Lei Xing , Ph.D. & Jacob Haimson Professor Department of Radiation Oncology & MIPS Stanford University School of Medicine …………………………… 6/30/13 Case study – TrueBeam 6 MV FFF RapidArc Tx of a Lung SBRT 3D modeling Pt setup and treatment delivery Treatment planning Imaging 4D imaging Biological imaging 3D/4D CBCT 4D planning 4D modeling Gated tx planning Adaptive therapy (imaging, planning, delivery) 6/30/13 6/30/13 Day 0 Day 14 Day 24 Head and neck CT, PET, and IMRT treatment plan Supine Craniospinal Irradiation with RA Jianzhou Chen, Z. Chen, T. Atwood, I. Gibbs, S. Soltys, & L. Xing, Supine Craniospinal Irradiation with VMAT to Improve Target Dose Conformity and Homogeneity, JRO, 2012. @01-258_via99-011_hepatoma_onscreen 1 sensitivity Available Imaging Tools O im ptica ag l ing XLCT PET SPECT XFCT MRSI MRI US CT Spatial resolution Radioluminescence & X-ray Luminescence CT CT Molecular Imaging using nanophosphors Principle a Optical radiation Ionizing radiation Current applications - PET and SPECT scintillators - CT detectors - Portal imaging - - Dosimetry Scintillation counting - High-energy physics G. Pratx, 2012 Pratx, Sun, Carpenter & Xing, Optics Letters, 2011. CT Molecular Imaging using QD and nanophosphors QD710-RGD peptide A h E B C D F a a b c d 6/30/13 QD705 b Modification of QD710-Dendron with a dimeric RGD peptide, RGD2. B: Excellent solubility and monodisperity in aqueous solution for the QD710-Dendron (left) and QD710-RGD2 (right). C: TEM image of QD710-RGD2. D: UV absorbance and NIRF of the QD710-Dendron (bottom) and QD710-RGD2 (top). In vivo NIRF imaging of QD710-RGD2 (active targeting, E) and QD710-Dendron (passive targeting, F) in mice bearing SKOV3 tumor (Cheng’s lab). QD800 @01-258_via99-011_hepatoma_onscreen 2 b a Photon yield vs dose d 0.25 0.1 LaO2:Eu e 0.5 0.3 pM 0.75 1 2 µg/mL Gd2O2S:Eu White light Phos in Agar Phos Luminescence Tissue-mimicking material c f Varian 100keV fluoro 1 cGy g 10 cGy 100 cGy The white light image (a) and luminescence image (b) of the nanophosphor phantom. (c) X-ray luminescence spectrum of Gd2O2S:Eu. The Gd2O2S:Eu phantoms with different concentrations (d) and their X-ray 6/30/13 luminescence images under different X-ray irradiation dose 1 cGy (e), 10 cGy (f) and 100 cGy (g). Multiplexing X-ray induced optical luminescence images ssDNA-Agx Lysozyme-Au8 BSA-Au25 8 Int. 6 Blank (a) Schematic of the locations of each type of RLNP. The inactive particles are indicated with the abbreviation (Ctrl). (b,c) 6/30/13 The unmixed signal from the BaYF4:Tb and BaYF4:Eu particles, respectively. (d) The unmixed multiplexed image with colorbars for the relative concentrations of BaYF4:Tb and BaYF4:Eu. (C. Carpenter et! al, 2012) 4. 1. 2. 3. Water ssDNAssDNA LyzLyz BSABSA Agx Au8 Au25 4 2 0 1 2 3 4 1 ! X-ray induced optical luminescence intensities Gultathione Au18?? Gultathione-Au Or polymer-Au ion complex 60 Int. 40 Blank 1. 2. 3. Water solution solid 20 0 1 2 3 3 @01-258_via99-011_hepatoma_onscreen 3 X-ray Luminescence Tomography 1% Agar 99% water TiO2 for optical sctter Ink for optical absorption 100 µM phosphor G. Pratx et al, IEEE Trans. Med. Ima., 2010 1cm phosphor plug 6/30/13 Reconstruction: ML-EM Noise from counting statistics: Molecular sensitivity = 0.3 pM @ 1cGy 0.3 pM Yi ~ Poisson(yi) 0.5 Log-likelihood: 0.75 10 cGy 1 cGy 0.25 Optimization: 1 0.1 2 µg/mL Expectation-Maximization: Tissue-mimicking 6/30/13 material 6/30/13 100 cGy @.4<,<487E05/; Spatially Encoded Light Emission X-ray Luminescence Tomography 6/30/13 C. Carpenter et al, PMB 2012 @01-258_via99-011_hepatoma_onscreen 4 Reconstruction & linearity Spatial resolution ~ 1 mm 50 radial positions 1.5 1 5 10 mg/mL 1 Phantom 2 3 4 mm 100 radial positions 0.5 64 angles Offset (background) 128 angles 6/30/13 Reconstructed image (ML-EM) Sinogram Simulation vs Experiment 10 mg/mL 5 mg/mL Reconstructed image Simulation Sinogram Experiment 1 mg/mL 6/30/13 X-ray Fluorescence Molecular CT Imaging 6/30/13 X-ray Fluorescence Molecular CT Imaging XFCT CT Sinograms (top) and reconstructed CT images (bottom) for XFCT (left) and transmission CT (right) of the low-resolution phantom loaded with gold for a 0.1 mGy imaging dose. (Magda Bozalova et al) M. Balazova, Y. Kuang, G. Pratx, L. Xing, X-ray Fluorescence Molecular CT Imaging, IEEE Trans Med Ima., 2012 M. Balazova, Y. Kuang, G. Pratx, L. Xing, X-ray Fluorescence Molecular CT Imaging, IEEE Trans Med Ima., 2012 @01-258_via99-011_hepatoma_onscreen 5 X-ray Fluorescence Molecular CT Imaging X-ray Fluorescence Molecular CT Imaging M. Balazova, Y. Kuang, G. Pratx, L. Xing, X-ray Fluorescence Molecular CT Imaging, IEEE Trans Med Ima., 2012 Au Pt Fig. 1. (left) Proposed XFCT/CT system. (top) Physical mechanism of X-ray fluorescence from K-shell electrons. 6/30/13 6/30/13 K. Yu et al, AAPM 2012 (best paper in imaging) Medical Physics Letters, 2013. Multiplexing K. Yu et al, AAPM 2012 (best paper in imaging) Medical Physics Letters, 2013. Multiplexing 6/30/13 K. Yu et al, AAPM 2012 (best paper in imaging) Medical Physics Letters, 2013. Overcoming Compton Scatter Moiz Ahmad et al, Order of Magnitude Sensitivity Increase in X-ray Fluorescence CT (XFCT) Imaging With an Optimized Spectro;9,<4,50<0.<8:87E2=:,<487!0/Ima, 2013 @01-258_via99-011_hepatoma_onscreen 6 Going Beyond K-Schell Imaging High-sensitivity x-ray fluorescence CT imaging of Cisplatin with L-shell x-rays Magda ML-EM Bazalova et al, ML-EM (w/o correction) (w correction) FBP to be published Magda Bazalova, to be published, 2013 80 keV 30 keV 15 keV CT Figure 2: CT images (first column, W/L = 800/0) and XFCT images reconstructed with filtered backprojection (FBP, second column) and maximum likelihood expectation maximization (ML-EM, 20 High-sensitivity x-ray fluorescence CT imaging of Cisplatin with L-shell x-rays X-ray acoustic tomography (XACT) with pulsed ! X-ray beam from a medical linear accelerator Guillem Pratx, Yu Kuang, and Lei Xing Liangzhong Xiang, Bin Han, Colin Carpenter, Figure 5: Profiles along a horizontal (left) and vertical (right) line across the phantom for the 15 keV images reconstructed with FBP (green), ML-EM without (blue) and with (red) attenuation correction.The actual profile is marked by the black dashed line. The accuracy of concentration reconstruction is significantly increased when attenuation correction is applied. ! 30 picoseconds per pulse ! Xiang L et al, Medical Physics Letters, 2013 D Interaction of X-ay with endogenous or exogenous media provides the basis for X-ray molecular imaging. D 4235A;07;4<4>0,7/;90.4E.):,A6850.=5,: imaging is possible. D XFCT, XLCT and XACT are a few examples of X-ray molecular/physiological imaging that are being developed at Stanford. @01-258_via99-011_hepatoma_onscreen 7