Radiation imaging utilizing data reconstruction to provide transforms which accurately reflect wave propagation characteristics

• US 5,170,170 A
• Filed: 08/13/1991
• Issued: 12/08/1992
• Est. Priority Date: 08/13/1991
• Status: Expired due to Fees

• Current Assignee: State University of New York
• Original Assignee: State University of New York
• Inventors: Soumekh, Mehrdad
• Primary Examiner(s): Barron, Jr., Gilberto
• Application Number:
  US07/744,603
• Time in Patent Office: 483 Days
• Field of Search: 342/179, 367/7, 73/603, 128/660.07, 128/661.01, 128/661.02
• US Class Current: 342/179
• CPC Class Codes: G01S 15/8904 using synthetic aperture techniques
• CPC Class Codes: G01S 15/8906 Short-range imaging systems; Acoustic microscope systems using pulse-echo techniques
• CPC Class Codes: G01S 15/8997 using synthetic aperture techniques

Abstract

A system for radiation imaging of an object in response to echo signals from a target area of the object, such as a region of the anatomy of a body. Data is obtained by time domain measurements at monostatic transducers which can be disposed in different locations. The data is processed by two-dimensional Fourier transformations reconstructed using a mapping function and which compensates for variation in the radiation pattern at the various detector locations by using a phase correction function which avoids the need for Fresnel or plane wave approximations.

Claims

1. In a system for providing images derive from echo signals from a target in a region illuminated by multifrequency radiant energy, wherein the signals are transformed into data by two-dimensional (time (t) and position (u)) Fourier transformation into frequency domain (ω

) data and the spatial frequency domain (k_u) data and then is inversely transformed into data from which images can be produced, the improvement comprising means utilizing phase of the signals in the form of a phase function to account for the receipt of said echo signals in the form of spherical wavefronts and reconstructing said frequency domain and spatial frequency domain data in response to said phase function, and means for operating upon said reconstructed data to provide inverse transforms containing said data from which images can be produced with high resolution.

2. The improvement according to claim 1 wherein said signals are synthetic aperture data signals from transducer means at spatial locations u₁ to u_n and which are disposed at different distances y_i along a first line perpendicular to a second line to the center of the target, and said reconstructing means includes means for translating said frequency and spatial frequency domain data into corresponding two-dimensional Fourier transform data in accordance with a phase function ##EQU8## where k=w/c is the wavenumber, c is the velocity of propagation in the medium surrounding the target, (X₁, Y₁ +u_i), i=1, . . . N are the coordinates of the i-th transmitting/receiving element (the transducers);

u_i takes on values in a vertical line in the y direction along which the element is disposed at position u_i, i=1, . . . N (synthesized aperture);

(X₁, Y₁) are the coordinates of the element at the center of the synthetic array (mid-point on the vertical line);

the target is centered around the origin;

i.e., (0,0);

√

(X₁ -x)² +(Y₁ +u_i -y)² is the distance from a reflector at the coordinates (x,y) in the target region to the element located at (X₁, Y₁ +u_i).

4. The improvement according to claim 1 wherein said reconstructing means includes means for translating said echo signals into said frequency and spatial frequency domain data so that said data corresponds directly to the said spherical wavefronts without Fresnel or plane wave approximations.

5. The improvement according to claim 4 wherein said signals are received at different locations in an x, y plane spaced from the target and said translating means includes means operative to account for said illuminating energy propagating in the form of said spherical wavefronts by processing each frequency of said signals in accordance with a phase function ##EQU10## where k=δ

/c, δ

being each frequency of said signal in radians per second, and c is the velocity of propagation of said signals in the medium surrounding the target, x and y are locations in the plane, X₁ and Y₁, and U₁, are coordinates of said locations, X₁ and Y ₁, being reference coordinates.

3. In a system for providing images derived from echo signals from a target illuminated by multifrequency radiant energy, wherein the signals are transformed into data by two-dimensional (time (t) and position (u)) Fourier transformation into frequency domain (ω

) data and the spatial frequency domain (k_u) data and then is inversely transformed into data from which images can be produced, the improvement comprising reconstructing means for translating said frequency and spatial frequency domain data into corresponding two-dimensional Fourier transform data in accordance with a phase function ##EQU9## where said signals are synthetic aperture data signals from transducer means at spatial location u₁ to u_n and which are disposed at different distances y_i along a first line perpendicular to a second line to the center of the target;

k=w/c is the wavenumber, c is the velocity of propagation in the medium surrounding the target, (X_i, Y₁ +u_i), i=1, . . . N are the coordinates of the i-th transmitting/receiving element (the transducers);

u_i takes on values in a vertical line in the y direction along which the element is disposed at position u_i, i=1, . . . N (synthesized aperture);

(X₁, Y₁) are the coordinates of the element at the center of the synthetic array (mid-point on the vertical line);

the target is center around the origin;

i.e., (0,0);

(X₁ -x)² +(Y₁ +u_i -y)² is the distance from the reflector at the coordinates (x,y) in the target region to the element located at (X₁, Y₁ +u_i); and

, wherein means are provided for mapping of said two-dimensional Fourier transform data into corresponding two-dimensional (K_x and K_y) data which is operated upon by means to provide inverse transforms from which images can be produced, where K_x =4K² -k_u² and K_y =k_u and k_u is the spatial frequency domain data for each frequency of the multifrequency energy.