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Revision History

Shown below are VISRAD revision summaries for:

 

Version 16.1.1

 

Version 16.1.0

 

Version 16.0.0

    

NIF CPP
HWHM R-major (mm)
HWHM R-minor (mm)
Supergaussian n *
No CPP
75
75
2.0
400 um CPP
189
189
7.145

 

Version 15.0.0

A laser beam cone is considered to be fully captured by the target grid if both the "boundary" of the beam cone is fully contained within the target grid and it hits the target surface at an incident angle which is less than a specified allowed maximum. The beam cone is given an enhanced radius to ensure a that minimum clearance is maintained.

In performing laser beam capture calculations, only Target Components are considered in the calculation. Chamber Components are ignored. Also, calculations are performed only for blue (3ω) cones; for NIF, calculations are not supported for red (1ω) and green (2ω) cones.

The beam capture report contains two tables: one containing the beam "capture fraction", the other containing the maximum allowed incidence angle.

      

The capture fraction is the fraction of test rays that are incident on the grid of Target Components (see table above, left). For each beam cone, a grid of rays extends from the laser beam final optic toward the beam focus. The intersection of each ray with the target grid is then computed, and the number of hits on each Target Component is tallied. The fraction of rays hitting each target component is shown in the table, as well as the total for the target mesh. If the capture fraction for the total mesh is less than one, the result is highlighted.

For each ray hitting a surface element of a Target Component, the angle with respect to the surface normal is computed. The maximum angle recorded for each Target Component is then reported in the incident angle table (see table above, right). If the maximum incident angle exceeds the value specified by the user, the result is highlighted.

A laser beam cone is considered to clear a Target Component (or Chamber Component) if none of its surface elements is contained within a cone test volume which is specified using: (1) the intensity threshold (I/Imax), which is used to define the outer radius of the beam cone, and (2) a minimum clearance, which is the amount by which the cone radius is expanded

For each laser beam cone, all Target Components and Chamber Components are checked to see if any of their surface elements lie within the test volume. If any surface elements lie within the test volume, the component fails the clearance test. The beam clearance report contains a table showing, for each beam cone, which Target Components and which Chamber Components are either cleared (shown as green) or not cleared (shown as red). This allows users to easily see which items fail the clearance test for each beam.

 

Input for the blue (3ω) clearance calculations include the intensity threshold to use in defining the outer radius of the cone test volume, and the amount by which the test cone radius is enhanced. This enhancement to the cone radius is applied along the entire length (z-axis) of the cone.

For red (1ω) clearance calculations (for NIF), separate clearance parameters are applied to Target Components and Chamber Components. For the value specified for Target Components, the enhancement applied to the test volume is constant along the cone axis. For Chamber Components, the enhancement to the radius varies linearly with z (i.e., the distance from the focus). In this case, the clearance is specified using two parameters:

Additional parameters that affect the cone test volume are the number of angular (i.e., azimuthal) points, and the number of points along the z-direction (see the Lasers tab in Setting Preferences).

Additional information regarding beam clearance can be obtained using the check boxes at the bottom of the Laser Beam Clearance Report. The laser power deposition intensity on the target grid (i.e., Target Components only) can be shown in the Main Window, where the radius of each beam's intensity profile is enhanced by a specified amount. (If the enhanced radius is zero, the results are the same as obtained when selecting the Display | Direct Laser Power Deposited.)

Also in the Main Window, the surface elements of Target Components and Chamber Components that lie within the cone test volume of a specified laser beam can be displayed. To do this, check the box, and click on the Update Main Window Graphics button.

 

 

Version 14.1.0

NIF CPP
HWHM R-major (mm)
HWHM R-minor (mm)
Supergaussian n
Rev3-Inner-2w
890
660
7.6
1.0 Rev1a-Inner-2w
860
610
8.0
Rev3-Outer-2w
640
370
4.8
Rev1-Outer-2w
620
360
4.5
NIF CPP
Ring (Cone)
Rev3-Inner-2w
23 and 157
1.0 Rev1a-Inner-2w
30 and 150
Rev3-Outer-2w
44 and 135
Rev1-Outer-2w
50 and 130

 

 

Version 14.0.0

 

 

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