Bethe-Bloch Energy Loss Calculator

Find the mean ionization energy loss (dE/dx) of a heavy charged particle through matter using the PDG Bethe-Bloch formula.

📉 Bethe-Bloch Energy Loss Calculator
MeV/c2
e
betagamma (momentum / mass c)
0.1100
g/mol
eV
g/cm3
Mass stopping power (dE/dx)
Linear stopping power
β used
γ used
Step-by-step working

📉 What is the Bethe-Bloch Energy Loss Calculator?

This Bethe-Bloch energy loss calculator computes the mean ionization energy loss, or stopping power, of a fast heavy charged particle passing through matter, using the PDG's standard Bethe-Bloch formula. It reports both mass stopping power (MeV cm2/g), which is independent of material density, and linear stopping power (MeV/cm) in the chosen absorber.

Physicists use this calculation constantly in detector design: tracking detectors like silicon strip trackers, time projection chambers, and scintillators all rely on ionization energy loss to register a charged particle's passage, and dE/dx measurements are routinely used to help identify particle species by mass. Radiation shielding and dosimetry calculations start from the same physics.

A common point of confusion is the "minimum-ionizing particle" (MIP): this refers to a particle whose betagamma sits near the minimum of the dE/dx curve, roughly betagamma of 3 to 4, not a particle that ionizes weakly in some absolute sense. Cosmic-ray muons passing through detectors at sea level are frequently close to minimum-ionizing.

This calculator omits the density-effect correction that flattens the relativistic rise at very high betagamma in dense media, since that correction needs material-specific Sternheimer parameters not available for arbitrary custom materials. It is intended as an educational tool for understanding the shape and scale of the Bethe-Bloch curve, not a substitute for a full PDG stopping-power table.

📐 Formula

−dE/dx  =  K z² (Z/A) (1/β²) [0.5 ln(2mec²β²γ²Tmax/I²) − β²]
K = 0.307075 MeV mol-1 cm² (PDG constant)
z = incident particle charge, Z, A = absorber atomic number and mass
β, γ = incident particle speed and Lorentz factor, from βγ = p/(Mc)
Tmax = (2mec²β²γ²) / (1 + 2γ(mec²/M) + (mec²/M)²), the maximum single-collision energy transfer
I = mean excitation energy of the absorber, in eV
Example: a minimum-ionizing muon (βγ=3.5) in copper gives dE/dx ≈ 1.459 MeV cm2/g.

📖 How to Use This Calculator

Steps

1
Choose the incident particle and charge.
2
Set betagamma.
3
Choose the absorber material.
4
Read the stopping power.

💡 Example Calculations

Example 1 - Minimum-ionizing muon in copper

1
Muon (M=105.658 MeV/c2), z=1, betagamma=3.5, absorber = copper (Z=29, A=63.546, I=322 eV, density=8.96 g/cm3)
2
gamma = 3.640055, beta = 0.961524, Tmax = 12.093393 MeV
3
dE/dx = 1.459144 MeV cm2/g, linear = 13.073928 MeV/cm
dE/dx = 1.459144 MeV cm2/g (13.073928 MeV/cm)
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Example 2 - Fast proton in lead

1
Proton (M=938.272 MeV/c2), z=1, betagamma=10, absorber = lead (Z=82, A=207.2, I=823 eV, density=11.35 g/cm3)
2
gamma = 10.049876, beta = 0.995037, Tmax = 101.093127 MeV
3
dE/dx = 1.317496 MeV cm2/g, linear = 14.953574 MeV/cm
dE/dx = 1.317496 MeV cm2/g (14.953574 MeV/cm)
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Example 3 - Slow charged pion in silicon

1
Charged pion (M=139.570 MeV/c2), z=1, betagamma=1.0, absorber = silicon (Z=14, A=28.0855, I=173 eV, density=2.329 g/cm3)
2
gamma = 1.414214, beta = 0.707107, Tmax = 1.011510 MeV
3
dE/dx = 2.503866 MeV cm2/g, linear = 5.831503 MeV/cm, well above the minimum-ionizing value since betagamma=1 is left of the dip
dE/dx = 2.503866 MeV cm2/g (5.831503 MeV/cm)
Try this example →

❓ Frequently Asked Questions

What is the Bethe-Bloch formula?+
The Bethe-Bloch formula gives the mean rate of energy loss per unit path length (dE/dx) of a fast charged particle passing through matter, dominated by ionization and excitation of the absorber's atoms. It is the standard starting point for understanding how detectors measure particle energy loss.
What is a minimum-ionizing particle (MIP)?+
A minimum-ionizing particle is one whose betagamma sits near the minimum of the Bethe-Bloch curve, roughly betagamma 3 to 4, where dE/dx is at its lowest. Cosmic-ray muons passing through a detector are commonly close to minimum-ionizing, which is why MIP energy deposit is a standard detector calibration reference.
Why does dE/dx first fall and then rise with betagamma?+
At low betagamma, the 1/beta squared term dominates and dE/dx falls sharply as speed increases. Past the minimum, the relativistic logarithmic term takes over and dE/dx slowly rises again, an effect called the relativistic rise, before eventually flattening due to the density effect (not modeled by this simplified calculator).
Why does this calculator omit the density-effect correction?+
The full density-effect correction needs material-specific Sternheimer parameters that are not available for every material a user might enter. Omitting it keeps the tool simple and transparent for educational use, but it means results at very high betagamma (above roughly 20 to 30) will overestimate dE/dx compared to a full PDG table.
What does mass stopping power mean versus linear stopping power?+
Mass stopping power (MeV cm2/g) is dE/dx divided by density, so it can be compared across materials directly. Linear stopping power (MeV/cm) multiplies mass stopping power by the absorber's density, giving the actual energy lost per centimetre of path in that specific material.
What is Tmax in the Bethe-Bloch formula?+
Tmax is the maximum kinetic energy that can be transferred to a free electron in a single collision, computed from the incident particle's mass, betagamma, and the electron rest mass. It sets the upper limit of the energy-transfer spectrum used inside the logarithmic term.
What is the mean excitation energy I?+
The mean excitation energy I (in electron volts) is an empirical, material-specific parameter that summarizes the average atomic excitation and ionization energy of the absorber. Larger I generally means the material is harder to ionize per unit mass, lowering dE/dx slightly.
How does charge z affect energy loss?+
Energy loss scales as z squared, so a particle with charge 2e loses energy four times faster than a singly charged particle with the same betagamma passing through the same material. This calculator lets you set any integer charge.
Which particle presets does this calculator include?+
Muon (105.658 MeV/c2), charged pion (139.570 MeV/c2), kaon (493.677 MeV/c2), and proton (938.272 MeV/c2) are built in, or you can enter any custom rest mass in MeV/c2.
Which absorber materials does this calculator include?+
Silicon, aluminum, copper, lead, and liquid argon are built in with their standard PDG Z, A, mean excitation energy, and density values, or you can enter a custom material's Z, A, I, and density directly.

What is the Bethe-Bloch formula?

The Bethe-Bloch formula gives the mean rate of energy loss per unit path length (dE/dx) of a fast charged particle passing through matter, dominated by ionization and excitation of the absorber's atoms. It is the standard starting point for understanding how detectors measure particle energy loss.

What is a minimum-ionizing particle (MIP)?

A minimum-ionizing particle is one whose betagamma sits near the minimum of the Bethe-Bloch curve, roughly betagamma 3 to 4, where dE/dx is at its lowest. Cosmic-ray muons passing through a detector are commonly close to minimum-ionizing, which is why MIP energy deposit is a standard detector calibration reference.

Why does dE/dx first fall and then rise with betagamma?

At low betagamma, the 1/beta squared term dominates and dE/dx falls sharply as speed increases. Past the minimum, the relativistic logarithmic term takes over and dE/dx slowly rises again, an effect called the relativistic rise, before eventually flattening due to the density effect (not modeled by this simplified calculator).

Why does this calculator omit the density-effect correction?

The full density-effect correction needs material-specific Sternheimer parameters that are not available for every material a user might enter. Omitting it keeps the tool simple and transparent for educational use, but it means results at very high betagamma (above roughly 20 to 30) will overestimate dE/dx compared to a full PDG table.

What does mass stopping power mean versus linear stopping power?

Mass stopping power (MeV cm2/g) is dE/dx divided by density, so it can be compared across materials directly. Linear stopping power (MeV/cm) multiplies mass stopping power by the absorber's density, giving the actual energy lost per centimetre of path in that specific material.

What is Tmax in the Bethe-Bloch formula?

Tmax is the maximum kinetic energy that can be transferred to a free electron in a single collision, computed from the incident particle's mass, betagamma, and the electron rest mass. It sets the upper limit of the energy-transfer spectrum used inside the logarithmic term.

What is the mean excitation energy I?

The mean excitation energy I (in electron volts) is an empirical, material-specific parameter that summarizes the average atomic excitation and ionization energy of the absorber. Larger I generally means the material is harder to ionize per unit mass, lowering dE/dx slightly.

How does charge z affect energy loss?

Energy loss scales as z squared, so a particle with charge 2e loses energy four times faster than a singly charged particle with the same betagamma passing through the same material. This calculator lets you set any integer charge.

Which particle presets does this calculator include?

Muon (105.658 MeV/c2), charged pion (139.570 MeV/c2), kaon (493.677 MeV/c2), and proton (938.272 MeV/c2) are built in, or you can enter any custom rest mass in MeV/c2.

Which absorber materials does this calculator include?

Silicon, aluminum, copper, lead, and liquid argon are built in with their standard PDG Z, A, mean excitation energy, and density values, or you can enter a custom material's Z, A, I, and density directly.