CITIUS Instrumentation
1. High-harmonic generation beamline
The CITIUS laboratory is equipped with a high-harmonic generation (HHG) beamline delivering extreme-ultraviolet pulses as short as 30 fs in the spectral range from 16 to 62 nm (20 to 80 eV) at a repetition rate of 5 kHz. The beamline consists of a generation chamber that contains a gas cell (typically filled with Ar or Ne) and a monochromator with a set of off-plane geometry gratings for ultrafast time resolution (from few to several tens of fs) and medium energy resolution (from 100 meV to 400 meV), and a set of classical geometry gratings for high energy resolution (from 15 meV to 40 meV) and a long time response (a few 100 fs).
HHG performance
HHG photon flux as a function of photon energy for Ar and Ne.
HHG pulse characteristics (100 μm monochromator exit slit; H15, i.e., 23.2 eV)
Grating | Duration (fs) | Energy resolution (eV) | Fourier limit (eV) |
OPG G200 | 23 ± 1.2 | 0.5 | 0.08 |
OPG G400 | 35 ± 1.7 | 0.25 | 0.052 |
OPG G600 | 35 ± 1.9 | 0.16 | 0.052 |
CG G300 | 170 ± 10 | 0.03 | 0.01 |
Characteristics of the monochromator gratings
Off-plane geometry (OPG)
|
Classical geometry (CG)
|
The HHG beamline with the generation chamber (left), monochromator (middle) and slits (right) for adjusting the spectral resolution and photon flux. 2. Experimental chamberThe experimental chamber for time and angle resolved photoemission spectroscopy is equipped with a VG-Scienta R3000 electron spectrometer, 5 degrees of freedom (x,y,z and two rotational axes) cryogenic manipulator (minimum sample temperature of 18 K) and a monochromatized X-ray source (Al Kα, 1486 eV) for static XPS measurements. An angle resolved time-of-flight (ARTOF 10K from VG-Scienta) electron spectrometer is currently being commissioned.R3000 (VG-Scienta) electron spectrometer specifications:
ARTOF 10K (VG-Scienta) electron spectrometer specifications:
The experimental chamber is also equipped with the following sample preparation/manipulation tools:
The time and angle resolved photoemission spectroscopy experimental chamber.
3. Ti:sapphire laser source
The HHG beamline is pumped by a Coherent Ti:Sa laser system operating at 800 nm (Micra Ti:Sa oscillator and a Legend Elite Duo two-stage amplifier), which provides 35 fs pulses with an energy of 3 mJ per pulse at a repetition rate of 5 kHz. By focusing such pulses, intensities on the order of 1016 W/cm2 can be reached, which is enough to generate high harmonics of the driving laser in gas.
The Coherent Ti:Sa laser system. 4. Optical parametric amplifierPart of the light from the Ti:Sa laser system is used to pump an optical parametric amplifier (OPA), which can provide ultrashort pulses (~50 fs) tunable in the wavelength range from 230 nm to 2600 nm. Such pulses are used as a pump in a time-resolved photoemission spectroscopy setup.OPA performance
Measured OPA energy per pulse for a pump pulse duration and energy of 40 fs and 0.92 mJ, respectively.
|