Status of the 16 T Dipole Development Program for a Future Hadron Collider

A next step of energy increase of hadron colliders beyond the LHC requires high-field superconducting magnets capable of providing a dipolar field in the range of 16 T in a 50-mm aperture with accelerator quality. These characteristics could meet the requirements for an upgrade of the LHC to twice the present beam energy or for a 100-TeV center of mass energy future circular collider. This paper summarizes the activities and plans for the development of these magnets, in particular within the 16 T Magnet Technology Program, the WP5 of the EuroCirCol, and the U.S. Magnet Development Program.

Future circular collider (FCC)
superconducting
Nb $_{3}$ Sn
16 T
activity report
magnet: superconductivity
magnet: technology
beam: energy
CERN LHC Coll: upgrade
bending magnet

References(23)

Figures(0)

[1]

The European strategy for particle physics

[2]

Proceedings of the EuCARD-AccNet-EuroLumi Workshop: The high-energy large hadron collider (HE-LHC10) Villa Bighi Malta Oct. 2010 Republic of Malta

[3]

Progress on the Development of the Nb $_3$ Sn 11T Dipole for the High Luminosity Upgrade of LHC

et al.

- IEEE Trans.Appl.Supercond. 27 (2017) 4, 4003505
•
DOI:
- 10.1109/TASC.2017.2666142

[4]

Development of MQXF: The Nb $_{3}$ Sn Low- $\beta$ Quadrupole for the HiLumi LHC

et al.

- IEEE Trans.Appl.Supercond. 26 (2016) 4, 4000207
•
DOI:
- 10.1109/TASC.2015.2510508

[5]

The 16 T Dipole Development Program for FCC

et al.

- IEEE Trans.Appl.Supercond. 27 (2017) 4, 4000405
•
DOI:
- 10.1109/TASC.2016.2634600

[6]

Horizon2020 EuroCirCol Consortium Agreement

[7]

[online] Available:

[8]

Conceptual design of a 16 T cosθ bending dipole for the future circular collider

V. Marinozzi

[9]

Design of a Nb 3 Sn 16 T block dipole for the future circular collider

C. Lorin
,
M. Durante
,
H. Felice
,
M. Segreti

[10]

Magnetic and mechanical design of a 16 T common coil dipole for FCC

F. Toral
,
J. Munilla

[11]

Superconducting coil compression by scissor laminations

A. Ijspeert
,
J. Salminen

[12]

Electromechanical Design of a 16-T CCT Twin-Aperture Dipole for FCC

et al.

- IEEE Trans.Appl.Supercond. 28 (2018) 3, 4000705
•
DOI:
- 10.1109/TASC.2017.2772898

[13]

CLIQ. A new quench protection technology for superconducting magnets

Emmanuele Ravaioli
(
- Twente U., Enschede
)

DOI:
- 10.3990/1.9789036539081

[14]

Conductor choices for upgrades of CERN magnets

L. Rossi

[15]

Characterization of irreversible degradation of Nb 3 Sn Rutherford cables due to transversal compression stress at room temperature

Patrick Ebermann

[16]

Status of the Activities on the [FORMULA] Dipole SMC and of the Design of the RMC

et al.

- IEEE Trans.Appl.Supercond. 23 (2013) 3, 4002308
•
DOI:
- 10.1109/TASC.2013.2244932

[17]

Design of ERMC and RMM, the Base of the Nb $_3$ Sn 16 T Magnet Development at CERN

- IEEE Trans.Appl.Supercond. 27 (2017) 4, 4002004
•
DOI:
- 10.1109/TASC.2017.2651403

[18]

3D Magnetic and mechanical design of coil ends for the racetrack model magnet RMM

E. Rochepault
,
S. Izquierdo Bermudez
,
J.C. Perez
,
D. Schoerling
,
D. Tommasini

[19]

The US magnet development program for high field accelerator magnet R&D

S. Prestemon

[20]

Design concept and parameters of a 15 T Nb 3 Sn dipole demonstrator for a 100 TeV hadron collider

A.V. Zlobin

[21]

Development of a 15 T Nb $_3$ Sn Accelerator Dipole Demonstrator at Fermilab

et al.

- IEEE Trans.Appl.Supercond. 26 (2016) 4, 4001007
•
DOI:
- 10.1109/TASC.2016.2517024

[22]

FEA model and mechanical analysis of the Nb 3 Sn 15 T dipole demonstrator

C. Kokkinos

[23]

Design and fabrication of a 15 T Nb 3 Sn accelerator dipole demonstrator

I. Novitski