共查询到19条相似文献,搜索用时 140 毫秒
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采用空间综合辐照设备对Kapton/Al薄膜进行了质子辐照地面模拟试验,选取质子能量90 keV,辐照通量5.0×1011 cm12·s-1。通过辐照前后光谱反射系数的变化考察了实验样品的光学性能退化特征。借助于反射光谱和紫外-可见吸收光谱和傅里叶转换红外光谱分析技术分析了辐照后Kapton/Al光学性能的退化机理。研究结果表明:辐照过程中样品表面发生了复杂的化学反应,随着辐照剂量的增加光能隙逐渐减小,Kapton吸收曲线的末端边缘发生红移并且在可见光区吸收强度增加。 相似文献
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为了检验应用在极紫外(EUV)波段空间太阳望远镜上Al滤光片在空间辐射环境下透过率的变化情况,我们模拟部分空间太阳望远镜运行轨道的辐射环境,应用Monte Carlo(M-C)方法对Al材料进行低能量的质子和α粒子辐照损伤模拟,计算给出了质子和α粒子辐照对Al材料产生的缺陷、电离以及声子等辐照效应,最后对结果进行了比较和分析,从而预测质子和α粒子辐照对Al滤光片性能和使用寿命的影响. 相似文献
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用正电子淹没寿命谱方法(PALS)研究了质子辐照对空间级硅橡胶KH-L-Y微观结构的影响。试验结果表明,PALS谱所揭示的最长寿命成分的t3, I3及自由体积分数Vf随辐照剂量的增加开始明显下降;而当辐照剂量大于1015cm-2后,随剂量的增加平缓上升。辐照剂量小于1015cm-2时,质子辐照使硅橡胶自由体积减小,分子链间堆砌紧密;辐照剂量大于1015cm-2时,质子辐照使硅橡胶自由体积增大。交联密度及DMA测试结果同样表明,质子辐照在剂量较小时硅橡胶的交联密度及玻璃化转变温度增加,辐照以交联效应为主;而剂量较大时辐照降解占优势。 相似文献
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分析了连续激光辐照ZnSe/MgF2/K9滤光片引起透射特性的变化。在室温条件下,用波长0.632 8μm激光作为探测光束,测量了1.06μm连续激光辐照ZnSe/MgF2/K9滤光片温升引起薄膜折射率的改变,导致探测光束通过干涉滤光片后透过率的热致非线性变化。在光斑直径0.75mm条件下,测量了不同功率激光辐照ZnSe/MgF2/K9滤光片引起温升随时间的变化。在激光功率30W,辐照时间2.52s条件下,实验观测到ZnSe/MgF2/K9滤光片薄膜破坏温度约为90℃,辐照时间10s时干涉滤光片形成的薄膜龟裂形貌。 相似文献
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对用能量为7.5MeV和20MeV,注量为1011~1013cm-2的质子辐照后的砷化镓材料制作的光电导探测器的光电流和暗电流进行了测试,并由此推得电导率的变化。结果表明,经过能量为7.5MeV的质子改性后的砷化镓探测器相对于未改性的附加光电导率Δσ减少,而且随着辐照注量的增加而越小,而对于先用能量为20MeV质子辐照后再用能量为7.5MeV的质子辐照的砷化镓材料制作的探测器,其附加光电导率Δσ的减少则更为明显。对上述现象进行了分析,并根据其相应关系预测了该种探测器的响应时间、灵敏度、拖尾现象及受X射线激发的输出脉冲的后延的变化情况。 相似文献
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研究了用HZ-B串列加速器的18MeV质子辐照对TiNi形状记忆合金R相变的影响,辐照在奥氏体母相状态下进行。示差扫描量热法(DSC)表明,辐照后R相变开始温度TsR和逆马氏体相变结束温度TfA随辐照注量的增加而降低。当注量为1.53×1014/cm2时,TsR和TfA分别下降6K和13K,辐照未引起R相变结束温度TsR和逆马氏体相变开始温度TfA的变化。表明辐照后母相(奥氏体相)稳定。透射电镜(TEM)分析表明辐照后没有引起合金可观察的微观组织变化。辐照对R相变开始温度TsR和逆马氏体相变结束温度Af的影响可能是由于质子辐照后产生了孤立的缺陷团,形成了局部应力场,引起晶格有序度的下降所造成的。 相似文献
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实验研究了注量在1.0×1011—1.0×1016p/cm2范围依次变化时110keV质子辐照引起的温控涂层热光性能的变化,并使用XPS谱仪分析了辐照样品化学态的变化. 实验结果表明,质子注量不高于1.0×1014p/cm2时,同种材料的温控涂层样品的相对光反射率变化很小,同时同种材料样品的表面化学结构如化学位移和元素的比例变化很小.当注量高于1.0×1014p/cm2时, 样品的相对光反射率变化明显,样品表面的原子化学结构变化大, 化学位移明显增加, 元素比例变化显著,所有样品表面的C元素比例明显增大而O元素比例明显减小.一定注量的低能质子辐照能够使某些低太阳吸收率αs的温控涂层的太阳吸收率变得更低, 具有改善热光性能的效果.质子辐照之后温控涂层样品表面化学结构的变化与样品的物理性能的变化存在直接的关联. 相似文献
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研制出CVD金刚石薄膜探测器,在国家串列加速器和60Co稳态辐射源上分别完成了该探测器对9 MeV质子束流和1.25 MeV γ射线的辐照性能研究。结果表明:该探测器在9 MeV质子照射累积强度达到1013 cm-2时,探测器信号电荷收集效率减小量低于3.5%,辐照前后探测器暗电流没有明显变化。计算得到9 MeV质子对该探测器的损伤系数为1.3×10-16 μm-1·cm2。由于γ射线与金刚石作用产生的电子起到了填补缺陷的作用,探测器信号电荷收集效率随γ射线照射剂量的增加略有增加,在γ射线累积照射量达到10.32 C/kg时,其增幅小于0.7%。说明金刚石薄膜探测器具有较高耐辐照强度,适用于高强度辐射测量领域。 相似文献
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研究了AlGaN/GaN 高电子迁移率晶体管(HEMT)的质子辐照效应. 在3 MeV质子辐照下, 当辐照剂量达到1× 1015 protons/cm2时, 漏极饱和电流下降了20%, 最大跨导降低了5%. 随着剂量增加, 阈值电压向正向漂移, 栅泄露电流增加. 在相同辐照剂量下, 1.8 MeV质子辐照要比3 MeV质子辐照退化严重. 从SRIM软件仿真中得到不同能量质子在AlGaN/GaN异质结中的辐射损伤区, 以及在一定深度形成的空位密度. 结合变频C-V测试结果进行分析, 表明了质子辐照引入空位缺陷可能是AlGaN/GaN HEMT器件电学特性退化的主要原因. 相似文献
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Mohamed Bencheikh Abdelmajid Maghnouj Jaouad Tajmouati 《Moscow University Physics Bulletin》2017,72(3):263-270
Determination and understanding the photon beam attenuation by the photon beam modifier and the radiation beam softening for clinical use is more important part of material study for the beam modifier enhancements and the linac improvements. A Monte Carlo model was used to simulate 6 MeV photon beams from a Varian Clinac 2100 accelerator with the flattening filter and the later was replaced by the aluminum slab with variable thickness. The Monte Carlo geometry was validated by a gamma index acceptance rate of 99% in PDD and 98% in dose profiles, the gamma criteria was 3% for dose difference and 3 mm for distance to agreement. The purpose was to investigate aluminum material attenuation and beam softening coefficients as a function of the inserted aluminum slab thickness and of off-axis distance. The attenuation and beam softening coefficients were not identical for the same off-axis distance and they varied as a function of aluminum slab thickness. The results of our study were shown that the beam softening coefficients were varied with thickness beam modifier material used for beam softening and the off-axis distance inside the irradiation field. Thereafter, the softening coefficient a 1 have a maximum of 2.5 × 10–1 cm–1 for the aluminum slab thickness of 1 mm, 1.4 × 10–1 cm–1 for the aluminum slab thickness of 1.5 mm and 4.47 × 10–2 cm–1 for the aluminum slab thickness of 2 mm. The maximum of the second softening coefficient a 2 was 1.02 × 10–2 cm–2 for the aluminum slab thickness of 1 mm, was 1.92 × 10–2 cm–2 for the aluminum slab thickness of 1.5 mm and was 1.93 × 10–2 cm–2 for the aluminum slab thickness of 2 mm. Our study can be a basic investigation of photon beam softening material that will be used in the future linac configuration and also in the photon beam modifiers. 相似文献
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为了检验应用在极紫外波段空间太阳望远镜上Mo/Si多层膜反射镜在空间辐射环境下反射率的变化情况, 模拟了部分空间太阳望远镜运行轨道的辐射环境, 利用不同能量和剂量的质子对Mo/Si多层膜反射镜进行辐照实验.辐照前后反射率测量结果显示,由于带电粒子的辐照损伤,质子辐照会使Mo/Si多层膜反射镜的反射率降低,且质子能量越低、剂量越大,对多层膜的反射率影响越明显. 当质子能量E=160keV,剂量=6×1011/mm2时,反射率降低4.1%;能量E=100keV,剂量=6×1011/mm2时, 反射率降低5.7%;能量E=50keV,剂量=8×1012/mm2时,反射率降低10.4%. 用原子力显微镜测量辐照后Mo/Si多层膜反射镜的表面粗糙度比辐照前明显增加,致使散射光线能量逐渐增大并最终导致反射率的降低.
关键词:
质子辐照
Mo/Si多层膜反射镜
辐照损伤 相似文献
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B. K. Kardashev O. A. Plaksin V. A. Stepanov V. M. Chernov 《Physics of the Solid State》2004,46(8):1449-1455
The behavior of Young’s modulus E and the decrement of ultrasonic vibrations δ in a V-4Ti-4Cr alloy is studied during proton (8-MeV protons, dose rate 104 Gy/s) or IR laser (YAG: Nd3+ laser, wavelength 1.06 μm, intensity up to 102 W/cm2) irradiation. Measurements are performed using the method of a composite piezoelectric oscillator (longitudinal 100-kHz resonance
vibrations). The sizes of the irradiated surface regions of a sample in the proton and laser experiments are the same in order
to provide the same thermal conditions in the sample-quartz transducer system. The amplitude, time, and temperature dependences
of E and δ are measured before and after preliminary plastic deformation, as well as before, during, and after irradiation of
a sample. The process of postdeformation aging (the kinetics of recovery of internal friction after deformation) during proton
irradiation is shown to differ substantially from that during laser irradiation. The specific features detected can be explained
by the more intense evolution of the defect structure during proton irradiation. Analysis shows that radiation annealing is
related to the ionizing component of proton irradiation, which excites the electronic subsystem of the metallic alloy and,
thus, creates hot electrons and plasmons. The electron excitations relax at lattice defects (dislocations) and increase the
dislocation mobility; this results in a relatively rapid decrease in the dislocation density and in a more significant (as
compared to the laser irradiation) decrease in the level of internal stresses in the material.
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Translated from Fizika Tverdogo Tela, Vol. 46, No. 8, 2004, pp. 1409–1415.
Original Russian Text Copyright ? 2004 by Kardashev, Plaksin, Stepanov, Chernov. 相似文献
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Sung Wook HyunKang Ryong Choi Sam Jin KimChul Sung Kim 《Journal of magnetism and magnetic materials》2012,324(4):445-448
We have studied the magnetic properties of 57Fe-doped TiO2 compounds irradiated by proton with 0, 5 and 10 pC/μm2. We have observed the enhancement of the magnetic moment, measured by superconducting quantum interference device magnetometer, with increasing proton irradiation ranging from 0 to 10 pC/μm2. Mössbauer spectra of proton irradiated Ti0.9957Fe0.01O2 samples were taken at room temperature. Two sites of the wing (sextet) and the central (doublet) are shown in the spectra, which suggest the magnetically ordered phase and the paramagnetic phase, respectively. With increasing proton irradiation, the part of Fe3+ ions was converted to Fe2+ ions by compensation charge. This clearly suggests that the enhancement of magnetic moment after proton irradiation is contributed to the moment by the spin-orbit coupling of Fe2+ ions. 相似文献
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Thomaz R. S. de Souza C. T. Papaléo R. M. 《Applied Physics A: Materials Science & Processing》2011,104(4):1223-1227
We report on the effect of light-ion irradiation on the size distribution of etched tracks produced by medium energy heavy-ions
in polycarbonate. Makrofol KG polycarbonate foils were treated with 2 MeV H+ ions at different fluences φ either before or after a short irradiation with 18 MeV Au7+. The heavy ion irradiation was used to produce the latent tracks in the foils and the proton beam acted as a perturbation
to the matrix. The proton irradiation causes initially a decrease in the mean etched pore size, as compared to samples only
bombarded by Au ions, reaching a minimum at H+ fluences around 2–5×1013 cm−2, while at higher φ the pore size starts to grow again. This effect is attributed to the action of two competitive processes that dominate in
different fluence regimes. The decrease in the pore radii at low fluences is attributed to an increase in crystallinity induced
by the proton beam. As the total dose builds up, this effect is surpassed by chain scission and amorphization that grow at
a lower rate and cause the pore radii to increase again. 相似文献
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紫外光辐照聚乙烯醇的1H NMR研究 总被引:1,自引:1,他引:0
用1H NMR谱,自旋-晶格弛豫时间(T1)和X-射线衍射研究了聚乙烯醇(PVA)在紫外光(UV)辐照后-OH基团与溶剂中残余水质子间氢键的生成与质子交换. 结果表明随着UV光辐照时间的增长,水峰与-OH质子峰逐渐相互靠近,同时水峰逐渐变宽,向低场方向移动,这与-OH基团与溶剂DMSO中残余水的质子之间既有氢键生成又有质子交换有关. 对辐照前后的PVA的DMSO溶液进行变温氢谱的研究,表明随着温度的升高,二者的-OH基团共振峰均逐渐变弱,溶剂残余水峰与-OH基团峰逐渐移向高场. PVA辐照前后随着浓度增大,羟基质子峰“变钝”. 辐照后的PVA的X-射线衍射表明聚集态结构中部分分子间氢键受到了破坏. 相似文献