% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@INPROCEEDINGS{Ferrari:622552,
author = {Ferrari, Eugenio},
title = {{T}win {E}cho-{E}nabled {H}armonic {G}eneration for
{E}nhanced {C}oherent {B}unching at {S}hort {W}avelength},
reportid = {PUBDB-2025-00389},
year = {2025},
abstract = {We present a novel externally seeded cascaded free-electron
laser (FEL) scheme based on two echo-enabled har-monic
generation stages to obtaining unprecedented bunching
independently on the final FEL wavelength.Externally seeded
free-electron lasers (FELs) based on harmonic up-conversion
schemes represent the mostsuccessful approach for obtaining
radiation with laser-like properties at short wavelengths.
They are howeverlimited in the shortest achievable
wavelengths, as the harmonic conversion efficiency decreases
with increasingharmonic number, even for echo-enabled
harmonic generation (EEHG) [1]. Higher bunching is critical
to improvethe performance of seeded FELs in the soft X-rays,
with large output power and more compact footprint. We
analyze the performance at 4 nm and shorter via numerical
simulations, demonstrating multi-GW level, fully
coherentpulses with laser-like properties, paving the way
for externally seeded radiation at 1 nm and beyond.The setup
is schematically reported in Fig.1(a). The first dispersive
section (DS1) smears the energy modulationgenerated in MOD1
by seed 1 creating stripes in the longitudinal phase space
(LPS) of the e-beam. The seconddispersive section (DS2) is
tuned to maximize the bunching at the required intermediate
wavelength, emitted by thefirst radiator (RAD1) to produce
the seed for the subsequent stage (seed 3) towards the tail
of the bunch, leavingenough space for the fresh bunch
approach [2]. The second stage is used to remodulate the
same e-beam withamplitude A3, in a fresh region where the
interaction of seed 2 in ECHO-1 did not take place. The
energy stripesgenerated by seed 1 in MOD1 and smeared in DS1
are still present thanks to the long pulse duration of seed
1.By proper tuning of the third dispersive section (DS3) an
unprecedented amount of bunching is optimized at thefinal
wavelength, emitted by the main radiator (RAD2). While
conventionally the cascaded approach relies onthe second
stage operated in up-conversion (i.e., shorter wavelengths),
the proposed scheme can operate both inup- and
down-conversion, going towards (slightly) longer
wavelengths. This gives best performance in terms ofminimum
required seed 3 power (nJ-level) and maximum achievable
bunching. An example of LPS for one e-beamslice, before and
after interaction in ECHO-2 is reported in Fig.1(b-e). The
predicted bunching at 4 nm is $28.7\%,an$ unprecedented
level at soft-X-rays for an externally seeded FEL, as one
can see from Fig.1(f, g).References[1] G. Stupakov.,
“Using the Beam-Echo Effect for Generation of
Short-Wavelength Radiation”, Phys. Rev. Lett., 102,
074801, (2009).[2] L. H. Yu and I. Ben-Zvi, “High-gain
harmonic generation of soft X-rays with the “fresh
bunch” technique”, Nuclear Inst. and Methods inPhysics
Research, A, 393, (1) 96–99, (1997)},
month = {Jun},
date = {2025-06-23},
organization = {European Conference on Lasers and
Electro-Optics, Munich (Germany), 23
Jun 2025 - 27 Jun 2025},
cin = {MPY},
cid = {I:(DE-H253)MPY-20120731},
pnm = {621 - Accelerator Research and Development (POF4-621)},
pid = {G:(DE-HGF)POF4-621},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)1},
url = {https://bib-pubdb1.desy.de/record/622552},
}