ✱ ✼ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ❫ ✹ ✻ ✴ ✰ ✸ ✳ ✺ ✷ ✱ ✹ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✺ ❴ ❂ ✻ ✵ ❀ ✻ ✱ ✵ ❀ ✳ ✺ ✴ ✳ ✲ ✻ ✽ ✻ ✳ ✹ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✺ ❂ ✻ ✵ ❀ ✷ ✴ ✴ ✾ ✰ ✴ ✾ ✻ ✷ ✵ ✳ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✿ ✷ ✾ ✼ ✻ ✱ ✺ ✷ ✱ ✹ ✷ ✲ ✲ ✳ ✸ ✳ ✾ ✷ ✵ ✰ ✾ ✽ ✻ ✳ ✸ ✹ ❖ ✶ ✷ ✸ ✻ ✵ ❈ ❄

Table 1: MC Storage Ring Parameters.

❵ ❛ ❜ ❛ ❝ ❞ ❡ ❞ ❜ ❢ ❣ ❤ ❡ ✐ ❛ ❥ ❦ ❞ ❧ ♠ ♥ ♦ ♠ ♣ ♠ q r s t ♠ ✉ ✈ ✇ ① ② ③ ④ ♦ ⑤ ♣ ♥ ⑥ ⑦ ⑤ ⑧ ④ ⑥ ♠ ⑨ ⑤ ♠ ⑥ ⑦ t ⑩ ✈ ❶ ⑤ q ❷ ❸ ♦ ⑨ ♠ q ♠ ♣ ❷ ♠ ❹ ♦ ❺ ✇ ② ❻ ④ ♦ ♠ ♣ ❼ ❸ ♦ ♥ ❷ ❷ ♠ ⑧ ❼ ♥ ♣ ❷ ♠ ❽ ❾ ⑩ ✇ ❺ t q ♥ ♣ ❿ ➀ ♠ q ❿ ♠ ♠ ♦ ⑤ ❼ ❼ ♥ ♣ ❷ ♠ ➁ ! ➂

·mm·mrad

❺ ② ③ ❸ ♦ ➃ ♠ q ④ ⑨ ➄ ➅ ❿ ❺

❷ ♦ ⑩

Figure 1: MC IR layout and beam size in magnets.

➆ ➇ ➈ ❱ ➉ ❲ ❳ ➉ ➊ ❬ ❯ ❳ ➉ ➆ ➉ ❱ ❲ ➋ ❁ ✶ ✰ ✱ ✯ ✰ ✸ ✸ ✻ ✹ ✳ ✾ ✵ ✷ ✾ ✼ ✳ ✵ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ✷ ✾ ✳ ✺ ✶ ✿ ✿ ✷ ✾ ✻ ❘ ✳ ✹ ✻ ✱ ❆ ✷ ▲ ✸ ✳ ❃ ❄ ❆ ❀ ✳ ✺ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ✸ ✷ ✵ ✵ ✻ ✲ ✳ ✷ ✱ ✹ ✵ ❀ ✳ ➌ ❪ ✸ ✷ ❈ ✰ ✶ ✵ ✲ ✰ ✱ ✺ ✻ ✺ ✵ ✳ ✱ ✵ ❂ ✻ ✵ ❀ ✵ ❀ ✳ ✺ ✳ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ❂ ✳ ✾ ✳ ✹ ✳ ❉ ✳ ✸ ✰ ✴ ✳ ✹ ✷ ✱ ✹ ✾ ✳ ✴ ✰ ✾ ✵ ✳ ✹ ✻ ✱ ➍ ➎ ➏ ❄ ❆ ❀ ✳ ❁ ✯ ✺ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ✻ ✺ ▲ ✷ ✺ ✳ ✹ ✰ ✱ ❃ ❊ ❆ ✹ ✻ ✴ ✰ ✸ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ❄ ❆ ❀ ✳ ✺ ✿ ✷ ✸ ✸ ✵ ✾ ✷ ✱ ✺ ❉ ✳ ✾ ✺ ✳ ▲ ✳ ✷ ✿ ✺ ✻ ❘ ✳ ❫ " ➐ ❊ ❄ ❅ ✿ ✿ ❴ ✾ ✳ ❖ ✶ ✻ ✾ ✳ ✺ ✷ ✺ ✿ ✷ ✸ ✸ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✰ ✱ ✸ ❈ ➐ ❃ ❊ ✿ ✿ ✻ ✱ ✹ ✻ ✷ ✿ ✳ ✵ ✳ ✾ ❄ ➑ ✰ ❂ ✳ ❉ ✳ ✾ ➒ ✵ ❀ ✳ ✿ ✶ ✰ ✱ ✹ ✳ ✲ ✷ ❈ ✴ ✷ ✾ ✵ ✻ ✲ ✸ ✳ ✺ ✷ ✱ ✹ ✵ ❀ ✳ ❊ ❄ ❅ ❙ ❚ P ✿ ✹ ❈ ✱ ✷ ✿ ✻ ✲ ❀ ✳ ✷ ✵ ✸ ✰ ✷ ✹ ✷ ✺ ✺ ✰ ✲ ✻ ✷ ✵ ✳ ✹ ❂ ✻ ✵ ❀ ✵ ❀ ✳ ✿ ✷ ✱ ✹ ✸ ✰ ✲ ✷ ✸ ✻ ❘ ✳ ✹ ✻ ✱ ✵ ❀ ✳ ❀ ✰ ✾ ✻ ❘ ✰ ✱ ✵ ✷ ✸ ✹ ✻ ✾ ✳ ✲ ✵ ✻ ✰ ✱ ✰ ✱ ✵ ❀ ✳ ✻ ✱ ✱ ✳ ✾ ✺ ✻ ✹ ✳ ✰ ✽ ✵ ❀ ✳ ✺ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ➒ ✱ ✳ ✳ ✹ ✵ ✰ ▲ ✳ ✻ ✱ ✵ ✳ ✾ ✲ ✳ ✴ ✵ ✳ ✹ ✰ ✶ ✵ ✺ ✻ ✹ ✳ ✰ ✽ ✵ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ❀ ✳ ✸ ✻ ✶ ✿ ❉ ✳ ✺ ✺ ✳ ✸ ✰ ✱ ✷ ✺ ✷ ✽ ✳ ✹ ✻ ✺ ✵ ✷ ✱ ✲ ✳ ✽ ✾ ✰ ✿ ✴ ✾ ✻ ✿ ✷ ✾ ❈ ▲ ✳ ✷ ✿ ✺ ❄ ❆ ❀ ✳ ✽ ✻ ✱ ✷ ✸ ✽ ✰ ✲ ✶ ✺ ✰ ✽ ✿ ✶ ✰ ✱ ▲ ✳ ✷ ✿ ✺ ✻ ✺ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ✹ ▲ ❈ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✹ ✰ ✶ ▲ ✸ ✳ ✵ ✺ ✽ ✰ ✾ ✿ ✳ ✹ ▲ ❈ ✽ ✻ ❉ ✳ ✺ ❀ ✰ ✾ ✵ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ➓ ❃ ◗ ➓ ❅ ❄ ❆ ❀ ✳ ▲ ✳ ✱ ✹ ✻ ✱ ✼ ✹ ✻ ✴ ✰ ✸ ✳ ✺ ➔ ❃ ➒ ✴ ✸ ✷ ✲ ✳ ✹ ✻ ✿ ✿ ✳ ✹ ✻ ✷ ✵ ✳ ✸ ❈ ✷ ✽ ✵ ✳ ✾ ✵ ❀ ✳ ✽ ✻ ✱ ✷ ✸ ◗ ✽ ✰ ✲ ✶ ✺ ✹ ✰ ✶ ▲ ✸ ✳ ✵ ➒ ✼ ✳ ✱ ✳ ✾ ✷ ✵ ✳ ✷ ✸ ✷ ✾ ✼ ✳ ✹ ✻ ✺ ✴ ✳ ✾ ✺ ✻ ✰ ✱ ✽ ✶ ✱ ✲ ✵ ✻ ✰ ✱ ✷ ✵ ✵ ❀ ✳ ✸ ✰ ✲ ✷ ✵ ✻ ✰ ✱ ✰ ✽ ✵ ❀ ✳ ✺ ✳ → ✵ ✶ ✴ ✰ ✸ ✳ ✱ ✳ ✷ ✾ ✳ ✺ ✵ ✵ ✰ ✵ ❀ ✳ ➌ ➣ ✵ ✰ ✲ ✰ ✿ ✴ ✳ ✱ ✺ ✷ ✵ ✳ ✽ ✰ ✾ ✵ ❀ ✳ ❉ ✳ ✾ ✵ ✻ ✲ ✷ ✸ ✲ ❀ ✾ ✰ ✿ ✷ ✵ ✻ ✲ ✻ ✵ ❈ ❄ ❆ ❀ ✳ ➌ ❪ ✸ ✷ ❈ ✰ ✶ ✵ ❂ ✻ ✵ ❀ ✵ ❀ ✳ ❉ ✳ ✾ ✵ ✻ ✲ ✷ ✸ ✷ ✱ ✹ ❀ ✰ ✾ ✻ ❘ ✰ ✱ ✵ ✷ ✸ ▲ ✳ ✷ ✿ ✺ ✻ ❘ ✳ ❉ ✷ ✾ ✻ ✷ ✵ ✻ ✰ ✱ ✺ ✻ ✺ ✺ ❀ ✰ ❂ ✱ ✻ ✱ ↔ ✻ ✼ ❄ ❃ ❄

The IR quadrupoles are divided into short pieces Q1- Q4 to provide space for protecting tungsten masks.

❆ ❀ ✳ ✺ ✴ ✷ ✲ ✳ ▲ ✳ ✵ ❂ ✳ ✳ ✱ ✵ ❀ ✳ ➓ ↕ ✷ ✱ ✹ ➓ ❅ ✻ ✺ ✾ ✳ ✺ ✳ ✾ ❉ ✳ ✹ ✽ ✰ ✾ ▲ ✳ ✷ ✿ ✹ ✻ ✷ ✼ ✱ ✰ ✺ ✵ ✻ ✲ ✺ ✷ ✱ ✹ ✲ ✰ ✾ ✾ ✳ ✲ ✵ ✰ ✾ ✺ ❄ ❆ ❀ ✳

IR magnet design parameters are summarized in Table 2. The aperture of the magnets is determined by the following criterion Dx/y=10smax+20 mm. Table 2: IR Magnet Parameters.

➙ ❛ ➛ ❣ ❞ ❡ ❡ ➜ ➝ ❞ ➙ ❛ ➛ ❣ ❞ ❡ ❤ ➞ ❥ ❞ ❣ ➛ ❡ ➟ ➠ ❝ ➙ ❛ ➛ ❣ ❞ ❡ ❛ ➝ ❞ ❜ ❡ ❦ ❜ ❞ ➡ ➢ ➤ ➥ ➠ ❝ ❝ ➦ ➧ ➨ ➩ ➫ ➧ ➨ ➭ ➠ ➯ ➲ ❝ ➩ ➯ ➭ ➳ ⑩ ⑩ ✇ ② ① ✈ ❺ ② ✈ ➳ ❺ ⑩ ✇ ① ⑩ ✈ ✈ ⑩ ➵ ① ➳ ➸ ⑩ ✇ ① ⑩ ② ✈ ⑩ ➸ ✈ ➳ ➺ ⑩ ✇ ① ⑩ ② ✈ ⑩ ➸ ✈ ➳ ② ⑩ ✇ ✈ ⑩ ② ✈ ➻ ② ❧ ⑩ ➼ ✇ ✈ ① ② ➽ ⑩ ② ✈ ➾ ➵ ➚ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➪ ➶ ➹ ➘ ➴ ➷ ➬ ➮ ➱ ➱ ➘ ➴ ✃ ❐ ❒ ❮ ❰ Ï ❐ ➴ Ð Ñ Ò ❐ ➬ ❐ Ó ➴ Ô Õ Ö × × Ñ Ó Ø Ô ❐ Ù Ú Ú Û ➮ Ø ❒ ❐ ➴ Û ➘ Ø ✃ ➴ Ó Ô ✃ Ü Ý Þ Ö Û ß à Þ ß á Û â ã ã ä å æ ç Ñ ✃ Õ ✃ Õ ❐ è é ê é Ü ë Ý é ì í × ➘ ❮ Ñ Ø î ï Ø Ó × é ð ➘ ñ

SLIDE 2

Figure 2: MC Storage Ring dipole based on 4-layer block- type coil (left) or 4-layer shell-type coil (right).

➆ ➇ ➈ ❱ ➉ ❲ ❩ ➉ ➋ ❯ ➈ ❱ ➋ ➇ ❱ ❩ ò ➇ ❳ ➇ ➆ ➉ ❲ ➉ ❳ ➋ ❆ ❀ ✳ ✸ ✳ ❉ ✳ ✸ ✰ ✽ ✿ ✷ ✼ ✱ ✳ ✵ ✻ ✲ ✽ ✻ ✳ ✸ ✹ ✺ ✻ ✱ ✺ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✺ ✶ ✼ ✼ ✳ ✺ ✵ ✺ ✶ ✺ ✻ ✱ ✼ ▼ ▲ ❋ ◆ ✱ ✺ ✶ ✴ ✳ ✾ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✰ ✾ ➒ ❂ ❀ ✻ ✲ ❀ ❀ ✷ ✺ ✵ ❀ ✳ ✿ ✰ ✺ ✵ ✷ ✴ ✴ ✾ ✰ ✴ ✾ ✻ ✷ ✵ ✳ ✲ ✰ ✿ ▲ ✻ ✱ ✷ ✵ ✻ ✰ ✱ ✰ ✽ ✵ ❀ ✳ ✲ ✾ ✻ ✵ ✻ ✲ ✷ ✸ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ó ô ➒ ❆ ô ➒ ➔ ô ■ ✷ ✱ ✹ ✻ ✺ ✲ ✰ ✿ ✿ ✳ ✾ ✲ ✻ ✷ ✸ ✸ ❈ ✴ ✾ ✰ ✹ ✶ ✲ ✳ ✹ ✷ ✵ ✵ ❀ ✳ ✴ ✾ ✳ ✺ ✳ ✱ ✵ ✵ ✻ ✿ ✳ ✻ ✱ ✸ ✰ ✱ ✼ ✸ ✳ ✱ ✼ ✵ ❀ ❄ ▼ ▲ ❋ ◆ ✱ ✺ ✵ ✾ ✷ ✱ ✹ ✷ ✱ ✹ ✲ ✷ ▲ ✸ ✳ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ✶ ✺ ✳ ✹ ✻ ✱ ✵ ❀ ✻ ✺ ✺ ✵ ✶ ✹ ❈ ✷ ✾ ✳ ✺ ✶ ✿ ✿ ✷ ✾ ✻ ❘ ✳ ✹ ✻ ✱ ❆ ✷ ▲ ✸ ✳ ➎ ❄

Table 3: Cable Parameters.

❵ ❛ ❜ ❛ ❝ ❞ ❡ ❞ ❜ ❢ ❣ ❤ ❡ õ ❛ ö ❥ ❞ ÷ õ ❛ ö ❥ ❞ ø ③ ❸ ♦ ➃ ♠ q ④ ⑨ ❿ ❼ q ♥ ♣ ⑦ ❿ ➸ ① ❺ ➵ ù ❼ q ♥ ♣ ⑦ ⑦ ⑤ ♥ ♦ ♠ ❼ ♠ q ♦ ♦ ✈ ✇ ➵ ✈ ⑩ ✇ ✈ ✈ ❶ ♥ ➃ ⑥ ♠ ⑤ ♣ ♣ ♠ q ❼ ú ⑤ ❷ ❹ ♣ ♠ ❿ ❿ ♦ ♦ ⑩ ✇ ➼ ➸ ⑩ ✇ ➵ ✈ ❶ ♥ ➃ ⑥ ♠ ④ ❸ ❼ ♠ q ❼ ú ⑤ ❷ ❹ ♣ ♠ ❿ ❿ ♦ ♦ ⑩ ✇ ➵ ➺ ⑩ ✇ ➵ ✈ ❶ ♥ ➃ ⑥ ♠ û ⑤ ⑦ ❼ ú ♦ ♦ ⑩ ➼ ✇ ➸ ❺ ⑩ ➺ ✇ ① ✈ ❶ ❸ ➽ ♣ ④ ♣ ❶ ❸ q ♥ ❼ ⑤ ④ ⑩ ✇ ⑩ ① ⑩ ✇ ✈ ✈ ü ❷ ➾ ⑩ ❺ t ➁ ➺ ✇ ❺ ý ➚ þ ➽ ♦ ♦ ÿ ❺ ① ② ✈ ❺ ① ② ✈

✁ ✬ ✭ ✂ ✄ ☎ ✆ ✝ ✂ ✞ ✆ ✟ ✁ ✠ ✄ ❆ ❀ ✳ ✹ ✻ ✴ ✰ ✸ ✳ ✾ ✳ ❖ ✶ ✻ ✾ ✳ ✿ ✳ ✱ ✵ ✺ ✷ ✱ ✹ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✲ ✰ ✱ ✹ ✻ ✵ ✻ ✰ ✱ ✺ ✲ ✷ ✸ ✸ ✽ ✰ ✾ ✷ ✱ ✰ ✴ ✳ ✱ ✿ ✻ ✹ ◗ ✴ ✸ ✷ ✱ ✳ ✹ ✳ ✺ ✻ ✼ ✱ ✷ ✴ ✴ ✾ ✰ ✷ ✲ ❀ ➍ ↕ ➏ ✷ ✱ ✹ ✷ ▲ ✳ ✷ ✿ ✴ ✻ ✴ ✳ ❂ ✻ ✵ ❀ ✸ ✷ ✾ ✼ ✳ ❀ ✰ ✾ ✻ ❘ ✰ ✱ ✵ ✷ ✸ ✺ ✻ ❘ ✳ ❄ ✯ ✾ ✰ ✺ ✺ ◗ ✺ ✳ ✲ ✵ ✻ ✰ ✱ ✺ ✰ ✽ ❁ ✯ ◆ ✵ ✰ ✾ ✷ ✼ ✳ ❪ ✻ ✱ ✼ ✹ ✻ ✴ ✰ ✸ ✳ ✺ ▲ ✷ ✺ ✳ ✹ ✰ ✱ ↕ ◗ ✸ ✷ ❈ ✳ ✾ ▲ ✸ ✰ ✲ ❙ ◗ ✵ ❈ ✴ ✳ ❫ ✸ ✳ ✽ ✵ ❴ ✷ ✱ ✹ ✺ ❀ ✳ ✸ ✸ ◗ ✵ ❈ ✴ ✳ ❫ ✾ ✻ ✼ ❀ ✵ ❴ ✲ ✰ ✻ ✸ ✺ ✷ ✾ ✳ ✺ ❀ ✰ ❂ ✱ ✻ ✱ ↔ ✻ ✼ ❄ ✡ ❄ ❆ ❀ ✳ ✿ ✷ ✻ ✱ ✿ ✷ ✼ ✱ ✳ ✵ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ✷ ✾ ✳ ✺ ✶ ✿ ✿ ✷ ✾ ✻ ❘ ✳ ✹ ✻ ✱ ❆ ✷ ▲ ✸ ✳ ↕ ❄ ❆ ❀ ✳ ✺ ❀ ✳ ✸ ✸ ◗ ✵ ❈ ✴ ✳ ✲ ✰ ✻ ✸ ✻ ✺ ▲ ✷ ✺ ✳ ✹ ✰ ✱ ❙ ✳ ❈ ✺ ✵ ✰ ✱ ✳ ✹ ✯ ✷ ▲ ✸ ✳ ❃ ✷ ✱ ✹ ✷ ✱ ✻ ✾ ✰ ✱ ❈ ✰ ❙ ✳ ❂ ✻ ✵ ❀ ✷ ✱ ✻ ✱ ✱ ✳ ✾ ✹ ✻ ✷ ✿ ✳ ✵ ✳ ✾ ❫ ➌ ☛ ❴ ✰ ✽ ✡ ↕ ❊ ✿ ✿ ❄ ❆ ❀ ✳ ▲ ✸ ✰ ✲ ❙ ◗ ✵ ❈ ✴ ✳ ✲ ✰ ✻ ✸ ✶ ✺ ✳ ✺ ✾ ✳ ✲ ✵ ✷ ✱ ✼ ✶ ✸ ✷ ✾ ✯ ✷ ▲ ✸ ✳ ✡ ✷ ✱ ✹ ✷ ✱ ❈ ✰ ❙ ✳ ❂ ✻ ✵ ❀ ✷ ✱ ➌ ☛ ✰ ✽ ✡ ❅ ❊ ✿ ✿ ❄ ❆ ❀ ✳ ✿ ✻ ✹ ◗ ✴ ✸ ✷ ✱ ✳ ✲ ✰ ✻ ✸ ◗ ✵ ✰ ◗ ✲ ✰ ✻ ✸ ✼ ✷ ✴ ✻ ✱ ▲ ✰ ✵ ❀ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ✻ ✺ ➎ ❊ ✿ ✿ ✵ ✰ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ✷ ✿ ✻ ✹ ◗ ✴ ✸ ✷ ✱ ✳ ✰ ✴ ✳ ✱ ✺ ✴ ✷ ✲ ✳ ✰ ✽ ✷ ✵ ✸ ✳ ✷ ✺ ✵ ❃ ❊ ✿ ✿ ❄ ➔ ✰ ✵ ❀ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ❀ ✷ ❉ ✳ ✴ ✾ ✷ ✲ ✵ ✻ ✲ ✷ ✸ ✸ ❈ ✵ ❀ ✳ ✺ ✷ ✿ ✳ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✰ ✾ ❉ ✰ ✸ ✶ ✿ ✳ ✷ ✱ ✹ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ✵ ❀ ✳ ✿ ✷ → ✻ ✿ ✶ ✿ ✽ ✻ ✳ ✸ ✹ ✻ ✱ ✷ ✱ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✰ ✽ ➐ ❃ ❃ ❄ ✡ ❆ ❂ ❀ ✻ ✲ ❀ ✲ ✰ ✾ ✾ ✳ ✺ ✴ ✰ ✱ ✹ ✺ ✵ ✰ ➐ ❃ ❃ ☞ ✿ ✷ ✾ ✼ ✻ ✱ ❂ ✻ ✵ ❀ ✾ ✳ ✺ ✴ ✳ ✲ ✵ ✵ ✰ ✵ ❀ ✳ ✱ ✰ ✿ ✻ ✱ ✷ ✸ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✽ ✻ ✳ ✸ ✹ ✷ ✵ ↕ ❄ ❅ ✌ ❄ ➣ ✾ ✳ ✺ ✳ ✱ ✵ ✳ ✹ ✹ ✻ ✴ ✰ ✸ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ❀ ✷ ❉ ✳ ❖ ✶ ✻ ✵ ✳ ✸ ✷ ✾ ✼ ✳ ❀ ✰ ✾ ✻ ❘ ✰ ✱ ✵ ✷ ✸ ✷ ✱ ✹ ❉ ✳ ✾ ✵ ✻ ✲ ✷ ✸ ✍ ✰ ✾ ✳ ✱ ✵ ❘ ✽ ✰ ✾ ✲ ✳ ✲ ✰ ✿ ✴ ✰ ✱ ✳ ✱ ✵ ✺ ❂ ❀ ✻ ✲ ❀ ✸ ✳ ✷ ✹ ✵ ✰ ✷ ❀ ✻ ✼ ❀ ✺ ✵ ✾ ✳ ✺ ✺ ✸ ✳ ❉ ✳ ✸ ✻ ✱ ✵ ❀ ✳ ✲ ✰ ✻ ✸ ❄ ➔ ✰ ✵ ❀ ✲ ✰ ✿ ✴ ✰ ✱ ✳ ✱ ✵ ✺ ✱ ✳ ✳ ✹ ✵ ✰ ▲ ✳ ✺ ✶ ✴ ✴ ✰ ✾ ✵ ✳ ✹ ▲ ❈ ✷ ✱ ✷ ✹ ✳ ❖ ✶ ✷ ✵ ✳ ✿ ✳ ✲ ❀ ✷ ✱ ✻ ✲ ✷ ✸ ✺ ✶ ✴ ✴ ✰ ✾ ✵ ✺ ✵ ✾ ✶ ✲ ✵ ✶ ✾ ✳ ✵ ✰ ✿ ✻ ✱ ✻ ✿ ✻ ❘ ✳ ✵ ✶ ✾ ✱ ✿ ✰ ✵ ✻ ✰ ✱ ❂ ❀ ✻ ✲ ❀ ✿ ✷ ❈ ✲ ✷ ✶ ✺ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ❖ ✶ ✳ ✱ ✲ ❀ ✷ ✱ ✹ ✽ ✻ ✳ ✸ ✹ ❖ ✶ ✷ ✸ ✻ ✵ ❈ ✹ ✳ ✼ ✾ ✷ ✹ ✷ ✵ ✻ ✰ ✱ ❄

Table 4: Storage Ring Dipole Parameters.

❵ ❛ ❜ ❛ ❝ ❞ ❡ ❞ ❜ ➫ ❥ ✎ ➞ ✏ ✑ ❞ ✒ ❤ ➛ ❣ ✓ ➟ ❞ ❥ ❥ ✑ ❞ ✒ ❤ ➛ ❣ ❧ ✔ ✕ ✖ ❷ ④ ⑤ ⑥ ♥ ❼ ➺ ✇ ② ý ➾ t ➚ ⑩ ➸ ✇ ➸ ① ⑩ ➸ ✇ ⑩ ➸ ❧ ✔ ✕ ✖ ♥ ❼ ➺ ✇ ② ý ➾ t ➚ ⑩ ⑩ ✇ ❺ ➺ ⑩ ⑩ ✇ ❺ ➺ ❧ ✗ ✘ ➾ t ➚ ⑩ ✈ ✇ ✈ ⑩ ✈ ✇ ✈ ➄ ♣ ⑦ ❸ ❷ ❼ ♥ ♣ ❷ ♠ ♥ ❼ ❧ ✗ ✘ ➾ ♦ ✙ ➽ ♦ ➚ ➼ ✇ ① ❺ ➻ ✇ ② ❺ ù ❼ ④ q ♠ ⑦ ♠ ♣ ♠ q r s ♥ ❼ ❧ ✗ ✘ ➾ ❹ ü ➽ ♦ ➚ ⑩ ❺ ➵ ✈ ⑩ ⑩ ✈ ✈ ✚ ✖ ♥ ❼ ❧ ✗ ✘ ➾ ❹ ③ ➽ ♦ ➚ ➺ ✈ ➵ ➺

3990

✚ ✛ ♥ ❼ ❧ ✗ ✘ ➾ ❹ ③ ➽ ♦ ➚ ✜ ❺ ❺ ⑩ ➼ ✜ 1870

Figure 3: Q1 (a), Q2 (b), Q3-Q5 (c) cross-sections. Geometrical field harmonics for both designs are reported in Table 5. In the shell-type design the accelerator field quality is achieved within a 50 mm circle and in the block-type design within an ellipse with 40 mm horizontal and 20 mm vertical size (blue area in Fig.2). In both cases it is sufficient to accommodate the orbit sagitta and large dispersion contribution to the beam size. Table 5: Geometrical Harmonics at Rref=10 mm (10-4).

✢ ❛ ❜ ❝ ✎ ❣ ❤ ➞ ✣ ➫ ❥ ✎ ➞ ✏ ✑ ❞ ✒ ❤ ➛ ❣ ✓ ➟ ❞ ❥ ❥ ✑ ❞ ✒ ❤ ➛ ❣ ➃ ✤ ✜ ✈ ✇ ✈ ➵ ⑩ ✈ ✇ ✈ ✈ ⑩ ➃ ✥ ✈ ✇ ✈ ➻ ⑩ ✜ ✈ ✇ ✈ ✈ ⑩ ➃ ✦ ✜ ✈ ✇ ✈ ⑩ ➸ ✈ ✇ ✈ ✈ ❺ ➃ ✧ ✜ ✈ ✇ ✈ ✈ ❺ ✜ ✈ ✇ ✈ ✈ ② ★ ✭ ✬ ✂ ✄ ✩ ✭ ✟ ✄ ✬ ✫ ✪ ✬ ✄ ✫ ☎ ✬ ✪ ✭ ✭ ✬ ✪ ✟ ✁ ✠ ✄ ✪ ➔ ✷ ✺ ✳ ✹ ✰ ✱ ❆ ✷ ▲ ✸ ✳ ✡ ✵ ❀ ✳ ➌ ❪ ✹ ✰ ✶ ▲ ✸ ✳ ✵ ✱ ✳ ✳ ✹ ✺ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✺ ❂ ✻ ✵ ❀ ✵ ❀ ✾ ✳ ✳ ✹ ✻ ✽ ✽ ✳ ✾ ✳ ✱ ✵ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✺ ✷ ✱ ✹ ✱ ✰ ✿ ✻ ✱ ✷ ✸ ✼ ✾ ✷ ✹ ✻ ✳ ✱ ✵ ✺ ✲ ✰ ✾ ✾ ✳ ✺ ✴ ✰ ✱ ✹ ✻ ✱ ✼ ✵ ✰ ➓ ❃ ➒ ➓ ✡ ✷ ✱ ✹ ➓ ➎ ◗ ➓ ↕ ❄ ➓ ❅ ❂ ✻ ✸ ✸ ✰ ✴ ✳ ✾ ✷ ✵ ✳ ✷ ✵ ✷ ✸ ✰ ❂ ✳ ✾ ✼ ✾ ✷ ✹ ✻ ✳ ✱ ✵ ✰ ✾ ✷ ✵ ✵ ❀ ✳ ✺ ✷ ✿ ✳ ✼ ✾ ✷ ✹ ✻ ✳ ✱ ✵ ▲ ✶ ✵ ▲ ✳ ✴ ✾ ✰ ✴ ✰ ✾ ✵ ✻ ✰ ✱ ✷ ✸ ✸ ❈ ✺ ❀ ✰ ✾ ✵ ✳ ✾ ❄ ❆ ❀ ✾ ✳ ✳ ▲ ✷ ✺ ✻ ✲ ➌ ❪ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✲ ✾ ✰ ✺ ✺ ◗ ✺ ✳ ✲ ✵ ✻ ✰ ✱ ✺ ✷ ✾ ✳ ✺ ❀ ✰ ❂ ✱ ✻ ✱ ↔ ✻ ✼ ❄ ➎ ➒ ✷ ✱ ✹ ✿ ✷ ✼ ✱ ✳ ✵ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ✷ ✾ ✳ ✺ ✶ ✿ ✿ ✷ ✾ ✻ ❘ ✳ ✹ ✻ ✱ ❆ ✷ ▲ ✸ ✳ ✮ ❄ ❆ ❀ ✳ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✺ ✺ ❀ ✰ ❂ ✱ ✻ ✱ ❆ ✷ ▲ ✸ ✳ ✮ ❂ ✳ ✾ ✳ ✻ ✱ ✲ ✾ ✳ ✷ ✺ ✳ ✹ ❂ ✻ ✵ ❀ ✾ ✳ ✺ ✴ ✳ ✲ ✵ ✵ ✰ ✵ ❀ ✰ ✺ ✳ ✻ ✱ ❆ ✷ ▲ ✸ ✳ ✡ ▲ ❈ ✷ ✱ ✷ ✹ ✹ ✻ ✵ ✻ ✰ ✱ ✷ ✸ ❃ ❊ ✿ ✿ ✵ ✰ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ✷ ✹ ✳ ❖ ✶ ✷ ✵ ✳ ✺ ✴ ✷ ✲ ✳ ✽ ✰ ✾ ✵ ❀ ✳ ▲ ✳ ✷ ✿ ✴ ✻ ✴ ✳ ➒ ✷ ✱ ✱ ✶ ✸ ✷ ✾ ❀ ✳ ✸ ✻ ✶ ✿ ✲ ❀ ✷ ✱ ✱ ✳ ✸ ➒ ✰ ✴ ✵ ✻ ✰ ✱ ✷ ✸ ✻ ✱ ✱ ✳ ✾ ✷ ▲ ✺ ✰ ✾ ▲ ✳ ✾ ❫ ✸ ✻ ✱ ✳ ✾ ❴ ✷ ✱ ✹ ✴ ✰ ✺ ✺ ✻ ▲ ✻ ✸ ✻ ✵ ❈ ✵ ✰ ✺ ❀ ✻ ✽ ✵ ✵ ❀ ✳ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✷ → ✻ ✺ ✵ ✰ ✲ ✾ ✳ ✷ ✵ ✳ ✷ ❉ ✳ ✾ ✵ ✻ ✲ ✷ ✸ ▲ ✳ ✱ ✹ ✻ ✱ ✼ ✽ ✻ ✳ ✸ ✹ ✻ ✱ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✺ ➍ ❅ ➏ ❄ ❆ ❀ ✳ ➌ ❪ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✺ ✷ ✾ ✳ ▲ ✷ ✺ ✳ ✹ ✰ ✱ ✡ ◗ ✸ ✷ ❈ ✳ ✾ ✺ ❀ ✳ ✸ ✸ ◗ ✵ ❈ ✴ ✳ ✲ ✰ ✻ ✸ ✺ ✷ ✱ ✹ ✷ ✲ ✰ ✸ ✹ ✻ ✾ ✰ ✱ ❈ ✰ ❙ ✳ ✺ ✳ ✴ ✷ ✾ ✷ ✵ ✳ ✹ ✽ ✾ ✰ ✿ ✵ ❀ ✳ ✲ ✰ ✻ ✸ ✺ ▲ ❈ ✷ ❃ ❊ ✿ ✿ ✺ ✴ ✷ ✲ ✳ ✾ ❄ ❑ ✸ ✸ ✵ ❀ ✳ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ✶ ✺ ✳ ✯ ✷ ▲ ✸ ✳ ❃ ❫ ✺ ✳ ✳ ❆ ✷ ▲ ✸ ✳ ➎ ❴ ✇ ❑ ✺ ✲ ✷ ✱ ▲ ✳ ✺ ✳ ✳ ✱ ➒ ✷ ✸ ✸ ✵ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ➐ ❃ ✡ ☞ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✿ ✷ ✾ ✼ ✻ ✱ ✷ ✵ ↕ ❄ ❅ ✌ ❄ ➌ ✽ ✱ ✳ ✲ ✳ ✺ ✺ ✷ ✾ ❈ ➒ ✵ ❀ ✳ ✿ ✷ ✾ ✼ ✻ ✱ ✲ ✷ ✱ ▲ ✳ ✻ ✱ ✲ ✾ ✳ ✷ ✺ ✳ ✹ ▲ ❈ ✷ ✹ ✹ ✻ ✱ ✼ ✷ ✹ ✹ ✻ ✵ ✻ ✰ ✱ ✷ ✸ ✲ ✰ ✻ ✸ ✸ ✷ ❈ ✳ ✾ ✺ ✰ ✾ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✵ ❀ ✳ ➌ ❪ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✺ ✷ ✵ ❃ ❄ ✯ ✌ ❄

Geometrical field harmonics for IR quadrupoles Q1-Q5 are presented in Table 7. The accelerator field quality is achieved within the circles (blue areas in Fig. 3) equal to 2/3 of the corresponding coil aperture. Table 6: IR Quadrupole Parameters.

❵ ❛ ❜ ❛ ❝ ❞ ❡ ❞ ❜ ✰ ÷ ✰ ø ✰ ✱ ✲ ✰ ✳ þ ⑧ ♠ q ❼ ❸ q ♠ ➾ ♦ ♦ ➚ ➵ ✈ ⑩ ⑩ ✈ ⑩ ➼ ✈ ❧ ✔ ✕ ✖ ❷ ④ ⑤ ⑥ ♥ ❼ ➺ ✇ ② ý ➾ t ➚ ⑩ ❺ ✇ ① ➼ ⑩ ➸ ✇ ⑩ ➻ ⑩ ➸ ✇ ➺ ➻ ✴ ✔ ✕ ✖ ♥ ⑧ ♠ q ❼ ♥ ❼ ➺ ✇ ② ý ➾ t ➽ ♦ ➚ ❺ ➵ ⑩ ✇ ② ❺ ✈ ➻ ✇ ✈ ⑩ ➺ ➼ ✇ ✈ ✴ ✗ ✘ ➾ t ➽ ♦ ➚ ❺ ② ✈ ⑩ ➵ ① ⑩ ➸ ✈ ➄ ♣ ⑦ ❸ ❷ ❼ ♥ ♣ ❷ ♠ ♥ ❼ ✴ ✗ ✘ ➾ ♦ ✙ ➽ ♦ ➚ ➸ ✇ ② ① ➼ ✇ ② ➵ ⑩ ❺ ✇ ➵ ➵ ù ❼ ④ q ♠ ⑦ ♠ ♣ ♠ q r s ♥ ❼ ✴ ✗ ✘ ➾ ❹ ü ➽ ♦ ➚ ➺ ➻ ➸ ✇ ✈ ① ① ⑩ ✇ ➸ ⑩ ➸ ➻ ⑩ ✇ ➵ ✚ ✖ ♥ ❼ ✴ ✗ ✘ ➾ ❹ ③ ➽ ♦ ➚ ⑩ ① ➻ ✈ ❺ ❺ ❺ ② ❺ ① ➻ ✈ ✚ ✛ ♥ ❼ ✴ ✗ ✘ ➾ ❹ ③ ➽ ♦ ➚ ✜ ❺ ⑩ ➵ ✈ ✜ ❺ ① ⑩ ➸ ✜ ➸ ➸ ➵ ✈

SLIDE 3

Table 7: Geometrical Harmonics at Rref (10-4).

✢ ❛ ❜ ❝ ✎ ❣ ❤ ➞ ✣ ✰ ÷ ✰ ø ✰ ✱ ✲ ✰ ✳ ✵ ✶ ✷ ✸ ➾ ♦ ♦ ➚ ❺ ① ➸ ① ② ➸ ➃ ✹ ✈ ✇ ✈ ✈ ✈ ✈ ✇ ✈ ✈ ✈ ✈ ✇ ✈ ✈ ✈ ➃ ✺ ✻ ✜ ✈ ✇ ✈ ➸ ➺ ✈ ✇ ✈ ✈ ❺ ✈ ✇ ✈ ✈ ❺ ➃ ✺ ✼ ✈ ✇ ➵ ➼ ❺ ✈ ✇ ✈ ➻ ✈ ✈ ✇ ✈ ➵ ➼ ✫ ☎ ✞ ✆ ✟ ✁ ✠ ✄ ❆ ❀ ✳ ✸ ✷ ✾ ✼ ✳ ❉ ✳ ✾ ✵ ✻ ✲ ✷ ✸ ▲ ✳ ✷ ✿ ✺ ✻ ❘ ✳ ✻ ✱ ✵ ❀ ✳ ➌ ❪ ✾ ✳ ✼ ✻ ✰ ✱ ❫ ✺ ✳ ✳ ↔ ✻ ✼ ❄ ❃ ❴ ✿ ✷ ❙ ✳ ✺ ✵ ❀ ✳ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ✰ ✽ ✵ ❀ ✳ ➌ ❪ ✹ ✻ ✴ ✰ ✸ ✳ ➔ ❃ ❉ ✳ ✾ ❈ ✲ ❀ ✷ ✸ ✸ ✳ ✱ ✼ ✻ ✱ ✼ ❄ ❑ ✺ ✽ ✰ ✾ ✵ ❀ ✳ ◆ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ✹ ✻ ✴ ✰ ✸ ✳ ➒ ✻ ✵ ✻ ✺ ✻ ✿ ✴ ✰ ✾ ✵ ✷ ✱ ✵ ✽ ✰ ✾ ✵ ❀ ✳ ➌ ❪ ✹ ✻ ✴ ✰ ✸ ✳ ✺ ✵ ✰ ❀ ✷ ❉ ✳ ✷ ✱ ✰ ✴ ✳ ✱ ✿ ✻ ✹ ◗ ✴ ✸ ✷ ✱ ✳ ✵ ✰ ✷ ❉ ✰ ✻ ✹ ✺ ❀ ✰ ❂ ✳ ✾ ✻ ✱ ✼ ✰ ✽ ✿ ✶ ✰ ✱ ✹ ✳ ✲ ✷ ❈ ✳ ✸ ✳ ✲ ✵ ✾ ✰ ✱ ✺ ✻ ✱ ✵ ❀ ✳ ❉ ✻ ✲ ✻ ✱ ✻ ✵ ❈ ✰ ✽ ✵ ❀ ✳ ✺ ✶ ✴ ✳ ✾ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✻ ✱ ✼ ✲ ✰ ✻ ✸ ✺ ✷ ✺ ❂ ✳ ✸ ✸ ✷ ✺ ✵ ✰ ✾ ✳ ✹ ✶ ✲ ✳ ▲ ✷ ✲ ❙ ✼ ✾ ✰ ✶ ✱ ✹ ✽ ✸ ✶ → ✳ ✺ ✻ ✱ ✷ ✹ ✳ ✵ ✳ ✲ ✵ ✰ ✾ ✲ ✳ ✱ ✵ ✾ ✷ ✸ ✵ ✾ ✷ ✲ ❙ ✳ ✾ ❄ ❆ ✰ ✾ ✳ ✿ ✰ ❉ ✳ ✯ ❅ ☞ ✰ ✽ ✵ ❀ ✳ ✾ ✷ ✹ ✻ ✷ ✵ ✻ ✰ ✱ ✽ ✾ ✰ ✿ ✵ ❀ ✳ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✵ ✰ ✵ ❀ ✳ ✳ → ✵ ✳ ✾ ✱ ✷ ✸ ✷ ▲ ✺ ✰ ✾ ▲ ✳ ✾ ✵ ❀ ✳ ✰ ✴ ✳ ✱ ✿ ✻ ✹ ◗ ✴ ✸ ✷ ✱ ✳ ✼ ✷ ✴ ✻ ✱ ➔ ❃ ✺ ❀ ✰ ✶ ✸ ✹ ▲ ✳ ✷ ✵ ✸ ✳ ✷ ✺ ✵ ❅ s ✽ ❄ ❆ ❀ ✳ ✸ ✷ ✾ ✼ ✳ ❃ ✮ ❊ ✿ ✿ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✷ ✱ ✹ ✵ ❀ ✳ ✸ ✷ ✾ ✼ ✳ ✮ ✲ ✿ ✼ ✷ ✴ ✸ ✻ ✿ ✻ ✵ ✵ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✱ ✰ ✿ ✻ ✱ ✷ ✸ ✽ ✻ ✳ ✸ ✹ ❂ ❀ ✻ ✲ ❀ ✲ ✷ ✱ ▲ ✳ ✷ ✲ ❀ ✻ ✳ ❉ ✳ ✹ ❂ ✻ ✵ ❀ ▼ ▲ ❋ ◆ ✱ ✲ ✰ ✻ ✸ ✺ ✷ ✱ ✹ ✿ ✷ ❙ ✳ ✻ ✵ ✹ ✻ ✽ ✽ ✻ ✲ ✶ ✸ ✵ ✵ ✰ ✷ ✲ ❀ ✻ ✳ ❉ ✳ ✷ ✱ ✷ ✲ ✲ ✳ ✴ ✵ ✷ ▲ ✸ ✳ ✽ ✻ ✳ ✸ ✹ ❖ ✶ ✷ ✸ ✻ ✵ ❈ ✻ ✱ ✵ ❀ ✳ ✷ ✾ ✳ ✷ ✰ ✲ ✲ ✶ ✴ ✻ ✳ ✹ ▲ ❈ ▲ ✳ ✷ ✿ ✺ ❄ ❆ ❀ ✳ ✲ ✾ ✰ ✺ ✺ ◗ ✺ ✳ ✲ ✵ ✻ ✰ ✱ ✺ ✰ ✽ ✷ ✱ ➌ ❪ ✹ ✻ ✴ ✰ ✸ ✳ ▲ ✷ ✺ ✳ ✹ ✰ ✱ ↕ ◗ ✸ ✷ ❈ ✳ ✾ ✺ ❀ ✳ ✸ ✸ ◗ ✵ ❈ ✴ ✳ ✲ ✰ ✻ ✸ ✷ ✱ ✹ ✷ ✱ ✻ ✾ ✰ ✱ ❈ ✰ ❙ ✳ ❂ ✻ ✵ ❀ ✵ ❀ ✳ ➌ ☛ ✰ ✽ ➎ ✡ ❊ ✿ ✿ ✻ ✺ ✺ ❀ ✰ ❂ ✱ ✻ ✱ ↔ ✻ ✼ ❄ ↕ ❄ ❆ ❀ ✳ ✹ ✻ ✴ ✰ ✸ ✳ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ✷ ✾ ✳ ✺ ✶ ✿ ✿ ✷ ✾ ✻ ❘ ✳ ✹ ✻ ✱ ❆ ✷ ▲ ✸ ✳ ✾ ❄

Table 8: IR Dipole Parameters.

❵ ❛ ❜ ❛ ❝ ❞ ❡ ❞ ❜ ✐ ❛ ❥ ❦ ❞ þ ⑧ ♠ q ❼ ❸ q ♠ ➾ ♦ ♦ ➚ ⑩ ➼ ✈ ❧ ✔ ✕ ✖ ⑤ ♣ ❷ ④ ⑤ ⑥ ♥ ❼ ➺ ✇ ② ý ➾ t ➚ ⑩ ➸ ✇ ✈ ➸ ❧ ✔ ✕ ✖ ⑤ ♣ ♥ ⑧ ♠ q ❼ ❸ q ♠ ♥ ❼ ➺ ✇ ② ý ➾ t ➚ ➻ ✇ ➵ ❺ ❧ ✗ ✘ ➾ t ➚ ➵ ✇ ✈ ➄ ♣ ⑦ ❸ ❷ ❼ ♥ ♣ ❷ ♠ ♥ ❼ ❧ ✗ ✘ ➾ ♦ ✙ ➽ ♦ ➚ ⑩ ② ✇ ➵ ➻ ù ❼ ④ q ♠ ⑦ ♠ ♣ ♠ q r s ♥ ❼ ❧ ✗ ✘ ➾ ❹ ü ➽ ♦ ➚ ⑩ ② ② ➵ ✚ ✖ ♥ ❼ ❧ ✗ ✘ ➾ ❹ ③ ➽ ♦ ➚ ➸ ➻ ➼ ✈ ✚ ✛ ♥ ❼ ❧ ✗ ✘ ➾ ❹ ③ ➽ ♦ ➚ ✜ ⑩ ➼ ② ✈

The dipole design is based on Cable 1 and provides the maximum design field in an aperture of 9.82 T at 4.5 K, which corresponds to ~23% margin with respect to the nominal field of 8 T. Note that the maximum field in the coil is as high as 13 T. The shell-type coil design was chosen due to its better ratio between the magnet aperture and the mid-plane gap. Studies of alternative magnet design approaches for B1 will continue. The IR dipole has a high level of Lorentz forces as the storage ring dipole. Geometrical field harmonics for IR dipole B1 are presented in Table 9. The accelerator field quality is provided within a required elliptical area with 50 mm horizontal and 110 mm vertical size (blue area in Fig. 4). It was achieved by an appropriate combination of relatively large values of low order geometrical harmonics. Table 9: Geometrical Harmonics at Rref=40 mm (10-4).

✢ ❛ ❜ ❝ ✎ ❣ ❤ ➞ ✣ ✐ ❛ ❥ ❦ ❞ ➃ ✤ ✜ ② ✇ ➵ ① ② ➃ ✥ ✜ ⑩ ➵ ✇ ➸ ❺ ✈ ➃ ✦ ✜ ⑩ ① ✇ ⑩ ✈ ② ➃ ✧ ✜ ➺ ✇ ➼ ✈ ➻

Figure 4: IR dipole cross-section.

☎ ✭ ✭ ✆ ✭ ✫ ✆ ✁ ✝ ✪ ✫ ✪ ✭ ✆ ✄ ✪

Radiation studies for IR magnets have been started [5].

❆ ❀ ✾ ✳ ✳ ✲ ✷ ✺ ✳ ✺ ❂ ✳ ✾ ✳ ✷ ✱ ✷ ✸ ❈ ❘ ✳ ✹ ✿ ❃ ❴ ❃ ❊ ◗ ✲ ✿ ✵ ❀ ✻ ✲ ❙ ✵ ✶ ✱ ✼ ✺ ✵ ✳ ✱ ✿ ✷ ✺ ❙ ✺ ❂ ✻ ✵ ❀ ❃ ❊ " ❀ ❁ ✽ ✳ ✸ ✸ ✻ ✴ ✵ ✻ ✲ ▲ ✰ ✾ ✳ ✴ ✸ ✷ ✲ ✳ ✹ ▲ ✳ ✵ ❂ ✳ ✳ ✱ ✵ ❀ ✳ ➌ ❪ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ❂ ✡ ❴ ✷ ✹ ✹ ✻ ✵ ✻ ✰ ✱ ✷ ✸ ✵ ✶ ✱ ✼ ✺ ✵ ✳ ✱ ✸ ✻ ✱ ✳ ✾ ✺ ✻ ✱ ✺ ✻ ✹ ✳ ✵ ❀ ✳ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✺ ❂ ✻ ✵ ❀ ❃ ❊ " ❀ ❁ ✽ ✳ ✸ ✸ ✻ ✴ ✵ ✻ ✲ ▲ ✰ ✾ ✳ ❂ ➎ ❴ ✲ ✷ ✺ ✳ ❃ ❂ ✻ ✵ ❀ ✵ ❀ ✳ ➌ ❪ ❖ ✶ ✷ ✹ ✾ ✶ ✴ ✰ ✸ ✳ ✺ ✹ ✻ ✺ ✴ ✸ ✷ ✲ ✳ ✹ ❀ ✰ ✾ ✻ ❘ ✰ ✱ ✵ ✷ ✸ ✸ ❈ ▲ ❈ ❃ ❊ ☞ ✰ ✽ ✵ ❀ ✳ ✻ ✾ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ✺ ✵ ✰ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ➐ ✡ ❆ ▲ ✳ ✱ ✹ ✻ ✱ ✼ ✽ ✻ ✳ ✸ ✹ ❄ ❆ ❀ ✻ ✺ ✷ ✹ ✹ ✻ ✵ ✻ ✰ ✱ ✷ ✸ ✽ ✻ ✳ ✸ ✹ ❀ ✳ ✸ ✴ ✺ ✷ ✸ ✺ ✰ ✵ ✰ ✽ ✷ ✲ ✻ ✸ ✻ ✵ ✷ ✵ ✳ ✵ ❀ ✳ ✲ ❀ ✾ ✰ ✿ ✷ ✵ ✻ ✲ ✻ ✵ ❈ ✲ ✰ ✾ ✾ ✳ ✲ ✵ ✻ ✰ ✱ ✷ ✱ ✹ ✹ ✳ ✽ ✸ ✳ ✲ ✵ ✸ ✰ ❂ ◗ ✳ ✱ ✳ ✾ ✼ ❈ ✲ ❀ ✷ ✾ ✼ ✳ ✹ ✴ ✷ ✾ ✵ ✻ ✲ ✸ ✳ ✺ ✽ ✾ ✰ ✿ ✵ ❀ ✳ ✹ ✳ ✵ ✳ ✲ ✵ ✰ ✾ ❄ ❚ ❀ ✻ ✸ ✳ ✷ ✸ ✸ ✵ ❀ ✳ ✲ ✷ ✺ ✳ ✺ ❀ ✷ ❉ ✳ ✷ ✹ ❉ ✷ ✱ ✵ ✷ ✼ ✳ ✺ ✷ ✱ ✹ ✸ ✻ ✿ ✻ ✵ ✷ ✵ ✻ ✰ ✱ ✺ ➒ ✻ ✵ ❂ ✷ ✺ ✽ ✰ ✶ ✱ ✹ ✵ ❀ ✷ ✵ ✷ ✲ ✰ ✿ ▲ ✻ ✱ ✷ ✵ ✻ ✰ ✱ ✰ ✽ ✷ ✸ ✸ ✵ ❀ ✾ ✳ ✳ ✲ ✷ ✺ ✳ ✺ ✿ ✷ ❈ ✷ ✸ ✸ ✰ ❂ ✵ ❀ ✳ ✴ ✳ ✷ ❙ ✴ ✰ ❂ ✳ ✾ ✹ ✳ ✱ ✺ ✻ ✵ ❈ ✻ ✱ ✵ ❀ ✳ ➌ ❪ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✵ ✰ ▲ ✳ ❙ ✳ ✴ ✵ ▲ ✳ ✸ ✰ ❂ ✵ ❀ ✳ ✻ ✾ ❖ ✶ ✳ ✱ ✲ ❀ ✸ ✻ ✿ ✻ ✵ ✺ ❄ ❭ ❨ ❱ ❭ ❃ ❬ ➋ ❯ ❨ ❱ ➋ ✯ ✰ ✱ ✲ ✳ ✴ ✵ ✶ ✷ ✸ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ✰ ✽ ✺ ✶ ✴ ✳ ✾ ✲ ✰ ✱ ✹ ✶ ✲ ✵ ✻ ✱ ✼ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✽ ✰ ✾ ✵ ❀ ✳ ◆ ✵ ✰ ✾ ✷ ✼ ✳ ✾ ✻ ✱ ✼ ✰ ✽ ✷ ❁ ✶ ✰ ✱ ✯ ✰ ✸ ✸ ✻ ✹ ✳ ✾ ❂ ✻ ✵ ❀ ✷ ❃ ❄ ❅ ❆ ✳ ❇ ✲ ❄ ✰ ❄ ✿ ❄ ✳ ✱ ✳ ✾ ✼ ❈ ✷ ✱ ✹ ✷ ✱ ✷ ❉ ✳ ✾ ✷ ✼ ✳ ✸ ✶ ✿ ✻ ✱ ✰ ✺ ✻ ✵ ❈ ✰ ✽ ❃ ❊ ❋

✿ ❍ ■ ✺ ❍ ❏ ❂ ✳ ✾ ✳ ✹ ✳ ❉ ✳ ✸ ✰ ✴ ✳ ✹ ▲ ✷ ✺ ✳ ✹ ✰ ✱ ✺ ✵ ✷ ✵ ✳ ◗ ✰ ✽ ◗ ✵ ❀ ✳ ◗ ✷ ✾ ✵ ▼ ▲ ❋ ◆ ✱ ✺ ✵ ✾ ✷ ✱ ✹ ✺ ✷ ✱ ✹ ❪ ✶ ✵ ❀ ✳ ✾ ✽ ✰ ✾ ✹ ✲ ✷ ▲ ✸ ✳ ✺ ❄ ❆ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ✷ ✾ ✳ ✹ ✳ ✺ ✻ ✼ ✱ ✳ ✹ ✵ ✰ ✰ ✴ ✳ ✾ ✷ ✵ ✳ ✷ ✵ ↕ ❄ ❅ ✌ ✷ ✱ ✹ ✴ ✾ ✰ ❉ ✻ ✹ ✳ ✺ ✴ ✳ ✲ ✻ ✽ ✻ ✳ ✹ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✽ ✻ ✳ ✸ ✹ P ✽ ✻ ✳ ✸ ✹ ✼ ✾ ✷ ✹ ✻ ✳ ✱ ✵ ❂ ✻ ✵ ❀ ✺ ✰ ✿ ✳ ✿ ✷ ✾ ✼ ✻ ✱ ✷ ✱ ✹ ✷ ✲ ✲ ✳ ✸ ✳ ✾ ✷ ✵ ✰ ✾ ✽ ✻ ✳ ✸ ✹ ❖ ✶ ✷ ✸ ✻ ✵ ❈ ✻ ✱ ✵ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✷ ✴ ✳ ✾ ✵ ✶ ✾ ✳ ❄ ❑ ✸ ✸ ✵ ❀ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ✺ ❀ ✷ ❉ ✳ ❖ ✶ ✻ ✵ ✳ ✸ ✷ ✾ ✼ ✳ ❀ ✰ ✾ ✻ ❘ ✰ ✱ ✵ ✷ ✸ ✷ ✱ ✹ ❉ ✳ ✾ ✵ ✻ ✲ ✷ ✸ ✍ ✰ ✾ ✳ ✱ ✵ ❘ ✽ ✰ ✾ ✲ ✳ ✲ ✰ ✿ ✴ ✰ ✱ ✳ ✱ ✵ ✺ ❄ ➔ ✰ ✵ ❀ ✲ ✰ ✿ ✴ ✰ ✱ ✳ ✱ ✵ ✺ ✱ ✳ ✳ ✹ ✵ ✰ ▲ ✳ ✺ ✶ ✴ ✴ ✰ ✾ ✵ ✳ ✹ ▲ ❈ ✷ ✹ ✳ ❖ ✶ ✷ ✵ ✳ ✿ ✳ ✲ ❀ ✷ ✱ ✻ ✲ ✷ ✸ ✺ ✵ ✾ ✶ ✲ ✵ ✶ ✾ ✳ ✺ ✵ ✰ ✿ ✻ ✱ ✻ ✿ ✻ ❘ ✳ ✵ ✶ ✾ ✱ ✿ ✰ ✵ ✻ ✰ ✱ ❂ ❀ ✻ ✲ ❀ ✿ ✷ ❈ ✲ ✷ ✶ ✺ ✳ ✿ ✷ ✼ ✱ ✳ ✵ ❖ ✶ ✳ ✱ ✲ ❀ ✻ ✱ ✼ ✷ ✱ ✹ ✽ ✻ ✳ ✸ ✹ ❖ ✶ ✷ ✸ ✻ ✵ ❈ ✹ ✳ ✼ ✾ ✷ ✹ ✷ ✵ ✻ ✰ ✱ ❄ ➑ ✷ ✱ ✹ ✸ ✻ ✱ ✼ ✵ ❀ ✳ ❉ ✳ ✾ ✵ ✻ ✲ ✷ ✸ ✍ ✰ ✾ ✳ ✱ ✵ ❘ ✽ ✰ ✾ ✲ ✳ ✲ ✰ ✿ ✴ ✰ ✱ ✳ ✱ ✵ ✻ ✺ ✵ ❀ ✳ ✿ ✷ ✻ ✱ ✲ ❀ ✷ ✸ ✸ ✳ ✱ ✼ ✳ ✰ ✽ ✵ ❀ ✳ ✰ ✴ ✳ ✱ ✿ ✻ ✹ ◗ ✴ ✸ ✷ ✱ ✳ ✹ ✳ ✺ ✻ ✼ ✱ ✺ ❄ ➣ ✾ ✷ ✲ ✵ ✻ ✲ ✷ ✸ ✺ ✰ ✸ ✶ ✵ ✻ ✰ ✱ ✺ ✵ ✰ ✵ ❀ ✻ ✺ ✴ ✾ ✰ ▲ ✸ ✳ ✿ ➒ ✵ ❀ ✳ ✺ ✵ ✶ ✹ ❈ ✷ ✱ ✹ ✰ ✴ ✵ ✻ ✿ ✻ ❘ ✷ ✵ ✻ ✰ ✱ ✰ ✽ ✿ ✷ ✼ ✱ ✳ ✵ ✰ ✴ ✳ ✾ ✷ ✵ ✻ ✱ ✼ ✿ ✷ ✾ ✼ ✻ ✱ ✷ ✱ ✹ ✰ ✵ ❀ ✳ ✾ ✴ ✷ ✾ ✷ ✿ ✳ ✵ ✳ ✾ ✺ ❂ ✻ ✸ ✸ ▲ ✳ ✹ ✰ ✱ ✳ ✹ ✶ ✾ ✻ ✱ ✼ ✺ ❀ ✰ ✾ ✵ ✿ ✰ ✹ ✳ ✸ ❪ ❄ ☛ ✴ ❀ ✷ ✺ ✳ ❄ ❳ ➉ ❅ ➉ ❳ ➉ ❱ ❭ ➉ ➋

[1] Steve Geer, “Muon Colliders and Neutrino Factories”,

Annu. Rev. of Nucl. Part. Sci. 2009.59:347-65.

[2] Y. Alexahin, E. Gianfelice-Wendt, “Muon Collider Lattice with Local Interaction Region Chromaticity Correction”,

➣ ✾ ✰ ✲ . ✰ ✽ PAC2009, Vancouver, 2009.

[3] Y. Alexahin, E. Gianfelice-Wendt, A. Netepenko, “Conceptual Design of the Muon Collider Ring Lattice”, paper TUPEB021, this Conference.

➍ ↕ ➏ ➔ ❄ ➣ ✷ ✾ ❙ ✳ ✾ ✳ ✵ ✷ ✸ .,!“Magnets for a Muon Storage Ring”,! ➣ ✾ ✰ ✲ ❄ ✰ ✽ ➣ ❑ ✯ ✡ ❊ ❊ ❃ ➒ ✯ ❀ ✻ ✲ ✷ ✼ ✰ ➒ ✡ ❊ ❊ ❃ ❄ ➍ ❅ ➏

Y.I.! Alexahin! et! al.,! “Muon!

✯ ✰ ✸ ✸ ✻ ✹ ✳ ✾ ➌ ✱ ✵ ✳ ✾ ✷ ✲ ✵ ✻ ✰ ✱ ❪ ✳ ✼ ✻ ✰ ✱ ☛ esign”,! ❆ ❇ ❆ ❈ ❉ ❊ ❋

■ ❏ ❑ ❑ ▲ ▼ ◆ ❖ P ◗ ❘ ❙ ❚ ❈ ❉ ❈ ❙ ❯ ❈ ❄