Picture of Hydrogen
    

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Periodic Table

Ground State Electron Configuration of Hydrogen

 1  

 

H
1
Li
3
Na
11
K
19
Rb
37
Cs
55
Fr
87
Uue
119
Uhe
169
Bue
219

Hydrogen           Truss Element

Symbol H
Atomic Number 1
Relative Atomic Mass
12C = 12.0000
1.00794
Atomic Radius pm 37
First Ionisation Energy
kJ mol -1
1312.0
Ionization energy (eV) 13,5984
Electronegativity 2.20
Density
kg m -3
76.0 [11 K]
70.8 [b.p.]
0.08988 [273 K]
Molar Volume cm 3 13.26 [11 K]
Thermal Conductivity
W m -1 K -1
0.1815 [300 K]
Melting Point K 14.01
Boiling Point K 20.28
Number of Isotopes 3
Inner + outer Shells
 0   +  1   = 1
Inner + outer Orbital(s)
 0   +  1   = 1
Filling Orbital
  1s 1    
Ground State Electron
Configuration 
 1s 1 
Ground State Electron
Configuration with
free Orbitals (n= 1)

 

 1 

Ground State Electron Configuration with free Orbitals of Hydrogen
Ground State Electron
Configuration with
compressed Orbitals (n= 0)

 

 0 

Ground State Electron Configuration with compressed Orbitals of Hydrogen
Singularity     S(n=1)
2 0 + 1 + 1 + 0
 

s

p

d

 f

g

h

i

j

1

1

1

 

 

 

 

 

 

 

2

 

 

 

 

 

 

 

 

3

 

 

 

 

 

 

 

 

4

 

 

 

 

 

 

 

 

5

 

 

 

 

 

 

 

 

6

 

 

 

 

 

 

 

 

7

 

 

 

 

 

 

 

 

8

 

 

 

 

 

 

 

 

 
Term Symbol 2S 1/2
Discovery H. Cavendish (London, England) in 1766
Name Derived From Greek hydro genes meaning 'water forming'
 

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Physical Review Letters, Band 95, Artikel 135301
 
Observation of a Metallic Superfluid in a Numerical Experiment
E. Smørgrav,1 E. Babaev,2,1 J. Smiseth,1 and A. Sudbø1

 
1Department of Physics, Norwegian University of Science and Technology, N-7491 Trondheim, Norway
2Laboratory of Atomic and Solid State Physics, Cornell University, Ithaca, New York 14853-2501, USA
(Received 8 June 2005; published 23 September 2005)

We report the observation, in Monte Carlo simulations, of a novel type of quantum ordered state: the metallic superfluid. The metallic superfluid features Ohmic resistance to counterflows of protons and electrons, while featuring dissipationless coflows of electrons and protons. One of the candidates for a physical realization of this remarkable state of matter is hydrogen or its isotopes under high compression. This adds another potential candidate to the presently known quantum dissipationless states, namely, superconductors, superfluid liquids and vapors, and supersolids.
 

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2002-06-04

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