Phto-injector laser chain NEWS Massimo Petrarca & Marta Divall.

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Presentation transcript:

Phto-injector laser chain NEWS Massimo Petrarca & Marta Divall

History: 1 Amp2 Problems (for energy) 1 Synch. Problems (Laser -> Gun) 2 Harmonic Conversion Efficiency &Stability Major issues in January 2008 When NO Harmonic generation was performed! May June 2008 Harmonic generation Performed with Amp1 only: New Problems discovered! 1 Amp1 Problems (Over most of the other problems): June July 2008 Amp1 problems (pulses train instability, ASE, parasitic lasing) 2 Amp2 Problems (for energy) 2 Synch. Problems (Laser -> Gun) 3 Harmonic Conversion Efficiency &Stability

3-pass Nd:YLF amplifier 2 pass Nd:YLF amplifier Optical gate (Pockels cell) PC 22 44 Drive Beam (PHIN); Probe beam ~600ps=<  t=<  tPC 1.5 GHz Nd:YLF Oscillator + Nd:YLF Preamplifier 1047nm Micro pulses at 1.5 GHz ~666ps; 10W 400us amplification window for AMP1 Macro pulse 200us amplification window for AMP2 Macro pulse UV tt tt Green tt IR Laser overview Pulse picker

First Amplifier layout M1 M2 M3 M4 M5 1 st pass 2 nd pass 3 rd pass F1 = +1146mm Preamp. beam 58cm54cm 21cm 3.5cm 2.5cm 5cm M6 Nd:Ylf rod -Final configuration: 3passages trough the rod with F1 to ~ compensate for the beam divergence: X(3 rd pass)-X(1 st pass)~1.2mm; Y(3rd pass)-Y(1st pass)~1mm. Nominal power ~3KW has been reached Satisfactory trace pulse stability has been reached Transverse beam parameters:M 2 x ~2.38; M 2 x ~1.94 Power Measurements Amp1: Unamplified  ~ amps  ~ amps  ~ amps  ~ amps  ~ amps  ~ 9.7 W  ~3.0 KW

Amp2: layout M12 M11 1 st pass 2 nd pass F2 = +300mm M6 Nd:Ylf rod Pericope+Farady F3 = -114mm Amp1 3 rd pass. M7M8 M9 M10 94 cm 57.5 cm 20.5 cm 122 cm 2.5cm 29.5cm 22cm 75 cm 156 cm Tot:48 cm Pockels Cell 20 cm 25 cm 26 cm 7 cm F4 = +802mm F5 = +402mm 14.5 cm 7 cm -Present configuration: 2passages trough the rod with F3 and F2 for the matching: “beam size rod size” Satisfactory trace pulse stability has been achieved Power ~6.3KW has been reached with 90A Way to Harmonic G. crystal

Amp1 + 90A Power Measurements Amp1: Unamplified  ~ amps  ~ amps  ~ amps  ~ amps  ~ amps  ~ 9.7 W  ~3.0 KW Power Measurements 50 amps  ~ 60 amps  ~ amps  ~ amps  ~ amps  ~ 12.3 W  ~6.3 KW

Amp1+Amp2 Harmonic Generation IR energy within 2  s gate GREEN energy within 2  s gate UV Energy within 2  s gate PC on 2  s ( Best Result ) ( )mJ std=0.06mJ ~1.2 mJ Std=0.016mJ mJ Std=0.012  nJ in a micro pulse ~44 % efficiency ~34 % efficiency PC on 2  s ( )mJ std=0.26mJ 3.23 mJ Std=0.07mJ 40% efficiency mJ Std=0.024  ~234 nJ in a micro pulse 22% efficiency A decrease on the conversion efficiency has been observed when both amplifiers Optimization of the beam size onto the conversion crystals has to be done; nevertheless the conversion efficiency is still acceptable yielding a micropulse energy of ~230nJ (nominal 730nJ) Collaboration with Guy Cheymol “CEA”

On site synchronization meas.: J real ~ 634 fs (rms jitter required <1ps) JNF: jitter noise floor ~ 350 fs Jmeas: 724fs Lecroy SDA (16GHz, 60GS/s+ NewFocus Photodetector25GHz) After on site investigation, oscillator cavity perturbations due to thermal effects were suspected HighQ expert came and fixed the settings of the oscillator end-cavity mirror (semiconductor saturable absorber mirror “SESAM”): 50C Degree Problem has been fixed

HighQ Jitter behavior (over a day) HighQ company provided the unit to synchronize the laser to the ext. rf master clock (~1.499):“Synch” From this unit it is possible to monitories the jitter “Laser vs Ext-rf”

Open Issues: Even more difficult (it takes time!!): The rod probably has to be changed to improve transverse beam profile (poor quality now!). Third passage has to installed to extract more energy and to compensate for thermal effect introduced by Amp1. Lenses system for the matching “rod -beam” size along the 3 passages has to be installed …… …..(optimization of the whole beam line that comes after!!!!!) Coupling: “Pumping beam vs Nd:Ylf rod” has to be study (no cylindrical lenses installed now; it could be necessary to replaced those lenses to focus pumping beam into the rod.) Conversion efficiency studies (saturation, best size onto crystals….)

The end