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Electrons cannot enter the solid until their energies are higher than the vacuum level and this furnishes a simple way for measuring the work function, provided that the energy of the beam has been carefully calibrated (see Ref.).
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Electrons cannot enter the solid until their energies are higher than the vacuum level and this furnishes a simple way for measuring the work function, provided that the energy of the beam has been carefully calibrated (see Ref.).
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Actually the peak B1 is more attenuated by the MgO film than for the rest of the spectruism, but this is a well-known result explained in terms of the high sensitivity of this peak to the surface order, which is altered after MgO deposition, see also Refs..
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Actually the peak B1 is more attenuated by the MgO film than for the rest of the spectruism, but this is a well-known result explained in terms of the high sensitivity of this peak to the surface order, which is altered after MgO deposition, see also Refs..
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Note that the value of Δ EC is much higher than that previously reported by some of the authors in Ref. from the clean Fe(001) surface, but the same holds true also for the Fe (001) -p (1×1) O surface. This is probably due to the higher surface order of the samples investigated in the present paper and to some differences in the experimental apparatus.
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Note that the value of Δ EC is much higher than that previously reported by some of the authors in Ref. from the clean Fe(001) surface, but the same holds true also for the Fe (001) -p (1×1) O surface. This is probably due to the higher surface order of the samples investigated in the present paper and to some differences in the experimental apparatus.
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