Chemical elements
    Physical Properties
      Mechanical Properties
      Plastic Flow
      Coefficient of Expansion
      Thermal Conductivity
      Molten Nickel
      Magnetic Power
      Thermal Properties
      Index of Refraction
      Radiation Energy
      Absorption Spectra
      X-ray Spectrum
      Emission of Electrons
      Photoelectric Effect
      Ionization Potentials
      Conductivity of Crystal Nickel
      Contact Potential
      Electrochemical Series
      Electrode Potential
      Salts Solutions
      Nickel-Iron Accumulator
      Thermoelectric Force
      Peltier effect
      Thomson effect
    PDB 1a5n-1g2a
    PDB 1g3v-1mn0
    PDB 1mro-1s9b
    PDB 1scr-1xmk
    PDB 1xu1-2cg5
    PDB 2cqz-2jih
    PDB 2jk8-2v4b
    PDB 2vbq-3c2q
    PDB 3c6c-3h85
    PDB 3hdp-3kvb
    PDB 3l1m-3o00
    PDB 3o01-4ubp
    PDB 8icl-9ant

Emission of Electrons by Nickel

A. T. Waterman, H. Schenck, C. Davisson and C. H. Kunsman, K. Hayakawa, S. R. Rao, H. Schenck, H. Nukiyama and H. Horikawa, H. E. Farnsworth, A. L. Patterson, E. W. B. Gill, R. M. Chaudhri, R. L. Petry, W. Espe, and P. Tartakovsky and V. Kudrjavzeva studied the emission of electrons by nickel; H. A. Barton, the emission of electrons from oxide-coated filaments; E. F. Richter, the emission from films coated with barium oxide; W. Distler and G. Monch, the potential of electronic emission from glowing nickel; G. Glockler, electron affinities; W. Uyterhoven and M. C. Harrington, H. A. Erikson, C. Hurst, S. R. Rao, E. Shearer, and M. L. E. Oliphant and P. B. Moon, the liberation of electrons by positive ions; H. B. Wahlin, the emission of electrons from hot wires; R. Viohl, the heat of condensation of electrons on nickel; C. H. Thomas, A. L. Klein, M. C. Harrington, S. R. Rao, M. N. Davis, B. J. Thomson, W. S. Stein, S. R. Rao, H. Nukiyama and H. Horikawa, K. S. Woodcock, P. B. Moon, P. Tartakovsky and V. Kudrjavzeva, R. M. Chaudhri, W. Uyterhoven and M. C. Harrington, N. C. Beese, W. J. Jackson, and M. L. E. Oliphant, the secondary emission of electrons from nickel bombarded by positive rays; L. H. Germer, H. Raether, C. Davisson and L. H. Germer, K. L. Horovitz and co-workers, T. Benecke', and E. Rupp, the diffraction of electrons by nickel; H. E. Farnsworth, C. Davisson and co-workers, R. W. G. Wyckoff, A. L. Patterson, and R. L. Doan, the scattering of electrons; L. H. Germer, H. W. Edwards, and E. Rupp, the reflection of electrons; C. Boeckner, the radiations emitted by bombardment with slow electrons; 0. Klemperer, electronic collisions; E. Rupp, C. Davisson and co-workers, the absorption of electrons; C. Davisson and L. H. Germer. the anomalous dispersion at 1.3 A. of electron waves by nickel; C. Davisson and L. H. Germer, the refraction of electrons; G. W. Fox and R. M. Bowie, and H. E. Farnsworth, and D. A. Wells, the energy of distribution of secondary electrons; and E. D. Eastman, the thermal capacity of the electrons; L. H. Germer, the electronic motions and gas absorption; R. Ruedy, the free and bound electrons in nickel; D. A. Wells, the energy of the emission; and W. Distler and G. Monch, the thermionic work function.

L. L. Barnes studied the emission of positive ions from nickel; A. K. Brewer, the effect of ammonia on the emission of positive ions; H. R. von Traubenberg, the range of the a-particles in nickel; and K. S. Woodcock, the emission of electrons from nickel bombarded by a-rays. J. K. Roberts studied the exchange of energy between helium atoms and a nickel surface; P. B. Moon, the emission of electrons from nickel bombarded by caesium ions; R. B. Sawyer, and A. Longacre, the reflection and scattering of lithium ions from nickel crystals; and A. Coehn and K. Sperling, the action on a photographic plate. W. G. Guy observed no radioactivity with nickel.

R. D. Kleeman found the ionization produced by the α-, β-, and γ-rays to be in the proportion 1.72: 2.67: 2.81. H. Pattersson studied the reflection of α-particles from atomic nuclei; and E. Rie, the penetration of radium rays. G. P. Thomson studied the diffraction of the cathode rays by nickel; J. A. Becker, the loss in intensity on transmitting slow cathode rays through nickel films of thickness 0.02μ and 0.04μμ, at 20 volts - it amounts to 1.12×10-4, and 0.047×10-4, respectively; and G. Fournier, the absorption of β-rays. E. Rie observed that the depth of penetration of radioactive recoil atoms from radium emanations is 10μμ. I. Curie and F. Joliot, E. Fermi and co-workers, and W. G. Guy studied the induced radioactivity of nickel. W. Arkadieff studied the electric and magnetic spectra of electro-magnetic waves; and Y. H. Woo, the Compton effect. A. Imhof showed that stationary waves are emitted by wires heated by an alternating current.

N. Piltschikoff said that nickel emits Moser rays capable of passing through paper, celluloid, or aluminium, and of decomposing silver bromide. E. Amaldi and co-workers observed no induced radioactivity with nickel. R. Robl observed no luminescence with nickel in ultra-violet light.

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