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Principles of Fluorescence Spectroscopy

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PRINCIPLES OF FLUORESCENCE SPECTROSCOPY 113<br />

Figure 4.19. Coaxial nanosecond flashlamp. Revised and reprinted<br />

with permission from [52]. Copyright © 1981, American Institute <strong>of</strong><br />

Physics.<br />

occurred whenever the voltage across the electrodes<br />

reached the breakdown value. Almost all presently used<br />

lamps are gated. The electrodes are charged to high voltage.<br />

At the desired time the thyratron is gated on to rapidly discharge<br />

the top electrode to ground potential. A spark discharge<br />

occurs across the electrodes, which results in a<br />

flash <strong>of</strong> light. These pulses are rather weak, and one frequently<br />

has to block the room light to see the flash with the<br />

naked eye.<br />

Compared to ion or Ti:sapphire laser sources, flashlamps<br />

are simple and inexpensive. Hence, there have been<br />

considerable efforts to obtain the shortest pulse widths and<br />

highest repetition rates. Despite these efforts, the flashes are<br />

much wider than that available with a laser source. One <strong>of</strong><br />

the shortest time pr<strong>of</strong>iles is shown in Figure 4.20 (left),<br />

where the full width at half maximum is 730 ps FWHM.<br />

More typical is the 1.2-ns FWHM for a flashlamp in which<br />

the gas is an argon–hydrogen mixture. Also typical <strong>of</strong> flashlamps<br />

is the long tail that persists after the initial pulse. The<br />

spectral output <strong>of</strong> the pulse lamps depends on the gas, and<br />

the pulse width typically depends on both the type <strong>of</strong> gas<br />

and the pressure. Hydrogen or deuterium (Figure 4.21) provides<br />

a wide range <strong>of</strong> wavelengths in the UV, but at low<br />

intensity. Nitrogen provides higher intensity at its peak<br />

wavelengths, but little output between these wavelengths. In<br />

recognition <strong>of</strong> the growing interest in red and near-infrared<br />

(NIR) fluorescence, flashlamps have been developed with<br />

red and NIR outputs. 53–54 Given the availability <strong>of</strong> pulsed<br />

LDs and LEDs laser diodes in the red and NIR, there is less<br />

motivation to develop red and NIR flashlamps.<br />

The most significant drawback <strong>of</strong> using a flashlamp is<br />

the low repetition rate. The fastest flashlamps have repeti-<br />

Figure 4.20. Time-pr<strong>of</strong>iles <strong>of</strong> coaxial flashlamps. Revised and reprinted from [9] and [53]. Copyright © 1991, American Institute <strong>of</strong> Physics.

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