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Sun Nuclear Corporation 2d ic profiler array
2d Ic Profiler Array, supplied by Sun Nuclear Corporation, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/2d+array+system/2d+ic+profiler+array/pmc12260257-121-7-11
Average 90 stars, based on 1 article reviews
2d ic profiler array - by Bioz Stars, 2026-09
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Article Title: Commissioning and clinical implementation of low dose dual‐field rotational TSET
Article Snippet: Monthly profile constancy was performed using the 2D IC Profiler array (Sun Nuclear Corporation, USA).

Article Title: Development of a quasi-3D dosimeter using radiochromic plastic for patient-specific quality assurance.
Article Snippet: Funding information National Research Foundation of Korea (NRF) funded by the Ministry of Education, Grant/Award Number, Grant/Award Number: 2019K1A3A1A80113183; National Research Foundation of Korea (NRF) funded by the Ministry of Science and ICT, Grant/Award Number, Grant/Award Number: 2021R1I1A1A01059845 Abstract Background: Patient-specific QA verification ensures patient safety and treatment by verifying radiation delivery and dose calculations in treatment plans for errors.. However, a two-dimensional (2D) dose distribution is insufficient for detecting information on the three-dimensional (3D) dose delivered to the patient.. In addition, 3D radiochromic plastic dosimeters (RPDs) such as PRESAGE® represent the volume effect in which the dosimeters have different sensitivities according to the size of the dosimeters.

Article Title: Beam data commissioning, validation and clinical implementation of SRS gyroscopic system.
Article Snippet: For patient-specific QA, an anthropomorphic phantom (RT Safe Inc), a 2D array (Sun Nuclear Corporation) and SciMoCaTM were used for 1D dose verification, 2D and 3D evaluation gamma assessment, respectively.

Article Title: Beam data commissioning, validation and clinical implementation of SRS gyroscopic system.
Article Snippet: A 2D high resolution array SRS MapCHECK® (Sun Nuclear Corporation), inserted into the StereoPHANTM phantom (Sun Nuclear Corporation) was used, providing a composite measurement that includes rotation of the gantry.

Article Title: 57th ANNUAL MEETING AND EXHIBITION.
Article Snippet: REVIEWERS J. Adamovics, H. Aerts, N. Agazaryan, E. Ahunbay, P. Alaei, A. Alessio, A. Altman, M. Andre, E. Angel, K. Antes, J. Antolak, F. Araki, G. Arbique, L. Archambault, M. Aristophanous, B. Arjomandy, S. Armato, B. Arnold, P. Aryal, M. Aspradakis, S. Avery, A. Badal, A. Badano, C. Baird, D. Bakalyar, P. Bakic, P. Balter, J. Battista, L. Beaulieu, G. Bednarz, R. Behling, C. Beltran, E. Bender, R. Berbeco, T. Bichay, J. Bissonnette, B. Blankenship, C. Bloch, W. Bolch, E. Boote, M. Bostani, S. Both, J. Bourland, S. Brady, I. Brezovich, K. Brock, D. Broga, S. Brown, K. Brown, J. Burmeister, J. Bushberg, J. Cai, D. Cao, Y. Cao, M. Cao, A. Carabe-Fernandez, D. Carlson, M. Chan, H. Chan, Z. Chang, J. Chang, S. Chang, Y. Chen, J. Chen, H. Chen, Q. Chen, G. Chen, Z. Chen, I. Chetty, K. Cheung, N. Childress, Y. Cho, S. Cho, J. Chow, E. Christodoulou, C. Chuang, G. Clarke, C. Clements, J. Clements, D. Cody, D. Connor, C. Coolens, R. Cormack, A. Corrao, O. Craciunescu, G. Cranmer-Sargison, J. Cunha, B. Curran, J. Daartz, M. Dahlbom, M. Danielsson, I. Das, G. David, J.. De Wyngaert, J. Deasy, A. Dekker, C. Delaney, J. DeMarco, M. Descovich, L. DeWerd, J. Deye, C. Diederich, S. Dieterich, G. Ding, Q. Diot, J. Dobbins, L. Dong, F. Dong, K. Drukker, W. D'Souza, W. Du, J. Ducote, E. Ehler, I. El Naqa, C. Esquivel, J. Evans, G. Ezzell, F. Fahey, B. Fahimian, K. Farahani, J. Farr, E. Feleppa, W. Feng, A. Fenster, K. Fetterly, V. Feygelman, M. Fix, J. Flanz, T. Flohr, D. Followill, J. Fontenot, E. Ford, R. Foster, J. Fowlkes, B. Fraass, P. Francescon, E. Frey, R. Fulkerson, H. Gao, O. Gayou, J. Gibbons, M. Giger, M. Gillin, E. Gingold, S. Glick, C. Glide-Hurst, S. Goddu, M. Goodsitt, J. Goodwin, J. Gordon, D. Gress, J. Grimm, X. Gu, H. Guan, M. Guerrero, F. Guo, A. Gutierrez, L. Hadjiiski, S. Hadley, J. Halama, X. Han, J. Hazle, K. Hendrickson, M. Herman, J. Hiatt, D. Hintenlang, E. Hipp, C. Holdsworth, M. Howard, R. Howell, D. Hristov, J. Hsieh, C. Hua, G. Hugo, K. Hulme, J. Humm, M. Hunt, Z. Huo, M. Huq, G. Ibbott, P. Imbergamo, D. Ionascu, E. Jackson, A. Jain, R. Jeraj, G. Jia, X. Jia, S. Jiang, J. Jin, J. Johnson, A. Jones, D. Jordan, M. Kachelriess, G. Kagadis, K. Kanal, H. Kang, R. Kapoor, S. Kappadath, A. Karellas, P. Keall, C. Keener, M. Kessler, G. Kim, Y. Kim, M. Kim, D. Kim, P. Kinahan, M. King, A. Kirov, E. Klein, T. Knoos, J. Kofler, J. Kruse, S. Kry, R. Kudchadker, Z. Labby, J. Lagendijk, K. Langen, U. Langner, R. LeClair, R. Lee, C. Lee, T. Lee, J. Lehmann, S. Leng, J. Lewis, X. Li, H. Li, X. Li, Y. Li, X. Li, G. Li, R. Li, S. Li, H. Li, J. Li, T. Li, K. Li, H. Li, H. Li, B. Libby, J. Limmer, T. Liu, C. Liu, B. Liu, W. Liu, C. Liu, H. Liu, X. Liu, T. LoSasso, D. Low, H. Lu, Z. Lu, W. Lu, G. Luxton, Y. Lyatskaya, C. Ma, J. Ma, L. MacDonald, R. MacDougall, J. MacFall, M. Madsen, G. Mageras, M. Mahesh, A. Maidment, G. Makrigiorgos, H. Malhotra, M. Mamalui-Hunter, P. Manser, A. Markovic, M. Martin, A. Mascia, J. Masten, R. Mather, K. Matthews, M. Matuszak, P. Mavroidis, O. Mawlawi, C. Mayo, S. McCullough, J. McDonough, K. McGee, S. McGuire, M. McKee, M. McKetty, M. McNitt-Gray, J. Mechalakos, M. Meineke, M. Meltsner, J. Meyer, T. Mian, M. Miften, D. Mihailidis, B. Miller, R. Miller, T. Mills, R. Miyaoka, V. Moiseenko, A. Molineu, S. Molloi, V. Montemayor, J. Moran, F. Mourtada, M. Moyers, S. Mutic, M. Nakamura, D. Nazareth, J. Nelson, W. Ngwa, K. Nie, R. Nishikawa, T. Nurushev, J. Nye, J. Oh, A. Olch, M. Oldham, L. Olsen, B. O'Neill, Z. Ouhib, N. Ozturk, H. Paganetti, H. Palmans, J. Palta, X. Pan, T. Pan, A. Panda, M. Pankuch, N. Papanikolaou, P. Parikh, S. Park, M. Park, S. Park, K. Parodi, G. Parraga, E. Parsai, A. Pasciak, V. Patel, W. Pavlicek, D. Pavord, N. Pelc, S. Pella, J.. Perks, J. Perl, P. Petti, M. Phillips, D. Pickens, T. Podder, M. Podgorsak, F. Poenisch, B. Pogue, R. Pooley, R. Price, A. Pugachev, T. Purdie, F. Ranallo, D. Rangaraj, K. Rasmussen, C. Reft, J. Reiff, I. Reiser, N. Remmes, L. Ren, S. Richard, S. Richardson, M. Rivard, S. Rivetti, D. Robinson, R. Rodgers, L. Rothenberg, D. Ruan, M. Rzeszotarski, J. Sabol, B. Sahiner, N. Sahoo, E. Sajo, M. Salehpour, B. Salter, V. Sathiaseelan, C. Saw, G. Sawakuchi, D. Scanderbeg, S. Schafer, M. Schell, J. Schewe, D. Schlesinger, T. Schmidt, D. Schofield, E. Schreibmann, B. Schueler, R. Schulte, I. Sechopoulos, J. Seco, J. Seibert, W. Sensakovic, C. Serago, J. Seuntjens, Y. Shao, G. Sharp, M. Sharpe, K. Sheng, D. Shepard, C. Shi, Y. Shu, J. Siebers, J. Siewerdsen, D. Simpkin, R. Sloboda, W. Smith, W. Smith, M. Snyder, J. Soen, E. Soisson, T. Solberg, J. Sonke, M. Speidel, J. St. Germain, R. Stafford, T. Stanescu, K. Stantz, G. Starkschall, J. Star-Lack, S. Stathakis, R. Staton, J. Stayman, S. Steciw, R. Stern, D. Stevens, R. Stewart, M. Su, T. Suh, M. Supanich, M. Svatos, D. Switzer, K. Taguchi, J. Tang, R. Tarver, M. Taylor, R. Ten Haken, R. Thomson, J. Timmer, J. Ting, D. Todor, J. Tomlinson, R. Tosh, A. Trofimov, B. Tsui, J. Unkelbach, F. Van den Heuvel, M. Vanderhoek, T. Varghese, S. Vedam, S. Vedantham, Y. Vinogradskiy, G. Virshup, D. Visvikis, A. Walz-Flannigan, L. Wang, D. Wang, J. Wang, A. Wang, J. Weaver, J. Weiser, D. Wells, R. Wendt, B. Whiting, K. Wijesooriya, C. Willis, T. Willoughby, B. Winey, J. Wong, E. Wong, A. Wroe, Q. Wu, H. Wu, P. Xia, Y. Xiao, L. Xing, T. Yamamoto, C. Yan, D. Yan, N. Yanasak, J. Yang, J. Yang, J. Yang, K. Yang, D. Yang, T. Yankeelov, S. Ye, S. Yee, K. Yenice, M. Yester, I. Yeung, B. Yi, F. Yin, E. Yorke, J. Yorkston, L. Yu, Y. Yu, C. Yu, M. Zaider, H. Zaidi, J. Zambelli, W. Zbijewski, O. Zeidan, D. Zhang, G. Zhang, D. Zhang, X. Zhang, B. Zhao, W. Zhao, Y. Zheng, H. Zhong, L. Zhu, X. Zhu, T. Zhu, X. Zhu, P. Zygmanski 3098 3098

Article Title: Technical Note: Dosimetric characterization of the dynamic beam flattening MLC sequence on a ring shaped, Jawless Linear Accelerator with double stacked MLC.
Article Snippet: Purpose: To characterize the dosimetric features and limitations of the dynamic beam flattening (DBF) on the Halcyon 2.0 linear accelerator (Varian Medical Systems).. Methods: A pre-defined multi-leaf collimator (MLC) sequence was introduced and used to flatten the 6MV flattening filter free (FFF) beam on the Halcyon 2.0.. Dosimetric characterizations of the flattened beams, including beam flatness, symmetry, percent depth dose (PDD), output factor and MU linearity, were investigated.

Imaging:

Article Title: Impact of Dosimetric Parameters on Interplay Effects in 6 MV Flattening Filter-Free Photon Beams to Treat Lung Cancer
Article Snippet: .. Robotic platform: The MotionSimXY/four-dimensional (4D) platform from Sun Nuclear Corporation, Melbourne, FL was a precision instrument designed to use together with the 2D diode array for quality assurance study of motion effects in radiation therapy imaging and delivery by moving a phantom through programmable motion patterns (an operating system same as MapCHECK2). ..

Produced:

Article Title: Impact of systematic MLC positional uncertainties on the quality of single‐isocenter multi‐target VMAT‐SRS treatment plans
Article Snippet: .. Moreover, the commercially available StereoPHAN phantom in combination with the SRS mapCHECK 2D diode array (both produced by Sun Nuclear Corp., Melbourne, FL) were used for plan verification of a challenging VMAT‐SRS case and results are compared with TPS‐calculated dose distributions obtained after changing the clinically used leaf offset parameter. ..



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Image Search Results


Signal amplitude from the CROSSmini detector with signal fitting and zoomed in views. Figures A, B and C, on the left, shows the signal amplitude from the CROSSmini detector of a spill duration for energy level 70.2, 150.2, and 228.7 MeV, respectively, with nominal beam current 8 MU/s. The red line represents the original signal from CROSSmini and the black line represents the piecewise fitting for the edges. On the right is the zoomed in view of the fitting. The piecewise fitting quantifies the risetime ( t rise ) and measured nominal beam current ( I 0 , measured ).

Journal: International Journal of Particle Therapy

Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

doi: 10.1016/j.ijpt.2026.101315

Figure Lengend Snippet: Signal amplitude from the CROSSmini detector with signal fitting and zoomed in views. Figures A, B and C, on the left, shows the signal amplitude from the CROSSmini detector of a spill duration for energy level 70.2, 150.2, and 228.7 MeV, respectively, with nominal beam current 8 MU/s. The red line represents the original signal from CROSSmini and the black line represents the piecewise fitting for the edges. On the right is the zoomed in view of the fitting. The piecewise fitting quantifies the risetime ( t rise ) and measured nominal beam current ( I 0 , measured ).

Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

Techniques:

Signal amplitude from the CROSSmini detector with signal fitting. shows the signal amplitude as a function of time measured by the CROSSmini detector and the piecewise fittings. Figures A, B, and C are measurements for energy level 70.2 MeV with nominal beam current 8, 14, and 20 MU/s, respectively. Figures D, E, and F are the measurements for energy level 228.7 MeV with nominal beam current 8, 14, and 20 MU/s, respectively.

Journal: International Journal of Particle Therapy

Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

doi: 10.1016/j.ijpt.2026.101315

Figure Lengend Snippet: Signal amplitude from the CROSSmini detector with signal fitting. shows the signal amplitude as a function of time measured by the CROSSmini detector and the piecewise fittings. Figures A, B, and C are measurements for energy level 70.2 MeV with nominal beam current 8, 14, and 20 MU/s, respectively. Figures D, E, and F are the measurements for energy level 228.7 MeV with nominal beam current 8, 14, and 20 MU/s, respectively.

Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

Techniques:

t rise comparison between analytical and measured. The blue and red plots represent the analytically derived t rise and CROSSmini measured t rise , respectively, across the various nominal beam current settings.

Journal: International Journal of Particle Therapy

Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

doi: 10.1016/j.ijpt.2026.101315

Figure Lengend Snippet: t rise comparison between analytical and measured. The blue and red plots represent the analytically derived t rise and CROSSmini measured t rise , respectively, across the various nominal beam current settings.

Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

Techniques: Comparison, Derivative Assay