tailieunhanh - Applications of High Tc Superconductivity Part 2

Tham khảo tài liệu 'applications of high tc superconductivity part 2', kỹ thuật - công nghệ, cơ khí - chế tạo máy phục vụ nhu cầu học tập, nghiên cứu và làm việc hiệu quả | Overview of Possible Applications of High Tc Superconductors 9 possibility of applications of superconductor devices in digital signal processing is available in a review article Van Duzer Lee 1990 . On the other hand the use of other types of superconducting circuits is also possible in analog signal processing and in analog-to-digital converters. A discussion about the possibility of applications of superconductor devices in wideband analog signal processing is available in review articles Clarke 1988 Withers 1990 . Other reviews are available in a book Van Duzer Turner 1998 . Three-terminal devices using HTS In Section we have described the possibility of applications of two-terminal superconducting devices based on SNS junctions for a number of applications o HTS in superconducting electronics. However it is also feasible to use three-terminal superconducting devices in applications of HTS in superconducting electronics. The most important three-terminal superconducting devices are superconducting transistors. A study about the characteristics and the performance of HTS transistors is available in a review article Mannhart 1996 . Digital computer quantum computer and flux qubit An exciting application of superconducting electronics should be provided by the possible applications of HTS in digital computers. The most important components of a digital computer are memory units and arithmetic units. The metallic interconnections of the traditional semiconductor digital computer should be substituted by superconducting interconnections. The memory ferromagnetic units of the traditional digital computer should be substituted by superconducting memories containing superconducting loops. In Section equation 5 we have emphasized that in superconductors we must apply the flux quantization rule that is the magnetic flux ỉ must be quantized in a superconducting loop according to the rule ỉ n 0 where A is a quantum of magnetic flux. Thus using appropriate .

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