Optical fiber design and the trapping of Cerenkov radiation.

Cerenkov radiation is generated in optical fibers immersed in radiation fields and can interfere with signal transmission. We develop a theory for predicting the intensity of Cerenkov radiation generated within the core of a multimode optical fiber by using a ray optic approach and use it to make predictions of the intensity of radiation transmitted down the fiber in propagating modes. The intensity transmitted down the fiber is found to be dominated by bound rays with a contribution from tunneling rays. It is confirmed that for relativistic particles the intensity of the radiation that is transmitted along the fiber is a function of the angle between the particle beam and the fiber axis. The angle of peak intensity is found to be a function of the fiber refractive index difference as well as the core refractive index, with larger refractive index differences shifting the peak significantly toward lower angles. The angular range of the distribution is also significantly increased in both directions by increasing the fiber refractive index difference. The intensity of the radiation is found to be proportional to the cube of the fiber core radius in addition to its dependence on refractive index difference. As the particle energy is reduced into the nonrelativistic range the entire distribution is shifted toward lower angles. Recommendations on minimizing the quantity of Cerenkov light transmitted in the fiber optic system in a radiation field are given.

[1]  P. Lecoq,et al.  Cerium doped heavy metal fluoride glasses a possible alternative for electromagnetic calorimetry , 1996 .

[2]  A S Beddar,et al.  Optical filtering and spectral measurements of radiation-induced light in plastic scintillation dosimetry , 1993 .

[3]  S. Gripp,et al.  Clinical in vivo dosimetry using optical fibers. , 1998, Radiation oncology investigations.

[4]  F. H. Attix,et al.  Water-equivalent plastic scintillation detectors for high-energy beam dosimetry: II. Properties and measurements. , 1992, Physics in medicine and biology.

[5]  F. H. Attix,et al.  Water-equivalent plastic scintillation detectors for high-energy beam dosimetry: I. Physical characteristics and theoretical consideration. , 1992, Physics in medicine and biology.

[6]  S. McKeever,et al.  A real-time, fibre optic dosimetry system using Al2O3 fibres. , 2002, Radiation protection dosimetry.

[7]  Yves Charon,et al.  SIC, an intracerebral radiosensitive probe for in vivo neuropharmacology investigations in small laboratory animals: theoretical considerations and practical characteristics , 2000 .

[8]  B. L. Pruett,et al.  Gamma-Ray To Cerenkov-Light Conversion Efficiency For Pure-Silica-Core Optical Fibers , 1984, Optics & Photonics.

[9]  P N Johnston,et al.  A temporal method of avoiding the Cerenkov radiation generated in organic scintillator dosimeters by pulsed mega-voltage electron and photon beams. , 2002, Physics in medicine and biology.

[10]  J. M. Fontbonne,et al.  Scintillating fiber dosimeter for radiation therapy accelerator , 2001 .

[11]  M. Clift,et al.  Dealing with Cerenkov radiation generated in organic scintillator dosimeters by bremsstrahlung beams. , 2000, Physics in medicine and biology.

[12]  Holly Ning,et al.  Gated fiber-optic-coupled detector for in vivo real-time radiation dosimetry. , 2004, Applied optics.

[13]  R. Schmidt-Ullrich,et al.  Radiation-induced light in optical fibers and plastic scintillators: application to brachytherapy dosimetry , 1996 .

[14]  Sören Mattsson,et al.  Real-time optical-fibre luminescence dosimetry for radiotherapy: physical characteristics and applications in photon beams , 2004, Physics in medicine and biology.