The main characteristic peaks identify nickel and phosphorus: the spectrum has a strong Ni peak near , the Ni region near and P near . Weaker associated lines, including Ni near , can accompany them. The continuous background is bremsstrahlung from decelerated electrons.
Small carbon and oxygen signals at low energy can arise from contamination, surface oxide or preparation materials; a copper contribution can arise from the adjacent substrate within the finite interaction volume. The Cu region lies close to Ni , so overlap is particularly troublesome at low energy. A weak Cu contribution near is better separated, though still close to Ni . At the beam can excite these K lines.
Peak height is not an atomic fraction: ionization cross-sections, fluorescence yields, absorption, detector response, background and line overlap require correction. The large nickel peak therefore supports the nickel-rich assignment but does not directly give the nickel-to-phosphorus atomic ratio.
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