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138

C.E. Riva

 

 

desired site, namely the rim of the optic disk or the fovea, respectively. The light scattered from the illuminated volume of tissue is collected and guided to a photodetector [5, 67].

Various means have been used to process the output photocurrent. Early studies in cats used the electronic systems of a commercial laser Doppler ßowmeter (PeriFlux PF3, Perimed, Inc., Stockholm,SwedenoraTSILaserFlo,Vasamedics, Minneapolis, USA) [6, 68]. More recent methods process the photocurrent using an algorithm developed for the NeXT computer [29]. Since this computer is no longer available, this algorithm is now implemented on a PC-based system [30].

The LDF parameters are calculated according to the procedure described by Bonner and Nossal [65]. These parameters include (1) the ÒvelocityÓ (Vel) of the RBCs, which is a measure of the broadening of the DSPS. For a tissue where the blood volume represents only a small percentage of the tissue volume (this is the case for the ONH), Vel is proportional to the root mean square of the RBC velocities; (2) ÒvolumeÓ (Vol), the number of moving RBCs in the sampled volume, which is proportional to the area under the DSPS; and (3) Flow, which is proportional to the product Vel ×Vol. Flow is usually referred to as Òblood ßow.Ó However, what Flow actually measures is the flux of the RBCs. Blood ßow is directly proportional to RBC ßux only if the hematocrit remains constant during an experiment. Before the calculation of these parameters, the DSPS is corrected for the shot noise power present in the photocurrent.

The LDF parameter Vel is expressed in Hz. The parameters Vol and Flow are in arbitrary units. The inability of LDF to provide absolute ßow measurements is due to the fact that laser radiation incident on a tissue undergoes scattering and absorption, both processes inßuencing the penetration pattern of the light. Penetration may differ from one region of a tissue to another, depending upon the optical properties of the tissue. Thus, spatial or temporal variations in tissue structure and vascularization, as is the case for example in the ONH in glaucoma, will affect the LDF parameters. Furthermore, direct comparison between the LDF parameters obtained from different tissues may not be valid due to variations in optical properties resulting from differences in tissue structure and

composition. In addition, light scattering by the ocular media will also inßuence the LDF parameters, as demonstrated by scanning laser Doppler ßowmetry performed in the presence of simulated light scatter induced by polystyrene microspheres placed in a cell in front of the eye of volunteers. This scatter induced an artifactual increase in the Flow in the retinal capillaries [69].

In addition to the LDF parameters, the mean of the photocurrent (so-called direct current, DC) is also recorded. The DC is proportional to the intensityofthelightincidentonthedetector(shifted+nonshifted scattered light). For repeated measurements from the same site of the fundus, it is important to maintain this parameter constant (arbitrarily within 10% of the mean) to insure that the variations of the LDF parameters are not due to variations in the intensity of the probing beam at the fundus or changes of the measurement site. Constancy of the DC can be further improved by maintaining constant the location of the entrance of the probing beam at the pupil of the tested subject, particularly in the measurements of ONH blood ßow [70].

7.3.3Detection Scheme for Optic Nerve and Subfoveal Choroidal Blood Flow

Two LDF measurement modes have been implemented. The Þrst is the continuous mode for online, continuous recording of the LDF parameters at a discrete site of the vascular beds of the ONH, subfoveal region of the choroid, or the iris. The second mode was based on a scanning technique, which provides a two-dimensional image of the RBC ßux in the capillaries of the ONH and retina. This technique is no longer available. This chapter describes only the former one.

7.3.3.1Real-Time Recording of the LDF Signal in the ONH and Subfoveal

Choroid (SFCH)

With the fundus-camera-based LDF system, originally described by Riva et al., to record the LDF signal from the ONH and the SFCH [6, 9], a laser beam from a HeNe (623 nm) or diode laser

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