A Gage Block Measurement Process Using Single Wavelength Interferometry, Issues 152-155 |
From inside the book
Results 1-5 of 45
Page
Light returning to this assembly from dielectric surfaces in the interferometer is reversed in polarization direction by the 180 ° phase shift at reflection . Thus , light emerging from the isolator polarized in a clockwise direction ...
Light returning to this assembly from dielectric surfaces in the interferometer is reversed in polarization direction by the 180 ° phase shift at reflection . Thus , light emerging from the isolator polarized in a clockwise direction ...
Page
The direction of increasing fringe order is verified by pressing down on the eyepiece and observing fringe flow . A photograph is taken of the pattern . Block temperature , air temperature , barometric pressure , and humidity are ...
The direction of increasing fringe order is verified by pressing down on the eyepiece and observing fringe flow . A photograph is taken of the pattern . Block temperature , air temperature , barometric pressure , and humidity are ...
Page
A translation in the x , direction is generated by P. The unitary operator which represents a infinitesimal translation 2 , in the xy direction is L ( a , l ) = 1 – ia „ PM ( 2.6 ) Any finite transformation of the proper Lorentz group ...
A translation in the x , direction is generated by P. The unitary operator which represents a infinitesimal translation 2 , in the xy direction is L ( a , l ) = 1 – ia „ PM ( 2.6 ) Any finite transformation of the proper Lorentz group ...
Page
upon N : ( since L 12 is zero in the rest system ) , yields a state with momentum p along the z direction . The particular spatial rotation D ( 5 ) - ( 0,0 , - " ) = e - ioJ3e - 103 ze i $ J : e - in . ) ( 2.46 ) yields a state with ...
upon N : ( since L 12 is zero in the rest system ) , yields a state with momentum p along the z direction . The particular spatial rotation D ( 5 ) - ( 0,0 , - " ) = e - ioJ3e - 103 ze i $ J : e - in . ) ( 2.46 ) yields a state with ...
Page
We are limited to only one physically permissible irreducible representation of the two dimensional little group , a rotation in the plane perpendicular to the direction of propagation . The vector Pw = ( 0,0 , p , ip ) is unchanged by ...
We are limited to only one physically permissible irreducible representation of the two dimensional little group , a rotation in the plane perpendicular to the direction of propagation . The vector Pw = ( 0,0 , p , ip ) is unchanged by ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Other editions - View all
Common terms and phrases
Appendix atomic better broadcast Bureau called Classification Classified Lines clock commutation complete components Continued correct defined depend described determined device direction discussed distance earth effect electric electronic energy equations error example field frequency Intensity Wave Intensity Wave Wave interval invariance keep kind Lagrangian laser laws length air levels light limit Lines of Hf Lorentz mass means measurement mechanical MICHIGAN minutes motion moving nature number 0-C number Wave Observed and Classified obtained operator particles particular pendulum period physical position possible precise problem produce properties provides quantum mechanics radio reference relations representation resonator result rotation signal space speed spin standard star swings temperature theory tion transformation Tube Spark Tube Spark cm United universe vector watch Wave number
Bibliographic information
| Title | A Gage Block Measurement Process Using Single Wavelength Interferometry, Issues 152-155 A Gage Block Measurement Process Using Single Wavelength Interferometry, John S. Beers Volume 152 of NBS monograph |
| Author | John S. Beers |
| Publisher | U.S. Department of Commerce, National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 30 pages |
| Export Citation | BiBTeX EndNote RefMan |