<p>The domestically developed prompt fission neutron uranium logging (PFNUL) instrument for uranium exploration represents a significant advancement in China’s deep uranium mining efforts, although it has considerable challenges and complexity. This paper presents the development of a new prompt fission neutron uranium logging instrument (named UNL4) that integrates a domestic D-T neutron generator, two <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({^{3}\hbox {He}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>3</mn> </mmultiscripts> <mtext>He</mtext> </mrow> </math></EquationSource> </InlineEquation> proportional detectors, a lanthanum bromide (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\hbox {LaBr}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>LaBr</mtext> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation>) gamma-ray detector, and a digital multi-channel pulse amplitude analyzer. The near <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({^{3}\hbox {He}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>3</mn> </mmultiscripts> <mtext>He</mtext> </mrow> </math></EquationSource> </InlineEquation> detector is shielded with 1&#xa0;mm of cadmium (Cd) and 5&#xa0;mm of high-density polyethylene (HDPE), enabling efficient epithermal neutron detection, whereas the far <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({^{3}\hbox {He}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>3</mn> </mmultiscripts> <mtext>He</mtext> </mrow> </math></EquationSource> </InlineEquation> detector measures thermal neutrons. A <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\hbox {LaBr}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>LaBr</mtext> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> detector is employed for gamma-ray detection, primarily originating from uranium decay. High-speed analog-to-digital converter (ADC) and field-programmable gate array (FPGA) technologies are used to achieve rapid acquisition and transmission of both dual-energy neutron time spectra and gamma spectra. Moreover, this paper proposes a fast signal-shaping method, which reduces the dead time effect in <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({^{3}\hbox {He}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>3</mn> </mmultiscripts> <mtext>He</mtext> </mrow> </math></EquationSource> </InlineEquation> detectors on neutron time spectra. Experiments conducted in standard model boreholes with varying uranium contents demonstrated a strong linear relationship between the epithermal-to-thermal neutron ratio (<i>E</i>/<i>T</i>) and uranium content, with a fitting coefficient of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(R^2&gt;0.999\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>R</mi> <mn>2</mn> </msup> <mo>&gt;</mo> <mn>0.999</mn> </mrow> </math></EquationSource> </InlineEquation>, confirming the accuracy of the instrument. The <i>E</i>/<i>T</i> value repeatability, in both short-term (3.16% <i>RSD</i>) and long-term (1.2% <i>RSD</i>) measurements, showed excellent stability. In addition, the instrument demonstrated good performance at neutron-logging speeds of <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(0.3\sim {3\,\mathrm{m/min}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0.3</mn> <mo>∼</mo> <mrow> <mn>3</mn> <mspace width="0.166667em" /> <mrow> <mi mathvariant="normal">m</mi> <mo stretchy="false">/</mo> <mi mathvariant="normal">min</mi> </mrow> </mrow> </mrow> </math></EquationSource> </InlineEquation> (<i>E</i>/<i>T</i> values) and gamma logging speeds of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(1\sim {10\,\mathrm{m/min}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>∼</mo> <mrow> <mn>10</mn> <mspace width="0.166667em" /> <mrow> <mi mathvariant="normal">m</mi> <mo stretchy="false">/</mo> <mi mathvariant="normal">min</mi> </mrow> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Through measurements in two ore sections of the PU model with uranium contents of 87.1&#xa0;ppm and 45.6&#xa0;ppm&#xa0;showed that <i>RD</i> remained below approximately 10% at logging speeds of 0–2 m/s in both&#xa0;cases, satisfying the requirements for engineering applications. This marks the first successful development of a neutron-logging instrument for uranium exploration based on a domestic neutron generator and signifies an important contribution to uranium resource exploration.</p>

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Prompt fission neutron uranium logging (III): logging instrument

  • Hai-Tao Wang,
  • Yan Zhang,
  • Chi Liu,
  • Jian-Qiang Xu,
  • Li-Jiao Zhang,
  • Zhi-Feng Liu,
  • Xiong-Jie Zhang,
  • Rui Chen,
  • Qi Liu,
  • Ren-Bo Wang,
  • Shu-Min Zhou,
  • Bin Tang

摘要

The domestically developed prompt fission neutron uranium logging (PFNUL) instrument for uranium exploration represents a significant advancement in China’s deep uranium mining efforts, although it has considerable challenges and complexity. This paper presents the development of a new prompt fission neutron uranium logging instrument (named UNL4) that integrates a domestic D-T neutron generator, two \({^{3}\hbox {He}}\) 3 He proportional detectors, a lanthanum bromide ( \(\hbox {LaBr}_{3}\) LaBr 3 ) gamma-ray detector, and a digital multi-channel pulse amplitude analyzer. The near \({^{3}\hbox {He}}\) 3 He detector is shielded with 1 mm of cadmium (Cd) and 5 mm of high-density polyethylene (HDPE), enabling efficient epithermal neutron detection, whereas the far \({^{3}\hbox {He}}\) 3 He detector measures thermal neutrons. A \(\hbox {LaBr}_{3}\) LaBr 3 detector is employed for gamma-ray detection, primarily originating from uranium decay. High-speed analog-to-digital converter (ADC) and field-programmable gate array (FPGA) technologies are used to achieve rapid acquisition and transmission of both dual-energy neutron time spectra and gamma spectra. Moreover, this paper proposes a fast signal-shaping method, which reduces the dead time effect in \({^{3}\hbox {He}}\) 3 He detectors on neutron time spectra. Experiments conducted in standard model boreholes with varying uranium contents demonstrated a strong linear relationship between the epithermal-to-thermal neutron ratio (E/T) and uranium content, with a fitting coefficient of \(R^2>0.999\) R 2 > 0.999 , confirming the accuracy of the instrument. The E/T value repeatability, in both short-term (3.16% RSD) and long-term (1.2% RSD) measurements, showed excellent stability. In addition, the instrument demonstrated good performance at neutron-logging speeds of \(0.3\sim {3\,\mathrm{m/min}}\) 0.3 3 m / min (E/T values) and gamma logging speeds of \(1\sim {10\,\mathrm{m/min}}\) 1 10 m / min . Through measurements in two ore sections of the PU model with uranium contents of 87.1 ppm and 45.6 ppm showed that RD remained below approximately 10% at logging speeds of 0–2 m/s in both cases, satisfying the requirements for engineering applications. This marks the first successful development of a neutron-logging instrument for uranium exploration based on a domestic neutron generator and signifies an important contribution to uranium resource exploration.