Liquid-Helium Configuration around a Metastable Excited Helium Atom

1972 ◽  
Vol 5 (5) ◽  
pp. 2214-2216 ◽  
Author(s):  
J. P. Hansen ◽  
E. L. Pollock
1999 ◽  
Vol 60 (2) ◽  
pp. 986-995 ◽  
Author(s):  
A. Derevianko ◽  
W. R. Johnson ◽  
V. D. Ovsiannikov ◽  
V. G. Pal’chikov ◽  
D. R. Plante ◽  
...  

2020 ◽  
Vol 74 (7) ◽  
Author(s):  
Tasko P. Grozdanov ◽  
Alexander A. Gusev ◽  
Evgeni A. Solov’ev ◽  
Sergue I. Vinitsky

1964 ◽  
Vol 42 (8) ◽  
pp. 1522-1528 ◽  
Author(s):  
H. C. Khare ◽  
P. R. Wallace ◽  
G. G. Bach ◽  
A. Chodos

It is shown that it is possible for a positron to form a bound state with a helium atom, with a binding energy of about 0.55 electron volt. The lifetime of positrons in liquid helium is substantially longer than the predicted lifetime for annihilation from this state, indicating that capture into such a state takes a time considerably longer than the annihilation lifetime. On the other hand, the observed lifetime implies an electron density at the positron larger than the mean electron density in the material, consistent with the expected attraction of the positron toward the helium atom.


1990 ◽  
Vol 42 (5) ◽  
pp. 2550-2554 ◽  
Author(s):  
P. Froelich ◽  
S. A. Alexander

1975 ◽  
Vol 12 (9) ◽  
pp. 3705-3717 ◽  
Author(s):  
A. P. Hickman ◽  
W. Steets ◽  
Neal F. Lane

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):  
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.


2003 ◽  
Vol 50 (3-4) ◽  
pp. 353-364 ◽  
Author(s):  
S. Laulan ◽  
H. Bachau ◽  
B. Piraux ◽  
J. Bauer ◽  
G. Lagmago Kamta
Keyword(s):  

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