2023
DOI: 10.3788/col202321.043802
|View full text |Cite
|
Sign up to set email alerts
|

Generation and application of high-contrast laser pulses using plasma mirror in the SULF-1PW beamline

Abstract: The plasma mirror system was installed on the 1 PW laser beamline of Shanghai Superintense Ultrafast Laser Facility (SULF) for enhancing the temporal contrast of the laser pulse. About 2 orders of magnitude improvement on pulse contrast was measured on picosecond and nanosecond time scales. The experiments show that high-contrast laser pulses can significantly improve the cutoff energy and quantity of proton beams. Then different target distributions are assumed in particles in cell simulations, which can qual… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

2024
2024
2024
2024

Publication Types

Select...
4

Relationship

2
2

Authors

Journals

citations
Cited by 4 publications
(2 citation statements)
references
References 33 publications
0
2
0
Order By: Relevance
“…Using the recently developed multi-petawatt laser technology, laser intensities up to an order of 10 22 W cm −2 can be achieved [1][2][3]. Energetic ion beams can be realized via intense laser interactions induced on solid targets [4][5][6] using different acceleration mechanisms, such as target normal sheath acceleration (TNSA) [7][8][9], radiation pressure acceleration, collisionless shock acceleration (CSA) [10][11][12], and so on. Among these mechanisms, TNSA is the easiest and most robust method for generating proton beams with energies of the order of ∼100 MeV under current laboratory conditions [7][8][9]13].…”
Section: Introductionmentioning
confidence: 99%
“…Using the recently developed multi-petawatt laser technology, laser intensities up to an order of 10 22 W cm −2 can be achieved [1][2][3]. Energetic ion beams can be realized via intense laser interactions induced on solid targets [4][5][6] using different acceleration mechanisms, such as target normal sheath acceleration (TNSA) [7][8][9], radiation pressure acceleration, collisionless shock acceleration (CSA) [10][11][12], and so on. Among these mechanisms, TNSA is the easiest and most robust method for generating proton beams with energies of the order of ∼100 MeV under current laboratory conditions [7][8][9]13].…”
Section: Introductionmentioning
confidence: 99%
“…So far, the highest peak power has reached 10 PW, and the largest focused peak intensity has exceeded 10 23 W=cm 2 [7][8][9] . For such high-intensity laser facilities, the temporal contrast has become a crucial parameter for laser-matter interactions [10][11][12] . Since the prepulses or pedestals with intensity over 10 11 W=cm 2 would inevitably generate preplasma prior to the main pulse in the laser-matter interaction process [13] , the methods and techniques to suppress the unwanted prepulses or pedestals while maintaining the focused peak intensity of the main pulse deserve to be taken into consideration.…”
Section: Introductionmentioning
confidence: 99%