Mango wiggler as a novel insertion device providing a large and symmetrical imaging field of view

Zhang, D.; Li, M.; Li, X.; Lu, H.; Li, Y.; Zhang, J.; Li, G.; Zhang, W.; Dong, Y.; Tao, Y.; Sheng, W.; Liu, P.

doi:10.1107/S1600577524004429

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Figure 14
Photon fluxes within a 3 mrad acceptance angle for different wigglers. (a) Planar wiggler [B_y(z) = B_y0sin(2πz/λ_uy), B_y0 = 1.8 T, λ_uy = 60 mm and N_u = 18]. (b) The ideal Mango wiggler. (c) Planar wiggler [B_y(z) = B_y0sin(2πz/λ_uy), B_y0 = $[1.8\sqrt{2}]$ T, λ_uy = 60 mm and N_u = 18]. (d) Helical wiggler [B_x(z) = B_x0cos(2πz/λ_ux), B_y(z) = B_y0sin(2πz/λ_uy), B_x0 = B_y0 = 1.8 T, λ_ux = λ_uy = 60 mm and N_u = 18].

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 31| Part 4| July 2024| Pages 791-803

https://doi.org/10.1107/S1600577524004429

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