Laser cone beam computed tomography scanner geometry for large volume 3D dosimetry
被引:10
作者:
Jordan, K. J.
论文数: 0引用数: 0
h-index: 0
机构:
Univ Western Ontario, London Hlth Sci Ctr, London Reg Canc Program, London, ON, CanadaUniv Western Ontario, London Hlth Sci Ctr, London Reg Canc Program, London, ON, Canada
Jordan, K. J.
[1
]
Turnbull, D.
论文数: 0引用数: 0
h-index: 0
机构:
Univ Western Ontario, London Hlth Sci Ctr, London Reg Canc Program, London, ON, CanadaUniv Western Ontario, London Hlth Sci Ctr, London Reg Canc Program, London, ON, Canada
Turnbull, D.
[1
]
Batista, J. J.
论文数: 0引用数: 0
h-index: 0
机构:
Univ Western Ontario, London Hlth Sci Ctr, London Reg Canc Program, London, ON, CanadaUniv Western Ontario, London Hlth Sci Ctr, London Reg Canc Program, London, ON, Canada
Batista, J. J.
[1
]
机构:
[1] Univ Western Ontario, London Hlth Sci Ctr, London Reg Canc Program, London, ON, Canada
来源:
7TH INTERNATIONAL CONFERENCE ON 3D RADIATION DOSIMETRY (IC3DDOSE)
|
2013年
/
444卷
关键词:
GELS;
D O I:
10.1088/1742-6596/444/1/012062
中图分类号:
O4 [物理学];
学科分类号:
0702 ;
摘要:
A new scanner geometry for fast optical cone-beam computed tomography is reported. The system consists of a low power laser beam, raster scanned, under computer control, through a transparent object in a refractive index matching aquarium. The transmitted beam is scattered from a diffuser screen and detected by a photomultiplier tube. Modest stray light is present in the projection images since only a single ray is present in the object during measurement and there is no imaging optics to introduce further stray light in the form of glare. A scan time of 30 minutes was required for 512 projections with a field of view of 12 x 18 cm. Initial performance from scanning a 15 cm diameter jar with black solutions is presented. Averaged reconstruction coefficients are within 2% along the height of the jar and within the central 85% of diameter, due to the index mismatch of the jar. Agreement with spectrometer measurements was better than 0.5% for a minimum transmission of 4% and within 4% for a dark, 0.1% transmission sample. This geometry's advantages include high dynamic range and low cost of scaling to larger (>15 cm) fields of view.