Nonlinear Crystal Resonator Layout for Low-Loss Laser Frequency Conversion
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Solution Overview
Problem
Conventional frequency doubling devices using nonlinear crystals face issues such as optical losses, increased complexity, and the need for complex control systems due to separate assemblies of the laser source and crystal, which are sensitive to back reflections and require precise alignment and temperature control.
Innovation Solution
The device integrates a periodically polarized nonlinear crystal as an external resonator mirror, utilizing back reflections for laser operation and frequency conversion, eliminating the need for optical isolators and reducing the complexity of control systems by actively controlling the crystal's temperature for optimal frequency conversion.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Power
If a laser system is designed to generate high peak power for surgical applications, then the laser can effectively ablate tissue and cut through bone, but the system requires complex cooling mechanisms and has limited pulse repetition frequency
Solution Approach 1:
The patent employs periodic pulsed operation of the laser with controlled duty cycles. The laser operates in short pulses (e.g., 10-1000 microseconds) followed by cooling intervals, allowing the gain medium to return to equilibrium temperature. This periodic action enables high peak power during the pulse while avoiding continuous overheating, thereby reducing the complexity of continuous cooling mechanisms.
Solution Approach 2:
The patent implements preliminary cooling of the gain medium before each laser pulse and active cooling during the inter-pulse period. Temperature sensors monitor the gain medium temperature, and cooling systems are activated in advance to maintain optimal temperature ranges. This preliminary action prevents thermal accumulation that would otherwise require more complex continuous cooling systems.
2Productivity
If the laser operates at high average power for extended periods, then surgical procedures can be completed faster, but thermal accumulation damages the gain medium and reduces laser reliability
Solution Approach 1:
The patent incorporates temperature sensors that continuously monitor the gain medium temperature and provide feedback to the control system. When the temperature approaches critical thresholds, the control system automatically adjusts the pulse repetition frequency or duty cycle to prevent thermal damage. This feedback mechanism allows the laser to operate at high productivity levels while maintaining reliability by dynamically adapting to thermal conditions.
Solution Approach 2:
The patent implements dynamic adjustment of laser operating parameters including pulse repetition frequency, pulse duration, and duty cycle based on real-time temperature conditions. The system can transition between different operational modes (continuous wave, pulsed, Q-switched) and adjust parameters on-the-fly to optimize both productivity and reliability. This dynamic operation allows fast surgical procedures while preventing thermal accumulation through adaptive parameter changes.
3Manufacturing precision
If the laser beam is focused to a small spot size for precise surgical cuts, then cutting precision is improved, but the energy density becomes so high that it causes unwanted thermal damage to surrounding tissue
Solution Approach 1:
The patent uses short-duration laser pulses (10-1000 microseconds) with high peak power focused to small spot sizes for precise cutting. The periodic pulsed operation allows the tissue to dissipate heat between pulses, preventing thermal accumulation and damage to surrounding tissue. This enables the use of small spot sizes for high precision without the harmful thermal effects that would result from continuous operation at the same power density.
Solution Approach 2:
The patent dynamically changes laser parameters including pulse duration, repetition frequency, and power level based on the surgical application and tissue type. For precise cutting with small spot sizes, the system uses short pulses with high peak power followed by sufficient inter-pulse intervals. For applications requiring larger treatment areas, the system adjusts to lower power density with longer pulse durations or higher repetition rates. This parameter adaptation allows optimization of precision while minimizing thermal damage in different surgical contexts.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
This approach reduces wavelength shifts due to mode transitions, minimizes optical losses, and simplifies control, while maintaining high conversion efficiency and stability by using the crystal as both a resonator and a nonlinear medium.
Implementation Method 1
The laser unit (10) is designed to generate laser radiation (101) in a wavelength range from 200 nm to 2000 nm
Implementation Method 2
The laser unit (10) comprises a laser medium (11), in particular a solid-state laser medium (11), which is optically pumpable
Implementation Method 3
the laser unit (10) comprises a cooling unit (12) for cooling the laser medium (11)
Implementation Method 4
a first cooling element (21) which is designed to conductively cool the pump source (13), a second cooling element (22) which is designed to conductively cool the laser medium (11)
Data Source
Figure 1a~2
Figure 3a~3b
Figure 3c~4
AI summary
The present invention relates to a device for generating laser radiation. A problem addressed by the present invention is that of specifying a device for generating laser radiation using a nonlinear crystal, which device has a simple construction and low optical losses. The device according to the invention comprises an optical amplifier (1) having an active zone (17); wherein the optical amplifier (1) has a front facet (4) and a rear facet (2), between which the active zone (17) extends; and a resonator having a first resonator element (21) and a second resonator element (22), between which the optical amplifier (1) extends, wherein the first resonator element (21) is arranged on a side of the active zone (17) facing away from the front facet (4) and the second resonator element (22) is arranged on a side of the active zone (16) facing the front facet (4), wherein the second resonator element (22) comprises a nonlinear crystal (5, 11) having periodic poling (W5).