Berkeley Center for Magnet Technology
Parent: Physical Sciences
eScholarship stats: Breakdown by Item for July through October, 2026
| Item | Title | Total requests | Download | View-only | %Dnld |
|---|---|---|---|---|---|
| 9zp8p7nm | FCC-hh: The Hadron Collider | 705 | 300 | 405 | 42.6% |
| 1n1690zv | Progress on HL-LHC Nb<sub>3</sub>Sn Magnets | 579 | 214 | 365 | 37.0% |
| 06v28277 | Computation of the Strain Induced Critical Current Reduction in the 16 T Nb3Sn Test Facility Dipole | 410 | 206 | 204 | 50.2% |
| 81n2j28n | User defined elements in ANSYS for 2D multiphysics modeling of superconducting magnets | 361 | 173 | 188 | 47.9% |
| 065858zx | Dipole Magnets above 20 Tesla: Research Needs for a Path via High-Temperature Superconducting REBCO Conductors | 346 | 246 | 100 | 71.1% |
| 7xn8533z | Superconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR | 339 | 243 | 96 | 71.7% |
| 6qj90586 | Thermoeconomic cost optimization of superconducting magnets for proton therapy gantries | 337 | 234 | 103 | 69.4% |
| 94k948wv | A Review of the Mechanical Properties of Materials Used in Nb3Sn Magnets for Particle Accelerators | 334 | 209 | 125 | 62.6% |
| 5w02m2h9 | The ABC130 barrel module prototyping programme for the ATLAS strip tracker | 332 | 285 | 47 | 85.8% |
| 7m2390f3 | Challenges and Lessons Learned From Fabrication, Testing, and Analysis of Eight MQXFA Low Beta Quadrupole Magnets for HL-LHC | 323 | 266 | 57 | 82.4% |
| 1xp428p2 | HE-LHC: The High-Energy Large Hadron Collider | 309 | 243 | 66 | 78.6% |
| 5vq8x5js | A viable dipole magnet concept with REBCO CORC® wires and further development needs for high-field magnet applications | 302 | 218 | 84 | 72.2% |
| 74q7w0bc | Development and performance of a 2.9 Tesla dipole magnet using high-temperature superconducting CORC wires | 294 | 216 | 78 | 73.5% |
| 4tn523mk | Field Quality of the 4.5-m-Long MQXFA Pre-Series Magnets for the HL-LHC Upgrade as Observed During Magnet Assembly | 293 | 214 | 79 | 73.0% |
| 3813v2ts | Stabilization and control of persistent current magnets using variable inductance | 288 | 191 | 97 | 66.3% |
| 9b14n7g1 | The ATLAS Experiment at the CERN Large Hadron Collider | 287 | 150 | 137 | 52.3% |
| 0f42b5m0 | Irradiation-induced gas production in REBCO-based magnet materials used for future compact fusion reactors | 285 | 177 | 108 | 62.1% |
| 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 | 284 | 224 | 60 | 78.9% |
| 44q234z2 | Fabrication and Test of C3a: A Six-Layer Subscale Canted $\cos \theta$ Dipole Magnet Using High-Temperature Superconducting corc Wires | 280 | 164 | 116 | 58.6% |
| 4d484805 | Superconducting Magnets for Particle Accelerators | 278 | 186 | 92 | 66.9% |
| 9003s15v | Analysis of Defect Irrelevancy in a Non-Insulated REBCO Pancake Coil Using an Electric Network Model | 278 | 222 | 56 | 79.9% |
| 7q7732kp | Quench protection for high-temperature superconductor cables using active control of current distribution | 274 | 141 | 133 | 51.5% |
| 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 | 272 | 185 | 87 | 68.0% |
| 6xw0x69d | Carbon nanotube substrates enhance SARS-CoV-2 spike protein ion yields in matrix-assisted laser desorption–ionization mass spectrometry | 268 | 220 | 48 | 82.1% |
| 65v2946m | Quench Detection for High-Temperature Superconductor Conductors Using Acoustic Thermometry | 259 | 184 | 75 | 71.0% |
| 8wh413h5 | Design of a High Toughness Epoxy for Superconducting Magnets and Its Key Properties | 258 | 176 | 82 | 68.2% |
| 2d62z9b7 | Magnetic Analysis of the MQXF Quadrupole for the High-Luminosity LHC | 253 | 160 | 93 | 63.2% |
| 9qr8d32z | Distributed Fiber Optic Sensing to Identify Locations of Resistive Transitions in REBCO Conductors and Magnets | 253 | 153 | 100 | 60.5% |
| 7kb4v6dr | An Electric-Circuit Model on the Inter-Tape Contact Resistance and Current Sharing for REBCO Cable and Magnet Applications | 245 | 167 | 78 | 68.2% |
| 8588945c | A Novel Design for Improving the Control on the Stainless-Steel Vessel Welding Process for Superconducting Magnets | 240 | 156 | 84 | 65.0% |
| 1qh2x8w2 | CORC ® cable terminations with integrated Hall arrays for quench detection | 239 | 169 | 70 | 70.7% |
| 760535cn | Finite-Element Analysis of the Strain Distribution Due to Bending in a REBCO Coated Conductor for Canted Cosine Theta Dipole Magnet Applications | 237 | 158 | 79 | 66.7% |
| 8zv5z294 | The STAR MAPS-based PiXeL detector | 235 | 194 | 41 | 82.6% |
| 9fz7k751 | Summary of Test Results of MQXFS1—The First Short Model 150 mm Aperture Nb3Sn Quadrupole for the High-Luminosity LHC Upgrade | 234 | 171 | 63 | 73.1% |
| 8j65c1qs | Shell-Based Support Structure for the 45 GHz ECR Ion Source MARS-D | 230 | 164 | 66 | 71.3% |
| 9vp4840m | Production and integration of the ATLAS Insertable B-Layer | 229 | 132 | 97 | 57.6% |
| 7dn9w1rs | A methodology to compute the critical current limit in Nb3Sn magnets | 225 | 138 | 87 | 61.3% |
| 9r61z7r8 | Flux Creep in a Bi-2212 Rutherford Cable for Particle Accelerator Applications | 220 | 183 | 37 | 83.2% |
| 389784f6 | Conceptual Design of a 20 T Hybrid Cos-Theta Dipole Superconducting Magnet for Future High-Energy Particle Accelerators | 218 | 151 | 67 | 69.3% |
| 3dj971tm | A 1.2 T canted cosθ dipole magnet using high-temperature superconducting CORC® wires | 217 | 177 | 40 | 81.6% |
| 6hr1r29p | Stable, predictable and training-free operation of superconducting Bi-2212 Rutherford cable racetrack coils at the wire current density of 1000 A/mm2 | 217 | 163 | 54 | 75.1% |
| 91m9t787 | Pion contamination in the MICE muon beam | 217 | 72 | 145 | 33.2% |
| 02x5z351 | Inverse Biot–Savart Optimization for Superconducting Accelerator Magnets | 215 | 132 | 83 | 61.4% |
| 4156s2n4 | Vanadium oxide coatings to self-regulate current sharing in high-temperature superconducting cables and magnets | 215 | 154 | 61 | 71.6% |
| 78x084jd | High-Performance Bi-2212 Round Wires Made With Recent Powders | 213 | 47 | 166 | 22.1% |
| 7fs202d9 | Mechanical and Thermal Analysis of an HTS Superconducting Magnet for an Achromatic Gantry for Proton Therapy | 213 | 172 | 41 | 80.8% |
| 40d4p820 | A new quench detection method for HTS magnets: stray-capacitance change monitoring | 212 | 158 | 54 | 74.5% |
| 1hp6d3c7 | Residual resistance ratio measurement system for Nb3Sn wires extracted from Rutherford cables | 207 | 67 | 140 | 32.4% |
| 6bx4496b | Mechanical Design Analysis of MQXFB, the 7.2-m-Long Low- $\beta$ Quadrupole for the High-Luminosity LHC Upgrade | 204 | 153 | 51 | 75.0% |
| 2mg2k6h7 | Processing of Low T C Conductors: The Compound Nb3Sn | 197 | 182 | 15 | 92.4% |
Note: Due to the evolving nature of web traffic, the data presented here should be considered approximate and subject to revision. Learn more.