Claims Analysis
Total Claims: 9
Claim 1
Independent Claim
161 words
A non-reciprocal optical element, particularly for use as an isolator or circulator, and for connection to at least two monomode optical waveguides and which has a magneto-optical waveguide structure intended to be subjected to a transverse magnetic field directed perpendicularly to the direction of propagation of the optical wave, comprising: the magneto-optical waveguide structure being formed as a multimode waveguide which can propagate at least one fundamental mode and the first-order mode, the optical waveguides are located off-center with respect to the waveguide structure, at least one of the dimensions and the cross-sectional distribution of the refractive index of the optical waveguide structure is chosen to be such that the two modes have a reciprocal phase difference of π/2+2nπ and at least one of the magnetic field strength and the structure of the magneto-optical waveguide structure is chosen to be such that the two modes have non-reciprocal phase difference of π/2+2mπand in which n and m may be integers including 0.
Claim 2
Dependent Claim
161 words
A non-reciprocal optical element, particularly for use as an isolator or circulator, and for connection to at least two monomode optical waveguides and which has a magneto-optical waveguide structure intended to be subjected to a transverse magnetic field directed perpendicularly to the direction of propagation of the optical wave, comprising: the magneto-optical waveguide structure being formed as a multimode waveguide which can propagate at least one fundamental mode and the first-order mode, the optical waveguides are located off-center with respect to the waveguide structure, at least one of the dimensions and the cross-sectional distribution of the refractive index of the optical waveguide structure is chosen to be such that the two modes have a reciprocal phase difference of π/2+2nπ and at least one of the magnetic field strength and the structure of the magneto-optical waveguide structure is chosen to be such that the two modes have non-reciprocal phase difference of π/2+2mπand in which n and m may be integers including 0.
Claim 3
Dependent Claim
34 words
An arrangement as claimed in claim 1, characterized in that the magneto-optical waveguide structure is adapted to be influenced by a mechanical stress acting perpendicularly to the direction of propagation of the optical wave.
Claim 4
Dependent Claim
20 words
An arrangement as claimed in claim 1, characterized in that the magneto-optical waveguide structure consists of yttrium iron garnet (YIG).
Claim 5
Dependent Claim
34 words
An arrangement as claimed in claim 1, characterized in that the magneto-optical waveguide structure is provided on a substrate area and is approximately twice as wide as the monomode optical waveguides connected to it.
Claim 6
Dependent Claim
36 words
An arrangement as claimed in claim 1, characterized in that the magneto-optical waveguide structure is provided on the substrate at a height corresponding to approximately twice the height of the monomode optical waveguides connected to it.
Claim 7
Dependent Claim
30 words
An arrangement as claimed in claim 1, characterized in that in the device functions as a circulator and the magneto-optical waveguide structure is bilaterally connected to two monomode optical waveguides.
Claim 8
Dependent Claim
54 words
An arrangement as claimed in claim 1, characterized in that for use as an isolator each side of the magneto-optical waveguide structure is connected to a monomode optical waveguide essentially covering a peripheral half of the cross-sectional area of the magneto-optical waveguide structure, whilst the uncovered cross-sectional areas are provided with an absorbing layer.
Claim 9
Dependent Claim
59 words
An arrangement as claimed in claim 1, characterized in that a doping which is different from the neighbouring peripheral areas is applied in the central portion of the cross-sectional area of the magneto-optical waveguide structure in order to locally vary at least one of the refractive index and the magneto-optical constant in order to selectively influencing the fundamental mode.