Optical: systems and elements – Optical modulator – Light wave temporal modulation
Reexamination Certificate
2000-08-10
2003-09-02
Lester, Evelyn (Department: 2873)
Optical: systems and elements
Optical modulator
Light wave temporal modulation
C359S351000, C257S461000, C257S465000, C257S466000, C257S444000, C257S448000, C257S003000, C250S338400, C250S370100, C250S492100, C250S492200, C385S146000, C385S129000
Reexamination Certificate
active
06614575
ABSTRACT:
BACKGROUND OF THE INVENTION
Field of the Invention
The invention relates to an optical structure which is suitable for modulating or for switching light. The invention also relates to a method for producing the optical structure.
Optoelectronic components are integrated monolithically with integrated circuits for various applications, for example for optical data transmission. In that case, semiconductor-based optical structures are required as a switch or modulator for light.
The utilization of dispersion by free charge carriers to modulate light is disclosed in a paper by G. V. Treyz et al. in Appl. Phys. Lett., Vol. 59, 1991, pages 771 ff, and in a paper by L. S. Yu et al. in Appl. Phys. Lett., Vol. 68, 1996, pages 1546 ff. A mesa-shaped structure in a silicon substrate is used in that case as a waveguide. The light is guided in the waveguide by total reflection. Free charge carriers which pass into the region of the waveguide through the use of dispersion are injected through a PIN diode which is polarized in the conducting direction. Those free charge carriers change the refractive index in the waveguide and thereby influence the total reflection. The waveguide is detuned in that way. A relatively long path is required for the waveguide in order to influence the light intensity due to the low possibility of detuning the waveguides.
SUMMARY OF THE INVENTION
It is accordingly an object of the invention to provide an optical structure with which light can be modulated and which can be implemented more compactly than known structures, as well as a method for producing the same, that overcome the hereinafore-mentioned disadvantages of the heretofore-known devices and methods of this general type.
With the foregoing and other objects in view there is provided, in accordance with the invention, an optical structure, comprising a substrate having a grating structure with a surface; the substrate having semiconductor material at least in a vicinity of the grating structure; the grating structure emitting at least one frequency band preventing light having a frequency from the at least one frequency band from propagating in the grating structure; the grating structure having a configuration of pores with a defective region, the pores disposed outside the defective region in a periodic array, and the periodic array disturbed in the defective region; and a conductive layer disposed at the surface of the grating structure, at least in a vicinity of the defective region.
With the objects of the invention in view, there is also provided a method for producing an optical structure, which comprises producing a periodic array of depressions in a main surface of an n-doped silicon substrate, the array having a defective region in which the periodic array is disturbed; etching pores in the silicon substrate starting from the depressions by electrochemical etching in an electrolyte in contact with the main surface, by connecting the silicon substrate as an anode and by setting a current density influencing etching erosion; and providing a conductive layer at a surface of a grating structure of the silicon substrate at least in a vicinity of the defective region.
In the optical structure according to the invention, a grating structure is provided in a substrate. The substrate has semiconductor material at least in the region of the grating structure. It is implemented, in particular, from a III-V semiconductor or from silicon.
The grating structure has a photonic band gap, that is to say it has the property that it emits at least one frequency band so that light having a frequency from this frequency band cannot propagate in the grating structure. The grating structure constitutes a dielectric grating at which this light undergoes Bragg reflection.
The grating structure is formed by a configuration of pores having essentially the same cross section. The cross section of the pores is preferably round. It can also be angular, for example square. The pores are disposed in a periodic array outside a defective region in the grating structure. In contrast, the periodic array is disturbed in the defective region. The disturbance can be a changed grating spacing between at least two pores, the absence of at least one pore, or at least one pore which is filled with another material or has a different diameter.
In accordance with another feature of the invention, the pores run essentially perpendicular to a main surface of the substrate. The optical structure can thereby be produced extremely simply.
The surface of the grating structure is provided with a conductive layer at least in the region of the defective region. The surface of the grating structure in this case also includes the entire surface of the pores. The conductive layer likewise clads the latter.
An optical structure which has a substrate with a grating structure having a photonic band gap and a defective region has already been proposed in German Published, Non-Prosecuted Patent Application DE 195 26 734 A1. However, the problem of modulating or switching light is not addressed in German Published, Non-Prosecuted Patent Application DE 195 26 734 A1.
Light from the frequency band which corresponds to the photonic band gap is guided in the defective region in the optical structure by virtue of the fact that it cannot propagate into the grating structure because of its wavelength. The defective region therefore constitutes a very narrow-band filter. The transmission through the defective region can be varied by virtue of the fact that the refractive index and/or absorption are varied within the defective region. Such a variation in refractive index can be achieved by varying the free charge carrier concentration in the defective region. Such a variation can also be achieved by virtue of the fact that the defective region is irradiated with light, the energy of which is above the band edge of the semiconductor material. The variation in refractive index is preferably achieved by virtue of the fact that charge carriers are injected into the defective region over the conductive layer. The conductive layer thereby renders it possible to modulate or switch the light simply.
In accordance with a further feature of the invention, the conductive layer is implemented by a doped zone which differs from the substrate in conductivity type and/or doping concentration. The substrate is doped in this case. If the doped zone differs from the substrate in the conductivity type, the pn junction which is thereby formed is polarized in the non-conducting direction so as to form a space charge zone which is poor in charge carriers. The result of this is that light can pass without hindrance. If the pn junction is polarized in the conducting direction, the defective region is flooded with charge carriers. Absorption and refractive index are changed thereby, and the light flux is interrupted.
Alternatively, the conductive layer is implemented as a layer made from conductive material which is located on the surface and is transparent to light. Doped polysilicon, metal or metal silicide is particularly suitable for the conductive layer. The thickness of the layer is dimensioned in such a way that it is transparent to light.
It is within the scope of the invention to place the defective region between optical conductors in order to use the defective region as a modulator or switch. Defective regions having a strip-shaped geometrical form are likewise used as optical conductors. The defective region, which acts as a switch, is disposed between the optical conductors. Alternatively, the defective region can be constructed on the basis of its geometrical form as an optical conductor, the transmission of which can be varied by changing the charge carrier concentration.
Further properties of the optical structure can be set through the shape of the periodic array. If the periodic array is square, the optical structure is suitable for polarized light. In this case, photonic band gaps which do not overlap result for the two directions of polarization. If, by contrast, the
Grüning Ulrike
Lehmann Volker
Reisinger Hans
Stengl Reinhard
Wendt Hermann
Greenberg Laurence A.
Infineon - Technologies AG
Lester Evelyn
Locher Ralph E.
Stemer Werner W.
LandOfFree
Optical structure and method for producing the same does not yet have a rating. At this time, there are no reviews or comments for this patent.
If you have personal experience with Optical structure and method for producing the same, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Optical structure and method for producing the same will most certainly appreciate the feedback.
Profile ID: LFUS-PAI-O-3060714