Available "beam size" for sample measurements

Available "beam size" for sample measurements

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Motorised pinholes are fitted in the Hyperion microscope, controlled with a QEGui program. While the pinhole sizes are fixed, the projected aperture (i.e. size of beam hitting sample and detector) will be dependent on the technique and the objective being used.

The calculation is simple enough:

For transmission:

Spot size (μm) = pinhole size (μm) / magnification

For ATR experiments, the refractive index (n) of the crystal being used needs to be factor in:

Spot size (μm) = pinhole size (μm) / magnification / n

image-20250718-052743.png
Figure: Available pinhole sizes at the IRM beamline. The values in grey are below our standard working size and you should contact a beamline scientist if you wish to use these very small sizes

The final considerations when selecting pinhole size are resolution and signal intensity (smaller pinhole size = fewer photons = more noisy data). Please refer to the appropriate sections on diffraction limited resolution and experimentally determined spatial resolution for further discussion of these topics.

Example spectra from a range of pinhole sizes using the narrowband and wideband detector

Figure [left]: Effect of pinhole size on an example spectrum of a salt crystal extracted from a mature gouda cheese

  • NARROWBAND detector

  • Transmission acquisition mode

  • 36× objective (NA = 0.5)

  • Diamond infrared window

  • 32 co-added scans per spectrum

  • 40kHz, 4cm-1 resolution

  • 5 spectra averaged

  • Spectra max-min normalised on band at 1100cm-1

Figure [right]: Effect of pinhole size on an example spectrum of a salt crystal extracted from a mature gouda cheese

  • WIDEBAND detector

  • Transmission acquisition mode

  • 36× objective (NA = 0.5)

  • Diamond infrared window

  • 256 co-added scans per spectrum*

  • 40kHz, 4cm-1 resolution

  • 3 spectra averaged

  • Spectra max-min normalised on band at 1100cm-1

*The wideband detector has ~10× less detectivity (sensitivity) compared with the narrowband detector, therefore more co-added scans are required to achieve similar signal-to-noise. Example spectra collected using 32 and 256 scans are shown HERE.

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