City University of Hong Kong · FACULTY OF ELECTRICAL ENGINEERING

SYE6207 Chap.5 Transmission and Reflection Spectroscopy

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Chapter 5 of 7 · SYE6207

Transmission and Reflection Spectroscopy

Close the spectral energy budget

Transmission, absorption and reflection divide incident intensity. A fall in transmission therefore indicates stronger loss but does not identify absorption until reflection and scattering are handled.

Sample thickness, reference choice, geometry and roughness must remain visible in comparisons.

Read features in layers

An absorption onset can relate to a transition threshold, a peak to resonant coupling, a width to damping or disorder, and interference fringes to film optical path. Graph interpretation starts by naming axes and plotted quantity, reading a value at sensible precision, and only then calculating.

Beer-Lambert extraction is strongest when interface and scattering losses are corrected; otherwise the result is an effective attenuation.

Make reference and normalization explicit

A transmission trace may be divided by the incident beam or by a bare substrate, while reflection may be compared with a calibrated standard.

Those choices determine which lamp, detector, substrate and interface responses remain in the curve. Absorbance is a logarithmic transform of a referenced transmission value; it is not identical to the physical fraction absorbed. State the plotted quantity before assigning a peak or edge.

Thickness affects both exponential attenuation and the spacing of interference fringes.

Two samples of the same material can therefore show different raw transmission without different intrinsic optical constants. Compare normalized quantities and use the same baseline, feature definition and geometry. When transmission falls while reflection rises by a similar amount, absorption may be unchanged. When both fall, absorption or scattering becomes a stronger candidate and needs a channel-resolving measurement.

In this chapter

What this chapter covers

  • 01

    Transmission, absorption and reflection budget

  • 02

    Spectral references and geometry

  • 03

    Absorption edges

  • 04

    Peak position and width

  • 05

    Interference fringes

  • 06

    Attenuation and penetration depth

Worked example · free

Convert transmittance into penetration depth

Q [9 marks]. A 2.00 μm film has corrected internal transmittance 0.250. Find α and 1/α. These marks are not an official university marking scheme; AskSia assigned them for revision.
The incident channel divides into transmission, absorption and reflection.The incident channel divides into transmission, absorption and reflection. A fall in transmission supports stronger loss, but assigning that loss to absorption requires reflection and scattering to be accounted for.Account for every incident photon channelIncident I₀100%TART + A + R = 1Missing intensity is not automatically absorption unless reflection is known.
The incident channel divides into transmission, absorption and reflection. A fall in transmission supports stronger loss, but assigning that loss to absorption requires reflection and scattering to be accounted for.
  • 3Rearrange the exponential relation.
  • 3Calculate with length units.
  • 3Back-substitute and interpret.
α = −ln(0.250)/2.00 = 0.693 μm⁻¹ = 6.93 × 10⁵ m⁻¹. The penetration depth is 1.44 μm. Back-substitution gives exp(−1.386) = 0.250, so the result is internally consistent.
Sia tip — State whether reflection and scattering were corrected before calling α intrinsic absorption.
Glossary

Key terms

Transmittance
The fraction of incident intensity emerging through a sample.
Absorptance
The fraction of incident intensity converted within a sample.
Reflectance
The fraction of incident intensity returned from a surface or stack.
Absorption Edge
The spectral onset where a transition begins to absorb strongly.
Effective Attenuation
A measured intensity loss that may include absorption, reflection and scattering effects.
FAQ

Transmission and Reflection Spectroscopy FAQ

Can low transmission be called strong absorption?

Only after reflection, scattering and geometry are considered. A sample can transmit less because light reflects at an interface, scatters outside the detector, or travels through a greater thickness even when intrinsic absorption is unchanged.

How should I read a spectral graph in an exam?

Name the axis variable and units, identify the plotted quantity, read the feature at the precision supported by the scale, and write that value separately from the equation. Then interpret the calculated result physically.

Why compare minus log transmission divided by thickness?

For simple exponential attenuation, −ln(T)/x estimates α. Dividing by thickness allows samples of different thickness to be compared and prevents a thicker specimen from being misread as a changed material response.

What do interference fringes reveal?

Fringe spacing is controlled by optical thickness and measurement geometry. It can carry film-thickness information, but the material absorption and interface reflection shape the envelope, so a fringe minimum should not automatically be labelled an absorption peak.

Why should one baseline method be used across samples?

Changing the baseline or feature definition can move a fitted onset, centre or area even when the specimen is unchanged. A consistent analysis makes the reported difference traceable to the spectra rather than to the processing method.

Study strategy

Exam move

Build a spectral checklist: axes, quantity, reference, thickness, feature position, feature width and energy budget. Practise reading one value and writing it before any substitution. For calculations, keep the logarithm sign and length unit visible, then back-substitute to recover the printed transmission.

Compare paired transmission and reflection changes before naming absorption, and annotate whether scattering was captured. Use the same baseline and feature rule across every process split, then finish with the manufacturing action that the evidence supports. Take two spectra with different thickness and convert them to a common attenuation metric before comparing material response.

Mark every fringe, edge and peak with a competing explanation. Then describe which reference, reflection measurement or integrating collection geometry would test each alternative. Keep the raw and normalized curves side by side throughout the exercise.

Working through Transmission and Reflection Spectroscopy in SYE6207? Sia is AskSia’s AI Electrical Engineering tutor — ask any SYE6207 Transmission and Reflection Spectroscopy question and get a clear, step-by-step explanation grounded in how SYE6207 is taught and assessed. Read this chapter free, then take your hardest questions to Sia.

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