IP Library Granted Patent US 10,326,036
Granted Patent B2
US 10,326,036 · App. 15/636,775 · Granted Jun 18, 2019

Device with a quantum well layer

Inventors: Stephen Sweeney (Stevenage, GB); Yaping Zhang (Stevenage, GB)
Assignee: ASTRIUM LIMITED
H01L31/035236B82Y20/00G01J3/0205G01J3/0259G01J3/42G02B6/29341G02F1/01708G06F17/5045H01L27/1446H01L31/02325G02F2001/0155
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 10,326,036
App. No.
15/636,775
Granted
Jun 18, 2019
Kind
B2
Abstract

A device for guiding and absorbing electromagnetic radiation, the device including: absorbing means for absorbing the electromagnetic radiation; and a coupled to the absorbing means for guiding the electromagnetic radiation to the absorbing means, wherein the waveguide and the absorbing means are formed from a structure including a first cladding layer, a second cladding layer over the first cladding layer, and a quantum-well layer between the first and second cladding layers, the quantum-well layer being formed of a material having a different composition to the first and second cladding layers, wherein the thickness and the composition of the quantum-well layer is optimised to provide an acceptable level of absorption of electromagnetic radiation in the waveguide while providing an appropriate band gap for absorption of the electromagnetic radiation in the absorbing means.

Claims (21)

1. A method of optimising a layer thickness and composition of a quantum-well layer for a device for guiding and absorbing electromagnetic radiation, the device comprising a substrate; at least one resonator located on the substrate for absorbing the electromagnetic radiation, the or each of the at least one resonators being resonant at a predetermined wavelength of radiation; a waveguide on the substrate, the waveguide being coupled to the at least one resonator for guiding the electromagnetic radiation to the at least one resonator, wherein the waveguide and the at least one resonator are formed from a structure comprising a first cladding layer, a second cladding layer over the first cladding layer, and the quantum-well layer between the first and second cladding layers, the quantum-well layer being formed of a material having a different composition to the first and second cladding layers, the method comprising:

determining an appropriate quantum well ground state transition energy for the quantum-well layer for absorption of the electromagnetic radiation in the at least one resonator; and

determining the thickness and the composition of the quantum well that are configured to provide the desired ground state transition energy and provide an acceptable level of absorption in the waveguide, while maximizing a quality Q factor of resonance of the at least one resonator and keeping the strain within the quantum-well layer lower than a predetermined limit,

wherein determining the thickness and the composition of the quantum well comprises:

selecting an initial thickness and composition of the quantum-well layer from a predetermined range of thicknesses and compositions;

determining a bend loss in the at least one resonators based on the initial thickness and composition;

obtaining a value of the Q factor for the resonator, based on the bend loss;

determining whether the obtained value of the Q factor is a maximum available value of the Q factor within the predetermined range of thicknesses and compositions;

obtaining a value of strain in the quantum-well layer based on the selected thickness and composition;

determining whether the obtained value of the strain is below the predetermined acceptable limit; and

using the selected thickness and composition as the final thickness and composition of the quantum-well layer, if it is determined that the value of the Q factor is a maximum available value, and if the obtained strain is below the predetermined acceptable limit.

2. The method of claim 1 , wherein the predetermined acceptable limit is 1.5%.

3. The method of claim 1 , further comprising, if it is determined that the value of the Q factor for the initial thickness and composition is not a maximum value or if the obtained strain is not below the predetermined acceptable limit, adjusting the initial thickness and composition to obtain a new thickness and composition and repeating the steps of obtaining a bend loss, determining a Q factor value, determining whether the obtained value is a maximum, obtaining a strain value and determining whether the obtained strain value is below a predetermined acceptable limit for the new thickness and composition.

4. The method of claim 3 , wherein the initial thickness and composition are selected based on a target value of a band gap for the quantum-well layer.

5. The method of claim 4 , wherein the at least one resonator has a minimum free-spectral range FSR value, the method further comprising:

obtaining a wavelength difference value that is less than a minimum FSR value of the plurality of resonators; and

obtaining the target value of the band gap by obtaining a value corresponding to the energy of radiation at a wavelength equal to the sum of the wavelength difference value and the predetermined wavelength.

6. The method of claim 1 , wherein the acceptable level of absorption in the waveguide is a minimum level of absorption obtainable within a predetermined range of thicknesses and compositions of the quantum-well layer, such that the thickness and composition of the quantum-well is optimised to minimise absorption in the waveguide.

7. The method of claim 1 , wherein the thickness of the quantum-well layer is determined to be substantially less than a thickness of the waveguide.

8. The method of claim 1 , wherein the device is a spectrometer.

9. The method of claim 8 , wherein the thickness and the composition of the quantum well are determined so as provide a band-gap that is less than or equal to a predetermined energy, the predetermined energy corresponding to a maximum wavelength Amax of electromagnetic radiation that the spectrometer is configured to detect.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 28, 2020
From: AIRBUS DEFENCE AND SPANCE LIMITED
To: ZINIR LIMITED
Reel/Frame 054187/0605 →
CHANGE OF NAME Recorded Oct 26, 2020
From: ASTRIUM LIMITED
To: AIRBUS DEFENCE AND SPANCE LIMITED
Reel/Frame 054161/0023 →
Priority Claims (1)
EP 11275125 · Oct 14, 2011 · regional
Continuity (2)
Continuation 14351696
Related Publication 20170309763A1 · Oct 26, 2017
Cited By (8)
US 12,193,800 US 12,390,117 US 12,396,648 US 12,484,796 US 12,490,934 US 12,578,323 US 12,685,449 US 12,733,827