Lecture 2 - Center for Biomedical Optics and New Laser Systems
Lecture 2 - Center for Biomedical Optics and New Laser Systems Lecture 2 - Center for Biomedical Optics and New Laser Systems
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10.07.2015
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lack x = µ s ’ < 10µ ablue = const µ s', red = const µ a10 1 0.001Oblique R(r)µ a10 01.00.10.011.0mfp' [cm]10 -110 µ s '10 -210010 -3100010 -2 10 -1 10 0 10 1 10 2delta [cm]
R(r)Reflectance as a function ofsource-detector separation
- Page 2: Consider a cup of coffee with cream
- Page 8 and 9: R ≈ e −µ a Ladd a drop ofabsor
- Page 10 and 11: Measurement vs properties gridColle
- Page 12 and 13: lack x = µ s ’ < 10µ ablue = co
- Page 14 and 15: lack x = µ s ’ < 10µ ablue = co
- Page 16 and 17: µ a = 0.1 cm -1
- Page 18 and 19: µ a = 0.1 cm -1
- Page 20 and 21: µ a = 0.1 cm -1
- Page 22 and 23: Oblique R(r)Light is delivered at a
- Page 26 and 27: CameraBeam of lightM total.std exam
- Page 28 and 29: mua = 0.1mua = 0
- Page 30 and 31: mua = 0.5mua = 0
- Page 32 and 33: R std M total M total.std RM total
- Page 34 and 35: Added absorber methodDetector sense
- Page 36 and 37: Added absorber methodBeam of lightD
- Page 38 and 39: Added absorber methodDetector sense
- Page 40 and 41: Added absorber methodDetector sense
- Page 42 and 43: 10.90.8blue = const µ s', red = co
- Page 44 and 45: R total + added absorber10.90.80.70
- Page 46 and 47: M = M tissueM std= S T tissueG tiss
- Page 48 and 49: M = M tissueM std= S T tissueG tiss
- Page 50 and 51: M = M tissueM std= S T tissueG tiss
- Page 52: Reflectance-mode ConfocalMicroscopy
- Page 55 and 56: Coherence gate of OCT provides a 45
- Page 57 and 58: ρe −µz€~1/1000 thCMOCT
- Page 59 and 60: R(z)€ρ = local reflectivity [-]
- Page 61 and 62: T inT out= e −a(g)µ s z f 2Gag
- Page 63 and 64: R = T inρT out= ρe −µz f= µ s
- Page 65: Mietheory
- Page 68 and 69: Consider a rCLSM or OCT image…
- Page 70 and 71: Consider a rCLSM or OCT image…R(z
R(r)Reflectance as a function ofsource-detector separation
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