IP Library Granted Patent US 10,882,938
Granted Patent B2
US 10,882,938 · App. 16/287,421 · Granted Jan 5, 2021

Quasicrystalline structures and uses thereof

Inventors: Paul Joseph Steinhardt (Princeton, NJ); Paul Michael Chaikin (New York, NY); Weining Man (Princeton, NJ)
Assignee: The Trustees of Princeton University
C08F220/56B82Y20/00B82Y30/00C08F222/385C08G59/245C08G65/22G02B6/1225H01L33/002B33Y80/00
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Quick Facts
Patent No.
US 10,882,938
App. No.
16/287,421
Granted
Jan 5, 2021
Kind
B2
Abstract

This invention relates generally to the field of quasicrystalline structures. In preferred embodiments, the stopgap structure is more spherically symmetric than periodic structures facilitating the formation of stopgaps in nearly all directions because of higher rotational symmetries. More particularly, the invention relates to the use of quasicrystalline structures for optical, mechanical, electrical and magnetic purposes. In some embodiments, the invention relates to manipulating, controlling, modulating and directing waves including electromagnetic, sound, spin, and surface waves, for pre-selected range of wavelengths propagating in multiple directions.

Claims (6)

1. The method of using a quasicrystalline composition of matter to produce a device, said method comprising: a) providing a quasicrystalline composition comprising dielectric material elements; b) arranging said material elements such that said quasicrystalline composition has at least a five-fold symmetry axis and not a six-fold symmetry axis; and c) selecting said material elements such that said composition is a dielectric heterostructure that exhibits a photonic band structure of corresponding symmetry, forbidden in crystals in a two- or three-dimensional space, and characterized by a complete band gap, so as to produce a device comprising said quasicrystalline composition, wherein said device comprising said quasicrystalline composition emits radiation.

2. The method of claim 1 , wherein said radiation is substantially only within the visible spectrum.

3. A device comprising said quasicrystalline composition comprising dielectric material elements, wherein

a) said material elements are arranged such that said quasicrystalline composition has at least a five-fold symmetry axis and not a six-fold symmetry axis; and

b) said material elements are selected such that said composition is a dielectric heterostructure that exhibits a photonic band structure of corresponding symmetry, forbidden in crystals in a two- or three-dimensional space, and characterized by a complete hand gap, wherein said device emits radiation.

4. The device of claim 3 , wherein said radiation is substantially only within the visible spectrum.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Mar 5, 2019
From: STEINHARDT, PAUL J.; CHAIKIN, PAUL MICHAEL; MAN, WEINING
To: THE TRUSTEES OF PRINCETON UNIVERSITY
Reel/Frame 048507/0575 →
Continuity (9)
Continuation 15410396 · Jan 19, 2017
Continuation 14059003 · Oct 21, 2013
Continuation 13906792 · May 31, 2013
Continuation 13553149 · Jul 19, 2012
Continuation 13271969 · Oct 12, 2011
Continuation 11988480
Provisional Application 60697829 · Jul 8, 2005
Provisional Application 60697872 · Jul 8, 2005
Related Publication 20190248941A1 · Aug 15, 2019