This superposition of wavelengths, which would lead to ambiguous spectroscopic data, is inherent in the grating equation itself and must be prevented by suitable filtering (called order sorting), since the detector cannot generally distinguish between light of different wavelengths incident on it (within its range of sensitivity). A detector sensitive at both wavelengths would see both simultaneously. In this example, the red light (600 nm) in the first spectral order will overlap the ultraviolet light (300 nm) in the second order. that is, for any grating instrument configuration, the light of wavelength λ diffracted in the m = 1 order will coincide with the light of wavelength λ/2 diffracted in the m = 2 order, etc. It is evident from the grating equation that light of wavelength λ diffracted by a grating along direction β will be accompanied by integral fractions λ/2, λ/3, etc. The most troublesome aspect of multiple order behavior is that suc-cessive spectra overlap, as shown in Figure 2-5. This convention is shown graphically in Figure 2-4. β 0 if the diffracted ray lies to the left (the counter-clockwise side) of the zero order (m = 0), and m Explicitly, spectra of all orders m exist for which In most cases, the grating equation allows light of wavelength λ to be diffracted into both negative and positive orders as well. Specular reflection, for which m = 0, is always possible that is, the zero order always exists (it simply requires β = – α). This restriction prevents light of wavelength λ from being diffracted in more than a finite number of orders. When the laser light is incident normally on a diffraction grating the first order maximum is produced at an angle of 12. The grating equation reveals that only those spectral orders for which |m λ/d| 2, which is physically meaningless. Similarly, the second order (m = 2) and negative second order (m = –2) are those for which the path difference between rays diffracted from adjacent grooves equals two wavelengths. This happens, for example, when the path difference is one wavelength, in which case we speak of the positive first diffraction order (m = 1) or the negative first diffraction order (m = –1), depending on whether the rays are advanced or retarded as we move from groove to groove. The physical significance of this is that the constructive reinforcement of wavelets diffracted by successive grooves merely requires that each ray be retarded (or advanced) in phase with every other this phase difference must therefore correspond to a real distance (path difference) which equals an integral multiple of the wavelength. In fact, subject to restrictions discussed below, there will be several discrete angles at which the condition for constructive interference is satisfied. For a particular groove spacing d, wavelength λ and incidence angle α, the grating equation is generally satisfied by more than one diffraction angle β.
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