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Generation of ultrashort light pulses Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg

Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

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Page 1: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Generation of ultrashort light pulses

Adriana Pálffy-Buß

Max-Planck-Institut für Kernphysik, Heidelberg

Page 2: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Visualising fast processes

1877 - galloping horse ms resolution

Shutter controls exposure/illumination time

Short time scales – ultrashort light pulses

Page 3: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Time scales

Age of the universe14 Billion years1 second Shortest pulse

ever generated - 67 as

Human/biological time scale

geological/astronomicaltime scale

CamerasLaser pulses

Nuclear time scale

Electronic timescale

Molecular timescale

Page 4: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Historical development

1960, T. MaimanFirst laser – short pulses

1991, W. Sibbett Kerr-lense mode locking: few fs

1961 Q-Switching – ns pulses

1964 Mode locking: ps to fs pulses

„few-cycle pulse“

Limitation - 1 cycle @ 800 nm – 2.7 fs

Page 5: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Attosecond pulses

Require higher frequencies – XUV, X-ray!

1987 – 1988 – ''High harmonic generation'' - HHG

fs laser pulse

atomic mediumnoble gas

as pulse

Experiment/Detector

Intensity > 10¹ W/cm²⁴

M. Ferray, A. L’Huillier et al. J. Phys. B 21, L31 (1988)

Page 6: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Mechanism

Semiclassical: „3-Step-Model“

P. Corkum, Phys. Rev. Lett. 71, 1994 (1993)

Phase relation between the optical fs pulse and the as pulse!

Page 7: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Why high harmonics?

Classical trajectories starting close to phase 0

Laser phase

Ele

ctro

n po

sitio

n

Lase

r fie

ld

„short“ and „long“ trajectories with the same energy

„Cutoff“-trajectory with maximal energy

Page 8: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Why high harmonics?

Classical trajectories starting close to phase 0

Laser phase

Ele

ctro

n po

sitio

n

Lase

r fie

ld

Next field max/min are starting point for further trajectories

In symmetrical atoms and fields this leads to identical recollision energies!

Superposition at detector:

only odd multiples of laser frequency „High harmonics“

Page 9: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

HHG

„high harmonic generation“

Energy

Inte

nsity

M. Ferray, A. L’Huillier et al. J. Phys. B 21, L31 (1988)

„cutoff“-Energy

@Plateau, Fourier limit

perturbative regime Not yet HHG!

Page 10: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Scattering of the wave packet – 10 ³ geometrical conversion factor in 2D⁻

Realization

Many atoms instead of one - „Phase Matching“

→ index of refraction

Generation of a single as pulse

ionizes!

3,3 fs, 720 nm

Conversion factor 10⁻⁶

80 eV, < 100 as

E. Goulielmakis et al., Science 320, 1614 (2008)

Pulse duration record 67 as K. Zhao et al., Opt. Lett. 37, 3891 (2012)

Photon energy record 1.6 keV T. Popmintchev et al., Science 336, 1287 (2012)

Requires same transit time for optical and HHG pulse!

Page 11: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Application example

streaking

„Streaking“ - visualizing a fs pulse

Ionization on the as time scale

E. Goulielmakis, Science 305, 1267 (2004)

Page 12: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping

Summary

sub-fs pulses, as short as 67 as

10 eV – 1.6 keV

Semiclassical trajectories„3-Step“-Model

Generation of ultrashort laser pulses for observation of fast electron dynamics

HHG- High Harmonic Generation

Energy

Inte

nsi

ty

Exciting applications

Attosecond pulses, Agostini & DiMauro, Rep. Prog. Phys. 67, 813 (2004) Attosecond physics, Krausz & Ivanov, Rev. Mod. Phys. 81, 163 (2009) HHG, Kohler et al., Adv. At. Mol. Opt. Phys. 61, 159 (2012)

Page 13: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping
Page 14: Adriana Pálffy-Buß Max-Planck-Institut für Kernphysik, Heidelberg · 2015-07-17 · Max-Planck-Institut für Kernphysik, Heidelberg. Visualising fast processes 1877 - galloping