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Mannheim BiomedicalEngineering Laboratories
Introduction / literature
Chap. 1: Basics of laser physics
Chap. 2: Matter acting on light
Chap. 3: Light acting on matter
Chap. 4: Medical laser applications
Chap. 5: Laser safety
Prof. Dr. Markolf Niemz
- Lecture notes -
- Exam preparation -
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Electromagnetic
spectrum
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LASER: Light Amplified by Stimulated Emission of Radiation
transition rates at photon density n and transition probabilities A12, A21 and B21:
A12nN1 B21N2 A21nN2
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Laser beam characteristics
• monochromaticity
• collinearity
• spatial and temporal coherence
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Matter acting on light
• reflection and refraction
• absorption and scattering
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Reflection und refraction
law of reflection: θ = θ‘
law of refraction: n1 sin θ = n2 sin θ‘‘n1 n2
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Absorption
tissue absorption according to Lambert-Beer: I(z) = I0 exp (−αz)
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Scattering
Rayleigh scattering: I(λ) ~ λ− 4
Mie scattering: I(λ) ~ λ− x
with 0.4 < x < 0.5
Rayleigh scattering
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Light acting on matter
process interaction type mechanism
non-ionizing processes photochemical interaction photokatalysis
thermal interaction increase in temperature
ionizing processes photoablation UV photodissociation
plasma-induced ablation plasma ionization
photodisruption shock wave generation
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Laser-tissue interactions
examples:
• cataract
• keratomileusis
• sclerostomy
• coagulation
• photodynamictherapy
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Photochemical interaction
photodynamic therapy (PDT)
−
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Thermal interaction
temperature effect
37 oC −> 42 oC hyperthermia
> 60 oC coagulation
100 oC vaporization
> 100 oC carbonization
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Extra: Laser-induced interstitial thermotherapy (LITT)
temperature effect
37 oC −> 42 oC hyperthermia
> 60 oC coagulation
100 oC vaporization
> 100 oC carbonization
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Photoablation
excitation:
AB + hν (AB)*
deactivation:
(AB)* A + B + Ekin
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Plasma-induced ablation
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Photodisruption
pulse duration: 10−15 − 10− 9 sec
energy density: 1 − 1000 J/cm2
power density: 1011 − 1013 W/cm2
electric field strength: 107 − 108 V/cm
H2O
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Laser applications in medicine
ophthalmology: retinal detachment, cataract, glaucoma, wrong-sightedness
dentistry: caries, feeling of pain
neurosurgery: brain tumor
gynecology: cervical intraepithelial neoplasia (CIN), endometriosis,
obstruction of the uterine tube, twin-syndrome
urology: bladder tumor, benign prostatic hyperplasia (BPH)
angioplasty: atherosclerosis, stenosis
dermatology: port wine stain, tattoo, skin cancer
orthopedics: arthrosis, herniated disc, otosclerosis
otorhinolaryngology: laryngeal tumor, otosclerosis
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Laser applications in ophthalmology
indications:
• retinal detachment
• cataract
• glaucoma
• wrong-sightedness
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Wrong-sightedness
index of refraction
air 1.00
cornea 1.37
aqueous humor 1.33
lens 1.42
vitreous 1.33
• cornea is responsible for 70 % of refractive power
• minimally invasive surgery of cornea is possible
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Refractive power of the eye
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Techniques in refractive corneal surgery
alternatives to glasses
and contact lenses
advantages:
• expensive eyewear becomes needless
• strongly deviating wrong-sightedness curable as well
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Model of keratomileusis - part II
ablation depth: ca. 10 µm per diopter (ymax = 2.5 mm) ablation curve of the cornea (ArF laser, 193 nm)
∆D (dpt) Rf (mm) d(0) (µm)
1 7.965 9.0
2 8.137 17.9
3 8.316 26.8
4 8.504 35.7
5 8.700 44.6
6 8.906 53.4
7 9.121 62.2
8 9.347 71.0
9 9.585 79.7
10 9.835 88.4
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fs-LASIK: Laser in situ keratomileusis with the femtosecond laser
advantages:
• original surface
• without scalpel
• without UV light
laser parameters:
• Nd:Glass laser (500 fs)
• 3 µJ / pulse
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Laser applications in dentistry
indications:
• caries
• feeling of pain
(biostimulation)
pain caused by mechanical drill
dental surgery with laser light
• vibrations (typ. 100 − 1000 Hz)
• increase in temperature due to friction (at ∆T > 5 oC)
• without vibrations (contactless)
• increase in temperature negligible at ultrashort pulse durations
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Painfree caries therapy: Investigated laser systems
Ho:YAG laser Er:YAG laser Nd:YLF laser
λ = 2.12 µm λ = 2.94 µm λ = 1.053 µm
τ = 250 µs τ = 60 µs τ = 30 ps
E = 300 mJ E = 50 mJ E = 1 mJ
n = 100 n = 2 n = 16 000
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Caries diagnostics by plasma spectroscopy
LIBS: Laser-Induced Breakdown Spectroscopy
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Plasma spectroscopy
healthy tooth
carious tooth
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Laser applications in neurosurgery
indication:
• brain tumor
potential therapies
of a brain tumor
• radiotherapy (inaccurate deposition of energy)
• chemotherapy (difficult due to blood-brain-barrier)
• mechanical resection (not minimally invasive, bleeding)
• coagulation and ablation with laser light (under investigation)
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Laser safety
spectral range eye skin
UVC: 100 − 280 nm keratitis (inflammation) erythema, skin cancer
UVB: 280 − 315 nm keratitis (inflammation) erythema, pigmentation
UVA: 315 − 400 nm cataract pigmentation
VIS: 400 − 780 nm retinal burn skin burn
IRA: 780 − 1400 nm retinal burn, cataract skin burn
IRB: 1.4 − 3.0 µm retinal burn, cataract skin burn
IRC: 3.0 − 10 µm corneal burn skin burn
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Laser safety of the eye
VIS, IRA
IRB, IRC,UVB, UVC
UVA
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Laser safety of the skin
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Laser safety classes
class threshold laser types protection
1 < 0.4 µW capsuled lasers, low power lasers none
2 < 1 mW soft lasers (defined in VIS only) natural reflex of the eye lid
3a < 5 mW lasers for alignment purposes safety glasses
3b < 0.5 W medium power lasers safety glasses
skin protection (UV)
4 > 0.5 W high power lasers safety glasses
skin protection (UV)
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Realized laser safety
• laser safety officer
• laser safety equipment:
1) warning sign and warning lamp
2) safety curtain
3) safety glasses
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Determination of safety glasses
example: Nd:YAG laser (80 mJ, 15 nsec)
MPE = 5 × 10− 6 J/cm2 (from table)
H0 = 80 mJ / π r 2
= 80 mJ / π (0.35 cm) 2
= 0.21 J/cm2
OD = log (H0 / MPE)
= log (0.21 / 5E−6)
= 4.6
recommended filter density: 5
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Mannheim BiomedicalEngineering Laboratories
University Mannheim Technical University of Heidelberg Medical Center of Mannheim
Biomedical engineering: characterization and processing of biomaterialsinternet database for tissue parameters
Medical physics: design of medical applicators and sensorsbioelectrical multichannel measurement devices
Laser medicine: laser-tissue interactionsmedical applications of ultrashort laser pulses