Ultralow background multiple photon detector

• US 5,866,907 A
• Filed: 06/25/1996
• Issued: 02/02/1999
• Est. Priority Date: 10/12/1993
• Status: Expired due to Fees

• Current Assignee: Biotraces Incorporated
• Original Assignee: Biotraces Incorporated
• Inventors: Drukier, Andrzej J., Sagdejev, Igor R.
• Primary Examiner(s): Hannaher, Constantine
• Application Number:
  US08/669,970
• Time in Patent Office: 952 Days
• Field of Search: 250/328, 250/366, 250/393, 250/394, 250/395, 250/515.1
• US Class Current: 250/366
• CPC Class Codes: G01N 33/60 involving radioactive labelled substances
• CPC Class Codes: G01T 1/2008 using a combination of different types of scintillation detectors, e.g. phoswich
• CPC Class Codes: G01T 1/204 the detector being a liquid
• CPC Class Codes: G01T 1/208 Circuits specially adapted for scintillation detectors, e.g. for the photo-multiplier section
• CPC Class Codes: G01T 7/08 Means for conveying samples received
• CPC Class Codes: Y10S 436/804 Radioisotope, e.g. radioimmunoassay
• CPC Class Codes: Y10S 436/807 Apparatus included in process claim, e.g. physical support structures
• CPC Class Codes: Y10T 436/13 Tracers or tags

Abstract

An ultralow background multiphoton detectors device for radioisotopes has a background of about one count per day. Two opposed gamma and X-ray photon detectors each preferably include a scintillation crystal and a photomultiplier tube. Sandwiched between the detectors are a separator and a sample holder for a sample labelled with a radioisotope such as I¹²⁵. The detectors convert emissions from the radioisotope into electric output pulses which are then subjected to signal processing for pulse shape analysis, discrimination of coincident from non-coincident events, and quantification of the radioisotope. Detector materials and components are selected to minimize background, and are shielded from external radiation. The device may further be constructed to resolve and provide images of two dimensional sample arrays.

Claims

1. An apparatus for detecting a radioisotope in a sample, comprising:

(a) a detector assembly including two opposed detectors for detecting emissions from the radioisotope in the sample when the sample is placed in a sample holder between the detectors, and for converting the emissions into electric output pulses, and

(b) a pulse shape analyzer, operatively connected to the detectors, for analyzing the output pulses from each detector and comparing them to predetermined acceptance criteria for the two detectors, rejecting pulses that do not satisfy the predetermined acceptance criteria, and counting output pulses that satisfy the predetermined acceptance criteria.

2. An apparatus for detecting a radioisotope in a sample according to claim 1, wherein the counting is done separately for pulses corresponding to coincident and non-coincident emissions.

3. An apparatus according to claim 2, wherein counted coincident pulses are used to build a three dimensional scatter plot matrix.

4. An apparatus according to claim 1, wherein at least one of the detectors comprises a thin inorganic scintillator crystal that produces a signal when impacted with an emission from the radioisotope.

5. An apparatus according to claim 4, wherein the scintillator is selected from the group consisting of NaI(Tl), CsI(Tl), CaF₂ (Eu), and YAP.

6. An apparatus according to claim 4, further comprising a photosensor, wherein a low radioactive background optically transparent window is placed between the scintillator and the photosensor.

7. An apparatus according to claim 6, wherein the window comprises quartz or a high density (>

4 g/cc ) and high atomic number (greater than about

     50) optically transparent material.

8. An apparatus according to claim 6, wherein the window is made of material selected from the group consisting of high-purity GeO₂ or germanium-based glass, high density glasses based on lead, PbF₂, and undoped bismuth germanite (BGO), and wherein the windows are optically connected to the scintillator and the photosensor with an optical grease that matches the optical properties of the photo sensor.

9. The apparatus according to claim 6, wherein the scintillator and photosensor are covered by at least three subsequent layers of nontransparent plastic tape followed by thin metal tape.

10. The apparatus according to claim 9, wherein the metal tapes include a special metal tape with high magnetic permeability, and the assembly is covered by a few layers of copper tape.

11. The apparatus according to claim 4, wherein the surfaces of the scintillator are covered with a thin low radioactive background housing of density less than about 0.1 g/cm² and made of elements having molecular weight below about 13.

12. The apparatus of claim 11, in which the housing comprises an element selected from the group consisting of beryllium, aluminum, and plastic.

13. An apparatus according to claim 1, wherein at least one detector further comprises a photosensor.

14. An apparatus according to claim 13, wherein the photosensor is a photomultiplier, a large surface photodiode, or an avalanche photodiode.

15. An apparatus according to claim 14, wherein the spatially resolving photosensor is a photomultiplier having four outputs, and the position of impact of an X-ray is calculated from the iterative algorithm, the first approximation given by x₀ =(SL-SR)/TS and y₀ =(ST-SB)/TS and following approximations obtained from:

space="preserve" listing-type="equation">x.sub.i =(a x.sub.i-1 !*SL-b x.sub.i-1 !*SR)/TS

and

space="preserve" listing-type="equation">y.sub.i =(c y.sub.i-1 !*ST-d x.sub.i-1 !*SB)/TS

wherein SL=signal left, SR=signal right, ST=signal top and SB=signal bottom (SB) and TS=SL+SR+ST+SB and where a(x), b(x), c(y) and d(y) are the calibration functions established empirically for the spatially resolving photomultiplier.

16. An apparatus according to claim 15, wherein the true energy of an X-ray is calculated from the impact position of the X-ray using the look up calibration tables established empirically for the spatially resolving photomultiplier.

17. An apparatus according to claim 13, wherein the photosensor is a photomultiplier tube made of low radioactive material selected to have radioactivity lower than about 10 pCi.

18. An apparatus according to claim 17, wherein the diameter of the photomultiplier is about 2" to about 3".

19. An apparatus according to claim 17, wherein the diameter of the scintillation crystal is about 7% to about 25% smaller than the diameter of the photomultiplier tube.

20. An apparatus according to claim 1, wherein the detector assembly comprises a separator placed between the detectors;

and a shield array isolating the detectors from external radiation.

21. An apparatus according to claim 20, wherein the detectors are identical CaF₂ (Eu) crystals with a thickness less than about 0.5 inch.

22. The apparatus according to claim 1, wherein the detector assembly is placed within a shield of which at least one of the components is a metal having an atomic number greater than about 61, or a compound thereof having a density greater than about 5 g/cc, and the shield materials are selected to have a radioactive background less than about 10 pCi/g.

23. The apparatus according to claim 22, whereip the shield comprises subsequent layers of materials with low atomic number (Z<

20), medium atomic number (21<

Z<

60) and high atomic number (Z>

61), and where the high atomic number layer is the most external.

24. The apparatus according to claim 23, wherein the material with low atomic number comprises copper and the material with medium atomic number comprises tin.

25. An apparatus according to claim 1, wherein a separator absorbing the majority of X-rays is sandwiched between the detectors.

26. The apparatus according to claim 25, wherein the separator comprises a layer of a high atomic number material (Z>

61) with a thickness larger than about 2 mm.

27. The apparatus according to claim 26, wherein the separator is cladded on both surfaces with thin layers of materials with medium and low atomic number.

28. The apparatus according to claim 27, wherein the low and medium atomic number materials are copper and tin, respectively.

29. The apparatus according to claim 25, wherein the sample holder is a hole in the separator.

30. The apparatus according to claim 25, wherein the separator has two parts configured to receive the sample holder.

31. The apparatus according to claim 30, wherein the sample holder is made of materials having atomic number below about 13, and low radioactive background.

32. The apparatus according to claim 30, wherein the sample holder is a plastic tray with dimensions of between about 12×

13 mm and about 75×

100 mm.

33. The apparatus according to claim 25, wherein the sample holder is a narrow microcapillary with a receptacle tip sized to contain up to about 0.1 cm³ of liquid.

34. The apparatus according to claim 1, wherein at least one of the detectors is a phoswich module comprising two optically coupled scintillators with different characteristic response times.

35. The apparatus according to claim 34, wherein the scintillator closer to the sample is a very thin scintillator with high energy resolution, the second scintillator is a thick, high stopping power scintillator, and the two scintillators are separated by a few millimeters of optically transparent material with low radioactive background.

36. An apparatus according to claim 35, wherein the scintillator closer to the sample is NaI(Tl) or CaF₂ (Eu), the second scintillator is CsI or BGO, and the optically transparent material is acrylic plastic or quartz.

37. An apparatus according to claim 35, further comprising a fast, low noise shaping amplifier that amplifies the signal from the phoswich, and the pulse shape analyzer localizes the scintillator element inside the phoswich within which the photon is absorbed.

38. An apparatus according to claim 1, wherein at least one of the detectors comprises a semiconducting detector.

39. An apparatus according to claim 1, wherein at least one of the detectors comprises a gas detector.

40. An apparatus according to claim 1, wherein each detector further comprises a low noise preamplifier that shapes signals into characteristic triangular output pulses with rise times shorter than about 200 nsec and fall time between about 0.5 and about 5 microseconds, and matches the pulse shapes and amplitudes in both detectors to better than about 10%.

41. An apparatus according to claim 40, wherein the pulse shape analyzer comprises single channel analyzers (SCAs) that analyze the triangular output pulses for amplitude, and a coincidence circuit with a well defined time window that analyzes the output pulses and provides a trigger pulse when it receives coincident output pulses.

42. An apparatus according to claim 41, wherein the pulse shape analyzer further comprises a spectrum analyzer having a speed of at least about 10 MHz per channel that stores in memory and analyzes the shape of the triangular output pulses when it receives a trigger pulse from the coincidence circuit.

43. An apparatus according to claim 42, wherein the spectrum analyzer is an analog-to-digital converter or digital storage oscilloscope.

44. An apparatus according to claim 42, wherein the pulse shape analyzer further comprises a computer having a fast memory into which data from the spectrum analyzer is transferred.

45. An apparatus according to claim 1, wherein the pulse shape analyzer analyzes output pulse shape criteria from the group consisting of pulse amplitude, total pulse width, shape of the rising part of the pulse, shape of the falling part of the pulse, delay between the pulses from the two detectors, pulse multiplicity, and pre-pulse trace;

and compares the output pulse criteria with predetermined acceptance criteria, accepts the output pulse for counting if the acceptance criteria are satisfied, and rejects the output pulse if the acceptance criteria are not satisfied.

46. An apparatus according to claim 45, wherein the acceptance criteria are obtained from a high energy photon pulse shape, and comparison of the signal pulse to the acceptance criteria uses a least squares technique.

47. An apparatus according to claim 1, wherein the sample holder comprises an encapsulated sample spot and is thin enough and made of low enough density/low enough atomic number material that the sample holder absorbs negligible amounts of X-rays and does not contaminate the detectors.

48. An apparatus according to claim 47, wherein the sample spot is encapsulated with a thin layer of material with very low radiactive background less than about 0.1 pCi/cm² and low atomic number.

49. An apparatus according to claim 48, wherein the encapsulating material is selected from the group consisting of spray, lacquer, acrylic paint, silicon paint, and varnish.

50. An apparatus according to claim 48, wherein the sample is affixed to a solid, flat sheet within an encapsulating pouch made from a thin film selected from the group consisting of berylium films thinner than about 1 mm, plastic films thinner than about 0.5 mm, and aluminum films thinner than about 0.2 mm.

51. An apparatus according to claim 1, wherein one of the detectors comprises a scintillator crystal and is substantially smaller than the other detector, and further comprising a thin film of high density/high atomic number heavy metal having a small aperture placed in front of the small detector for scaning the sample.

52. An apparatus according to claim 51, wherein both detectors comprise scintillator crystals of CaF₂ (Eu) with thickness less than about 3 mm, and diameters between about 0.5 and about 1 inch for the smaller crystal, and between about 2 and about 3 inches for the bigger crystal.

53. A scanning apparatus according to claim 52, wherein the small scintillator is thinner than about 0.1 mm, is sensitive to Auger electrons or very low energy X-rays (E<

10 keV), and has a diameter between about 0.1 and about 0.5 inch.

54. A scanning apparatus according to claim 51, wherein the pulse shape analyzer has two modes, an OR mode accepting both non-coincident and coincident pulses for counting, and an AND mode accepting only coincident pulses for counting;

and further comprising a sample mover adapted for holding and moving the sample holder in two dimensions with spatial resolution adequate to present essentially flat samples to the aperture in front of the small scintillation crystal; and

a controller that identifies the position of the sample mover and permits correlation with the count rate for each position; and

optimizes the time of data acquisition for each sample position such that data acquisition can be stopped when the accumulated data reaches a predetermined signal to background ratio or signal to statistical uncertainty ratio; and

the pulse shape analyzer and controller present the acquired data as a two dimensional image.

55. A scanning apparatus according to claim 54, wherein the sample mover and the controller cooperate to permit two scans of the samples to be performed, first with low spatial resolution, and second with higher spatial resolution in selected areas in which the count rate is above a predetermined value.

56. An apparatus according to claim 1, wherein the detector assembly comprises a silicon scintillator or spatially resolving CCD detector thinner than 0.1 mm, sensitive to Auger electrons or very low energy X-rays (E<

10 keV).

57. An apparatus according to claim 56, wherein the CCD detector is located between the sample holder and one of the opposed detectors.

58. A spatially resolving apparatus according to claim 1, adapted for a plurality of samples arrayed in a two dimensional pattern, wherein at least one of the detectors comprises a scintillator with a high density/heavy metal mask affixed to it, the mask having a coded aperture pattern corresponding to the pattern of the samples, and wherein the scintillator is coupled with a spatially resolving photomultiplier tube having a plurality of outputs each operatively connected to a matched low noise amplifier, the outputs of which are summated electronically into a sum output, and the individual and sum outputs are input to multichannel spectrum analyzers.

59. An apparatus according to claim 58, wherein the spectrum analyzers are analog-to-digital converters or digital storage oscilloscopes.

60. An apparatus according to claim 58, wherein the amplified output pulses from the spatially resolving PMT are compared with "standard shape" pulses according to pulse shape acceptance criteria, and only events satisfying the "standard shape" condition in both the spatially resolved and non-spatially resolved PMTs are accepted and used to build a two dimensional sample image.

61. An apparatus according to claim 60, wherein the amplified pulses from the spatially resolving PMT outputs are digitized by an appropriate spectrum analyzer and are stored in computer memory and subsequently used to build a two dimensional sample image.

62. An apparatus according to claim 58, wherein the diameter of the scintillator is at least 0.5 inch smaller than the size of the spatially resolving photomultiplier.

63. An imaging apparatus according to claim 58, wherein the scintillator has affixed to it a coded aperture mask made of high density/high atomic number film with a regular pattern of up to about 50 holes or slits;

the sample holder is a flat two dimensional array of samples; and

further comprising a computer-controlled mover which sequentially places samples in measurement positions in front of the aperture mask for a pre-set time.

64. An imaging apparatus according to claim 63, further comprising an imaging analyzer wherein the image is reconstructed from the counting data;

the resolution-defining aperture pattern is such that to obtain a continuous image the pixels have to be interleaved in both X and Y dimensions and the pattern allows interleaving;

for each available resolution mask the system has a separate calibration file containing the software mask defining the mapping of the apertures to the image surface;

a user interface allows selecting a rectangular area to be scanned and pre-setting the counting time for each pixel; and

a data presentation system permits visualization of the image in false colors, shades of grey, a contour map or as a 3D surface, and stores the image in a number of standard formats for analysis by other image processing programs.

65. An apparatus according to claim 1, wherein one of the detectors is a Ge-semiconducting detector optimized for detection of X-rays.

66. An apparatus according to claim 65, wherein the Ge-semiconducting detector is less than about 0.5 inch thick and uses a cryostat with thin beryllium or aluminum windows.

67. An apparatus according to claim 1, wherein one of the detectors is a silicon detector.

68. An apparatus according to claim 1, wherein one of the detectors is a spatially resolving gas detector.

69. An apparatus according to claim 68, wherein the spatially resolving detector is a thin self-limiting streamer chamber, wherein the spatial resolution is obtained by imaging, using a CCD.

70. An apparatus according to claim 1 wherein

the detector assembly comprises means for holding samples sandwiched between means for converting the emissions from the isotope to electrical output pulses, and

the pulse shape analyzer comprises means for counting and timing the output pulses,

means for normalizing output pulse amplitude to fall within a predetermined range over a baseline and to correlate with the energy of the emissions,

means for generating a first trigger pulse when there is an output pulse having an amplitude which exceeds a predetermined threshold value, and generating a second trigger pulse when there are two substantially simultaneous output pulses having respective amplitudes which exceed the predetermined threshold value, and rejecting output pulses that do not exceed the predetermined threshold value,

means responsive to a trigger pulse for capturing a predetermined number of subsequent normalized output pulses, and

means for analyzing the captured output pulses based on predetermined isotope and system-dependant acceptance criteria selected from the group consisting of pulse shape, height, coordinates, and coincidence,

means for counting pulses that satisfy the predetermined isotope and system-dependant acceptance criteria and rejecting pulses that do not satisfy the acceptance criteria.

71. An apparatus according to claim 70, further comprising means for shielding the detectors from radioactive background.

72. An apparatus according to claim 70, further comprising means for absorbing the majority of external X-rays.

73. An apparatus according to claim 1, wherein the sample holder has a plurality of holes ordered into an easily distinguished pattern, such that samples to be studied can be placed adjacent to the holes.

74. An apparatus according to claim 73, further comprising a separator absorbing the majority of X-rays, between the opposed detectors, and having a hole pattern corresponding to the pattern in the sample holder, wherein the sample holder aligns samples blotted upon an appropriate thin film with a pattern corresponding to the pattern in the sample holder such that the sample pattern is aligned with the holes in the sample holder and the separator.

75. An apparatus according to claim 74, wherein the sample holder has two parts, each with identical hole patterns, and the blotted film is placed between these two parts.

76. An apparatus according to claim 1, wherein the detector assembly comprises for each detector a preamplifier, amplifier and shaping amplifier.

77. An apparatus according to claim 1, wherein the pulse shape analyzer comprises means for analysing each pulse shape record by at least one software module having acceptance criteria, rejecting a pulse on-line if it does not satisfy the acceptance criteria of all the software modules utilized, and counting the pulse if it satisfies the acceptance criteria of all the software modules utilized.

78. An apparatus according to claim 77, wherein the at least one software module is selected from the group consisting of:

a) analyzer of pulse amplitude;

b) analyzer of the total pulse width;

c) analyzer of the shape of the rising part of the pulse;

d) analyzer of the shape of the falling part of the pulse;

e) analyzer of the delay between the pulses from the two detectors;

f) analyzer of pulse multiplicity;

g) analyzer of the pre-pulse trace; and

h) comparator of the pulse shape with a standard high energy photon pulse shape using a least squares technique;

individually or in combination.

79. An apparatus according to claim 1 for selective quantitation of a coincident gamma/X-ray (CGX) emitter in a sample, wherein the detector assembly comprises

(a) means for detecting coincident gamma and x-ray emissions from the CGX emitter as output pulses in separate radiation detectors, and the pulse shape analyzer comprises

(b) means for analyzing the shape and height of the output pulses from the detectors,

(c) means for discriminating and rejecting non-coincident output pulses,

(d) means for discriminating and rejecting spurious coincident output pulses, and

(e) means for using the remaining output pulses to quantify the presence of the CGX emitter in the sample.

80. An apparatus according to claim 1, wherein the radioisotope is selected from the group consisting of the lighter electron capture (EC) isotopes Be ⁷ (53.6 d), Na²² (2.58 y), Ar³⁷ (34.3 d), V ⁴⁹ (330.0 d), Cr⁴⁸ (23.0 h), Cr⁵¹ (27.8 d), Mn⁵² (5.6 d), Mn⁵⁴ (291.0 d), Fe⁵² (8.0 h), Fe⁵⁵ (2.7 y), Co⁵⁵ (18.0 h), Co⁵⁶ (77.3 d), Co⁵⁷ (270.0 d), Co⁵⁸ (71.0 d), Ni⁵⁶ (6.4 d), Ni⁵⁷ (1.5 d), Cu⁶⁴ (12.8 h), Zn⁶² (9.3 h), Zn⁶⁵ (245.0 d), Ga⁶⁶ (9.5 h), Ga⁶⁷ (78.0 h), As⁷¹ (62.0 h), As⁷² (26.0 h), As⁷³ (76.0 d), As⁷⁴ (18.0 d), Se⁷² (8.4 d), Se⁷⁵ (120.0 d), Br⁷⁶ (16.5 h), Br⁷⁷ (2.6 d), Kr⁷⁶ (10.0 h), Kr⁷⁹ (1.6 d), Rb^82m (6.3 h), Rb⁸³ (83.0 d), Rb⁸⁴ (33.0 d), Sr⁸² (25.5 d), Sr⁸³ (1.6 d), Sr⁸⁵ (64.0 d), Y ⁸³ (108.0 d), Y ⁴⁶ (14.6 h), Y ⁸⁷ (3.33 d), Zr⁸⁸ (85.0 d), Zr⁸⁹ (3.29 d), Nb⁹² (10.1 d), Tc^93m (60. d), Tc⁹⁶ (4.3 d), Tc^99m (6.0 h), Ru⁹⁷ (2.9 d), Rh⁹⁹ (16. d), Rh¹⁰⁰ (21. h), Rh¹⁰² (206 d), Pd¹⁰⁰ (4.0 d), Pd¹⁰¹ (8.5 h), Pd¹⁰³ (17 d), Ag¹⁰⁵ (40 d), Ag^106m (8.3 d), Ag^108m (>

5 y), Cd¹⁰⁷ (6.7 h), Cd¹⁰⁹ (470 d), In¹¹¹ (2.81 d), In¹¹³ (118 d), Sn¹¹³ (118 d), Sb¹¹⁹ (158 d), Sb¹²² (2.8 d), Te¹¹⁸ (60 d), Te¹¹⁹ (45 d), Te¹²¹ (17 d), I ¹²³ (4.2 d), I ¹²⁵ (60 d), I ¹²⁶ (13.2 d), Cs¹³² (6.5 d), Ba¹²⁸ (2.4 d), Ba¹³¹ (11.6 d);

the EC isotopes of lanthanides La¹³⁵ (19.8 h), Ce¹³³ (6.3 h), Ce¹³⁴ (3.0 d), Ce¹³⁵ (22.0 h), Ce¹³⁷ ( 9.0 h), Ce¹³⁹ (140 d), Nd¹⁴⁰ ( 3.3 d), Pm¹⁴³ (265 d), Pm¹⁴⁴ (440 d), Pm¹⁴⁵ (18 y), Pm¹⁴⁶ (710 d), Pm^158m (40.6 d), Sm¹⁴⁵ (340 d), Eu¹⁴⁵ (5.6 d), Eu^146m (1.58 d), Eu¹⁴⁶ (4.6 d), Eu¹⁴⁷ (24 d), Eu¹⁴⁸ (54 d), Eu¹⁴⁹ (120 d), Eu^150m (14 h), Eu¹⁵⁰ (5 y), Eu¹⁵² (13 y), Gd¹⁴⁶ (48 d), Gd¹⁴⁷ (35 h), Gd¹⁴⁹ (9 d), Gd¹⁵¹ (120 d), Gd¹⁵³ (200 d), Tb¹⁵¹ (19 h), Tb¹⁵² (18 h), Tb¹⁵³ (2.58 d), Tb^154m (8 h), Tb¹⁵⁴ (21 h), Tb¹⁶⁵ (5.4 d), Tb¹⁶⁰ (73 d), Dy¹⁵⁵ (10 h), Dy¹⁵⁷ (8.2 h), Tm¹⁶⁵ (1.21d), Tm¹⁶⁷ (9.6 d), Tm¹⁶⁸ (85 d), Yb¹⁶⁹ (32 d), Lu¹⁶⁹ (1.5 d), Lu¹⁷⁰ (2.0 d), Lu¹⁷¹ (8.3 d), Lu¹⁷² (6.7 d), Lu¹⁷³ (1.3 y), Lu^174m (165 d), Hf¹⁷³ (24 h), Hf¹⁷⁵ (70 d), Ta¹⁷⁵ (11 h), Ta¹⁷⁶ (8.0 h), Ta¹⁷⁷ (2.21 d), Ta¹⁷⁹ (1.6 y), Ta^180m (8.1 h);

the EC isotopes of very heavy metals W¹⁸¹ (130 d), Re¹⁸¹ (20 h), Re^182m (13 h), Re¹⁸² (64 h), Re¹⁸³ (71 d), Re^184m (2.2 d), Re¹⁸⁴ (50 d), Re¹⁸⁶ (90 h), Os^183m (10 h), Os¹⁸³ (12 h), Os¹⁸⁵ (94 d), Ir¹⁸⁵ (15 h), Ir¹⁸⁷ (12 h), Ir¹⁸⁸ (1.71 d), Ir¹⁸⁹ (11 d), Ir¹⁹⁰ (11 d), Ir¹⁹² (74 d), Pt¹⁹¹ (3.0 d), Au¹⁹³ (15.8 h), Au¹⁹⁴ (39 h), Au¹⁹⁵ (200 d), Au¹⁹⁶ (5.55 d), Hg^193m (1.1 d), Hg¹⁹³ (6 h), Hg¹⁹⁴ (130 d), Hg¹⁹⁵ (1.66 d), Hg¹⁹⁵ (9.5 h), Hg^197m (24 h), Hg¹⁹⁷ (2.71 d), Tl²⁰⁰ (1.08 d), Tl²⁰¹ (3.04 d), Tl²⁰² (12 d), Tl²⁰⁴ (3.9 y), Pb²⁰⁰ (21 h), Pb²⁰¹ (9.4 h), Pb²⁰² (2.17 d), Bi²⁰³ (12.3 h), Bi²⁰⁴ (11.6 h), Bi^206m (15.3 d), Bi²⁰⁶ (6.3 d), Bi²⁰⁷ (30 y); and

the EC isotopes of actinides Po²⁰⁶ (8.8 d), At²¹⁰ (8.3 h), At²¹¹ (7.2 h), Rn²¹¹ (16 h), Ac²²⁶ (29 h), Pa²²⁸ (22 h), Pa²²⁹ (1.5 d), U²³¹ (4.2 d), Np²³⁴ (4.4 d), Pu²³⁴ (9 h), Pu²³⁷ (45.6 d), Am²³⁹ (12 h), Cm²⁴¹ (35 d), Bk²⁴⁵ (4.95 d), Bk²⁴⁶ (1.8 d).

81. An apparatus according to claim 80, wherein the radioisotope is adducted to an organic compound.

82. An apparatus according to claim 1, wherein the isotope is I¹²³, I¹²⁵, I¹²⁶, Br⁷⁶, or Br⁷⁷.

83. An apparatus according to claim 1, wherein the pulse shape analyzer comprises an article of manufacture comprising a computer readable storage medium having a substrate physically configured to represent a computer program, the computer program comprising means for analysing each pulse shape record by at least one software module having acceptance criteria, rejecting a pulse on-line if it does not satisfy the acceptance criteria of all the software modules utilized, and counting the pulse if it satisfies the acceptance criteria of all the software modules utilized.

84. An apparatus according to claim 1, wherein the detector assembly comprises:

a scintillator crystal,

a photomultiplier optically connected to the scintillator crystal,

an integral photomultiplier base electronics module connected to the photomultiplier, comprising a high voltage power supply, voltage divider, and amplifier,

shields between the base module and the photomultiplier, between the photomultiplier and the scintillator crystal, around the photomultiplier, and around the scintillator-photomultiplier-base module assembly.

85. An apparatus according to claim 1, further comprising an imaging processor that receives counting data from the pulse shape analyzer for a two dimensional array of multiple samples, and reconstructs an image of the array showing the presence of radioisotope.

86. A method for detecting a radioisotope in a sample, comprising:

placing the sample in a sample holder between two opposed detectors;

detecting emissions from the sample using the two opposed detectors to obtain electrical output pulses;

comparing the output pulses to predetermined acceptance criteria for the two detectors;

rejecting output pulses that do not satisfy the predetermined acceptance criteria; and

accepting output pulses that satisfy the predetermined acceptance criteria.

87. A method for detecting a radioisotope in a sample as in claim 86, further comprising:

normalizing the output pulse amplitude to fall within a predetermined range over a baseline and to correlate with the energy of the emissions;

generating a first trigger pulse when there is a triggering output pulse for which the amplitude of the output pulse exceeds a predetermined threshold value, and generating a second trigger pulse when there are two simultaneous triggering output pulses for which the amplitude of the output pulses exceeds the predetermined threshold value, and rejecting pulses that do not exceed the predetermined threshold value;

responsive to a trigger pulse, capturing a predetermined number of subsequent normalized output pulses;

analyzing the captured output pulses as to predetermined isotope and system-dependent acceptance criteria; and

counting pulses that satisfy the acceptance criteria and rejecting pulses that do not satisfy the acceptance criteria.

88. A method according to claim 86, wherein the radioisotope is a coincident gamma/x-ray emitter and the method can detect an amount of the CGX emitter in the sample of about 100 picoCurie.

89. A method according to claim 86, wherein the radioisotope is a coincident gamma/x-ray emitter and the method can detect an amount of the CGX emitter in the sample of about 1 picoCurie.

90. A method according to claim 86, further comprising the step of selecting the radioisotope from the lighter electron capture (EC) isotopes, the EC isotopes of lanthanides, the EC isotopes of heavy metals, and the EC isotopes of actinides.

91. A method according to claim 86, wherein the radioisotope is an isotope of an element that forms covalent bonds.

92. A method according to claim 86, wherein the radioisotope is I¹²³, I¹²⁵, I¹²⁶, Br⁷⁶, or Br⁷⁷.

93. A method according to claim 86, wherein the radioisotope is I¹²⁵.

94. A method according to claim 86, wherein the radioisotope is bound to a chelator conjugated to an organic compound.

95. A method according to claim 86, wherein the radioisotope is an isotope of the family of CGX lanthanide isotopes.

96. A method according to claim 86, wherein the radioisotope is adducted to an organic molecule.

97. A method according to claim 96, wherein the organic molecule is a monoclonal or polyclonal antibody or an antigen.

98. A method according to claim 97, wherein an antibody is used to detect cancerous cells in a physiological sample.

99. A method according to claim 96, wherein the organic molecule is used in a competitive assay.

100. A method according to claim 99, wherein the competitive assay is used to detect contamination of human physiological fluids.

101. A method according to claim 100, wherein the physiological fluid is blood, urine, sputum, tear drops, sweat, amniotic fluid or cerebro-spinal fluid.

102. A method according to claim 99, wherein the competitive assay is used to detect contamination of animal physiological fluids.

103. A method according to claim 99, wherein the competitive assay is used to detect contamination of food and agricultural products.

104. A method according to claim 103, wherein the contamination is the presence of microorganisms and their toxic byproducts.

105. A method according to claim 104, wherein the contamination comprises aflatoxins or mycotoxins.

106. A method according to claim 99, wherein the competitive assay is used to detect contamination of samples of water, soil or air from the environment.

107. A method according to claim 106, wherein the competitive assay is used to detect chemical contamination.

108. A method according to claim 99, wherein the competitive assay is performed upon airborne substances in a clean room environment, and data are used to estimate the number and size distribution of particulates in the air.

109. A method according to claim 86, wherein the method permits detection of one attomole of labeled molecule.

110. A method according to claim 86, wherein the radioisotope is adducted to an organic precursor for the synthesis of a macromolecule.

111. A method according to claim 86, wherein the radioisotope is adducted to a steroid compound.

112. A method according to claim 86, wherein the radioisotope is adducted to estrogen.

113. A method according to claim 112, wherein the level of estrogen and other steroids in physiological fluids is used to diagnose breast cancer.

114. A method according to claim 86, wherein the radioisotope is adducted to a protein.

115. A method according to claim 86, wherein the radioisotope is coupled to a precursor of nucleic acids.

116. A method according to claim 86, wherein the radioisotope is incorporated in a primer for nucleic chain elongation.

117. A method according to claim 116, further comprising using the primer in an in vitro nucleic acid amplification protocol.

118. A method according to claim 116, further comprising using the primer in the polymerase chain reaction (PCR) process.

119. A method according to claim 118, wherein the polynierase chain reaction is stopped while the amplification is still exponential.

120. A method according to claim 116, wherein the primer is used in a linear polymerase reaction.

121. A method according to claim 86, wherein the radioisotope is coupled to a virus, a bacterial cell, an algae cell, a fungal cell, other cell or a protozoa.

122. A method according to claim 121, wherein the virus is an agent of sexually or blood transfusion transmitted disease, and the bacteria is tubercular bacillus or bacteria which are precursors of sexually transmitted diseases.

123. The method of claim 86, further comprising:

performing a setup of the apparatus by;

determining and storing detector dependent permitted ranges for a plurality of pulse shape rejection parameters for at least one detector, the parameters being associated with a desired characteristic emission to be detected;

operating the, apparatus to detect the desired characteristic emission by;

determining pulse shape parameters of an output signal from the at least one detector; and

comparing the pulse shape parameters of an output signal from the at least one detector with the stored detector dependent permitted ranges;

wherein, if the pulse shape parameters of the output signal from the at least one detector do not compare closely with the stored detector dependent permitted ranges, the output signal from the at least one detector is rejected as a detection of the desired characteristic emission.

124. The method according to claim 123, wherein the setup comprises:

providing to the at least one detector a sample of a source of the desired characteristic emission;

acquiring a plurality of pulses from the at least one detector;

building and storing histograms of the plurality of pulses, including current baseline, and pulse widths at 1/4, 1/2 and 3/4 of the pulse amplitude;

determining the detector dependent permitted ranges for a plurality of pulse shape rejection parameters for the at least one detector as those accepting 99%, for each histogram, of the contiguous dominant peak area of the histogram;

storing the determined detector dependent permitted ranges for the plurality of pulse shape rejection parameters for the at least one detector.

125. The method according to claim 123, wherein the at least one detector comprises a first and a second detector, and wherein the setup is performed for the first detector and repeated for the second detector.

126. The method according to claim 125, wherein the setup further comprises:

acquiring a plurality of coincident events, a coincident event being substantial coincidence of output from the first and second detectors;

determining and storing permitted ranges of pulse displacement parameters by building histograms and using the 99% accepting contiguous dominant peak area of the histogram approach; and

storing the permitted ranges of pulse displacement parameters.

127. The method according to claim 126, wherein the setup further comprises:

building three separate energy spectra associated with the desired characteristic emission, including a spectrum for the first detector, a spectrum for the second detector, and a two-dimensional spectrum of coincident events.

128. The method according to claim 123, wherein, in the operating of the apparatus to detect the desired characteristic emission, the determining pulse shape parameters of an output signal from the at least one detector comprises:

acquiring a plurality of data points for a received pulse over a time window spanning the whole width of the pulse and a short time prior to the rise of the pulse;

calculating an average of the first few data points to determine a current baseline;

if the calculated current baseline differs significantly from 0, rejecting the pulse as distorted by pile-up;

if the pulse was not rejected in the preceding step, scanning a plurality of next data points to find a maximum value;

if the maximum value found exceeds an overflow amount, rejecting the pulse;

if the pulse was not rejected in any of the preceding steps, calculating a peak amplitude of the pulse as the difference between the maximum value and the current baseline;

scanning forward and backward from the peak of the pulse to determine time offsets for amplitude levels at a plurality of fractions of the peak amplitude; and

using at least the determined time offsets as the pulse shape parameters of the output signal from the at least one detector.

129. The method according to claim 128, wherein, in operating the apparatus to detect the desired characteristic emission, the comparing of the pulse shape parameters of the output signal with the stored detector dependent permitted ranges comprises:

determining if the time offsets for amplitude levels of 1/2, 1/4 and 3/4, of the peak amplitude of the pulse are within the stored detector dependent permitted ranges.

130. The method according to claim 128, wherein the at least one detector comprises a first and a second detector,

wherein the setup further comprises:

acquiring a plurality of coincident events, a coincident event being substantial coincidence of output from the first and second detectors;

determining and storing permitted ranges of pulse displacement parameters by building histograms and using a 99% accepting contiguous dominant peak area of the histogram approach; and

storing the permitted ranges of pulse displacement parameters; and

wherein operating the apparatus to detect the desired characteristic emission further comprises testing for the occurrence of coincidence during operation, including;

determining the distance between the respective time offsets for the 1/4 amplitude levels on the rising front of the respective pulses from the first and second detectors; and

comparing the determined distance with the stored permitted ranges of pulse displacement parameters.

131. The method according to claim 123, further comprising calibrating the apparatus for a particular isotope.

132. The method of claim 87, wherein the sample comprises a biomolecule to which is adducted a radioisotope selected from the group consisting of the lighter EC isotopes Be ⁷ (53.6 d), Na²² (2.58 y), Ar³⁷ (34.3 d), V ⁴⁹ (330.0 d), Cr⁴⁸ (23.0 h), Cr⁵¹ (27.8 d), Mn⁵² (5.6 d), Mn⁵⁴ (291.0 d), Fe⁵² (8.0 h), Fe⁵⁵ (2.7 y), Co⁵⁵ (18.0 h), Co⁵⁶ (77.3 d), Co⁵⁷ (270.0 d), Co⁵⁸ (71.0 d), Ni⁵⁶ (6.4 d), Ni⁵⁷ (1.5 d), Cu⁶⁴ (12.8 h), Zn⁶² (9.3 h), Zn⁶⁵ (245.0 d), Ga⁶⁶ (9.5 h), Ga⁶⁷ (78.0 h), As⁷¹ (62.0 h), As⁷² (26.0 h), As⁷³ (76.0 d), As⁷⁴ (18.0 d), Se⁷² (8.4 d), Se⁷⁵ (120.0 d), Br⁷⁶ (16.5 h), Br⁷⁷ (2.6 d), Kr⁷⁶ (10.0 h), Kr⁷⁹ (1.6 d), Rb^82m (6.3 h), Rb⁸³ (83.0 d), Rb⁸⁴ (33.0 d), Sr⁸² (25.5 d), Sr⁸³ (1.6 d), Sr⁸⁵ (64.0 d), Y ⁸³ (108.0 d), Y ⁸⁶ (14.6 h), Y ⁸⁷ (3.33 d), Zr⁸⁸ (85.0 d), Zr⁸⁹ (3.29 d), Nb⁹² (10.1 d), Tc^93m (60. d), Tc⁹⁶ (4.3 d), Tc^99m (6.0 h), Ru⁹⁷ (2.9 d), Rh⁹⁹ (16. d), Rh¹⁰⁰ (21. h), Rh¹⁰² (206 d), Pd¹⁰⁰ (4.0 d), Pd¹⁰¹ (8.5 h), Pd¹⁰³ (17 d), Ag¹⁰⁵ (40 d), Ag^106m (8.3 d), Ag^108m (>

5 y), Cd¹⁰⁷ (6.7 h), Cd¹⁰⁹ (470 d), In¹¹¹ (2.81 d), In¹¹³ (118 d), Sn¹¹³ (118 d), Sb¹¹⁹ (158 d), Sb¹²² (2.8 d), Te¹¹⁸ (60 d), Te¹¹⁹ (45 d), Te¹²¹ (17 d), I ¹²³ (4.2 d), I ¹²⁶ (13.2 d), Cs¹³² (6.5 d), Ba¹²⁸ (2.4 d), Ba¹³¹ (11.6 d);

the EC isotopes of lanthanides La¹³⁵ (19.8 h), Ce¹³³ (6.3 h), Ce¹³⁴ (3.0 d), Ce¹³⁵ (22.0 h), Ce¹³⁷ ( 9.0 h), Ce¹³⁹ (140 d), Nd¹⁴⁰ ( 3.3 d), Pm¹⁴³ (265 d), Pm¹⁴⁴ (440 d), Pm¹⁴⁵ (18 y), Pm¹⁴⁶ (710 d), Pm^158m (40.6 d), Sm¹⁴⁵ (340 d), Eu¹⁴⁵ (5.6 d), Eu^146m (1.58 d), Eu¹⁴⁶ (4.6 d), Eu¹⁴⁷ (24 d), Eu¹⁴⁸ (54 d), Eu¹⁴⁹ (120 d), EU^150m (14 h), Eu¹⁵⁰ ( 5 y), Eu¹⁵² (13 y), Gd¹⁴⁶ (48 d), Gd¹⁴⁷ (35 h), Gd¹⁴⁹ (9 d), Gd¹⁵¹ (120 d), Gd¹⁵³ (200 d), Tb¹⁵¹ (19 h), Tb¹⁵² (18 h), Tb¹⁵³ (2.58 d), Tb^154m (8 h), Tb¹⁵⁴ (21 h), Tb¹⁶⁵ (5.4 d), Tb¹⁶⁰ (73 d), Dy¹⁵⁵ (10 h), Dy¹⁵⁷ (8.2 h), Tm¹⁶⁵ (1.21d), Tm¹⁶⁷ (9.6 d), Tm¹⁶⁸ (85 d), Yb¹⁶⁹ (32 d), Lu¹⁶⁹ (1.5 d), Lu¹⁷⁰ (2.0 d), Lu¹⁷¹ (8.3 d), Lu¹⁷² (6.7 d), Lu¹⁷³ (1.3 y), Lu^l74m (165 d), Hf¹⁷³ (24 h), Hf¹⁷⁵ (70 d), Ta¹⁷⁵ (11 h), Ta¹⁷⁶ (8.0 h), Ta¹⁷⁷ (2.21 d), Ta¹⁷⁹ (1.6 y), Ta^180m (8.1 h);

the EC isotopes of very heavy metals W¹⁸¹ (130 d), Re¹⁸¹ (20 h), Re^182m (13 h), Re¹⁸² (64 h), Re¹⁸³ (71 d), Re^184m (2.2 d), Re¹⁸⁴ (50 d), Re¹⁸⁶ (90 h), Os^183m (10 h), Os¹⁸³ (12 h), Os¹⁸⁵ (94 d), Ir¹⁸⁵ (15 h), Ir¹⁸⁷ (12 h), Ir¹⁸⁸ (1.71 d), Ir¹⁸⁹ (11 d), Ir¹⁹⁰ (11 d), Ir¹⁹² (74 d), Pt¹⁹¹ (3.0 d), Au¹⁹³ (15.8 h), Au¹⁹⁴ (39 h), Au¹⁹⁵ (200 d), Au¹⁹⁶ (5.55 d), Hg^193m (1.1 d), Hg¹⁹³ (6 h), Hg¹⁹⁴ (130 d), Hg¹⁹⁵ (1.66 d), Hg¹⁹⁵ (9.5 h), Hg^197m (24 h), Hg¹⁹⁷ (2.71 d), Tl²⁰⁰ (1.08 d), Tl²⁰¹ (3.04 d), Tl²⁰² (12 d), Tl²⁰⁴ (3.9 y), Pb²⁰⁰ (21 h), Pb²⁰¹ (9.4 h), Pb²⁰² (2.17 d), Bi²⁰³ (12.3 h), Bi²⁰⁴ (11.6 h), Bi²⁰⁶ (15.3 d), Bi²⁰⁶ (6.3 d), Bi²⁰⁷ (30 y); and

the EC isotopes of actinides Po²⁰⁶ (8.8 d), At²¹⁰ (8.3 h), At²¹¹ (7.2 h), Rn²¹¹ (16 h), Ac²²⁶ (29 h), Pa²²⁸ (22 h), Pa²²⁹ (1.5 d), U²³¹ (4.2 d), Np²³⁴ (4.4 d), Pu²³⁴ (9 h), Pu²³⁷ (45.6 d), Am²³⁹ (12 h), Cm²⁴¹ (35 d), Kb²⁴⁵ (4.95 d), Kb²⁴⁶ (1.8 d).