High resolution resonance ionization imaging detector and method

• US 6,008,496 A
• Filed: 05/05/1998
• Issued: 12/28/1999
• Est. Priority Date: 05/05/1997
• Status: Expired due to Fees

• Current Assignee: University of Florida (State University System of Florida)
• Original Assignee: University of Florida (State University System of Florida)
• Inventors: Smith, Benjamin W., Winefordner, James D., Matveev, Oleg I.
• Primary Examiner(s): NGUYEN, KIET TUAN
• Application Number:
  US09/072,581
• Time in Patent Office: 602 Days
• Field of Search: 250/423 P, 250/397
• US Class Current: 250/423.00P
• CPC Class Codes: H01J 47/02 Ionisation chambers

Abstract

A resonance ionization imaging device (RIID) and method for imaging objects using the RIID are provided, the RIID system including a RIID cell containing an ionizable vapor including monoisotopic atoms or molecules, the cell being positioned to intercept scattered radiation of a resonance wavelength λ₁ from the object which is to be detected or imaged, a laser source disposed to illuminate the RIID cell with laser radiation having a wavelength λ₂ or wavelengths λ₂, λ₃ selected to ionize atoms in the cell that are in an excited state by virtue of having absorbed the scattered resonance laser radiation, and a luminescent screen at the back surface of the RIID cell which presents an image of the number and position of charged particles present in the RIID cell as a result of the ionization of the excited state atoms. The method of the invention further includes the step of initially illuminating the object to be detected or imaged with a laser having a wavelength selected such that the object will scatter laser radiation having the resonance wavelength λ₁.

Claims

1. A resonance ionization imaging device comprising:

a cell having an ionizable vapor of monoisotopic atoms or molecules contained therein;

said cell having means for receiving laser radiation scattered by an object to be imaged, said scattered laser radiation being of a first predetermined wavelength λ

₁, said first predetermined wavelength being a resonance wavelength of said ionizable vapor;

means for illuminating said cell with laser radiation sufficient to ionize a portion of said ionizable vapor, said portion being the atoms that have absorbed said scattered resonance laser radiation and are in an excited state; and

means for detecting a number and a position of charged particles created within said cell as a result of said ionization of said portion of said ionizable vapor.

2. A resonance ionization imaging device as set forth in claim 1 further comprising means for illuminating an object to be imaged with laser radiation of said first predetermined wavelength.

3. A resonance ionization imaging device as set forth in claim 2, wherein said cell illuminating means comprises means so constructed and arranged to irradiate said cell with laser radiation of a second predetermined wavelength λ

₂, said second predetermined wavelength λ

₂ being a narrowband ionization wavelength corresponding to said ionizable vapor and which will ionize said portion of said ionizable vapor that has absorbed said scattered resonance laser radiation of wavelength λ

₁.

4. A resonance ionization imaging device as set forth in claim 2, wherein said cell illuminating means comprises means so constructed and arranged to irradiate said cell with laser radiation of a second predetermined wavelength λ

₂ and a third predetermined wavelength λ

₃, said second and third predetermined wavelengths being narrowband ionization wavelengths corresponding to said ionizable vapor, and which radiation will ionize said portion of said ionizable vapor that has absorbed said scattered resonance laser radiation of wavelength λ

₁.

5. A resonance ionization imaging device as set forth in claim 1, wherein said scattered radiation receiving means is a front planar surface which is at least partially transparent to said scattered radiation.

6. A resonance ionization imaging device as set forth in claim 5, wherein said cell further comprises a luminescent screen disposed in substantially parallel relation to said front planar surface and being spaced apart therefrom.

7. A resonance ionization imaging device as set forth in claim 1, wherein said cell comprises a front planar surface and a back planar surface and further comprises means for generating a high voltage bias in said cell between said front and back surfaces.

8. A resonance ionization imaging device as set forth in claim 1, wherein said cell illuminating means is disposed to propagate said laser radiation perpendicularly to a direction of observation defined by a portion of said cell facing said object to be imaged.

9. A resonance ionization imaging device as set forth in claim 1, wherein said cell illuminating means is disposed to propagate said laser radiation in a direction colinear with a direction of observation defined by a portion of said cell facing said object to be imaged.

10. A resonance ionization imaging device as recited in claim 1, wherein said cell comprises a planar front surface facing said object to be imaged, and a planar back surface disposed substantially parallel to said front surface and separated therefrom to define a volume in said cell for containing said ionizable vapor therein.

11. A resonance ionization imaging device as recited in claim 10, further comprising a luminescent screen disposed at said back surface of said cell.

12. A resonance ionization imaging device as recited in claim 10, wherein said cell further includes a pair of electrodes adapted to create a high voltage potential in said cell between said electrodes.

13. A resonance ionization imaging device as recited in claim 10, wherein said cell further includes a cellular array of capillary tubes extending between said back surface of said cell and a semitransparent electrode, said capillary tubes being so constructed and arranged to lengthen an optical path of said cell.

14. A resonance ionization imaging device as recited in claim 10, further comprising means for further processing an image of said object to be imaged obtained by said cell.

15. A method for imaging an object comprising the steps of:

positioning a detector cell having contained therein an ionizable vapor comprising monoisotopic particles to intercept scattered radiation from an object to be detected, a front surface of said detector cell facing and defining a direction of observation;

illuminating an object to be detected with laser radiation of a frequency and wavelength selected such that a wavelength λ

₁ of radiation scattered from said object corresponds to a resonance wavelength of said monoisotopic particles;

receiving at least a portion of said scattered radiation of wavelength λ

₁ in said detector cell, said scattered radiation being absorbed by a portion of said monoisotopic particles in said ionizable vapor, thereby producing an excited state in said portion of monoisotopic particles;

ionizing said portion of said monoisotopic particles that are in said excited state, by illuminating said ionizable vapor in said detector cell with narrowband ionization laser radiation of at least one wavelength λ

₂ selected to ionize said portion of said monoisotopic particles that are in said excited state; and

detecting a number and position of charged particles in said detector cell created by said ionization of said excited state monoisotopic particles.

16. A method as recited in claim 15, wherein said ionization of said excited-state monoisotopic particles is effected with narrowband ionization laser radiation of said at least one wavelength λ

₂ and with narrowband ionization laser radiation of a further wavelength λ

₃, causing further ionization of said excited-state monoisotopic particles.

17. A method as recited in claim 16, wherein said narrowband ionization laser radiation having wavelengths λ

₂ and λ

₃ is propagated colinearly with said direction of observation, defined by said front surface of said detector cell.

18. A method as recited in claim 16, wherein said narrowband ionization laser radiation having wavelengths λ

₂ and λ

₃ is propagated perpendicularly to said direction of observation defined by said front surface of said detector cell.

19. A method as recited in claim 15, wherein said narrowband ionization laser radiation having wavelength λ

₂ is propagated colinearly with said direction of observation defined by said front surface of said detector cell.

20. A method as recited in claim 15, wherein said narrowband ionization laser radiation having wavelength λ

₂ is propagated perpendicularly to said direction of observation defined by said front surface of said detector cell.

21. A method as recited in claim 15, wherein a linewidth λ

η

of said narrowband ionization laser radiation having wavelength λ

₂ satisfies the condition;

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

λ

.sub.n ≦

Δ

λ

<

Δ

λ

.sub.R,

wherein Δ

λ

_N is a natural line width of an atomic or molecular transition of said monoisotopic particles of said ionizable vapor, and wherein Δ

λ

_R is a predetermined spectral resolution required for the method.

22. A method as recited in claim 15, wherein a linewidth Δ

λ

of said narrowband ionization laser radiation having wavelengths λ

₂ and λ

₃ satisfies the condition;

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

λ

.sub.N ≦

Δ

λ

<

Δ

λ

.sub.R,

wherein Δ

λ

_N is a natural linewidth of an atomic or molecular transition of said monoisotopic particles of said ionizable vapor, and wherein Δ

λ

_R is a predetermined spectral resolution required for the method.

23. A method as recited in claim 15, wherein said excited state produced in said portion of said monoisotopic particles has a lifetime (τ

₁), and said method further includes rapidly scanning said narrowband ionization laser radiation during said excited state lifetime (τ

₁).

24. A method as recited in claim 23, further comprising:

acquiring all images for a predetermined spectral interval in a time interval which is equal to or less than a lifetime (τ

₂) of a second excited state hcreated in said excited state monoisotopic particles by said narrowband ionization laser radiation of wavelength μ

₂.