Superlattice quantum well material

• US 5,550,387 A
• Filed: 08/29/1994
• Issued: 08/27/1996
• Est. Priority Date: 01/24/1994
• Status: Expired due to Term

• Current Assignee: HI-Z Technology, Inc.
• Original Assignee: HI-Z Corporation
• Inventors: Elsner, Norbert B., Ghamaty, Saeid
• Primary Examiner(s): SAADAT, MAHSHID D
• Application Number:
  US08/297,601
• Time in Patent Office: 729 Days
• Field of Search: 257/15, 257/18, 257/613, 257/614, 257/616, 257/625, 257/930, 62/3.2, 136/203
• US Class Current: 257/15
• CPC Class Codes: H01L 29/16 including, apart from doping materials or other impurities, only elements of Group IV of the Periodic Table
• CPC Class Codes: H10N 10/855 comprising compounds containing boron, carbon, oxygen or nitrogen
• CPC Class Codes: Y10S 257/93 Thermoelectric, e.g. peltier effect cooling

Abstract

A thermoelectric element having a very large number of alternating layers of semiconductor material. The alternating layers all have the same crystalline structure. The inventors have demonstrated that materials produced in accordance with this invention provide figures of merit more than six times that of prior art thermoelectric materials. A preferred embodiment is a superlattice of Si, as a barrier material, and SiGe, as a conducting material, both of which have the same cubic structure. Another preferred embodiment is a superlattice of B--C alloys, the layers of which would be different stoichiometric forms of B--C but in all cases the crystalline structure would be alpha 0. In a preferred embodiment the layers are grown under conditions as to cause them to be strained at their operating temperature range in order to improve the thermoelectric properties.

Claims

1. A thermoelectric element for use in a thermoelectric device comprised of:

a plurality of alternating layers of at least two different semiconducting materials, the first of said two materials, defining a barrier material and the second of said two materials defining a conducting material, said alternating materials defining band gaps,

said barrier material and said conducting material being strained having the same crystalline structure,

said barrier material having a band gap higher than the band gap of said conducting material,

said conducting material being doped to create conducting properties,

said layer arrangement of said at least two different materials creating a superlattice and quantum wells within said layers of said conducting material.

2. A thermoelectric element as in claim 1 wherein said crystal structure is cubic.

3. A thermoelectric element as in claim 2 wherein said barrier material is silicon and said conducting material is silicon germanium.

4. A thermoelectric element as in claim 3 wherein the concentration of germanium in said conducting material is between 10 percent and 40 percent.

5. A thermoelectric element as in claim 4 wherein said conducting material is doped with a dopant.

6. A thermoelectric element as in claim 5 wherein said dopant is an n-type dopant.

7. A thermoelectric element as in claim 5 wherein said dopant is a p-type dopant.

8. A thermoelectric element as in claim 1 wherein said plurality of alternating layers is at least 100 layers with each of said 100 layers being less than 100 A thick.

9. A thermoelectric element as in claim 1 wherein said crystal structure is alpha rhombohedral.

10. A thermoelectric element as in claim 4 wherein at least one of said two different materials is an alloy of boron and carbon.

11. A thermoelectric element as in claim 4 wherein at least two of said at least two different materials are both alloys of boron and carbon.

12. A thermoelectric element as in claim 1 wherein said barrier material is strained in tension and said conduction material is strained in compression.

13. A thermoelectric element as in claim 1 wherein said element defines an operating temperature range and is fabricated at a temperature higher than said operating temperature range so as to cause said barrier material and said conduction material to be strained.