Gamma-ray detectors for downhole applications

Patent metadata

Field	Value
Publication number	US-10145979-B2
Application number	US-201715454458-A
Country	US
Kind code	B2
Filing date	Mar 9, 2017
Priority date	May 22, 2009
Publication date	Dec 4, 2018
Grant date	Dec 4, 2018

Abstract

Methods and related systems are described for gamma-ray detection. A gamma-ray detector is made depending on its properties and how those properties are affected by the data analysis. Desirable properties for a downhole detector include; high temperature operation, reliable/robust packaging, good resolution, high countrate capability, high density, high Z, low radioactive background, low neutron cross-section, high light output, single decay time, efficiency, linearity, size availability, etc. Since no single detector has the optimum of all these properties, a downhole tool design preferably picks the best combination of these in existing detectors, which will optimize the performance of the measurement in the required environment and live with the remaining non-optimum properties. A preferable detector choice is one where the required measurement precision (logging speed) is obtained for all of the required inelastic elements and/or minimization of unwanted background signals that complicate the data analysis.

First claim

What is claimed is:

1. A system for detecting gamma-rays downhole comprising:
a tool housing adapted and dimensioned to be deployed in a borehole within a subterranean formation; and
a scintillator material mounted within the tool housing and emitting light when gamma-rays are absorbed, and the scintillator material having an associated decay time of less than about 40 ns.

2. The system according to claim 1 , wherein the scintillator material is selected from a group consisting of: GSO-Z, LuAP, LaCl 3 , LaBr 3 , La(Br,Cl) 3 , YAP, and LuAG.

3. The system according to claim 1 further comprising a photodetector mounted within the tool housing and adapted so as to detect light emitted by the scintillator material.

4. The system according to claim 1 , wherein the system is adapted to detect gamma-rays primarily produced by neutron inelastic scattering.

5. The system according to claim 1 , wherein the system is adapted to detect gamma-rays primarily produced by neutron capture events.

6. The system according to claim 1 , wherein the system is adapted to detect x-rays or gamma-rays scattered by the subterranean formation.

7. The system according to claim 1 , wherein the system is adapted to detect gamma-rays primarily produced by inelastic scattering and minimize the sensitivity to epithermal neutrons.

8. The system according to claim 1 , further comprising a nuclear source mounted within the tool housing and adapted so as to emit nuclear radiation into the subterranean formation.

9. The system according to claim 8 , wherein the nuclear source includes a neutron source adapted to emit neutrons into the subterranean formation so as to produce gamma-rays.

10. The system according to claim 8 , wherein the nuclear source is an x-ray source adapted to emit x-rays into the subterranean formation.

11. The system according to claim 10 , wherein the x-ray source is an accelerator-based x-ray source.

12. A downhole tool comprising:
a tool housing adapted and dimensioned to be deployed in a borehole within a subterranean formation;
an x-ray or gamma ray source mounted within the tool housing and adapted so as to emit x-rays or gamma rays into the subterranean formation; and
a scintillator material mounted within the tool housing, and emitting light when x-rays or gamma rays are absorbed, the scintillator material being selected from a group consisting of: GSO-Z, LuAP, LaCl 3 , LaBr 3 , La(Br,Cl) 3 and LuAG.

13. The downhole tool according to claim 12 , wherein the scintillator material has an associated decay time that is short enough to allow for processing of x-ray or gamma ray counts having reduced losses and distortion.

14. The downhole tool according to claim 13 , wherein the associated decay time is less than about 100 ns.

15. The downhole tool according to claim 13 , wherein the associated decay time is less than about 40 ns.

16. The downhole tool according to claim 12 , wherein the x-ray source is an accelerator-based x-ray source.

17. The downhole tool according to claim 12 , wherein the gamma ray source is a radioactive gamma ray source.

18. A method comprising:
deploying a tool in a borehole within a subterranean formation; and
detecting gamma-rays using a scintillator material and a photodetector mounted within the tool, and the scintillator material having an associated decay time of less than about 40 ns, the scintillator material emitting light when gamma-rays are absorbed, and the photodetector detecting light emitted by the scintillator material, and
determining one or more properties of the subterranean formation based at least in part on the detected gamma-rays.

19. The method according to claim 18 , wherein the scintillator material is primarily of a type selected from the group consisting of: LaCl 3 , LaBr 3 , La(Br,Cl) 3 , YAP, and LuAG.

20. The method according to claim 18 , wherein the one or more properties of the subterranean formation comprise elemental yields.

Assignees

• Schlumberger Technology Corp

Inventors

• Roscoe Bradley Albert
• Grau James A
• Zhou Zilu
• Stephenson Kenneth E
• Berheide Markus

Classifications

• G01T1/20

  with scintillation detectors · CPC title

• G01V5/105

  the neutron source being of the pulsed type · CPC title

• G01T1/208

  Circuits specially adapted for scintillation detectors, e.g. for the photo-multiplier section · CPC title

• G01V5/08

  using primary nuclear radiation sources or X-rays {(, e.g. for inducing radioactivity; investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays, neutrons G01N23/00)} · CPC title

• G01V5/102

  the neutron source being of the pulsed type · CPC title