In describing preferred embodiments of the present invention illustrated in the drawings, specific terminology is employed for the sake of clarity. However, the invention is not intended to be limited to the specific terminology so selected, and it is to be understood that each specific element includes all technical equivalents that operate in a similar manner to accomplish a similar purpose.
A falling-in, mainly parallel light bundle 10, falls on a diffraction grating 1. This will be diffracted spectrally by appropriate dimensioning of the diffraction grating 1 in a light bundle 11 diffraction order 1 and split in a light bundle 12 diffraction order 0. The light bundle 11 diffraction order 1 falls on a focusing mirror as optics 2 and is concentrated on a detector line 8 of a line receiver 3 along the expansion direction of the line. The detector line consists of individual CCD elements 7. In the expansion direction of the line the spectral split of the light bundle diffraction order 1 is detected.
To the diffraction grating 1 a first deflecting mirror 4 is so arranged that it reflects the light bundle 12 diffraction order 0 in the direction of falling-in light bundle 10. On a place which is closest possible to the falling light 10 a second deflecting mirror 5 is so positioned that it deflects the light bundle diffraction order 0 parallel to the falling-in light bundle 10 again on the diffraction grating 1. In this, the place lighted on the diffraction grating 1 from the diffraction order 0 is shifted by the amount a1 from the place of the falling-in light bundle 10 in the X direction. The light bundle 12 diffraction order 0 is diffracted there under the same conditions as the falling-in light bundle 10. The diffraction order 0 14 arising again here is freshly high shifted, through the two deflecting mirrors 4 and 5 coupled in and reaches the grating at a distance of a2. A further recycle of the light bundle 16 diffraction order 0 reaches the grating at the distance of a3. In general it is already sufficient, three such recycles, realized here with the diffraction order 0 light bundles 12, 14 and 16, to achieve a significant increase in efficiency. In the example the diffraction order 0 light bundle from the third recycle 18 is not used because it is negligible.
All the same wavelengths of the diffraction order 1 light bundle 11, 13, 15 and 17 are formed each in a corresponding point on the detector line 8 through the optics 2 so that one line on the detector line 8 reproduces the spectral characteristic. The light bundle diffraction order 1 which can be assigned to one wavelength, for example the wavelengths λ1, λ2 and λ3 are shown, meet each at one place on the detector line 8. Because the detector line 8 is made in the end from large single elements 7, in the width b of the single element 7 of about less than 1 mm a wavelength range of about 10 nm is received. In this example 32 individual receivers 7 are arranged on the detector line 8 which is 32 mm wide. The individual receivers have a height h of 10 mm. The measured wavelength range lies between 380 nm and 780 nm.
So that the process works optimally, the profile design of the diffraction grating 1 must be so made that as far as possible only diffraction order 0 occurs as false light order. This can be achieved by the maximum blaze of the grating being shifted in the short wave range. With mechanical triangular profiles this would mean that the flank angle is flatter. For example with a diffraction grating which at 500 nm diffracts 70% in diffraction order 1 and the remaining 30% in the diffraction order 0, the following behavior appears:
With this example calculation the absorption losses are not taken into consideration because these are negligible.
Details of the translation in directions x, y, z
Rotation around the corresponding surface particular X axis (alpha angle)
Rotation around the corresponding surface particular Y axis (beta angle)
Rotation around the corresponding surface particular Z axis (gamma angle)
The invention makes it possible to detect a spectral range from 380 nm-700 nm. In this the length of the spectrum is 31.2 mm. The diameter of the falling-in light bundle 10 is 3.0 mm and the grating density is ascertained at 1300 lines/mm. The offset of the 0 diffraction order light bundle in X direction comes to 5.00 mm per cycle. The first deflecting mirror 4 and the second deflecting mirror 5 are plane mirrors, the optics 2 is a mirror with a radius of 151.0 mm (cc).
Further the Figure shows that with an increasing number of back couplings of the 0 diffraction order light bundle an increasing efficiency increase is achieved. To the intensity of diffraction order 1 light bundle 11 from the falling-in light bundle are added the intensities of the 1 diffraction order light bundle 13 from the first recycle as well as the intensities of light bundle 15 and 17 from further recycles. The corresponding resulting curves are identified in the graph as 11, 13, 15 and 17.
The light bundle going out from the probe 27 reaches through the lens 26, the tubular lens 25, the scan optics 23, the x-y scanner 22, the main color splitter 21 as well as a pinhole optics 28, a pinhole 29, a collimator optics 30 and an emission filter 31 to the diffraction grating 1.
Between the scan optics 23 and the tubular lens 25 arises an intermediate image 24. With the Spectral Analytical Unit according to the invention an increase of up to more than 40% in the light yield with a spectral measurement is achieved with comparatively smaller expense. Thereby the space requirement for the additional deflecting facility and the additional radiation flow is small. Particularly advantageous is also that the invention can be built in already available Laser Scanning Microscopes and other spectrometric devices.
According to
It is to be understood that the present invention is not limited to the illustrated embodiments described herein. Modifications and variations of the above-described embodiments of the present invention are possible, as appreciated by those skilled in the art in light of the above teachings. It is therefore to be understood that, within the scope of the appended claims and their equivalents, the invention may be practiced otherwise than as specifically described.
Number | Date | Country | Kind |
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10 2006 017 705.3 | Apr 2006 | DE | national |