Modes of operation

You can define the light emission during the cathodoluminescence (CL) process by its distributions in:

  • Wavelength (color or energy)
  • Angle (momentum)
  • Polarization
  • Time

During a CL measurement, you can analyze one or more of these distributions. Analyses can originate from a single, user-defined spot or area on the surface of a specimen, or in a spatially-resolved manner. In other words, when the electron beam scans across the specimen surface in a pre-defined pattern, it captures the light distribution(s) of interest at each step.

The term -filtered describes analysis modes that select a single or small range of wavelength, angle, or polarization distributions, whereas -resolved designates the recording of an entire distribution (in parallel).

In some advanced analysis methods, you can measure more than one distribution. In these cases, the data may be described in a string—for example, polarization-filtered emission pattern or wavelength- and time-resolved spectrum.  

For a more detailed chart, please see the download available.

Investigating the optical properties of nanophotonic materials far below the diffraction limit

Unfiltered

Overview

In unfiltered mode, the intensity (magnitude) of the cathodoluminescence (CL) signal is measured. The measurement is integrated over all wavelengths, angles, and polarizations for a defined time interval.

Sometimes referred to as panchromatic, polychromatic, or black and white imaging.

Data collection

Unfiltered signal: The magnitude of the total CL signal (count rate or intensity) is measured using a light-sensitive detector such as a photomultiplier tube (PMT) or solid-state diode. The electron beam of the electron microscope may be continuously positioned at a defined location on the specimen (spot mode) or scanned rapidly over a defined area and the measured CL signal integrated over all locations.

Unfiltered map: The electron beam is scanned across the specimen surface, and the emitted light intensity is recorded at each location and displayed as a map.

Uses

Reveal texture in mineralogy, zonation, overgrowths, and micro-cracks; and reveal extended defects in semiconductor materials and devices.


Example of an unfiltered CL image showing the spatial variation in the integrated CL emission from an array of compound semiconductor microrods.

Cathodoluminescence techniques for the geosciences

Wavelength-Resolved

Overview

In wavelength-resolved mode, the wavelength distribution of the emitted light is analyzed. Light collected from the specimen is focused onto the entrance slit of a spectrograph that disperses light by wavelength (energy) using a pixelated detector to record a wavelength spectrum—a histogram displaying the intensity of light by wavelength.

Sometimes referred to as hyperspectral cathodoluminescence analysis or wavelength imaging.

Data collection

Wavelength-resolved spectrum: The wavelength distribution of emitted light is recorded from a point or region of the sample exposed to the electron beam of the electron microscope. One-dimensional data is displayed by plotting a histogram of count rate (intensity) versus wavelength or energy—wavelength and energy being inversely proportional.

Wavelength-resolved spectrum image: The electron beam is scanned across the specimen surface in a pre-defined pattern, and a wavelength-resolved spectrum is recorded at each location, creating hyperspectral (3D) data.

Uses

Identify compounds and phases, determine the electronic structure, reveal and determine trace elements, map composition, and/or stress.


An example 3D spectrum image data construct (x,y,λ) recorded from a polished zircon grain. At each pixel in the image, a complete wavelength-resolved spectrum has been recorded and is displayed as a true-color representation based on the analysis of the measured spectrum. At each spatial location (xn,yn) a full wavelength-resolved emission spectrum may be extracted from the data construct.

Determining photonic band structure by energy-momentum spectroscopy in an electron microscope Cathodoluminescence techniques for the geosciences

Wavelength-Filtered

Overview

In wavelength-filtered mode, cathodoluminescence (CL) information is captured using only a (narrow) range of wavelengths. Typically, wavelength-filtering is performed by detecting the light that passes through the wavelength selecting (exit) slit of a scanning spectrometer or an optical transmission filter. The use of an optical spectrometer provides the greatest flexibility in the selection of the wavelength and wavelength range (bandpass). Still, images generated in this way have a more inferior signal-to-noise ratio than an equivalent image captured using an optical filter due to higher losses through the spectrometer. However, it is impractical to have hundreds (or thousands) of optical filters with the desired transmission parameters, so scanning spectrometers are used widely.

Sometimes referred to as monochromatic imaging or spectral imaging.

Data collection

Wavelength-filtered signal: The intensity of the emitted light recorded from a point or region of the sample exposed to the electron beam of the scanning electron microscope (SEM). The signal is limited to a small range of (user-defined) wavelengths; no angle or polarization information is contained.

Wavelength-filtered spectrum: The wavelength distribution of the emitted light is captured. The wavelength-filtered signal is recorded over a user-defined range of wavelengths, one wavelength at a time. A scanning spectrometer is used to step through the wavelength range to build up a spectrum in a (wavelength) step-by-step approach. Sometimes referred to as serial spectroscopy.  

Wavelength-filtered map: The electron beam is scanned across the specimen surface, and the wavelength-filtered signal is recorded at each location and displayed as a (2D) map. More than one wavelength-filtered map may be recorded from the same region of the specimen. Typically, a user defines two (or more) wavelength ranges enabling the spatial distribution of emission centers to be discriminated against.


Wavelength-filtered images of a polished reservoir quartz thin section.

Color map: A unique form of wavelength-filtered mapping captures three discrete wavelength bands corresponding to the red, green, and blue components of the visible spectrum. The three components are recombined to form a color image in much the same way as the viewing screen of a color television. Some specialized detectors such as the ChromaCL2™ detector capture the color components simultaneously, enabling color images to be captured in a single pass of the electron beam. More typically, sequential scans of the electron beam are required, with the user changing the color component detected between scans of the electron beam.

Wavelength-filtered spectrum image: A spatially- and spectrally-resolved (3D) hyperspectral data cube is captured by collecting a series of (aligned) wavelength-filtered maps.

In this acquisition mode, a PMT detector is used to collect n wavelength-filtered CL images whose pixel time in each image slice can be collected thousands of times faster than by an array detector used in the wavelength-resolved approach. Spectrum images with 167 wavelength channels may be collected up to 30x quicker as a result.

Uses

Discriminate materials by composition and/or crystal structure, reveal the purity of semiconductor materials, determine resonance modes in nanophotonic materials.


An example 3D spectrum image data construct (x,y,λ) recorded from a polished zircon grain. At each captured wavelength in the spectrum, a complete spatial image has been recorded and is displayed as a true-color representation based on the analysis of the measured spectrum. At each spatial location (xn,yn), a full wavelength-resolved emission spectrum may be extracted from the data construct.

Determining photonic band structure by energy-momentum spectroscopy in an electron microscope Cathodoluminescence techniques for the geosciences

Angle-Resolved

Overview

In the angle-resolved cathodoluminescence (ARCL) mode, the direction in which a photon is emitted is determined. An objective lens or, more commonly, a collection mirror projects an image of the emitted light onto a pixelated detector, e.g., a camera. When an appropriate optical system is used, each pixel in the captured image corresponds to a unique emission direction from the specimen. Typically, the raw image is transformed into polar coordinates for display and interpretation.

The result of an angle-resolved measurement contains no wavelength or polarization information unless additional filtering of dispersion is used (e.g., wavelength- and angle-resolved mode).

Angle-filtered information may be captured by using an iris or a pinhole to select a certain (range of) angle(s). However, the low resolution and highly serial nature of this particular acquisition mode have limited its usefulness.

Sometimes referred to as Fourier imaging or momentum spectroscopy.


Schematic ray diagrams demonstrating the experimental setup for intensity (left) and angle-resolved (right) measurements. A specialized optical system is required for angle-resolved measurements with the transfer optics and detector changed such that a 2D image is projected and sensed by a pixelated detector.

Data collection

Emission pattern or angle-resolved emission pattern: The emission pattern is a plot of the direction in which photons are emitted from a specimen, typically presented in polar coordinates where the emission direction is described by the azimuthal and zenith angles. A single emission pattern may be captured from a point or region of the sample exposed to the electron beam of the electron microscope.

Emission pattern image or angle-resolved spectrum image: The electron beam is scanned across the specimen surface, and an emission pattern is recorded at each location, creating a hyperspectral (4D) data construct.

Uses

Investigating the optical properties of nanophotonic materials far below the diffraction limit

Polarization

Overview

Light is a transverse electromagnetic wave. The electric and magnetic fields that compose the light wave always oscillate transversely to the propagation direction; the polarization describes the direction that these electromagnetic fields oscillate.

A polarization analyzer can be incorporated into the optical chain of another cathodoluminescence (CL) mode to provide polarization-filtered or polarization-resolved data. For example, a polarization- and wavelength-filtered map or a polarization- and angle-resolved emission pattern (polarimetry).

Data collection

Polarization filtered: The polarization analyzer consists of a linear polarizer with a user-defined orientation.

Polarization-resolved: The polarization analyzer consists of a quarter-wave plate and linear polarizer. When images are captured over six different analyzer settings, the Stokes parameters that describe the full polarization state of the emitted light may be retrieved.

Uses 

Polarization plays a key role in light-matter interactions and is helpful to study coherence, scattering, birefringence, and chirality finding wide applications in nanophotonic applications. More recently, the degree of polarization has been used to characterize strain in single-crystal semiconductors and insulators. While in (multi-crystalline) samples such as meteorite thin sections, the polarization of the emitted light has also been used to reveal crystal orientation and mineral texture.


An example of how analysis using polarization filtering enhances understanding of a nanophotonic particle. In this example, a 100 nm nanostar (a) exhibits four resonance nodes however, a polarization-filtered spectrum-image (b) demonstrates that the emission consists of two distinct dipole modes that also exhibit different emission patterns (c).

Experiment briefs and application notes

Observation of crystal structure orientation by cathodoluminescence (CL) polarization-filtered spectrum imaging Investigating the optical properties of nanophotonic materials far below the diffraction limit

Time-Resolved

Overview

Time-resolved cathodoluminescence (CL) experiments record how the CL signal varies with time; the signal may be from any of the modes of operation but is more typically restricted to the wavelength-filtered intensity or wavelength-spectrum.

The term time-resolved covers a very broad range of time domains extending from several minutes or hours, such as in experiments that monitor the impact of electron beam exposure on the sample, to picoseconds where the dynamics of excitons and free carriers in semiconductors are analyzed.

Wavelength- and Angle-Resolved

Overview

Wavelength- and angle-resolved cathodoluminescence (WARCL) mode enables spectroscopic analysis of the emission pattern of a sample. The data collected as a 3D data cube (λ,θ,Φ) and can be thought of as a stack of wavelength-filtered emission patterns or a (wavelength) spectrum recorded in every emission direction.

Sometimes referred to as energy-momentum spectroscopy.

 

Data collection

Data collection utilizes an angle-selecting slit to select a portion of angle-space before using an imaging spectrograph to disperse by wavelength. Commonly, for higher spatial and spectral resolutions, the angular range is scanned sequentially to reconstruct the data cube (λ,θ,Φ).

 

Uses

Understand the wavelength distribution (color) of light-emitting devices as a function of viewing angle, determine energy-momentum diagrams of photonic samples to gain deep insight into how light and matter interact down to the nanoscale.

An emission pattern spectrum from a micro-LED array revealing distinct emission patterns to be observed at each wavelength; the data has been colorized according to the wavelength. The static images show the emission pattern at each corresponding color and the video represents the entire dataset that consists of emission patterns recorded at 1340 wavelengths across the visible spectrum.

Determining photonic band structure by energy-momentum spectroscopy in an electron microscope