PROFILE S and C Series

Similar documents
PROFILE S and C Series P-type Semi-planar and Coaxial HPGe Detectors

ORTEC. PROFILE Coaxial HPGe Photon Detector Product Configuration Guide

EFFICIENCY AND RESOLUTION OF GERMANIUM DETECTORS AS A FUNCTION OF ENERGY AND INCIDENT GEOMETRY

The Shape of the Full-Energy Gamma Ray Peak in Germanium Detectors for Different Energies and Incident Geometries

ORTEC. Overview of Semiconductor Photon Detectors. GEM (P-type) and GAMMA-X (N-type) Coaxial Detectors. Efficiency as a Function of Energy

ORTEC. GEM Series Coaxial HPGe Detector Product Configuration Guide. Configuration Guidelines

ORTEC. GEM Series Coaxial HPGe Detector Product Configuration Guide. Configuration Guidelines

High-Performance Germanium Coaxial Detectors for Safeguards and Non-Destructive Assay Product Configuration Guide

Advanced and Special Detector Programs from ORTEC Historical and Next Step Perspective

ORTEC GMX Series Coaxial HPGe Detector Product Configuration Guide

Background Reduction Using Collimators on a Portable HPGe Nuclide Identifier

FRAM V5.2. Plutonium and Uranium Isotopic Analysis Software

ISOCS / LabSOCS. Calibration software for Gamma Spectroscopy

Performance of the True Coincidence Correction Method in GammaVision. Keyser, Ronald M., Haywood, Susan E., and Upp, Daniel L.

ANGLE 4. Advanced Gamma Spectroscopy Efficiency Calibration Software

Compton suppression spectrometry

Gamma Analyst Performance Characteristics (MDAs)

Calibration of A Small Anode Germanium Well Detector

A Digital Method for Dead Time Compensation in Nuclear Spectroscopy

ORTEC. SLP Series Silicon Lithium-Drifted Planar Low-Energy X Ray Detector Product Configuration Guide

ENERGY PEAK STABILITY WITH COUNT RATE FOR DIGITAL AND ANALOG SPECTROMETERS

EFFICIENCY SIMULATION OF A HPGE DETECTOR FOR THE ENVIRONMENTAL RADIOACTIVITY LABORATORY/CDTN USING A MCNP-GAMMAVISION METHOD

The Best Gamma-Ray Detector

COUNT RATE EFFECTS ON PEAK SHAPE AND THROUGHPUT IN DIGITAL AND ANALOG GAMMA RAY SPECTROMETRY

Minimum Detectable Activity Estimates for a Germanium-Detector Based Spectroscopic Portal Monitor

Establishing an ISO-CART Measurement Station to Meet Government Burial Regulations for Radioactive Material

Geometric Considerations in the

Identification of Naturally Occurring Radioactive Material in Sand

ORTEC. GLP Series Planar HPGe Low-Energy Detector Product Configuration Guide. Configuration Guidelines

Non-Destructive Assay Applications Using Temperature-Stabilized Large Volume CeBr Detectors 14277

Chem 481 Lecture Material 3/20/09

Radioactive Waste Management

DESIGN, DEVELOPMENT AND TESTING OF AN AUTOMATED SEGMENTED GAMMA SCANNER FOR MEASURING NUCLEAR POWER STATION RADIOACTIVE WASTE

VALIDATION OF IQ3 MEASUREMENTS FOR HIGH-DENSITY LOW-ENRICHED-URANIUM WASTE DRUMS AT PELINDABA

The first model was based only on the CANBERRA information which we. drawing. Canberra refused any other information.

European Project Metrology for Radioactive Waste Management

GLP Series Planar HPGe Low-Energy Detector Product Configuration Guide

Recent improvements in on-site detection and identification of radioactive and nuclear material

Inaccuracy Determination in Mathematical Model of Labsocs Efficiency Calibration Program

Determination of the activity of radionuclides

DETERMINATION OF CORRECTION FACTORS RELATED TO THE MANGANESE SULPHATE BATH TECHNIQUE

SOME ASPECTS OF MONTE CARLO SIMULATION FOR EFFICIENCY CALIBRATION OF GERMANIUM DETECTORS

Enriched Uranium Waste Assay at AWE

ORTEC was founded in 1960 by researchers from Oak Ridge National Labs to commercialize charged particle detectors

WM2014 Conference, March 2 6, 2014, Phoenix, Arizona, USA

PINS3-CW. Portable Chemical Identification System

NUCL 3000/5030 Laboratory 2 Fall 2013

Collimated LaBr 3 detector response function in radioactivity analysis of nuclear waste drums

Ultra-Low Background Counting and Assay Studies At SNOLAB

PINS3-CF. Portable Chemical and Explosive Identification System

Indian J.Sci.Res.2(3) :25-32, 2011

Library of uranium and plutonium reference spectra Introduction

PYCKO SCIENTIFIC LIMITED

arxiv:nucl-ex/ v2 21 Jul 2005

Interactive Web Accessible Gamma-Spectrum Generator & EasyMonteCarlo Tools

Characteristics of Filtered Neutron Beam Energy Spectra at Dalat Reactor

Renewed whole-body counting chamber in STUK

List of Nuclear Medicine Radionuclides. Nuclear Medicine Imaging Systems: The Scintillation Camera. Crystal and light guide

1 cm. Cu electrode. Ge crystal. end cap. Dead layer. crystal cup

Application of Spectral Summing to Indeterminate Suspect Low-Level Drums at Los Alamos National Laboratory

1 Introduction. 2 Method. Robert Metzger 1,*, Kenneth Van Riper 2, and George Lasche 3

Depth Distribution of H-3, C-14 and Co-60 in Decommissioning of the Biological Shielding Concrete of KRR-2

Digital simulation of neutron and gamma measurement devices

ISOTOPIC. A Practical, Flexible, and Defendable Solution for Gamma Spectrometry Waste Assay Measurements

First tests of the big volume ultra low background gamma spectrometer

Ultra-Low Background Measurement Capabilities At SNOLAB

Distinguishing fissions of 232 Th, 237 Np and 238 U with beta-delayed gamma rays

IdentiFINDER Digital Hand Held Spectrometer & Dose Rate Meter for Portable Applications

Detection efficiency of a BEGe detector using the Monte Carlo method and a comparison to other calibration methods. Abstract

Alternative Approach for Efficiency Data Generation in Neutron Activation Analysis

Semiconductor Detector

Hands on LUNA: Detector Simulations with Geant4

GUIDE TO LABORATORY SURVEYS. Introduction

Introduction to gamma spectroscopy on a budget. Daniel Emes SA Radiation

Compton Camera. Compton Camera

High Purity Germanium Detector Calibration at ISOLDE

The Efficiency Characterization of Germanium Detectors at Energies less than 45 kev

Gamma and X-Ray Detection

RMCC CANBERRA Latest developments

Nuclear Lifetimes. = (Eq. 1) (Eq. 2)

NGN PhD Studentship Proposal

Low Background Counting At SNOLAB

"Neutron Flux Distribution"

IDENTIFICATION AND QUANTIFICATION OF RADIONUCLIDES IN HISTORICAL WASTE AT ANSTO

Silicon Drift Detectors: Understanding the Advantages for EDS Microanalysis. Patrick Camus, PhD Applications Scientist March 18, 2010

WM2013 Conference, February 24 28, 2013, Phoenix, Arizona USA. Screening and Spectral Summing of LANL Empty Waste Drums 13226

arxiv: v1 [physics.ins-det] 14 Nov 2017

TECHNICAL WORKING GROUP ITWG GUIDELINE ON LABORATORY APPLICATIONS OF HIGH-RESOLUTION GAMMA SPECTROMETRY

Simulations, backgrounds, and uncertainties in PICO-2L. Alan Robinson May 20, 2015 AARM, Rapid City South Dakota

ɣ-radiochromatography

Application of Nuclear Physics

CVD Diamond History Introduction to DDL Properties of Diamond DDL Proprietary Contact Technology Detector Applications BDD Sensors

Neutron Induced Nuclear Counter Effect in Hamamatsu Silicon APDs and PIN Diodes

WM 05 Conference, February 27 - March 3, 2005, Tucson, AZ INTEGRATED WASTE ASSAY SYSTEM (IWAS) AND ANALYSIS ENHANCEMENTS

QSM 5.1 FAQs. For a test with a recommended maximum holding time measured in hours, the holding time shall be tracked by the hour.

Gamma-Spectrum Generator

PRODUCTS FOR EDUCATION AND TRAINING

IAEA-TECDOC-1049 XA

AGATA preamplifier performance on large signals from a 241 Am+Be source. F. Zocca, A. Pullia, D. Bazzacco, G. Pascovici

Transcription:

P-type Semi-planar and Coaxial HPGe Detectors Exceptional Resolution and Stable, Low-Energy Efficiency Comprehensive Solutions to Demanding Applications

Exceptional resolution and stable, low energy efficiency are critical requirements to optimize sample counting which improves your results accuracy and throughput. PROFILE "S" and "C" Series HPGe detectors offer both. The ORTEC PROFILE Series of P-type High Purity Germanium (HPGe) detectors match the crystal dimensions to your application for optimal counting geometry and results. Both S and C Series crystals incorporate a Stable, Thin Front Contact (STFC) which provides excellent gamma transmission for energies as low as 3 kev. This advanced contact design does not penetrate into the germanium crystal at room temperature which ensures stable detector efficiency, even when stored warm. Benefits Greater counting efficiency lower counting time and lower Minimum Detectable Activity Improved X-ray nuclide identification extended lower energy range operation down to 3 kev Improved multi-peak nuclide identification enhanced resolution Features Thin front contact Maximized crystal diameter within the endcap Thin front contact P-type detectors with multiple crystal geometries Simplified handling and lower storage costs without loss of detector efficiency warm storage capability Stable contact (no dead layer growth at room temperature). PROFILE C-Series detectors employ "nearly square" (diameter < length) coaxial crystal structures. This provides the same resolution, but better absolute efficiency than conventional P-type coaxial (GEM) detectors below kev. The C-Series detectors offer better resolution than N-type (GMX) detectors for a given front window efficiency. For energies above 1 MeV, C-Series detectors offer excellent resolution and efficiency performance, similar to conventional P-type coaxial detectors (GEM). PROFILE S-Series detectors employ "over-square" (diameter > length) semi-planar crystal structures. This over-square geometry improves low to medium energy resolution, compared to coaxial crystal geometry, by reducing the back-contact capacitance. The detector s surface area improves low to medium energy efficiency when used for samples such as: Point sources on-endcap Filter paper samples on-endcap Samples presented in bottles and pots on-endcap Bio-assay applications (e.g., lung monitoring) Waste drum monitoring For a given relative (IEEE) efficiency, PROFILE Series detectors represent the "best use" of germanium material producing the maximum absolute counting efficiency for all geometries. Figure 1. P-type HPGe crystal geometries. 2

Figure 2 shows the extensive improvement in efficiency at lower energies for a PROFILE S detector when measuring a point source. The S85 S-Series detector s absolute efficiency is significantly higher between 0 kev and 20 kev when compared to the same % relative efficiency coaxial P- and N-type detectors. At 59 kev, the S-Series detector area is nearly 6X more efficient than a P-type coaxial detector (GEM) and almost 2X more efficient than a coaxial N-type (GMX) low-energy detector due to its greater front surface area. As expected, curves converge at 1332 kev, where relative efficiency is measured. Measured (color) and calculated (black) curves show absolute efficiency versus energy for a point source positioned cm from the detector endcap. Measured data points are obtained using mixed NIST traceable sources. Calculated data points were generated using MCNP-X. Note, energy range shown is from 20 kev to 4 MeV. Figure 2. Efficiency vs. Energy for S85, GEM and GMX detectors having % relative efficiency and a Point Source positioned cm away from the front of the endcap. Figure 3 reinforces the marked improvement in efficiency for the PROFILE S detectors when measuring a filter paper on-endcap source. S85 has significantly higher absolute efficiency at all energies below 1 MeV down to 10 kev. Due to a diameter crystal, at 122 kev, the S-Series detector is 2.5X more efficient than a P-type coaxial and nearly 2X more efficient than an N-type low-energy detector. Calculated (color) curves show absolute efficiency versus energy for a 100 mm diameter filter paper source positioned on the detector endcap. Note, energy range shown is from 10 kev to 4 MeV. Figures 4 and 5 highlight the robust peak shape of PROFILE S and C detectors measuring 55 Fe and 109 Cd spectra respectively. Low energy peak at 5.9 kev on the left, and 22 and 88 kev peaks on the right are well defined above the background. Figure 3. Efficiency vs. Energy for S85, GEM and GMX detectors having % relative efficiency and a 100 mm diameter Filter Paper Source positioned on the endcap. Figure 4. 55 Fe spectra measured with S. Figure 5. 109 Cd spectra measured with C20. 3

General Guidelines for Choosing a Profile S Detector For a close or on-endcap sample, the detector diameter should exceed the sample diameter by 20% or more. Beyond % the gain in efficiency is small. In addition, if the detector diameter exceeds the sample diameter by 20% or more, errors due to irreproducibility of the sample position will be minimal. If budget constraints must be considered, first select the largest diameter in comparison with the optimum diameter. Selection of a deeper detector will further increase the absolute efficiency, specifically at higher energies. If the application or situation includes prolonged storage of the detector in an ambient environment, selection of the S- or C-Series PROFILE detector will maintain excellent performance, with no degradation in the low-energy range. Table 1. HPGe Detector Selection Guide for Various Counting Geometries Relative to Energies of Interest Overall Guidelines on the Choice of High Purity Germanium (HPGe) Detector Source Energy (kev) Marinelli Beaker Near or Far Point Source Large Surface Area Preference Efficiency Resolution Efficiency Resolution Efficiency Resolution 3 to 2000 GMX PROFILE C PROFILE S PROFILE S PROFILE S PROFILE S 3 to 00 GMX PROFILE C PROFILE C PROFILE C PROFILE C PROFILE S 20 to 2000 GMX PROFILE M PROFILE F PROFILE F PROFILE F PROFILE F to 00 GEM GEM GEM GEM or PROFILE F GEM or PROFILE F PROFILE F 20 to above 00 GMX or PROFILE C or PROFILE C or PROFILE C or PROFILE C or PROFILE C or above 00 GEM or GEM or GEM or GEM or GEM or GEM or Neutron Damage GMX GMX GMX GMX GMX GMX High Count Rate small GEM or GMX small GEM or GMX small GEM small PROFILE F or small PROFILE S small PROFILE F or small PROFILE S small PROFILE F or small PROFILE S 4

Table 2. PROFILE Series GEM Detector Specification Information Model No. GEM-S20 GEM-S58 GEM-S GEM-S GEM-S85 GEM-S94 GEM-C10 GEM-C15 GEM-C20 GEM-C GEM-C GEM-C35 GEM-C40 GEM-C45 GEM-C GEM-C55 GEM-C GEM-C65 GEM-C GEM-C75 GEM-C GEM-C90 GEM-C100 GEM-C110 GEM-C120 GEM-C1 GEM-C140 GEM-C1 GEM-C175 Crystal Dimension Energy Resolution () Peak Shape (+0/ 2 mm) 58 85 94 (+2/ 2 mm) * * * 57 57 57 ** 82** 92 92 92 94** Length Minimum 20 Length Minimum 44 62 75 58 62 77 86 85 56 61 82 91 98 67 74 81 100 5.9 kev 3 400 4 4 0 0 5.9 kev 0 635 690 715 7 7 0 0 0 0 0 0 0 10 10 46 kev 4 0 575 0 6 46 kev @122 kev 0 0 0 @122 kev 0 820 820 8 8 8 8 1200 1200 10 10 @1.33 MeV (kev) @1.33 MeV (kev) 2.2 2.3 2.3 FW.1M/ 0 0 5 0 0 0 FW.1M/ FW.02M/ 2.65 2.75 2.90 2.90 2.90 FW.02M/ 2. P:C 35 35 40 40 55 65 P:C 41 46 56 62 66 67 73 75 73 73 85 86 90 90 Nominal Relative Efficiency % 7 15 20 28 65 Nominal Relative Efficiency % 10 15 20 35 40 45 55 65 75 90 100 110 120 1 140 1 175 Endcap (mm) Endcap (mm) 76 76 Notes 1) = Full Width at Half Maximum; FW.1M = Full Width at One-Tenth Maximum; FW.02M = Full Width at One-Fiftieth Maximum; total system resolution for a source at counts/s measured in accordance with ANSI/IEEE Std. 3-1996, using ORTEC standard electronics. 2) Measured at optimum analog or equivalent digital shaping time using ORTEC electronics. 3) PROFILE S and C detectors come with a standard Carbon Fiber window. For improved performance between 3 and 5 kev select the Beryllium window option. 4) The proprietary contact employed in the S- and C-Series detectors offer exceptionally high transmission at energies below 40 kev. Warm storage will not degrade the transmission efficiency of the front contact. *) May include 59 mm maximum diameter. **) tolerance +0/ 2. Ordering Information See the PROFILE Detector Configuration Guide for complete ordering information. 5

Specifications subject to change 102317