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Frequency Converted Lasers<br />

TA-SHG <strong>pro</strong><br />

Frequency Doubled High Power Diode Lasers<br />

TA-SHG <strong>pro</strong> — high power, cw, tunable<br />

UV, blue or green laser source<br />

(inside view).<br />

Key features<br />

· UV, blue, green laser radiation:<br />

323 .. 540 nm (with only few gaps)<br />

· Up to 400 mW output power<br />

· Tunable single-frequency emission, typ.<br />

linewidth < 500 kHz<br />

· Probe beam output of fundamental<br />

laser<br />

· Increased amplitude stability with<br />

“noise eater” option<br />

Schematic of the TA-SHG <strong>pro</strong> system:<br />

high power at common and exotic<br />

wavelengths.<br />

26 www.toptica.com<br />

High power, tunable UV, blue<br />

or green laser light<br />

Many applications require narrow linewidth,<br />

tunable high power laser radiation at<br />

specifi c wavelengths ranging from the UV<br />

to the green spectrum of light. Examples<br />

are laser cooling of atoms and ions, plasma<br />

spectroscopy or holography. The TA-<br />

SHG <strong>pro</strong> is not only the system of choice<br />

for these applications but also serves as<br />

a replacement of HeCd or Ar-ion lasers,<br />

especially if single frequency operation and/<br />

or tunability are required.<br />

From a conceptual point of view as well<br />

as from the physical size of control rack<br />

and laser head, the TA-SHG <strong>pro</strong> system is<br />

very similar to the DL-SHG <strong>pro</strong> laser. The<br />

main difference between the two is that in<br />

the TA-SHG <strong>pro</strong> system the master laser<br />

is amplifi ed by a tapered amplifi er section<br />

and additionally optically isolated before<br />

it is coupled into the SHG <strong>pro</strong> resonator.<br />

Therefore, signifi cantly higher output powers<br />

are possible. A special feature of the TA-SHG<br />

<strong>pro</strong> is the optional output power regulation.<br />

All other premium characteristics of the DL-<br />

SHG <strong>pro</strong> are maintained also in the TA-SHG<br />

<strong>pro</strong>. Ultra-low noise sensitivity, best long<br />

term stability of the laser frequency and<br />

output power as well as ease of use are just<br />

a few of them.<br />

The TA-SHG <strong>pro</strong> lasers are available<br />

within a wide wavelength range (currently<br />

available 323 .. 540 nm with only few<br />

spectral gaps). Being customized systems,<br />

TA-SHG <strong>pro</strong> characteristics might vary<br />

from solution to solution. Depending on the<br />

design wavelength, typical output powers<br />

of 10 mW to 400 mW are available. Besides<br />

the output power, the other parameters are<br />

similar to the ones achieved in the DL SHG<br />

<strong>pro</strong> systems (see table “Specifi cations<br />

Frequency Converted Lasers”, page 29).<br />

TA-SHG applications<br />

· Laser cooling and spectroscopy of atoms<br />

(e.g. Sr, Yb, Ca, Cr, Er, He, Mg, ...)<br />

· Laser cooling and spectroscopy of ions<br />

(e.g. Ca, Yb, Ba, ...)<br />

· Rydberg excitation<br />

· Plasma spectroscopy<br />

· Optical data storage, holography<br />

and interferometry

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