Few-cycle pulse generation by double-stage hybrid multi-pass multi-plate nonlinear pulse compression Anne-Lise Viotti12 Chen Li1 Gunnar Arisholm3 Lutz Winkelmann1 Ingmar Hartl1 Christoph M. Heyl145 and

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Few-cycle pulse generation by double-stage hybrid multi-pass multi-plate nonlinear
pulse compression
Anne-Lise Viotti1,2, Chen Li1, Gunnar Arisholm3, Lutz Winkelmann1, Ingmar Hartl1, Christoph M. Heyl1,4,5, and
Marcus Seidel1,*
1Deutsches Elektronen-Synchrotron DESY, Notkestr. 85, 22607 Hamburg, Germany
2Department of Physics, Lund University, P.O. Box 118, SE-221 00 Lund, Sweden
3FFI (Norwegian Defence Research Establishment), P. O. Box 25, NO-2027 Kjeller, Norway
4Helmholtz-Institute Jena, Fröbelstieg 3,07743 Jena, Germany
5GSI Helmholtzzentrum für Schwerionenforschnung GmbH, Planckstrasse 1, 64291 Darmstadt, Germany
*Corresponding author: marcus.seidel@desy.de
Abstract
Few-cycle pulses present an essential tool to track ultrafast dynamics in matter and drive strong field effects. To
address photon-hungry applications, high average power lasers are used which, however, cannot directly provide
sub-100 fs pulse durations. Post-compression of laser pulses by spectral broadening and dispersion compensation is
the most efficient method to overcome this limitation. Here, we demonstrate a notably compact setup which turns a
0.1 GW peak power, picosecond laser into a 2.9 GW peak power, 8.2 fs source. The 120-fold pulse duration shortening
is accomplished in a two-stage hybrid multi-pass, multi-plate compression setup. To our knowledge, neither shorter
pulses, nor higher peak powers have been reported to-date from bulk multi-pass cells alone, manifesting the power of the
hybrid approach. It puts, for instance, compact, cost-efficient and high repetition rate attosecond sources within reach.
Few-cycle pulses have pushed the frontiers of nonlinear
optics far beyond the perturbative regime. The (tempo-
rary) detachment of weakly bound electrons from the nu-
clei by strong fields leads to the creation of large electric
dipole moments [1]. The atomic polarization is switched
by few-cycle pulses on sub-femtosecond timescales with-
out prior distortions of the interacting matter [1]. Many
unique applications emerged, most prominent, the gener-
ation of coherent extreme ultraviolet or X-ray radiation
and its temporal confinement to attosecond durations [2].
This, in turn, enabled tracking of ionization dynamics and
performing electron microscopy with highest temporal and
spatial resolution [3, 4]. Beyond that, few-cycle pulses
prospectively enable PHz bandwidth signal processing in
semiconductors, dielectrics and novel quantum materials
[5, 6]. Initial few-cycle sources relied on broadband laser
gain media that are difficult to scale in average power
[1]. However, high pulse repetition rates are important to
achieve good signal-to-noise ratios despite the low efficien-
cies of extremely nonlinear processes or limitations caused
by Coulomb interactions after ionization [4]. The advance-
ment of ultrafast lasers in the past years to substantially
higher average powers [7], has allowed to overcome the rep-
etition rate short-coming of few-cycle sources, but has also
imposed the challenge to reduce the inherent pulse dura-
tions of power-scalable lasers from hundreds or thousands
of femtoseconds to the sub-10 fs regime. One approach to
accomplish this is optical parametric chirped pulse ampli-
fication [8]. It provides wavelength tunability and excel-
lent pulse contrast but is a relatively inefficient, complex
method. Alternatively, nonlinear spectral broadening and
pulse post-compression present a direct, cost-efficient path
to the few-cycle regime [9]. In particular, the multi-pass
cell (MPC) spectral broadening technique has combined
large pulse compression factors, i.e. the input to output
pulse duration ratios, and high power efficiencies in an out-
standing manner [10, 11, 12]. Recently, several few-cycle
pulse generation schemes by means of MPCs have been re-
ported [13, 14, 15, 16, 17]. However, all experiments were
based on gas-filled MPCs which require hundreds of µJ of
pulse energies as well as a chamber that needs to be evac-
uated and refilled with up to several bars of nonlinear gas.
In contrast, bulk material based few-cycle or even single-
cycle pulse generation was demonstrated in the past years
by the multiple plate continuum approach [18, 19, 20]. We
have recently shown that combining the multiple plate and
the bulk MPC techniques can clearly overcome the com-
pression factors that are achievable by the methods alone
in a single stage [21, 22]. Here, we apply this novel hybrid
approach to demonstrate more than hundred times dura-
tion reduction of powerful ultrashort pulses, that is from
the picosecond regime to 8.2 fs FWHM duration. More-
over, we report the first bulk-based MPC that delivers
sub-10 fs pulses with multi-GW peak powers.
The compression setup was based on an Yb:YAG laser
and two spectral broadening stages (Fig. 1a). The laser
and the first MPC stage (MPC 1) were similar to the setup
reported in ref. [21]. The front-end of the amplifier was
improved, which led to 15 % more pulse energy than in
[21] and pulses with down to 1 ps FWHM duration. The
amplifier emitted laser bursts every 100 ms with a variable
number of pulses and a 1 MHz pulse repetition rate. We
adjusted the number of pulses to the dynamic range of
our measurement devices and typically worked with 150
- 200 pulses per burst. MPC 1 consisted of two quarter-
wave stack dielectric mirrors with 200 mm radius of curva-
ture (ROC) and five 1 mm thin anti-reflection coated silica
substrates. The sixth plate used in ref. [21] mainly intro-
duced additional chirp without lowering decisively the 43 fs
Fourier transform limit (FTL) of the MPC 1 output spec-
trum (Fig. 2, blue line). After 68 reflections from chirped
mirrors with -200 fs2group delay dispersion (GDD), the
1
arXiv:2210.11619v1 [physics.optics] 20 Oct 2022
摘要:

Few-cyclepulsegenerationbydouble-stagehybridmulti-passmulti-platenonlinearpulsecompressionAnne-LiseViotti1,2,ChenLi1,GunnarArisholm3,LutzWinkelmann1,IngmarHartl1,ChristophM.Heyl1,4,5,andMarcusSeidel1,*1DeutschesElektronen-SynchrotronDESY,Notkestr.85,22607Hamburg,Germany2DepartmentofPhysics,LundUnive...

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