Polarizing Beamsplitter

Slides:



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

Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford.
Fundamental of Optical Engineering Lecture 4.  Recall for the four Maxwell’s equation:
Light and Optics 4.1 Mirrors form images by reflecting light. 4.2
Currently: 3 year ( ) NSF-supported UF/IAP collaborative project "Methods and Instruments for High-Precision Characterization of LIGO Optical Components"
Spectroscopy 2: Electronic Transitions CHAPTER 14.
Optimizing power to the detectors To avoid dark-current errors and bit-noise errors in your data, all four PSD detectors need a high SUM reading. However.
Spectral Registration Relative Z Position (  m) Relative Intensity nm, 100X Plan Apo Lenses (1.4NA) Lens ALens B  m0.305  m
Multiple current exposure without mark detection Possible? Tolerance? Using only the 4 th lens: –1 st exposure: 0.1nA, 2 nd aperture (min. current) –2.
G R PHOTON ACTUATION R&D PROGRAM Michael Smith 8 Oct 02.
RF Synchronization, control and stability Takuya Natsui.
Basic optics lab skills Optics care, types of optics, alignment tricks.
What’s already existing?What’s already existing? Laser system & impacts on Optics TransportLaser system & impacts on Optics Transport –Laser power –Focusing.
Prof. Truman D. Black Optics Magnetism The eye
LPOL-cavity Introduction Tests at Orsay Optics (laser polarisation) Calorimeter DAQ Mechanics & installation at DESY  Norbert’s talk.
LPOL-cavity Mechanics Test cavity (pb of the gain)
The Hobby-Eberly Telescope Mirror Alignment Recovery System Marsha Wolf Graduate Student UT Astronomy Department.
Nicholas DiPreta.  Science of light  How light behaves and interacts with matter.
Practice Slides Unlabeled. Copyright © 2010 Pearson Education, Inc. Plate 1.
Photo-thermal Deflection Spectroscopy George Noid LIGO SURF Student.
GSFC Scanning Holographic Receivers for Air and Space Geary Schwemmer Meeting of the Working Group on Space-based Lidar Winds Sedona, Arizona January 27.
Today’s topic Alignment Polarization Mechanism 1.
Notes 2-5 OPTICAL TOOLS. Cameras: How do they work? Light from object travels through one or more convex lenses Lens focuses light Puts an image on film.
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.
Development of high-power and stable laser for gravitational wave detection Mio Laboratory Kohei Takeno.
PHYSICS 222 SI FINAL EXAM REVIEW WITH SI LEADER: ROSALIE.
Nonlinear generation of radiation by periodically poled LiTaO 3 crystals Single pass UV generation Intracavity Second Harmonic Generation HWP: half wave.
Adam J. Fleisher Philip J. Morgan David W. Pratt Department of Chemistry University of Pittsburgh Non-symmetric push-pull molecules in the gas phase: High.
Source Systematics PITA - type effects The importance of controlling the analyzer-axis –Two Pockels cells –Half-wave plate Position asymmetries –Lensing.
For off-center points on screen, Fresnel zones on aperture are displaced …harder to “integrate” mentally. When white and black areas are equal, light at.
Upgrade of the HSX Thomson Scattering System HSX TS upgrade requirement K. Zhai, F. S. B. Anderson, D. T. Anderson, C. Clark, HSX Plasma Laboratory, Univ.
Four Important Properties of Waves. 1.Reflection 2.Refraction 3.Diffraction 4.Interference.
Compressor Helium filled optional equivalent plane imaging laser beam dump hole in mirror for e-beam SSA and more.
An H- stripping laser using commercial, diode-pumped Nd:YAG amplifiers Russell Wilcox Laser Stripping Workshop, April 11, 2011.
0 Frequency Gain 1/R 1 R 2 R 3 0 Frequency Intensity Longitudinal modes of the cavity c/L G 0 ( ) Case of homogeneous broadening R2R2 R3R3 R1R1 G 0 ( )
Design for a New Optical Table of the Shintake Monitor Takashi Yamanaka The University of Tokyo ATF2 weekly meeting 2007/9/26.
Reflection of Light Reflection – The bouncing back of a particle or wave that strikes the boundary between two media. Law of Reflection – The angle of.
Date of download: 6/26/2016 Copyright © 2016 SPIE. All rights reserved. (a) Schematic of a photoporation system using a 405-nm diode laser: L (L1=50mm.
Laser Adaptive Optics for Advanced LIGO
Date of download: 7/9/2016 Copyright © 2016 SPIE. All rights reserved. (a) z-scan of the PTLS signal calculated in the mode-matched configuration for different.
Date of download: 7/10/2016 Copyright © 2016 SPIE. All rights reserved. Experimental diagram. A MgO:PPLN crystal is pumped and seeded by a Q-switch Nd:YAG.
Date of download: 9/19/2016 Copyright © 2016 SPIE. All rights reserved. Experimental design. Experimental setup showing laser beam delivery and dual imaging.
Peter Beyersdorf TAMA300 Results from the Stanford 10m all-reflective polarization Sagnac interferometer Peter Beyersdorf TAMA300.
Light.
Light and Optics 18.1 Mirrors form images by reflecting light. 18.2
Figure 2. Experimental scheme of the optical investigation: Nd-YAG laser –1, polarizer –2, interference mirror –3, total reflection mirror –4, standard.
Update on Virus Diagnosis and Detection Programs
Plasmonic lens for avalanche photodiode
Images in Lenses.
Dual Laser Fiber Launch System
TRIVIA QUESTION! How big (diameter of largest reflective mirror) is the LARGEST telescope in the world? (a) (b) (c ) (d) 34 feet (e) Telescope, Location,
Physics 202 Lecture 9 Geometric Optics.
Application of a Streak camera at PITZ
Trivia Question We have all seen ‘one way’ mirrors in use on TV police shows, in which of the following are one way mirrors NOT used? (a) The “Haunted.
Wave Interactions.
Mirror: A surface that reflects light in a regular (clear reflection)
Grade: Microscope.
Correcting Spherical Aberrations
Review calculation of Fresnel zones
Unit 3 – Light and Optics Topic 1 – Light – Visible form of energy. Radiation is the energy transfer method for light. Natural light source – comes from.
Calibrating for Light backscatter from fractal aggregates
Kansas Light Source Laser System J. R. Macdonald Laboratory
Optics Investigate the properties and behaviors of mechanical and electromagnetic waves. Explore and explain the nature of sound and light energy.
Chapter II The Propagation of Rays and Beams
Lidar Lidar!.
EM Wave & Polarization 林志民 Jim Jr-Min Lin
Fig. 1 Experimental setup.
Electro-Optical Modulation Nonlinear Optics Techniques Self Focussing
Fig. 2 The experimental setup.
Presentation transcript:

Polarizing Beamsplitter Cube Laser: CrystaLaser, Nd:YAG, 500 mW, Model # IRCL-500-1047 Half-Wave Plate: [ν] 9401, QWP0-1064-05-2-R10 Polarizing Beamsplitter Cube: [ν] 9411 Mirrors: 2 New Focus 5104, 1 New Focus 5104/Nd. YAG Lenses: ThorLabs, Inc. LMR1, Models BICC-25.4-51.8-UV-1064 and PLCX-25.4-64.4-UV-1064 Laser Mirror Half-Wave Plate Dump Lens Mirror Lens Mirror Iris Beam to Beamsplitter

Breadboard Beamsplitter Iris Integrating Sphere Iris Beamsplitter: Model LW-3-2037-UV Integrating Sphere: Labsphere Model 3P-LPM-020-SL Breadboard Beamsplitter Iris Integrating Sphere Iris Integrating Sphere

Feedback: Privacy Policy Feedback
Do Not Sell My Personal Information
About project: SlidePlayer Terms of Service

© 2025 SlidePlayer.com. Inc. All rights reserved.