The Spin Polaron Model and the Comparison with Liquid Helium

2021 ◽  
pp. 271-294
Author(s):  
Ν F Mott
Keyword(s):  
Liquid Helium ◽  
Spin Polaron ◽  
Polaron Model

Small spin-polaron model for a hole in the CuO 2 layer

1989 ◽  
Vol 162-164 ◽  
pp. 1499-1500 ◽  
Author(s):  
J. Appel ◽  
P. Hertel ◽  
F. Richter
Keyword(s):  
Spin Polaron ◽  
Polaron Model

scholarly journals Spin-polaron model: Transport properties ofEuB6

2004 ◽  
Vol 69 (13) ◽  
Author(s):  
Jayita Chatterjee ◽  
Unjong Yu ◽  
B. I. Min
Keyword(s):  
Transport Properties ◽  
Spin Polaron ◽  
Polaron Model

A spin polaron model of high-Tc superconductivity

1990 ◽  
Vol 165 (1) ◽  
pp. 97-106 ◽  
Author(s):  
R.F. Wood ◽  
Mark Mostoller ◽  
J.F. Cooke
Keyword(s):  
Spin Polaron ◽  
Polaron Model ◽  
High Tc ◽  
High Tc Superconductivity

A Superconducting Microscope

1971 ◽  
Vol 29 ◽  
pp. 10-11 ◽  
Author(s):  
R. E. Worsham ◽  
J. E. Mann ◽  
E. G. Richardson
Keyword(s):  
Liquid Helium ◽  
Focal Length ◽  
Vacuum System ◽  
Objective Lens ◽  
Electrical Instability ◽  
Radiation Shields ◽  
And Control ◽  
Thermal Oscillations ◽  
Flux Pump

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.

Water accumulation as a function of temperature on specimens in an electron microscope cold stage

1986 ◽  
Vol 44 ◽  
pp. 114-115 ◽  
Author(s):  
M.K. Lamvik ◽  
D.A. Kopf ◽  
S.D. Davilla ◽  
J.D. Robertson
Keyword(s):  
Electron Microscope ◽  
Mass Loss ◽  
Liquid Helium ◽  
Liquid Nitrogen ◽  
Liquid Nitrogen Temperature ◽  
Liquid Helium Temperature ◽  
Helium Temperature ◽  
Cold Stage ◽  
Water Accumulation ◽  
Better Than

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.

Sign in / Sign up

Export Citation Format

Share Document