Physica

03 Nuclear

Recovery coefficient

RC = C_measured / C_true. Partial-volume loss for lesions smaller than ~3× FWHM.

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Simulation

Recovery coefficient — Change the numbers; the scene follows.

Where it works

PET/CT

PET/CT

Patient / uptake

In the patient on the PET couch — activity concentration, SUV, and internal dose.

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Formula

RC=Cmeas/Ctrue\mathrm{RC}=C_{\mathrm{meas}}/C_{\mathrm{true}}

Variables

Results

  • RC

    Recovery coefficient

    0.5

  • 1/RC

    Correction multiplier

    2

Explanation

RC=Cmeas/Ctrue\mathrm{RC}=C_{\mathrm{meas}}/C_{\mathrm{true}}

What it means

A sphere smaller than the reconstructed PSF spills counts into the background (spill-out) and the measured SUV underestimates truth. Recovery coefficient vs diameter is the NEMA image-quality curve: RC ≈ 0.3 at 10 mm, ≈ 0.8 at 22 mm, ≈ 1 at 37 mm on a typical TOF PET. Partial-volume correction multiplies by 1/RC or deconvolves the PSF. This is a working relation in Nuclear medicine.

Where it is used

Clinically it sits on the PET/CT — Patient / uptake. In the patient on the PET couch — activity concentration, SUV, and internal dose. Nuclear-medicine relations sit in the hot lab, on the camera, and in the voxel: decay, SUV, TOF, and counting statistics. They decide whether an uptake is real or a clock error.

PET/CT · Open this machine

How to use it

Enter measured and true concentration (or SUV). Read RC and the correction multiplier. A 13 mm sphere, C_meas=4, C_true=8 → RC=0.5 → multiply SUV by 2. Change one input and watch the curve and the simulation follow.

Symbols

  • C_measMeasured concentration4
  • C_trueTrue concentration8

Worked example

A typical case from the default values: C_meas = 4 (Measured concentration); C_true = 8 (True concentration). Substituting into the relation gives RC = 0.5; 1/RC = 2. These are teaching numbers — align them with your machine.

Typical values give

  • RC = 0.5
  • 1/RC = 2

Where it comes from

The displayed formula is the working relation. RC = C_measured / C_true. Partial-volume loss for lesions smaller than ~3× FWHM. Usual reference: NEMA NU 2 / Soret. Derive it in the specialty lesson, then return here to pin the numbers.

Reference: NEMA NU 2 / Soret

Assumptions & limits

Hot sphere in cold (or uniform) background; spill-in from a hot background is the opposite problem. RC depends on reconstruction, filter, TOF, and the VOI rule (max vs mean vs 50% isocontour). Never apply a phantom RC blindly to a patient lesion of different shape.

Pitfalls

Activity is not counts. SUV needs the true injected activity, the residual, and the correct decay time — a clock off by 10 min on ¹⁸F is a several-percent error. Do not compare SUVs across reconstructions. Hot sphere in cold (or uniform) background; spill-in from a hot background is the opposite problem. RC depends on reconstruction, filter, TOF, and the VOI rule (max vs mean vs 50% isocontour). Never apply a phantom RC blindly to a patient lesion of different shape.

Keep this

Write the assay time next to every activity. Decay does the rest. Hot sphere in cold (or uniform) background; spill-in from a hot background is the opposite problem. RC depends on reconstruction, filter, TOF, and the VOI rule (max vs mean vs 50% isocontour). Never apply a phantom RC blindly to a patient lesion of different shape.

In this specialty

Nuclear medicine