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| 001 | 622631 | ||
| 005 | 20250715171500.0 | ||
| 020 | _ | _ | |a 979-8-3503-7032-4 |
| 024 | 7 | _ | |a 10.1109/IRMMW-THz60956.2024.10697916 |2 doi |
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| 100 | 1 | _ | |a Bazrafshan, Reza |0 P:(DE-H253)PIP1092237 |b 0 |e First author |
| 111 | 2 | _ | |a 2024 49th International Conference on Infrared, Millimeter, and Terahertz Waves (IRMMW-THz) |c Perth |d 2024-09-01 - 2024-09-06 |w Australia |
| 245 | _ | _ | |a Powering a THz gun: Optimizing THz Generation, Transportation and Coupling |
| 260 | _ | _ | |a [Piscataway, NJ] |c 2024 |b IEEE |
| 295 | 1 | 0 | |a [Ebook] 2024 49th International Conference on Infrared, Millimeter, and Terahertz Waves : 1st-6th September 2024 : Perth, Australia, the University Club of the University of Western Australia / IRMMW-THz, the University of Western Australia, Western Australia, Business Events Perth , [Piscataway, NJ] : IEEE, 2024, |
| 300 | _ | _ | |a 3 |
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| 500 | _ | _ | |a Literaturangaben; |
| 520 | _ | _ | |a Scaling the RF-accelerator concept to terahertz (THz) frequencies possesses several compelling advantages including compactness and intrinsic timing between the photoemission and driving field sources. However, the 2-orders-of-magnitude reduction in scale, brings new challenges in constructing and characterizing accelerator devices. A key factor is optimization of the transport of THz energy from the nonlinear optical source to the interaction point, low efficiencies of which can severely limit device performance. Here we report on the development of an electron gun pumped transversely by twin 120 µJ single-cycle THz pulses predicted to produce 100 fC electron bunches with 100 keV energy and a bunch duration of 20-40 fs |
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| 700 | 1 | _ | |a Zhang, Junhao |0 P:(DE-H253)PIP1104992 |b 1 |
| 700 | 1 | _ | |a Kroh, Tobias |0 P:(DE-H253)PIP1028053 |b 2 |
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| 700 | 1 | _ | |a Matlis, Nicholas |0 P:(DE-H253)PIP1026174 |b 8 |
| 700 | 1 | _ | |a Kärtner, Franz |0 P:(DE-H253)PIP1013198 |b 9 |e Corresponding author |
| 773 | _ | _ | |a 10.1109/IRMMW-THz60956.2024.10697916 |
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