IP Library Granted Patent US 9,068,883
Granted Patent B2
US 9,068,883 · App. 14/149,321 · Granted Jun 30, 2015

Compact, low cost raman monitor for single substances

Inventors: Boris Leonidovich Volodin (Pennington, NJ); Vladimir Sinisa Ban (Princeton, NJ)
Assignee: PD-LD, Inc.
G01J3/10G01J3/4412G01N21/65G01N21/658G01N2021/1793G01N2201/0221G01N2201/129G01N2201/1296G01J3/0256G01J3/1895G01J3/44G02B6/29319
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Quick Facts
Patent No.
US 9,068,883
App. No.
14/149,321
Granted
Jun 30, 2015
Kind
B2
Abstract

Apparatus for performing Raman spectroscopy may include a first laser source having a first emission wavelength and a second laser source having a second emission wavelength. A separation between the first and second emission wavelengths may correspond to a width of a Raman band of a substance of interest. A switch may provide switching between the first and second laser sources. An ensemble of individually addressable laser emitters may be provided. A Bragg grating element may receive laser light from the ensemble. An optical system may direct light from the Bragg grating element into an optical fiber. A combined beam through the optical fiber may contain light from each of the emitters.

Claims (26)

1. Apparatus for performing Raman spectroscopy, the apparatus comprising:

an ensemble of individually addressable laser emitters, the ensemble being adapted to emit first laser light having a first wavelength and second laser light having a second wavelength, wherein a separation between the first and second wavelengths corresponds to a width of a Raman band of a substance of interest;

a Bragg grating element that is adapted to receive the first laser light and the second laser light, the Bragg grating element comprising a three-dimensional bulk of optical material having recorded therein a first Bragg grating having a first period and a second Bragg grating having a second period; and

an optical system that is adapted to form a combined beam that contains light at each of the first and second wavelengths.

2. The apparatus of claim 1 , further comprising a beam transformation system that receives the first laser light and the second laser light, and rotates images of the laser emitters by 90 degrees.

3. The apparatus of claim 1 , wherein each of the laser emitters is a p-n junction.

4. The apparatus of claim 1 , wherein the laser emitters are respective p-n junctions in a single chip.

5. The apparatus of claim 1 , wherein the laser emitters are individually addressable to emit respective laser light sequentially.

6. The apparatus of claim 2 , further comprising a fast-axis collimator between the ensemble of laser emitters and the beam transformation system, and a slow-axis collimator between the beam transformation system and the optical system.

7. The apparatus of claim 1 , wherein the Bragg grating element reflects a respective portion of the light it receives from each of the emitters back into the emitters as a narrowband seed that causes each of the emitters to lase at its respective wavelength.

8. The apparatus of claim 1 , wherein the ensemble is further adapted to emit third laser light having a third wavelength, and wherein a separation between the second and third wavelengths corresponds to a width of a second Raman band of the substance of interest.

9. The apparatus of claim 1 , wherein the ensemble is further adapted to emit third laser light having a third wavelength, and wherein a separation between the second and third wavelengths corresponds to a width of a Raman band of a second substance of interest.

10. The apparatus of claim 1 , wherein the Bragg grating element has a longitudinal axis, and has recorded therein a Bragg grating having a period that varies as a function of position along the longitudinal axis of the Bragg grating element.

11. Apparatus for performing Raman spectroscopy, the apparatus comprising:

an ensemble of individually addressable laser emitters, the ensemble comprising a first laser emitter that emits laser light having a first wavelength and a second laser emitter that emits laser light having a second wavelength, wherein a separation between the first and second wavelengths corresponds to a width of a Raman band of a substance of interest;

a Bragg grating element that receives the laser light from the laser emitters, the Bragg grating element comprising a three-dimensional bulk of optical material having recorded therein a first Bragg grating having a first period and a second Bragg grating having a second period; and

an optical system that forms a combined beam that contains light from each of the first emitter and the second emitter.

12. The apparatus of claim 11 , further comprising a beam transformation system that receives the laser light from the laser emitters and rotates images of the laser emitters by 90 degrees.

13. The apparatus of claim 11 , wherein each of the first and second laser emitters is a p-n junction.

14. The apparatus of claim 11 , wherein the first and second laser emitters are respective p-n junctions in a single chip.

15. The apparatus of claim 11 , wherein the first and second laser emitters are individually addressable to emit respective laser light sequentially.

16. The apparatus of claim 12 , further comprising a fast-axis collimator between the ensemble of laser emitters and the beam transformation system, and a slow-axis collimator between the beam transformation system and the optical system.

17. The apparatus of claim 11 , wherein the Bragg grating element reflects a respective portion of the light it receives from each of the emitters back into the emitters as a narrowband seed that causes each of the emitters to lase at its respective wavelength.

18. The apparatus of claim 11 , wherein the ensemble comprises a third laser emitter that emits laser light having a third wavelength, wherein a separation between the second and third wavelengths corresponds to a width of a second Raman band of the substance of interest.

19. The apparatus of claim 11 , wherein the ensemble comprises a third laser emitter that emits laser light having a third wavelength, wherein a separation between the second and third wavelengths corresponds to a width of a Raman band of a second substance of interest.

20. The apparatus of claim 11 , wherein the Bragg grating element has a longitudinal axis, and has recorded therein a Bragg grating having a period that varies as a function of position along the longitudinal axis of the Bragg grating element.

Assignments (1)
MERGER AND CHANGE OF NAME Recorded Sep 8, 2016
From: PD-LD, INC.; NECSEL INTELLECTUAL PROPERTY, INC.
To: NECSEL INTELLECTUAL PROPERTY, INC.
Reel/Frame 039953/0595 →
Continuity (7)
Continuation 14013359 · Aug 29, 2013
Continuation 13547469 · Jul 12, 2012
Continuation In Part 13361072 · Jan 30, 2012
Continuation 13165333 · Jun 21, 2011
Continuation 11923571 · Oct 24, 2007
Provisional Application 60854339 · Oct 24, 2006
Related Publication 20140125977A1 · May 8, 2014