Focusing electromagnetic radiation within a turbid medium using ultrasonic modulation

• US 8,917,442 B2
• Filed: 09/20/2012
• Issued: 12/23/2014
• Est. Priority Date: 09/20/2012
• Status: Expired due to Fees

• Current Assignee: Elwha LLC (Intellectual Ventures LLC)
• Original Assignee: Elwha LLC (Intellectual Ventures LLC)
• Inventors: Baym, Michael H., Hyde, Roderick A., Kare, Jordin T., Wood, Lowell L. Jr.
• Primary Examiner(s): Ben, Loha
• Application Number:
  US13/623,703
• Publication Number:
  US 20140078578A1
• Time in Patent Office: 824 Days
• Field of Search: 359/305, 359/308, 600/323, 600/328, 600/407, 600/473, 356/51, 604/93.01, 73/52, 736/20
• US Class Current: 359/305
• CPC Class Codes: A61B 5/0075 by spectroscopy, i.e. measuring spectra, e.g. Raman spectroscopy, infrared absorption spectroscopy A61B5/0071 takes precedence
• CPC Class Codes: A61B 5/0097 by applying acoustic waves and detecting light, i.e. acoustooptic measurements
• CPC Class Codes: A61B 5/1455 using optical sensors, e.g. spectral photometrical oximeters
• CPC Class Codes: A61B 5/14551 for measuring blood gases
• CPC Class Codes: G02F 1/11 based on acousto-optical elements, e.g. using variable diffraction by sound or like mechanical waves acousto-optical deflection G02F1/33
• CPC Class Codes: G02F 1/33 Acousto-optical deflection devices circuit or control arrangements therefor G02F1/113

Abstract

The present disclosure provides various systems and methods for focusing electromagnetic radiation (EMR) within a diffusion medium, such as a turbid medium. A diffusion medium is irradiated with EMR. The EMR may be modulated by an acoustical wave focused on a focus volume within the diffusion medium. The EMR may be modulated by a beat frequency or other function of multiple focused acoustical waves. The EMR may be modulated at a harmonic of a fundamental frequency of one or more acoustical waves. A filter may filter the emerging EMR to remove all but specifically modulated EMR scattered from the focus volume. The modulated EMR may be focused and/or used for various purposes, including imaging. In some embodiments, the modulated EMR may be reflected and/or amplified by a phase conjugating mirror. Furthermore, in some embodiments, acoustical phase conjugation may be used to focus an acoustical wave on a focus volume.

Claims

1. A method for focusing electromagnetic radiation, comprising:

vibrating a focus volume within a diffusion medium at a first acoustical frequency, f_a, using a first focused acoustical wave;

vibrating the focus volume within the diffusion medium at a second acoustical frequency, f_b, using a second acoustical wave;

irradiating the diffusion medium with electromagnetic radiation at a radiation frequency, f_r; and

receiving diffused electromagnetic radiation scattered from the focus volume, including modulated electromagnetic radiation from the focus volume at a modulated frequency that is the radiation frequency, f_r, shifted by a function of the first acoustical frequency, f_a, and the second acoustical frequency, f_b.

2. The method of claim 1, wherein the second acoustical wave comprises a focused acoustical wave focused on the focus volume.

3. The method of claim 1, wherein the modulated frequency of the received modulated electromagnetic radiation is the radiation frequency, f_r, shifted by an absolute value of a difference between the first acoustical frequency, f_a, and the second acoustical frequency, f_b, (|f_a−

f_b|), where |f_a−

f_b| is a beat frequency of the first acoustical wave and the second acoustical wave.

4. The method of claim 1, wherein the modulated frequency of the received modulated electromagnetic radiation is the radiation frequency, f_r, shifted by the sum of the first acoustical frequency, f_a, and the second acoustical frequency f_b, (|f_a+f_b|).

5. The method of claim 1, wherein the modulated frequency of the received modulated electromagnetic radiation is the radiation frequency, f_r, shifted by a function of a harmonic of the first acoustical frequency, Nf_a, and the second acoustical frequency, f_b, where N is an integer with an absolute value greater than 1.

6. The method of claim 1, wherein the modulated frequency of the received modulated electromagnetic radiation is the radiation frequency, f_r, shifted by a function of a harmonic of the first acoustical frequency, Nf_a, and a harmonic of the second acoustical frequency, Mf_b, where N and M are each a non-zero integer.

7. The method of claim 1, further comprising:

receiving diffused electromagnetic radiation scattered from the focus volume, including secondary modulated electromagnetic radiation from the focus volume at a secondary modulated frequency that is the radiation frequency, f_r, shifted by a second function of the first acoustical wave and the second acoustical wave.

8. The method of claim 1, wherein the source of the first focused acoustical wave and the source of the second acoustical wave are at an acute angle relative to the focus volume.

9. The method of claim 1, wherein the second acoustical wave comprises a focused acoustical wave,

wherein the first focused acoustical wave has a first array factor, such that the first focused acoustical wave comprises a main lobe and at least one side lobe,

wherein the second focused acoustical wave has a second array factor, such that the second focused acoustical wave comprises a main lobe and at least one side lobe,

wherein the main lobe of the first focused acoustical wave and the main lobe of the second focused acoustical wave are configured to overlap within the focus volume, and

wherein the at least one side lobe of the first focused acoustical wave and the at least one side lobe of the second focused acoustical wave are configured to be non-overlapping.

10. The method of claim 1, further comprising:

filtering the received diffused electromagnetic radiation to remove electromagnetic radiation at the radiation frequency f_r and at modulated frequencies shifted by a harmonic of the first acoustical frequency, Nf_a, and shifted by a harmonic of the second acoustical frequency, Mf_b, where at least one of N and M is zero.

11. The method of claim 10, further comprising:

transmitting phase conjugated electromagnetic radiation of the filtered modulated electromagnetic radiation, such that the phase conjugated electromagnetic radiation substantially converges at the focus volume.

12. The method of claim 11, further comprising:

receiving diffused electromagnetic radiation scattered from the focus volume, including secondary modulated electromagnetic radiation from the focus volume at a secondary modulated frequency that is the radiation frequency, f_r, shifted by a second function of the first focused acoustical wave and the second acoustical wave; and

transmitting secondary phase conjugated electromagnetic radiation of the received secondary modulated electromagnetic radiation, such that the secondary phase conjugated electromagnetic radiation substantially converges at the focus volume.

13. The method of claim 12, further comprising:

receiving diffused phase conjugated electromagnetic radiation modulated at the modulated frequency and the secondary modulated frequency scattered substantially from the focus volume; and

generating an image of the focus volume using the received diffused phase conjugated electromagnetic radiation from the focus volume.

14. The method of claim 11, wherein transmitting the phase conjugated electromagnetic radiation is performed in real-time using a phase conjugate mirror (PCM).

15. The method of claim 1, further comprising:

determining absorption rates of the modulated electromagnetic radiation in hemoglobin in the focus volume at a plurality of radiation frequencies; and

calculating a blood oxygenation within the focus volume using the determined absorption rates.

16. The method of claim 1, further comprising:

generating an image of the focus volume using the received modulated electromagnetic radiation from the focus volume.

17. A system for focusing electromagnetic radiation, comprising:

a first transducer configured to generate a first focused acoustical wave to vibrate a focus volume within a diffusion medium at a first acoustical frequency, f_a;

a second transducer configured to generate a second acoustical wave to vibrate the focus volume within the diffusion medium at a second acoustical frequency, f_b;

a light source configured to irradiate the diffusion medium with electromagnetic radiation at a radiation frequency, f_r; and

a receiver configured to receive diffused electromagnetic radiation scattered from the focus volume, including modulated electromagnetic radiation from the focus volume at a modulated frequency that is the radiation frequency, f_r, shifted by a function of the first acoustical frequency, f_a, and the second acoustical frequency, f_b.

18. The system of claim 17, wherein the first and second transducers are at an acute angle relative to the focus volume.

19. The system of claim 17, further comprising an imaging device configured to generate an image of the focus volume using the received modulated electromagnetic radiation from the focus volume.

20. The system of claim 17, wherein the electromagnetic radiation has a frequency bandwidth less than that of the acoustical frequency, f_a.

21. The system of claim 17, wherein the electromagnetic radiation has a frequency bandwidth less than that of the acoustical frequency, f_b.

22. The system of claim 17, wherein the light source is configured to sweep the radiation frequency, f_r, between an initial frequency and a final frequency.

23. The system of claim 17, wherein the focus volume comprises an elongated focus volume having a first end and a second end,

wherein the first and second transducers are configured to vibrate the elongated volume, and

wherein the first acoustical frequency, f_a, of the elongated volume is configured to transition from a first acoustical frequency, f_a1, at the first end of the elongated volume to a second acoustical frequency, f_a2, at the second end of the elongated volume, such that the modulated electromagnetic radiation is shifted by a function of unique acoustical frequency between f_a1 and f_a2, depending on from where along the elongated volume the electromagnetic radiation was scattered.

24. The system of claim 23, wherein the second acoustical frequency, f_b, of the elongated volume is configured to transition from a third acoustical frequency, f_b1, at the first end of the elongated volume to a fourth acoustical frequency, f_b2, at the second end of the elongated volume, such that the modulated electromagnetic radiation is shifted by a function of unique acoustical frequency between f_b1 and f_b2, depending on from where along the elongated volume the electromagnetic radiation was scattered.

25. The system of claim 23, further comprising an acoustical diffraction system configured to diffract the first focused acoustical wave such that the first acoustical frequency of the elongated volume transitions from the first acoustical frequency, f_a1, at the first end of the elongated volume to the second acoustical frequency, f_a2, at the second end of the elongated volume.

26. The system of claim 17, further comprising:

a blood oxygenation module configured to;

determine absorption rates of the modulated electromagnetic radiation in hemoglobin in the focus volume at a plurality of frequencies; and

calculate a blood oxygenation within the focus volume using the determined absorption rates; and

a transmitter configured to transmit phase conjugated electromagnetic radiation of the modulated electromagnetic radiation, such that the phase conjugated electromagnetic radiation substantially converges at the focus volume.

27. The system of claim 26, wherein the receiver is further configured to receive diffused phase conjugated electromagnetic radiation scattered substantially from the focus volume, and

wherein the system further comprises an imaging device configured to generate an image of the focus volume using the received diffused phase conjugated electromagnetic radiation from the focus volume.

28. The system of claim 26, wherein the transmitter comprises a phase conjugate mirror configured to use a pumping beam to create an energy build up in a non-linear standing wave in order to amplify the phase conjugated electromagnetic radiation relative to the amplitude of the modulated electromagnetic radiation.

29. The system of claim 26,

wherein the transmitter comprises a phase conjugate mirror configured to shift the frequency of the phase conjugated electromagnetic radiation by a function of the first acoustical frequency, f_a, and the second acoustical frequency, f_b, such that the frequency of the phase conjugated electromagnetic radiation that substantially converges at the focus volume is the radiation frequency, f_r.

30. The system of claim 26,

wherein the transmitter comprises a phase conjugate mirror configured to shift the frequency of the phase conjugated electromagnetic radiation by a calibration frequency, f_c, such that the frequency of the phase conjugated electromagnetic radiation is useful for electromagnetic radiation therapy.