Abstract

Multiobjective genetic algorithm optimizations of a single-shot ultrafast electron diffraction beam line comprised of a $100\text{ }\text{ }\mathrm{MV}/\mathrm{m}$ 1.6-cell normal conducting rf (NCRF) gun, as well as a nine-cell $2\ensuremath{\pi}/3$ bunching cavity placed between two solenoids, have been performed. These include optimization of the normalized transverse emittance as a function of bunch charge, as well as optimization of the transverse coherence length as a function of the rms bunch length of the beam at the sample location for a fixed charge of $1{0}^{6}$ electrons. Analysis of the resulting solutions is discussed in terms of the relevant scaling laws, and a detailed description of one of the resulting solutions from the coherence length optimizations is given. For a charge of $1{0}^{6}$ electrons and final beam sizes of ${\ensuremath{\sigma}}_{x}\ensuremath{\ge}25\text{ }\text{ }\ensuremath{\mu}\mathrm{m}$ and ${\ensuremath{\sigma}}_{t}\ensuremath{\approx}5\text{ }\text{ }\mathrm{fs}$, we found a relative coherence length of ${L}_{c,x}/{\ensuremath{\sigma}}_{x}\ensuremath{\approx}0.07$ using direct optimization of the coherence length. Additionally, based on optimizations of the emittance as a function of final bunch length, we estimate the relative coherence length for bunch lengths of 30 and 100 fs to be roughly 0.1 and $0.2\text{ }\text{ }\mathrm{nm}/\ensuremath{\mu}\mathrm{m}$, respectively. Finally, using the scaling of the optimal emittance with bunch charge, for a charge of $1{0}^{5}$ electrons, we estimate relative coherence lengths of 0.3, 0.5, and $0.92\text{ }\text{ }\mathrm{nm}/\ensuremath{\mu}\mathrm{m}$ for final bunch lengths of 5, 30 and 100 fs, respectively.

Highlights

  • INTRODUCTIONThe desire for single-shot ultrafast electron diffraction (UED) beam lines with sufficient resolution (σt ≲ 30 fs, q ∼ 106 electrons) for use with biological samples, such as proteins, continues to push the development of both photocathode and cold atom electron sources [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17]

  • Building on the successful application of multiobjective genetic algorithm (MOGA) optimized simulations of space charge dominated beams used in the design and operation of the Cornell photoinjector [19,20,21], as well as the optimization of a cryocooled DC gun ultrafast electron diffraction (UED) setup [22], we apply the same techniques to a 100 MV=m 1.6-cell normal conducting rf guns (NCRF) gun followed by a nine-cell, 2π=3 buncher cavity

  • We make use of the same MOGA software used in previous work [19,20,22] in combination with the 3D space charge code general particle tracer (GPT)

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Summary

INTRODUCTION

The desire for single-shot ultrafast electron diffraction (UED) beam lines with sufficient resolution (σt ≲ 30 fs, q ∼ 106 electrons) for use with biological samples, such as proteins, continues to push the development of both photocathode and cold atom electron sources [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17]. Building on the successful application of multiobjective genetic algorithm (MOGA) optimized simulations of space charge dominated beams used in the design and operation of the Cornell photoinjector [19,20,21], as well as the optimization of a cryocooled DC gun UED setup [22], we apply the same techniques to a 100 MV=m 1.6-cell NCRF gun followed by a nine-cell, 2π=3 buncher cavity. The NCRF gun based UED setup in this work consists of a 1.6-cell 2.856 GHz NCRF gun followed by a buncher cavity placed between two solenoid magnets [24,25,26]. ; ð1Þ where ΔzÆ 1⁄4 z Æ L=2 and fit this model to solenoid field map data [22].

RESULTS
Optimal emittance
Optimal coherence length
Example solution
CONCLUSION
Full Text
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