Pulse slicer in laser systems

Patent metadata

Field	Value
Publication number	US-11228153-B2
Application number	US-201816121284-A
Country	US
Kind code	B2
Filing date	Sep 4, 2018
Priority date	Mar 21, 2016
Publication date	Jan 18, 2022
Grant date	Jan 18, 2022

Abstract

An apparatus (such as a laser-based system) and method for providing optical pulses in a broad range of pulse widths and pulse energies uses a pulse slicer which is configured to slice a predefined portion having a desired pulse width of each of the one or more output optical pulses from a laser oscillator, in which timings of a rising edge and a falling edge of each sliced optical pulse relative to a time instance of a maximum of the corresponding each of the one or more output optical pulses from the laser oscillator, are chosen at least to maximize amplification efficiency of the optical amplifier, which may be located after the pulse slicer, and to provide the one or more amplified output optical pulses each having the desired pulse energy and pulse width.

First claim

I claim:

1. A system comprising:
a laser oscillator having a lasing medium and a back reflection mirror;
an output mirror, configured to provide one or more output optical pulses;
a pulse forming element between the back reflection mirror and the output mirror, the pulse forming element configured to provide formation of the one or more output optical pulses;
a pulse slicer downstream of the laser oscillator and configured to slice a portion having a desired pulse width of each of the one or more output optical pulses;
an optical amplifier downstream of the pulse slicer and configured to amplify the sliced portion of each of the one or more output optical pulses to a desired pulse energy to provide one or more amplified output optical pulses;
wherein timings of a rising edge and a falling edge of each sliced optical pulse, relative to a time instance of a maximum of the corresponding each of the one or more output optical pulses, is chosen at least to maximize amplification efficiency of the optical amplifier and to provide the one or more amplified output optical pulses each having the desired pulse energy and pulse width;
wherein the pulse forming element is a Q-switch component;
wherein the Q-switch component is a single Pockels cell.

2. The system of claim 1 , wherein the pulse slicer comprises an input polarizer and an output polarizer which is crossed with the input polarizer to provide an optical isolation between the laser oscillator and the optical amplifier.

3. The system of claim 1 , wherein a range of pulse widths of the amplified output pulses is between 8 nanoseconds and 500 picoseconds.

4. The system of claim 1 , wherein the lasing medium comprises one of: a solid-state material or a gas lasing medium.

5. The system of claim 4 , wherein the solid-state material comprises a neodymium-doped yttrium aluminum garnet (Nd:YAG).

6. The system of claim 1 , wherein the lasing medium comprises a solid-state material pumped by an array of semiconductor lasers.

7. The system of claim 1 , wherein the lasing medium comprises a solid-state material pumped by a double flash lamp.

8. The system of claim 1 , wherein the single Pockels cell comprises a single crystal, a central terminal and two end terminals, and wherein the central and each end terminals form a Pockels cell switching element to implement the pulse slicer.

9. A system comprising:
a laser oscillator having a lasing medium and a back reflection mirror;
an output mirror, configured to provide one or more output optical pulses;
a pulse forming element between the back reflection mirror and the output mirror, the pulse forming element configured to provide formation of the one or more output optical pulses;
a pulse slicer downstream of the laser oscillator and configured to slice a portion having a desired pulse width of each of the one or more output optical pulses;
an optical amplifier downstream of the pulse slicer and configured to amplify the sliced portion of each of the one or more output optical pulses to a desired pulse energy to provide one or more amplified output optical pulses;
wherein timings of a rising edge and a falling edge of each sliced optical pulse, relative to a time instance of a maximum of the corresponding each of the one or more output optical pulses, is chosen at least to maximize amplification efficiency of the optical amplifier and to provide the one or more amplified output optical pulses each having the desired pulse energy and pulse width; and
wherein the Q-switch component is one of: a single Pockels cell, a dual Pockels cell, a mechanical shutter, an acoustic optic device, an electro-optic device, or a passive Q-switch having a storable absorber.

10. A system comprising:
a laser oscillator having a lasing medium and a back reflection mirror;
an output mirror, configured to provide one or more output optical pulses;
a pulse forming element between the back reflection mirror and the output mirror, the pulse forming element configured to provide formation of the one or more output optical pulses;
a pulse slicer downstream of the laser oscillator and configured to slice a portion having a desired pulse width of each of the one or more output optical pulses;
an optical amplifier downstream of the pulse slicer and configured to amplify the sliced portion of each of the one or more output optical pulses to a desired pulse energy to provide one or more amplified output optical pulses;
wherein timings of a rising edge and a falling edge of each sliced optical pulse, relative to a time instance of a maximum of the corresponding each of the one or more output optical pulses, is chosen at least to maximize amplification efficiency of the optical amplifier and to provide the one or more amplified output optical pulses each having the desired pulse energy and pulse width; and
wherein the pulse forming element is a dual Pockels cell.

11. The system of claim 10 , wherein the rising and falling edges of each sliced optical pulse may be provided by two separate crystals respectively.

12. The system of claim 11 , wherein the two separate crystals are arranged in series and are run by two different voltage drivers connected in parallel.

13. The system of claim 12 , wherein one of the two voltage drivers provide a half-wave voltage to one of the two separate crystals that rotates 90 degrees the polarization plane of the output optical pulse so that the pulse goes through a polarizer in the pulse slicer without loss and defines the rising edge of the output pulse.

14. The system of claim 13 , wherein the other of the two voltage drivers provides a half-wave voltage to other of the two separate crystals that further rotates 90 degrees the polarization plane of the optical output pulse, so that the output optical pulse would not go through the polarizer in the pulse slicer, thus defining the falling edge of the sliced pulse.

Assignees

• Lumenis Ltd
• Lumenis Be Ltd

Inventors

• Lee Jr John B

Classifications

• H01S2301/08

  Generation of pulses with special temporal shape or frequency spectrum · CPC title

• H01S3/2308

  Amplifier arrangements, e.g. MOPA · CPC title

• H01S3/1643

  YAG · CPC title

• H01S3/1611

  neodymium · CPC title

• H01S3/1306

  Stabilisation of the amplitude · CPC title