lei xing , ph.d. & jacob haimson professor stanford...
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Department of Radiation Oncology & MIPS Stanford University School of Medicine
Lei Xing , Ph.D. & Jacob Haimson Professor
6/30/13 ……………………………
Imaging
3D modeling Treatment planning Pt setup and treatment delivery
4D modeling
Gated tx planning
4D planning
Adaptive therapy (imaging, planning, delivery)
Day 0 Day 14 Day 24
3D/4D CBCT 4D imaging Biological imaging
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Case study – TrueBeam 6 MV FFF RapidArc Tx of a Lung SBRT
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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.
Head and neck CT, PET, and IMRT treatment plan
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Available Imaging Tools
Spatial resolution
sens
itivi
ty
XLCT
XFCT
PET
SPECT
CT
MRI
Optical imaging
US
MRSI
Radioluminescence & X-ray Luminescence CT
Ionizing radiation Optical radiation
- PET and SPECT scintillators - CT detectors
- Portal imaging
- Dosimetry - Scintillation counting
- High-energy physics
Current applications
Principle
G. Pratx, 2012
CT Molecular Imaging using nanophosphors
a
Pratx, Sun, Carpenter & Xing, Optics Letters, 2011.
CT Molecular Imaging using QD and nanophosphors
a b c d
QD705 QD800
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a b
h A
B C D
E
F
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).
QD710-RGD peptide
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Phos
Phos in
Agar
Varian 100keV fluoro
Gd2O2S:Eu LaO2:Eu
Photon yield vs dose
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 luminescence images under different X-ray irradiation dose 1 cGy (e), 10 cGy (f) and 100 cGy (g).
White light Luminescence
a b
cTissue-mimicking
material 1 cGy
10 cGy 100 cGy
0.3 pM
0.1
0.250.5
0.75
1
2 µg/mL
d e
f g
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(a) Schematic of the locations of each type of RLNP. The inactive particles are indicated with the abbreviation (Ctrl). (b,c) 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) !
Multiplexing
!
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X-ray induced optical luminescence images
BSA-Au25Lysozyme-Au8ssDNA-Agx
6
8
4.BSA-
3.Lyz-
2. ssDNA-
Blank 1.Water
2
4Int.
1
BSAAu25
LyzAu8
ssDNAAgx
Water1 2 3 4
0
X-ray induced optical luminescence intensities
Gultathione-Au18??Gultathione Au18?? Or
polymer-Au ion complex
40
60
Blank 1.Water
2. solution
3.solid
20
Int.
3
Water solution solid1 2 3
0
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X-ray Luminescence TomographyG. Pratx et al, IEEE Trans. Med. Ima., 2010
1% Agar 99% water TiO2 for optical sctter Ink for optical absorption 100 µM phosphor
1cm phosphor plug
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Reconstruction: ML-EM
Log-likelihood:
Yi ~ Poisson(yi) Noise from counting statistics:
Optimization:
Expectation-Maximization:
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Molecular sensitivity = 0.3 pM @ 1cGy
Tissue-mimicking material
0.1
0.25
0.5
0.75
1
2 µg/mL
1 cGy 10 cGy
100 cGy
0.3 pM
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Spatially Encoded Light Emission
X-ray Luminescence Tomography 6/30/13
C. Carpenter et al, PMB 2012
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Spatial resolution ~ 1 mm
4 mm 3
2
1.5 1
0.5
64 angles 128 angles
50 ra
dial
pos
ition
s 10
0 ra
dial
pos
ition
s
Reconstruction & linearity
Phantom
Reconstructed image (ML-EM)
10 mg/mL 5
1
Offset (background)
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Sinogram
10 mg/mL
1 mg/mL
5 mg/mL
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Simulation vs Experiment S
imul
atio
n E
xper
imen
t
Sinogram Reconstructed image
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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
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)
XFCT CT
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
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Au
Pt
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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
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Fig. 1. (left) Proposed XFCT/CT system. (top) Physical mechanism of X-ray fluorescence from K-shell electrons.
X-ray Fluorescence Molecular CT Imaging
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 Ima, 2013
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Magda Bazalova, to be published, 2013
Going Beyond K-Schell Imaging CT FBP ML-EM (w/o correction) ML-EM (w correction)
15 k
eV
30 k
eV
80 k
eV
Figure 2: CT images (first column, W/L = 800/0) and XFCT images reconstructed with filtered back-projection (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
Magda Bazalova et al, to be published
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.
!
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
!
Liangzhong Xiang, Bin Han, Colin Carpenter, Guillem Pratx, Yu Kuang, and Lei Xing
30 picoseconds per pulse Xiang L et al, Medical Physics Letters, 2013
Interaction of X-ay with endogenous or exogenous media provides the basis for X-ray molecular imaging.
imaging is possible. XFCT, XLCT and XACT are a few examples of
X-ray molecular/physiological imaging that are being developed at Stanford.