Description, performance, and wavelengths of iodine stabilized lasers.

A description is given of lasers stabilized to components of the (129)I(2) spectrum in the region of the 633-nm laser lines for (3)He-(20)Ne and (3)He-(22)Ne. Relationships between operational characteristics such as power output, peak size, and peak width are shown, along with their relationships to some of the controllable parameters such as excitation level, iodine absorption, and iodine pressure. We found an iodine pressure broadening of about 13 MHz/Torr with a 2.6-MHz zero-pressure intercept. The frequency shift associated with iodine pressure is roughly 2 x 10(-9) nu/Torr to the red. Power broadening and power shifts are small, about a 10% increase in width and about 2 x 10(-11) nu variation in frequency for a fivefold to sixfold increase in power. These lasers exhibit a frequency stability for 10-sec sampling time of about 2 x 10(-12) nu and a resetability of about 1 x 10(-10) nu. The absolute vacuum wavelength for one iodine component has been measured against the (86)Kr standard-(3)He-(20)Ne:(129)I(2), kappa lambda = 632 991.2670 +/- 0.0009 pm. The wavelengths of several other iodine components have been determined by measuring the frequency difference between them and the (129)I(2), kappa component. Among these are (3)He-(20)Ne:(129)I(2), i lambda = 632 990.0742 +/- 0.0009 pm: and (3)He-(20)Ne:(127)I(2), i lambda = 632 991.3954 +/-0.0009 pm. These results were obtained using the Rowley-Hamon model for asymmetry in the krypton line and assume that the defined value for the standard is axssociated with the center of gravity of the line profile. The indicated uncertainties are statistical. No allowance has been included for imperfect realization of the krypton standard or for uncertainty in the asymmetry model.

[1]  K. M. Baird,et al.  Stability, Reproducibility, and Absolute Wavelength of a 633-nm He-Ne Laser Stabilized to an Iodine Hyperfine Component. , 1973, Applied optics.

[2]  P. W. Smith,et al.  Linewidth and Saturation Parameters for the 6328‐Å Transition in a He–Ne Laser , 1966 .

[3]  H. Greenstein.  Theory of a Gas Laser with Internal Absorption Cell , 1972 .

[4]  John L. Hall,et al.  Wavelength of the 3.39‐μm laser‐saturated absorption line of methane , 1973 .

[5]  K. M. Baird,et al.  Wavelength of the CH4 line at 3.39 μm , 1973 .

[6]  K. M. Baird,et al.  Primary Standard of Length , 1962 .

[7]  J. D. Knox,et al.  ABSORPTION PROFILES AND INVERTED LAMB DIPS OF I2 VAPOR AT 633 nm AS STUDIED WITH A He–Ne LASER , 1970 .

[8]  C. Bordé,et al.  Measurement of Methane Hyperfine Structure Using Laser Saturated Absorption , 1973 .

[9]  G. R. Hanes,et al.  IODINE HYPERFINE STRUCTURE OBSERVED IN SATURATED ABSORPTION AT 633 nm , 1969 .

[10]  M. Skolnick,et al.  SATURATED NEON ABSORPTION INSIDE A 6238‐Å LASER , 1967 .

[11]  J. W. Watson,et al.  Tests of the Peripheral Model for a Cluster Knockout Reaction , 1969 .

[12]  P. Bunker,et al.  Nuclear hyperfine structure in the electronic spectrum of 127I2 by saturated absorption spectroscopy, and comparison with theory , 1971 .

[13]  Yoh-Han Pao,et al.  HIGH‐RESOLUTION SATURATION SPECTRA OF THE IODINE ISOTOPE I2129 IN THE 633‐nm WAVELENGTH REGION , 1971 .

[14]  Gordon W. Day,et al.  Accurate frequencies of molecular transitions used in laser stabilization: the 3.39‐μm transition in CH4 and the 9.33‐ and 10.18‐μm transitions in CO2 , 1973 .