Probe assembly and method for contactless electrical characterization of buried conducting layers
US-2015022223-A1 · Jan 22, 2015 · US
US10215796B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10215796-B2 |
| Application number | US-201615151216-A |
| Country | US |
| Kind code | B2 |
| Filing date | May 10, 2016 |
| Priority date | May 11, 2015 |
| Publication date | Feb 26, 2019 |
| Grant date | Feb 26, 2019 |
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A system and a method determine a quality of a doped semiconductor layer in terms of a charge carrier density gradient by measuring two magnetic-field-dependent resistances using four contacts of a specimen.
Opening claim text (preview).
We claim: 1. A system, comprising: a measuring device including terminal contacts, the terminal contacts contacting a specimen of a semiconductor, where the measuring device applies a current and measures the voltage at the terminal contacts to determine a quality of the specimen in terms of a charge carrier density gradient by measuring two magnetic-field-dependent resistances using the terminal contacts. 2. The system of claim 1 , where the measuring device extracts either an angle or a magnitude of the charge carrier density gradient, or both the angle and the magnitude of the charge carrier density gradient. 3. The system of claim 2 , where the charge carrier density gradient reveals a density distribution of a surrounding area of the specimen, allowing estimates of neighboring densities to be accurately made. 4. The system of claim 1 , where the charge carrier density gradient reveals a density distribution of the surrounding area of the specimen, allowing estimates of neighboring densities to be accurately made. 5. The system of claim 1 , further comprising examining a few scattered specimen from a large area of the semiconductor to determine a uniformity of a density distribution over an entire semiconductor without testing every position. 6. The system of claim 1 , where an angle of the charge carrier density gradient θ = tan - 1 ( η y η x ) is determined by application of magnetic field. 7. The system of claim 1 , where a magnitude of the charge carrier density gradient |η|=√{square root over (η x 2 +η y 2 )} is determined by application of magnetic field. 8. The system of claim 1 , where the terminal contacts rotate the charge carrier density gradient angle by about 45 degrees to measure the charge carrier density gradient. 9. The system of claim 1 , where a number of terminal contacts comprises at least four. 10. The system of claim 9 , where only two magnetic-field-dependent resistances are measured using the at least four terminal contacts. 11. A method, comprising: contacting a specimen at terminal contacts; applying a current and measuring a voltage at the terminal contacts; and measuring two magnetic-field-dependent resistances using the terminal contacts to determine a quality of the specimen in terms of a charge carrier density gradient. 12. The method of claim 11 , where the measuring extracts both an angle and a magnitude of the charge carrier density gradient. 13. The method of claim 12 , where the charge carrier density gradient reveals a density distribution of a surrounding area of the specimen, allowing estimates of neighboring densities to be accurately made. 14. The method of claim 11 , where the charge carrier density gradient reveals a density distribution of the surrounding area of the specimen, allowing estimates of neighboring densities to be accurately made. 15. The method of claim 11 , further comprising: examining a few scattered specimen from a large area of the semiconductor; and determining a uniformity of a density distribution over an entire semiconductor without testing every position. 16. The method of claim 11 , further comprising determining an angle of the charge carrier density gradient θ = tan - 1 ( η y η x ) by applying a magnetic field. 17. The method of claim 11 , determining a magnitude of the charge carrier density gradient |η|=√{square root over (η x 2 +η y 2 )} from applying a magnetic field. 18. The method of claim 11 , further comprising rotating the charge carrier density gradient angle by about 45 degrees to measure the charge carrier density gradient. 19. The method of claim 11 , where a number of terminal contacts comprises at least four. 20. The method of claim 19 , where only two magnetic-field-dependent resistances are measured using the at least four terminal contacts.
Characterising semiconductor materials (testing of materials or semi-finished products G01R31/2831; testing during manufacture H10P74/00) · CPC title
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