STRETCHER-FREE ULTRAFAST LASER SYSTEM EMPLOYING A PICOSECOND FIBER OSCILLATOR AND POSITIVELY CHIRPED INTRACAVITY MIRRORS FOR PULSE ELONGATION

Abstract

Disclosed is a laser system that incudes a chirped fiber oscillator, a laser amplifier, and a compressor. The laser amplifier includes a laser Faraday isolator. The fiber oscillator output is directly coupled to the laser Faraday isolator.

Claims

1. A laser system comprising: a chirped fiber oscillator; a laser amplifier comprising a laser Faraday isolator; and a compressor, wherein the fiber oscillator output is directly coupled to the laser Faraday isolator.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0007] FIG. 1 is a diagram of a simplified laser system design.

[0008] FIG. 2 depicts the components of a regenerative laser amplifier cavity.

[0009] FIG. 3 provides a dispersion curve of positive GDD mirrors utilized in laser cavity.

[0010] FIG. 4 provides a comparison of intracavity peak powers of pulses stretched by a Chirped Volume Bragg Grating (CVBG) and Positive GDD mirrors (Chirped Optics).

[0011] FIG. 5 provides a mode quality (M2) plot of the laser cavity.

DETAILED DESCRIPTION

[0012] FIG. 1 is a diagram of a simplified laser system design. As shown, the laser system includes a chirped fiber oscillator, a laser amplifier, and a compressor.

[0013] The fiber oscillator output is directly coupled to the laser Faraday isolator to avoid the possibility of misalignment as shown in FIG. 2, which depicts the components of a regenerative laser amplifier cavity.

[0014] As shown in FIG. 2, multiple positive Group Delay Dispersion (GDD) mirrors may be utilized in the cavity. The coating of the mirrors was custom designed for this application and each one provides 4000 fs.sup.2 of dispersion to the input laser pulse per reflection.

[0015] The seed laser beam reflects offs the positive GDD mirrors as it cycles through the laser amplifier cavity. During each cycle through the amplifier cavity, or round trip, the seed laser pulse is amplified. In order to reach the desired pulse energy, the seed laser must complete numerous round trips. The peak power of the laser pulses as it cycles through the cavity would damage the cavity optics if it was not temporally stretched. The positive GDD mirrors accomplish the stretching and keep the intracavity peak powers at levels comparable to lasers where a chirped volume Bragg grating (CVBG) is used for pulse stretching prior to amplification as shown in FIG. 4.

[0016] However, unlike a system utilizing a CVBG, the input and output beam profiles of our laser are not compromised by the stretching and compressing optics. Through the use of the positive GDD mirrors for stretching and compressing by several passes through a single, conventional, transmission grating our beam profile is dependent solely upon our laser amplifier cavity design. This design of delivers a highly symmetric beam with a mode quality (M2) value less than 1.3 as shown in FIG. 5.

[0017] In addition to superior beam quality the use of positive dispersion mirrors also allows for our laser to operate and dynamically switch repetition rate from single-shot to 1 MHz without compromising laser performance (see Table 1 below, which provides laser output energy at operating repetition rates).

TABLE-US-00001 Repetition Rate Max. Energy Peak Power (kHz) (J) (MW) 20* 150.0 300.0 40 75.0 150.0 60 50.0 100.0 80 37.5 75.0 100 30.0 60.0 200 15.0 30.0 300 10.0 20.0 400 7.5 15.0 500 6.0 12.0 500 5.0 10.0 700 4.3 8.6 800 3.8 7.5 900 3.3 6.7 1000 3.0 6.0

[0018] Finally, as a result of our novel design and incorporation of experience our compact design can operate over a large range of environmental conditions and repetition rates (see Table 2 below, which provides laser specifications of novel ultrafast laser system).

TABLE-US-00002 Wavelength (nm) 1030 (+/2) Average Power (W) 3 (Low Cost Model) Pulse Duration (fs) <500 Repetition Rate (kHz) SS-1000 Mode Quality (M2) <1.35 Pulse to Pulse Stability 1% over 10 minutes Pulse Contrast >20:1 Start Up Time (Warm) 2 minutes Operating Temperature 15 C.-40 C. Humidity 90% noncondensing Cooling Water (closed-loop) Power Requirements 110 V/15 A (50 Hz/60 Hz) Laser Head Dimensions <450 mm 350 mm 220 mm Weight (kg) <22