Liquid helium-free high-T c superconducting terahertz emission system and its applications

2020 ◽  
Vol 59 (10) ◽  
pp. 105004
Author(s):  
Yoshihiko Saiwai ◽  
Takanari Kashiwagi ◽  
Kurama Nakade ◽  
Manabu Tsujimoto ◽  
Hidetoshi Minami ◽  
...  
2005 ◽  
Vol 86 (26) ◽  
pp. 261102 ◽  
Author(s):  
Toshihiko Kiwa ◽  
Keiji Tsukada ◽  
Masato Suzuki ◽  
Masayoshi Tonouchi ◽  
Sonoko Migitaka ◽  
...  

2012 ◽  
Vol 717-720 ◽  
pp. 553-556 ◽  
Author(s):  
Vladimir Ilich Sankin ◽  
Alexander V. Andrianov ◽  
A.G. Petrov ◽  
P.P. Shkrebiy ◽  
A.O. Zacharin

We report on efficient terahertz emission in the region of 1.5-2 THz from high electric field biased 6H-SiC structures with a natural superlattice at liquid helium temperatures. The shape of the emission spectrum, the linear dependence of its maximum on the bias and the characteristic field strength required to achieve the emission allow the emission to be attributed to steady-state Bloch oscillations of electrons in the SiC natural superlattice.


Author(s):  
R. E. Worsham ◽  
J. E. Mann ◽  
E. G. Richardson

This superconducting microscope, Figure 1, was first operated in May, 1970. The column, which started life as a Siemens Elmiskop I, was modified by removing the objective and intermediate lenses, the specimen chamber, and the complete vacuum system. The large cryostat contains the objective lens and stage. They are attached to the bottom of the 7-liter helium vessel and are surrounded by two vapor-cooled radiation shields.In the initial operational period 5-mm and 2-mm focal length objective lens pole pieces were used giving magnification up to 45000X. Without a stigmator and precision ground pole pieces, a resolution of about 50-100Å was achieved. The boil-off rate of the liquid helium was reduced to 0.2-0.3ℓ/hour after elimination of thermal oscillations in the cryostat. The calculated boil-off was 0.2ℓ/hour. No effect caused by mechanical or electrical instability was found. Both 4.2°K and 1.7-1.9°K operation were routine. Flux pump excitation and control of the lens were quite smooth, simple, and, apparently highly stable. Alignment of the objective lens proved quite awkward, however, with the long-thin epoxy glass posts used for supporting the lens.


Author(s):  
Michel Troyonal ◽  
Huei Pei Kuoal ◽  
Benjamin M. Siegelal

A field emission system for our experimental ultra high vacuum electron microscope has been designed, constructed and tested. The electron optical system is based on the prototype whose performance has already been reported. A cross-sectional schematic illustrating the field emission source, preaccelerator lens and accelerator is given in Fig. 1. This field emission system is designed to be used with an electron microscope operated at 100-150kV in the conventional transmission mode. The electron optical system used to control the imaging of the field emission beam on the specimen consists of a weak condenser lens and the pre-field of a strong objective lens. The pre-accelerator lens is an einzel lens and is operated together with the accelerator in the constant angular magnification mode (CAM).


Author(s):  
M.K. Lamvik ◽  
D.A. Kopf ◽  
S.D. Davilla ◽  
J.D. Robertson

Last year we reported1 that there is a striking reduction in the rate of mass loss when a specimen is observed at liquid helium temperature. It is important to determine whether liquid helium temperature is significantly better than liquid nitrogen temperature. This requires a good understanding of mass loss effects in cold stages around 100K.


1978 ◽  
Vol 126 (12) ◽  
pp. 693-694
Author(s):  
D.M. Chernikova ◽  
L.P. Gor'kov

1978 ◽  
Vol 126 (12) ◽  
pp. 690-691
Author(s):  
V.B. Shikin
Keyword(s):  

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