Skip to content

Two-Photon Absorption Coefficient Calculator

Calculates the two-photon absorption coefficient (β) of a material from its wavelength, intensity, and pulse duration, using the formula β = K(Iτ)/λ².

Two-Photon Absorption Calculator

Calculates the two-photon absorption coefficient (β) from your laser parameters. Enter wavelength, peak intensity, and pulse duration to estimate how efficiently your material absorbs two photons simultaneously.

Formula Used

β = K × (I × τ) / λ²

Where:

  • β = Two-photon absorption coefficient (cm/GW)
  • K = Constant (1.5)
  • I = Intensity (W/cm²)
  • τ = Pulse duration (fs)
  • λ = Wavelength (nm)
nm

The wavelength of the incident light (400-1200 nm is typical)

W/cm²

The intensity of the incident light (typically 10¹⁰ to 10¹⁴ W/cm²)

fs

The duration of the light pulse (typically 10-1000 fs)

Result

Two-Photon Absorption Coefficient:
0.2344cm/GW

Calculation Details

The two-photon absorption coefficient is calculated as:

K = 1.5

I = 1.0000 × 10^+3 GW/cm²

τ = 100 fs

λ = 800 nm

β = 1.5 × (1.0000 × 10^+3 × 100) / 800² = 0.2344 cm/GW

Visualization

VisualizationMaterialAbsorptionWeak absorptionλ = 800 nmI = 1.0000 × 10^+3 GW/cm²β = 0.2344 cm/GW
Loading calculator...
📚

Documentation

Two-Photon Absorption Calculator

A two-photon absorption calculator estimates the two-photon absorption coefficient (β) of a material from three laser settings: wavelength, intensity, and pulse duration. Two-photon absorption is a process in which a molecule absorbs two photons of light at almost the same instant instead of one, and it only happens at high light intensity.

What Is Two-Photon Absorption?

In ordinary, single-photon absorption, a molecule absorbs one photon of light and jumps to a higher energy state. Two-photon absorption (TPA) is different: the molecule absorbs two photons within femtoseconds of each other and uses their combined energy to make the same jump. A femtosecond is one millionth of one billionth of a second.

This double absorption is rare. It only happens often enough to matter when light is extremely intense, because two photons must arrive almost simultaneously at the same molecule. Ordinary light, even sunlight, is far too weak. Lasers that pack their energy into short, intense pulses make TPA practical to observe and use.

The physicist Maria Göppert-Mayer predicted two-photon absorption in 1931, as part of her doctoral thesis. No light source of the time was intense enough to show it. The laser, invented in 1960, changed that. In 1961, researchers Wilhelm Kaiser and C. G. B. Garrett at Bell Labs observed two-photon absorption for the first time, using a ruby laser and a crystal doped with europium. Göppert-Mayer later shared the 1963 Nobel Prize in Physics for other work on nuclear structure.

Two-Photon Absorption Coefficient Formula

This calculator uses a simplified formula to estimate β:

β=K×I×τλ2\beta = K \times \frac{I \times \tau}{\lambda^2}

Where:

  • β — two-photon absorption coefficient, in cm/GW
  • K — a fixed constant, set to 1.5 in this calculator
  • I — intensity of the light, converted from W/cm² to GW/cm² (divide by 10⁹)
  • τ — pulse duration, in femtoseconds (fs)
  • λ — wavelength of the light, in nanometers (nm)

This is a simplified, order-of-magnitude model, not an exact physical formula. In a real material, β is usually treated as a fixed property that depends on the material's electronic structure and the light's wavelength, not on the intensity or pulse duration used in a particular experiment. This calculator's formula scales β with intensity and pulse duration instead, which makes it useful for comparing laser setups but not for predicting the true coefficient of a specific substance. Measuring β directly, or using a full quantum-mechanical model, is necessary for precise work.

How Each Variable Behaves

Wavelength (λ) appears squared in the denominator, so β falls as wavelength increases, following an inverse-square relationship. Going from 800 nm to 1000 nm, with intensity and pulse duration unchanged, multiplies β by (800/1000)² = 0.64 — a drop of 36%, not a drop of more than half. Most two-photon experiments use near-infrared light, roughly 700–1000 nm, because it penetrates biological tissue well. Titanium-sapphire (Ti:Sapphire) lasers, tunable around 800 nm, are the most common light source for this reason.

Intensity (I) must reach roughly 10¹⁰ to 10¹⁴ W/cm² for two-photon absorption to become significant. Sunlight at the earth's surface is only about 0.1 W/cm², far too weak. Reaching these intensities requires pulsed lasers, which concentrate their energy into brief bursts rather than spreading it out continuously.

Pulse duration (τ) typically ranges from 10 to 1000 femtoseconds in TPA experiments. Shorter pulses concentrate a given amount of energy into less time, producing higher peak intensity, but they also require more complex and costly laser equipment.

Worked Example

Using the formula with typical Ti:Sapphire laser parameters:

  • Wavelength: 800 nm
  • Intensity: 10¹² W/cm²
  • Pulse duration: 100 fs
  • K = 1.5

First, convert intensity to GW/cm²: 10¹² ÷ 10⁹ = 1000 GW/cm².

Then apply the formula:

β = 1.5 × (1000 × 100) ÷ 800² = 1.5 × 100,000 ÷ 640,000 ≈ 0.2344 cm/GW

Keeping intensity and pulse duration the same but changing the wavelength to 1000 nm gives:

β = 1.5 × (1000 × 100) ÷ 1000² = 150,000 ÷ 1,000,000 = 0.15 cm/GW

That is a 36% decrease, matching the inverse-square relationship described above.

Applications of Two-Photon Absorption

Two-photon microscopy. Because absorption only happens where the laser beam is tightly focused, this technique excites fluorescent molecules only at a single point deep inside a sample. It is widely used to image living brain tissue, since it avoids damaging or bleaching regions outside the focal point. Winfried Denk, James Strickler, and Watt Webb built the first two-photon microscope at Cornell University in 1990.

Photodynamic therapy. Near-infrared light reaches deeper into tissue than visible light. Two-photon excitation can activate a light-sensitive drug only at the laser's focal point, which helps target tumors while sparing surrounding healthy tissue.

3D optical data storage. Focusing a laser at different depths inside a block of material lets two-photon absorption mark data at that depth alone, offering higher storage density than surface-based formats like DVDs.

Two-photon microfabrication. Also called two-photon polymerization, this technique hardens light-sensitive resin only at the laser's focal point, producing 3D-printed structures with features smaller than 100 nanometers.

Optical limiting. Materials with a high β stay transparent at normal light levels but absorb strongly under an intense laser pulse. This property is used in protective eyewear and sensor filters against accidental laser exposure.

How to Calculate the Absorption Coefficient Manually

  1. Convert the light's intensity from W/cm² to GW/cm² by dividing by 10⁹.
  2. Multiply the result by the pulse duration in femtoseconds.
  3. Multiply by the constant K (1.5 in this simplified model).
  4. Divide by the wavelength in nanometers, squared.

The calculator performs these same four steps and flags any input that falls outside the typical experimental range: 400–1200 nm for wavelength, 10¹⁰–10¹⁴ W/cm² for intensity, and 10–1000 fs for pulse duration. Values outside these ranges still produce a result, but the simplified model becomes less reliable there.

Frequently Asked Questions

What is two-photon absorption? It is a process where a molecule absorbs two photons of light almost simultaneously, instead of one, to reach a higher energy state. It only becomes significant at very high light intensity.

What does the coefficient β measure? β measures how strongly a material undergoes two-photon absorption, in units of cm/GW. A higher β means the material absorbs more efficiently at a given intensity.

Why does two-photon absorption need such intense light? Two photons must strike a molecule within femtoseconds of each other, which is very unlikely at ordinary light levels. Pulsed lasers concentrate energy into short bursts to make this likely enough to observe and use.

How does wavelength affect β in this calculator? β falls as the square of the wavelength increases. Moving from 800 nm to 1000 nm, with other settings unchanged, reduces β by 36%, from about 0.2344 cm/GW to 0.15 cm/GW in the worked example above.

Can this formula be used for three-photon absorption? No. Three-photon absorption follows a different relationship, scaling with the cube of intensity rather than appearing linearly as in this simplified two-photon formula. It requires a separate model.

How accurate is the simplified formula? It gives a rough, order-of-magnitude estimate and is useful for comparing laser setups. It does not account for a material's specific electronic structure or resonances, so it should not be used to predict an exact coefficient for a real substance. Experimental measurement or quantum-mechanical modeling is needed for that.

References

  1. Göppert-Mayer, M. (1931). "Über Elementarakte mit zwei Quantensprüngen." Annalen der Physik, 401(3), 273–294.
  2. Kaiser, W., & Garrett, C. G. B. (1961). "Two-Photon Excitation in CaF₂: Eu²⁺." Physical Review Letters, 7(6), 229–231.
  3. Denk, W., Strickler, J. H., & Webb, W. W. (1990). "Two-photon laser scanning fluorescence microscopy." Science, 248(4951), 73–76.
  4. Rumi, M., & Perry, J. W. (2010). "Two-photon absorption: an overview of measurements and principles." Advances in Optics and Photonics, 2(4), 451–518.