Applied Laser Medicine by G. Müller (auth.), Professor Dr. H.-Peter Berlien, Professor

By G. Müller (auth.), Professor Dr. H.-Peter Berlien, Professor Dr.-Ing. Gerhard J. Müller (eds.)

The background of laser functions in drugs begins al­ within the early Nineties a concerted motion application so much with the discovery of the laser itself. subsidized via the ecu fee used to be conducted in Europe for the dissemination of the secure use of It used to be just a couple of months after Maiman's invention lasers in medication, and in 1996 the same software was once whilst this new high-intensity mild resource used to be used for clinical functions. gentle as a healing instrument built with Russia. It was once this German--Russian had lengthy been utilized in medication, in particular in oph­ cooperation that resulted in a Russian model of the Ger­ thalmology and dermatology. as a result, those disci­ guy unique loose-leaf guide. The editors actual­ plines have been the 1st to use this new software. ized an ever-growing call for for an English model of this guide, too. as a result, the editors are very even supposing the early effects weren't as promising as thankful to the Springer publishing apartment for help­ anticipated, a brand new box for clinical analysis and deal with­ ment have been outlined. lots of the problems within the ing the English version of the German original.

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2. Position of the energy levels and the laser transition This arrangement ensures a high pumping efficiency. The system is cooled by passing purified water around the rod and lamps (see Fig. 4). g. diode laser, A is about 805 nm). 1 - 10 W. The very high price of laser diodes prevents their use in commercial solidstate lasers. There are various ways to construct the resonator: in most cases the active medium serves also as the optical resonator. The resonator mirrors are vacuumcoated directly onto the terminal faces of the crystal rod.

Helfmann Fig. 6. Resonator of a pulsed dye laser Mirror Dye cuvette Resonators The following describes various designs of resonators for pulsed and continuous-wave dye lasers. Resonators for Pulsed Dye Laser Systems Figure 6 presents a resonator for a flash lamppumped dye laser. e. by turning the prism the output wavelength can in rough steps be varied. Resonators for cw Dye Laser Systems Figure 7 presents the typical design of a cw dye laser resonator. The pumping laser, in this case an argon ion laser, is focused by a mirror into the dye beam.

064 }lm, in the near infrared, to take place. 32 }lm. Figure 3 presents relative intensity versus wavelength. 0645 }lm fuse due to their close proximity. 320 }lm. g. 9 }lm agree relatively well with the pumping levels. The pumping arrangement may be a double elliptic reflector made of a high-reflectivity, gold-coated material. A cylindrical YAG rod is placed at the common focal point. The two arc discharge lamps are centred at the other two focal points. 24 2 B. 3. 2. Position of the energy levels and the laser transition This arrangement ensures a high pumping efficiency.

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