
Research Article Optica 1
Spectral phase interferometry for direct electric-field
reconstruction of synchrotron radiation
TAKAO FUJI1,*, TATSUO KANEYASU2,3, MASAKI FUJIMOTO3, YASUAKI OKANO3, ELHAM SALEHI3,
MASAHITO HOSAKA4,5, YOSHIFUMI TAKASHIMA4, ATSUSHI MANO4, YASUMASA HIKOSAKA6, SHIN-ICHI
WADA7,AND MASAHIRO KATOH8,3,†
1Laser Science Laboratory, Toyota Technological Institute, Nagoya 468–8511, Japan
2SAGA Light Source, Tosu 841-0005, Japan
3Institute for Molecular Science, Okazaki 444-8585, Japan
4Synchrotron Radiation Research Center, Nagoya University, Nagoya, 464-0814, Japan
5National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230029, China
6Institute of Liberal Arts and Sciences, University of Toyama, Toyama 930-0194, Japan
7Graduate School of Advanced Science and Engineering, Hiroshima University, Higashi-Hiroshima 739-8526, Japan
8Hiroshima Synchrotron Radiation Center, Hiroshima University, Higashi-Hiroshima 739-0046, Japan
*Corresponding author: fuji@toyota-ti.ac.jp
†Corresponding author: mkatoh@hiroshima-u.ac.jp
Compiled October 14, 2022
Ultraviolet and extreme ultraviolet electric-fields produced by relativistic electrons in an undulator of a
synchrotron light source are characterized by using spectral phase interferometry for direct electric-field
reconstruction (SPIDER). A tandem undulator with a phase shifter produces a pair of wavelength shifted
wave packets with some delay. The interferogram between the pair of the wave packets is analyzed with
a SPIDER algorithm, which is widely used for ultrashort pulse characterization. As a result, a 10-cycle
square shaped electric-field is reconstructed. The waveform corresponds to the radiation from an electron
accelerated with the undulator which consists of 10 periods of permanent magnets. ©
2022 Optica Publishing
Group
http://dx.doi.org/10.1364/ao.XX.XXXXXX
1. INTRODUCTION
Synchrotron light sources have been developed for more than 70
years and currently ultrashort X-ray pulses are generated with
some free electron lasers (FELs) [
1
–
5
]. Characterization of the
pulses generated from such sources is very challenging due to
the short wavelength and the short pulse duration.
To characterize ultrashort pulses in the ultraviolet (UV) or
extreme ultraviolet (XUV) region, it is straightforward to mea-
sure the cross-correlation between the test and reference pulses.
However, it is very difficult to prepare a reference pulse for
synchrotron light sources. Several synchronization systems be-
tween an ultrashort pulse laser and a synchrotron light source
have been realized and used for the estimation of the duration
of the pulses from some FELs [
6
–
8
], however, it is always chal-
lenging to synchronize such very different light sources within
femtosecond timing jitter.
The waveform of the electric-field produced by an relativistic
electron in the undulator is basically defined by the number of
magnets and the gap between the magnets in the undulator. The
number of permanent magnets and the gap between the magnets
define the number of oscillations and the carrier wavelength of
the waveform respectively. In the UVSOR-III synchrotron light
source, there is a tandem undulator which can produce two
wave packets. The wavelength can be scanned from XUV to
visible region. By changing the gap between the permanent
magnets of each undulator, it is possible to change the wave-
length of each wave packet individually. A phase shifter, which
consists of three pairs of electromagnets and forms a small chi-
cane for the electron beam, between the undulators can control
the delay between the wave packets in femtosecond regime with
an attosecond accuracy. The system was applied for coherent
control of atoms and molecules [
9
–
11
]. It is important to char-
acterize the electric-field produced in the undulator for such
experiments.
We reported linear interferometric autocorrelation measure-
ments in the UV region for the spontaneous radiation from the
tandem undulator of UVSOR-III recently [
12
]. The shapes of the
measured autocorrelation traces were well reproduced by the
calculations assuming that the wave packet had the form of a
double-pulsed 10-cycle sinusoidal wave. However, the wave-
form of the wave packet cannot be directly reconstructed only
arXiv:2210.06652v1 [physics.optics] 13 Oct 2022