Accelerator Tech-Applied Phys
Parent: Physical Sciences
eScholarship stats: Breakdown by Item for October, 2024 through January, 2025
Item | Title | Total requests | Download | View-only | %Dnld |
---|---|---|---|---|---|
2c14z63t | The Absence of Plasma in "Spark Plasma Sintering" | 259 | 14 | 245 | 5.4% |
3261x4bm | A structure zone diagram including plasma based deposition and ion etching | 161 | 122 | 39 | 75.8% |
74s0t81f | Tutorial: Reactive high power impulse magnetron sputtering (R-HiPIMS) | 153 | 104 | 49 | 68.0% |
80s8d996 | Physics of arcing, and implications to sputter deposition | 148 | 22 | 126 | 14.9% |
7fs202d9 | Mechanical and Thermal Analysis of an HTS Superconducting Magnet for an Achromatic Gantry for Proton Therapy | 102 | 20 | 82 | 19.6% |
2mk960ks | Broadband impedance modeling and single bunch instabilities estimations of the advanced light source upgrade project | 99 | 8 | 91 | 8.1% |
6q91s5fx | An IFU View of the Active Galactic Nuclei in MaNGA Galaxy Pairs | 99 | 9 | 90 | 9.1% |
48r7d71q | Off-harmonic optical probing of high intensity laser plasma expansion dynamics in solid density hydrogen jets | 92 | 4 | 88 | 4.3% |
1k79p6pk | Formation of diamonds in laser-compressed hydrocarbons at planetary interior conditions | 91 | 69 | 22 | 75.8% |
5sz6k69h | Charged particle motion and radiation in strong electromagnetic fields | 90 | 25 | 65 | 27.8% |
7215p48m | Beam delivery and final focus systems for multi-TeV advanced linear colliders | 90 | 2 | 88 | 2.2% |
7nk4t123 | DFBX boxes -- electrical and cryogenic distribution boxes for the superconducting magnets in the LHC straight sections | 88 | 2 | 86 | 2.3% |
5zf03001 | Acceleration of electrons in the plasma wakefield of a proton bunch | 82 | 2 | 80 | 2.4% |
5q63r9ph | Pushing the Frontier in the Design of Laser-Based Electron Accelerators with Groundbreaking Mesh-Refined Particle-In-Cell Simulations on Exascale-Class Supercomputers | 81 | 33 | 48 | 40.7% |
7dj1d5sr | Design of the Superconducting Magnet System for a 45 GHz ECR Ion Source | 80 | 6 | 74 | 7.5% |
41f3q1m5 | Investigation of light ion fusion reactions with plasma discharges (II) | 79 | 3 | 76 | 3.8% |
7x86q4vk | A new quench detection method for HTS magnets: stray-capacitance change monitoring | 79 | 3 | 76 | 3.8% |
9kx0g1fb | Filling in the Roadmap for Self-Consistent Electron Cloud and Gas Modeling | 79 | 7 | 72 | 8.9% |
2b53f897 | HiPACE++: A portable, 3D quasi-static particle-in-cell code | 77 | 14 | 63 | 18.2% |
8738n203 | Simulation of space-charge effects using a quantum Schrödinger approach | 77 | 2 | 75 | 2.6% |
89c1q3cb | Multiple colliding laser pulses as a basis for studying high-field high-energy physics | 77 | 7 | 70 | 9.1% |
0kg7g1v9 | Obtaining attosecond X-ray pulses using a self-amplified spontaneous emission free electron laser | 75 | 2 | 73 | 2.7% |
92t419x8 | Radial density profile and stability of capillary discharge plasma waveguides of lengths up to 40 cm | 74 | 4 | 70 | 5.4% |
40f4888d | Characterization of pseudosingle bunch kick-and-cancel operational mode | 73 | 1 | 72 | 1.4% |
4d484805 | Superconducting Magnets for Particle Accelerators | 71 | 8 | 63 | 11.3% |
8pz9p43n | High Intensity, Pulsed, D-D Neutron Generator | 71 | 5 | 66 | 7.0% |
1f59p4q1 | Advances in numerical methods under wiggler period averaging for free electron laser simulation | 69 | 0 | 69 | 0.0% |
3m46m1fw | High-throughput homogenization of a quasi-Gaussian ultrafast laser beam using a combined refractive beam shaper and spatial light modulator | 67 | 34 | 33 | 50.7% |
4n16r221 | Energetic Electron-Assisted Synthesis of Tailored Magnetite (Fe3O4) and Maghemite (γ−Fe2O3) Nanoparticles: Structure and Magnetic Properties | 62 | 48 | 14 | 77.4% |
3bn193b1 | The science case for an intermediate energy advanced and novel accelerator linear collider facility | 56 | 34 | 22 | 60.7% |
7xn8533z | Superconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR | 53 | 22 | 31 | 41.5% |
84k974r2 | Plasma-based ion implantation and deposition: A review of physics, technology, and applications | 53 | 18 | 35 | 34.0% |
0w17c8fn | The BErkeley Lab Laser Accelerator (BELLA): A 10 GeV Laser Plasma Accelerator | 51 | 13 | 38 | 25.5% |
5nt2c3rf | Engineering current density over 5 kA mm−2 at 4.2 K, 14 T in thick film REBCO tapes | 51 | 33 | 18 | 64.7% |
5vq8x5js | A viable dipole magnet concept with REBCO CORC® wires and further development needs for high-field magnet applications | 50 | 28 | 22 | 56.0% |
7m2390f3 | Challenges and Lessons Learned From Fabrication, Testing, and Analysis of Eight MQXFA Low Beta Quadrupole Magnets for HL-LHC | 50 | 28 | 22 | 56.0% |
560579fw | Studies in Optimal Configuration of the LTP | 48 | 4 | 44 | 8.3% |
8bp1p31b | The WARP Code: Modeling High Intensity Ion Beams | 48 | 4 | 44 | 8.3% |
8wh413h5 | Design of a High Toughness Epoxy for Superconducting Magnets and Its Key Properties | 47 | 32 | 15 | 68.1% |
7c8279qx | QubiC: An open source FPGA-based control and measurement system for superconducting quantum information processors | 46 | 4 | 42 | 8.7% |
538805vh | Diagnostics, Control and Performance Parameters for the BELLA High Repetition Rate Petawatt Class Laser | 45 | 27 | 18 | 60.0% |
7cz4g23b | Deposition Rates of High Power Impulse Magnetron Sputtering: Physics and Economics | 45 | 15 | 30 | 33.3% |
1n1690zv | Progress on HL-LHC Nb<sub>3</sub>Sn Magnets | 43 | 17 | 26 | 39.5% |
6qj90586 | Thermoeconomic cost optimization of superconducting magnets for proton therapy gantries | 42 | 24 | 18 | 57.1% |
7n41725b | Discharge Physics of High Power Impulse Magnetron Sputtering | 42 | 16 | 26 | 38.1% |
9zp8p7nm | FCC-hh: The Hadron Collider | 42 | 24 | 18 | 57.1% |
0947k7gj | Generation of high-quality electron beams from a laser-based advanced accelerator | 41 | 34 | 7 | 82.9% |
1xp428p2 | HE-LHC: The High-Energy Large Hadron Collider | 41 | 21 | 20 | 51.2% |
7kb4v6dr | An Electric-Circuit Model on the Inter-Tape Contact Resistance and Current Sharing for REBCO Cable and Magnet Applications | 41 | 32 | 9 | 78.0% |
7q7732kp | Quench protection for high-temperature superconductor cables using active control of current distribution | 41 | 19 | 22 | 46.3% |
Note: Due to the evolving nature of web traffic, the data presented here should be considered approximate and subject to revision. Learn more.