1030 nm diode-laser based light source delivering pulses with nanojoule energies and picosecond duration adjustable by mode locking or pulse gating operation

被引:2
作者
Klehr, A. [1 ]
Liero, A. [1 ]
Wenzel, H. [1 ]
Bugge, F. [1 ]
Brox, O. [1 ]
Fricke, J. [1 ]
Ressel, P. [1 ]
Knigge, A. [1 ]
Heinrich, W. [1 ]
Traenkle, G. [1 ]
机构
[1] Leibniz Inst Hochstfrequenztech Forsch Verbund Be, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, Germany
来源
NOVEL IN-PLANE SEMICONDUCTOR LASERS XVI | 2017年 / 10123卷
关键词
semiconductor laser; DBR laser; mode locking; high power optical pulse generation; pulse picking; pulse gating;
D O I
10.1117/12.2250093
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
A new compact 1030 nm picosecond light source which can be switched between pulse gating and mode locking operation is presented. It consists of a multi-section distributed Bragg reflector (DBR) laser, an ultrafast multisection optical gate and a flared power amplifier (PA), mounted together with high frequency electronics and optical elements on a 5x4 cm micro bench. The master oscillator (MO) is a 10 mm long ridge wave-guide (RW) laser consisting of 200 mu m long saturable absorber, 1500 mu m long gain, 8000 mu m long cavity, 200 mu m long DBR and 100 mu m long monitor sections. The 2 mm long optical gate consisting of several RW sections is monolithically integrated with the 4 mm long gain-guided tapered amplifier on a single chip. The light source can be switched between pulse gating and passive mode locking operation. For pulse gating all sections of the MO (except of the DBR and monitor sections) are forward biased and driven by a constant current. By injecting electrical pulses into one section of the optical gate the CW beam emitted by the MO is converted into a train of optical pulses with adjustable widths between 250 ps and 1000 ps. Peak powers of 20 W and spectral linewidths in the MHz range are achieved. Shorter pulses with widths between 4 ps and 15 ps and peak powers up to 50 W but larger spectral widths of about 300 pm are generated by mode locking where the saturable absorber section of the MO is reversed biased. The repetition rate of 4.2 GHz of the pulse train emitted by the MO can be reduced to values between 1 kHz and 100 MHz by utilizing the optical gate as pulse picker. The pulse-to-pulse distance can be controlled by an external trigger source.
引用
收藏
页数:11
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