Four-piece infrared single wavelength lens system
a single wavelength, infrared technology, applied in the field of lenses, can solve the problems of poor material transparency, inability to meet the 3d game, inability to focus accurately, and change the focal length of the lens group, and achieve the effects of wide field of view, short length, and high resolution
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first embodiment
[0043]The equation for the aspheric surface profiles of the respective lens elements of the first embodiment is expressed as follows:
[0044]wherein:
z=ch21+[1-(k+1)c2h2]0.5+Ah4+Bh6+Ch8+Dh10+Eh12+Gh14+…z
[0045]represents the value of a reference position with respect to a vertex of the surface of a lens and a position with a height h along the optical axis 190;
[0046]c represents a paraxial curvature equal to 1 / R (R: a paraxial radius of curvature);
[0047]h represents a vertical distance from the point on the curve of the aspheric surface to the optical axis 190;
[0048]k represents the conic constant;
[0049]A, B, C, D, E, G, . . . : represent the high-order aspheric coefficients.
[0050]In the first embodiment of the present four-piece infrared single wavelength lens system, a focal length of the four-piece infrared single wavelength lens system is f, a f-number of the four-piece infrared single wavelength lens system is Fno, the four-piece infrared single wavelength lens system has a maximum...
second embodiment
[0072]The detailed optical data of the second embodiment is shown in table 3, and the aspheric surface data is shown in table 4.
TABLE 3Embodiment 2f(focal length) = 1.24 mm, Fno = 1.4, FOV = 60 deg.surfaceCurvature RadiusThicknessMaterialIndexAbbe #Focal length0objectinfinity400.0001infinity0.4002Lens 1−2.076(ASP)0.270plastic1.53556.000603.5383−2.155(ASP)0.1644stopinfinity−0.0435Lens 22.343(ASP)0.525plastic1.53556.0001.5756−1.187(ASP)0.2787Lens 3−0.438(ASP)0.339plastic1.63623.9706.1768−0.509(ASP)0.0329Lens 40.765(ASP)0.279plastic1.63623.9708.599100.770(ASP)0.54011IR-filterinfinity0.300glass1.51064.167—12infinity0.04513Image planeinfinity0.000
TABLE 4Aspheric Coefficientssurface 2356K:−1.9344E+01−4.1274E+01 1.9796E+01−1.3866E+00 A: 0.0000E+000.0000E+000.0000E+000.0000E+00B: 6.3906E−011.7297E+001.0624E+001.0126E−01C:−6.4418E−01−4.1896E+00 −6.3821E+00 −2.5618E+00 D:−3.3596E−011.8910E+011.9827E+019.5996E+00E: 1.0656E+00−6.8506E+01 −1.0523E+02 −1.2610E+00 F:−1.0869E+009.7292E+014.6618E+0...
third embodiment
[0081]The detailed optical data of the third embodiment is shown in table 5, and the aspheric surface data is shown in table 6.
TABLE 5Embodiment 3f(focal length) = 1.137 mm, Fno = 1.6, FOV = 65 deg.surfaceCurvature RadiusThicknessMaterialIndexAbbe #Focal length0objectinfinity600.0001infinity0.4002Lens 1−0.761(ASP)0.311plastic1.53556.000−17.2693−0.947(ASP)0.3084stopinfinity−0.0135Lens 22.438(ASP)0.488plastic1.53556.0001.6476−1.255(ASP)0.2867Lens 3−0.467(ASP)0.267plastic1.63623.970139.1148−0.565(ASP)0.0309Lens 40.610(ASP)0.296plastic1.53556.0003.759100.734(ASP)0.56911IR-filterinfinity0.300glass1.51064.167—12infinity0.04513Image planeinfinity0.000
TABLE 6Aspheric Coefficientssurface 2356K:−4.2894E+00 −8.3994E+00 1.9519E+01−2.6858E−01 A:0.0000E+000.0000E+000.0000E+000.0000E+00B:4.5540E−016.3321E−014.0053E−01−2.2477E−01 C:−2.4186E−01 8.0617E−01−6.2522E+00 −4.0891E−01 D:1.0748E+00−3.0908E+00 4.6866E+01−9.4895E+00 E:−4.5161E+00 2.1199E+01−3.1816E+02 6.7333E+01F:6.9923E+00−8.1978E+01 1.0791...
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