In vivo optical characterization of human prostate tissue using near-infrared timeresolved spectroscopy.Svensson, Tomas; Andersson-Engels, Stefan; Einarsdóttír, Margrét; Svanberg, Katarina General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights.• Users may download and print one copy of any publication from the public portal for the purpose of private study or research.• You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal Take down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim.In vivo optical characterization of human prostate tissue using near-infrared time-resolved spectroscopy
Tomas Svensson Stefan Andersson-EngelsLund University Department of Physics SE-221 00 Lund Sweden
Margrét Einarsdóttír Katarina SvanbergLund University Hospital Department of Oncology SE-221 00 Lund Sweden Abstract. The development of photodynamic therapy into a modality for treatment of prostate cancer calls for reliable optical dosimetry. We employ, for the first time, interstitial time-resolved spectroscopy to determine in vivo optical properties of human prostate tissue. Nine patients are included in the study, and measurements are conducted prior to primary brachytherapy treatment of prostate cancer. Intrasubject variability is examined by measuring across three tissue volumes within each prostate. The time-resolved instrumentation proves its usefulness by producing good signal levels in all measurements. We are able to present consistent values on reduced scattering coefficients ͑ s Ј͒, absorption coefficients ͑ a ͒, and effective attenuation ͑ eff ͒ at the wavelengths 660, 786, and 916 nm. At 660 nm, s Ј is found to be 9±2 cm −1 , and a is 0.5± 0.