2021
DOI: 10.1103/physreva.104.033506
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Long-range propagation of ultrafast ionizing laser pulses in a resonant nonlinear medium

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Cited by 9 publications
(17 citation statements)
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“…2). The spectrum also had significant intensity at the 795 nm D 1 resonance line (5s 2 S 1/2 → 5p 2 P 1/2 transition) and the 776 nm transitions to higher lying excited states (5p 2 P 3/2 → 5d 2 D 3/2 and 5d 2 D 5/2 ), similarly to our previous experiments [9]. In the other half of the measurements, spectral shaping was used to obtain laser pulses with the central wavelength shifted away from these resonances.…”
Section: Experiments a Laser Propagation Experiments Apparatussupporting
confidence: 89%
See 1 more Smart Citation
“…2). The spectrum also had significant intensity at the 795 nm D 1 resonance line (5s 2 S 1/2 → 5p 2 P 1/2 transition) and the 776 nm transitions to higher lying excited states (5p 2 P 3/2 → 5d 2 D 3/2 and 5d 2 D 5/2 ), similarly to our previous experiments [9]. In the other half of the measurements, spectral shaping was used to obtain laser pulses with the central wavelength shifted away from these resonances.…”
Section: Experiments a Laser Propagation Experiments Apparatussupporting
confidence: 89%
“…These single-photon resonances also have a major impact on the propagation of the ionizing laser pulse -a question studied only very recently in the context of ultra-short pulse propagation [8]. It has been suggested [9], that the single-photon resonances give rise to a strong but saturable nonlinearity which can be very advantageous for the propagation of the ionizing pulse. In particular, theoretical indication was that the plasma column becomes longer and more sharply bounded with the use of a resonant ionizing pulse.…”
Section: Introductionmentioning
confidence: 99%
“…The proton bunch propagates in a plasma created by a relativistic ionisation front (RIF). The RIF is the result of the propagation of a short and intense laser pulse in a rubidium vapour [24][25][26][27]. When the RIF is placed within the proton bunch, the part of the bunch behind the RIF travelling in plasma is transformed into a train of microbunches.…”
Section: Summary Of Experimental Results From Awake Runmentioning
confidence: 99%
“…This is can be fulfilled by carefully tailoring rubidium vapor density in the chamber and achieving single-electron ionization of the atoms with a probability very close to unity [30]. The propagation of the ultra-short, TW ionizing pulse along the vapor source is itself a complex nonlinear process [26], especially because it is resonant with the rubidium D 2 transition line [27,28]. Validating the quality of the plasma can be done near the downstream end of the vapor source, where a pair of observation ports on opposite sides of the chamber allow the passage of a probe beam transverse to the plasma channel axis.…”
Section: Schlieren Imaging Of a Plasma Channel Cross-section A Measur...mentioning
confidence: 99%
“…At the heart of the novel accelerator device, a 10-meter-long plasma channel achieves the modulation of the energetic proton bunch and the acceleration of witness electron bunches in the emerging wakefields. Created via photoionization using a terawatt laser system in a rubidium vapor source chamber [24,25], plasma channel generation is in itself a complex problem of laser beam propagation/filamentation [26][27][28]. Optical diagnostic tools monitoring the plasma channel can thus have a significant role in optimizing, improving the accelerator device and understanding wakefield physics.…”
Section: Introductionmentioning
confidence: 99%