24 results on '"Gholami, Yaser"'
Search Results
2. Towards personalised dosimetry in patients with liver malignancy treated with 90Y-SIRT using in vivo-driven radiobiological parameters
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Gholami, Yaser H., Willowson, Kathy P., and Bailey, Dale L.
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- 2022
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3. Overlooked potential of positrons in cancer therapy
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Hioki, Takanori, Gholami, Yaser H., McKelvey, Kelly J., Aslani, Alireza, Marquis, Harry, Eslick, Enid M., Willowson, Kathy P., Howell, Viive M., and Bailey, Dale L.
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- 2021
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4. Positron annihilation localization by nanoscale magnetization
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Gholami, Yaser H., Yuan, Hushan, Wilks, Moses Q., Josephson, Lee, El Fakhri, Georges, Normandin, Marc D., and Kuncic, Zdenka
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- 2020
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- View/download PDF
5. Toward Personalized Dosimetry with 32P Microparticle Therapy for Advanced Pancreatic Cancer
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Gholami, Yaser Hadi, Wilson, Nicole, James, David, and Kuncic, Zdenka
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- 2017
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- View/download PDF
6. Radio-enhancement effects by radiolabeled nanoparticles
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Gholami, Yaser Hadi, Maschmeyer, Richard, and Kuncic, Zdenka
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- 2019
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7. Comparison of radiobiological parameters for 90Y radionuclide therapy (RNT) and external beam radiotherapy (EBRT) in vitro
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Gholami, Yaser H., Willowson, Kathy P., Forwood, Nicholas J., Harvie, Rozelle, Hardcastle, Nicholas, Bromley, Regina, Ryu, HyunJu, Yuen, Samuel, Howell, Viive M., Kuncic, Zdenka, and Bailey, Dale L.
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- 2018
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8. A Radio-Nano-Platform for T1/T2 Dual-Mode PET-MR Imaging
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Gholami, Yaser Hadi, Yuan, Hushan, Wilks, Moses Q, Maschmeyer, Richard, Normandin, Marc D, Josephson, Lee, El Fakhri, Georges, and Kuncic, Zdenka
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radiolabeling ,Radioisotopes ,Phantoms, Imaging ,Contrast Media ,multimodal imaging ,Signal-To-Noise Ratio ,HIR ,Magnetic Resonance Imaging ,Ferrosoferric Oxide ,SPIONs ,PET ,International Journal of Nanomedicine ,Positron-Emission Tomography ,Chromatography, Gel ,Humans ,Chromatography, Thin Layer ,Zirconium ,Radiopharmaceuticals ,Magnetite Nanoparticles ,Original Research ,MRI - Abstract
Purpose This study aimed to develop a chelate-free radiolabeled nanoparticle platform for simultaneous positron emission tomography (PET) and magnetic resonance (MR) imaging that provides contrast-enhanced diagnostic imaging and significant image quality gain by integrating the high spatial resolution of MR with the high sensitivity of PET. Methods A commercially available super-paramagnetic iron oxide nanoparticle (SPION) (Feraheme®, FH) was labeled with the [89Zr]Zr using a novel chelate-free radiolabeling technique, heat-induced radiolabeling (HIR). Radiochemical yield (RCY) and purity (RCP) were measured using size exclusion chromatography (SEC) and radio-thin layer chromatography (radio-TLC). Characterization of the non-radioactive isotope 90Zr-labeled FH was performed by transmission electron microscopy (TEM). Simultaneous PET-MR phantom imaging was performed with different 89Zr-FH concentrations. The MR quantitative image analysis determined the contrast-enhancing properties of FH. The signal-to-noise ratio (SNR) and full-width half-maximum (FWHM) of the line spread function (LSF) were calculated before and after co-registering the PET and MR image data. Results High RCY (92%) and RCP (98%) of the [89Zr]Zr-FH product was achieved. TEM analysis confirmed the 90Zr atoms adsorption onto the SPION surface (≈ 10% average radial increase). Simultaneous PET-MR scans confirmed the capability of the [89Zr]Zr-FH nano-platform for this multi-modal imaging technique. Relative contrast image analysis showed that [89Zr]Zr-FH can act as a dual-mode T1/T2 contrast agent. For co-registered PET-MR images, higher spatial resolution (FWHM enhancement ≈ 3) and SNR (enhancement ≈ 8) was achieved at a clinical dose of radio-isotope and Fe. Conclusion Our results demonstrate FH is a highly suitable SPION-based platform for chelate-free labeling of PET tracers for hybrid PET-MR. The high RCY and RCP confirmed the robustness of the chelate-free HIR technique. An overall image quality gain was achieved compared to PET- or MR-alone imaging with a relatively low dosage of [89Zr]Zr-FH. Additionally, FH is suitable as a dual-mode T1/T2 MR image contrast agent., Video abstract Point your SmartPhone at the code above. If you have a QR code reader the video abstract will appear. Or use: http://youtu.be/Me_QBfX7I3s
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- 2020
9. Using Active and Passive Near-Field Hydrophones to Image the Near-Surface in Ultra-Shallow Waters Offshore Abu Dhabi
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Khakimov, Oleg, additional, Gholami, Yaser, additional, Tertrais, Bertrand, additional, Cambois, Guillaume, additional, and Mahgoub, Mohamed, additional
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- 2021
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10. Towards personalised dosimetry in patients with liver malignancy treated with 90Y-SIRT using in vivo-driven radiobiological parameters.
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Gholami, Yaser H., Willowson, Kathy P., and Bailey, Dale L.
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RADIATION dosimetry , *LIVER , *COLORECTAL cancer , *TREATMENT effectiveness , *METASTASIS , *CHOLANGIOCARCINOMA , *ADENOMATOUS polyps - Abstract
Background: The prediction of response is one of the major challenges in radiation-based therapies. Although the selection of accurate linear–quadratic model parameters is essential for the estimation of radiation response and treatment outcome, there is a limited knowledge about these radiobiological parameters for liver tumours using radionuclide treatments. Methods: The "clinical radiobiological" parameters ( T p , T k , α , α / β ) for twenty-five patients were derived using the generalised linear–quadratic model, the diagnostic ([18F] FDG PET/CT) and therapeutic ([90Y]-SIR-Spheres PET/CT) images to compute the biological effective dose and tumour control probability (TCP) for each patient. Results: It was estimated that the values for α and α / β parameters range in ≈ 0.001–1 Gy−1 and ≈ 1–49 Gy, respectively. We have demonstrated that the time factors, T p , T k and T critic are the key parameters when evaluating liver malignancy lesional response to [90Y]SIR-Spheres treatment. Patients with cholangiocarcinoma have been shown to have the longest average T p (≈ 236 ± 67 d), highest TCP (≈ 53 ± 17%) and total liver lesion glycolysis response ( Δ TLG liver ≈ 64%), while patients with metastatic colorectal cancer tumours have the shortest average T p (≈ 129 ± 19 d), lowest TCP (≈ 28 ± 13%) and Δ TLG liver ≈ 8%, respectively. Conclusions: Tumours with shorter T k have shown a shorter T critic and thus poorer TCP and Δ TLG liver . Therefore, these results suggest for such tumours the [90Y]SIR-Spheres will be only effective at higher initial dose rate (e.g. > 50 Gy/day). [ABSTRACT FROM AUTHOR]
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- 2022
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11. A Chelate-Free Nano-Platform for Incorporation of Diagnostic and Therapeutic Isotopes
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Gholami, Yaser H, Josephson, Lee, Akam, Eman A, Caravan, Peter, Wilks, Moses Q, Pan, Xiang-Zuo, Maschmeyer, Richard, Kolnick, Aleksandra, El Fakhri, Georges, Normandin, Marc D, Kuncic, Zdenka, and Yuan, Hushan
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radiolabeling ,Radioisotopes ,Feraheme ,Magnetic Resonance Spectroscopy ,radionuclide therapy ,Lutetium ,HIR ,nanomedicine ,Dynamic Light Scattering ,Ferrosoferric Oxide ,Copper Radioisotopes ,International Journal of Nanomedicine ,Isotope Labeling ,Chromatography, Gel ,Nanoparticles ,Radiopharmaceuticals ,Original Research ,Chelating Agents - Abstract
Purpose Using our chelate-free, heat-induced radiolabeling (HIR) method, we show that a wide range of metals, including those with radioactive isotopologues used for diagnostic imaging and radionuclide therapy, bind to the Feraheme (FH) nanoparticle (NP), a drug approved for the treatment of iron anemia. Material and methods FH NPs were heated (120°C) with nonradioactive metals, the resulting metal-FH NPs were characterized by inductively coupled plasma mass spectrometry (ICP-MS), dynamic light scattering (DLS), and r1 and r2 relaxivities obtained by nuclear magnetic relaxation spectrometry (NMRS). In addition, the HIR method was performed with [90Y]Y3+, [177Lu]Lu3+, and [64Cu]Cu2+, the latter with an HIR technique optimized for this isotope. Optimization included modifying reaction time, temperature, and vortex technique. Radiochemical yield (RCY) and purity (RCP) were measured using size exclusion chromatography (SEC) and thin-layer chromatography (TLC). Results With ICP-MS, metals incorporated into FH at high efficiency were bismuth, indium, yttrium, lutetium, samarium, terbium and europium (>75% @ 120 oC). Incorporation occurred with a small (less than 20%) but statistically significant increases in size and the r2 relaxivity. An improved HIR technique (faster heating rate and improved vortexing) was developed specifically for copper and used with the HIR technique and [64Cu]Cu2+. Using SEC and TLC analyses with [90Y]Y3+, [177Lu]Lu3+ and [64Cu]Cu2+, RCYs were greater than 85% and RCPs were greater than 95% in all cases. Conclusion The chelate-free HIR technique for binding metals to FH NPs has been extended to a range of metals with radioisotopes used in therapeutic and diagnostic applications. Cations with f-orbital electrons, more empty d-orbitals, larger radii, and higher positive charges achieved higher values of RCY and RCP in the HIR reaction. The ability to use a simple heating step to bind a wide range of metals to the FH NP, a widely available approved drug, may allow this NP to become a platform for obtaining radiolabeled nanoparticles in many settings., Video abstract Point your SmartPhone at the code above. If you have a QR code reader the video abstract will appear. Or use: https://youtu.be/_SYXGLeZuWM
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- 2020
12. A Radio-Nano-Platform for T1/T2 Dual-Mode PET-MR Imaging
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Gholami,Yaser Hadi, Yuan,Hushan, Wilks,Moses Q, Maschmeyer,Richard, Normandin,Marc D, Josephson,Lee, El Fakhri,Georges, Kuncic,Zdenka, Gholami,Yaser Hadi, Yuan,Hushan, Wilks,Moses Q, Maschmeyer,Richard, Normandin,Marc D, Josephson,Lee, El Fakhri,Georges, and Kuncic,Zdenka
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Yaser Hadi Gholami, 1–3 Hushan Yuan, 4 Moses Q Wilks, 4 Richard Maschmeyer, 1 Marc D Normandin, 4 Lee Josephson, 4 Georges El Fakhri, 4 Zdenka Kuncic 1, 2, 5 1Faculty of Science, School of Physics, The University of Sydney, Sydney, NSW, Australia; 2Sydney Vital Translational Cancer Research Centre, St Leonards, NSW, Australia; 3Bill Walsh Translational Cancer Research Laboratory, The Kolling Institute, Northern Sydney Local Health District, Sydney, NSW, Australia; 4Gordon Center for Medical Imaging, Massachusetts General Hospital, Harvard Medical School, Boston, MA, USA; 5The University of Sydney Nano Institute, Sydney, NSW, AustraliaCorrespondence: Zdenka Kuncic; Yaser Hadi GholamiSchool of Physics A28, The University of Sydney, Sydney, NSW 2006, AustraliaTel +61 2 9351 3162Fax +61 2 9351 7726Email zdenka.kuncic@sydney.edu.au; yaser.gholami@sydney.edu.auPurpose: This study aimed to develop a chelate-free radiolabeled nanoparticle platform for simultaneous positron emission tomography (PET) and magnetic resonance (MR) imaging that provides contrast-enhanced diagnostic imaging and significant image quality gain by integrating the high spatial resolution of MR with the high sensitivity of PET.Methods: A commercially available super-paramagnetic iron oxide nanoparticle (SPION) (Feraheme®, FH) was labeled with the [ 89Zr]Zr using a novel chelate-free radiolabeling technique, heat-induced radiolabeling (HIR). Radiochemical yield (RCY) and purity (RCP) were measured using size exclusion chromatography (SEC) and radio-thin layer chromatography (radio-TLC). Characterization of the non-radioactive isotope 90Zr-labeled FH was performed by transmission electron microscopy (TEM). Simultaneous PET-MR phantom imaging was performed with different 89Zr-FH concentrations. The MR quantitative image analysis determined the contrast-enhancing properties of FH. The signal-to-noise ratio (SNR) and full-width half-maximum (FWHM) of the line spread function (LSF
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- 2020
13. A Chelate-Free Nano-Platform for Incorporation of Diagnostic and Therapeutic Isotopes
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Gholami,Yaser H., Josephson,Lee, Akam,Eman A., Caravan,Peter, Wilks,Moses Q., Pan,Xiang-Zuo, Maschmeyer,Richard, Kolnick,Aleksandra, El Fakhri,Georges, Normandin,Marc D., Kuncic,Zdenka, Yuan,Hushan, Gholami,Yaser H., Josephson,Lee, Akam,Eman A., Caravan,Peter, Wilks,Moses Q., Pan,Xiang-Zuo, Maschmeyer,Richard, Kolnick,Aleksandra, El Fakhri,Georges, Normandin,Marc D., Kuncic,Zdenka, and Yuan,Hushan
- Abstract
Yaser H Gholami, 1– 4 Lee Josephson, 3 Eman A Akam, 5 Peter Caravan, 5 Moses Q Wilks, 3 Xiang-Zuo Pan, 3, 6 Richard Maschmeyer, 1 Aleksandra Kolnick, 3, 7 Georges El Fakhri, 3 Marc D Normandin, 3 Zdenka Kuncic, 1, 4, 8 Hushan Yuan 3 1The University of Sydney, Faculty of Science, School of Physics, Sydney, NSW, Australia; 2Bill Walsh Translational Cancer Research Laboratory, The Kolling Institute, Northern Sydney Local Health District, Sydney, Australia; 3Gordon Center for Medical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Boston, MA, United States; 4Sydney Vital Translational Cancer Research Centre, St Leonards, NSW, Australia; 5The Institute for Innovation in Imaging and the A. A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, MA, United States; 6Bouve College of Health Sciences, CaNCURE Program, Northeastern University, Boston, MA, USA; 7Internal Medicine Residency Program, Lahey Hospital and Medical Center, Burlington, MA, USA; 8The University of Sydney Nano Institute, Sydney, NSW, AustraliaCorrespondence: Hushan YuanGordon Center for Medical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, 149 13 th Street, Charlestown, MA 02129, USATel +1 617-643-1963Email hyuan@mgh.harvard.eduPurpose: Using our chelate-free, heat-induced radiolabeling (HIR) method, we show that a wide range of metals, including those with radioactive isotopologues used for diagnostic imaging and radionuclide therapy, bind to the Feraheme (FH) nanoparticle (NP), a drug approved for the treatment of iron anemia.Material and methods: FH NPs were heated (120°C) with nonradioactive metals, the resulting metal-FH NPs were characterized by inductively coupled plasma mass spectrometry (ICP-MS), dynamic light scattering (DLS), and r 1 and r 2 relaxivities obtained by nuclear magnetic relaxation spectrome
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- 2020
14. Developing A Novel Theranostic Nano-Platform For Simultaneous Multimodal Imaging And Radionuclide Therapy
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Gholami, Yaser Hadi
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Radiation Dosimetry ,Nanomedicine ,Radiolabelling ,Radionuclide therapy ,Multimodal Imaging ,Monte Carlo simulation - Abstract
The aim of this project was to develop and evaluate a theranostic nano-platform to enable Radionuclide Therapy (RNT) and multimodal imaging to improve the therapy and diagnosis of lymph node metastases. The work presented in this thesis consists of four main studies. First, Feraheme (FH) and two other superparamagnetic iron-oxide nanoparticles (SPIONs) were radiolabelled with radioisotopes commonly used in the clinic (89Zr, 177Lu and 90Y) for imaging and therapy utilising a novel chelate-free technique, which produced a high radiochemical yield and purity (up to 98%). FH nanoparticles were successfully radiolabelled with 90Y and 177Lu which was the first experimental demonstration that the HIR technique can be extended to radiolabel FH with these isotopes. In the second study, a series of phantom experiments were performed and results demonstrated that 89Zr-FH is a novel nanotechnology for simultaneous PET/MR imaging providing the capability of integrating the spatial resolution and tissue contrast provided by MR imaging with the high sensitivity of PET. An additional phantom study demonstrated the ability to image 177Lu-FH using Single Photon Emission Computed Tomography. The third study was a proof of concept for 90Y RNT. Results revealed that in RNT, the kinetics of DNA double strand break (DSB) induction, repair and misrepair must be considered when deriving radiobiological parameters. The fourth study, a Monte Carlo simulation study, was performed to study the subcellular mechanisms of dose delivery of the radionuclide 223Ra when treating metastases. These simulations showed that indirect cell damage may play an important role in RNT with alpha emitters due to the stochastic nature of alpha particle energy deposition. In conclusion, these results open a pathway towards a novel nuclear nanoplatform for multimodal imaging and RNT of lymph node metastases.
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- 2019
15. Roadmap for metal nanoparticles in radiation therapy: current status, translational challenges, and future directions
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Schuemann, Jan, primary, Bagley, Alexander F, additional, Berbeco, Ross, additional, Bromma, Kyle, additional, Butterworth, Karl T, additional, Byrne, Hilary L, additional, Chithrani, B Devika, additional, Cho, Sang Hyun, additional, Cook, Jason R, additional, Favaudon, Vincent, additional, Gholami, Yaser H, additional, Gargioni, Elisabetta, additional, Hainfeld, James F, additional, Hespeels, Félicien, additional, Heuskin, Anne-Catherine, additional, Ibeh, Udoka M, additional, Kuncic, Zdenka, additional, Kunjachan, Sijumon, additional, Lacombe, Sandrine, additional, Lucas, Stéphane, additional, Lux, François, additional, McMahon, Stephen, additional, Nevozhay, Dmitry, additional, Ngwa, Wilfred, additional, Payne, J Donald, additional, Penninckx, Sébastien, additional, Porcel, Erika, additional, Prise, Kevin M, additional, Rabus, Hans, additional, Ridwan, Sharif M, additional, Rudek, Benedikt, additional, Sanche, Léon, additional, Singh, Bijay, additional, Smilowitz, Henry M, additional, Sokolov, Konstantin V, additional, Sridhar, Srinivas, additional, Stanishevskiy, Yaroslav, additional, Sung, Wonmo, additional, Tillement, Olivier, additional, Virani, Needa, additional, Yantasee, Wassana, additional, and Krishnan, Sunil, additional
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- 2020
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16. Theranostic nanoplatforms for treatment and diagnosis of rectal and colon cancer: a brief review
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Gholami, Yaser Hadi, primary and Engel, Alexander, additional
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- 2018
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17. Toward Personalized Dosimetry with 32 P Microparticle Therapy for Advanced Pancreatic Cancer
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Gholami, Yaser Hadi, primary, Wilson, Nicole, additional, James, David, additional, and Kuncic, Zdenka, additional
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- 2017
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18. A unique alpha dosimetry technique using Gafchromic EBT3®film and feasibility study for an activity calibrator for alpha-emitting radiopharmaceuticals
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Mukherjee, Bhaskar, primary, Gholami, Yaser H, additional, Bhonsle, Uday, additional, Hentschel, Reinhard, additional, and Khachan, Joseph, additional
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- 2015
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19. On the footprint of anisotropy on isotropic full waveform inversion: the Valhall case study
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Prieux, Vincent, Brossier, Romain, Gholami, Yaser, Operto, Stéphane, Virieux, Jean, Barkved, O.I., Kommedal, J.H., Géoazur (GEOAZUR 6526), Institut de Recherche pour le Développement (IRD)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Université Nice Sophia Antipolis (1965 - 2019) (UNS), COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de la Côte d'Azur, COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Université Côte d'Azur (UCA)-Université Côte d'Azur (UCA)-Centre National de la Recherche Scientifique (CNRS), Risques (Risques), Laboratoire de Géophysique Interne et Tectonophysique (LGIT), Observatoire des Sciences de l'Univers de Grenoble (OSUG), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Laboratoire Central des Ponts et Chaussées (LCPC)-Centre National de la Recherche Scientifique (CNRS)-Observatoire des Sciences de l'Univers de Grenoble (OSUG), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Laboratoire Central des Ponts et Chaussées (LCPC)-Centre National de la Recherche Scientifique (CNRS), SEISCOPE consortium, Observatoire de la Côte d'Azur, Université Côte d'Azur (UCA)-Université Côte d'Azur (UCA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Nice Sophia Antipolis (... - 2019) (UNS), Université Côte d'Azur (UCA)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS), Risques, Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Joseph Fourier - Grenoble 1 (UJF)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Joseph Fourier - Grenoble 1 (UJF)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Laboratoire Central des Ponts et Chaussées (LCPC)-Institut des Sciences de la Terre (ISTerre), Université Grenoble Alpes (UGA)-Centre National de la Recherche Scientifique (CNRS)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-PRES Université de Grenoble-Institut de recherche pour le développement [IRD] : UR219-Institut national des sciences de l'Univers (INSU - CNRS)-Institut Français des Sciences et Technologies des Transports, de l'Aménagement et des Réseaux (IFSTTAR)-Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS)-PRES Université de Grenoble-Institut de recherche pour le développement [IRD] : UR219-Institut Français des Sciences et Technologies des Transports, de l'Aménagement et des Réseaux (IFSTTAR)-Observatoire des Sciences de l'Univers de Grenoble (OSUG), Université Grenoble Alpes (UGA)-Centre National de la Recherche Scientifique (CNRS)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-PRES Université de Grenoble-Institut de recherche pour le développement [IRD] : UR219-Institut national des sciences de l'Univers (INSU - CNRS)-Institut Français des Sciences et Technologies des Transports, de l'Aménagement et des Réseaux (IFSTTAR)-Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS)-PRES Université de Grenoble-Institut de recherche pour le développement [IRD] : UR219-Institut Français des Sciences et Technologies des Transports, de l'Aménagement et des Réseaux (IFSTTAR), BP Norge, BP NORGE, Institut de Recherche pour le Développement (IRD)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Université Nice Sophia Antipolis (... - 2019) (UNS), Université Côte d'Azur (UCA)-Université Côte d'Azur (UCA)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de la Côte d'Azur, Université Côte d'Azur (UCA)-Centre National de la Recherche Scientifique (CNRS), Université Côte d'Azur (UCA)-COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Université Côte d'Azur (UCA)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Central des Ponts et Chaussées (LCPC)-Observatoire des Sciences de l'Univers de Grenoble (OSUG), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Centre National de la Recherche Scientifique (CNRS)-Laboratoire Central des Ponts et Chaussées (LCPC)-Observatoire des Sciences de l'Univers de Grenoble (OSUG), and Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Centre National de la Recherche Scientifique (CNRS)
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Computational seismology ,Controlled source seismology ,Seismic tomography ,Wave propagation ,[SDU.STU.GP]Sciences of the Universe [physics]/Earth Sciences/Geophysics [physics.geo-ph] ,[SDU.STU]Sciences of the Universe [physics]/Earth Sciences ,Inverse theory ,Seismic anisotropy - Abstract
International audience; The validity of isotropic approximation to perform acoustic full waveform inversion (FWI) of real wide-aperture anisotropic data can be questioned due to the intrinsic kinematic inconsistency between short- and large-aperture components of the data. This inconsistency is mainly related to the differences between the vertical and horizontal velocities in vertical-transverse isotropic (VTI) media. The footprint of VTI anisotropy on 2-D acoustic isotropic FWI is illustrated on a hydrophone data set of an ocean-bottom cable that was collected over the Valhall field in the North Sea. Multiscale FWI is implemented in the frequency domain by hierarchical inversions of increasing frequencies and decreasing aperture angles. The FWI models are appraised by local comparison with well information, seismic modelling, reverse-time migration (RTM) and source-wavelet estimation. A smooth initial VTI model parameterized by the vertical velocity V0 and the Thomsen parameters δ and ε were previously developed by anisotropic reflection traveltime tomography. The normal moveout (inline image) and horizontal (inline image) velocity models were inferred from the anisotropic models to perform isotropic FWI. The VNMO models allows for an accurate match of short-spread reflection traveltimes, whereas the Vh model, after updating by first-arrival traveltime tomography (FATT), allows for an accurate match of first-arrival traveltimes. Ray tracing in the velocity models shows that the first 1.5 km of the medium are sampled by both diving waves and reflections, whereas the deeper structure at the reservoir level is mainly controlled by short-spread reflections. Starting from the initial anisotropic model and keeping fixed δ and ε models, anisotropic FWI allows us to build a vertical velocity model that matches reasonably well the well-log velocities. Isotropic FWI is performed using either the NMO model or the FATT model as initial model. In both cases, horizontal velocities are mainly reconstructed in the first 1.5 km of the medium. This suggests that the wide-aperture components of the data have a dominant control on the velocity estimation at these depths. These high velocities in the upper structure lead to low values of velocity in the underlying gas layers (either equal or lower than vertical velocities of the well log), and/or a vertical stretching of the structure at the reservoir level below the gas. This bias in the gas velocities and the mispositioning in depth of the deep reflectors, also shown in the RTM images, are required to match the deep reflections in the isotropic approximation and highlight the footprint of anisotropy in the isotropic FWI of long-offset data. Despite the significant differences between the anisotropic and isotropic FWI models, each of these models produce a nearly-equivalent match of the data, which highlights the ill-posedness of acoustic anisotropic FWI. Hence, we conclude with the importance of considering anisotropy in FWI of wide-aperture data to avoid bias in the velocity reconstructions and mispositioning in depth of reflectors. Designing a suitable parameterization of the VTI acoustic FWI is a central issue to manage the ill-posedness of the FWI.
- Published
- 2011
20. Toward Personalized Dosimetry with 32P Microparticle Therapy for Advanced Pancreatic Cancer.
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Gholami, Yaser Hadi, Wilson, Nicole, James, David, and Kuncic, Zdenka
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PANCREATIC cancer treatment , *INDIVIDUALIZED medicine , *RADIATION dosimetry , *RADIOISOTOPES , *MONTE Carlo method - Abstract
Purpose: To develop a Monte Carlo model for patient-specific dosimetry of 32P microparticle localized internal radionuclide therapy for advanced pancreatic cancer.Methods and Materials: Spherical tumor geometries and a pancreatic phantom were modeled, as well as different 3-dimensional non-uniform clinical pancreatic geometries based on patient-specific ultrasound images. The dosimetry simulations modeled the dose distribution due to the energy spectrum of emitted beta particles.Results: The average dose for small (3-cm diameter) and large (6-cm diameter) spherical tumors was 111 Gy (for 7.6 MBq administered activity) and 128 Gy (for 58 MBq), respectively. For the clinical 3-dimensional geometries, on the basis of patient data, the mean doses delivered to the tumor were calculated to be in the range 102 to 113 Gy, with negligible dose to the pancreas for the smallest tumor volumes. The calculated dose distributions are highly non-uniform. For the largest tumor studied, the pancreas received approximately 6% of the tumor dose (5.7 Gy). Importantly, we found that because the smallest tumor studied exhibited the most dynamic changes in volume in response to the treatment, the dose to tumor and pancreas is significantly underestimated if a static tumor volume is assumed.Conclusions: These results demonstrate the dosimetry of 32P microparticle localized internal radionuclide therapy for pancreatic cancer and the possibility of developing personalized treatment strategies. The results also highlight the importance of considering the effects of non-uniform dose distributions and dynamic change of tumor mass during treatment on the dosimetry of the tumor and critical organs. [ABSTRACT FROM AUTHOR]- Published
- 2017
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21. Which parameterization is suitable for acoustic vertical transverse isotropic full waveform inversion? Part 2: Synthetic and real data case studies from Valhall
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Gholami, Yaser, primary, Brossier, Romain, additional, Operto, Stéphane, additional, Prieux, Vincent, additional, Ribodetti, Alessandra, additional, and Virieux, Jean, additional
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- 2013
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22. Which parameterization is suitable for acoustic vertical transverse isotropic full waveform inversion? Part 1: Sensitivity and trade-off analysis
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Gholami, Yaser, primary, Brossier, Romain, additional, Operto, Stéphane, additional, Ribodetti, Alessandra, additional, and Virieux, Jean, additional
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- 2013
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23. A unique alpha dosimetry technique using Gafchromic EBT3® film and feasibility study for an activity calibrator for alpha-emitting radiopharmaceuticals.
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MUKHERJEE, BHASKAR, GHOLAMI, YASER H., BHONSLE, UDAY, HENTSCHEL, REINHARD, and KHACHAN, JOSEPH
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RADIATION dosimetry , *RADIOPHARMACEUTICALS , *RADIATION-sensitizing agents , *OPACITY (Optics) , *DENSITOMETERS (Optical detectors) - Abstract
Objective: To develop an alpha dosimetry technique for activity calibration of alpha-emitting radiopharmaceuticals using the Gafchromic EBT3 (Gaf-EBT3) radio chromic film (International Speciality product, Wayne, NJ). Methods: The Gaf-EBT3 has a tissue equivalent radiosensitive layer (approximately 28p,m) sandwiched between two 100-μm thick polyester sheaths, thereby making it insensitive to alpha particles. We have split a Gaf-EBT3 sheet using a surgical scalpel to remove one of the polyester protective layers and covered the radiosensitive layer with thin Mylar* foil (Goodfellow Cambridge Limited, Huntingdon, UK) (2.5μm). Small pieces of modified film were exposed at contact with a 560-Bq thin 241Am source for 5, 10, 24 and 94 h. The optical density of the films was evaluated using an optical densitometer. The alpha energy spectra of the 241Am source were recorded using a Si(Li) surface barrier detector. Results: Time-integrated specific alpha surface activity ( kBq cm-2h) was represented as a function of optical density. Conclusion: By removing one of the 100 μm thick polyester protective layers, the authors have modified the Gaf- EBT3 film to a sensitive alpha dosemeter. The calibration function relevant to a 241,Am reference source was evaluated from the optical densities of the dosemeter foils. Furthermore, calibration functions for important alpha emitters such as 223Ra, 225Ac or 210Bi were parameterized from the 241Am reference data. Advances in knowledge: The authors have developed and tested the principle of a clinical alpha dosemeter using Gaf-EBT3 radiochromic films originally developed for photon dosimetry. This novel, user-friendly technique could be implemented in quality assurance and calibration procedures of important alpha-emitting radiopharmaceuticals prior to their clinical applications. [ABSTRACT FROM AUTHOR]
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- 2015
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24. Comparison of radiobiological parameters for 90Y radionuclide therapy (RNT) and external beam radiotherapy (EBRT) in vitro.
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Gholami, Yaser H., Willowson, Kathy P., Forwood, Nicholas J., Harvie, Rozelle, Hardcastle, Nicholas, Bromley, Regina, Ryu, HyunJu, Yuen, Samuel, Howell, Viive M., Kuncic, Zdenka, and Bailey, Dale L.
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RADIOBIOLOGY , *RADIOISOTOPES , *RADIOTHERAPY , *IRRADIATION , *COLON cancer - Abstract
Background: Dose rate variation is a critical factor affecting radionuclide therapy (RNT) efficacy. Relatively few studies to date have investigated the dose rate effect in RNT. Therefore, the aim of this study was to benchmark 90Y RNT (at different dose rates) against external beam radiotherapy (EBRT) in vitro and compare cell kill responses between the two irradiation processes.Results: Three human colorectal carcinoma (CRC) cell lines (HT29, HCT116, SW48) were exposed to 90Y doses in the ranges 1-10.4 and 6.2-62.3 Gy with initial dose rates of 0.013-0.13 Gy/hr (low dose rate, LDR) and 0.077-0.77 Gy/hr (high dose rate, HDR), respectively. Results were compared to a 6-MV photon beam doses in the range from 1-9 Gy with constant dose rate of 277 Gy/hr. The cell survival parameters from the linear quadratic (LQ) model were determined. Additionally, Monte Carlo simulations were performed to calculate the average dose, dose rate and the number of hits in the cell nucleus.For the HT29 cell line, which was the most radioresistant, the α/β ratio was found to be ≈ 31 for HDR-90Y and ≈ 3.5 for EBRT. LDR-90Y resulting in insignificant cell death compared to HDR-90Y and EBRT. Simulation results also showed for LDR-90Y, for doses ≲ 3 Gy, the average number of hits per cell nucleus is ≲ 2 indicating insufficiently delivered lethal dose. For 90Y doses ≳
3 Gy the number of hits per nucleus decreases rapidly and falls below ≈ 2 after ≈ 5 days of incubation time. Therefore, our results demonstrate that LDR-90Y is radiobiologically less effective than EBRT. However, HDR-90Y at ≈ 56 Gy was found to be radiobiologically as effective as acute ≈ 8 Gy EBRT.Conclusion: These results demonstrate that the efficacy of RNT is dependent on the initial dose rate at which radiation is delivered. Therefore, for a relatively long half-life radionuclide such as 90Y, a higher initial activity is required to achieve an outcome as effective as EBRT. [ABSTRACT FROM AUTHOR] - Published
- 2018
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