|
||||||||||||||||||||||||||
Technical Notes
Here m is the (integral) diffraction order (usually |m| = 2), l is the wavelength, d the groove spacing and b the angle of diffraction (measured from the normal). Figure 1 Transmission grating in use. The incident light is usually normal to the grating surface and strikes the back of the grating. Only three spectral orders are shown.
The efficiency behavior of transmission gratings is simpler than that for reflection gratings, since no metals are present to introduce complicated electromagnetic effects and since the angles of diffraction are usually small. Thus, polarization effects are virtually absent. BLAZED TRANSMISSION GRATINGS The peak efficiency of a blazed (triangular-groove) transmission grating occurs when the refraction of the incident beam though the mini-prism that constitutes a groove lies in the same direction as the diffraction given by the grating equation (see Fig. 2). Unlike reflection gratings, the groove angle is much larger than the blaze angle for a transmission grating, since the phase retardation doubles upon reflection but is multiplied by n-1 for a transmission grating, where n is the refractive index of the grating medium. Figure 2 A blazed transmission grating. For the wavelength l to be blazed in the direction shown, both the grating equation (1) and Snell's law (2) must be satisfied.
Applying Snell's law to the interface between the groove facet and air,
Combining this relation with the grating equation, yields the relationship between the blaze angle bB and the groove angle c:
For small groove angles and for l << d, a useful approximation to Eq. (3) relates the blaze wavelength of a reflection grating to that of the corresponding transmission grating. For transmission gratings used in air or vacuum, the ratio of its blaze wavelength (for normal incidence) to that of the equivalent reflection grating (used in Littrow) is
where
A corollary to this approximation is that, for n » 1.6, the grooves of a transmission grating are about 10/3 times as deep as those of the corresponding reflection grating. For small diffraction angles (i.e., diffraction near the normal), this ratio holds for the angle c as well. The choice of groove angle for transmission gratings is limited by total internal reflection effects:
For n » 1.6, this yields about 40° as the upper limit on c, though in many cases the effective limit is somewhat lower. This means that transmission gratings cannot be used for high-dispersion applications. TRANSMISSION GRATING EFFICIENCY The shape of an ideal efficiency curve for a blazed transmission grating is the same as for a reflection grating in the scalar region (c < 8°). Peak efficiency occurs at
It can be shown that most of the incident light will be diffracted into either the zero order or positive first order if
very little light will go into the negative first order or higher orders. TRANSMISSION GRATINGS AS BEAM DIVIDERS When the angle between two divided beams is small, transmission gratings serve as ideal beamsplitting elements. Most of the transmitted light will be in the zero and first diffracted order when the grating is used off-blaze, and the ratio of the zero order efficiency to the first order efficiency can be varied over a wide range. [For three beams, a symmetrical groove profile is required.] ORDERING INFORMATION Popular transmission grating sizes and prices are listed in the Diffraction Grating Catalog and Price Guide. Different specifications can be accommodated: please contact us for price quotations. Prices are subject to change without notice. FOR FURTHER INFORMATION For additional information, please contact us. back to topNewport Corporation |
||||||||||||||||||||||||||
|
||||||||||||||||||||||||||
| Newport Home |
| Richardson Gratings Home |
| Product Tables >> |
| Supplemental Information >> |
| How to request a quote... |
| New Products |
| 1: Plane Ruled Diffraction Gratings |
| 2: Plane Holographic Diffraction Gratings |
| 3: Concave Ruled Reflectance Gratings |
| 4: Echelle Gratings |
| 5: Large Astronomical Gratings |
| 6: Plane Transmission Gratings -- Visible |
| 7: Plane Transmission Gratings -- Ultraviolet |
| 8: Dye Laser Tuning Gratings |
| 9: Molecular Laser Tuning Gratings |
| 10: Concave Holographic Reflectance Gratings |
| 11: Pulse Compression Gratings |
| 12: Fiber Optic Telecommunication Gratings |
| 13: UV / Vis Gratings |
| The Catalog Number System |
| Types of Diffraction Gratings |
| Special Requests & Custom Gratings |
| Grating Specifications |
| Grating Efficiency |
| Standard Tolerances |
| Certification & Warranty |
| Cleaning Gratings & Surface Defects |
| Terms & Conditions of Sale |
| Addendum to Terms & Conditions of Sale – Master Gratings |
| Credit Application |
| Diffraction Grating Handbook |
| Technical Data >> |
| Technical Notes >> |
| Publications |
| Our Capabilities |
| About Richardson Gratings |
| Reflectance Curves of Standard Coatings, UV-VIS-NIR |
| Epoxy Transmission Curves, UV-VIS-NIR |
| Relative Index of Epoxies in the Visible Spectrum |
| Relative Index of Epoxies in the Infrared Spectrum |
| Blaze Angle vs Blaze Wavelength curves (Littrow Angle) |
| 1: Laser Tuning with Diffraction Gratings |
| 2: Pulse Compression and Stretching with Diffraction Gratings |
| 3: Concave Gratings |
| 4: Transmission Gratings |
| 5: Grisms |
| 6: Echelle Gratings |
| 7: The Blaze Arrow |
| 8: Handling Gratings |
| 9: Scattered Light and Stray Light |
| 10: Guidelines for Specifying Diffraction Gratings |
| 11: Determination of the Blaze Wavelength |
| 12: Sources of Error in Monochromator-Mode Efficiency Measurements of Plane Diffraction Gratings |
| 13: Measurement of Polarization-Dependent Loss (PDL) for Plane Diffraction Gratings |
| 14: Fundamentals of Diffraction Grating Technology and Industrial Laser Applications of Gratings |
| Sales Offices |
| Information Request |
| Literature Request >> |
| Quotation Request |
| Catalog Request |
| Handbook Request |