Advertisement
100% x 90
Two-Photon Absorption Calculator

Two-Photon Absorption Calculator

Calculate two-photon excitation rates and photon flux for laser-induced molecular absorption

Calculate Two-Photon Absorption

Cross-section in GM units (1 GM = 10⁻⁵⁰ cm⁴⋅s⋅ph⁻¹)

Average power of the laser beam

Wavelength of the laser light

Full width at half maximum of the focused beam (μm)

Duration of laser exposure

Two-Photon Absorption Results

18.66
Photon Flux (×10²⁴ ph/(cm²⋅s))
365.6
Excitations per Molecule
Very High Excitation
Excitation Level
4.41e+6
Intensity (W/cm²)
12.0
Beam Radius (μm)
1.48
Photon Energy (eV)

Formula: N = (1/2) × δ × φ² × τ

Beam radius: w = FWHM / (2√ln2) = 12.0 μm

Analysis: Intense two-photon absorption events - Very high efficiency

Common Laser Examples

Ti:Sapphire Laser

Standard two-photon microscopy laser

λ: 800 nm, P: 10 W, FWHM: 15 μm, δ: 200 GM

Nd:YAG Laser (doubled)

Frequency-doubled Nd:YAG

λ: 532 nm, P: 5 W, FWHM: 25 μm, δ: 150 GM

Er:Glass Laser

Near-infrared applications

λ: 1540 nm, P: 15 W, FWHM: 30 μm, δ: 300 GM

Femtosecond Ti:Sapphire

Ultrafast two-photon processes

λ: 840 nm, P: 20 W, FWHM: 10 μm, δ: 250 GM

Advertisement
100% x 280

TPA Cross-Section Values

Small Molecules

1-100 GM

Organic dyes, simple aromatics

Fluorescent Proteins

10-200 GM

GFP, RFP, and variants

Optimized Dyes

100-1000 GM

Specially designed TPA chromophores

Quantum Dots

1000-10000 GM

Semiconductor nanocrystals

Key Formulas

Excitations per molecule
N = (1/2) × δ × φ² × τ
Photon flux
φ = I × λ / (h × c)
Intensity
I = 2P / (π × w²)
Beam radius
w = FWHM / (2√ln2)

Where: δ = cross-section (GM), φ = photon flux (ph/cm²/s), τ = time (s), I = intensity (W/cm²), P = power (W)

TPA Applications

Two-photon microscopyImaging
Photodynamic therapyMedical
3D microfabricationManufacturing
Optical limitingProtection

Understanding Two-Photon Absorption

What is Two-Photon Absorption?

Two-photon absorption (TPA) is a nonlinear optical process where an atom or molecule simultaneously absorbs two photons to reach an excited state. The energy of both photons combined equals the energy difference between the ground and excited states.

Key Characteristics

  • Simultaneous absorption of two photons
  • Quadratic dependence on light intensity
  • Virtual intermediate state involvement
  • Confined to focal volume (3D localization)

Historical Background

The phenomenon was first theoretically predicted by Maria Göppert-Mayer in 1931 as part of her doctoral dissertation. It was experimentally verified by Kaiser and Garrett in 1963 using a ruby laser, confirming the quadratic intensity dependence.

Mathematical Framework

En - E0 = 2hc/λ

N = (1/2) × δ × φ² × τ

φ = Iλ/(hc)

Parameters

  • δ: Two-photon absorption cross-section (GM units)
  • φ: Photon flux at beam center (ph/cm²/s)
  • τ: Exposure time (s)
  • I: Laser intensity (W/cm²)
  • λ: Wavelength (m)
  • N: Number of excitations per molecule

Note: The GM unit honors Maria Göppert-Mayer. 1 GM = 10⁻⁵⁰ cm⁴⋅s⋅photon⁻¹

Applications and Advantages

Two-Photon Microscopy

Deep tissue imaging with reduced photobleaching and improved 3D resolution due to nonlinear excitation.

Photodynamic Therapy

Precise spatial control of therapeutic activation, minimizing damage to surrounding healthy tissue.

3D Microfabrication

Sub-diffraction-limited manufacturing through precise two-photon polymerization processes.

Advertisement
100% x 250