Status of the SOLEIL femtosecond X-ray source

http://accelconf.web.cern.ch/AccelConf/FEL2012/papers/wepd04.pdfInternational audienceAn electron bunch slicing setup is presently under construction on the SOLEIL storage ring for delivering 100 fs (rms) long photon pulses to two undulator-based beamlines providing soft (TEMPO) and hard X-rays (CRISTAL). Thanks to the non-zero dispersion function present in all straight sections of the storage ring, the sliced bunches can be easily separated from the core bunches. The modulator is a wiggler composed of 20 periods of 164.4 mm. It produces a magnetic field of 1.8 T at a minimum gap of 14.5 mm. To modulate the kinetic energy of the electrons in the wiggler, a Ti:Sa laser will be used, which produces 50 fs pulses at 800 nm with a repetition rate of 2.5 kHz. The laser beam is splitted into two branches in order to provide 2 mJ to the modulator and 0.5 mJ as pump pulse for the CRISTAL and TEMPO end stations. Focusing optics and beam path, from the laser hutch to the inside of the storage ring tunnel are presently under finalization. In this paper, we will report on the specificities of the SOLEIL setup, the status of its installation and the expected performances

A NEW SCHEME FOR ELECTRO-OPTIC SAMPLING AT RECORD REPETITION RATES: PRINCIPLE AND APPLICATION TO THE FIRST (TURN-BY-TURN) RECORDINGS OF THz CSR BURSTS AT SOLEIL

Abstract The microbunching instability is an ubiquitous problem in storage rings at high current density. However, the involved fast time-scales hampered the possibility to make direct real-time recordings of theses structures. When the structures occur at a cm scale, recent works at UVSOR [1], revealed that direct recording of the coherent synchrotron radiation (CSR) electric field with ultra-high speed electronics (17 ps) provides extremely precious informations on the microbunching dynamics. However, when CSR occurs at THz frequencies (and is thus out of reach of electronics), the problem remained largely open. Here we present a new opto-electronic strategy that enabled to record series of successive electric field pulses shapes with picosecond resolution (including carrier and envelope), every 12 ns, over a total duration of several milliseconds. We also present the first experimental results obtained with this method at Synchrotron SOLEIL, above the microbunching instability threshold. The method can be applied to the detection of ps electric fields in other situations where high repetition rate is also an issue

High repetition-rate electro-optic sampling: Recent studies using photonic time-stretch

Single-shot electro-optic sampling (EOS) is a powerful characterization tool for monitoring the shape of electron bunches, and coherent synchrotron radiation pulses. For reaching high acquisition rates, an efficient possibility consists to associate classic EOS systems with the so-called photonic time-stretch technique [1]. We present recent results obtained at SOLEIL and ANKA using this strategy. In particular, we show how a high sensitivity variant of photonic time stretch [2] EOS enabled to monitor the CSR pulses emitted by short electron bunches at SOLEIL [3]. We could thus confirm in a very direct way the theories predicting an interplay between two physical processes. Below a critical bunch charge, we observe a train of identical THz pulses stemming from the shortness of the electron bunches. Above this threshold, CSR emission is dominated by drifting structures appearing through spontaneous self-organization. We also consider the association of time-stretch and EOS for recording electron bunch near fields at high repetition rate. We present preliminary results obtained at ANKA, aiming at recording the electron bunch shape evolution during the microbunching instability

High-resolution spectroscopy and analysis of the ν3, ν4 and 2ν4 bands of SiF4 in natural isotopic abundance

International audienceSilicon tetrafluoride (SiF4) is a trace component of volcanic gases. However, a better knowledge of spectroscopic parameters is needed for this molecule in order to derive accurate concentrations. This motivated FTIR measurements with high-spectral resolution (0.001 cm-1) and an extensive study of its infrared absorption bands, including the fundamentals and overtone and combinations. We present here a detailed analysis and modeling of the strongly absorbing ν3and ν4 fundamental bands, for the three isotopologues in natural abundance: 28SiF4 (92.23 %), 29SiF4 (4.67 %) and 30SiF4 (3.10 %). It includes a global fit with consistent parameter sets for the ground and excited states. In particular, all existing rotational line data have been included. The 2ν4 band of 28SiF4 could also be analyzed in detail. A first fit of the dipole moment derivative for the ν3 band for 28SiF4 has been performed, along with two independent estimates of the integrated band intensity; the results are consistent with literature values, around 690 km/mol. The isotopic dependence of band centers and Coriolis parameters has also been studied. TFSiCaSDa, a new database of cross sections and calculated lines for the ν3 band of SiF4, has been set up

Analysis of high-resolution spectra of SiF4 combination bands

International audienceThe infrared spectra of the silicon tetrafluoride molecule (SiF4) recorded on the AILES Beamline of the SOLEIL Synchrotron facility, have been studied in the range where the combination bands ν1+ν3, ν1+ν4, ν2+ν3 and ν2+ν4 are located. For each band, between 1100 and more than 2300 lines have been assigned and fitted with the effective Hamiltonian model for J values up to 55 (up to 82 for ν1+ν3). The obtained set of spectroscopic parameters allows one to reproduce experimentally obtained line positions with a root mean square deviation better than drms = 0.863 × 10−3 cm−1

Comment on the paper ;NDSD-1000: High-resolution, high-temperature nitrogen dioxide spectroscopic Databank; by A.A. Lukashevskaya, N.N. Lavrentieva, A.C. Dudaryonok, V.I. Perevalov, J Quant Spectrosc Radiat Transfer 2016;184:205-17

International audienceA recent paper [1] presents a high-resolution, high-temperature version of the Nitrogen Dioxide Spectroscopic Databank called NDSD-1000. The NDSD-1000 database contains line parameters (positions, intensities, self- and air-broadening coefficients, exponents of the temperature dependence of self- and air-broadening coefficients) for numerous cold and hot bands of the 14N16O2 isotopomer of nitrogen dioxide. The parameters used for the line positions and intensities calculation were generated through a global modeling of experimental data collected in the literature within the framework of the method of effective operators. However, the form of the effective dipole moment operator used to compute the NO2 line intensities in the NDSD-1000 database differs from the classical one used for line intensities calculation in the NO2 infrared literature [12]. Using Fourier transform spectra recorded at high resolution in the 6.3 μm region, it is shown here, that the NDSD-1000 formulation is incorrect since the computed intensities do not account properly for the (Int(+)/Int(-)) intensity ratio between the (+) (J = N+ 1/2) and (-) (J = N-1/2) electron - spin rotation subcomponents of the computed vibration rotation transitions. On the other hand, in the HITRAN or GEISA spectroscopic databases, the NO2 line intensities were computed using the classical theoretical approach, and it is shown here that these data lead to a significant better agreement between the observed and calculated spectra

Etude par spectroscopie vibrationnelle de la solvatation de l'eau par des bases organiques en matrices

L'analyse des spectres vibrationnels de matrices d'argon ou d'azote doublement dopées en eau et acétonitrile (B) a permis l'identification de quatre types de complexes : un complexe 1:1, HOH. . .B, caractérisé par des fréquences de H2O proches de celles mesurées lorsque B = OH2 ou O ((CH3)2 ; un complexe 1 : 2 de structure HOH. . .B2 caractérisé par des fréquences de H2O proches de celles obtenues pour le complexe 1 : 1 ; un complexe 1 : n, n > 2, de structure Bi. . . HOH. . . Bj, i ou j étant nécessairement plus grand que 1, dans lequel les fréquences de H2O se rapprochent de celles mesurées pour l'agrégat 1 : 2 lorsque B = O ((CH3)2 ; enfin un complexe 2 : 1 dans lequel une molécule d'acétonitrile se fixe sur un dimere d'eau selon l'enchaînement HOH. . .OH. . .B. Ces résultats sont compares a ceux obtenus a l'etat liquide en solution binaire ou ternaire

High-Resolution spectroscopy and analysis of the fundamental modes of 28 Si F 4 . Accurate experimental determination of the Si − F bond length

International audienceSilicon tetrafluoride (SiF 4) is a trace component of volcanic gases and is gaining industrial importance. However, a better knowledge of spectroscopic parameters is needed for this molecule in order to derive accurate concentrations. Following a previous reinvestigation of the ν 3 and ν 4 fundamentals [J. Quant. Spectrosc. Radiat. Transfer 260 (2021) 107474], we have undertaken an extensive high-resolution study of its infrared absorption bands. We present here an update of this study. It features the recording of new far-infrared spectra, taking advantage of synchrotron radiation, and a global fit giving a consistent parameter set for the ground and fundamental states of 28 SiF 4 , now including the v 1 = 1 and v 2 = 1 states, by adding to the global analysis the newly measured ν 2 , ν 1 − ν 4 , and ν 4 − ν 2 bands near 264, 412, and 125 cm −1 , respectively. Nearly 20 000 assigned lines pertaining to seven distinct rovibrational bands were fitted with an excellent accuracy (global standard deviation of 0.296). This allows us to obtain an accurate experimental value for the Si−F bond length, r e (SiF 4) = 1.5516985(30)Å. Some new band intensity estimates allow us to update our SiF 4 calculated spectroscopic database