Berkeley Center for Magnet Technology
Parent: Physical Sciences
eScholarship stats: History by Item for August through November, 2024
Item | Title | Total requests | 2024-11 | 2024-10 | 2024-09 | 2024-08 |
---|---|---|---|---|---|---|
7fs202d9 | Mechanical and Thermal Analysis of an HTS Superconducting Magnet for an Achromatic Gantry for Proton Therapy | 107 | 14 | 30 | 20 | 43 |
7dj1d5sr | Design of the Superconducting Magnet System for a 45 GHz ECR Ion Source | 89 | 15 | 20 | 15 | 39 |
7nk4t123 | DFBX boxes -- electrical and cryogenic distribution boxes for the superconducting magnets in the LHC straight sections | 89 | 20 | 29 | 22 | 18 |
4d484805 | Superconducting Magnets for Particle Accelerators | 85 | 14 | 18 | 7 | 46 |
7x86q4vk | A new quench detection method for HTS magnets: stray-capacitance change monitoring | 81 | 18 | 21 | 12 | 30 |
5vq8x5js | A viable dipole magnet concept with REBCO CORC® wires and further development needs for high-field magnet applications | 72 | 14 | 16 | 8 | 34 |
1xp428p2 | HE-LHC: The High-Energy Large Hadron Collider | 57 | 10 | 13 | 11 | 23 |
5nt2c3rf | Engineering current density over 5 kA mm−2 at 4.2 K, 14 T in thick film REBCO tapes | 55 | 28 | 11 | 4 | 12 |
5w02m2h9 | The ABC130 barrel module prototyping programme for the ATLAS strip tracker | 55 | 10 | 12 | 5 | 28 |
9003s15v | Analysis of Defect Irrelevancy in a Non-Insulated REBCO Pancake Coil Using an Electric Network Model | 55 | 6 | 8 | 5 | 36 |
3xk5h52x | Technological developments and accelerator improvements for the FRIB beam power ramp-up | 54 | 2 | 9 | 3 | 40 |
7q7732kp | Quench protection for high-temperature superconductor cables using active control of current distribution | 54 | 9 | 9 | 6 | 30 |
7kb4v6dr | An Electric-Circuit Model on the Inter-Tape Contact Resistance and Current Sharing for REBCO Cable and Magnet Applications | 51 | 8 | 8 | 20 | 15 |
3dj971tm | A 1.2 T canted cosθ dipole magnet using high-temperature superconducting CORC® wires | 48 | 11 | 5 | 3 | 29 |
0km96259 | An Initial Look at the Magnetic Design of a 150 mm Aperture High-Temperature Superconducting Magnet With a Dipole Field of 8 to 10 T | 47 | 3 | 15 | 5 | 24 |
7dn9w1rs | A methodology to compute the critical current limit in Nb3Sn magnets | 47 | 8 | 10 | 1 | 28 |
7qc1f9j0 | Field Quality of HD3—A Nb$_3$Sn Dipole Magnet Based on Block Design | 47 | 5 | 7 | 9 | 26 |
7xn8533z | Superconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR | 46 | 14 | 15 | 8 | 9 |
389784f6 | Conceptual Design of a 20 T Hybrid Cos-Theta Dipole Superconducting Magnet for Future High-Energy Particle Accelerators | 45 | 1 | 11 | 3 | 30 |
72w7c0wp | Characterisation of the muon beams for the Muon Ionisation Cooling Experiment | 45 | 8 | 10 | 6 | 21 |
9vp4840m | Production and integration of the ATLAS Insertable B-Layer | 45 | 11 | 10 | 3 | 21 |
57r6k92z | Advances of the FRIB project | 44 | 6 | 11 | 4 | 23 |
94k948wv | A Review of the Mechanical Properties of Materials Used in Nb3Sn Magnets for Particle Accelerators | 44 | 8 | 12 | 6 | 18 |
8588945c | A Novel Design for Improving the Control on the Stainless-Steel Vessel Welding Process for Superconducting Magnets | 43 | 4 | 12 | 7 | 20 |
3f57f3h5 | Design choices for the integrated beam experiment (IBX) | 42 | 3 | 4 | 35 | |
7m2390f3 | Challenges and Lessons Learned From Fabrication, Testing, and Analysis of Eight MQXFA Low Beta Quadrupole Magnets for HL-LHC | 42 | 6 | 25 | 3 | 8 |
9qr8d32z | Distributed Fiber Optic Sensing to Identify Locations of Resistive Transitions in REBCO Conductors and Magnets | 42 | 2 | 10 | 5 | 25 |
9zp8p7nm | FCC-hh: The Hadron Collider | 42 | 8 | 10 | 11 | 13 |
6qj90586 | Thermoeconomic cost optimization of superconducting magnets for proton therapy gantries | 41 | 6 | 13 | 5 | 17 |
6ww3t420 | Mechanical analysis of the Nb 3 Sn 11 T dipole short models for the High Luminosity Large Hadron Collider | 41 | 5 | 9 | 9 | 18 |
8wh413h5 | Design of a High Toughness Epoxy for Superconducting Magnets and Its Key Properties | 41 | 13 | 8 | 4 | 16 |
9b14n7g1 | The ATLAS Experiment at the CERN Large Hadron Collider | 41 | 5 | 12 | 7 | 17 |
8zv5z294 | The STAR MAPS-based PiXeL detector | 40 | 3 | 8 | 1 | 28 |
68k7s9bm | REBCO -- a silver bullet for our next high-field magnet and collider budget? | 39 | 7 | 5 | 6 | 21 |
053243mv | A Superconducting transformer system for high current cable testing | 38 | 7 | 12 | 6 | 13 |
06v28277 | Computation of the Strain Induced Critical Current Reduction in the 16 T Nb3Sn Test Facility Dipole | 38 | 1 | 13 | 3 | 21 |
2d62z9b7 | Magnetic Analysis of the MQXF Quadrupole for the High-Luminosity LHC | 38 | 1 | 6 | 31 | |
7tr3p333 | Magnetic Field Correction Methods for Hybrid Permanent Magnet and Superconducting Undulators | 38 | 1 | 6 | 31 | |
0098n6gw | Mechanical Design of a Second Generation LHC IR Quadrupole | 37 | 1 | 7 | 4 | 25 |
6v1337v6 | Overview of the Quench Heater Performance for MQXF, the Nb<sub>3</sub>Sn Low-<i>β</i> Quadrupole for the High Luminosity LHC | 37 | 2 | 5 | 30 | |
0223286h | Superfluid Performance of Tevatron IR Quad Heaters | 36 | 1 | 7 | 3 | 25 |
189079b0 | The Structural Design for a “Canted Cosine–Theta” Superconducting Dipole Coil and Magnet Structure—CCT1 | 36 | 2 | 4 | 3 | 27 |
2s0663db | Development of Wind-and-React Bi-2212 Accelerator Magnet Technology | 36 | 4 | 3 | 29 | |
56v8s1kh | Diameter Quality Control of Nb3Sn Wires for MQXF Cables in the USA | 36 | 4 | 12 | 20 | |
6xw0x69d | Carbon nanotube substrates enhance SARS-CoV-2 spike protein ion yields in matrix-assisted laser desorption–ionization mass spectrometry | 36 | 5 | 12 | 1 | 18 |
00s3830w | Development of Wind-and-React Bi-2212 Accelerator Magnet Technology | 35 | 2 | 5 | 10 | 18 |
25z2r88s | Next Generation Light Source R&D and Design Studies at LBNL | 35 | 1 | 5 | 2 | 27 |
2fs8q35q | On impinging near-field granular jets | 35 | 1 | 3 | 3 | 28 |
4tz8f9q1 | An initial magnet experiment using high-temperature superconducting STAR® wires | 35 | 3 | 8 | 6 | 18 |
0sf9z6v3 | Measurements of the Strain Dependence of Critical Current of Commercial REBCO Tapes at 15 T Between 4.2 and 40 K for High Field Magnets | 34 | 7 | 5 | 5 | 17 |
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