The corresponding wavelength is called the "blaze wavelength" and is represented by λB. Combining equations (8) and (9) gives the following:
It can be seen from this equation that the blaze wavelength varies with the blaze angle B and the incident angle (i.e., the usage method). In gerneral, the wavelength (λB(Litt)) where first-order diffracted light returns along the same path as the incident light is used to represent the blaze characteristics of gratings. In this case, = = B then equation (8) gives the following:
This is called the "Littrow mounting". In our catalogs, the blaze wavelengths given for plane gratings are the blaze wavelengths for this configuration. Equation (12) is Substituted equation (11) for equation (10) and applied to both sides.
The relationship between the blaze wavelength λB for other configurations and the blaze wavelength λB(Litt) used in the catalog is given by the following:
It can be seen from this equation that, when not using the Littrow configuration, the blaze wavelength λB is shorter than λB(Litt).
For incident angle , the relationship between λB(Litt) and λB is given by the following:
For example, for a groove density of 600 grooves/mm and an incident angle α of 60°, in order to obtain first-order light with a wavelength of 300 nm, substiture λB = 300 nm in equation (13) to obtain λB(Litt) = 484 nm. In this case, then, select a grating for which λB(Litt) = 500 nm from the catalog.
The blaze wavelengths given for concave gratings in catalog are the blaze wavelengths for the configuration (mounting) in the optical system used.
The arrows on the gratings indicate the blaze direction and the relationship between the groove profile and this direction is shown in Fig. 6.
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