IP Library › Granted Patent US 8,701,998
Granted Patent B2
US 8,701,998 · App. 12/602,677 · Granted Apr 22, 2014

System and method for strong photon localization by disordered photonic crystal structures

Inventors: Frank Vollmer (Cambridge, MA); Juraj Topolancik (Malden, MA)
Assignee: President and Fellows of Harvard College
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Quick Facts
Patent No.
US 8,701,998
App. No.
12/602,677
Granted
Apr 22, 2014
Kind
B2
Abstract

Periodic high-index-contrast photonic crystal (PhC) structures such as two-dimensional arrays of air holes in dielectric slabs inhibit light propagation in bands of frequencies and confine light in dislocations where the lattice periodicity is broken. The present invention is a conceptually different approach to photon localization in PhC structures. The disclosed design concept introduces structural perturbations uniformly throughout the fabricated crystal by deliberately changing the shape or orientations of elements that form the lattice. Optimized introduction of such random structural perturbations produces optical nanocavities with ultra-small modal volumes and high quality (Q) factors of over 250,000. Applications of such disordered photonic crystal structures are disclosed for optical sensing systems and random nano-lasers.

Claims (30)

1. An optical device comprising:

a slab, said slab comprising a material; and

a plurality of elements arranged in a lattice surrounding a photonic crystal waveguide, said lattice elements being formed in said slab by removing the material, with each said lattice element having a center located at a position (x,y), wherein first and second lattice elements differ in shape or orientation depending on their position (x,y) in the lattice, and said lattice is disordered due to randomized orientation of said lattice elements or geometrical perturbations introduced into said lattice elements, and wherein said lattice elements cause a localized guided light field of the waveguide; wherein said difference in the shape of said first and said second lattice elements is defined by a disorder function of permittivity Δ£(x,y) so that Δ£(x,y)=£ real (x,y)−£ ideal (x,y), where £ ideal (x,y) represents the permittivity of an ideal lattice with perfect translational symmetry, (x,y) correspond to any position (point) in the lattice, £ real (X,y) corresponds to the permittivity values at points (x,y).

2. The optical device according to claim 1 , wherein area of said lattice elements, spacing of said lattice elements, symmetry of said lattice and arrangement of said lattice elements is chosen so that the device exhibits photonic band gap.

3. The optical device according to claim 1 , wherein said slab material comprises one or more of the following: silicon, silicon nitride, Gallium-Arsenide, a metal, a semiconductor, a polymer, a composite material, quantum dots, quantum wells.

4. The optical device according to claim 1 , wherein said lattice elements have been removed at lattice positions (x,y) so that a row of missing elements is formed along a certain crystallographic direction of the lattice.

5. The optical device according to claim 1 , wherein said different shapes of the lattice elements comprise a circular shape where a radius r is parameterized as r(alpha,x,y), where alpha is an angle and (x,y) the position of the element in the lattice and r(alpha,x,y) is not a constant.

6. The optical device according to claim 1 , wherein said lattice elements comprise polygons and wherein orientations of said polygons is varied by rotating a given polygon by an angle alpha(x,y) that varies with the lattice position (x,y).

7. The optical device according to claim 1 , wherein said lattice elements comprise ellipses and wherein orientations of said ellipses is varied by rotating a major axis of a given ellipse by an angle alpha (x,y) that varies with the lattice position (x,y).

8. The optical device according to claim 1 , wherein a number of said lattice elements is removed to define a defect cavity, an add-drop filter, a Mach-Zehnder interferometer, or a waveguide.

9. The optical device according to claim 1 , wherein parts of the device surface are further modified by adding one of the following: photochromic molecules, protein, DNA, fluorophore, colloidal quantum dots, hydrogel, dextran, biotinylated polymers, antibodies, chelating ligands, biospecific recognition elements.

10. The optical device according to claim 1 , wherein said slab material further contains optical gain material such as wherein said optical gain material comprises at least one of quantum dots, quantum wells, one or more layers of quantum dots grown by molecular beam epitaxy, and one or more layers of quantum wells grown by molecular beam epitaxy.

11. The optical device according to claim 1 , wherein a tapered optical fiber tip is used to evanescently couple light to one or more lattice positions (x,y) where said lattice elements have been removed.

12. The optical device according to claim 1 that is exposed to a sample comprising one of the following: a solution, a gas, an aerosol, protein, DNA, viral particles, cells, body fluids.

13. The optical device according to claim 1 comprising a barcode label reader comprising the steps of:

measuring a scattering or transmission spectrum using a laser; recording said transmission spectrum on a computer; matching the spectrum to a database using computer algorithms.

14. A method for measurements of spectral features comprising the steps of:

excitation of an optical device using a tunable laser, said optical device comprising a slab, said slab comprising a material and a plurality of elements arranged in a lattice surrounding a photonic crystal waveguide, said lattice elements being formed in said slab by removing the material, with each said lattice element having a center located at a position (x,y), wherein first and second lattice elements differ in shape or orientation depending on their position (x,y) in the lattice and said difference in the shape of said first and said second lattice elements is defined by a disorder function of permittivity Δ£(x,y) so that Δ£(x,y)=£ real (x,y)−£ ideal (x,y), where £ ideal (x,y) represents the permittivity of an ideal lattice with perfect translational symmetry, (x,y) correspond to any position (point) in the lattice, £ real (X,y) corresponds to the permittivity values at points (x,y), and said lattice is disordered due to randomized orientation of said lattice elements or said geometrical perturbations introduced into said lattice elements, wherein said randomize orientation of said lattice elements or said geometrical perturbations introduced into said lattice elements produce localized mode devices in said photonic crystal waveguide;

detection of transmission or scattering or backscattering spectra using a photodetector; and

analysis of a recorded spectrum using a computer.

15. A method for tracking changes in spectral features of a optical device, said optical device comprising a slab, said slab comprising a material and a plurality of elements arranged in a lattice surrounding a photonic crystal waveguide, said lattice elements being formed in said slab by removing the material, with each said lattice element having a center located at a position (x,y), wherein first and second lattice elements differ in shape or orientation depending on their position (x,y) in the lattice and said difference in the shape of said first and said second lattice elements is defined by a disorder function of permittivity Δ£(x,y) so that Δ£(x,y)=£ real (x,y)−£ ideal (x,y), where £ ideal (x,y) represents the permittivity of an ideal lattice with perfect translational symmetry, (x,y) correspond to any position (point) in the lattice, £ real (X,y) corresponds to the permittivity values at points (x,y), and said lattice is disordered due to randomized orientation of said lattice elements or geometrical perturbations introduced into said lattice elements, wherein said randomize orientation of said lattice elements or said geometrical perturbations introduced into said lattice elements produce localized mode devices in said photonic crystal waveguide, comprising the steps of:

identifying a wavelength associated with a minima or maxima in a recorded spectral feature using computer algorithms;

recording the wavelengths of said minima or maxima over time; and plotting a time trace of said recorded wavelengths for further analysis with a computer.

16. A method for tracking changes in spectral features of a device, said device comprising a slab, said slab comprising a material and a plurality of elements arranged in a lattice surrounding a photonic crystal waveguide, said lattice elements being formed in said slab by removing the material, with each said lattice element having a center located at a position (x,y), wherein first and second lattice elements differ in shape or orientation depending on their position (x,y) in the lattice and said difference in the shape of said first and said second lattice elements is defined by a disorder function of permittivity Δ£(x,y) so that Δ£(x,y)=£ real (x,y)−£ ideal (x,y), where £ ideal (x,y) represents the permittivity of an ideal lattice with perfect translational symmetry, (x,y) correspond to any position (point) in the lattice, £ real (X,y) corresponds to the permittivity values at points (x,y) and said lattice is disordered due to randomized orientation of said lattice elements or geometrical perturbations introduced into said lattice elements, wherein said randomize orientation of said lattice elements or said geometrical perturbations introduced into said lattice elements produce localized mode devices in said photonic crystal waveguide, comprising the steps of:

recording spectral features before exposure to a sample; exposing said device to said sample; recording spectral features during and after sample exposure; and

analyzing changes in spectral features using computer algorithms.

17. The method for tracking changes in spectral features of a device according to claim 16 , wherein said step of exposing said device to the sample comprises the steps of:

sample delivery by microfluidic flow, electrophoretic flow, aerosol flow or by electrowetting;

exposure of said device to said sample for a certain time period; and

removing of said sample by exposing said optical device to a second microfluidic or electrophoretic flow.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 6, 2010
From: TOPOLANCIK, JURAJ; VOLLMER, FRANK
To: PRESIDENT AND FELLOWS OF HARVARD COLLEGE
Reel/Frame 024800/0689 →
Continuity (3)
Provisional Application 60941950 · Jun 4, 2007
Provisional Application 60980816 · Oct 18, 2007
Related Publication 20100176200A1 · Jul 15, 2010