Summary of the invention
In view of this, be necessary to provide a kind of optically coupled device that improves light utilization efficiency.
A kind of optically coupled device, it comprises that a substrate, one are formed at this suprabasil planar light waveguide, dielectric grating and an a pair of electrode that is arranged on this planar light waveguide and is positioned at these dielectric grating both sides being formed on this planar light waveguide.This planar light waveguide is for docking to receive with a LASER Light Source laser beam that this LASER Light Source is sent.This dielectric grating edge is parallel to the incident direction setting of this laser beam, and forms diffraction type optical waveguide lens (diffractive waveguide lens) to assemble this laser beam with this planar light waveguide.Thereby this changes the focal length of this diffraction type optical waveguide lens to change the refractive index of this planar light waveguide by electrooptical effect for load-modulate electric field to electrode.
According to integrated optics theory, this dielectric grating and this planar light waveguide form loaded type optical waveguide (strip/grating loaded waveguide), and the equivalent refractive index that this planar light waveguide loads the part of this dielectric grating becomes large.So, by the structure of this dielectric grating is rationally set, for example, be arranged to chirp grating (chirped grating) and just can form the diffraction type optical waveguide lens of a chirp grating type.Thereby and this can change the refractive index of this planar light waveguide by load-modulate electric field to electrode by electrooptical effect, thereby change the focal length of this diffraction type optical waveguide lens, effectively this laser beam is assembled into optical element.
Embodiment
Refer to Fig. 1 and Fig. 2, the optically coupleddevice 10 of preferred embodiments of the present invention comprises that asubstrate 110, one are formed at planar light waveguide in thissubstrate 110 120, one and are formed atdielectric grating 130 and a pair ofelectrode 140 that is arranged on thisplanar light waveguide 120 and is set in parallel in thesedielectric grating 130 both sides on this planar light waveguide 120.Thisplanar light waveguide 120 is for docking to receive thelaser beam 21 that this LASER Light Source 20 is sent with a LASER Light Source 20.Thesedielectric grating 130 edges are parallel to the incident direction setting of thislaser beam 21, and form a diffraction type optical waveguide lens to assemble thislaser beam 21 with this planar light waveguide 120.Thereby this changes the focal length of this diffraction type optical waveguide lens to change the refractive index of thisplanar light waveguide 120 by electrooptical effect for load-modulate electric field toelectrode 140.
According to integrated optics theory, thisdielectric grating 130 forms loaded type optical waveguide with thisplanar light waveguide 120, and the equivalent refractive index that this planar light waveguide 120 loads the part of thisdielectric grating 130 becomes large.So, by the structure of thisdielectric grating 130 is rationally set, for example, be arranged to chirp grating and just can form the diffraction type optical waveguide lens of a chirp grating type.Thereby and this can change the refractive index of thisplanar light waveguide 120 by load-modulate electric field toelectrode 140 by electrooptical effect, thereby change the focal length of this diffraction type optical waveguide lens, effectively thislaser beam 21 is assembled into anoptical element 30.
Thissubstrate 110 is substantially rectangular, and comprises anend face 111 and aside 112 being connected with this end face 111.Due to lithium niobate (LiNbO3) crystal (LN) has higher reaction velocity, and consider that lithium niobate diffuse metal titanium (simple substance) can form the loaded lightguide of gradually changed refractive index type, therefore, the material of thissubstrate 110 adopts lithium columbate crystal.
Thisplanar light waveguide 120 diffuses into thissubstrate 110 by Titanium and forms by plate after Titanium high temperature to this end face 111.So, loading after thisdielectric grating 130, the refractive index generation gradual change of thisplanar light waveguide 120, is the advantage that produces the diffraction type optical waveguide lens of chirp grating type.In the present embodiment, to shape that should substrate 110, thisplanar light waveguide 120 is rectangle, and thisend face 111 is the end face of thisplanar light waveguide 120, and thisside 112 is the side of thisplanar light waveguide 120.
Thisdielectric grating 130 forms by the end face from this planar light waveguide 120 (i.e. this end face 111) thisplanar light waveguide 120 of etching, and therefore material also has the lithium columbate crystal of Titanium for diffusion.Thisdielectric grating 130 can be a chirp grating.Concrete, thisdielectric grating 130 comprisesmedium part 131 multiple rectangles, that be arranged in parallel, the plurality ofmedium part 131 arranges perpendicular to thisside 112, and highly basic identical.The number of the plurality ofmedium part 131 is odd number, and symmetrical about an axis of symmetry O, and along this axis of symmetry O to the direction away from this axis of symmetry O, the width of thismedium part 131 is more and more less, and the gap of adjacent two thesemedium parts 131 is also more and more less.
Refer to Fig. 3, in present embodiment, taking the Width of this
dielectric grating 130 as
axle, this axis of symmetry O with
the joining of axle is initial point, along this axis of symmetry O to away from the direction of this axis of symmetry O being
axle forward, exists with this
laser beam 21
place with the phase differential at initial point place is
axle, can obtain according to planar light waveguide wave theory:
, wherein
.Of this
medium part 131
individual border
meet following condition:
, wherein,
for positive integer,
(for forming this diffraction type optical waveguide lens),
and
for constant relevant to the focal length of this diffraction type optical waveguide lens.So, can be derived from:
.And
situation, the border of this
medium part 131 on this axis of symmetry O left side can obtain by symmetry.
The interpolar electric field that this produces after load-modulate
electric field electrode 140
to cross this
planar light waveguide 120, thereby can further change the equivalent refractive index of this
planar light waveguide 120, change equivalently the refractive power (being focal length) of the diffraction type optical waveguide lens of chirp grating type, thereby can be coupled this LASER
Light Source 10 and this
optical element 30 that arrange with various distances.This length to
electrode 140 and be greater than or equal to highly respectively length and the height of this
dielectric grating 130, this length to
electrode 140 and highly equal this by the length of this
dielectric grating 130 and height in present embodiment.
This LASER Light Source 20 adopts distributed feedback laser (distributed feedback laser, DFB), it belongs to the semiconductor laser of side-emitted, can luminous side be welded direct on thisside 112 by chips welding (die bond) mode, so that thislaser beam 21 is along this axis of symmetry O incident.Certainly, this LASER Light Source 20 also can adopt other types LASER Light Source, and arranges by other means, as long as ensure that it can be along thislaser beam 21 of this axis of symmetry O outgoing.
Thisoptical element 30 can be strip optical waveguide, optical fiber or optical splitter (splitter).In present embodiment, thisoptical element 30 is strip optical waveguide.
In a word; those skilled in the art will be appreciated that; above embodiment is only for the present invention is described; and be not used as limitation of the invention; as long as within connotation scope of the present invention, within the appropriate change that above embodiment is done and variation all drop on the scope of protection of present invention.