Filtered Back-Projection
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Filtered back-projection (FBP) is the standard algorithm for reconstructing images in computed tomography (CT). It implements the inverse Radon transform.
The Problem with Simple Back-Projection
Naive back-projection (smearing each projection back across the image) produces a blurred result. This blur has a $1/r$ characteristic — the point spread function of unfiltered back-projection.
The Ramp Filter
The solution is to filter each projection before back-projecting. The required filter has frequency response:
$$ H(\nu) = |\nu| $$This is called the ramp filter because its magnitude increases linearly with frequency.
Why a Ramp?
The projection-slice theorem fills Fourier space along radial lines. Near the origin, samples are densely packed; far from the origin, they’re sparse. The ramp filter compensates for this non-uniform sampling density.
Algorithm
- Acquire projections $p_\theta(s)$ at angles $\theta \in [0, \pi)$
- Filter each projection:
where $h(s) = \mathcal{F}^{-1}\{|\nu|\}$ 3. Back-project the filtered projections:
$$ f(x,y) = \int_0^\pi q_\theta(x\cos\theta + y\sin\theta) \, d\theta $$Practical Considerations
Windowing
The pure ramp filter amplifies high-frequency noise. Practical implementations multiply by a window function:
- Ram-Lak: $|\nu|$ (no windowing)
- Shepp-Logan: $|\nu| \cdot \text{sinc}(\nu/2\nu_{max})$
- Hamming: $|\nu| \cdot (0.54 + 0.46\cos(\pi\nu/\nu_{max}))$
Discrete Implementation
In practice:
- Projections are sampled discretely
- FFT is used for filtering
- Back-projection uses interpolation