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1 ectly affected the assessment of the RNFL by scanning laser polarimetry.
2 ologies including scanning laser tomography, scanning laser polarimetry and optical coherence tomogra
3 ch as retinal nerve fiber layer observation, scanning laser polarimetry, and confocal scanning laser
4 r-domain optical coherence tomography (OCT), scanning laser polarimetry, and confocal scanning laser
5 main OCT (coefficient of variation 2%-2.9%), scanning laser polarimetry (coefficient of variation 2.6
6 al assessment, optical coherence tomography, scanning laser polarimetry, confocal scanning laser opht
7 yer (RNFL) was measured by three techniques: scanning laser polarimetry (GDx ECC; Carl Zeiss Meditec,
8 he HRT Moorfields regression analysis (MRA), scanning laser polarimetry (GDx enhanced corneal compens
10 ng with Scanning Laser Ophthalmoscopy (HRT), Scanning Laser Polarimetry (GDx) and Optical Coherence T
11 lberg Engineering, Heidelberg, Germany), and scanning laser polarimetry (GDx-VCC; Carl Zeiss Meditec,
13 s in recent literature concerning the use of scanning laser polarimetry, Heidelberg retinal tomograph
15 s to assess RNFL measurements acquired using scanning laser polarimetry (SLP) and optical coherence t
16 , confocal scanning laser tomography (CSLT), scanning laser polarimetry (SLP) and photographic imagin
17 R/T, where R is RNFL retardance measured by scanning laser polarimetry (SLP) and T is RNFL thickness
19 around the ONH is assumed, the conversion of scanning laser polarimetry (SLP) phase-retardation measu
22 gnostic accuracies for glaucoma detection of scanning laser polarimetry (SLP) with enhanced corneal c
23 ination, optical coherence tomography (OCT), scanning laser polarimetry (SLP), and visual evoked pote
26 perimetry, optic disc stereophotographs, and scanning laser polarimetry with enhanced corneal compens
28 A and the control participant also underwent scanning laser polarimetry with variable corneal compens
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