排序方式: 共有148条查询结果,搜索用时 15 毫秒
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超导量子干涉器(SQUID)能探测到微弱的心脏磁场信号. 通过对所得的心磁信号进行分析,可为许多心脏疾病的诊断提供依据. 利用心磁信号,采用极小范数最小二乘法(MNLS)对心脏的电流偶极子阵列进行重建,从而实现了对心脏内部等效电流源的成像. 在使用MNLS进行电流偶极子阵列反演重建的过程中,反演所需的心磁信号,分别由单电流偶极子和电流多极子作为激发源模拟得到,以及由SQUID实际测量得到. 同时,对不同心磁信号反演得到的电流偶极子的分布规律进行了分析. 此外,还给模拟的人体外心磁信号施加了均匀噪声和随机噪声,研究不同信噪比的均匀噪声和随机噪声对电流偶极子阵列重建的影响. 相似文献
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表面抛光可能给K9基片带来额外的杂质和吸收,分离K9基片的表面吸收率与体吸收率有助于改进基片的加工质量和抛光工艺,对抗损伤能力研究具有重要意义。分析了激光量热法测量弱吸收的原理,采用符合ISO 11551要求的激光量热计测量K9基片的弱吸收。对相同工艺抛光的不同厚度K9基片进行了弱吸收表征,实验发现K9基片的弱吸收随着厚度增加近似线性增大。推导了表面吸收率和体吸收率的计算式,实验得出本样品的表面吸收率为1.2110-5,体吸收率远大于表面吸收率,体吸收系数为1.7210-3/cm。实验结果显示所用K9样品的吸收主要来自于材料本身,改善抛光工艺对降低其吸收率作用不大。 相似文献
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The principle and experimental results of the open microwave resonant cavity measurement system were introduced. The models were steel ball models and the ball models coated with copper. The diameter of the models was 10mm . The models were launched in ballistic range. The model velocity was 5.44 km .s-1. The wake electron density of the models was obtained. The experimental results presents that the response time of the open microwave resonant cavity measurement system was quicker than 1ms. The results showed the wake electron density ranged from 109cm -3 to 1011cm -3 could be achieved. 相似文献
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采用电子束蒸发的方式,制备了有氧化硅内保护层和没有氧化硅内保护层的1 064 nm高透过、532 nm高反射的HfO2/SiO2双色膜,测量了它们的光学性能以及在基频和倍频激光辐照下的抗损伤性能。结果表明:氧化硅内保护层提高了双色膜在基频光辐照下的损伤阈值,对双色膜在倍频光辐照下的损伤阈值无明显影响。通过观察薄膜的损伤形貌,分析破斑的深度信息结合驻波场分布,对两类双色膜在基频光和倍频光下的损伤机制做了初步探讨。分析表明:氧化硅内保护层提高了膜基界面的抗损伤性能,从而提高了双色膜在基频光下的损伤阈值。 相似文献
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为降低高功率激光系统中连续相位板(CPP)后续元件的强激光损伤风险,综合考虑入射光强调制、干涉及衍射作用等多种影响因素,建立了CPP近场计算分析模型,模拟和分析了这些因素对CPP后的近场均匀性的影响。理论分析结果表明:CPP后的光束近场均匀性主要受入射光调制、CPP表面剩余反射率和衍射传输距离的影响;当入射光束质量较差时,CPP后的近场均匀性主要由入射光束质量决定,CPP剩余反射率和衍射传输距离对近场均匀性影响相对较小;但当光束质量比较理想时,干涉和衍射作用会破坏CPP的近场均匀性,衍射传输距离影响尤为突出。 相似文献
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Fabrication and properties of high performance YBa_2Cu_3O_(7-δ) radio frequency SQUIDs with step-edge Josephson junctions 下载免费PDF全文
We describe the fabrication of high performance YBa2Cu3O7-δ(YBCO) radio frequency(RF) superconducting quantum interference devices(SQUIDs), which were prepared on 5 mm×5 mm LaAlO3(LAO) substrates by employing stepedge junctions(SEJs) and in flip-chip configuration with 12 mm×12 mm resonators. The step in the substrate was produced by Ar ion etching with step angles ranging from 47°to 61°, which is steep enough to ensure the formation of grain boundaries(GBs) at the step edges. The YBCO film was deposited using the pulsed laser deposition(PLD) technique with a film thickness half of the height of the substrate step. The inductance of the SQUID washer was designed to be about 157 pH.Under these circumstances, high performance YBCO RF SQUIDs were successfully fabricated with a typical flux-voltage transfer ratio of 83 mV/Φ0, a white flux noise of 29 μΦ0/(Hz)1/2, and the magnetic field sensitivity as high as 80 fT/(Hz)1/2.These devices have been applied in magnetocardiography and geological surveys. 相似文献
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Simulation of dielectric resonator for a high-To radio frequency superconducting quantum interference device 下载免费PDF全文
Nowadays, the high-critical-temperature radio frequency superconducting quantum interference device (high-Tc rf SQUID) is usually coupled to a dielectric resonator that is a standard 10× 10×1 mm^3 SrTiO3 (STO) substrate with a YBa2Cu3O7-δ (YBCO) thin-film flux focuser deposited on it. Recently, we have simulated a dielectric resonator for the high-Tc rf SQUID by using the ANSOFT High Frequency Structure Simulator (ANSOFT HFSS). We simulate the resonant frequency and the quality factor of our dielectric resonator when it is unloaded or matches a 50-Ω impedance. The simulation results are quite close to the practical measurements. Our study shows that ANSOFT HFSS is quite suitable for simulating the dielectric resonator used for the high-Tc rf SQUID. Therefore, we think the ANSOFT HFSS can be very helpful for investigating the characteristics of dielectric resonators for high-Tc rf SQUIDs. 相似文献
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