development of a high-power and stable laser for large ... · development of a high-power and...
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Development of a high-power and stable laser for Large-scale cryogenic
gravitational wave telescope
University of TokyoKohei Takeno
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
GW Detectors in Japan
TAMA300– RFPMI– 300-m baseline
Large-scale cryogenic gravitational wave telescope(LCGT)
– RFPMI (with RSE) – 3-km baseline– Cooled mirrors Talk by Uchiyama on Friday
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
LCGT
Target– Coalescence of binary neutron stars– Signal
Noise– Shot noise
×
+××≈ −2
2001102.2
[Hz]24
shotfh P
[W]100
)kHz1Hz100(@Hz/10 22 −≈ −h
Hz/
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Requirement
Light source for LCGT– Nd:YAG (λ = 1.064µm)– Output Power: 300W– Single longitudinal mode– Single transverse mode (M2 < 1.1)– Linearly polarized– Frequency noise– Relative intensity noise
Hz/Hz10 7−<Hz/10 8−<
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Strategy for a high power laser
Injection Locking Chain + MOPA
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Strategy for a high power laser
Injection Locking Chain + MOPA
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Strategy for a high power laser
Injection Locking Chain + MOPA
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
The key to a stable and high-power laser
Efficiency– Uniform pumping
Mode– Cavity design
Coupling Efficiency– Output coupler
Compensation of thermal effects– Thermal lens, thermal birefringence
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Overview of laser development
Two lasers for injection locking chain– First slave laser
30 W, TEM00 (Linear cavity)17 W, Linearly polarized (Ring cavity)Thermal birefringence compensation
– Second slave laser60 W, TEM00 , Linearly polarized (Linear cavity)Thermal birefringence compensation~40 W (Ring cavity)
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
First slave Laser (Ring cavity)
Current Status– Nd:YAG Rod (2-mm diameter, 63-mm length)– Total output power of 17 W– Thermal birefringence compensation– Transverse mode (M2=1.4 )– Linearly polarized
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Laser head
Manufactured by Cutting Edge Optronics– Nd:YAG Rod (2-mm diameter, 63-mm length)– 0.6% Nd3+ doped– LD pumping– Water cooling
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Thermal birefringence compensation
Rotate polarization
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Second slave Laser (Linear cavity)
Current status– Nd:YAG Rods (4-mm diameter, 70-mm length)– Output power: 60W (with one laser head)– Single transverse mode (M2=1.12 )– Linearly polarized– Relative intensity noise Hz100@ Hz/10 4−≈
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Laser head
Manufactured by Mitsubishi– Two Nd:YAG Rods
and a rotator– LD pumping– Diffusive Reflector– Water cooling
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Linear cavity
Convex mirrors (Curvature: 20cm)R=85% Output couplerThermal birefringence compensation
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Second slave Laser (Ring cavity)
Current status– Total output power: 39 W (Self-injection)
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Output Power
Maximum output power of 39 W (Self-injection)
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
Problems of the current design
AstigmatismIncomplete compensation of thermal effects
– Asymmetric beam mode at the Nd:YAG rods
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
How to improve?
Two-module cavity– Ring cavity with two laser modules
2003/07/105th Edoardo Amaldi ConferenceKohei Takeno
How to improve?
Two-module cavity– Cavity mode Simulation