For a better understanding of the invention, and to show how embodiments of the same may be carried into effect, reference will now be made, by way of example, to the accompanying diagrammatic drawings in which:
In order to address the problem of refractive index of an optical component (such as a pre-collimator, beam-shaper or sensor lens) varying with temperature it is proposed to integrate a wavelength sensitive (such as a grating structure or stepped phase structure) on the optical component, which structure compensates for the defocusing in temperature due to the change of the refractive index with temperature of the material. The wavelength sensitive structure forms part of an optical system of an optical read/write device.
For plastics materials the change of refraction index with temperature is larger than for glass materials. The invention is therefore most beneficial for plastics optical components.
In the case of a light path with two lasers (discrete lasers or separate laser-branches), such as that shown in
One possibility to address the change of the laser wavelength with temperature is the use of a non-periodic phase structure as described in Appl. Opt. Vol. 40 no 35 6548-6560, the contents of which are incorporated herein by reference. The height h of the steps in the structure are in fixed steps with
Say that j is the number of steps. For that case the zone height is mj.h with mj an integer. If Δλ is the wavelength shift and Δn is the refracting index change (both due to temperature) the phase steps ΔΦj are:
Another possibility is using other diffractive structures like a blazed grating or kinoform grating, which are also wavelength sensitive.
A blazed grating is a structure as shown in
The kinoform grating is like the blazed grating, but it has a more rounded shape.
For a lens having a wavelength sensitive diffractive grating structure, the power of the grating is part of the total power of the lens, which is the case of this invention.
The power of the grating structure is designed in such a way that the wavelength shift of the laser causes exactly the same focal length shift of the lens as by the change of the refracting index change with temperature of the body, however with opposite sign.
The servo or sensor lens 56 for the focus adjustment is also not in the common path: only in the detector path 26 and not in the laser path 14/22. The sensor lens 56 usually comprises a spherical and an astigmatic surface. It could also be that some chromatic aberration correction is implemented in this sensor lens 56.
The lens 56 will also cause defocus with temperature, because it is not in the common path. However this effect is not so strong, and is described by (approximation with planar convex or concave lens)
with the parameters as described with formula (1)
When a single detector is applied the servo or sensor lens 56 in front of the detector must operate correctly at 2 wavelength ranges (although as mentioned above more than 2 wavelength ranges could be used). The temperature compensation on this lens is chosen for the most critical application, which is in general the shortest wavelength (for instance DVD λ=660 nm). Alternatively, a structure may be used to give a mixed effect on both wavelengths.
The above is also for the situation when a beam-shaper or pre-collimator is applied together with a dual wavelength laser (two laser-chips having different wavelength ranges in one package).
A similar setup can easily be devised in the case that the optical read/write device uses more than two wavelength ranges. For example, in the case of an optical reading/writing device for CD, DVD and BD applications there would be three branches as opposed to the two laser branches 14/22 in the embodiment described above.
| Number | Date | Country | Kind |
|---|---|---|---|
| 03103812.8 | Oct 2003 | EP | regional |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/IB04/52013 | 10/7/2004 | WO | 00 | 4/16/2007 |