A cross-dispersed echelle spectrograph uses an echelle grating for strong dispersion and a cross-disperser in the perpendicular direction to separate overlapping diffraction orders. It records many orders simultaneously in an echellogram.
Echelle grating 2026-10-05
An echelle grating works in high diffraction orders. A separate cross-disperser separates their overlapping optical spectra on a two-dimensional detector.
Echellogram 2026-10-05
An echellogram is the two-dimensional detector pattern of separated diffraction orders from a cross-dispersed echelle spectrograph.
Use the signed-angle convention in which the reflection grating equation is , with positive diffraction order . For fixed incidence,
The second identity is the local focal-plane scale, measured about the camera axis aligned with the central diffracted ray. Since , the projected beam size cancels the cosine in the grating dispersion:
Writing for the number of illuminated grooves also gives . This connects the geometrical instrument invariant to the phase span of the illuminated diffraction grating.
The bright peaks occur when contributions from adjacent grooves have equal phase modulo , so all illuminated grooves contribute by constructive interference. Use the reflection-grating convention shown below: and are positive angles of the incident and outgoing ray lines on the same side of the normal. The incoming and outgoing path differences between neighboring grooves are and , respectively. Hence the grating equation is
The integer labels the diffraction order. With a different signed-angle convention, the same physical condition contains a difference of sines.
Figure 1.
Reflection-grating angle convention
. The incident ray and selected outgoing ray are both drawn on the positive side of the surface normal. Adjacent groove spacing contributes the sum of their two projected path differences.
The echellogram contains nearly parallel traces, one for each diffraction order. Choose the main echelle grating dispersion to increase wavelength toward the right and the cross-disperser to increase wavelength upward. At a fixed horizontal coordinate, order has a shorter wavelength than order , so it lies below order in this convention.
Figure 1.
Adjacent orders in a cross-dispersed echellogram
. Order m+1 is bluer than order m at the same main-dispersion coordinate. Within either order, wavelength increases along the trace to the right; the chosen cross-dispersion orientation puts longer wavelengths higher on the detector.