PHOTOACOUSTIC MICROCANTILEVERS

• US 20100033723A1
• Filed: 06/19/2009
• Published: 02/11/2010
• Est. Priority Date: 08/11/2008
• Status: Active Grant

• Current Assignee: University of Tennessee Research Foundation (University of Teesside), UT-Battelle LLC
• Original Assignee: UT-Battelle LLC
• Inventors: Brown, Gilbert M., Van Neste, Charles W., Thundat, Thomas G., Senesac, Lawrence R.
• Granted Patent: US 8,194,246 B2
• Time in Patent Office: Days
• US Class Current: 356/432
• CPC Class Codes: G01N 21/1702 with opto-acoustic detection, e.g. for gases or analysing solids
• CPC Class Codes: G01N 29/2418 using optoacoustic interaction with the material, e.g. laser radiation, photoacoustics photoacoustic cells G01N21/1702; measuring characteristics of vibrations by using radiation-sensitive means G01H9/00; acousto-optical conversion techniques for short-range imaging G01S15/8965; sound-producing devices using laser bundle G10K15/046

Abstract

A system generates a photoacoustic spectrum in an open or closed environment with reduced noise. A source focuses a beam on a target substance disposed on a base. The base supports a cantilever that measures acoustic waves generated as light is absorbed by the target substance. By focusing a chopped/pulsed light beam on the target substance, a range of optical absorbance may be measured as the wavelength of light changes. An identifying spectrum of the target may detected by monitoring the vibration intensity variation of the cantilever as a function of illuminating wavelength or color.

Claims

1. An apparatus for point spectroscopy comprising:

a light source;

an optical beam emitted from the light source that is chopped or pulsed at an optical frequency;

a substrate that receives the optical beam from the light source on a surface of the substrate;

a cantilever coupled to the substrate; and

a target material that is disposed on the surface of the substrate, where the target material is subject to the optical beam and results in a photoacoustic induced vibration that is measured by the cantilever as the optical frequency is changed.

2. The apparatus of claim 1 where a photoacoustic wave is generated on the surface of the substrate from the target material absorbing at least a portion of the optical beam.

3. The apparatus of claim 2 where the vibration that is measured by the cantilever is induced by the generated photoacoustic wave.

4. The apparatus of claim 3 further comprising a cantilever resonance measurer that measures the vibration detected by the cantilever.

5. The apparatus of claim 4 where the vibration is detected by optical beam deflection, a piezoelectric effect, a piezoresistive effect, electron tunneling, capacitance variation, drain current variation, or a combination.

6. The apparatus of claim 4 where the cantilever resonance measurer comprises a processor that analyzes the cantilever vibration as the optical frequency is changed to generate a spectrum.

7. The apparatus of claim 1 where the optical pulse frequency corresponds with a resonant frequency of the cantilever.

8. The apparatus of claim 7 where the cantilever comprises a mechanical resonator, where the optical pulse frequency corresponds with a resonant frequency of the mechanical resonator.

9. The apparatus of claim 1 where the target material is coated or covered over the surface of the base.

10. The apparatus of claim 1 where the target material comprises analyte molecules that are absorbed on the surface of the base.

11. The apparatus of claim 1 where the cantilever is micromachined from the substrate.

12. The apparatus of claim 11 where the substrate and cantilever comprise a silicon substrate.

13. The apparatus of claim 1 where the substrate is a micromachined monolithic structure suspended from scaffolding using thin flexible bridges.

14. A system for array spectroscopy comprising:

at least one source that emits at least one pulsed light beam at a programmed frequency;

an array of base substrates that each comprise an incident surface;

an array of cantilevers that correspond with the array of base substrates, where each base substrate is coupled to one of the cantilevers, further where each of the cantilevers includes a predetermined resonant frequency that corresponds with the predetermined chop frequency from at least one of the sources;

a target material that is coupled to one or more of the base substrates such that the incident surface of the one or more base substrates includes the target material and the pulsed light beams are directed at the target material;

where the target material reacts with the pulsed light beam to generate a photoacoustic wave that produces a vibration of the corresponding cantilever that is measured as the optical color is varied.

15. The system of claim 14 where the target material is disposed on one of the base substrates, but not disposed on an adjacent base substrate, further where the adjacent base substrate is used as a reference.

16. The system of claim 14 where the target material is coated on the incident surface of the one or more base substrates.

17. The system of claim 14 where each of the base substrates comprises a silicon substrate that includes the corresponding cantilever as a part of the silicon substrate.

18. The system of claim 14 where the measurement at each of the cantilever comprises an acoustic or vibrational measurement receiver that is tuned to the surface of the corresponding base substrate.

19. The system of claim 18 where a spectrum of the measurement correspond to the measured vibrational intensity at the optical colors of each of the sources.

20. The system of claim 19 where the vibration is detected by optical beam deflection, a piezoelectric effect, a piezoresistive effect, electron tunneling, capacitance variation, drain current variation, or combinations thereof.

21. The system of claim 14 where the at least one sources comprises a plurality of light sources or a single source with a grating that produces individual optical wavelengths corresponding to the base substrates in the base substrate array.

22. A method for photoacoustic spectroscopy comprising:

chopping light emitted from a light source at a programmed frequency;

focusing the emitted light towards an incident surface of a base substrate, where the base substrate includes a cantilever for monitoring a vibration of a target material that is disposed on the incident surface and reacts to the emitted light;

measuring the vibration of the cantilever by monitoring photoacoustic waves that are generated from the target material; and

measuring the vibration of the cantilever to photoacoustic waves that are generated from the target material as the color of the emitted light is adjusted.

23. The method of claim 22 where the light source comprises a monochromator.

24. The method of claim 22 where the acoustic wave is generated on the incident surface of the base substrate because the target material absorbs at least a portion of the emitted light.

25. The method of claim 22 further comprising analyzing the measurements to generate a spectrum and identify the target material.

26. The method of claim 22 where the chopping frequency is substantially similar to a resonant frequency of the detector.