Half-value layer

Last revised by Kanchanok Prasittimet on 15 Mar 2025

Half-value layer (HVL) is the thickness of a material required to reduce the air kerma of an X-ray or gamma-ray beam to half its original value. HVL is most accurately measured under narrow-beam geometry, as broad-beam setups allow scatter to reach the detector, leading to an underestimation of attenuation unless corrected.

Monoenergetic beams
For monoenergetic beams HVL is directly related to linear attenuation coefficient (µ):
HVL = 0.693 / μ.

This formula can be derived from the Beer-Lambert Law:
Ix = I0 e-μ x

To find HVL, set x = HVL and Ix = 0.5 I0

  • 0.5 I0 = I0 e-μ HVL

  • 0.5 = e-μ HVL

  • ln(0.5) = -μ HVL

  • -0.693 = -μ HVL

  • HVL = 0.693 / μ

Polyenergetic beams
HVL for polyenergetic beams is determined experimentally rather than through a simple formula. The attenuation curve is measured by passing the X-ray beam through increasing thicknesses of material, plotting intensity vs. thickness, and finding the point where intensity drops to 50%.

  • HVL is particularly useful for characterizing polyenergetic X-ray beams (such as those used in diagnostic radiology), where individual linear attenuation coefficients (μ) vary with energy. Unlike linear and mass attenuation coefficients, which are strictly energy-dependent and ideal for monoenergetic beams, HVL provides a practical summary of a beam’s overall penetrability.

  • HVL serves as a surrogate measure of beam quality or X-ray spectrum penetrability. A lower HVL suggests a beam with a lower mean photon energy and greater attenuation per unit thickness. HVL is conventionally measured in millimeters of aluminum for diagnostic X-rays.

As an X-ray beam passes through a filter or tissue, beam hardening occurs: lower-energy photons are preferentially absorbed via the photoelectric effect, increasing the average energy of the remaining photons. As a result, each subsequent HVL is larger than the first (1st HVL < 2nd HVL < 3rd HVL), since higher-energy photons require thicker material to be attenuated by half.

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