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超导量子干扰装置磁强仪用作肠系膜血管缺血的非损伤性诊断
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作者 蔡端 《国际外科学杂志》 北大核心 1996年第2期119-120,共2页
动脉缺血时小肠基础电节律(BER)减少,超导量子干扰装置(SQUID)磁强仪能测出小肠平滑肌电流所生成的磁场,故可用于非接触小肠方式以检出肠缺血时的BER降低.应用高分辨力的SQUID磁强仪,由位于4.4mm^2的4个超导铌测知线圈组成,置于充满液... 动脉缺血时小肠基础电节律(BER)减少,超导量子干扰装置(SQUID)磁强仪能测出小肠平滑肌电流所生成的磁场,故可用于非接触小肠方式以检出肠缺血时的BER降低.应用高分辨力的SQUID磁强仪,由位于4.4mm^2的4个超导铌测知线圈组成,置于充满液氦的真空间隙中,这一仪器能测出地球磁场百万分之一的强度.实验动物置于磁场防护室内以减少地球磁场的干扰.取新西兰兔进行两种实验,分别测定部分或完全性小肠缺血时的BER改变,前者阻断回肠的节段动脉,后者则阻断肠系膜上动脉血供.每一种实验用兔10只.结果 (一)实验一 阻断节段动脉的部分肠缺血模型中,经腹SQUID磁强仪测得的记录与电极放置在回肠浆膜上者相关.在基线测定,两种方法测得的BER比较恒定(14.9±0.8cpm),阻断小肠节段动.脉后15分钟,BER自基线值降至12.4±0.6cpm(P=0.03). 展开更多
关键词 超导量子干扰装置 肠系膜血管缺血 非损伤性 SQUID 节段动脉 地球磁场 磁强 小肠缺血 基础电节律 小肠平滑肌
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Scheme for Implementing Deutsch-Jozsa Algorithm Using Superconducting Quantum Interference Devices
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作者 MA Chi ZHANG Shi-Jun YE Liu 《Communications in Theoretical Physics》 SCIE CAS CSCD 2008年第2期373-376,共4页
We propose a physical scheme for implementing the Deutsch-Jozsa algorithm with superconducting quantum interference devices (SQUIDs) in cavity-QED. The scheme is based on SQUID coupled to a single-mode microwave cav... We propose a physical scheme for implementing the Deutsch-Jozsa algorithm with superconducting quantum interference devices (SQUIDs) in cavity-QED. The scheme is based on SQUID coupled to a single-mode microwave cavity field or classical microwave pluses. The scheme is very simple and may be realizable experimentally. 展开更多
关键词 cavity QED Deutsch Jozsa algorithm quantum information
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Generation of W States with Many Superconducting-Quantum-Interference-Devices in Cavity QED
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作者 詹志明 《Communications in Theoretical Physics》 SCIE CAS CSCD 2010年第8期355-358,共4页
We propose a scheme to generate the W states with many SQUIDs (superconducting-quantum-interferencedevices)in cavity QED via Raman transition.In this scheme,the transfer of quantum information between the SQUIDsand ca... We propose a scheme to generate the W states with many SQUIDs (superconducting-quantum-interferencedevices)in cavity QED via Raman transition.In this scheme,the transfer of quantum information between the SQUIDsand cavity is not required.And the cavity field is only virtually excited,thus the cavity decay is suppressed during theW states generation.The SQUIDs are always populated in the two ground states.Therefore,the scheme is insensitiveto the spontaneous emission of the excited level of the SQUID and cavity decay. 展开更多
关键词 W states SUPERCONDUCTING Raman transition
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