scholarly journals Hydrogen Molecule Ion in Strong Magnetic Fields

1976 ◽  
Vol 37 (11) ◽  
pp. 676-679 ◽  
Author(s):  
C. P. Melo ◽  
R. Ferreira ◽  
H. S. Brandi ◽  
L. C. M. Miranda
Keyword(s):  
Magnetic Fields ◽  
Hydrogen Molecule ◽  
Strong Magnetic Fields

Ionization energies of the hydrogen molecule ion in strong magnetic fields

1977 ◽  
Vol 55 (7-8) ◽  
pp. 609-614 ◽  
Author(s):  
C. S. Lai ◽  
B. Suen
Keyword(s):  
Variational Principle ◽  
Hydrogen Atom ◽  
Magnetic Fields ◽  
Ionization Energy ◽  
Hydrogen Molecule ◽  
Wave Functions ◽  
Internuclear Separation ◽  
Linear Combinations ◽  
Strong Magnetic Fields ◽  
Better Than

The variational principle is used to determine the ionization energy and equilibrium internuclear separation of a hydrogen molecule ion in the presence of magnetic fields of strength up to [Formula: see text]. The trial wave functions used are made of some linear combinations of the unperturbed wave functions of the hydrogen atom. The results are shown to be better than those of de Melo, Ferreira, Brandi, and Mirandi for fields less than ~3 × 1010 G.

Strong magnetic fields

1960 ◽  
Vol 70 (4) ◽  
pp. 693-714 ◽  
Author(s):  
G.M. Strakhovskii ◽  
N.V. Kravtsov
Keyword(s):  
Magnetic Fields ◽  
Strong Magnetic Fields

Magnetic molecular nanoclusters in strong magnetic fields

2002 ◽  
Vol 172 (11) ◽  
pp. 1303 ◽  
Author(s):  
Anatolii K. Zvezdin ◽  
Viktor V. Kostyuchenko ◽  
V.V. Platonov ◽  
V.I. Plis ◽  
A.I. Popov ◽  
...  
Keyword(s):  
Magnetic Fields ◽  
Strong Magnetic Fields

scholarly journals The measurement of the energy of cosmic rays - II—The curvature measurements and the energy spectrum

1936 ◽  
Vol 154 (883) ◽  
pp. 573-587 ◽  
Keyword(s):  
Magnetic Field ◽  
Energy Spectrum ◽  
Cosmic Rays ◽  
Magnetic Fields ◽  
Strong Magnetic Fields ◽  
The Earth ◽  
Primary Particles ◽  
Curvature Measurements

Both the penetrating power of the cosmic rays through material ab­sorbers and their ability to reach the earth in spite of its magnetic field, make it certain that the energy of many of the primary particles must reach at least 10 11 e-volts. However, the energy measurements by Kunze, and by Anderson, using cloud chambers in strong magnetic fields, have extended only to about 5 x 10 9 e-volts. Particles of greater energy were reported, but the curvature of their tracks was too small to be measured with certainty. We have extended these energy measurements to somewhat higher energies, using a large electro-magnet specially built for the purpose and described in Part I. As used in these experiments, the magnet allowed the photography of tracks 17 cm long in a field of about 14,000 gauss. The magnet weighed about 11,000 kilos and used a power of 25 kilowatts.

Sign in / Sign up

Export Citation Format

Share Document