Flat-panel detector with avalanche gain

• US 7,323,692 B2
• Filed: 08/10/2005
• Issued: 01/29/2008
• Est. Priority Date: 08/10/2004
• Status: Active Grant

• Current Assignee: The Research Foundation for The State University of New York (State University of New York), Sunnybrook & Women's College Health Sciences Centre
• Original Assignee: The Research Foundation for The State University of New York (State University of New York), Sunnybrook & Women's College Health Sciences Centre
• Inventors: Zhao, Wei, Rowlands, John A.
• Primary Examiner(s): Porta; David
• Assistant Examiner(s): Gaworecki; Mark R
• Application Number:
  US11/201,658
• Publication Number:
  US 20060054835A1
• Time in Patent Office: 902 Days
• Field of Search: 250/370.09, 250/370.11, 250/371
• US Class Current: 250/370.09
• CPC Class Codes: G01T 1/20184 Detector read-out circuitry, e.g. for clearing of traps, compensating for traps or compensating for direct hits
• CPC Class Codes: G01T 1/2928 using solid state detectors

Abstract

The present invention is an indirect AMFPI wherein a phosphor such as a structured cesium iodide (CsI) is used to convert x-ray energy to optical photons or a charge, which is then detected by a two-dimensional array of either thin-film transistors (TFTs) such as an amorphous a-Se TFTs or a photodiode array. A scanning control circuit generates pulses to turn on the TFTs one row at a time, and thus the charge in the individual arrays is transferred from the TFT to one or more external charge-sensitive amplifiers. The charge-sensitive amplifiers are shared by all the pixels in the same column. The two-dimensional array can be read in real time.

Claims

1. A flat panel detector, comprising:

a phosphor screen for receiving x-rays and converting the x-rays into optical photons;

an avalanche photoconductor for receiving the optical photons and converting the optical photons into electrical charges, the avalanche photoconductor having an avalanche gain programmable by changing an electric field applied across the avalanche photoconductor; and

an active matrix array for detecting the electrical charges.

2. The flat panel detector of claim 1, wherein the phosphor screen is structured cesium iodide (CsI).

3. The flat panel detector of claim 1, wherein the avalanche photoconductor is amorphous selenium (a-Se).

4. The flat panel detector of claim 1, wherein the active matrix array is comprised of one of thin film transistors and field emitters.

5. A flat panel detector, comprising:

a phosphor screen of structured cesium iodide (CsI) for converting x-rays into photon charges;

an avalanche photoconductor layer of amorphous selenium (a-Se) for receiving the photon charges and converting the photon charges into electrical charges, the avalanche photoconductor having an avalanche gain programmable by changing an electric field applied across the avalanche photoconductor; and

an active matrix of thin film transistors for detecting the electrical charges.

6. The flat panel detector of claim 5, further comprising an optical coupling located between the phosphor screen and the avalanche photoconductor layer.

7. The flat panel detector of claim 6, further comprising a transparent indium tin oxide layer located between the optical coupling and the avalanche photoconductor layer.

8. The flat panel detector of claim 7, further comprising a layer of cerium oxide located between the transparent indium tin oxide and the avalanche photoconductor layer.

9. The flat panel detector of claim 8, wherein a thin layer of the avalanche photoconductor layer, adjacent to the layer of cerium oxide layer, is doped with lithium fluoride.

10. The flat panel detector of claim 5, further comprising a thin layer of antimony trisulfide located between the avalanche photoconductor layer and the active matrix of thin film transistors.

11. A flat panel detector, comprising:

a phosphor screen of structured cesium iodide (CsI) for converting x-rays into photon charges;

an avalanche photoconductor layer of amorphous selenium (a-Se) for receiving the photon charges and converting the photon charges into electrical charges; and

an active matrix of field emitters for detecting the electrical charges.

12. The flat panel detector of claim 11, further comprising an optical coupling located between the phosphor screen and the avalanche photoconductor layer.

13. The flat panel detector of claim 12, further comprising a transparent indium tin oxide layer located between the optical coupling and the avalanche photoconductor layer.

14. The flat panel detector of claim 13, further comprising a hole-blocking layer located between the transparent indium tin oxide and the avalanche photoconductor layer.

15. The flat panel detector of claim 14, further comprising an electron-blocking layer located between the avalanche photoconductor layer and the active matrix of field emitters.

16. The flat panel detector of claim 11, further comprising a mesh electrode located between the avalanche photoconductor layer and the active matrix.

17. The flat panel detector of claim 16, further comprising a focusing electrode located between the mesh electrode and the active matrix.