Paper | Title | Page |
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MOOCB2 |
Modeling Underdense Plasma Photocathode Experiments | |
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Funding: Work supported by DOE under Contract Nos. DE-SC0009533, DE-FG02-07ER46272 and DE-FG03-92ER40693, and by ONR under Contract No. N00014-06-1-0925. NERSC computing resources are supported by DOE. The underdense plasma photocathode concept (aka Trojan horse) *,** is a promising approach to achieving fs-scale electron bunches with pC-scale charge and transverse normalized emittance below 0.01 mm-mrad, yielding peak currents of order 100 A and beam brightness as high as 1019 A/(m rad)2, for a wide range of achievable beam energies up to 10 GeV. A proof-of-principle experiment will be conducted at the FACET user facility in early 2014. We present 2D and 3D simulations with physical parameters relevant to the planned experiment. * Hidding et al., PRL 108:035001 (2012). ** Xi et al., PRST-AB 16:031303 (2013). |
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Slides MOOCB2 [3.913 MB] | |
MOPBA17 | A User Friendly, Modular Simulation Tool for Laser-Electron Beam Interactions | 213 |
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Funding: This work is supported by U.S. D.O.E. Contract number DE-SC0006287 Many advanced accelerator concepts require the co-propagation and interaction of the electron with a laser (e.g., laser-plasma accelerators, inverse Compton scattering, laser heaters, and electron beam diagnostics with laser light). The strict requirements on beam properties necessitate numerical modeling to fully understand the complexities of the beam dynamics. Laser-specific simulations often require a different set of modeling tools. This has resulted in a hodgepodge approach, where the output of one program must be inputted into another. This paper presents the Radtrack software highlights, which aims to simplify these issues by uniting key software components under an intuitive graphical interface while addressing key problems relevant in the accelerator community. |
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MOPHO25 | Removal of Residual Chirp in Compressed Beams Using a Passive Wakefield Technique | 291 |
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Funding: This is experiment is supported by an ongoing DOE Phase I Small Business Initiative for Research (SBIR) Grant, number DE–-SC0009550. The removal of residual chirp in XFELs is of paramount importance for efficient lasing. Although current S-band XFELs remove the unwanted residual chirp using off-crest acceleration after the final bunch compressor, this technique is not possible for XFELs with soft X-ray lines as there are no further accelerating structures. The off-crest dechirping technique is also expensive for future superconducting XFELs. In response, RadiaBeam Systems presents its work, building upon the theoretical work of Bane and Stupakov*, in RF-free residual chirp mitigation using only passive techniques. Beam-induced longitudinal wakefields are produced with opposing corrugated plates which allow for an entirely RF-free chirp removal. Theory, engineering, and experimental results are presented. * K.L.F. Bane, G. Stupakov, Nucl. Inst. Meth. 690 (2012) 106-110 |
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THPAC32 | Transverse Beam Profile Diagnostic Using Fiber Optic Array | 1205 |
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Funding: This work is supported by U.S. D.O.E Contract Number DE-SC0000870 The fiber-mesh diagnostic (FMD) is a transverse beam profile diagnostic based on the emission and detection of Cherenkov radiation produced as a relativistic electron beam traverses through an ordered bundle of fiber optics (SiO2), arranged in a hexagonal close-pack configuration. Sub-10μm transverse beam profile resolution is attainable due to fiber optic core concentricity. Adequate SNR is achieved using a standard CCD sensor. A fiber optic taper input maximizes light collection efficiency by coupling each output channel to approximately single-pixel pitch. A v-groove holder and assembly process was developed to hold many fiber layers in the desired configuration. In this paper, we present results from a fully functional FMD prototype evaluated at the BNL ATF facility that demonstrates the efficacy of this diagnostic. |
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THPAC37 | Surface Plasmon Resonance Enhanced Multiphoton Emission from Metallic Cathode | 1220 |
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We investigate the effect of surface plasmonic optical field enhancement on multiphoton emission from a metallic photocathode. In a previous experiment *, two orders of magnitude increase in charge yield was obtained using a slightly off resonance nanohole array plasmonic structure. In a new attempt, a nanohole structure will be fabricated, using focused ion beam milling, such that the resonance wavelength is at 800 nm, the central wavelength of the photoinjector driver laser pulse. The charge yield is expected to increase dramatically compared to the charge yield from previous nanostructure. We will also present optical characterization of the nanostructures as well the beam characteristics (intrinsic emittance and bunch length) from this nanostructured photocathode.
* Li et al., PRL 2013. |
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THPAC37 | Surface Plasmon Resonance Enhanced Multiphoton Emission from Metallic Cathode | 1220 |
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We investigate the effect of surface plasmonic optical field enhancement on multiphoton emission from a metallic photocathode. In a previous experiment *, two orders of magnitude increase in charge yield was obtained using a slightly off resonance nanohole array plasmonic structure. In a new attempt, a nanohole structure will be fabricated, using focused ion beam milling, such that the resonance wavelength is at 800 nm, the central wavelength of the photoinjector driver laser pulse. The charge yield is expected to increase dramatically compared to the charge yield from previous nanostructure. We will also present optical characterization of the nanostructures as well the beam characteristics (intrinsic emittance and bunch length) from this nanostructured photocathode.
* Li et al., PRL 2013. |
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