Magnetic photonic crystal structure for providing spatial frequency asymmetry for light propagating in different directions

• US 7,570,414 B2
• Filed: 06/17/2005
• Issued: 08/04/2009
• Est. Priority Date: 11/23/2004
• Status: Active Grant

• Current Assignee: Corning Incorporated
• Original Assignee: Corning Incorporated
• Inventors: Wight, John Forrest Jr., Allan, Douglas Clippinger, Borrelli, Nicholas Francis, Koch, Karl William III
• Primary Examiner(s): Sugarman; Scott J
• Assistant Examiner(s): Thomas; Brandi N
• Application Number:
  US11/156,042
• Publication Number:
  US 20060109530A1
• Time in Patent Office: 1,509 Days
• Field of Search: 359/280, 359/248, 359/252, 359298-300, 359/321, 359/586, 359652-655, 359241-244, 385/8, 385/122, 385/141, 385/147
• US Class Current: 359/280
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: G02B 6/1225 comprising photonic band-gap structures or photonic lattices

Abstract

A magnetic photonic crystal for providing asymmetry of spatial frequencies in the propagation of light is provided. The crystal is formed from at least two materials having different indices of refraction which are aligned along the longitudinal axis of the crystal. And arranged in an array whose symmetry does not include a spatial inversion operator such that (x,y)==/=(−x,−y). One or more of the materials forming the array is magnetic such that the magnetic group representation of the array does not include time inversion as a symmetric operator. In operation, when the magnetic material forming the material is magnetized, the group velocity property of light propagated in one direction along the axis of the array is different from the group velocity property of light transmitted in an opposite direction through the array. The magnetic photonic crystal may be used, for example, as an optical memory device or a high speed modulator/demodulator.

Claims

1. A medium for providing asymmetry of spatial frequencies in the propagation of electromagnetic radiation such that F(k)≠

F(−

k), where F is the frequency and k is the direction of propagation of the radiation, comprising;

at least two materials having different dielectric constants, said two materials being transmissive of said radiator and aligned along a direction of propagation in a two dimensional periodic array whose symmetry does not include a spatial inversion operator such that (x, y)≠

(−

x,−

y),

wherein one or more of the materials forming said array is magnetic such that the magnetic group representation of the array does not include time inversion as a symmetry operator.

2. The medium defined in claim 1, wherein at least one of the materials forming the array is selected from the point group classifications of magnetic materials that do not include time inversion as an included symmetry operation.

3. The medium defined in claim 1, wherein said beam of electromagnetic radiation is light, and said two materials have different indices of refraction.

4. The medium defined in claim 2, wherein said two materials are transparent.

5. The medium defined in claim 3, wherein one of said materials is a glass-ceramic composite.

6. The medium defined in claim 3, wherein one of said materials is a gas.

7. The medium defined in claim 5, wherein said gaseous material is air.

8. The medium defined in claim 3, wherein one of the materials is a vacuum.

9. The medium defined in claim 3, wherein said two materials are a magnetic glass-ceramic composite and air, respectively.

10. The medium defined in claim 8, wherein said periodic array is formed by a pattern of air-filled openings in said magnetic glass-ceramic composite.

11. The medium defined in claim 2, wherein said spectral asymmetry is sufficient to change the group velocity property of light through said medium to a near-zero speed.

12. The medium defined in claim 1, wherein said medium is a magnetic photonic crystal having air holes through its core and being formed from a magnetic ceramic composite selected from 58 of 122 point group classifications of magnetic materials which do not include time inversion as an included symmetry operator, said air holes forming said two-dimensional periodic array having no spatial inversion symmetry across a cross-section of said crystal transverse to a direction of propagation of said light.

13. The medium defined in claim 1, comprising an extruded magnetic material having air holes along an axis forming said array.