bubble acceleration with few-cycle pulses
DESCRIPTION
Max-Planck-Institut für Quantenoptik. Bubble Acceleration with few-cycle pulses. Michael Geissler, Jörg Schreiber , Florian Grüner and Jürgen Meyer-ter-Vehn. Outline. 3D-PIC Simulations of: few cycle pulses: Scaling Density Profile Closer look on “bubble-electrons” - PowerPoint PPT PresentationTRANSCRIPT
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Bubble Acceleration with few-cycle
pulses
Max-Planck-Institut für Quantenoptik
Michael Geissler, Jörg Schreiber, Florian Grüner
and Jürgen Meyer-ter-Vehn
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Outline
3D-PIC Simulations of:
few cycle pulses:
•Scaling
•Density Profile
•Closer look on “bubble-
electrons”
Experiments (Rutherford, Jena,
MPQ…)
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3D-PIC Code for Ideal Laser Matter Interaction:
ILLUMINATION ILLUMINATION
Numerical Tool
Laser Pulse
y
x – Laser Polarization z – Propagation direction
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5fs, a=5, w0=5µm, p=8µm
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5fs, a=5
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5fs, a=5, 70MeV e-
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5fs, a=5, 60-80MeV e-
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5fs, a=5, 60-80MeV e-
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5fs, a=5, 60-80MeV e-
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a=3
a=5
a=10
a=30
5fs, w0=5µm, p=8µm
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5fs Summary
a=3 a=5 a=10 a=30
Epeak (80MeV) 80MeV 130MeV 310MeV
Lmax 300µm 220µm 250µm 500µm
Ezmax 0.5TV/m 1.1TV/m 1.6TV/m 2.3TV/m
ne,peak Etot,pea
k
1.2x109
14mJ3.8x109
75mJ24x109
1300mJ
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5fs Scaling
125.025.0max ; IaRE Bubblez
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5fs, a=5
with Gas denstity profile:
N0
z200µm 200µm
Focus position
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5fs, a=5, p=8µm, profile
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MPQ: 5fs, a=5, w0=2µm; 20mJ
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RAL: 40fs, a=0.767, 390mJ
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z [µm]
z [µm] z [µm]
Ez [1012V/m]
Ne [10201/cm³] Intensity [1019 W/cm²]
RAL: 40fs, a=0.767, 390mJ
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Jena: 80fs, a=3
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80fs, a=3
Ne [10201/cm³]
I [1019W/cm²]
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Conclusions Few-cycle pulses are most efficent for bubble acceleration (longer pulses become few-cycle during propagation)
Acceleration is limited due:
•Rb=w0*a0.25 ~Eacc
•Short lifetime of the bubble (~200-400µm)
Precise control of gas density and length is necessary
Multistages:
Use a small amount (20-100mJ) in the first stage, but what afterwards?
Wakefield? second bubble? How to inject the electron?
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40fs, a=3