Blind beam coke spots and dynamic control systems and methods based on plasma regulation
A plasma and dynamic control technology, applied in optics, optical components, instruments, etc., can solve problems such as limited degrees of freedom, great influence of focal spot shape, and difficult technical means to achieve continuous dynamic changes and enhanced flexibility sexual effect
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Embodiment 1
[0046] A beam focal spot shaping and dynamic control system based on plasma control, wherein the incident main laser light (1) passes through a focusing lens (3) and then is focused on a distant focal plane (4) to generate a beam focal spot. In order to achieve dynamic control of the focal spot of the beam, the system places a plasma optical device (2) constructed using plasma in the near-field or quasi-near-field area where the beam is focused, with continuous phase plates and dynamic characteristics. The dispersion properties of the volume are controlled by the density and thickness of the plasma optical device (2), and then according to the design theory of the continuous phase plate, according to the requirements of the dynamic evolution of the target focal spot, the phase distribution of the plasma formation is designed. And further decompose the plasma dynamic evolution function η(x 0 ,y 0 ,t), to realize the shaping of the continuous phase plate; at the same time, the...
Embodiment 2
[0054] In one embodiment the plasma optics (2) are placed in front of the focusing lens (3), as figure 1 shown. After the beam passes through the plasma optical device (2), the phase distribution introduced by it is:
[0055]
[0056] Where λ is the beam wavelength, n e (x 0 ,y 0 ,t) is the plasma density distribution, x 0 ,y 0 is the near-field coordinates of the beam, t is the time, n c is the plasma critical density for wavelength λ, l(x 0 ,y 0 ) is the thickness of the plasma layer. The intensity distribution of the beam focal spot corresponding to the phase distribution of formula (1) is
[0057]
[0058] "F" in formula (2) represents Fourier transform, c' is a constant term, x, y are the far field coordinates, and E is the near field amplitude of the beam.
[0059] According to the design theory and method of the continuous phase plate in the foregoing embodiment 1, the phase distribution of the near field of the beam can be adjusted The focal spot I(x,...
Embodiment 3
[0062] In this embodiment, it is assumed that the focal spot dynamic I objn (x,y,t n ) evolution requires a specific parameter design method under the condition of linearly decreasing with time, at this time for A specific design is carried out, one of the design results is as follows: the initial phase distribution Such as image 3 As shown, the dynamic function η(x 0 ,y 0 ,t) is expressed as
[0063]
[0064] where T 0 is the rate parameter of the linear change of the focal spot.
[0065] Such as Figure 4 simulated in image 3 The initial phase of and the morphological characteristics of the focal spot under the dynamic function of formula (5), where in (a)-(f), the values of t are 0, 0.1T 0 , 0.2T 0 , 0.3T 0 , 0.4T 0 , 0.5T 0 , at this time, the near-field moment has the characteristics of full use of energy and overall random phase, and the corresponding focal spots have the same shape, and the major axis sizes are 1000 μm, 900 μm, 800 μm, 700 μm, 600 ...
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