Berkeley Center for Magnet Technology
Parent: Physical Sciences
eScholarship stats: Breakdown by Item for May through August, 2026
| Item | Title | Total requests | Download | View-only | %Dnld |
|---|---|---|---|---|---|
| 9zp8p7nm | FCC-hh: The Hadron Collider | 925 | 496 | 429 | 53.6% |
| 1n1690zv | Progress on HL-LHC Nb<sub>3</sub>Sn Magnets | 686 | 132 | 554 | 19.2% |
| 5w02m2h9 | The ABC130 barrel module prototyping programme for the ATLAS strip tracker | 387 | 294 | 93 | 76.0% |
| 9b14n7g1 | The ATLAS Experiment at the CERN Large Hadron Collider | 383 | 229 | 154 | 59.8% |
| 1xp428p2 | HE-LHC: The High-Energy Large Hadron Collider | 364 | 292 | 72 | 80.2% |
| 4d484805 | Superconducting Magnets for Particle Accelerators | 345 | 220 | 125 | 63.8% |
| 7xn8533z | Superconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR | 336 | 218 | 118 | 64.9% |
| 94k948wv | A Review of the Mechanical Properties of Materials Used in Nb3Sn Magnets for Particle Accelerators | 335 | 177 | 158 | 52.8% |
| 44q234z2 | Fabrication and Test of C3a: A Six-Layer Subscale Canted $\cos \theta$ Dipole Magnet Using High-Temperature Superconducting corc Wires | 326 | 257 | 69 | 78.8% |
| 3813v2ts | Stabilization and control of persistent current magnets using variable inductance | 314 | 150 | 164 | 47.8% |
| 9vp4840m | Production and integration of the ATLAS Insertable B-Layer | 312 | 175 | 137 | 56.1% |
| 065858zx | Dipole Magnets above 20 Tesla: Research Needs for a Path via High-Temperature Superconducting REBCO Conductors | 309 | 210 | 99 | 68.0% |
| 0f42b5m0 | Irradiation-induced gas production in REBCO-based magnet materials used for future compact fusion reactors | 303 | 221 | 82 | 72.9% |
| 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 | 281 | 192 | 89 | 68.3% |
| 6qj90586 | Thermoeconomic cost optimization of superconducting magnets for proton therapy gantries | 278 | 156 | 122 | 56.1% |
| 9qr8d32z | Distributed Fiber Optic Sensing to Identify Locations of Resistive Transitions in REBCO Conductors and Magnets | 265 | 120 | 145 | 45.3% |
| 7q7732kp | Quench protection for high-temperature superconductor cables using active control of current distribution | 256 | 151 | 105 | 59.0% |
| 3xk5h52x | Technological developments and accelerator improvements for the FRIB beam power ramp-up | 255 | 138 | 117 | 54.1% |
| 7m2390f3 | Challenges and Lessons Learned From Fabrication, Testing, and Analysis of Eight MQXFA Low Beta Quadrupole Magnets for HL-LHC | 241 | 172 | 69 | 71.4% |
| 9003s15v | Analysis of Defect Irrelevancy in a Non-Insulated REBCO Pancake Coil Using an Electric Network Model | 228 | 155 | 73 | 68.0% |
| 8zv5z294 | The STAR MAPS-based PiXeL detector | 225 | 160 | 65 | 71.1% |
| 06v28277 | Computation of the Strain Induced Critical Current Reduction in the 16 T Nb3Sn Test Facility Dipole | 223 | 138 | 85 | 61.9% |
| 74q7w0bc | Development and performance of a 2.9 Tesla dipole magnet using high-temperature superconducting CORC wires | 221 | 140 | 81 | 63.3% |
| 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 | 219 | 93 | 126 | 42.5% |
| 8j65c1qs | Shell-Based Support Structure for the 45 GHz ECR Ion Source MARS-D | 216 | 131 | 85 | 60.6% |
| 81n2j28n | User defined elements in ANSYS for 2D multiphysics modeling of superconducting magnets | 215 | 84 | 131 | 39.1% |
| 2d62z9b7 | Magnetic Analysis of the MQXF Quadrupole for the High-Luminosity LHC | 212 | 92 | 120 | 43.4% |
| 35m6p96d | High-Field Magnets for Future Hadron Colliders | 208 | 143 | 65 | 68.8% |
| 4tn523mk | Field Quality of the 4.5-m-Long MQXFA Pre-Series Magnets for the HL-LHC Upgrade as Observed During Magnet Assembly | 208 | 153 | 55 | 73.6% |
| 7dn9w1rs | A methodology to compute the critical current limit in Nb3Sn magnets | 208 | 126 | 82 | 60.6% |
| 4z161518 | 3D Toroidal Field Multipoles for Curved Accelerator Magnets | 205 | 107 | 98 | 52.2% |
| 40d4p820 | A new quench detection method for HTS magnets: stray-capacitance change monitoring | 204 | 104 | 100 | 51.0% |
| 8wh413h5 | Design of a High Toughness Epoxy for Superconducting Magnets and Its Key Properties | 204 | 115 | 89 | 56.4% |
| 78x084jd | High-Performance Bi-2212 Round Wires Made With Recent Powders | 202 | 58 | 144 | 28.7% |
| 5vq8x5js | A viable dipole magnet concept with REBCO CORC® wires and further development needs for high-field magnet applications | 201 | 116 | 85 | 57.7% |
| 8588945c | A Novel Design for Improving the Control on the Stainless-Steel Vessel Welding Process for Superconducting Magnets | 199 | 99 | 100 | 49.7% |
| 5zb4c7b8 | Nanoscale detection of metastable states in porous and granular media | 197 | 160 | 37 | 81.2% |
| 2v20h1xw | Canted–Cosine–Theta Magnet (CCT)—A Concept for High Field Accelerator Magnets | 196 | 89 | 107 | 45.4% |
| 1hp6d3c7 | Residual resistance ratio measurement system for Nb3Sn wires extracted from Rutherford cables | 191 | 82 | 109 | 42.9% |
| 87d1w3f4 | Voltage-Current Behavior of a Superconducting star Wire in a 6-Around-1 Cable Configuration | 190 | 117 | 73 | 61.6% |
| 66b3m2rd | Applied Metrology for the Assembly of the Nb3Sn MQXFA Quadrupole Magnets for the HL-LHC AUP | 186 | 100 | 86 | 53.8% |
| 6hr1r29p | Stable, predictable and training-free operation of superconducting Bi-2212 Rutherford cable racetrack coils at the wire current density of 1000 A/mm2 | 185 | 88 | 97 | 47.6% |
| 2mg2k6h7 | Processing of Low T C Conductors: The Compound Nb3Sn | 181 | 159 | 22 | 87.8% |
| 7dj1d5sr | Design of the Superconducting Magnet System for a 45 GHz ECR Ion Source | 180 | 56 | 124 | 31.1% |
| 13p1z31h | Thermal Performance of a Conduction-Cooled CCT Dipole ReBCO Magnet: Several Cycles of Cool-Down and Thermal Gradient Measurements | 178 | 123 | 55 | 69.1% |
| 8j18w836 | Magneto-Mechanical Optimization of Cross-Sections for $ \text{cos}(\theta)$Accelerator Magnets | 175 | 80 | 95 | 45.7% |
| 6xw0x69d | Carbon nanotube substrates enhance SARS-CoV-2 spike protein ion yields in matrix-assisted laser desorption–ionization mass spectrometry | 173 | 133 | 40 | 76.9% |
| 9fz7k751 | Summary of Test Results of MQXFS1—The First Short Model 150 mm Aperture Nb3Sn Quadrupole for the High-Luminosity LHC Upgrade | 173 | 110 | 63 | 63.6% |
| 1qh2x8w2 | CORC ® cable terminations with integrated Hall arrays for quench detection | 172 | 114 | 58 | 66.3% |
| 5hs0h07j | A plan for the development of superconducting Undulator prototypes for LCLS-II and future FELs | 171 | 76 | 95 | 44.4% |
Note: Due to the evolving nature of web traffic, the data presented here should be considered approximate and subject to revision. Learn more.