Knowledge What is the function of an 810 nm semiconductor laser in photoepilation? Precision Tools for Hair Removal Research
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Tech Team · Belislaser

Updated 2 days ago

What is the function of an 810 nm semiconductor laser in photoepilation? Precision Tools for Hair Removal Research


The high-precision 810 nm semiconductor laser system functions as the primary thermal induction tool in ex vivo photoepilation experiments, designed to rigorously simulate clinical hair removal. By emitting a wavelength specifically optimized for selective absorption by melanin, the system targets the hair follicle structure without damaging surrounding tissues. Through the precise modulation of energy density and pulse width, researchers use this system to dictate the biological fate of the follicle, ranging from growth cycle alteration to complete tissue destruction.

The core function of this system is to translate electrical energy into targeted photothermal damage, utilizing the 810 nm wavelength to precisely heat melanin within the follicle. This controlled thermal effect is the mechanism that drives the follicle from the anagen growth phase into regression or induces coagulative necrosis.

The Mechanism of Action

Selective Photothermolysis

The fundamental principle behind this laser system is the selective absorption of light. The 810 nm wavelength is chosen specifically because it interacts strongly with melanin, the pigment found in hair follicles.

This specificity allows the laser to deliver energy directly to the target area while minimizing interaction with non-pigmented structures.

Localized Thermal Effects

Once the laser energy is absorbed by the melanin, it converts into heat. This creates a localized thermal effect strictly confined to the follicle area.

The system acts as a precise heating element, raising the temperature of the follicle to levels required to trigger biological changes.

Biological Outcomes on Hair Follicles

Inducing Phase Transition

At specific energy levels, the thermal stress generated by the laser forces the hair follicle to exit its current state. The system is used to induce a transition from the anagen phase (active growth) to the catagen phase (regression).

This allows researchers to study the mechanisms of hair growth cessation under controlled conditions.

Triggering Coagulative Necrosis

When higher energy parameters are applied, the system functions to destroy the tissue structure entirely. The intense heat causes coagulative necrosis, effectively killing the follicle cells.

This simulates the permanent hair removal endpoint desired in clinical dermatology.

Critical Experimental Parameters

Modulating Energy Density

The system allows for the variation of energy density (fluence) between 1.7 and 26.4 J/cm². This wide range enables researchers to escalate from mild thermal stress to destructive heating.

Controlling Pulse Width

Precision is further achieved by adjusting the pulse width, which ranges from 4 to 64 ms. Controlling the duration of the laser pulse is essential for managing how heat diffuses within the tissue.

Understanding the Trade-offs

Specificity vs. Collateral Effects

While the 810 nm wavelength is selective, the precision of the outcome depends entirely on the parameter settings.

Improper calibration of pulse width relative to the follicle's thermal relaxation time could lead to inefficient heating or unwanted thermal spread.

Biological Response Variability

The system provides a uniform output, but biological responses can vary. Achieving a specific outcome—such as phase transition rather than necrosis—requires tight control over the energy density.

Crossing the threshold from "signaling regression" to "causing death" happens within a specific window of thermal intensity.

Optimizing Laser Settings for Experimental Goals

To effectively utilize a high-precision 810 nm semiconductor laser system in your research, consider the following biological targets:

  • If your primary focus is studying growth cycle regulation: Utilize lower energy densities and controlled pulse widths to induce the transition from anagen to catagen without destroying the tissue.
  • If your primary focus is simulating permanent hair removal: Increase the energy density toward the 26.4 J/cm² upper limit to achieve immediate coagulative necrosis of the follicle.

Success in ex vivo photoepilation relies on the exact correlation between the configured laser parameters and the resulting thermal impact on the follicle structure.

Summary Table:

Feature Experimental Specification Biological Impact
Wavelength 810 nm Targeted melanin absorption with minimal tissue damage
Energy Density 1.7 – 26.4 J/cm² Controls shift from growth regression to tissue necrosis
Pulse Width 4 – 64 ms Manages thermal diffusion and localized heating effects
Core Mechanism Selective Photothermolysis Converts electrical energy into targeted thermal damage

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References

  1. Marijke A. A. van Vlimmeren, Natallia E. Uzunbajakava. Dose‐response of human follicles during laser‐based hair removal: <i>Ex vivo</i> photoepilation model with classification system embracing morphological and histological features. DOI: 10.1002/lsm.23085

This article is also based on technical information from Belislaser Knowledge Base .

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