Development of a position sensitive neutron detector with high efficiency and energy resolution for use at high-flux beam sources.
We are developing a high-efficiency neutron detector with 1 cm position resolution and coarse energy resolution for use at high-flux neutron source Neutron source is a general term referring to a variety devices that emit neutrons, irrespective of the mechanism used to produce the neutrons. Depending upon variables including the energy of the neutrons emitted by the source, the rate of neutrons emitted by the source, the size facilities currently proposed or under construction. The detector concept integrates a segmented [.sup.3]He ionization ionization: see ion.
Process by which electrically neutral atoms or molecules are converted to electrically charged atoms or molecules (ions) by the removal or addition of negatively charged electrons. chamber with the position sensitive, charged particle charged particle
An elementary particle, such as a proton or electron, with a positive or negative electric charge. collection methods of a MicroMegas detector MicroMegas (MicroMEsh GAseous Structure) is a detector first developed at CERN in Geneva for high-energy physics charged-particle tracking applications. It has shown great promise for handling high data rates with a rather low-cost structure. References
1.  . Neutron absorption on the helium produces protons and tritons that ionize i·on·ize
To dissociate atoms or molecules into electrically charged atoms or radicals.
ion·iz the fill gas. The charge is amplified in the field region around a wire mesh wire mesh, wire netting n → tela metálica and subsequently detected in current mode by wire strips mounted on a substrate. One module consisting of a high-voltage plate, a field-shaping high-voltage plate, a grid and wire strips defines a detection region. For 100% efficiency, detector modules are consecutively placed along the beam axis. Analysis over several regions with alternating wire strip orientation provides a two-dimensional beam profile. By using [.sup.3]He, a 1/v absorption gas, each axial region captures neutrons of a different energy range, providing an energy-sensitive detection scheme especially useful at continuous beam sources.
Key words: cold neutrons; ionization chamber; MicroMegas detector; neutron detector.
1. Introduction and Discussion
The success of several proposed cold-neutron fundamental physics experiments depends on the ability to characterize the beam profile for understanding spatial and energy dependent systematics systematics: see classification. . Transmission experiments for both materials research and fundamental physics benefit from simultaneous characterization of the beam with downstream detectors. To achieve high count-rate profiles of the total beam area, a position and energy sensitive neutron detector must be capable of processing the high neutron source flux. Current good-resolution, position sensitive neutron detectors are limited in the flux they can process by intensity-dependent dead time. At present, there is no position sensitive neutron detector that can process neutron currents greater than [10.sup.6]/s with a nearly 100% efficiency over an active area of about 10 cm X 10 cm.
We are developing a neutron detector appropriate for high-flux sources in particular at the cold-neutron facility of the Spallation Neutron Source The Spallation Neutron Source (SNS) is an accelerator-based neutron source being built in Oak Ridge, Tennessee, USA, by the U.S. Department of Energy (DOE). SNS is being designed and constructed by a unique partnership of six DOE national laboratories: Argonne, Lawrence Berkeley, (SNS SNS sympathetic nervous system. )  currently under construction, and at the High Flux Isotope Reactor The High Flux Isotope Reactor (or HFIR) is a research nuclear reactor located at Oak Ridge National Laboratory in Oak Ridge, Tennessee, United States. Operational since 1966, the HFIR is an 85 MW reactor designed for the production of special radioisotopes (it is the only US (HFIR HFIR High Flux Isotope Reactor (at ORNI) )  currently being expanded to include a very low-energy beam line, both located at the Oak Ridge National Laboratory Oak Ridge National Laboratory (ORNL) is a multiprogram science and technology national laboratory managed for the United States Department of Energy by UT-Battelle, LLC. ORNL is located in Oak Ridge, Tennessee, near Knoxville. (ORNL ORNL Oak Ridge National Laboratory ). We aim to design a detector that can collect the entire neutron beam on the order of 5 X [10.sup.8] [cm.sup.-2] [s.sup.-1] over a surface area of ~100 [cm.sup.2] expected at these facilities.
Our detector design builds on the success of a segmented helium-3 ionization chamber and a neutron MicroMegas detector. The ionization chamber technique is employed to convert neutrons to charged particles in a large spatial region. The MicroMegas (MicroMesh Gaseous Structure) detector concept developed at the European laboratory, CERN CERN or European Organization for Nuclear Research, nuclear and particle physics research center straddling the French-Swiss border W of Geneva, Switzerland. , is used to convert charged particles to an electron shower that is subsequently detected on one-dimensional wire strip arrays or on two-dimensional pixels.
A segmented ionization chamber based on a helium-3 and argon argon (är`gŏn) [Gr.,=inert], gaseous chemical element; symbol Ar; at. no. 18; at. wt. 39.948; m.p. −189.2°C;; b.p. −185.7°C;; density 1.784 grams per liter at STP; valence 0. gas mixture with coarse spatial and energy resolution was built for a preliminary fundamental physics measurement of the neutron spin rotation in a liquid helium Liquid helium target . (For a description of this experiment, please see the article in the Weak Hadronic Interaction section of these proceedings.) Neutrons are detected through their capture on [.sup.3]He producing a triton and proton: n + [.sup.3]He [right arrow] [.sup.3]H + [.sup.1]H with a Q value of 750 keV. These charged reaction products ionize the fill gas producing charged particles that are subsequently detected. In the segmented ionization chamber, a gas ratio of 0.5 bar [.sup.3]He and 3 bar Ar produced 2 X [10.sup.4] ion pairs on average per neutron absorbed, that were collected on charge collecting plates divided into independent quadrants. The quadrants provided coarse position sensitivity with valuable count-rate information as a function of upper, lower, right and left sides of the beam. To improve the position resolution, we propose to use wire strips to collect the electron charge associated with an absorbed neutron.
Originally designed for charged particle detection and later modified for fast neutron fast neutron
A neutron that is not in thermal equilibrium with the surrounding medium, especially one produced by fission. Compare slow neutron. See also fast-breeder reactor. detection, the MicroMegas detector concept has proven capable of processing a high charged particle rate with relatively fast recovery times to minimize dead time. Building on this success, a slow neutron slow neutron
A neutron in thermal equilibrium with the surrounding medium, especially one produced by fission and slowed by a moderator. Also called thermal neutron. MicroMegas detector has been developed by a team (including some of the authors of this paper) at ORNL ,. A solid neutron converter material of boron boron (bōr`ŏn) [New Gr. from borax], chemical element; symbol B; at. no. 5; at. wt. 10.81; m.p. about 2,300°C;; sublimation point about 2,550°C;; sp. gr. 2.3 at 25°C;; valence +3. is placed on the aluminum drift electrode producing alpha particles Alpha particles
Helium nuclei, which are abundant throughout the universe both as radioactive-decay products and as key participants in stellar fusion reactions. that ionize the fill gas mixture of argon and methane. The electrons are accelerated to a nickel mesh grid in the conversion gap and multiplied in the amplification gap to produce an electron shower that is subsequently detected on pixels in a two-dimensional array.
This neutron imaging system will be the first position sensitive transmission monitor that can process relatively high neutron rates and provide timing information. The low energy neutron MicroMegas detector is optimized for performance at the SNS as an upstream beam monitor by absorbing 10% or less of the neutrons while minimizing scattering effects that might disturb the beam . The short drift path for the ions ensures low dead time for the expected count rates.
In Fig. 1, we provide a schematic drawing Schematic drawing
Concise, graphical symbolism whereby the engineer communicates to others the functional relationship of the parts in a component and, in turn, of the components in a system. of our proposed detector that uses helium-3 to convert incoming neutrons to charged particles and detects the associated charge on wire strips. Our initial goal is for a 1 cm position resolution, using 5 mm wide strips located below a wire mesh that amplifies the electron charge in a localized region. The fill gas pressure of argon will be optimized for limiting the transverse range of the protons and tritons to maintain position sensitivity. The [.sup.3]He pressure and drift length will be optimized for efficient conversion of neutrons and localization Customizing software and documentation for a particular country. It includes the translation of menus and messages into the native spoken language as well as changes in the user interface to accommodate different alphabets and culture. See internationalization and l10n. of charge in the drift region. For increased efficiency and processing of high count rates, we expect to collect the charge in current mode operation. Since fast timing is not critical for this initial application, the drift length can be larger than the few millimeters in a typical MicroMegas detector. A half-voltage ring provides electric field shaping over the drift distance.
[FIGURE 1 OMITTED]
In the previous segmented ionization chamber, the collection plates and the high-voltage plates were repeated along the beam axis to divide the detector into regions. The plates were strategically located so that an appropriate electric field accelerated the charges to the correct collection plates. By using the [.sup.3]He neutron absorber Neutron absorbers are isotopes of certain elements that absorb free neutrons creating heavier isotopes of the same element. The most prolific neutron absorbers are elements that become stable by absorbing a neutron such as xenon-133 (Xe-133), which absorbs a neutron to become that follows the 1/v capture behavior, the distance the neutron travels in the detector before being captured increases with decreasing velocity. Each separate detection region collected neutrons of a different average velocity with the slowest ones detected in the first region and the faster ones detected in the following regions along the beam axis. A cross sectional diagram showing the four collection regions is given in Fig. 2.
Notice that the regions in the segmented ionization chamber increase in size further along the beam axis. This is necessary to maintain approximately equal neutron collection in each region with a single high-voltage and constant fill gas pressure. Note that the last two regions were summed to equal a third of the beam total as in the first two regions.
Similarly, we propose to construct a detector module from one set of high-voltage plates, wire mesh grid and array of wire strip electrodes as depicted in Fig. 1. Alternating modules will have alternating orientations of the wire strip arrays with the vertical orientation mounted on one side of the silica substrate and the horizontal orientation mounted on the other side, a module pair is naturally formed as two modules "back-to-back". Analysis over multiple modules provides 2-dimensional spatial information of the neutron beam. Each detector module will be designed to absorb approximately 5% of the neutron flux so that a series of 20 modules (or 10 module pairs) located along the beam axis absorbs the entire beam. As in the previous segmented ionization chamber, the high-voltage will be the same for each module and the fill gas pressures will be constant requiring varying drift distances to achieve equal neutron collection regions.
[FIGURE 2 OMITTED]
We are in the process of developing a 2 module prototype detector with 8 wire strips in each perpendicular orientation.
This position-sensitive neutron detector with energy separation will provide an easy to use and economical means of measuring the beam profile of an intense source to verify the neutron guide properties and study non-uniformities. This detector would serve as a beam intensity monitor located downstream of a transmission experiment, providing both spatial and energy information. A detector of this type would enable online, continuous monitoring of second order geometry-dependent beam characteristics that impose systematic limits on experiments that are sensitive to higher moments of the beam distribution . (See for example the article on the measurements of neutron decay correlation coefficients in these proceedings.) For a continuous reactor source where time-of-flight techniques for energy dependent neutron detection are unavailable, this detector segmentation scheme enables neutron detection as a function of both geometry and relatively large, though useful, energy bins where the energy resolution strongly depends upon the segmentation structure.
 Spallation Neutron Source http://www.sns.gov.
 High Flux Isotope Reactor http://www.ornl.gov/sci/rrd; G. L. Greene, Private communication (2003).
 S. Andriamonje, D. Cano-Ott, A. Delbart, J. Derre, S. Diez, I. Giomataris, E. M. Gonzales-Romero, F. Jeanneau, D. Karamanis, A. Lepretre, I. Papadopoulos, P. Pavlopoulos, and D. Villamarin, Experimental studies of a Micromegas neutron detector, Nucl. Instrum. Meth. A 481, 120 (2002).
 S. D. Penn, E. G. Adelberger, B. R. Heckel, D. M. Markoff, and H. E. Swanson, Development of a low-noise [.sup.3]He ionization chamber for measuring the energy spectrum of a cold neutron beam, Nucl. Instrum. Meth. A 457, 332 (2001).
 C. L. Britton, W. L. Bryan, A. L. Wintenberg, R. J. Warmack, T. E. McKnight, S. S. Frank, R. G. Cooper, N. J. Dudney, G. M. Veith, and A. C. Stephan, A detector for neutron imaging, IEEE (Institute of Electrical and Electronics Engineers, New York, www.ieee.org) A membership organization that includes engineers, scientists and students in electronics and allied fields. Transactions (2004).
 A. C. Stephan, R. G. Cooper, and L. F. Miller, Monte Carlo studies of a Micromegas neutron beam monitor, Nucl. Instrum. Meth. A 521, 441-453(2004).
 W. S. Wilburn et al., A new approach to measuring the neutron decay correlations with cold neutrons at LANSCE LANSCE Los Alamos Neutron Science Center , Fundamental Physics with Pulsed Neutron Beams, World Scientific, Singapore (2001) pp. 214; Private communication (2003).
About the authors: Diane M. Markoff is a research assistant professor in the Physics Department at the North Carolina State University History
Diane M. Markoff
North Carolina State University, Department of Physics, Raleigh, NC
Vince Cianciolo, Chuck L. Britton, and Ronald G. Cooper
Oak Ridge National Laboratory, Oak Ridge, TN
Geoff L. Greene
Oak Ridge National Laboratory, Oak Ridge, TN
University of Tennessee, Knoxville, TN
Accepted: August 11, 2004
Available online: http://www.nist.gov/jres