Dual Laser Fiber Launch System

Slides:



Advertisements
Similar presentations
PPLN Frequency- Doubling Project Diana Parno Hall A Parity Collaboration Meeting May 17, 2007.
Advertisements

IP Area Reconfiguration Conceptual Design Five Phases: 1.Transport (A) 2.Gas Chamber 3.Injection Chamber 4.Compressor 5.Transport (B) M. Litos July 24,
Bio-Rad Labs. Chromatic Aberration Sources and Measurement.
ILS and alignment revisited David Griffith, Voltaire Velazco University of Wollongong with very significant inputs from John Robinson (Lauder) Frank Hase.
Lab 1 Paraxial Optics Lab in 106A. Look at paraxial optics rules Use a bi-convex singlet at 1:1 conjugates Do it double pass so can see image Lateral.
Present status of the laser system for KAGRA Univ. of Tokyo Mio Lab. Photon Science Center SUZUKI, Ken-ichiro.
CHARA AO WFS Design JDM (+LS,MJI) 2012Sep06 v0.1 1.
R. Hui Photonics for bio-imaging and bio- sensing Rongqing Hui Dept. Electrical Engineering & Computer Science, The University of Kansas, Lawrence Kansas.
March 4, 2005 All rights reserved Torque – Angle in Slip Ring - Non-Contact Rotary Torque Sensor Installation Tips Foot mount torque sensor Driver Load.
Walking the Beam §Often a laser can work but the beam is not parallel to the bore. §This results in serious losses and low output power. §If left unchecked.
3. Image motion due to optical element motion
PALM-3000 P3K Stimulus Design Update Rick Burruss P3K Team Meeting #7 February 27, 2008.
G D Calibration of the LIGO Interferometer Using the Recoil of Photons Justice Bruursema Mentor: Daniel Sigg.
In practice, optical tweezers are very expensive, custom-built instruments. These instruments usually start with a commercial optical microscope.
A. Imaging sample: 1. Place sample on stage 2. Make sure sample does not interfere with C mirrors 3. Start “Sonic MyDVD” on both laser heating computers.
Example: What is the ratio of the irradiances at the central peak maximum to the first of the secondary maxima?
Calibration Bench for Fast Wire Scanners: Optical Design and Issues Student Meeting Jose Luis Sirvent.
Setup of laser tracker on DX side NOTE: X axis along M1s centers, towards SX Z axis along M1-M2 centers, towards M2.
Preliminary studies for Muon shield modification to accommodate LCLS II Alev Ibrahimov December, 2010 BSY.
Tweez 200si System Aresis Advanced Research Instrumentation Solutions.
Results Theory Abstract Evaluation of Scintillation Index and Intensity of Partially Coherent Laser Light MIDN 4/C Meredith L. Lipp and MIDN 4/C Kathryn.
Measurements with the KSTAR Beam Emission Spectroscopy diagnostic system Máté Lampert Wigner Research Centre for Physics Hungarian Academy of Sciences.
September 28, 2007LGS for SAM – PDR – Optics1 LGS for SAM Optical Alignment R.Tighe, A.Tokovinin. LGS for SAM Design Review September 2007, La Serena.
SAM PDR1 SAM LGS Mechanical Design A. Montane, A. Tokovinin, H. Ochoa SAM LGS Preliminary Design Review September 2007, La Serena.
Optical Tweezers Sarah Nichols March 17, Outline Motivations Operation Layout Successes and Difficulties Future Directions.
Joshua Smith December 2003 Detector Characterization of Dual-Recycled GEO600 Joshua Smith for the GEO600 team.
What’s already existing?What’s already existing? Laser system & impacts on Optics TransportLaser system & impacts on Optics Transport –Laser power –Focusing.
BMS 524: Lecture 3 Purdue University Cytometry Laboratories Lecture 4 The Principles of Confocal Microscopy: Components of the microscope. BMS “Introduction.
ATF2 meeting LAPP; David Urner 1 David Urner Paul Coe Matthew Warden Armin Reichold Geoffrey Rayner MPhys alumnus MONALISA Monitoring, Alignment.
MERLIN BEAMLINE RIXS refocusing mirror system D. Yegian
Freiburg 7/07/20001 laser beam lens CCD (long arm) screen + grid CCD (short arm) glass plates at  45° STAMP : Saclay Telescope for the Alignment of Many.
SAXS/WAXS Conversion for Beamline Engineering Review.
MICROSCOPE DESIGN. beam expander and objective Why do we need a beam expander? What facts about the laser do we need to know? How much expansion do we.
V. Sonnenschein, I. D. Moore, M. Reponen, S. Rothe, K.Wendt.
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
Power Launching and Coupling
Aerospace and Mechanical Engineering University of Arizona 1/21/2016 Microstructural Analysis of Soft Tissues Amanda E. Eskinazi Mentor: Dr. Jonathan Vande.
Current Balance MS&T Physics 2135, Lab E4.
Transmission test for waveguide Hideyuki Sakamoto Tracker Phone Meeting, 25 th May,2006 Contents Method Measured luminosity Results and next step.
Sensitivity of Virgo E. Tournefier (LAPP-CNRS) LSC-Virgo week May 23 rd,2007 LIGO-G Z.
Image: digikey.com 5 Image:
Date of download: 5/27/2016 Copyright © 2016 SPIE. All rights reserved. (a) Schematic of the light path. The galvo scanners are mounted above periscopes.
Date of download: 5/28/2016 Copyright © 2016 SPIE. All rights reserved. Confocal to multiphoton conversion. (a) Schematic of system adaptation. The near.
THE LASER QUALITY. ZAPHIRO, the new high range 2D laser machine by PRIMA INDUSTRIE, designed for very high productivity, quality, and flexibility. THE.
Sasha GilevichDrive Laser Meeting December Launch System Outline General Layout Incidence Angle Effect of the broad bandwidth.
Brenda Dingus Jan 2005 New Laser Calibration Status  New Laser vs Old Laser  Safety  Pond Data  Outrigger Data  How to Combine?
Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. Schematic optical layout of the instrument. Color box legend: Upright optical tweezers.
DECam Spectrophotometric Calibration DECam calibration workshop, TAMU April 20 th, 2009 Jean-Philippe Rheault, Texas A&M University.
Laser beam trajectory measurement with a CCD camera Georg Gassner.
Alignment Using a Beam Triangle
Performance of the Iris diaphragm laser alignment system of the SPring-8 C. Zhang JASRI / SPring-8 IWAA2014, October 13-17, 2014, IHEP, Beijing.
Lab 1 Paraxial Optics Lab in 106A.
Corey Stevenson, UW-Madison
Possible causes for SPS ZS2 misalignment
From: Coherent Anti-Stokes Raman Scattering (CARS) Microscopy: A Novel Technique for Imaging the Retina Invest. Ophthalmol. Vis. Sci ;54(5):
Fiber Laser Preamplifier
Thin-disk laser multi-pass amplifier
iKAGRA初期アラインメント手順 Initial Alignment Procedure for iKAGRA
Present status of the laser system for KAGRA
Spectral Flow Cytometry
RF modes for plasma processing
Measuring the Dynamics of Injected Boron Dust Particles in the Scrape-Off Layer Aaron Bader Dec 14, 2006 Ideas Forum 2007.
FiberBench Configurator
Sapun H. Parekh, Young Jong Lee, Khaled A. Aamer, Marcus T. Cicerone 
COMMUNICATION ENG. PROF. A.M.ALLAM
Design of Apparatus for colour matching.
Volume 104, Issue 1, Pages (January 2013)
New automation capability of the NDACC/TOLNet tropospheric
Polarizing Beamsplitter
A Low-cost, User-friendly, Smartphone-based
Presentation transcript:

Dual Laser Fiber Launch System I have build this laser fiber launch system using two Actoprobe lasers (405 and 532nm-20mW) and off the shelf components from ThorLabs. The System is compact, portable and easy to align and use.

Coupling Efficiency The coupling efficiency to SM fiber of this system is about 10%. I am using two mirrors for parallel alignment (decenter) and a fiber port PAF-X-18-A (to launch fiber) to control X-Y-Z offset and tilt. No beam expander is being used to overfill the back aperture of the port.

Alignment and Parts Lasers Upstream downstream IRIS and mirrors ND filters I first align the lasers by using upstream downstream mirrors along the alignment arm (upstream and down stream IRIS). Then I replace the alignment arm with port and adjust the X-Y-Z and tip on the fiber port. I also Installed two ND filter wheels to adjust the intensity.

Stability and Cost The system is built within the cage system so it has a good stiffness, the system does not get easily misaligned when moved from place to place. Right now it is blue and green but it is easy to add another channel to make it RGB. I am using off the shelf components so the cost of this system is around $1800 including the lasers. Fiber ports

By: Pranav Rathi (PhD) Confocal Raman Microscope