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Figure 3
The bremsstrahlung dose rate from the X13 straight section as a function of the IVUN magnet gap. The constant rate seen for magnet gaps between 10 and 5 mm is due to electron collisions with residual gas molecules in the straight section. |
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Figure 3
The bremsstrahlung dose rate from the X13 straight section as a function of the IVUN magnet gap. The constant rate seen for magnet gaps between 10 and 5 mm is due to electron collisions with residual gas molecules in the straight section. |