Berkeley Center for Magnet Technology

Parent: Physical Sciences

eScholarship stats: Breakdown by Item for May through August, 2026

ItemTitleTotal requestsDownloadView-only%Dnld
9zp8p7nmFCC-hh: The Hadron Collider92549642953.6%
1n1690zvProgress on HL-LHC Nb<sub>3</sub>Sn Magnets68613255419.2%
5w02m2h9The ABC130 barrel module prototyping programme for the ATLAS strip tracker3872949376.0%
9b14n7g1The ATLAS Experiment at the CERN Large Hadron Collider38322915459.8%
1xp428p2HE-LHC: The High-Energy Large Hadron Collider3642927280.2%
4d484805Superconducting Magnets for Particle Accelerators34522012563.8%
7xn8533zSuperconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR33621811864.9%
94k948wvA Review of the Mechanical Properties of Materials Used in Nb3Sn Magnets for Particle Accelerators33517715852.8%
44q234z2Fabrication and Test of C3a: A Six-Layer Subscale Canted $\cos \theta$ Dipole Magnet Using High-Temperature Superconducting corc Wires3262576978.8%
3813v2tsStabilization and control of persistent current magnets using variable inductance31415016447.8%
9vp4840mProduction and integration of the ATLAS Insertable B-Layer31217513756.1%
065858zxDipole Magnets above 20 Tesla: Research Needs for a Path via High-Temperature Superconducting REBCO Conductors3092109968.0%
0f42b5m0Irradiation-induced gas production in REBCO-based magnet materials used for future compact fusion reactors3032218272.9%
0km96259An Initial Look at the Magnetic Design of a 150 mm Aperture High-Temperature Superconducting Magnet With a Dipole Field of 8 to 10 T2811928968.3%
6qj90586Thermoeconomic cost optimization of superconducting magnets for proton therapy gantries27815612256.1%
9qr8d32zDistributed Fiber Optic Sensing to Identify Locations of Resistive Transitions in REBCO Conductors and Magnets26512014545.3%
7q7732kpQuench protection for high-temperature superconductor cables using active control of current distribution25615110559.0%
3xk5h52xTechnological developments and accelerator improvements for the FRIB beam power ramp-up25513811754.1%
7m2390f3Challenges and Lessons Learned From Fabrication, Testing, and Analysis of Eight MQXFA Low Beta Quadrupole Magnets for HL-LHC2411726971.4%
9003s15vAnalysis of Defect Irrelevancy in a Non-Insulated REBCO Pancake Coil Using an Electric Network Model2281557368.0%
8zv5z294The STAR MAPS-based PiXeL detector2251606571.1%
06v28277Computation of the Strain Induced Critical Current Reduction in the 16 T Nb3Sn Test Facility Dipole2231388561.9%
74q7w0bcDevelopment and performance of a 2.9 Tesla dipole magnet using high-temperature superconducting CORC wires2211408163.3%
0sf9z6v3Measurements of the Strain Dependence of Critical Current of Commercial REBCO Tapes at 15 T Between 4.2 and 40 K for High Field Magnets2199312642.5%
8j65c1qsShell-Based Support Structure for the 45 GHz ECR Ion Source MARS-D2161318560.6%
81n2j28nUser defined elements in ANSYS for 2D multiphysics modeling of superconducting magnets2158413139.1%
2d62z9b7Magnetic Analysis of the MQXF Quadrupole for the High-Luminosity LHC2129212043.4%
35m6p96dHigh-Field Magnets for Future Hadron Colliders2081436568.8%
4tn523mkField Quality of the 4.5-m-Long MQXFA Pre-Series Magnets for the HL-LHC Upgrade as Observed During Magnet Assembly2081535573.6%
7dn9w1rsA methodology to compute the critical current limit in Nb3Sn magnets2081268260.6%
4z1615183D Toroidal Field Multipoles for Curved Accelerator Magnets2051079852.2%
40d4p820A new quench detection method for HTS magnets: stray-capacitance change monitoring20410410051.0%
8wh413h5Design of a High Toughness Epoxy for Superconducting Magnets and Its Key Properties2041158956.4%
78x084jdHigh-Performance Bi-2212 Round Wires Made With Recent Powders2025814428.7%
5vq8x5jsA viable dipole magnet concept with REBCO CORC® wires and further development needs for high-field magnet applications2011168557.7%
8588945cA Novel Design for Improving the Control on the Stainless-Steel Vessel Welding Process for Superconducting Magnets1999910049.7%
5zb4c7b8Nanoscale detection of metastable states in porous and granular media1971603781.2%
2v20h1xwCanted–Cosine–Theta Magnet (CCT)—A Concept for High Field Accelerator Magnets1968910745.4%
1hp6d3c7Residual resistance ratio measurement system for Nb3Sn wires extracted from Rutherford cables1918210942.9%
87d1w3f4Voltage-Current Behavior of a Superconducting star Wire in a 6-Around-1 Cable Configuration1901177361.6%
66b3m2rdApplied Metrology for the Assembly of the Nb3Sn MQXFA Quadrupole Magnets for the HL-LHC AUP1861008653.8%
6hr1r29pStable, predictable and training-free operation of superconducting Bi-2212 Rutherford cable racetrack coils at the wire current density of 1000 A/mm2185889747.6%
2mg2k6h7Processing of Low T C Conductors: The Compound Nb3Sn1811592287.8%
7dj1d5srDesign of the Superconducting Magnet System for a 45 GHz ECR Ion Source1805612431.1%
13p1z31hThermal Performance of a Conduction-Cooled CCT Dipole ReBCO Magnet: Several Cycles of Cool-Down and Thermal Gradient Measurements1781235569.1%
8j18w836Magneto-Mechanical Optimization of Cross-Sections for $ \text{cos}(\theta)$Accelerator Magnets175809545.7%
6xw0x69dCarbon nanotube substrates enhance SARS-CoV-2 spike protein ion yields in matrix-assisted laser desorption–ionization mass spectrometry1731334076.9%
9fz7k751Summary of Test Results of MQXFS1—The First Short Model 150 mm Aperture Nb3Sn Quadrupole for the High-Luminosity LHC Upgrade1731106363.6%
1qh2x8w2CORC ® cable terminations with integrated Hall arrays for quench detection1721145866.3%
5hs0h07jA plan for the development of superconducting Undulator prototypes for LCLS-II and future FELs171769544.4%

Note: Due to the evolving nature of web traffic, the data presented here should be considered approximate and subject to revision. Learn more.