Patent Grant
11139631
Ultrafast lasers are utilized in a wide variety of fields. Most recently they have found uses in ophthalmic procedures and processing of materials which, historically, have been difficult to cut. As a result, lasers with increasingly high pulse energies and superior beam quality are necessary.
In order to amplify ultrafast pulses a process known as chirped pulse amplification is typically utilized. This process requires that the pulsewidth of a seed laser be temporally stretched before being injected into a laser amplifier and then recompressed once amplification has been accomplished.
Conventionally, the stretching of a laser pulse is accomplished through the use of reflective gratings in an optical setup commonly referred to as a Stretcher. Unfortunately, Stretchers are inherently lossy and the means by which they chirp the pulse can cause distortion of the laser beam. In order to avoid these losses and beam distortion we have designed, and built, a novel Yb:KYW regenerative amplifier for chirped pulse amplification of femtosecond laser pulses without a conventional Stretcher. Instead, our design utilizes positive dispersion mirrors within the amplifier cavity to elongate the laser pulse with each round trip through the cavity. This greatly simplifies alignment and maintains beam quality while dropping peak powers in the laser cavity to levels usually achieved through the use of a conventional stretcher.
Conventional ultrafast laser systems are composed of a laser oscillator, stretcher, pulse-picker, laser amplifier, and an optical pulse compressor. Our design eliminates the need for a stretcher through the use of positive GDD intracavity mirrors and a pre-chirped femtosecond oscillator. The amplified laser pulse is then compressed using a single transmissive grating which maintains beam quality.
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
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 then compressing by several passes through a single, conventional, transmission grating our beam profile is dependent solely upon our laser amplifier cavity design. The design of which delivers a highly symmetric beam with a mode quality (M2) value less than 1.3 as shown in
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).
Finally, as a result of our novel design the laser can operate over a large range of environmental conditions and use models (see Table 2 below, which provides laser specifications of novel ultrafast laser system).
This application claims priority from U.S. Provisional Application No. 62/841,750, filed May 1, 2019, the contents of which are hereby incorporated by reference herein.
| Number | Name | Date | Kind |
|---|---|---|---|
| 20100085994 | Resan | Apr 2010 | A1 |
| 20110206070 | Karavitis | Aug 2011 | A1 |
| 20110206071 | Karavitis | Aug 2011 | A1 |
| Number | Date | Country | |
|---|---|---|---|
| 20200366046 A1 | Nov 2020 | US |
| Number | Date | Country | |
|---|---|---|---|
| 62841750 | May 2019 | US |
