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論文

Effect of coaxial HPGe detector structure on $$gamma$$-ray beam measurements

Omer, M.; 静間 俊行*; 小泉 光生; 平 義隆*; Zen, H.*; 大垣 英明*; 羽島 良一*

Radiation Physics and Chemistry, 240, p.113467_1 - 113467_8, 2026/03

Coaxial high-purity germanium detectors are widely used in applications requiring high-resolution $$gamma$$-ray spectroscopy. However, the internal structure of these detectors, particularly the geometry of the inactive volumes inside the detector core, can significantly influence their performance in beam detection configurations. This study investigates the impact of detector structure on the spectral response to pencil-like $$gamma$$-ray beams, based on a comparison of $$gamma$$-ray spectra measured with two coaxial high-purity germanium detectors that have similar active volumes but distinct internal geometries. Experimental measurements were conducted at the UVSOR synchrotron facility using collimated laser Compton scattered $$gamma$$-ray beams with an energy of $$5.53^{+0.016}_{-0.580}$$ MeV. Monte Carlo simulations using the Geant4 toolkit were performed to refine the detector models and replicate experimental results. The results reveal that the front layer thickness and the presence of structural elements such as the cold finger strongly affect the spectral features, particularly the appearance of a coincidence sum peak of the annihilation radiation at 1.022 MeV. Off-axis irradiation significantly improves the detection efficiency and reduces undesired induced interactions within inactive volumes. Additionally, the observed pair production signatures are validated through the available theoretical cross section data, confirming the dominant role of internal structures in shaping the detector response under beam geometry. These findings are essential for optimizing detector configurations in precision $$gamma$$-ray beam experiments. This work is a contribution of the Japan Atomic Energy Agency (JAEA) to the International Atomic Energy Agency (IAEA) under the agreement of the coordinated research program (CRP), J02015 (Facilitation of Safe and Secure Trade Using Nuclear Detection Technology - Detection of RN and Other Contraband). A part of this work was conducted at the BL1U of UVSOR Synchrotron Facility, Institute for Molecular Science (IMS program 23IMS6602).

論文

Spatial polarization distribution measurements of gamma rays produced by inverse Compton scattering

Yang, Y.*; 平 義隆*; 静間 俊行*; Omer, M.

Proceedings of 16th International Particle Accelerator Conference (IPAC25) (Internet), p.194 - 196, 2025/11

Highly polarized MeV gamma-rays, produced by Laser Compton Scattered (LCS) of a polarized laser with an electron beam, offer a unique probe for basic and applied physics research. As the polarization characteristics of these gamma-rays vary with the position of the beam cross section, it is essential to understand the polarization properties when using polarized gamma-rays. However, detailed measurements of the two-dimensional spatial polarization distribution have not yet been conducted. In the UVSOR synchrotron facility, a polarimeter was developed to measure the spatial polarization distribution of linearly polarized gamma-rays. The polarimeter is based on asymmetry measurements of the Compton scattering cross section. In this conference, we will report on measurement results of the spatial polarization distribution of linearly and circularly polarized LCS gamma-rays. The polarization axis of the polarized gamma-rays was clearly measured to vary with scattering and azimuth angle. In the near future, we plan to use the developed polarimeter to also measure the spatial polarization distribution of gamma-rays generated by an axially symmetric polarized laser.

論文

Generation and measurement of gamma rays with axially symmetric polarization states via Compton scattering

平 義隆*; Yang, Y.*; 静間 俊行*; Omer, M.

Physical Review Research (Internet), 7(3), p.033130_1 - 033130_17, 2025/08

Highly polarized gamma rays with linear or circular polarization are essential light sources for nuclear and particle physics experiments, astronomical detector evaluations, and relativistic electron beam diagnostics. In this study, we demonstrate gamma-ray generation via Compton scattering with unique polarization states, termed axially symmetric polarization. To investigate this, we developed a polarimeter for Compton gamma-ray sources to measure their two-dimensional polarization distribution. We found two methods to generate gamma rays whose polarization axis follows the azimuthal direction. The first method exploits the inherent azimuthal polarization of gamma rays produced using a circularly polarized laser. In this configuration, the gamma rays along the central axis are circularly polarized, while the linear polarization components in the outer region of the beam cross section are aligned azimuthally. The second method utilizes azimuthal polarization that arises in the outer region of the beam due to the incoherent superposition of multiple linearly polarized gamma rays with varying polarization axes, generated by an axially symmetric polarized laser. Additionally, our calculations indicate the feasibility of generating gamma rays with polarization axes oriented along the radial direction. This radial polarization, observed near the beam axis, results from the incoherent superposition of second harmonic gamma rays produced through nonlinear interactions induced by an intense axially symmetric polarized laser.

論文

Circular polarization measurement for individual gamma rays in capture reactions with intense pulsed neutrons

遠藤 駿典; 安部 亮太*; 藤岡 宏之*; 猪野 隆*; 岩本 修; 岩本 信之; 河村 しほり*; 木村 敦; 北口 雅暁*; 小林 龍珠*; et al.

European Physical Journal A, 60(8), p.166_1 - 166_10, 2024/08

 被引用回数:3 パーセンタイル:67.20(Physics, Nuclear)

Measurements of $$gamma$$-ray circular polarization emitted from neutron capture reactions provide valuable information for nuclear physics studies. The spin and parity of excited states can be determined by measuring the circular polarization from polarized neutron capture reactions. Furthermore, the $$gamma$$-ray circular polarization in a neutron capture resonance is crucial for studying the enhancement effect of parity nonconservation in compound nuclei. The $$gamma$$-ray circular polarization can be measured using a polarimeter based on magnetic Compton scattering. A polarimeter was constructed, and its performance indicators were evaluated using a circularly polarized $$gamma$$-ray beam. Furthermore, as a demonstration, the $$gamma$$-ray circular polarization was measured in $$^{32}$$S(n,$$gamma$$)$$^{33}$$S reactions with polarized neutrons.

論文

Nondestructive determination of isotopic abundance using multi-energy nuclear resonance fluorescence driven by laser Compton scattering source

Omer, M.; 静間 俊行*; 羽島 良一*; 小泉 光生

Journal of Applied Physics, 135(18), p.184903_1 - 184903_10, 2024/05

 被引用回数:1 パーセンタイル:16.05(Physics, Applied)

We report on the findings of a quantitative nondestructive analysis of the natural isotopic abundances of hafnium and tungsten elements using nuclear resonance fluorescence. Commercial samples of hafnium and tungsten were irradiated to six quasi-monochromatic $$gamma$$-ray beams generated by laser Compton scattering in the energy range of 2.4-3.2 MeV. Multiple nuclei were simultaneously excited at each of the six $$gamma$$-ray beam energies. A high-purity germanium detector array detected deexcitations of the nuclei. In total, $$51$$ transitions were unprecedentedly employed to estimate the isotopic abundances of heavy elements nondestructively. The estimated abundances of three hafnium isotopes and three tungsten isotopes are consistent with standard known natural abundances within the experimental uncertainties. The deviation from the standard values ranges from 0.18% to 1.36%. This work is a contribution of the Japan Atomic Energy Agency (JAEA) to the International Atomic Energy Agency (IAEA) under the agreement of the coordinated research program (CRP), J02015 (Facilitation of Safe and Secure Trade Using Nuclear Detection Technology - Detection of RN and Other Contraband). This work was a part of a study of the nuclear resonance fluorescence aiming at nuclear security and safeguards applications, being supported by the subsidiary for "promotion of strengthening nuclear security or the like" of the Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan.

論文

Spin and parity assignments for low-lying states in the odd-mass nucleus $$^{181}$$Ta

静間 俊行*; Omer, M.; 羽島 良一*; 小泉 光生

Physical Review C, 109(5), p.054320_1 - 054320_8, 2024/05

 被引用回数:0 パーセンタイル:0.00(Physics, Nuclear)

Low-lying levels in the odd-mass nucleus $$^{181}$$Ta have been populated via nuclear resonance fluorescence using a quasi-monoenergetic, linearly polarized photon beam at the High Intensity $$gamma$$-ray Source (HI$$gamma$$S) facility at Duke University. The spin and parity of the levels were determined from the azimuthal intensity asymmetry of resonantly scattered $$gamma$$-rays with respect to the polarization plane of the incident photon beam. The electric and magnetic dipole strengths were obtained for excitation energies from 2.2 to 3.2 MeV. The results are discussed in terms of the nuclear scissors mode. This work is a contribution of the Japan Atomic Energy Agency (JAEA) to the International Atomic Energy Agency (IAEA) under the agreement of the coordinated research program (CRP), J02015 (Facilitation of Safe and Secure Trade Using Nuclear Detection Technology - Detection of RN and Other Contraband). This work was a part of a study of the nuclear resonance fluorescence aiming at nuclear security and safeguards applications, being supported by the subsidiary for "promotion of strengthening nuclear security or the like" of the Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan.

論文

Parity assignment for low-lying dipole states in $$^{58}$$Ni

静間 俊行*; Omer, M.; 早川 岳人*; 湊 太志*; 松葉 俊哉*; 宮本 修治*; 清水 則孝*; 宇都野 穣

Physical Review C, 109(1), p.014302_1 - 014302_7, 2024/01

 被引用回数:5 パーセンタイル:82.73(Physics, Nuclear)

Low-lying dipole states in the singly closed-shell nucleus $$^{58}$$Ni were studied via nuclear resonance fluorescence experiments using a quasi-monoenergetic, linearly polarized photon beam. The parity quantum numbers of the dipole states were determined by the intensity asymmetry of resonantly scattered $$gamma$$-rays with respect to the polarization plane of the incident photon beam. The electric and magnetic dipole (E1 and M1) strengths at excitation energies between 5.9 and 9.8 MeV were obtained based on dipole strengths taken from literature. The E1 and M1 strength distributions were compared with large-scale shell-model predictions in the $$fp$$-shell using the SDPFSDG-MU interaction.

論文

Cross section asymmetry of polarized $$gamma$$-ray elastic scattering

Omer, M.; 静間 俊行*; 小泉 光生; 羽島 良一*; 橋本 智*; 宮本 修治*

LASTI Annual Report, 24, p.20 - 22, 2023/12

Nondestructive elemental analysis is highly valued in many fields such as archeology, paleontology, space sciences, nuclear security, and nuclear nonproliferation. These fields usually impose estimating the elemental composition of bulk, large, and inhomogeneous samples nondestructively. Common elemental analysis techniques such as X-ray fluorescence (XRF) may fail in such situations due to self-absorption of low energy X-rays within thin layers of the sample. In the present study, we propose a novel nondestructive method that may be useful in distinguishing the elemental composition of a given sample based on the elastic scattering of linearly polarized and high-energy $$gamma$$-rays. Linear polarization of $$gamma$$-rays causes asymmetry of the elastic scattering cross sections with respect to the polarization plane of the incident $$gamma$$-rays. At specific $$gamma$$-ray energies and scattering angles, the asymmetry ratio, R, of the cross sections in two orthogonal planes is characteristic of each element. The measurement of asymmetry ratio of 1.62 MeV linearly polarized $$gamma$$-rays at NewSUBARU facility is presented. This work is a contribution of the JAEA to the International Atomic Energy Agency (IAEA) under the agreement of the coordinated research program (CRP), J02015 (Facilitation of Safe and Secure Trade Using Nuclear Detection Technology - Detection of RN and Other Contraband).

論文

Impact of the temperature on the non-destructive nuclide assay in the transmission NRF method

Omer, M.; 静間 俊行*; 小泉 光生; 平 義隆*; Zen, H.*; 大垣 英明*; 羽島 良一

UVSOR-50, P. 37, 2023/08

核共鳴蛍光(NRF)を用いた非破壊分析において、試料温度によるドップラー効果による影響を調べることを目的とした研究を開始した。今回は、波長1980nmのファイバーレーザーを加速エネルギー746MeVの電子ビームと衝突させて生成した最大エネルギー5.54MeVのレーザーコンプトンガンマ線を$$^{208}$$Pb標的に照射し、共鳴散乱ガンマ線を3台の高純度ゲルマニウム検出器を用いて測定した。その結果、レーザーコンプトンガンマ線最大エネルギーよりも高いエネルギーで、複数のガンマ線ピークが観測された。これらのガンマ線は、実験室内の制動放射線によって発生した中性子が測定装置の周囲の物質と反応した後に放出された中性子捕獲即発ガンマ線であると考えられる。そのため、バックグラウンドガンマ線の低減のため、ゲルマニウム検出器の周囲を厚さ10cmの鉛を用いて遮蔽した。その結果、即発ガンマ線のバックグラウンドは抑制され、$$^{208}$$Pbの共鳴散乱ガンマ線を観測することができた。

論文

Measurement of the spatial polarization distribution of circularly polarized gamma rays produced by inverse Compton scattering

平 義隆*; 遠藤 駿典; 河村 しほり*; 南部 太郎*; 奥泉 舞桜*; 静間 俊行*; Omer, M.; Zen, H.*; 岡野 泰彬*; 北口 雅暁*

Physical Review A, 107(6), p.063503_1 - 063503_10, 2023/06

 被引用回数:6 パーセンタイル:60.04(Optics)

偏光レーザーと電子による逆コンプトン散乱は偏光ガンマ線を生成する手法の一つであり、100%偏光のレーザーを用いることで100%の偏光ガンマ線を得ることができる。しかしながら、偏光具合はガンマ線の散乱角度に依存して変化する。本研究ではMeVのエネルギーのガンマ線の円偏光度を測定することが可能である磁化鉄を用いて、ガンマ線の円偏光度の空間分布を実験的に測定した。ガンマ線の磁化鉄の透過率の非対称性が確認され、中心軸付近において円偏光しているガンマ線が、散乱角度が大きくなると円偏光から直線偏光に変化することが確認された。

論文

Accurate estimation of spectral density of LCS gamma-ray source

Omer, M.; 静間 俊行*; 羽島 良一*; 小泉 光生

第43回日本核物質管理学会年次大会会議論文集(インターネット), 3 Pages, 2022/11

Gamma-rays originated from laser Compton scattering (LCS) are convenient photon sources for nondestructive interrogation of nuclear materials. LCS can be used with nuclear resonance fluorescence (NRF) and X-ray fluorescence (XRF), the two of which are considered photon-based active interrogation techniques. However, an accurate estimation of the incident LCS $$gamma$$-ray flux is crucial. The $$gamma$$-ray flux is customarily measured using high purity germanium (HPGe) detectors, usually calibrated using standard point-like radioactive $$gamma$$-ray sources. These standard sources are entirely different from LCS beams in terms of detection geometry. Therefore, the calibration process must be corrected to meet the LCS beam conditions. Here, we demonstrate how to implement the required corrections and provide experimental validation of these corrections.

論文

Calculating off-axis efficiency of coaxial HPGe detectors by Monte Carlo simulation

Omer, M.; 静間 俊行*; 羽島 良一*; 小泉 光生

Radiation Physics and Chemistry, 198, p.110241_1 - 110241_7, 2022/09

 被引用回数:4 パーセンタイル:53.41(Chemistry, Physical)

In beam geometries where a directed $$gamma$$-ray beam hits the surface of a coaxial high purity germanium detector (HPGe), the detector efficiency is sensitive to the position where $$gamma$$-rays initially hit the detector surface because the structure of the detector is nonuniform. This may cause inaccuracy of the detector efficiency when measured using standard sources that are point-like sources emitting $$gamma$$-rays isotropically. Obtaining a precise estimation of the full energy peak efficiency of the coaxial HPGe detector in the beam geometry for on-axis and off-axis measurements requires a Monte Carlo simulation. We performed a Monte Carlo simulation that calculates the detector efficiency in the beam geometry. The effects of the off-axis distance and $$gamma$$-ray beam size on the efficiency are quantitatively analyzed. We found that the intrinsic efficiency in the beam geometry is maximized when the beam hits the detector at specific off-axis distances. Our Monte Carlo calculations have been supported by a nuclear resonance fluorescence experiment using laser Compton scattering $$gamma$$-ray beam.

論文

Evaluation of analyzing power of gamma-ray polarimeter

遠藤 駿典; 静間 俊行*; Zen, H.*; 平 義隆*; Omer, M.; 河村 しほり*; 安部 亮太*; 奥平 琢也*; 北口 雅暁*; 清水 裕彦*

UVSOR-49, P. 38, 2022/08

To measure the circular polarization of gamma-rays, the gamma-ray polarimeter was developed. The analyzing power of the polarimeter was measured using circularly polarized gamma-rays in UVSOR BL1U. Magnetic hysteresis of the polarimeter was also observed. The analyzing power was obtained as 2.12$$pm$$0.04%.

論文

Low-lying electric and magnetic dipole strengths in $$^{207}$$Pb

静間 俊行*; 湊 太志; Omer, M.*; 早川 岳人*; 大垣 英明*; 宮本 修治*

Physical Review C, 103(2), p.024309_1 - 024309_8, 2021/02

AA2020-0675.pdf:0.29MB

 被引用回数:5 パーセンタイル:47.19(Physics, Nuclear)

$$^{207}$$Pbの低エネルギー双極子強度を準モノクロ=線形偏極フォトンビームの光核散乱を使って調べ、6.8MeVまでの励起エネルギーにおける電磁双極子($$E1$$)および磁気双極子強度($$M1$$)を導出した。今回の($$vec{gamma}$$,$$gamma'$$)反応の結果は、過去に行われた($$gamma$$,$$n$$)反応のデータと合わせて、中性子閾値近傍のエネルギーにおける$$E1$$$$M1$$の光吸収反応断面積を求めるために使った。得られた測定結果は、乱雑位相近似法+粒子振動カップリング法による理論計算の結果と比較し、核構造の観点から議論を行う。

論文

Compton scattering of quasi-monochromatic $$gamma$$-ray beam

Omer, M.; 静間 俊行*; 羽島 良一*

Nuclear Instruments and Methods in Physics Research A, 951, p.162998_1 - 162998_6, 2020/01

 被引用回数:3 パーセンタイル:27.13(Instruments & Instrumentation)

Compton scattering of a single-energy $$gamma$$-ray results in a one-to-one relationship between the incident and scattered photon energies. This relationship is altered when the incident beam has a definite energy distribution because of the broadening occurring in the energy distribution upon Compton scattering. This broadening causes a change in the spectral density of the Compton-scattered spectra. To restore the spectral density, the energy distribution of the scattered radiation must be manifested as a function of the scattering kinematics. Here, we propose a simple analytic way to calculate the energy spread of the scattered photons in terms of the geometry of the scattering process and the energy spread of the incident photon beam. The predictions of the model agree with measurements of Compton scattering of quasi-monochromatic $$gamma$$-ray beams, carried out at the High Intensity $$gamma$$-ray Source (HI$$gamma$$S) facility, Duke University. As a benchmark of our method, we measured the intensity profile of energy-distributed $$gamma$$-ray beams by direct measurements as well as by Compton scattering. We found that only when the spectral density of the scattered radiation is restored, the measured intensity profile agrees with the actual profile of the incident beam. The proposed method can continuously measure the flux of an energy-distributed $$gamma$$-ray beams in the real time and on a bin-by-bin basis. Such online monitoring of $$gamma$$-ray beams is indispensable for in-beam measurements and applications. This work was supported by the subsidiary for promotion of strengthening nuclear security or the like of the Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan.

論文

Validating polarization effects in $$gamma$$-rays elastic scattering by Monte Carlo simulation

Omer, M.; 羽島 良一*

New Journal of Physics (Internet), 21(11), p.113006_1 - 113006_10, 2019/11

AA2019-0407.pdf:0.73MB

 被引用回数:6 パーセンタイル:40.85(Physics, Multidisciplinary)

Nuclear resonance fluorescence (NRF) is a promising technique for nondestructive assay (NDA) of nuclear materials. Its strength is improved when polarized $$gamma$$-ray beams are used as probes because the polarized $$gamma$$-rays provide an asymmetry in the intensity of the scattered photons. Nonetheless, NRF interaction takes place with other interactions such as elastic scattering of $$gamma$$-rays. These interactions are unavoidable background which may limit the sensitivity of the NRF technique. Therefore, estimating polarization effects of elastic scattering is a significant factor in assessing the NRF method. Here, we implement a new Monte Carlo simulation to account for polarization effects of the elastic scattering. The simulation is based on explicit expressions driven in the Stokes parameters formalism. The scattering amplitudes of Rayleigh, nuclear Thomson, and Delbr${"u}$ck scattering processes have been superimposed into a two-orthogonal set of complex amplitudes. This set is then exploited to construct the core of the simulation in a way such that the simulation could handle arbitrary polarization states of the incoming beam and correspondingly generate polarization states for the outgoing beam. This work was supported by the subsidiary for promotion of strengthening nuclear security or the like of the Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan.

論文

Testing enrichment meter based on nuclear resonance fluorescence

Omer, M.; 静間 俊行*; 羽島 良一*; 小泉 光生

日本核物質管理学会第40回年次大会プロシーディングス集, p.59 - 62, 2019/11

Nuclear resonance fluorescence (NRF) is a phenomenon that a nuclide-specific $$gamma$$-ray is resonantly absorbed and re-emitted. This method is considered useful for the nondestructive detection of nuclear materials. In order to demonstrate how accurate the NRF method is able to measure the isotopic abundance, we performed NRF experiments on natural tungsten as a surrogate of nuclear materials at the High Intensity $$gamma$$-ray Source (HI$$gamma$$S) facility, Duke University. Our results show that the relative deviations between the reference and measured abundances are less than $$pm$$ 4%. This work was supported by the subsidiary for promotion of strengthening nuclear security or the like of the Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan.

論文

Spin and parity determination of the 3.004-MeV level in $$^{27}$$Al; Its low-lying multiplet structure

静間 俊行*; Omer, M.; 羽島 良一*; 清水 則孝*; 宇都野 穣

Physical Review C, 100(1), p.014307_1 - 014307_6, 2019/07

 被引用回数:8 パーセンタイル:54.43(Physics, Nuclear)

Nuclear resonance fluorescence (NRF) is a promising technique for the nondestructive assay (NDA) of nuclear materials. One of the features of the NRF is the angular distribution of the emitted photons in response to a linearly polarized incident beam. Here we irradiate the calibration standard of $$^{27}$$Al to linearly polarized beam. The spin and parity of the 3.004-MeV level in $$^{27}$$Al have been determined by measuring the angular correlation function of radiation emitted from levels populated by resonant absorption of polarized photons. The nuclear resonance fluorescence experiments were carried out at the High Intensity $$gamma$$-ray Source (HI$$gamma$$S) facility at Duke University using quasi-monoenergetic linearly polarized photon beams. The spin and parity of levels in $$^{27}$$Al were deduced from a comparison of the measured angular distribution ratios and azimuthal intensity asymmetries with theoretical predictions. The observed resonance properties were compared with shell model calculations using the universal sd interaction. The Monte Carlo shell model calculations were also performed to investigate low-energy structure of $$^{27}$$Al. This work was supported by the subsidiary for promotion of strengthening nuclear security or the like of the Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan.

報告書

Geant4 physics process for elastic scattering of $$gamma$$-rays

Omer, M.; 羽島 良一*

JAEA-Data/Code 2018-007, 32 Pages, 2018/06

JAEA-Data-Code-2018-007.pdf:2.64MB
JAEA-Data-Code-2018-007-appendix(CD-ROM).zip:22.71MB

原子核蛍光共鳴散乱(NRF)は、核物質の非破壊検査(NDA)において有用な技術である。NRFは同位体に固有のエネルギーをもったガンマ線と物質の相互作用であることから、同位体を識別したNDAを実現できる。しかしながら、NRFと競合する他の光核相互作用が存在し、そのため、NRFによるNDAの測定性能が制限される可能性がある。競合する相互作用のうち原子核によるガンマ線の弾性散乱(デルブリュック散乱)は、これまでのモンテカルロコードでは考慮されていなかった。日本原子力研究開発機構では、平成27年度からNRFに基づくNDAシステムの開発プログラムを開始し、その一環としてガンマ線の弾性散乱がNRF測定に及ぼす影響を評価するために、Geant4にガンマ線の弾性散乱を追加するためのコードを新規に開発した。今回刊行するJAEA-データ/コードレポートでは、シミュレーションコードの詳細な説明と、コード入力に用いたガンマ線弾性散乱断面積、および、コードの検証と妥当性確認に用いた計算結果を示す。このレポートを公開することで、当該コードの信頼性向上に必要なユーザーからのフィードバックの機会が得られる。本研究は文部科学省の核セキュリティ強化等推進事業費補助金の支援を受けた。

論文

Including Delbr$"u$ck scattering in GEANT4

Omer, M.; 羽島 良一*

Nuclear Instruments and Methods in Physics Research B, 405, p.43 - 49, 2017/08

 被引用回数:9 パーセンタイル:58.41(Instruments & Instrumentation)

原子核あるいは原子による$$gamma$$線の弾性散乱は、$$gamma$$線と物質の相互作用に関連付けられ、レイリー散乱、核トムソン散乱及びデルブリュック散乱がある。$$gamma$$線の弾性散乱を模擬するモンテカルロシミュレーションコードのほとんどは、現状では弾性散乱の全体像をカバーしていなく、レイリー散乱の寄与のみを取り扱い、核トムソン散乱及びデルブリュック散乱は無視されている。われわれは弾性散乱を模擬(シミュレート)するために、最も一般的なオープンソースのGeant4に、レイリー散乱に加えて、核トムソン散乱及びデルブリュック散乱を取込んだコードを開発した。この際のシミュレーションでは、これまでのフォームファクタ近似に基づくデータに代り、二次散乱行列に基づく微分散乱断面積を使っている。また、これらの3つの散乱プロセスの重ね合わせは、散乱振幅の複素数表示を考慮して慎重に行わった。このシミュレーションは、$$gamma$$線エネルギー範囲0.01$$leq$$E$$leq$$3MeVと1$$leq$$Z$$leq$$99の原子番号を持つすべての元素をカバーしている。さらに、われわれは、以前の実験で測定された微分断面積とシミュレーションから得られる微分断面積とを比較することによって、シミュレーションを検証した。この検証では、シミュレーションの結果は、実験の測定値と良い一致を示している。実験とシミュレーションとの違いは、$$gamma$$線エネルギーが2.754MeVで、ウランで21%、鉛で24%、タンタルで3%、及びセリウムで8%であった。高Z.(ウランや鉛)における比較的大きな差は、デルブリュック散乱振幅に対するクーロン補正により説明できる。

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