Biomedical Engineering Reference
In-Depth Information
Tabl e 1. 1
A summary of lasers and their spectral characteristics
Laser type
Wavelength range (nm)
Comments
ArC
457, 488, 514.5
Gas, CW or pulsed
He-Ne
632.8
Gas, CW
Nitrogen
337
Gas, pulsed
CO 2
10:6 m
Gas, CW or pulsed
HeAg
224
Gas
HeCd
325, 442
Gas, CW
Nd:YAG
1,064, 532
Solid state, CW or pulsed
Nd:YVO4
914, 1,064, 1,342
Solid state
Nd:YLF
1,047, 1,053
Solid state
Ti:sapphire
690-1,000
Solid state, CW or pulsed, Q-switched
Diode laser
300-900
Semiconductor, CW
Fiber laser
514, 780, 1,025-1,600
Pulsed, doped with Er, Nd, Yb, and Tm
Kr
C
406, 647, 752
Gas, CW, intermediate
KrCl
222
Excimer
KrF
248
Excimer
XeCl
308
Excimer
XeF
351
Excimer
Ruby
694.3
Solid state, pulsed
are also available, which are working in two ways. In one way, white LED is
generated by mixing the primary color red, green, and blue LEDs. In the other way,
white LED is generated by a second emission from a layer of phosphor material
excited by a blue or UV LED. Now, high-power LEDs are available. Because LED
has a very compact size and very long lifetime, it is expected that LED light source
will find broad applications in biomedical spectroscopy, particularly in absorption
spectroscopy, reflectance spectroscopy, and fluorescence spectroscopy.
1.2.2
Optical Fibers
Although free space light delivery is used in many optical spectroscopy systems,
they are usually inconvenient for use in biomedical applications. Nowadays most
biomedical spectroscopy systems use optical fiber-based light delivery. A cross
section of light transmission in optical fibers is shown in Fig. 1.3 .
The light transmission in fibers is based on the law of total internal reflection.
The acceptance angle of an optical fiber is determined by its numerical aperture
(NA), given by
q n co n cl ;
NA D n i sin max D
(1.1)
where n i , n co ,andn cl are the refractive index of the air, core, and cladding
material of the fiber and max is the maximum acceptance angle. When increasing
 
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