Photoelectron Spectrum

What is Photoelectron Spectroscopy (PES)?

Photoelectron spectroscopy (PES) is a method of determining the relative energy of electrons in atoms and molecules.

A photoelectron count vs. binding energy graph is called a PES spectrum.

PES peaks represent electrons in various subshells of an atom. Valence electrons are represented by the peaks with the lowest binding energies, whereas core electrons are represented by the peaks with the highest binding energies.

Table of Contents

• Introduction to Photoelectron Spectroscopy (PES)
  • Photoelectron Spectroscopy Fundamentals
  • Analyzation of PES spectra
  • Photoelectric Effect
• PES Spectrum of Lithium
• PES spectrum of Oxygen
• Photoelectron Spectroscopy in Practice
• Frequently Asked Questions

Introduction to Photoelectron Spectroscopy (PES)

PES (photoelectron spectroscopy) is a technique for determining the relative energy of electrons in atoms and molecules. PES is frequently used by scientists to investigate the elemental makeup of materials or to analyse molecular bonding.

Photoelectron spectroscopy (PES) studies the composition and electronic state of a sample’s surface region by ionising it and analysing the kinetic energy distribution of the emitted photoelectrons.

It analyses the electronic structure of molecules by measuring photoelectrons’ kinetic energy to determine the binding energy, intensity, and angular distributions of these electrons. It is distinct from standard spectroscopy in that it investigates a substance’s electrical structure by detecting electrons rather than photons.

Photoelectron Spectroscopy Fundamentals

The photoelectric effect, first described by Albert Einstein in 1905, provides the basis for photoelectron spectroscopy. When electrons in a metal are exposed to enough light, they are ejected off the metal surface, which is known as the photoelectric effect. We may determine the energy of the electrons in the solid metal if we know the kinetic energy of the expelled electrons (also known as photoelectrons) and the energy of the incident radiation.

PES involves bombarding a sample with high-energy radiation, usually UV or X-ray, which causes electrons to be expelled. The expelled electrons go from the sample to an energy analyzer, where their kinetic energies are recorded, and then to a detector, where the quantity of photoelectrons at different kinetic energies is counted. This procedure is depicted in a simplified graphic below.

The ionisation energy or binding energy of an electron is the amount of energy required to expel it from a substance.

Analyzation of PES spectra

Photoelectron count vs. binding energy graphs is obtained from PES studies, with binding energy commonly given in electron volts (eV) or megajoules (MJ) per mole.

Peaks with various binding energies can be found in a typical PES spectrum. Each of these peaks corresponds to electrons in a distinct subshell of an atom since electrons in the same subshell of an atom have the same binding energy. The binding energy of a peak indicates how much energy is required to remove an electron from a subshell, while the peak’s intensity indicates the subshell’s relative quantity of electrons.

Photoelectric Effect

A schematic illustration of the effect is shown in the diagram.

As Hertz observed empirically and as Einstein explained using energy quantization, electrons are expelled from a substance with kinetic energy connected to the energy of the incident radiation. In principle, the relationship is described. The photoelectron’s kinetic energy is Ekin, while the electron’s binding energy is EB. A well-known work function can be found in many materials. As is common when working with atoms, molecules, and clusters, all energies and spectra calibrations are reported in terms of the vacuum level in this publication.

PES Spectrum of Lithium

Let’s start with the lithium, Li, idealised PES spectrum. For comparison, lithium’s ground-state electron structure is 1s², 2s¹.

The PES spectrum reveals two peaks, which correspond to electrons in lithium’s two subshells (1s and 2s). The peak closest to the origin has twice the intensity of the peak further away. Because the 1s subshell of lithium has twice as many electrons as the 2s subshell (2 vs. 1), the peak closest to the origin must be the 1s subshell of lithium.

This is also consistent with binding energies: we know that electrons in the 1s subshell of lithium are closer to the nucleus and less protected than electrons in the 2s subshell. As a result, removing the 1s electrons requires more energy. This is supported by the fact that the PES spectrum’s 1s peak has greater binding energy.

It’s important to note that the binding energy of lithium’s 2s peak is the same as the initial ionisation energy of lithium–that is, the amount of energy necessary to remove a lithium atom’s outermost or least bonded electron. The binding energy of the 1s peak, however, is not equal to lithium’s second ionisation energy. The nucleus will hold the 1s electrons much tighter if the first electron is withdrawn from lithium, increasing the binding energy of these electrons.

PES spectrum of Oxygen

Let’s have a look at some elements with more electrons. The idealised PES spectrum for oxygen, O, is shown here. The ground-state electron configuration of oxygen is 1s²2s²2p⁴.

This spectrum has three peaks, each indicating electrons in a different subshell of oxygen (either 1s, 2s, or 2p). Because electrons in the 1s subshell are closer to the nucleus and less protected than those in the 2s or 2p subshells, we would anticipate the peak with the highest binding energy (the leftmost peak) to belong to electrons in the 1s subshell. The 2s subshell must correspond to the peak with the next highest binding energy and the 2p subshell to the peak with the lowest binding energy (the rightmost peak).

The 2p subshell of oxygen has twice as many electrons as the 1s or 2s subshells (4 vs. 2). As a result, we should expect the 2p peak to be twice as powerful as the 1s or 2s peak, as shown in the spectrum.

Because electrons in the same electron shell have similar energies, we’d expect to find peaks in a PES spectrum showing electrons in the same shell grouped together.

Photoelectron Spectroscopy in Practice

Detecting impurities, managing purification, investigating the kinetics of chemical processes, identifying molecular weight, and determining unknown concentrations are all applications of electronic spectroscopy.

XPS has a wider range of applications than UPS since it can probe down to core electrons. Except for two elements, XPS is useful for detecting elements, evaluating the chemical state of surfaces, and performing quantitative analysis. The chemical states of samples can be distinguished using XPS. Different oxidation states of compounds can also be distinguished using XPS.