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Crystalline undulators

Hard photons from periodically bent crystals

A crystal with periodically bent planes makes channeled particles wiggle with a sub-millimetre period and emit hard photons.

The physics.

A crystalline undulatorAtomic planes bent along a sine wave with a sub-millimetre period. A channeled electron or positron follows the planes, oscillates with the same period and emits hard photons in a narrow forward cone. γ λu < 1 mm e⁺/e⁻ periodically bent atomic planes (amplitude of a few nm) not to scale
A channeled particle follows periodically bent planes and emits hard photons forward. The amplitude is greatly exaggerated.

In a mag­net­ic un­du­la­tor a row of alternat­ing magnets makes a rel­a­tiv­is­tic elec­tron or po­si­tron wiggle, and it ra­di­ates in a narrow band of en­er­gies. For small deflec­tions the photon energy on axis is

Eγ ≈ 2γ2 hc / λu

where γ is the Lorentz factor of the par­ti­cle and λu the period. Mag­net­ic un­du­la­tors cannot have periods shorter than a few cen­ti­me­tres.

In a crystal whose planes are bent along a sine wave, a chan­neled par­ti­cle follows the planes and os­cil­lates with their period, which can be a frac­tion of a mil­li­me­tre. A period a hundred times shorter gives photons a hundred times harder from the same beam: with λu = 334 µm the formula gives about 30 keV for 1 GeV elec­trons and a few MeV at 10 GeV, from a crystal a few mil­li­me­tres long.

The deforma­tion has to be large com­pared with the 0.19 nm spacing of silicon (110) planes, with an am­pli­tude above about 1 nm, yet gentle enough that the par­ti­cles stay chan­neled, and it has to be uniform through the whole crystal, so that every channel os­cil­lates in step.

We bend crys­tals periodi­cally without dam­ag­ing the lattice. Stripes of silicon nitride, de­pos­it­ed under tension and pat­terned on the surface, impose a si­nu­soi­dal deforma­tion through the thick­ness; finite-element simula­tions choose the thick­ness and the period so that the shape is uniform and higher har­mon­ics are small. Earlier un­du­la­tors were made by groov­ing the surface and by ion implanta­tion.

What we have shown.

A crystal with periodi­cally bent planes makes chan­neled par­ti­cles os­cil­late with a sub-mil­li­me­tre period, so it can emit photons far harder than a mag­net­ic un­du­la­tor. Using pat­terned tensile films we pro­duced the first damage-free si­nu­soi­dal crys­tals: the latest is 160 µm thick with ten 334 µm periods. The method is covered by patent applica­tion WO 2026/078554.

10 × 334 µm

A 160 µm thick silicon crystalline undulator with ten sinusoidal periods of 334 µm, made with patterned silicon-nitride stressor films. The method is covered by patent application WO 2026/078554.

Nucl. Instrum. Methods A 1076 (2025)

Read first.

  1. Design of a crystalline undulator based on patterning by tensile Si₃N₄ strips on a Si crystalGuidi V., Lanzoni L., Mazzolari A., Martinelli G., Tralli A. · Applied Physics Letters 90 (2007)
  2. Experimental evidence of planar channeling in a periodically bent crystalBagli E., Bandiera L., Bellucci V. … Guidi V., Mazzolari A. et al. · European Physical Journal C 74 (2014)
  3. Silicon crystalline undulator prototypes: Manufacturing and X-ray characterizationCamattari R., Bandiera L., Tikhomirov V. … Romagnoni M., Sytov A., Mazzolari A. et al. · Physical Review Accelerators and Beams 22 (2019)
  4. From simulation to fabrication: Realizing silicon crystalline undulators with silicon nitride stressor layer patterningMalagutti L., Bandiera L., Bonafè F. … Fedeli P., Guidi V., Paternò G. et al. · Nucl. Instrum. Methods A 1076 (2025)
  5. Ion implantation for manufacturing bent and periodically bent crystalsBellucci V., Camattari R., Guidi V. … Mazzolari A., Paternò G. et al. · Applied Physics Letters 107 (2015)
  6. Photon emission by volume reflected electrons in bent crystalsNielsen C.F., Uggerhøj U.I., Holtzapple R. … Bandiera L., Guidi V., Mazzolari A. et al. · Physical Review Accelerators and Beams 22 (2019)

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