Photodynamic Therapy
Martin Hof, Radek Macháň
CZECH TECHNICAL UNIVERSITY IN PRAGUE
FACULTY OF BIOMEDICAL ENGINEERING
Photodynamic Therapy (PDT)
• Origin of tumors and the principles of their treatment
• Principles and history of PDT
• Photo-physical and -chemical aspects
• Photosensitizers (PS) of 1. generation
• Endogenous photosensitizer
• Photosensitizers of 2. and 3. generation
• Summary
Origin of tumors
A B
C
A. Individual cells with modified genome
B. Hyperplasia: mutated cells are phenotypically identical with the healthy ones but they multiply faster
C. Dysplasia: abnormalities in cell shape and orientation
D
E
D. Noninvasive carcinoma: The cells differ more in appearance and multiplication rate. The tumor does not spread to other tissues
E. Invasive carcinoma: Spreading out of the tissue of origin: individual cells are transported by cardiovascular and lymphatic system; a malignant tumor can lead to metastasis over the whole body
Origin of tumors
Principles of tumor treatment
Traditional• Surgery• Radiotherapy• Chemotherapy
New developments• Boron neutron capture
therapy• Monoclonal antibody
therapy• Antigene or antisense
therapy• Photodynamic therapy
(PDT)
Principles of photodynamic therapy of tumors (PDT)
• Photosensitizers (PS) are not toxic “at dark”
• PS accumulate in tumors
• Illumination of the tumor leads to a) Fluorescence: diagnosis of the tumor
b) Killing of tumor cells
(Apoptosis, Necrosis) - PDT
History of photodynamic therapy of tumors
• 1900 Acridin exhibits photo-toxicity (Raab)
• 1903 Eosin applied against skin cancer (von Tappeiner)
• 1908 Photo-toxicity of porphyrins (Hausmann)
• 1913 Mayer-Betz tested photodynamic therapy with porphyrins on his skin
• 1924 Porphyrin enriched tissue exhibits red fluorescence upon illumination with UV radiation (Policard)
• 1942 Different retention of porphyrins in helathy and malignant tissues (Auler, Banzer)
• 1948 Diagnosis and treatment of cancer by hematoporphyrin and its complexes with zinc (Figge)
• 1961 Lipson developed a hematoporphyrin derivative (HpD).
• 1966 first successful breast cancer treatment by HpD (Lipson)
• 1978 first systematic clinical studies (Dougherty)
• Today a few thousand patients treated by HpD
Photosensitizers of the first generation
History of photodynamic therapy of tumors
Photosensitizers of the first generation
are oligomers (HpD) of Hematoporphyrin (Hp)
• Absorption at 405, 505, 525, 565 and 630 nm
• Emission at 635 and 700 nm• Accumulation in tumors
Hp
Dihemato-porphyrin- ether
Photophysics (Jablonski)
S1
Nonradiative transitions: knrT
knrS
Fluorescence: kf
Intersystem Crossing: kisc
Energy of the states
Phosphorescence: kp
Excited state reactions of photosensitizer in T1 state represent an additional nonradiative decay pathway. Reaction with O2 gives rise to singlet oxygen 1O2. Electron transfer reactions give rise to free radicals
Quantum Yields: F: f = kf / (kf + knrS + kisc)
ISC: isc = kisc / (kf + knrS + kisc)
P: p = isc kp / (kp + knrT)
What is 1O2?
• O2 is paramagnetic (in triplet
state) in the ground state (according to Hund rule)
• Because of spin restriction triplet oxygen 3O2 participates
only in non-selective radical reactions
E
95 KJ/mol
3O2 1O2
Electron configuration of 3O2
1269 nm
• Singlet oxygen 1O2 is very reactive and selective
Photochemistry
S1
O2
REAKCE Volné radikály
Energy of the states
(1O2 ) = isc k [3O2 ] / (k [3O2 ] + kp + knrT)
Type 2 reaction (energy transfer)
FREE RADICALS
Type 1 reaction (electron transfer) + O2
Reactive Oxygen Species (ROS):
Superoxide ·O2-
Hydroxyl rad. ·OH…
k
HpD accumulates preferentially in
membranes
Plasma membrane
Mitochondria
outer membrane
Nuclear membrane
inner membrane
Lysosomes
Endoplasmatic reticulum
Affected sites
Reactionsof 1O2 and ROS
with biomolecules
Peroxidation
Addition on cycles
Oxidation
Cause oxidative damage, which can lead ultimately to cell death
AFTERBEFORE
BEFORE – The photodynamic diagnostics (PDD) of a tumor
AFTER – The tumor tissue has been removed by PDT
Pros and cons of the 1. generation of photosensitizers
• Photophysics: high isc and (1O2 ), but relatively short wavelength absorption with a low absorption coefficient
• in vivo activity: low dark activity, high photodynamic activity, but relatively low selectivity of absorption in tumors
An example of HpD-PDT
INJECTION
intravenous
ACUMULATION IN TISSUE
ELIMINATION FROM
ACUMULATION IN TUMOR
TUMOR ILLUMANTION
weeks
NECROSIS
Healthy tissue Skin Serum
APOPTOSIS
• Photosesitizer protoporphyrin IX (Pp IX) is an intermediate of heme synthesis
• The physiological concentration of Pp IX is low because of a controlled expression of its precursor 5-aminolevulinic acid (ALA)
Endogenous PS:
Cells produce their own PS
Heme
ALAPp IX
COO-
CH2
CH2
C O
CH2 NH2
Ferrochelatase
MIT
OC
HO
ND
RIA
succinyl-CoA+
glycine
ALA-synthase
• The expression of ALA is feedback controlled via heme concentration
• Administration of exogenous ALA breaks the feedback control and results in accumulation of Pp IX
Endogenous PS:
Cells produce their own PS
Heme
ALAPp IX
COO-
CH2
CH2
C O
CH2 NH2
Ferrochelatase
MIT
OC
HO
ND
RIA
succinyl-CoA+
glycine
ALA-synthase
• Concentration of Pp IX is higher in cancer cells due to their higher metabolic activity and in some cases also due to decreased efficiency of ferrochelatase and increased efficiency of Pp IX synthesis from ALA
Photosensitizers of 2. generation:
- long wavelength absorption with large extinction coefficient- selective accumulation in tumor
Naphtalocyanine: ex = 820 nm
Porphycen:ex = 710 nm
Phtalocyanine:maximal ex = 740 nm
Chlorin e6: ex = 750 nm
Photosensitizers of 3. generation (selective acculmulation)
• Monoclonal antibodies bind selectively to an antigen on cancer cells
• The spacer is either cyclodextrin or Avidin-Biotin-system
PS
Spacer
Antibody
„Drug Targeting“
Summary
Limitations:Low penetration depth in tissue (ideal for skin cancer or with endoscopic illumination)
Advantages:Low costRelatively low side effects
Goals:High selectivity for cancer cellsOptimal illumination dose
Triplet Oxygen
Singlet Oxygen
Free radicals
REAKCE
Energy of states
Type II reaction
Type I reaction
Methodological outlook:Multiphoton excitation
• High intensity of ps- or fs-lasers• Excitation by light of double or
triple wavelength compared to single photon excitation
• Light of longer wavelength penetrates deeper to the tissue
Longwave excitation of a PS with shortwave absorption
Acknowledgement
The course was inspired by courses of:
Prof. David M. Jameson, Ph.D.
Prof. RNDr. Jaromír Plášek, Csc.
Prof. William Reusch
Financial support from the grant:
FRVŠ 33/119970