Multi-stage MOPA with first-pulse suppression

• US 8,995,052 B1
• Filed: 09/09/2013
• Issued: 03/31/2015
• Est. Priority Date: 09/09/2013
• Status: Active Grant

• Current Assignee: Coherent Kaiserslautern GmbH (Coherent Corp.)
• Original Assignee: Coherent Kaiserslautern GmbH (Coherent Corp.)
• Inventors: Knappe, Ralf, Weis, Alexander, Seifert, Albert
• Primary Examiner(s): Diacou, Ari M
• Application Number:
  US14/022,129
• Publication Number:
  US 20150070753A1
• Time in Patent Office: 568 Days
• Field of Search: 359/333, 359/346, 359/349, 359/341.3, 372/70, 372/92
• US Class Current: 359/341.3
• CPC Class Codes: H01S 3/0085 Modulating the output, i.e. the laser beam is modulated outside the laser cavity
• CPC Class Codes: H01S 3/08072 Thermal lensing or thermally induced birefringence; Compensation thereof
• CPC Class Codes: H01S 3/0813 Configuration of resonator
• CPC Class Codes: H01S 3/091 using optical pumping
• CPC Class Codes: H01S 3/09415 the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
• CPC Class Codes: H01S 3/10015 by monitoring or controlling, e.g. attenuating, the input signal
• CPC Class Codes: H01S 3/10046 Pulse repetition rate control H01S3/11 takes precedence
• CPC Class Codes: H01S 3/1106 Mode locking
• CPC Class Codes: H01S 3/2308 Amplifier arrangements, e.g. MOPA
• CPC Class Codes: H01S 3/2316 Cascaded amplifiers
• CPC Class Codes: H01S 3/2341 Four pass amplifiers
• CPC Class Codes: H01S 5/041 Optical pumping

Abstract

A solid-state MOPA includes a mode-locked laser delivering a train of pulses. The pulses are input to a fast E-O shutter, including polarization-rotating elements, polarizing beam-splitters, and a Pockels cell that can be driven alternatively by high voltage (HV) pulses of fixed long and short durations. A multi-pass amplifier follows the E-O shutter. The E-O shutter selects every Nth pulse from the input train and delivers the selected pulses to the multi-pass amplifier. The multi-pass amplifier returns amplified seed-pulses to the E-O shutter. The shutter rejects or transmits the amplified pulses depending on whether the HV-pulse duration is respectively short or long. Transmitted amplified pulses are delivered to a transient amplifier configured for separately suppressing first-pulse over-amplification and residual pulse leakage.

Claims

1. Optical apparatus comprising:

a mode-locked laser delivering a first train of pulses at a first pulse-repetition frequency (PRF);

at least one transient optical amplifier having a solid-state gain-element optically pumped by radiation output from a diode-laser array for energizing the gain-element, the diode laser array having selectively variable output power;

a multi-pass optical amplifier;

an optical shutter arranged to select pulses from the first train thereof to provide a second train of pulses at a second PRF less than the first PRF, provide the selected pulses to the multi-pass amplifier to be amplified, receive a corresponding train of amplified pulses from the multi-pass amplifier and selectively transmit a plurality of pulses from the train of amplified pulses to the transient optical amplifier for further amplification, with pulses in the plurality thereof having about equal amplitude;

wherein the diode-laser array power is set at a first level when amplified pulses are not being received to maintain about constant thermal lensing in the gain-element, set at a second level lower than the first level for a predetermined first time period in response to the plurality of pulses being selected for depleting stored energy in the gain-element, and set to a third level higher than the first level for a second time period prior to the arrival of the plurality of amplified pulses from the optical shutter to restore stored energy in the gain-element, with the first and second time periods being selected such that, when further amplified, all further-amplified pulses in the plurality thereof have about equal amplitude; and

wherein the transient amplifier has a laser resonator including the gain-element, the laser-resonator generating CW radiation in response to the first-level pumping when amplified pulses are not being further amplified.

2. The apparatus of claim 1, wherein the optical shutter includes a Pockels cell operable alternatively by a first high-voltage signal of a first duration or a second high-voltage signal of a second duration longer than the first duration, and wherein the Pockels cell is operated by either the first or second high-voltage signal to select pulses from the first train thereof to provide the second train of pulses at the second PRF to the multi-pass amplifier, and operated by the second high voltage signal to transmit the plurality of pulses from the train of amplified pulses to the transient optical amplifier for further amplification.

3. The apparatus of claim 2, wherein the optical shutter includes a first polarizing beam-splitter in the path of the first train of pulses to the Pockels cell and a second polarizing beam-splitter in the path of the first train of pulses from the Pockels cell to the multi-pass amplifier.

4. The apparatus of claim 3, wherein if when the Pockels cell is not operated by any of the first and second high-voltage signals pulses from the first train thereof are transmitted by the second polarizing beam-splitter and not provided to the multi-pass amplifier.

5. The apparatus of claim 3, wherein when the Pockels cell is operated by any one of the first and second high-voltage signals, pulses from the first train thereof are reflected by the second polarizing beam-splitter and provided to the multi-pass amplifier.

6. The apparatus of claim 5, wherein when the Pockels cell is operated by the first high-voltage signal amplified pulses are reflected by the first polarizing beam splitter and not transmitted for the further amplification, and when the Pockels cell is operated by the second high-voltage signal amplified pulses are transmitted by the first polarizing beam-splitter to the transient amplifier for the further amplification.

7. The apparatus of claim 1, wherein the optical shutter includes a Pockels cell operable alternatively by a first high-voltage or a second high-voltage signal, with each signal having the same duration, but with second high voltage signal initiated later than the first signal by an amount less than the signal duration, and wherein the Pockels cell is operated by either the first or second high-voltage signal to select pulses from the first train thereof to provide the second train of pulses at the second PRF to the multi-pass amplifier, and operated by the second high voltage signal to transmit the plurality of pulses from the train of amplified pulses to the transient optical amplifier for further amplification.

8. The apparatus of claim 7, wherein the optical shutter includes a first polarizing beam-splitter in the path of the first train of pulses to the Pockels cell and a second polarizing beam-splitter in the path of the first train of pulses from the Pockels cell to the multi-pass amplifier.

9. The apparatus of claim 8, wherein if when the Pockels cell is not operated by any of the first and second high-voltage signals, pulses from the first train thereof are transmitted by the second polarizing beam-splitter and not provided to the multi-pass amplifier.

10. The apparatus of claim 8, wherein when the Pockels cell is operated by any one of the first and second high-voltage signals, pulses from the first train thereof are reflected by the second polarizing beam-splitter and provided to the multi-pass amplifier.

11. The apparatus of claim 10, wherein when the Pockels cell is operated by the first high-voltage signal amplified pulses are reflected by the first polarizing beam splitter and not transmitted for the further amplification, and when the Pockels cell is operated by the second high-voltage signal amplified pulses are transmitted by the first polarizing beam-splitter to the transient amplifier for the further amplification.

12. The apparatus of claim 1, wherein the optical shutter includes a Pockels cell operable alternatively by a first high-voltage signal of a first duration or a second high-voltage signal of a second duration longer than the first duration, and wherein the Pockels cell is operated by either the first or second high-voltage signal to select pulses from the first train thereof to provide the second train of pulses at the second PRF to the multi-pass amplifier, and operated by the first high voltage signal to transmit the plurality of pulses from the train of amplified pulses to the transient optical amplifier for further amplification.

13. The apparatus of claim 12, wherein the optical shutter includes a Faraday isolator, a half-wave plate, and first polarizing beam-splitter in the path of the first train of pulses to the Pockels cell, and a second polarizing beam-splitter in the path of the first train of pulses from the Pockels cell to the multi-pass amplifier.

14. The apparatus of claim 13, wherein if when the Pockels cell is not operated by any of the first and second high-voltage signals, pulses from the first train thereof are reflected by the second polarizing beam-splitter and not provided to the multi-pass amplifier.

15. The apparatus of claim 13, wherein when the Pockels cell is operated by any one of the first and second high-voltage signals, pulses from the first train thereof are transmitted by the second polarizing beam-splitter and provided to the multi-pass amplifier.

16. The apparatus of claim 15, wherein when the Pockels cell is operated by the second high-voltage signal amplified pulses are transmitted by the first polarizing beam-splitter through the half-wave plate to the Faraday isolator and directed by the Faraday isolator out of the optical shutter, and when the Pockels cell is operated by the first high-voltage signal amplified pulses are reflected by the first polarizing beam-splitter to the transient amplifier for the further amplification.