EEG spatial enhancement method and system

• US 5,331,970 A
• Filed: 04/14/1992
• Issued: 07/26/1994
• Est. Priority Date: 09/07/1990
• Status: Expired due to Term

• Current Assignee: SAM Technology, Inc.
• Original Assignee: SAM Technology, Inc.
• Inventors: Le, Jian, Gevins, Alan S.
• Primary Examiner(s): Cohen, Lee S.
• Assistant Examiner(s): Jastrzab, Jeffrey R.
• Application Number:
  US07/868,724
• Time in Patent Office: 833 Days
• Field of Search: 128/731, 128/732, 128/644
• US Class Current: 600/544
• CPC Class Codes: A61B 5/1077 Measuring of profiles
• CPC Class Codes: A61B 5/291 for electroencephalography [EEG]
• CPC Class Codes: A61B 8/0808 for diagnosis of the brain
• CPC Class Codes: G01R 33/28 Details of apparatus provided for in groups G01R33/44 - G01R33/64

Abstract

In an electroencephalographic (EEG) system and method the subject'"'"'s brain waves are recorded using electrodes removably connected to the scalp. The spatial resolution may be improved, in one embodiment, by "Deblurring", based on digital computer processing measurements of the positions of the electrodes; measurements of the subject'"'"'s head size, shape, scalp thickness, skull thickness and brain shape; and estimates of the conductivity of the skull, scalp and cerebral spinal fluid.

Claims

1. The method of obtaining and analyzing data recorded from a plurality of electroencephalograph (EGG) electrodes removably and electrically connected to the scalp of a subject, including the steps of:

(a) amplifying brain waves detected at the electrodes, converting the amplified brain waves into digital data and entering the data into computer system means to analyze the data;

(b) measuring a thickness of the skull of the subject, the thickness of the scalp of the subject and the head shape of the subject;

(c) measuring physical locations of the electrodes on the scalp of the subject;

(d) estimating an electrical conductivity of the skull, scalp and cerebral spinal fluid of the subject; and

(e) entering measurements derived from (b), the electrode locations derived from (c) and the conductivity estimate derived from (d) into the computer system means to analyze the entered brain wave data.

2. The method of claim 1 and including the step of obtaining the measurements of (b) by magnetic resonance image (MRI).

3. The method of claim 1 and including the step of obtaining the measurements of (b) by computerized tomographic scan (CT).

4. The method of claim 1 and including the step of obtaining the measurements of (b) by an ultrasonic scan.

5. The method of claim 1 wherein in step (e) the EEG electrode positions from (c) are registered with measurements of the scalp from (b) using an iterative numerical procedure which optimally matches each EEG electrode position with nearest scalp surface points.

6. The method of claim 1 in which in step (e) the computer system means uses a numerical finite element or surface integral model of the subject'"'"'s scalp, skull and brain surface.

7. The method of claim 1 in which the estimate (d) for the skull is estimated using an equivalent current dipole source model of a sensory stimulus whose major area of cortical activation is known.

8. The method of claim 1 in which the estimates (d) are obtained by measuring a reverse electromotive force produced by eddy currents induced by an applied external field generated by a coil placed against the head of the subject.

9. The method of claim 1 and including the further step of generating volumetric elements from medical images.

10. The method of claim 1 wherein in step (e) a numerical method finite element method or surface integral method are used to obtain spatial deconvolution with the following equation:

space="preserve" listing-type="equation">V·

(σ

(x,y,x)∇

u(x,y,z)=F(x,y,z) in Ω

.

where Ω

,is the conducting volume, σ

(x,y,z) is the conductivity tensor, u(x,y,z) is the potential distribution function, and F(x,y,z) is the source function.

11. The method of claim 1 wherein in step (e) measured EEG potential values are interpolated into potential values for scalp finite element points using a local spline interpolation function which is a linear combination of a set of basis functions which are solutions of the following equation:

space="preserve" listing-type="equation">V·

(σ

(x,y,z)∇

u(x,y,z)=F(x,y,z) in Ω

.

where Ω

, is the conducting volume, σ

(x,y,z) is the conductivity tensor, u(x,y,z) is the potential distribution function, and F(x,y,z) is the source function.

12. The method of claim 1 wherein in step (e) a forward solution from brain surface potential values to scalp potential values is performed using a finite element based forward transformation matrix which is solved with a sparse solver method.

13. The method of claim 1 wherein potentials at a brain surface are estimated using a multi-dimensional optimization method to minimize a difference between calculated and actual scalp potentials and a bipolar-vector space implementation is employed.