Berkeley Center for Magnet Technology

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

Item	Title	Total requests	2026-08	2026-07	2026-06	2026-05
9zp8p7nm	FCC-hh: The Hadron Collider	925	285	202	246	192
1n1690zv	Progress on HL-LHC Nb<sub>3</sub>Sn Magnets	686	119	173	206	188
5w02m2h9	The ABC130 barrel module prototyping programme for the ATLAS strip tracker	387	59	100	98	130
9b14n7g1	The ATLAS Experiment at the CERN Large Hadron Collider	383	84	72	117	110
1xp428p2	HE-LHC: The High-Energy Large Hadron Collider	364	111	41	102	110
4d484805	Superconducting Magnets for Particle Accelerators	345	92	94	53	106
7xn8533z	Superconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR	336	56	65	99	116
94k948wv	A Review of the Mechanical Properties of Materials Used in Nb3Sn Magnets for Particle Accelerators	335	85	56	64	130
44q234z2	Fabrication and Test of C3a: A Six-Layer Subscale Canted $\cos \theta$ Dipole Magnet Using High-Temperature Superconducting corc Wires	326	60	42	102	122
3813v2ts	Stabilization and control of persistent current magnets using variable inductance	314	57	61	74	122
9vp4840m	Production and integration of the ATLAS Insertable B-Layer	312	59	56	107	90
065858zx	Dipole Magnets above 20 Tesla: Research Needs for a Path via High-Temperature Superconducting REBCO Conductors	309	114	57	50	88
0f42b5m0	Irradiation-induced gas production in REBCO-based magnet materials used for future compact fusion reactors	303	78	47	95	83
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	46	54	78	103
6qj90586	Thermoeconomic cost optimization of superconducting magnets for proton therapy gantries	278	95	45	43	95
9qr8d32z	Distributed Fiber Optic Sensing to Identify Locations of Resistive Transitions in REBCO Conductors and Magnets	265	51	41	85	88
7q7732kp	Quench protection for high-temperature superconductor cables using active control of current distribution	256	59	53	55	89
3xk5h52x	Technological developments and accelerator improvements for the FRIB beam power ramp-up	255	42	34	71	108
7m2390f3	Challenges and Lessons Learned From Fabrication, Testing, and Analysis of Eight MQXFA Low Beta Quadrupole Magnets for HL-LHC	241	45	63	62	71
9003s15v	Analysis of Defect Irrelevancy in a Non-Insulated REBCO Pancake Coil Using an Electric Network Model	228	48	39	58	83
8zv5z294	The STAR MAPS-based PiXeL detector	225	42	42	60	81
06v28277	Computation of the Strain Induced Critical Current Reduction in the 16 T Nb3Sn Test Facility Dipole	223	43	36	48	96
74q7w0bc	Development and performance of a 2.9 Tesla dipole magnet using high-temperature superconducting CORC wires	221	56	57	44	64
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	49	44	48	78
8j65c1qs	Shell-Based Support Structure for the 45 GHz ECR Ion Source MARS-D	216	28	38	61	89
81n2j28n	User defined elements in ANSYS for 2D multiphysics modeling of superconducting magnets	215	95	30	38	52
2d62z9b7	Magnetic Analysis of the MQXF Quadrupole for the High-Luminosity LHC	212	63	32	39	78
35m6p96d	High-Field Magnets for Future Hadron Colliders	208	48	47	43	70
4tn523mk	Field Quality of the 4.5-m-Long MQXFA Pre-Series Magnets for the HL-LHC Upgrade as Observed During Magnet Assembly	208	27	64	54	63
7dn9w1rs	A methodology to compute the critical current limit in Nb3Sn magnets	208	37	56	42	73
4z161518	3D Toroidal Field Multipoles for Curved Accelerator Magnets	205	33	26	56	90
40d4p820	A new quench detection method for HTS magnets: stray-capacitance change monitoring	204	33	35	44	92
8wh413h5	Design of a High Toughness Epoxy for Superconducting Magnets and Its Key Properties	204	40	51	55	58
78x084jd	High-Performance Bi-2212 Round Wires Made With Recent Powders	202	83	29	43	47
5vq8x5js	A viable dipole magnet concept with REBCO CORC® wires and further development needs for high-field magnet applications	201	41	53	42	65
8588945c	A Novel Design for Improving the Control on the Stainless-Steel Vessel Welding Process for Superconducting Magnets	199	46	39	53	61
5zb4c7b8	Nanoscale detection of metastable states in porous and granular media	197	32	31	51	83
2v20h1xw	Canted–Cosine–Theta Magnet (CCT)—A Concept for High Field Accelerator Magnets	196	43	30	47	76
1hp6d3c7	Residual resistance ratio measurement system for Nb3Sn wires extracted from Rutherford cables	191	49	48	30	64
87d1w3f4	Voltage-Current Behavior of a Superconducting star Wire in a 6-Around-1 Cable Configuration	190	25	33	52	80
66b3m2rd	Applied Metrology for the Assembly of the Nb3Sn MQXFA Quadrupole Magnets for the HL-LHC AUP	186	27	40	54	65
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	35	35	19	96
2mg2k6h7	Processing of Low T C Conductors: The Compound Nb3Sn	181	59	30	47	45
7dj1d5sr	Design of the Superconducting Magnet System for a 45 GHz ECR Ion Source	180	21	20	43	96
13p1z31h	Thermal Performance of a Conduction-Cooled CCT Dipole ReBCO Magnet: Several Cycles of Cool-Down and Thermal Gradient Measurements	178	27	15	44	92
8j18w836	Magneto-Mechanical Optimization of Cross-Sections for $ \text{cos}(\theta)$Accelerator Magnets	175	26	24	37	88
6xw0x69d	Carbon nanotube substrates enhance SARS-CoV-2 spike protein ion yields in matrix-assisted laser desorption–ionization mass spectrometry	173	24	55	55	39
9fz7k751	Summary of Test Results of MQXFS1—The First Short Model 150 mm Aperture Nb3Sn Quadrupole for the High-Luminosity LHC Upgrade	173	36	48	45	44
1qh2x8w2	CORC ® cable terminations with integrated Hall arrays for quench detection	172	30	49	37	56
5hs0h07j	A plan for the development of superconducting Undulator prototypes for LCLS-II and future FELs	171	30	45	44	52

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