Adaptive nulling hyperthermia array

• US 5,251,645 A
• Filed: 06/26/1991
• Issued: 10/12/1993
• Est. Priority Date: 06/26/1991
• Status: Expired due to Term

• Current Assignee: Massachusetts Institute of Technology
• Original Assignee: Massachusetts Institute of Technology
• Inventors: Fenn, Alan J.
• Primary Examiner(s): Cohen, Lee S.
• Application Number:
  US07/722,612
• Time in Patent Office: 839 Days
• Field of Search: 128/804, 128/399, 128/653.1
• US Class Current: 607/154
• CPC Class Codes: A61N 5/02 using microwaves
• CPC Class Codes: A61N 5/04 Radiators for near-field treatment

Abstract

A hyperthermia array uses adaptive nulling with non-invasive auxiliary probes to reduce the electric field intensity at selected positions in the target body while maintaining a desired focus at a tumor thereby avoiding or reducing the occurrences of "hot spots" during ultrasonic or R.F. hyperthermia treatment. A hyperthermia applicator has an annular phased array of electric field radiators coupled to a source of electric radiation through a controllable transmit weighting network to control the phase and amplitude of the electric field radiation transmitted. The transmit weighting networks respond to feedback signals from a controller coupled to ele

GOVERNMENT SUPPORT

The invention described herein was supported in whole or in part by Contract No. F19628-90-C-0002 from the United States Air Force.

Claims

1. A hyperthermia applicator for inducing a temperature rise in a target, comprising

a plurality of electric field radiators;

a source of electric field radiation coupled to each electric field radiator through a controllable transmit weighting network coupled to a respective electric field radiator, each weighting network controlling the phase and amplitude of electric field radiation coupled from the source to the respective electric field radiator in response to a respective feedback signal;

at least one electric field probe for detecting electric field radiation from the plurality of radiators; and

a controller means coupled to the electric field probes for receiving the detected electric field radiation and generating the respective feedback signals, and for adjusting the feedback signal in response to the detected electric field radiation so that the detected electric field radiation is minimized at the electric field probe.

2. The apparatus of claim 1, wherein the plurality of electric field radiators comprises a phased-array of electric field transmit elements.

3. The apparatus of claim 2, wherein the phased-array of electric field transmit elements comprises an annular array for surrounding the target.

4. The apparatus of claim 3, wherein the annular array comprises between 4 and 12 transmit elements aligned substantially parallel to each other and substantially uniformly distributed along the perimeter of a cylinder.

5. The apparatus of claim 4, wherein the diameter of the cylinder is between 40 and 80 cm.

6. The apparatus of claim 1, wherein the electric field probes comprise a plurality of probe elements adapted to be disposed non-invasively along the perimeter of the target.

7. The apparatus of claim 6, wherein the target approximates an ellipse and the electric field probes comprise at least one probe element adapted to be positioned at the front, back, and on each side of the target.

8. The apparatus of claim 1, further comprising

at least one secondary electric field probe for detecting electric field radiation;

wherein the controller means adjusts the feedback signals in response to the electric field radiation detected by the secondary electric field probe so that the electric field radiation is maximized at the secondary electric field probe.

9. The apparatus of claim 8, wherein the plurality of electric field radiators comprises a phased-array of electric field transmit elements, and the secondary electric field probe is adapted to be disposed at the desired focus of the phased-array.

10. The apparatus of claim 9, wherein the phased-array of electric field transmit elements comprises an annular array for surrounding the target.

11. The apparatus of claim 10, wherein the annular array comprises between 4 and 12 transmit elements aligned substantially parallel to each other and substantially uniformly distributed along the perimeter of a cylinder.

12. The apparatus of claim 11, wherein the diameter of the cylinder is between 40 and 80 cm.

13. The apparatus of claim 12, wherein

the electric field probes comprise a plurality of probe elements adapted to be disposed non-invasively along the perimeter of the target;

and

the secondary electric field probe comprises at least one probe element adapted to be disposed invasively within the target at the desired focus of the electric field energy.

14. The apparatus of claim 13, wherein the target approximates an ellipse and

the electric field probes comprise at least one probe element adapted to be positioned at the front, back, and on each side of the target.

15. The apparatus of claim 14, wherein the plurality of electric field radiators comprises an annular phased-array of electric field transmit elements for surrounding the target;

and

the secondary electric field probe is adapted to be disposed at the desired focus of the phased-array.

16. The apparatus of claim 1, wherein the controller means performs a matrix inversion to generate the feedback signal.

17. The apparatus of claim 16, wherein the controller means comprises

a receiver coupled to the electric field probes for receiving voltages v₁ⁱ, v₂ⁱ, . . . , v_Nⁱ due to the mth and nth electric field radiator at the ith electric field probe;

means for forming a cross correlation R_mnⁱ of the received voltages, the cross correlation being given by

space="preserve" listing-type="equation">R.sub.mn.sup.i =E(v.sub.m.sup.i v.sub.n.sup.i*),

where ^* means complex conjugate and E(.) means mathematical expectation;

means for forming a channel correlation matrix R given by ##EQU39## where N_aux is the number of electric field probes, R_i is the sample correlation matrix observed at the ith electric field probe; and

means for generating an adapted transmit weight vector w_a given by

space="preserve" listing-type="equation">w.sub.a =R.sup.-1 w.sub.q,

where generally the transmit weight vector w=(w₁, w₂, . . . , w_N)^T represents the transmit weights of each of N controllable weighting networks, and w_q represents the quiescent transmit weight vector;

wherein the controller means adjusts the feedback signal in response to the adapted transmit weight vector w_a.

18. The apparatus of claim 1, wherein the controller means performs a gradient search algorithm to generate the feedback signal.

19. The apparatus of claim 18, wherein the controller means comprises

a receiver coupled to the electric field probes for receiving voltage amplitudes |v_1jⁱ |,|v_2jⁱ |, . . . ,|v_Njⁱ | due to the mth and nth electric field radiator at the ith electric field probe for the jth configuration of the transmit weights w_nj ;

means for calculating a figure of merit F_nj from the received voltage amplitudes given by ##EQU40## where N_aux is the number of electric field probes, means for dithering the transmit weights w_nj by a small amount in amplitude, Δ

A_nj, and phase, Δ

Φ

_nj ;

means for determining the figure of merit differences Δ

F_Anj and Δ

F.sub.Φ

nj caused by dithering the amplitude and phase, respectively,

means for determining gradient search directions search directions r_Anj and r.sub.Φ

nj given by ##EQU41## respectively, and means for generating the new transmit weight w_n(j+1) for the (j+1)th configuration where the amplitude component of the new weight is given by

space="preserve" listing-type="equation">A.sub.n,j+1 =A.sub.nj +Δ

Ar.sub.Anj

and the phase component of the new weight is given by

space="preserve" listing-type="equation">Φ

.sub.n,j+1 =Φ

.sub.nj +Δ

Φ

r.sub.Φ

nj.

20. A hyperthermia applicator for inducing a temperature rise in a target, comprising

an annular phased array of electric field radiators for surrounding a target;

a source of electric field radiation coupled to each electric field radiator through a controllable transmit weighting network coupled to a respective electric field radiator, each weighting network controlling the phase and amplitude of electric field radiation coupled from the source to the respective electric field radiator in response to a respective feedback signal;

a plurality of electric field probe elements adapted to be disposed non-invasively along the perimeter of the target for detecting electric field radiation from the annular phased array of radiators; and

a controller means coupled to the electric field probes for receiving the detected electric field radiation and generating the respective feedback signals, and for adjusting the feedback signal in response to the detected electric field radiation so that the detected electric field radiation is minimized at the electric field probe elements.

21. The apparatus of claim 20, wherein the annular array comprises between 4 and 12 transmit elements aligned substantially parallel to each other and substantially uniformly distributed along the perimeter of a cylinder.

22. The apparatus of claim 21, wherein the diameter of the cylinder is between 40 and 80 cm.

23. The apparatus of claim 20, wherein the target approximates an ellipse and the electric field probes comprise at least one probe element adapted to be positioned at the front, back, and on each side of the target.

24. The apparatus of claim 20, further comprising

at least one secondary electric field probe adapted to be disposed at the desired focus of the phased-array for detecting electric field radiation;

wherein the controller means adjusts the feedback signals in response to the electric field radiation detected by the secondary electric field probe so that the electric field radiation is maximized at the secondary electric field probe.

25. The apparatus of claim 24, wherein the secondary electric field probe comprises at least one probe element adapted to be disposed invasively within the target.

26. The apparatus of claim 20, wherein the controller means performs a matrix inversion to generate the feedback signal.

27. The apparatus of claim 26, wherein the controller means comprises

a receiver coupled to the electric field probes for receiving voltages v₁ⁱ, v₂ⁱ, . . . , v_Nⁱ due to the mth and nth electric field radiator at the ith electric field probe;

means for forming a cross correlation R_mnⁱ of the received voltages, the cross correlation being given by

space="preserve" listing-type="equation">R.sub.mn.sup.i =E(v.sub.m.sup.i v.sub.n.sup.i*),

where ^* means complex conjugate and E(.) means mathematical expectation;

means for forming a channel correlation matrix R given by ##EQU42## where N_aux is the number of electric field probes, R_i is the sample correlation matrix observed at the ith electric field probe; and

means for generating an adapted transmit weight vector w_a given by

space="preserve" listing-type="equation">w.sub.a =R.sup.-1 w.sub.q,

where generally the transmit weight vector w=(w₁,w₂, . . . ,w_N)^T represents the transmit weights of each of N controllable weighting networks, and w_q represents the quiescent transmit weight vector;

wherein the controller means adjusts the feedback signal in response to the adapted transmit weight vector w_a.

28. The apparatus of claim 20, wherein the controller means performs a gradient search algorithm to generate the feedback signal.

29. The apparatus of claim 28, wherein the controller means comprises

a receiver coupled to the electric field probes for receiving voltage amplitudes |v_1jⁱ |,|v_2jⁱ |, . . . ,|v_Njⁱ | due to the mth and nth electric field radiator at the ith electric field probe for the jth configuration of the transmit weights w_nj ;

means for calculating a figure of merit F_nj from the received voltage amplitudes given by ##EQU43## where N_aux is the number of electric field probes, means for dithering the transmit weights w_nj by a small amount in amplitude, Δ

A_nj, and phase, Δ

Φ

_nj ;

means for determining the figure of merit differences Δ

F_Anj and Δ

F.sub.Φ

nj caused by dithering the amplitude and phase, respectively,

means for determining gradient search directions search directions r_Anj and r.sub.Φ

nj given by ##EQU44## respectively, and means for generating the new transmit weight w_n,(j+1) for the (j+1)th configuration where the amplitude component of the new weight is given by

space="preserve" listing-type="equation">A.sub.n,j+1 =A.sub.nj +Δ

Ar.sub.Anj

and the phase component of the new weight is given by

space="preserve" listing-type="equation">Φ

.sub.n,j+1 =Φ

.sub.nj +Δ

Φ

r.sub.Φ

nj.

30. A method for inducing a temperature rise in a target, comprising the steps of:

surrounding a target with an annular phased array of electric field radiators;

coupling a source of electric field radiation to each electric field radiator through a controllable transmit weighting network coupled to a respective electric field radiator;

controlling the phase and amplitude of electric field radiation coupled from the source to the respective electric field radiator with each weighting network in response to a respective feedback signal;

detecting electric field radiation from the annular phased array of radiators with a plurality of electric field probe elements disposed non-invasively along the perimeter of the target; and

receiving the detected electric field radiation and generating the respective feedback signals for adjusting the controllable transmit weighting network in response to the detected electric field radiation so that the detected electric field radiation is minimized at the electric field probe elements.