Berkeley Center for Magnet Technology
Parent: Physical Sciences
eScholarship stats: Breakdown by Item for December, 2024 through March, 2025
| Item | Title | Total requests | Download | View-only | %Dnld |
|---|---|---|---|---|---|
| 7fs202d9 | Mechanical and Thermal Analysis of an HTS Superconducting Magnet for an Achromatic Gantry for Proton Therapy | 118 | 24 | 94 | 20.3% |
| 7dj1d5sr | Design of the Superconducting Magnet System for a 45 GHz ECR Ion Source | 88 | 7 | 81 | 8.0% |
| 7x86q4vk | A new quench detection method for HTS magnets: stray-capacitance change monitoring | 82 | 4 | 78 | 4.9% |
| 4d484805 | Superconducting Magnets for Particle Accelerators | 80 | 12 | 68 | 15.0% |
| 5w02m2h9 | The ABC130 barrel module prototyping programme for the ATLAS strip tracker | 73 | 24 | 49 | 32.9% |
| 7nk4t123 | DFBX boxes -- electrical and cryogenic distribution boxes for the superconducting magnets in the LHC straight sections | 73 | 6 | 67 | 8.2% |
| 7kb4v6dr | An Electric-Circuit Model on the Inter-Tape Contact Resistance and Current Sharing for REBCO Cable and Magnet Applications | 66 | 53 | 13 | 80.3% |
| 9b14n7g1 | The ATLAS Experiment at the CERN Large Hadron Collider | 61 | 8 | 53 | 13.1% |
| 81n2j28n | User defined elements in ANSYS for 2D multiphysics modeling of superconducting magnets | 59 | 21 | 38 | 35.6% |
| 8wh413h5 | Design of a High Toughness Epoxy for Superconducting Magnets and Its Key Properties | 58 | 40 | 18 | 69.0% |
| 9zp8p7nm | FCC-hh: The Hadron Collider | 57 | 37 | 20 | 64.9% |
| 7m2390f3 | Challenges and Lessons Learned From Fabrication, Testing, and Analysis of Eight MQXFA Low Beta Quadrupole Magnets for HL-LHC | 56 | 26 | 30 | 46.4% |
| 7xn8533z | Superconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR | 55 | 23 | 32 | 41.8% |
| 94k948wv | A Review of the Mechanical Properties of Materials Used in Nb3Sn Magnets for Particle Accelerators | 54 | 16 | 38 | 29.6% |
| 3813v2ts | Stabilization and control of persistent current magnets using variable inductance | 49 | 15 | 34 | 30.6% |
| 3dj971tm | A 1.2 T canted cosθ dipole magnet using high-temperature superconducting CORC® wires | 48 | 25 | 23 | 52.1% |
| 5vq8x5js | A viable dipole magnet concept with REBCO CORC® wires and further development needs for high-field magnet applications | 47 | 27 | 20 | 57.4% |
| 06v28277 | Computation of the Strain Induced Critical Current Reduction in the 16 T Nb3Sn Test Facility Dipole | 46 | 21 | 25 | 45.7% |
| 4tn523mk | Field Quality of the 4.5-m-Long MQXFA Pre-Series Magnets for the HL-LHC Upgrade as Observed During Magnet Assembly | 46 | 21 | 25 | 45.7% |
| 1xp428p2 | HE-LHC: The High-Energy Large Hadron Collider | 44 | 28 | 16 | 63.6% |
| 35m6p96d | High-Field Magnets for Future Hadron Colliders | 44 | 30 | 14 | 68.2% |
| 65v2946m | Quench Detection for High-Temperature Superconductor Conductors Using Acoustic Thermometry | 44 | 18 | 26 | 40.9% |
| 57r6k92z | Advances of the FRIB project | 42 | 6 | 36 | 14.3% |
| 6qj90586 | Thermoeconomic cost optimization of superconducting magnets for proton therapy gantries | 42 | 20 | 22 | 47.6% |
| 68k7s9bm | REBCO -- a silver bullet for our next high-field magnet and collider budget? | 41 | 5 | 36 | 12.2% |
| 7dn9w1rs | A methodology to compute the critical current limit in Nb3Sn magnets | 41 | 25 | 16 | 61.0% |
| 7q7732kp | Quench protection for high-temperature superconductor cables using active control of current distribution | 41 | 21 | 20 | 51.2% |
| 9qr8d32z | Distributed Fiber Optic Sensing to Identify Locations of Resistive Transitions in REBCO Conductors and Magnets | 41 | 28 | 13 | 68.3% |
| 9003s15v | Analysis of Defect Irrelevancy in a Non-Insulated REBCO Pancake Coil Using an Electric Network Model | 40 | 25 | 15 | 62.5% |
| 9vp4840m | Production and integration of the ATLAS Insertable B-Layer | 40 | 9 | 31 | 22.5% |
| 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 | 38 | 24 | 14 | 63.2% |
| 74q7w0bc | Development and performance of a 2.9 Tesla dipole magnet using high-temperature superconducting CORC wires | 38 | 26 | 12 | 68.4% |
| 3xk5h52x | Technological developments and accelerator improvements for the FRIB beam power ramp-up | 37 | 8 | 29 | 21.6% |
| 6ww3t420 | Mechanical analysis of the Nb 3 Sn 11 T dipole short models for the High Luminosity Large Hadron Collider | 37 | 17 | 20 | 45.9% |
| 8505r1k6 | Mechanical Analysis of the Short Model Magnets for the Nb $_{3}$Sn Low-$\beta$ Quadrupole MQXF | 37 | 23 | 14 | 62.2% |
| 065858zx | Dipole Magnets above 20 Tesla: Research Needs for a Path via High-Temperature Superconducting REBCO Conductors | 36 | 14 | 22 | 38.9% |
| 2ss0b9k8 | Progress with the SNS front-end systems | 36 | 8 | 28 | 22.2% |
| 8400d5fz | Test Results of the LARP Nb3Sn Quadrupole HQ03a | 36 | 6 | 30 | 16.7% |
| 8j65c1qs | Shell-Based Support Structure for the 45 GHz ECR Ion Source MARS-D | 36 | 23 | 13 | 63.9% |
| 189079b0 | The Structural Design for a “Canted Cosine–Theta” Superconducting Dipole Coil and Magnet Structure—CCT1 | 35 | 17 | 18 | 48.6% |
| 2cg440sv | The HL-LHC Low-β Quadrupole Magnet MQXF: From Short Models to Long Prototypes | 35 | 20 | 15 | 57.1% |
| 1n1690zv | Progress on HL-LHC Nb<sub>3</sub>Sn Magnets | 34 | 12 | 22 | 35.3% |
| 83p813mt | A Possible Alternative Concept of HTS Accelerator Magnets | 34 | 19 | 15 | 55.9% |
| 87d1w3f4 | Voltage-Current Behavior of a Superconducting star Wire in a 6-Around-1 Cable Configuration | 34 | 5 | 29 | 14.7% |
| 9sb5v3t3 | Quench Protection of a Nb$_3$Sn Superconducting Magnet System for a 45-GHz ECR Ion Source | 34 | 11 | 23 | 32.4% |
| 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 | 33 | 12 | 21 | 36.4% |
| 2p99w1z5 | Status of ECR ion sources for the Facility for Rare Isotope Beams (FRIB) (invited) | 33 | 13 | 20 | 39.4% |
| 2v20h1xw | Canted–Cosine–Theta Magnet (CCT)—A Concept for High Field Accelerator Magnets | 33 | 15 | 18 | 45.5% |
| 9g28r2jn | Assembly Tests of the First Nb3Sn Low-Beta Quadrupole Short Model for the Hi-Lumi LHC | 33 | 5 | 28 | 15.2% |
| 9gd011xp | The Majorana Demonstrator readout electronics system | 33 | 8 | 25 | 24.2% |
Note: Due to the evolving nature of web traffic, the data presented here should be considered approximate and subject to revision. Learn more.