SLIDE 1
1
Direct fibre excitation with a digital laser
SLIDE 2 2
Proof of principle
Mode source Mode transfer Mode detection
SLIDE 3
3
Digital laser resonator as the mode source
SLIDE 4 4
Digital laser in operation
CCD Monitor 2 PC 2 SLM Monitor 1 PC 1 Video signal SLM Driver Nd:YAG
time
SLIDE 5
5
SLIDE 6
6
Mode transfer - Standard step index fibre
SLIDE 7
7
Modal detection - Modal decomposition technique
SLIDE 8 8
We can determine the purity of the petals by azimuthal modal decomposition when using loss lines
1 2 3 4 5 6 0.0 0.1 0.2 0.3 0.4 0.5 |a
2|
Azimuthal, l
8petals-lines
l±4 97%
SLIDE 9 9
Generation of Linear Polarised (LP) fibre modes
- Digital Holograms: Generate Laguerre Gaussian (LG)
Modes from the digital laser
- LG modes approximation to Linearly Polarised (LP) modes
SLIDE 10 10
Injection and transmitted mode through the multimode fibre
- Injected modes into a multimode fibre
- Emitted modes through a multimode fibre
SLIDE 11
11
Modal power spectrum – LP01
Fibre input (Digital laser) Fibre output
SLIDE 12
12
Modal power spectrum – LP11
Fibre input (Digital laser) Fibre output
SLIDE 13
13
Modal power spectrum - LP21e
Fibre input (Digital laser) Fibre output
SLIDE 14
14
Modal power spectrum – LP21o
Fibre input (Digital laser) Fibre output
SLIDE 15 15
Control mode coupling of LP11e and LP11o
- Pre-calibration of the injected mode to achieve a desired outcome.
SLIDE 16 16
Conclusion
- Achieved to generate LP modes from a single source
and transmit these modes through an optical fibre with very high efficiency.
- Achieved to control cross talk between modes by
controlling the mode from the source.
- Next step will be to eliminate all telescope and optics
that cause aberration effects.
- Future work : Test and apply the technology to existing
fibre network cable.
SLIDE 17 17
Thank you
Dr Sandile Ngcobo (SNgcobo@csir.co.za)