TY - GEN
T1 - High-energy laser pulses at 1064 nm with complex temporal shapes
AU - Meijer, Randy A.
AU - Stodolna, Aneta
AU - Witte, Stefan
AU - Eikema, Kjeld S.E.
PY - 2017
Y1 - 2017
N2 - Laser pulses are a powerful tool for inducing a large diversity of dynamical phenomena in matter. Control over the temporal shape of light pulses therefore also provides a means to control such dynamics on a wide range of timescales. Our aim is to improve control over laser-produced plasmas (LPP) and its short-wavelength emission characteristics, where plasma dynamics at nanosecond (ns) timescales play an important role. To investigate and control such dynamics, we need to combine GHz bandwidth pulse shaping capabilities with high pulse energies. The development of fast, compact, integrated electro-optic modulators (EOM) has made arbitrary temporal shaping at GHz speed accessible [1, 2]. However, the penalty for their fast modulation speed is a low power threshold, usually in the mW regime. Therefore, to enable fast temporal shaping of high-energy laser pulses, amplification after shaping is necessary. Here we present a laser system capable of delivering arbitrary shaped pulses with 0.5 ns temporal resolution and up to 440 mJ of pulse energy at 1064 nm wavelength and 100 Hz repetition rate. A grazing incidence amplifier utilizing Nd:YVO 4 crystals pumped at 880 nm [3] is seeded by a modulated 2W CW laser. Further amplification is obtained by utilizing a quasi-CW diode-pumped Nd:YAG power amplifier. A schematic of the full setup is shown in Figure 1a.
AB - Laser pulses are a powerful tool for inducing a large diversity of dynamical phenomena in matter. Control over the temporal shape of light pulses therefore also provides a means to control such dynamics on a wide range of timescales. Our aim is to improve control over laser-produced plasmas (LPP) and its short-wavelength emission characteristics, where plasma dynamics at nanosecond (ns) timescales play an important role. To investigate and control such dynamics, we need to combine GHz bandwidth pulse shaping capabilities with high pulse energies. The development of fast, compact, integrated electro-optic modulators (EOM) has made arbitrary temporal shaping at GHz speed accessible [1, 2]. However, the penalty for their fast modulation speed is a low power threshold, usually in the mW regime. Therefore, to enable fast temporal shaping of high-energy laser pulses, amplification after shaping is necessary. Here we present a laser system capable of delivering arbitrary shaped pulses with 0.5 ns temporal resolution and up to 440 mJ of pulse energy at 1064 nm wavelength and 100 Hz repetition rate. A grazing incidence amplifier utilizing Nd:YVO 4 crystals pumped at 880 nm [3] is seeded by a modulated 2W CW laser. Further amplification is obtained by utilizing a quasi-CW diode-pumped Nd:YAG power amplifier. A schematic of the full setup is shown in Figure 1a.
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U2 - 10.1109/CLEOE-EQEC.2017.8086273
DO - 10.1109/CLEOE-EQEC.2017.8086273
M3 - Conference contribution
AN - SCOPUS:85039902351
SN - 9781509067374
T3 - Optics InfoBase Conference Papers
BT - 2017 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)
PB - IEEE
T2 - The European Conference on Lasers and Electro-Optics, CLEO_Europe 2017
Y2 - 25 June 2017 through 29 June 2017
ER -