BEGIN:VCALENDAR
VERSION:2.0
PRODID:-//CERN//INDICO//EN
BEGIN:VEVENT
SUMMARY:Diseño y validación de sistema de hipoxia para experimentos en r
 adiobiología
DTSTART;VALUE=DATE-TIME:20251029T094500Z
DTEND;VALUE=DATE-TIME:20251029T100000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28522@indico.ific.uv.es
DESCRIPTION:Speakers: Adrián Zazpe (Universidad Complutense de Madrid)\nI
 ntroducción. La hipoxia es una condición tumoral que dificulta la eficac
 ia de la radioterapia y exige modelos in vitro controlables y reproducible
 s. Presentamos una plataforma experimental compuesta por dos cámaras hip
 óxicas diseñadas y construidas in-house (una portátil y una de gran vol
 umen con guantes) y un modelo 1D de difusión de oxígeno para planificar 
 y validar exposiciones hipóxicas en ensayos biológicos.\n\nMétodos. La 
 cámara portátil permite transporte y sellado rápido y\, además\, posib
 ilita irradiar las muestras en su interior\, asegurando un entorno hipóxi
 co\; la cámara de guantes posibilita manipulación interna de las muestra
 s sin reoxigenación. El O₂ se monitoriza con un sensor óptico PicoO₂
  y con un LuminOx integrado a Arduino/BT para registro continuo. Se ha imp
 lementado un modelo explícito de difusión (Fick 1D) con condición super
 ficial dependiente del tiempo\, que distingue una fase de purga y una de r
 eposo. Este código de difusión se utiliza para determinar cuánto deben 
 permanecer las muestras dentro de la cámara (en función de la altura del
  medio) hasta alcanzar el nivel de O₂ objetivo. Se ha llevado a cabo un 
 análisis de sensibilidad de los parámetros del modelo (constante de difu
 sión\, altura del medio y discretización espacio-temporal). Para validac
 ión biológica se emplearon células de cáncer de mama humano MDA-MB-231
 \, que fueron irradiadas con fotones (¹³⁷Cs) con dosis entre 2.5–12.
 5 Gy en condiciones de normoxia (21%O₂) e hipoxia (4%O₂) y analizadas 
 en un ensayo clonogénico. \n\nResultados. La cámara portátil permite al
 canzar un nivel de hipoxia del 4% O₂ en aproximadamente 60 s y mantiene 
 la estabilidad por más de 3h\; la cámara de guantes permite alcanzar 4%O
 ₂ en 1 h 41 min y asegura una estabilidad hasta 8h sin volver a gasearla
 . El modelo de difusión 1D reprodujo los tiempos de establecimiento de hi
 poxia con desviaciones menores al 5% frente a mediciones directas en el me
 dio (PicoO₂). En el clonogénico\, las células hipoxicas mostraron mayo
 r supervivencia y morfología más alargada en comparación con las en nor
 moxia. Se estimó un Oxygen Enhancement Ratio (OER) ≈1.7 y no se observa
 ron diferencias significativas entre las curvas de supervivencia realizada
 s en la cámara portátil y en la cámara con guantes\n\nConclusiones. El 
 sistema de cámara dual\, junto con el modelo 1D\, permite generar y soste
 ner hipoxia fisiológica. El modelo cuantifica los tiempos de exposición 
 en función de la altura del medio\, con concordancia \n\nhttps://indico.i
 fic.uv.es/event/8181/contributions/28522/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28522/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Poster: The Physics of the Pupil: Age and Ethnicity Effects in Sta
 tic Mesopic Conditions
DTSTART;VALUE=DATE-TIME:20251028T155500Z
DTEND;VALUE=DATE-TIME:20251028T160000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28603@indico.ific.uv.es
DESCRIPTION:Speakers: MAME DIATOU TOURE SARR (UNIVERSIDAD COMPLUTENSE DE M
 ADRID)\, CELIA SANCHEZ RAMOS (Universidad Complutense de Madrid)\, VANESA 
 BLAZQUEZ SANCHEZ (Universidad Complutense de Madrid)\nPurpose:\nThis study
  aimed to compare static pupillometry under mesopic conditions between Eur
 opean\nand African populations\, given the limited data directly contrasti
 ng pupillary dimensions across\nethnic groups. Characterizing pupil diamet
 er is relevant in detecting ocular alterations\,\nparticularly in a multic
 ultural context. While age-related pupillary changes are well documented\n
 in Caucasian and Asian populations\, evidence in Africans is scarce. This 
 work establishes initial\nreference values for the Senegalese population a
 s a starting point for further studies.\nSettings:\nData were collected at
  three locations: Caucasian participants at the Optometry Clinic of the\nC
 omplutense University of Madrid\; Afro-Europeans (AFE\, African origin but
  lifelong residents in\nEurope) in the Lavapiés district of Madrid\; and 
 Africans (AFR) at Abass Ndao Hospital\, Dakar.\nThe study complied with th
 e Declaration of Helsinki.\nMethods:\nAnalytical cross-sectional observati
 onal study with 88 CAU\, 129 AFR\, and 78 AFE\, aged 18–75\nyears. All p
 rovided written informed consent. Static pupillometry was measured with th
 e Nidek\nHandyRef-K portable autorefractor-keratometer\; five measurements
  per participant by the same\nexaminer.\nResults:\n• Ethnic comparison: 
 mean pupil diameters: CAU 4.67 ± 0.7 mm\; AFR 5.11 ± 1.0 mm\;\nAFE 4.44 
 ± 1.0 mm (p 45\nyears groups (p > 0.05). Both AFR and AFE showed signific
 ant differences (p 45 years.\nConclusions:\nAfricans showed larger pupil d
 iameters compared to Caucasians and Afro-Europeans\, between\nwhom no sign
 ificant differences were observed. Age had no effect in Caucasians\, while
  both\nAfricans and Afro-Europeans showed decreasing diameters with age. T
 hese findings provide\nreference data for Senegalese populations and suppo
 rt further cross-ethnic research.\nKey words: Axial length\, Race\, Sex\, 
 Ocular Biometry\, Africans\, Caucasians\nReferences:\n1. Birren JE\, Caspe
 rson RC\, Botwinick J. Age changes in pupil size. Journal of\nGerontology.
  1950\;5(3):216-21.\n2. Winn B\, Whitaker D\, Elliott DB\, Phillips NJ. Fa
 ctors affecting light-adapted pupil size\nin normal human subjects. Invest
 igative ophthalmology & visual science.\n1994\;35(3):1132-7\n3. Tekin K\, 
 Sekeroglu MA\, Kiziltoprak H\, Doguizi S\, Inanc M\, Yilmazbas P. Static a
 nd\ndynamic pupillometry data of healthy individuals. Clin Exp Optom. 2018
 \nSep\;101(5):659-665. doi: 10.1111/cxo.12659. Epub 2018 Jan 21. PMID: 293
 5607\n\nhttps://indico.ific.uv.es/event/8181/contributions/28603/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28603/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Poster: EFECTO ESPECTRAL DE FILTRO SELECTIVO: CARACTERIZACIÓN COM
 PARATIVA ENTRE EMISIÓN DIGITAL Y REFLECTANCIA DEL PAPEL
DTSTART;VALUE=DATE-TIME:20251028T154000Z
DTEND;VALUE=DATE-TIME:20251028T154500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28602@indico.ific.uv.es
DESCRIPTION:Speakers: CARMEN MARTIN ARANDA (UNIVERSIDAD COMPLUTENSE DE MAD
 RID)\nEl uso de dispositivos digitales ha incrementado la exposición a fu
 entes de luz artificial con espectros distintos a los medios impresos. Muc
 has pantallas emiten un pico en la región azul del espectro visible(440-4
 60 nm)\, inexistente en el papel bajo iluminación normal(1). La luz azul\
 , por su mayor energía\, puede afectar a la fatiga ocular\, la supresión
  de melatonina y otros procesos biológicos(2). Para reducirla se emplean 
 filtros de absorbancia selectiva(3). Este trabajo compara la emisión espe
 ctral de una pantalla digital con y sin filtro frente a la reflectancia de
 l papel.\nPara la caracterización espectral del papel\, se dividió un fo
 lio en 9 áreas y se registraron mediciones espectrofotométricas en cada 
 una\, bajo una iluminación de 16.8cd/m² medida con luxómetro. Los valor
 es obtenidos se promediaron y se analizaron las longitudes de onda de 440 
 y 470nm principalmente.\nDe la misma forma\, la pantalla de un iPhone 13 s
 e dividió en 9 áreas\, realizándose mediciones en cada una con y sin fi
 ltro selectivo\, y con el brillo ajustado a tres niveles(mínimo\, medio y
  máximo). Los datos resultantes se promediaron para las mismas longitudes
  de onda de interés.\nLos resultados mostraron que la reflectancia del pa
 pel se mantuvo baja y estable en ambas longitudes de onda\, con una intens
 idad ≈700 cuentas\, en contraste con la pantalla digital\, cuya intensid
 ad de emisión se incrementó notablemente\, especialmente en 470nm\, alca
 nzando valores superiores a 10.000 cuentas con brillo máximo. La aplicaci
 ón del filtro de absorbancia selectiva redujo la intensidad emitida en es
 ta banda\, con descensos de alrededor del 10–20% según el nivel de bril
 lo\, mientras que en 440nm las diferencias fueron menores.\nLos resultados
  evidencian diferencia entre la emisión espectral de las pantallas digita
 les y la reflectancia del papel en la región de 460-470nm\, lo que refuer
 za la importancia de implementar medidas que limiten la exposición a esta
  franja del espectro durante el uso prolongado de pantallas\, en particula
 r cuando se utilizan con niveles altos de brillo.\n\nhttps://indico.ific.u
 v.es/event/8181/contributions/28602/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28602/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Production of medical radioisotopes using laser-plasma accelerator
 s
DTSTART;VALUE=DATE-TIME:20251029T111500Z
DTEND;VALUE=DATE-TIME:20251029T113000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28601@indico.ific.uv.es
DESCRIPTION:Speakers: Jose Benlliure (IFIC (CSIC - Universitat de Valencia
 ))\nThe development of novel medical imaging techniques such as PET (Posit
 ron Emission Tomography) and SPECT (Single-Photon Emission Computed Tomogr
 aphy) has increased the demand for nuclear radioisotopes in medical diagno
 stics. Currently\, the production of radioisotopes for medical imaging and
  treatment is primarily carried out using conventional accelerators (cyclo
 trons) and dedicated nuclear reactors. In the case of positron emitters us
 ed in PET imaging\, the current approach involves producing positron radio
 tracers at large facilities that are responsible for supplying radioisotop
 es on a regional or national scale. Due to the cost of production centres\
 , accelerators\, radio-pharmacies and\, in particular\, radiation shieldin
 g\, the economic viability of these centres depends on mass-producing sing
 le doses for distribution to as many hospitals and research centres as pos
 sible. As a result of this regional scope\, commercial production of PET r
 adioisotopes is mainly limited to 18F\, which has a half-life of around 11
 0 minutes and can therefore endure the time required for production\, post
 -processing and distribution. Consequently\, the production of a limited n
 umber of doses of shorter-lived radioisotopes\, such as 11C (with a half-l
 ife of ~20 min)\, 13N (with a half-life of ~10 min) and 15O (with a half-l
 ife of ~2 min)\, is generally beyond the capabilities of these facilities.
 \n\nOver the last few decades\, the use of ultra-short\, ultra-intense las
 ers for radioisotope production has been proposed as a cost-efficient alte
 rnative for the on-demand production of single doses of short-lived radioi
 sotopes. Through the target normal sheath acceleration (TNSA) mechanism\, 
 ultra-intense laser pulses (I > 10¹⁸ W/cm²) impinging on a micrometre-
 thick target can result in the acceleration of ion beams to energies of se
 veral tens of MeV. The nature and properties of this laser-induced acceler
 ation process overcome the main constraint of conventional production faci
 lities. As the laser-target interaction occurs over a micrometre-scale dis
 tance\, the shielding requirements are much lower than for nuclear reactor
 s or accelerators. Thus\, laser systems of this class become significantly
  more affordable for hospitals\, clinics and research centres. These facil
 ities could then produce radioisotopes on demand and explore shorter-lived
  emitters that are not currently produced.\n\nIn this talk\, we will prese
 nt our key accomplishments in this area. In particular\, we will demonstra
 te our ability to produce 11C using the 11B(p\,n)11C reaction with activat
 ion levels exceeding 4 MBq in a recent experiment conducted at CLPU in Sal
 amanca.\n\nhttps://indico.ific.uv.es/event/8181/contributions/28601/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28601/
END:VEVENT
BEGIN:VEVENT
SUMMARY:PTCOG 2025 award: Mapping intratumoral heterogeneity through PET-d
 erived washout and deep learning after proton therapy
DTSTART;VALUE=DATE-TIME:20251029T083000Z
DTEND;VALUE=DATE-TIME:20251029T090000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28517@indico.ific.uv.es
DESCRIPTION:Speakers: Pablo Cabrales (Grupo de Física Nuclear and IPARCOS
 \, Universidad Complutense de Madrid)\nThe distribution of produced isotop
 es during proton therapy can be imaged with Positron Emission Tomography (
 PET) to verify dose delivery. However\, biological washout\, driven by tis
 sue-dependent processes such as perfusion and cellular metabolism\, reduce
 s PET signal-to-noise ratio (SNR) and limits quantitative analysis. In thi
 s work\, we propose an uncertainty-aware deep learning framework to improv
 e the estimation of washout parameters in post-proton therapy PET\, not on
 ly enabling accurate correction for washout effects\, but also mapping int
 ratumoral heterogeneity as a surrogate marker of tumor status and treatmen
 t response. We trained the models on Monte Carlo-simulated data from eight
  head-and-neck cancer patients\, and tested them on four additional head-a
 nd-neck and one liver patient. Each patient was represented by 75 digital 
 twins with distinct tumoral washout dynamics and imaged 15 minutes after t
 reatment\, when slow washout components dominate. We also introduced "wash
 ed-out" maps\, quantifying the contribution of medium and fast washout com
 ponents to the loss in activity between the end of treatment and the start
  of PET imaging. Trained models significantly improved resolution and accu
 racy\, reducing average absolute errors by 60% and 28% for washout rate an
 d washed-out maps\, respectively. For intratumoral regions as small as 5 m
 L\, errors predominantly fell below thresholds for differentiating vascula
 r status\, and the models generalized across anatomical areas and acquisit
 ion delays. This study shows the potential of deep learning in post-proton
  therapy PET to non-invasively map washout kinetics and reveal intratumora
 l heterogeneity\, supporting dose verification\, tumor characterization\, 
 and treatment personalization. The framework is currently being validated 
 using phantom experiments at Clínica Universidad de Navarra\, Spain\, and
  clinical data at Massachusetts General Hospital\, USA. The implementation
  code is available at https://github.com/pcabrales/ppw.\n\nhttps://indico.
 ific.uv.es/event/8181/contributions/28517/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28517/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Pick-up badges
DTSTART;VALUE=DATE-TIME:20251027T093000Z
DTEND;VALUE=DATE-TIME:20251027T101000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28757@indico.ific.uv.es
DESCRIPTION:https://indico.ific.uv.es/event/8181/contributions/28757/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28757/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Closing session
DTSTART;VALUE=DATE-TIME:20251029T113000Z
DTEND;VALUE=DATE-TIME:20251029T114000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28756@indico.ific.uv.es
DESCRIPTION:Speakers: Gabriela Llosá (IFIC (CSIC-UV))\nhttps://indico.ifi
 c.uv.es/event/8181/contributions/28756/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28756/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Bridging physics\, biology\, and clinic: a forward view of UHDR ra
 diotherapy and VHEE FLASH
DTSTART;VALUE=DATE-TIME:20251028T140000Z
DTEND;VALUE=DATE-TIME:20251028T144500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28552@indico.ific.uv.es
DESCRIPTION:Speakers: Costanza Panaino (University of Manchester)\nhttps:/
 /indico.ific.uv.es/event/8181/contributions/28552/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28552/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Range Verification in Particle Therapy for Preclinical Research Us
 ing PET
DTSTART;VALUE=DATE-TIME:20251028T100000Z
DTEND;VALUE=DATE-TIME:20251028T104500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28551@indico.ific.uv.es
DESCRIPTION:Speakers: Giulio Lovatti (Ludwig Maximilian University of Muni
 ch\, Department of Physics )\nhttps://indico.ific.uv.es/event/8181/contrib
 utions/28551/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28551/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Expanding the Toolbox for Theranostics: From Chemical Probes to Re
 porter Genes
DTSTART;VALUE=DATE-TIME:20251028T080000Z
DTEND;VALUE=DATE-TIME:20251028T084500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28550@indico.ific.uv.es
DESCRIPTION:Speakers: Susana Carregal Romero (CIC biomaGUNE)\nhttps://indi
 co.ific.uv.es/event/8181/contributions/28550/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28550/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Hacia una integración eficiente de tecnologías de imagen y terap
 ias por radiación en la práctica clínica
DTSTART;VALUE=DATE-TIME:20251027T140000Z
DTEND;VALUE=DATE-TIME:20251027T144500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28549@indico.ific.uv.es
DESCRIPTION:Speakers: Montserrat Carles Farina (Hospital Universitario La 
 Fe)\nhttps://indico.ific.uv.es/event/8181/contributions/28549/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28549/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Protonterapia en la Comunidad Valenciana. ¿Cuándo y cómo?
DTSTART;VALUE=DATE-TIME:20251027T103000Z
DTEND;VALUE=DATE-TIME:20251027T111500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28548@indico.ific.uv.es
DESCRIPTION:Speakers: Francisco Javier Celada Álvarez (Hospital Universit
 ario y Politécnico La Fe)\nhttps://indico.ific.uv.es/event/8181/contribut
 ions/28548/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28548/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Real-Time Proton Therapy Monte Carlo Simulations in Highly Paralle
 lised Systems
DTSTART;VALUE=DATE-TIME:20251028T151500Z
DTEND;VALUE=DATE-TIME:20251028T153000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28529@indico.ific.uv.es
DESCRIPTION:Speakers: Declan  Garvey (Instituto de Física Corpuscular)\nW
 hen it comes to treating cancer in critical regions such as the brain\, pr
 ecision is vital\, as reducing margins of error can significantly decrease
  negative side effects of treatment. Due to their finite range and deposit
 ion profile\, protons are an ideal candidate for this sort of treatment. H
 owever\, this finite range of protons is both their biggest advantage and 
 their biggest challenge\, as a minor miscalculation of penetration depth c
 an have severe consequences for the patient. As such\, continuous monitori
 ng of the proton energy deposition throughout treatment is of the upmost i
 mportance. A class of continuous monitoring techniques that has shown grea
 t promise in recent years is prompt-gamma ray detection. Prompt-gamma ray 
 detection functions on the principle that\, as protons penetrate the patie
 nt\, gamma rays are emitted along their path. Currently\, this method depe
 nds largely on Monte Carlo simulations\, which is restricting as these sim
 ulations are very computationally expensive. \nIn practice\, a treatment o
 f ~1000 spots typically lasts a few minutes\, whereas the simulation of th
 is treatment typically takes several hours. In cases where the continuous 
 monitoring results during treatment do not match the simulation\, it becom
 es completely impractical to re-simulate scenarios in search of the discre
 pancy between simulated and true treatment parameters. Therefore\, if the 
 computation time of a single spot could be reduced to approximately one-te
 nth of a second\, real-time re-simulation of results would be possible. To
  achieve such simulation speeds\, standard Monte Carlo simulations have be
 en shown to be insufficient\, and as such simulation with a high degree of
  parallelisation is the theoretical solution.\nThe goal of this project is
  to provide an open source solution to this problem. The code is currently
  being written in SYCL (SYstem-wide Compute Language)\, a hardware-agnosti
 c language which creates parallelised software that can be ran on either G
 PU or CPU with minimal overhead. The present simulation model has shown gr
 eat promise in terms of computation times and accuracy when tested on a wa
 ter phantom. The code has shown an increase in computation speed by severa
 l orders of magnitude for energy deposition and depth of penetration calcu
 lations when compared with TOPAS\, whilst maintaining a maximal deviation 
 of 0.5 mm in 90% drop-off position (R90) and 3 MeV for total energy deposi
 tion across the full treatment range. These results are thought to be impr
 ovable with a more complex model and the appropriate optimisations. The fu
 ture aim of this project is to gradually increase simulation complexity by
  incorporating more processes such as gamma-ray transport and detection in
  an external scintillation detector\, whilst maintaining code clarity and 
 structure for possible public contributions\, and continuously simplifying
  user experience.\n\nhttps://indico.ific.uv.es/event/8181/contributions/28
 529/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28529/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Asamblea
DTSTART;VALUE=DATE-TIME:20251028T171000Z
DTEND;VALUE=DATE-TIME:20251028T174000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28559@indico.ific.uv.es
DESCRIPTION:https://indico.ific.uv.es/event/8181/contributions/28559/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28559/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Networking
DTSTART;VALUE=DATE-TIME:20251027T163000Z
DTEND;VALUE=DATE-TIME:20251027T173000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28558@indico.ific.uv.es
DESCRIPTION:https://indico.ific.uv.es/event/8181/contributions/28558/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28558/
END:VEVENT
BEGIN:VEVENT
SUMMARY:FLIP-HEDOS: modelo hemodinámico personalizado a cada paciente par
 a cuantificar dosis en sangre circulante durante tratamientos de radiotera
 pia
DTSTART;VALUE=DATE-TIME:20251029T104500Z
DTEND;VALUE=DATE-TIME:20251029T110000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28532@indico.ific.uv.es
DESCRIPTION:Speakers: Marina García-Cardosa (Universidad de Navarra)\n**I
 ntroducción:** La dosimetría sanguínea en radioterapia de protones o fo
 tones representa un desafío significativo debido al comportamiento dinám
 ico de la sangre como órgano a riesgo. Cuantificar con precisión la dosi
 s recibida por la sangre circulante de un paciente específico es esencial
  para poder minimizar efectos adversos en los pacientes. Por ello\, presen
 tamos FLIP-HEDOS\, un modelo innovador que integra el método FLIP (*FLow 
 and Irradiation Personalized*) con la herramienta computacional HEDOS (*HE
 matological DOSe*).\n\n**Material y métodos:** La metodología FLIP cuant
 ifica la dosis que recibe la sangre circulante de un paciente específico 
 haciendo uso de la segmentación obtenida de sus grandes vasos y el corres
 pondiente campo de velocidad de la sangre medido a partir de la RM de cont
 raste de fase. Por el contrario\, HEDOS es un modelo compartimental están
 dar y estocástico que simula la distribución espacio-temporal de las par
 tículas de sangre\, *blood particles* (BPs)\, en los órganos de todo el 
 cuerpo. Así\, FLIP se integra como un módulo arterial y venoso específi
 co del paciente que considera la localización del tumor\, el caudal de lo
 s vasos y el volumen vascular para mantener el sistema en equilibrio. Asum
 iendo un volumen total sanguíneo de 5.3 L\, se discretiza en BPs de 1 mm
 ³. Las BPs simuladas viajan por los módulos de FLIP con un enfoque Lagra
 ngiano a lo largo de trayectorias de flujo definidas por el campo de veloc
 idad\, pero se mueven estocásticamente a través de los compartimentos de
  HEDOS basándose en distribuciones temporales de tránsito predeterminada
 s. La simulación de la distribución espaciotemporal de las BPs nos permi
 tió acumular la dosis en sangre\, haciendo uso del conjunto de distribuci
 ones 3D de dosis y de los tiempos de irradiación de los haces. La cohorte
  de pacientes presenta tumores en regiones de tórax-abdomen y cabeza-cuel
 lo.\n\n**Resultados:** FLIP-HEDOS cuantifica la dosis recibida por cada BP
  (Figura 1) y verifica el número de veces que una BP ha (re)visitado la v
 asculatura específica del paciente (Tabla 1).\n\n**Discusión:** Los resu
 ltados indican que\, con independencia de la modalidad de radioterapia\, s
 i el tumor está cerca de grandes vasos (tumor de páncreas e hígado\, Fi
 gura 1)\, un mayor volumen de sangre recibirá dosis superiores a un umbra
 l de 0.1 Gy\, lo que puede causar daños en los linfocitos. Además\, se o
 bservó que el número de veces que una BP visita el módulo FLIP aumenta 
 con el tiempo total de tratamiento.\n\n**Conclusiones:** FLIP-HEDOS puede 
 ser crucial en escenarios clínicos en los que los tumores están cerca de
  la vasculatura\, el volumen de los vasos circundantes es comparable al vo
 lumen del tumor y el tiempo total de irradiación es extenso. Este modelo 
 podría permitir dosimetrías más precisas y personalizadas.\n\nhttps://i
 ndico.ific.uv.es/event/8181/contributions/28532/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28532/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Mejora dosimétrica en tratamientos de radioterapia adaptativa gui
 ada por resonancia magnética (MRgRT)
DTSTART;VALUE=DATE-TIME:20251029T103000Z
DTEND;VALUE=DATE-TIME:20251029T104500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28534@indico.ific.uv.es
DESCRIPTION:Speakers: Teresa Cuenca (Bandín)\n**Objetivo**\nLa imagen mé
 dica en radioterapia mejora la optimización de los tratamientos mediante 
 adaptación off y on-line. La radioterapia guiada por resonancia magnétic
 a (MRgRT) supone una revolución\, permitiendo seguir el tumor en tiempo r
 eal. Aun así\, los sistemas actuales no permiten cuantificar la dosis rec
 ibida en el tumor debido a sus movimientos.\nEl objetivo es usar imágenes
  de un equipo de MRgRT para el seguimiento del tumor y\, mediante un proce
 so de re-cálculo de la dosis en nuevas geometrías deformadas y su acumul
 ación posterior\, estimar la dosis recibida. Esta dosis se compara con un
 a dosimetría en un equipo convencional.\n**Material/Métodos**\nEl equipo
  empleado (Elekta Unity) combina LINAC y Resonancia Magnética (RM). Media
 nte el algoritmo *Comprehensive Motion Management* (CMM) toma imágenes RM
  2D en tiempo real (6fps) y rastrea la posición tumoral. El CMM pausa el 
 haz si el tumor sobresale de unos márgenes establecidos (3mm en cada dire
 cción en el caso analizado). Las posiciones se almacenan en un fichero an
 alizable. Estos datos los separamos en dos secuencias: completa (movimient
 o completo del tumor) y restringida (dentro de márgenes).\nCon el planifi
 cador RayStation se generaron RM sintéticas simulando el movimiento del t
 umor\, deformándolo en la RM diaria con Registro Deformable (ANACONDA) a 
 las posiciones obtenidas. Se calculó la matriz de dosis en cada RM con el
  planificador MONACO. Finalmente\, se acumuló la dosis recibida en cada f
 racción en RayStation ponderando cada RM según el tiempo que el tumor es
 tuvo en esa posición. Así\, calculamos la dosis recibida en el caso rest
 ringido (MRgRT). Esta dosis se compara con la recibida en un LINAC convenc
 ional\, sin adaptación ni guiado (movimiento completo).\nCon este método
  se analizó un sarcoma cardiaco de 68cc en el pre-tratamiento. Se realiz
 ó una secuencia T2 para la delimitación\, planificando una dosimetría d
 e 35Gy en 5 fracciones que se adaptó diariamente a los cambios anatómico
 s.\n**Resultados**\nLa figura 1(a) muestra las posiciones del centroide en
  la serie completa en una matriz de vóxeles de 1.5mm de lado del primer d
 ía de tratamiento\, y la 1(b) la serie restringida (margen de 3mm). El ha
 z estuvo activo un 69% del tiempo de irradiación.\nLas dosis obtenidas en
  el caso MRgRT\, figura 2(a)\, y el convencional\, figura 2(b)\, difieren 
 en la zona posterior del tumor y próxima al esófago.\nSi comparamos hist
 ogramas (figura 3) del caso MRgRT (línea continua) y del convencional (l
 ínea discontinua)\, se observa que en el segundo la dosis en GTV sería u
 n 16% inferior.\n**Conclusión**\nProponemos un método para estimar la do
 sis recibida en una fracción con los movimientos registrados en un equipo
  de MRgRT. Lo hemos aplicado a un sarcoma cardíaco\, analizando la difere
 ncia entre dosis planificada y depositada.\nEsta herramienta evidencia que
  en patologías sólo visibles en RM y afectadas por movimiento interno de
  órganos se experimenta una degradación dosimétrica si no se aplican es
 trategias de adaptación y guiado por imagen.\n\nhttps://indico.ific.uv.es
 /event/8181/contributions/28534/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28534/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Development of Compton camera imaging and dosimetry techniques for
  radionuclide therapies
DTSTART;VALUE=DATE-TIME:20251029T110000Z
DTEND;VALUE=DATE-TIME:20251029T110500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28539@indico.ific.uv.es
DESCRIPTION:Speakers: Matthew Strugari (IFIC/CSIC)\nTargeted radionuclide 
 therapy (TRT) with alpha-emitters is rapidly gaining importance in oncolog
 y due to the high linear energy transfer and short range of alpha particle
 s\, enabling effective tumour control while sparing healthy tissue. Howeve
 r\, accurate dosimetry remains a major challenge\, as conventional nuclear
  medicine imaging is not optimized to determine radionuclide distributions
  from high-energy photons commonly associated with alpha decay. In therano
 stics\, $^{212}$Pb has seen increasing therapeutic use due to its favourab
 le chemistry\, half-life\, and decay properties\, but dosimetry relies on 
 $^{203}$Pb as an imaging surrogate\, providing an indirect and limited est
 imate of the true $^{212}$Pb biodistribution. This work investigates the f
 easibility of Compton camera imaging for TRT verification with improved ac
 curacy.\n\nThe IRIS group has developed imaging and dosimetry methods for 
 radiotherapy applications using the MACACO III+ Compton camera\, which is 
 well-suited for high-energy photons. A model of the camera has been implem
 ented in GATE 10\, enabling efficient simulations with recent GATE feature
 s. To support correlation of detected photons and absorbed dose\, dose poi
 nt kernels for the $^{212}$Pb decay chain were calculated with 1E6 primari
 es in a 13.38$\\\,$mm water sphere\, equal to 1.2$\\times$ the CSDA range 
 of the maximum-energy $\\beta^-$ emission. The therapeutic range $X_{90}$ 
 was defined as the radius containing 90% of energy deposited\, and emissio
 n profiles were benchmarked with NuDat 3.0.\n\nFollowing $^{212}$Pb disint
 egration\, decays of $^{212}$Bi and $^{212}$Po contributed ~95% of the tot
 al energy deposited. The full decay chain deposited 8.9$\\\,$MeV/decay on 
 average with a therapeutic range of $X_{90}\\\,$=$\\\,$0.091$\\\,$mm. Indi
 vidual contributions from $^{212}$Pb\, $^{212}$Bi\, $^{212}$Po\, and $^{20
 8}$Tl yielded $X_{90}$ values of 0.41$\\\,$mm\, 1.8$\\\,$mm\, 0.086$\\\,$m
 m\, and 5.8$\\\,$mm\, respectively\, highlighting that dose is dominated b
 y $^{212}$Po decay and accurate reconstruction of radionuclide distributio
 ns requires high-resolution imaging. Furthermore\, discriminating the 727$
 \\\,$keV photons (6.7% intensity) in the $^{212}$Bi to $^{212}$Po branch f
 rom abundant $^{208}$Tl photons can help distinguish $\\alpha$ and $\\beta
 ^-$ decay pathways\, supporting precision dosimetry. Photon intensity hist
 ograms (photons/decay) showed excellent agreement with NuDat 3.0 and singl
 e-source GATE simulations. However\, initializing multiple sources to esta
 blish transient equilibrium uncovered a GATE timing issue that condensed e
 missions into the acquisition window\, inflating apparent count rates and 
 potentially biasing activity and dose estimates.\n\nFuture work will addre
 ss the GATE timing issue and establish correlations between Compton camera
  images and absorbed dose. Once validated\, the recent Photon from Ion Dec
 ay (PHID) source will be used to efficiently simulate photon emission with
 out tracking charged particles. This approach is expected to accelerate Co
 mpton camera studies and support robust dosimetry in TRT with alpha-emitte
 rs\, ultimately contributing to more precise and clinically viable treatme
 nt verification.\n\nhttps://indico.ific.uv.es/event/8181/contributions/285
 39/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28539/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Dosimetric Impact of the Interplay Effect between the Proton Beam 
 and Tumor Motion
DTSTART;VALUE=DATE-TIME:20251029T093000Z
DTEND;VALUE=DATE-TIME:20251029T094500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28518@indico.ific.uv.es
DESCRIPTION:Speakers: Alba Meneses-Felipe ((1) Department of Physics and A
 pplied Mathematics\, University of Navarra. )\nIntroduction: Pencil beam s
 canning (PBS) is one of the main delivery techniques in proton therapy (PT
 ). A narrow proton beam irradiates the tumor layer by layer\, delivering d
 ose to specific locations (spots) within each layer. However\, PBS is high
 ly sensitive to uncertainties\, making the treatment of moving targets in 
 PT especially challenging due to respiratory motion. The interplay effect\
 , caused by the relative motion between the tumor and the scanning beam\, 
 can degrade the delivered dose and reduce treatment effectiveness. The mai
 n objective of this study is to accurately determine the dose received by 
 moving tumors by quantifying the dosimetric impact of the interplay effect
 .\nMaterial and Methods: A planning computed tomography (pCT)\, in which t
 he treatment dose is planned\, and a 4D-CT\, consisting of eight CT images
  corresponding to different respiratory phases\, were used to evaluate tum
 or motion. A stochastic model based on the compact HITACHI synchrotron was
  employed to predict the proton beam temporal structure. After determining
  the delivery time of each spot in the treatment plan\, we can assign spot
 s to each of the eight respiratory phases depending on the phase in which 
 irradiation begins\, and the patient’s respiratory frequency. The freque
 ncy was varied between 5\, 12 and 20 breaths per minute (bpm)\, and the in
 itial respiratory phase was randomized for each treatment session/fraction
  across 100 simulations per frequency. The treatment plan dose was compute
 d for each phase according to the spot distribution and summed on the pCT.
  \nResults: Variability in delivery times and frequency influences layer d
 eposition within the tumor (Figure 1)\, resulting in regions receiving hig
 her doses (layers overlap\, in red) or lower doses (layers are separated\,
  in blue). Multiple (30) treatment sessions help mitigate the dosimetric i
 mpact of different starting respiratory phases (Figure 2). Higher frequenc
 ies reduce the interplay effect\, especially when fewer (3) sessions are u
 sed\, with standard deviations (SD) over 100 simulations in the tumor of 
 ±0.43 Gy (5 bpm)\, ±0.20 Gy (12 bpm)\, and ±0.13 Gy (20 bpm).\nConclusi
 on: Interplay between motion and dynamic beam delivery in PBS-PT degrades 
 the dose distribution and can compromise the absorption of the prescribed 
 dose in the tumor. Understanding the beam’s temporal structure\, which d
 epends on the proton accelerator\, and considering tumor motion\, frequenc
 y\, and number of treatment fractions\, are critical for accurately determ
 ining the dose delivered to each tumor.\n\nhttps://indico.ific.uv.es/event
 /8181/contributions/28518/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28518/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Primeros mapas microdosimétricos en protonterapia en el DCPT
DTSTART;VALUE=DATE-TIME:20251029T091500Z
DTEND;VALUE=DATE-TIME:20251029T093000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28521@indico.ific.uv.es
DESCRIPTION:Speakers: Celeste Fleta (IMB-CNM)\nRecientemente\, se han repo
 rtado algunas toxicidades en la terapia con protones [1–2]. Esto podría
  deberse a que los protones generan una mayor transferencia lineal de ener
 gía (LET) al final de su rango\, lo que puede generar daños colaterales\
 , como efectos agudos y tardíos. Por esto\, evaluar las distribuciones de
  LET podría ayudar a mejorar los resultados de la terapia.\n\nEn este con
 texto\, el Centro Nacional de Microelectrónica (IMB-CNM) ha diseñado y f
 abricado nuevos detectores de silicio 3D [3]\, basados en una novedosa arq
 uitectura de electrodos cilíndricos con tamaños microscópicos comparabl
 es a los de las células (15-25 μm). Esto permite cuantificar el LET a es
 cala micrométrica\, es decir\, la energía lineal. El  sistema desarrolla
 do es el primer conjunto de estos microdetectores 3D\, con una matriz de 3
  × 3 celdas unitarias y un espaciamiento de 200 μm entre ellas\, cubrien
 do un área total sensible a la radiación de 0.4 mm × 12 cm\, con una re
 solución espacial de 600 μm [4].\n\nSe realizaron pruebas de microdosime
 tría con esta matriz de sensores en el Danish Center for Particle Therapy
  (DCPT). Los experimentos se llevaron a cabo en diferentes configuraciones
 : desde una condición relativamente monoenergética –la meseta de entra
 da–\, pasando por la parte media del SOBP\, hasta el borde distal del SO
 BP –al 75% y 95% de la dosis–. Para obtener estas posiciones en los es
 pectros\, se utilizaron fantomas de agua sólida. Asimismo\, se empleó un
  fantoma antropomórfico con un campo clínico específico (Figura 1). Ade
 más\, se realizaron simulaciones Montecarlo (MC) basadas en TOPAS [5] par
 a su comparación con los resultados experimentales.\n\nSe registraron esp
 ectros de energía de microdosimetría en cada caso (Figura 2)\, y los val
 ores experimentales promedio de energía lineal por dosis (¯yD) en los de
 tectores de silicio se compararon con los valores de LETd simulados para e
 l paciente mediante el software RayStation\, así como con los valores de 
 las simulaciones (Figura 3).\n\nEstos resultados demuestran\, por primera 
 vez\, la viabilidad de cuantificar mapas de energía lineal de microdosime
 tría en condiciones clínicas. Esta matriz de sensores puede ser una herr
 amienta poderosa para verificar los valores de LETd simulados por RaySearc
 h.\n\nhttps://indico.ific.uv.es/event/8181/contributions/28521/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28521/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Radiation-Hard Silicon Carbide Dosimeters for Electron and Proton 
 FLASH QA
DTSTART;VALUE=DATE-TIME:20251029T090000Z
DTEND;VALUE=DATE-TIME:20251029T091500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28526@indico.ific.uv.es
DESCRIPTION:Speakers: Celeste Fleta (Instituto de Microelectrónica de Bar
 celona\, IMB-CNM (CSIC))\nThe central challenge in radiotherapy (RT) is to
  deliver a sufficiently high dose to achieve tumour control while sparing 
 healthy tissues. FLASH RT\, which delivers radiation at ultra-high dose ra
 tes (≥40 Gy/s) compared with conventional RT (≈0.05 Gy/s)\, has emerge
 d as a promising approach. Preclinical studies have shown that FLASH reduc
 es toxicity in normal tissues while preserving or even improving tumour co
 ntrol. It also shortens treatment times\, reducing the impact of patient a
 nd organ motion. However\, the clinical translation of FLASH RT requires n
 ew dosimetry solutions\, since conventional detectors saturate\, lose line
 arity\, or degrade rapidly under ultra-high dose rate conditions.\nSilicon
  carbide (SiC) is a promising semiconductor material to address these need
 s. Compared to silicon\, SiC has a wide bandgap that reduces leakage curre
 nt and noise\, a higher displacement energy threshold that increases radia
 tion hardness\, and lower signal yield per unit dose\, which prevents satu
 ration at very high instantaneous dose rates. Nowadays\, SiC technology is
  mature\, with reproducible wafer-scale fabrication. \nAt IMB-CNM (CSIC)\,
  4H-SiC PiN diodes have been designed and fabricated specifically for FLAS
 H RT applications. Their performance has been validated in different facil
 ities and radiation conditions. At PTB (Germany)\, the devices showed line
 arity up to 11 Gy per pulse (≈4 MGy/s) with 20 MeV electron beams and a 
 performance comparable to PTW’s flashDiamond. At CMAM (Spain)\, the diod
 es showed reproducible\, linear response to 7 MeV protons up to 26 Gy per 
 pulse. In addition\, radiation hardness experiments at CNA (Spain) demonst
 rated that\, after an initial sensitivity loss of ~1.3%/kGy\, stability wa
 s reached near 1 MGy of 2 MeV protons\, with linear response preserved up 
 to cumulative doses of at least 4 MGy. All measurements were performed wit
 hout external bias\, like conventional silicon diodes are used in clinical
  settings\, meaning no adaptation of existing workflows would be required.
 \nIn parallel\, pixelated SiC arrays have been produced for spatially reso
 lved dosimetry. A 12-pixel array was fabricated and tested with 7 MeV elec
 trons at the Institut Curie (France). The array produced accurate 2D dose 
 maps at 10 Gy per pulse\, demonstrating the feasibility of SiC arrays for 
 real-time QA under FLASH conditions. Efforts are currently underway to sca
 le up the pixellated system to a larger array of 400 channels with a custo
 m readout electronics for broader clinical and preclinical applications.\n
 \nhttps://indico.ific.uv.es/event/8181/contributions/28526/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28526/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Out-of-field thermal neutron characterization with thin 3D-silicon
  detectors in Varian TrueBeam and Elekta Synergy LINACs
DTSTART;VALUE=DATE-TIME:20251028T162500Z
DTEND;VALUE=DATE-TIME:20251028T164000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28516@indico.ific.uv.es
DESCRIPTION:Speakers: Felipe Eduardo Zamorano Labbe (Instituto de Microele
 ctrónica de Barcelona)\nOperating medical linear accelerators (LINACs) ab
 ove 6 MV generates unwanted neutrons through (γ\,n) interactions with hig
 h-Z materials in the accelerator head. These secondary neutrons contribute
  additional dose to healthy tissues and may lead to late-onset adverse eff
 ects [1]. Moreover\, the neutron yield shows high variability\, depending 
 on several factors\, e.g.\, LINAC model\, beam energy\, and delivery modal
 ity. Consequently\, real-time\, patient-specific neutron characterization 
 is essential for accurate assessment of secondary exposure and for optimiz
 ed radiation safety measures. \nTo address this challenge\, IMB-CNM has de
 veloped an ultra-thin (20 μm) neutron sensor based on silicon with an inn
 ovative 3D architecture coupled to a (45 ± 5) μm thick ¹⁰B-enriched c
 onversion layer to quantify thermal neutron fields. The ultra-thin active 
 volume provides a high gamma-rejection factor (>10⁻⁸)\, crucial for is
 olating neutron signals in high-gamma-ray environments. Custom readout ele
 ctronics enabled online acquisition.\nReal-time thermal neutron contributi
 ons were measured in two treatment rooms comparing two widely used LINACs
 —Varian TrueBeam and Elekta Synergy—operated with flattened (FF) 15 MV
  X-ray beams and 10×10 cm² field size. Measurements were compared agains
 t PHITS Monte Carlo simulations using an extended 15 MV TrueBeam head mode
 l that\, for the first time\, includes detailed head shielding and was val
 idated with PDD data (TPR20\,10 difference \n\nhttps://indico.ific.uv.es/e
 vent/8181/contributions/28516/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28516/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Characterization and Monte Carlo Modelling of ElectronFlash LINAC 
 at Institute Curie
DTSTART;VALUE=DATE-TIME:20251028T164000Z
DTEND;VALUE=DATE-TIME:20251028T165500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28524@indico.ific.uv.es
DESCRIPTION:Speakers: Angela Maria  Henao Isaza (Instituto de Microelectr
 ónica de Barcelona (IMB-CNM))\nThe electron LINAC ElectronFlash installed
  at the Institut Curie (France) is dedicated to the investigation of the F
 LASH effect on pre-clinical trials and radiobiology studies [1]. The accur
 ate beam characterization is essential for a proper dose calibration. Alth
 ough a few dosimeters operate under FLASH conditions\, e.g.\, diamond [2]\
 , ultra-thin ionization chambers (UTIC) [3]\, and SiC-based detectors [4]\
 , Monte Carlo (MC) simulations are a complementary tool for estimating dos
 es in scenarios where those dosimeters can have a limited use.\nThis study
  aims to present the experimental and simulated characterization of the El
 ectronFlash Linac for both FLASH and conventional modalities using a set o
 f dosimeters and MC simulations.   \nIrradiations were performed at 7 MeV\
 , with 0.5 – 5 μs pulse widths\, and up to 250 Hz with different poly m
 ethyl methacrylate (PMMA) applicators.  The experimental setup consisted i
 n a PTW Water Phantom and a PEEK plastic collimator designed for irradiati
 ng mouse lungs (Fig. 1\, left). The absolute dosimetry was made with Radio
 chromic EBT3 films\, a PTW FlashDiamond\, and UTIC to characterize the per
 centage depth dose (PDD) in that water tank (Fig. 2\, left). The scatter f
 actors were evaluated with new SiC detectors designed and fabricated at IM
 B-CNM. The beam FWHMs were also quantified with the radiochromic films. We
  used the open-source GATE MC (vs 10.0.2) to model the beamline starting f
 rom the experimental data gathered using the dosimeters mentioned above. S
 imulations were run in the computational cluster TIRANT v4.    \nConsideri
 ng the experimental work\, the PDDs obtained showed loss of electron equil
 ibrium at the beginning of the curve and non-negligible differences betwee
 n FLASH and conventional modalities (Fig 1\, right). Additionally\, there 
 was a significant difference (43%) in the FWHMs between these two modaliti
 es\, which suggests notable differences in the beam configuration for each
  one. The scatter factors evaluated with SiC diodes were in good agreement
  with those from flashDiamond. Interestingly\, these PDDs yielded an incre
 ase of electron energy compared to the previous PDD reported [3]\, which r
 einforce the need to model the LINAC. Regarding the MC study\, the simulat
 ed PDD showed an excellent agreement with the experimental measured (Fig 2
 \, right) validating the accuracy of the MC modelling. This enables calcul
 ate the dose distributions in cases where the dosimeters cannot easily be 
 used\, e.g.\, for small field sizes or large dose gradients.  \nThis work 
 shows the first comparison of experimental dose distributions with those o
 btained with accuracy MC model of the electronFLASH LINAC at Inst. Curie.\
 n\nhttps://indico.ific.uv.es/event/8181/contributions/28524/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28524/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Microtrack: the new Geant4 example for calculations on microdosime
 try.
DTSTART;VALUE=DATE-TIME:20251028T165500Z
DTEND;VALUE=DATE-TIME:20251028T171000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28533@indico.ific.uv.es
DESCRIPTION:Speakers: Miguel Galocha-Oliva (Universidad de Sevilla)\nThe s
 patial distribution of energy deposition events produced by the different 
 types of ionizing radiation is a key factor to determine their radiobiolog
 ical effects at the cellular scale. The theoretical framework provided by 
 microdosimetry has been widely employed to describe these stochastic inter
 actions\, particularly in studies addressing the characterization of Linea
 r Energy Transfer (LET) and Relative Biological Effectiveness (RBE) of ion
  beams in the context of hadron therapy. Such quantities are typically cal
 culated through Monte Carlo simulations. \n\nTo fulfill the purpose of cal
 culating these energy distributions\, a new track-structure Monte Carlo ap
 plication has been developed to incorporate it as a new Geant4-DNA example
  of the Geant4 toolkit. The code\, named Microtrack\, is designed to study
  the energy deposition in spherical sensitive volumes\, known as sites\, w
 hose diameter sizes may vary from nanometer to micrometer scale. These sen
 sitive volumes are sampled within a cubic water volume. This geometry is d
 efined by two input parameters: the site radius and the maximum electron r
 ange. \n\nA flexible primary generator controls particle type (protons by 
 default)\, energy\, and beam source position\, enabling reproducible irrad
 iation setups relevant to microdosimetry\, LET and RBE studies. \n\nScorin
 g is implemented through a dedicated sensitive detector that records per-s
 tep energy deposition and aggregates event-level observables. Simulation o
 utputs are handled by the Geant4 analysis manager and written to a ROOT fi
 le\, containing useful histograms for the aforementioned studies\, includi
 ng distributions of single-event energy imparted up to the second moment t
 o calculate weighted quantities such as dose-mean lineal energy. \n\nMicro
 track emphasizes transparency and flexibility: default options\, such as t
 he volume material\, particle\, beam energy\, or physics list\, can be mod
 ified through Messenger classes and macro files\, while multithreading ena
 bles faster simulations by distributing runs across multiple threads and m
 erging results. \n \nIn summary\, the future Geant4-DNA example Microtrack
  constitutes a versatile Monte Carlo tool for the calculation of microscop
 ic energy deposition patterns and assists research on microdosimetry for h
 adron therapy.\n\nhttps://indico.ific.uv.es/event/8181/contributions/28533
 /
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28533/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Shielding calculations for a low energy proton linac
DTSTART;VALUE=DATE-TIME:20251028T161000Z
DTEND;VALUE=DATE-TIME:20251028T162500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28541@indico.ific.uv.es
DESCRIPTION:Speakers: Amaia Villa Abaunza (TEKNIKER)\nIn the last years th
 ere is an increasing demand for advanced medical treatments\, a field wher
 e particle accelerators play a crucial role. However\, their availability 
 is significantly limited due to high maintenance and operational costs\, o
 n the one hand\, and the need for advanced technology and highly skilled p
 ersonnel for their design and construction\, on the other. The main goal o
 f the project LINAC7 is to face these limitations with the design\, fabric
 ation and testing of a low energy proton accelerator. For this\, all the c
 omponents of the accelerator are being developed by the personnel involved
  in the project and\, once constructed\, the accelerator will serve for tr
 aining students as well as for research studies.\nIn the current design\, 
 two experimental stations are to be constructed\, one for protons with 3 M
 eV and other for protons with 7 MeV. In the first case\, a 7Li target is a
 imed to be used for neutron production for different research purposes. In
  the second case\, irradiation of different materials\, such as cell cultu
 res\, and studies related with radioisotope generation are expected. Apart
  from that\, a beam stop for beam characterization will be placed at the e
 nd of a third line. \nThe accelerator will be installed in the university 
 of the Basque Country and its shielding design must guarantee adequate dos
 e rate values in the surrounding areas in beam-on and beam-off conditions.
  The present work considers the above-mentioned applications to calculate 
 the radiation that will be generated and the shielding needs. Moreover\, a
  portable neutron source that will also be located in the room has been ta
 ken into account. \nThe tools used for the calculations are the MCNP6.2 fo
 r radiation transport and the ACAB-2008 software to determine the radioiso
 tope inventory resultant from the activation of the materials. The startin
 g shielding configuration has been defined based on the literature\, and i
 ts optimization consists of an iterative process in which the geometry and
  type of the attenuating materials is modified basing on the dose rate val
 ues calculated in detectors positioned out from the accelerator room\, for
  beam-on conditions\, and in detectors located inside\, for beam-off condi
 tions. The plans of the building have been considered to obtain realistic 
 results.\nThe final solution consists of three different shieldings\, one 
 of them moveable to be used for the portable neutron source and for the ta
 rget station aimed for neutron generation. Highly efficient attenuating ma
 terials\, such as lead for gammas and polyethylene for neutrons\, allowed 
 for a more compact design. Moreover\, reduction of the iron quantity in th
 e external layer reduces dose values in beam-off conditions.\nIn conclusio
 n\, different shielding designs that guarantee dose rates below the limit 
 have been calculated and the next step is to discuss aspects related to fa
 brication and present the proposal to the CSN to advance with the construc
 tion of the setup.\n\nhttps://indico.ific.uv.es/event/8181/contributions/2
 8541/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28541/
END:VEVENT
BEGIN:VEVENT
SUMMARY:gVirtualXray for X-ray imaging simulations and education
DTSTART;VALUE=DATE-TIME:20251028T153000Z
DTEND;VALUE=DATE-TIME:20251028T153500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28515@indico.ific.uv.es
DESCRIPTION:Speakers: Alberto Corbi (Universidad Internacional de La Rioja
  (UNIR))\n# gVirtualXray for X-ray imaging simulations and education\n\ngV
 irtualXray is an open-source library designed to simulate X-ray images in 
 real time using the power of the GPU. Its core relies on the Beer–Lamber
 t law to model the absorption of photons by three-dimensional objects\, su
 ch as polygon meshes. This project has received numerous awards and recogn
 itions related to its use in education and *digital twins*\, including the
  recent Dirk Bartz Prize for Visual Computing in Medicine and Life Science
 s\, granted among others to the authors of this presentation (Vidal\, 2025
 ).\n\n# Technical Foundation and Design\n\ngVirtualXray is based on the fo
 llowing technical principles:\n\n- Implemented in C++ and using OpenGL/GLS
 L\, gVXR offers compatibility with both legacy and modern OpenGL implement
 ations\, without relying on deprecated functions.\n- Employs the Beer–La
 mbert law model\, in both monochromatic and polychromatic versions\, ideal
  for emulating X-ray tube sources and synchrotron radiation.\n- It is cros
 s-platform: works on Windows\, Linux\, and macOS\, and can even run on mac
 hines without GPUs\, albeit with lower performance.\n- Scalability is rema
 rkable: from Raspberry Pi to supercomputers and cloud environments (such a
 s Google Colab)\, and even Docker containers.\n- Available as a core C++ l
 ibrary. To facilitate usage in other languages\, there is SimpleGVXR\, a l
 ayer that adds wrappers for Python\, R\, Ruby\, Tcl\, C#\, Java\, and GNU 
 Octave.\n- In addition\, it provides a JSON configuration format to simpli
 fy simulation creation\, especially in Python environments.\n- Comes with 
 demos\, documentation\, tutorials\, and support through its website and re
 positories (SourceForge\, GitHub).\n\n# Validation and Accuracy\n\nBeyond 
 its reputed use as a software product\, gVirtualXray has been academically
  discussed in several publications such as Vidal et al. (2017) and Corbi e
 t al. (2024). Moreover:\n\n- Its accuracy has been validated against class
 ical tools such as VXI\, Geant4 (from CERN)\, and real experimental data.\
 n- A recent comparative study against Monte Carlo (MC) simulations showed 
 spectacular results: mean absolute percentage error (MAPE) of 3.12%\; zero
 -mean normalized cross-correlation (ZNCC) of 99.96%\; structural similarit
 y index (SSIM) of 0.99\; with execution times of milliseconds compared to 
 days with MC.\n- It was also evaluated with digitally reconstructed radiog
 raphs (DRRs)\, computed tomography (CT) slices\, and real radiographs\, co
 nfirming high-fidelity comparability.\n\n# Applications and Uses\n\nThe ap
 plications of gVirtualXray are diverse and multidisciplinary:\n\n- Educati
 on: in medical simulators and teaching tools for particle physics and engi
 neering (Corbi et al.\, 2019). This makes it an ideal educational tool\, a
 s it enables interactive teaching of X-ray physics\, training in medical s
 imulators (including virtual reality and haptic interfaces)\, generation o
 f synthetic data for AI\, safe experimentation without real radiation\, an
 d exploration of clinical and diagnostic scenarios\, all with support for 
 multiple programming languages and accessible web environments.\n- Medical
  research: simulation of respiratory motion\, CT artifacts\, image reconst
 ruction and image/image registration (Pointon et al.\, 2023).\n- Materials
  science: micro-CT\, artifact analysis\, optimization in reverse engineeri
 ng.\n- Machine Learning: generation of synthetic images for training or op
 timization.\n- Virtual reality and interactive environments: real-time sim
 ulation with deformations and animations.\n\n# Recognitions\n\nAs mentione
 d earlier\, gVirtualXray has been presented and awarded at multiple events
  and conferences:\n\n- Ken Brodlie Award at Theory and Practice of Compute
 r Graphics (2009).\n- Second place in Eurographics Medical Prize for medic
 al graphics innovation (2009).\n- Best Poster Award at dXCT (2022).\n- Cos
 ec Impact Award for advances in Digital Twins of XCT scanners\, with a ful
 ly open virtual workflow (2023).\n- The Dirk Bartz Prize for Visual Comput
 ing in Medicine and Life Sciences (2025).\n\n# Conclusion\n\ngVirtualXray 
 is a powerful X-ray image simulation library that combines scientific accu
 racy with speed\, thanks to its GPU implementation. It is accessible to de
 velopers and researchers due to its cross-platform compatibility and wrapp
 ers in multiple languages. Rigorously validated and adopted in education\,
  medicine\, materials science\, ML\, and interactive simulation\, the proj
 ect remains active and recognized for its technical\, scientific\, and edu
 cational contributions. In the context of the V RSEF/IFIMED Conference\, a
  brief and outreach-oriented presentation of the tool will be delivered\, 
 showcasing its potential and wide range of applications\, with an emphasis
  on its educational use.\n\n# References\n\n- Vidal\, F. P.\, et al. (2017
 ). gVirtualXRay: Virtual x-ray imaging library on GPU. In *Computer Graphi
 cs and Visual Computing*.\n- Corbi\, A.\, Burgos\, D.\, Vidal\, F.\, Albio
 l\, F.\, Albiol\, A. (2019). X-ray imaging virtual online laboratory for e
 ngineering undergraduates. *European Journal of Physics*.\n- Pointon\, J. 
 L.\, Vidal\, F. P.\, et al. (2023). Simulation of X-ray projections on GPU
 : Benchmarking gVirtualXray with clinically realistic phantoms. *Computer 
 Methods and Programs in Biomedicine*.\n- Corbi\, A.\, Vidal\, F.\, et al. 
 (2024). X-ray simulations with gVXR as a useful tool for education\, data 
 analysis\, set-up of CT scans\, and scanner development. In *Developments 
 in X-Ray Tomography XV*.\n* Vidal\, F.\, Albiol\, F.\, Albiol\, A.\, Corbi
 \, A.\, et al. (2025). X-ray simulations with gVirtualXray in medicine and
  life sciences. In *Eurographics Conference on Visualization (EUROVIS 2025
 )*. The Eurographics Association.\n\nhttps://indico.ific.uv.es/event/8181/
 contributions/28515/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28515/
END:VEVENT
BEGIN:VEVENT
SUMMARY:X-ray fluorescence imaging for breast cancer characterization and 
 treatment
DTSTART;VALUE=DATE-TIME:20251028T150000Z
DTEND;VALUE=DATE-TIME:20251028T151500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28544@indico.ific.uv.es
DESCRIPTION:Speakers: Siddharth Parashari (Instituto de Física Corpuscula
 r)\nX-ray fluorescence imaging (XFI) is an emerging molecular imaging tech
 nique that combines high sensitivity with high spatial resolution\, offeri
 ng significant penetration depth in tissues while minimizing ionizing radi
 ation exposure compared to current methods. This makes XFI a promising too
 l for early cancer detection and personalized treatment. The “Integrated
  Molecular Imaging for Personalized Biomarker-based Breast Cancer Characte
 rization and Treatment (IMMPRINT)” project aims to develop a proof-of-pr
 inciple (POP) demonstrator that leverages X-ray fluorescence computed tomo
 graphy (XFCT) as a novel hybrid modality for tumor profiling\, with a focu
 s on breast cancer (BC). Within IMMPRINT\, specifically engineered and tar
 geted nanoparticles\, such as gold nanoparticles (GNPs)\, will be employed
  to identify distinct signatures of intra and inter – tumor heterogeneit
 y in BC. The sensors chosen for the POP are the pnCCD sensors produced by 
 MPI HLL in Munich. To support system development\, Monte Carlo simulations
  are being performed on a tumor – bearing mouse model loaded with GNPs\,
  using the GEANT4 simulation toolkit. Fluorescence photons are generated w
 hen GNPs are excited by incident X-rays and detected with a silicon detect
 or. Simulation results that outline critical parameters for detector devel
 opment and system design will be presented.\n\nhttps://indico.ific.uv.es/e
 vent/8181/contributions/28544/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28544/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Whole-body dose computation system developed for the HARMONIC pati
 ent database
DTSTART;VALUE=DATE-TIME:20251028T144500Z
DTEND;VALUE=DATE-TIME:20251028T150000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28545@indico.ific.uv.es
DESCRIPTION:Speakers: Lorenzo Brualla (IFIC\, CSIC-UV)\nObjective: The qua
 ntitative relationship between dose delivered outside the treated volume a
 nd stochastic effects is not well understood\, although epidemiological ev
 idence supports the hypothesis that low to moderate doses of ionizing radi
 ation are associated with measurable excess risk of several types of cance
 r. Current studies of second primary cancer after radiotherapy demand the 
 possibility of computing whole-body dose distributions on patients treated
  with modern photon and proton external beam radiotherapy (EBRT) technique
 s.\nMethods: In the framework of the Horizon Euratom HARMONIC project a da
 tabase of pediatric modern radiotherapy patients\, treated with photon or 
 proton EBRT\, was created. This database stores for each patient DICOM-RT 
 computed tomography images and treatment plans. The whole-body dose comput
 ation requires a patient geometry in which to compute the corresponding do
 se distribution. A software developed within HARMONIC was employed for tha
 t purpose using anthropomorphic phantoms. For the computation of the whole
 -body absorbed dose distribution in photon treatments\, the Monte Carlo sy
 stem PRIMO was used\, while proton treatments were computed with the Monte
  Carlo code TOPAS/Geant4 . The imaging whole-body dose associated with dia
 gnostic and positioning procedures during therapy was also computed with t
 he Monte Carlo code PENELOPE. The developed codes and geometries were expe
 rimentally validated by means of an anthropomorphic pediatric material pha
 ntom (ATOM) irradiated with the considered therapeutic and imaging procedu
 res.\nResults: Out-of-field organ equivalent dose of proton therapy is up 
 to two orders of magnitude lower when compared to modern photon therapy. A
 s an example\, for a brain glioma treatment\, with a total target dose of 
 50.4Gy(RBE)\, it was found that the organ doses from the proton treatment 
 ranged between 0.6 mSv (testes) and 120 mSv (thyroid)\, while for photon t
 herapy (IMRT) 43 mSv (testes) and 575 mSv (thyroid). Dose delivered by pla
 nning CT ranged between 0.01 mSv (testes) and 72 mSv (scapula)\, while for
  the 28 fractions\, the imaging procedure for positioning (CBCT) yielded d
 oses ranging between 56 uSv (testes) and 36 mSv (thyroid).\nConclusions: T
 he developed and validated code systems for dose computation have shown to
  be suitable for the computation of whole-body dose distributions of patie
 nts stored in the HARMONIC database. The lower out-of-field dose of proton
  treatments respect to equivalent photon irradiations results in the fact 
 that the imaging dose from diagnostic and positioning procedures becomes s
 ignificant in proton therapy. This research is the result of the work cond
 ucted at the West German Proton Therapy Centre Essen\, the Belgian Nuclear
  Research Centre\, the French Alternative Energies and Atomic Energy Commi
 ssion\, the University Hospital Essen\, the University Hospital of Zürich
  and the Institut Gustave Roussy.\n\nhttps://indico.ific.uv.es/event/8181/
 contributions/28545/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28545/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Compton imaging for dose monitoring in boron neutron capture thera
 py
DTSTART;VALUE=DATE-TIME:20251028T110000Z
DTEND;VALUE=DATE-TIME:20251028T111500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28538@indico.ific.uv.es
DESCRIPTION:Speakers: Pablo Torres-Sánchez (Instituto de Física Corpuscu
 lar (CSIC-UV))\nBoron Neutron Capture Therapy (BNCT) is an experimental fo
 rm of radiotherapy that uses boron\, injected to the patient within a targ
 et molecule that accumulates selectively in cancerous cells. This therapy 
 exploits the large boron neutron capture cross-section to deliver a target
 ed dose from neutron irradiation. BNCT has shown great promise with the ad
 vent of accelerator-based technologies\, which facilitate high-quality neu
 tron beams in clinical environments [1]. \n\nOne of the primary challenges
  in current BNCT is the accurate determination of the dose delivered to th
 e patient. The state-of-the-art method uses simple extrapolations from pre
 vious PET scans and online monitoring of boron concentration in blood. Sin
 ce neutron captures in boron produce 478 keV gamma rays\, this radiation c
 ould be potentially used for real-time dose monitoring. To date\, the main
  challenges remain dealing with very intense radiation fields that generat
 e large count rates above detector reach\; and in achieving enough boron s
 ensitivity to image the boron in the tumor (65 ppm) above the overall boro
 n in nearby tissues (18 ppm)\, on top of the strong background induced by 
 harsh neutron and gamma ray fields generated during the treatments\; while
  attaining the spatial resolution required and moving towards true online 
 capabilities during treatment.\n\nThe i-TED Compton Camera array\, origina
 lly designed for nuclear physics measurements of astrophysics interest\, h
 as expanded into medical physics through ion-range monitoring in HT [2]\, 
 and further aiming now at BNCT [3]. Its large efficiency design and low ne
 utron sensitivity make i-TED especially well suited for this task.\n\nThis
  contribution will present the adaptations of the original i-TED imager\, 
 to optimize its performance for BNCT dosimetry. In this context\, we requi
 re the use of pixelated detectors in order to cope with the very large cou
 nt rates present in these treatments. We will discuss the characterization
  and implementation of a first pixelated crystal and its integration in th
 e i-TED module and data process pipeline. Additionally\, since BNCT requir
 es imaging of large body regions\, we have integrated LM-MLEM algorithms t
 o enable 3D image reconstruction.  For that purpose\, we have developed in
  our lab a tomographic Compton-PET-capable rotatory system using i-TED mod
 ules.\n\nReferences\n[1] K. Hirose et al.\, “Boron neutron capture thera
 py using cyclotron-based epithermal neutron source and borofalan (10B) for
  recurrent or locally advanced head and neck cancer (JHN002): An open-labe
 l phase II trial”\, Rad. & Onc. Vol 155\, pp. 182-187\, (2021)\n[2] J. B
 alibrea-Correa et al.\, “Hybrid compton-PET imaging for ion-range verifi
 cation: a preclinical study for proton\, helium\, and carbon therapy at HI
 T”\, The Eur. Phys. Jour. Plus\, Volume 140\, 870 (2025) \n[3] P. Torres
 -Sánchez et al.\, “The potential of the i-TED Compton camera array for 
 real-time boron imaging and determination during treatments in Boron Neutr
 on Capture Therapy”\, App. Radiat. Isot. 217\, 111649 (2025)\n\nhttps://
 indico.ific.uv.es/event/8181/contributions/28538/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28538/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Proton Range Verification Using a Multidetector Setup: Preliminary
  Results from the PRIDE Project
DTSTART;VALUE=DATE-TIME:20251028T113000Z
DTEND;VALUE=DATE-TIME:20251028T114500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28536@indico.ific.uv.es
DESCRIPTION:Speakers: Carolina Fonseca Vargas (IFIC-UV)\nThe PRIDE project
  (Proton Range and Imaging Device) aims to integrate a proton computed tom
 ography (pCT) scanner and a proton range verification (pRV) detector into 
 a single device for proton therapy. Our collaboration has carried out exte
 nsive work on pCT  with experiments taking place in June and December 2022
  at the Krakow CCB facility.\nProton range verification (pRV) consists of 
 determining the proton range in a patient during treatment by inferring th
 e Bragg peak position from the detection of scattered secondary radiation.
  In February 2025\, we performed measurements at the Krakow CCB facility t
 o evaluate the components of our setup\, using water and PMMA phantoms\, a
 nd varying the beam energies between 70 and 160 MeV. Two independent measu
 rements were carried out: one with a non-commercial\, pure LaCl3 crystal p
 roviding excellent neutron-gamma discrimination in a coaxial configuration
  for independent detection of forward-emitted gamma rays and neutrons\, an
 d another with a position-sensitive plastic scintillator combined with two
  double-sided silicon strip detectors for the detection of laterally scatt
 ered neutrons and protons.\nIn this work\, we present a preliminary analys
 is of the experimental results and discuss their relevance for the develop
 ment of the integrated PRIDE device\, and compare them with Monte Carlo si
 mulations for validation.\n\nhttps://indico.ific.uv.es/event/8181/contribu
 tions/28536/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28536/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Hybrid Compton-PET imaging for ion-range monitoring  in hadron the
 rapy:  a performance study with synchrotrons\, iso-cyclotrons and synchro-
 cyclotrons
DTSTART;VALUE=DATE-TIME:20251028T111500Z
DTEND;VALUE=DATE-TIME:20251028T113000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28535@indico.ific.uv.es
DESCRIPTION:Speakers: Javier Balibrea Correa (Instituto de física corpusc
 ular IFIC)\nHadron therapy provides notable advantages compared to traditi
 onal radiotherapy\, largely because it allows for precise dose delivery at
  the Bragg peak. The effectiveness of this approach could be further impro
 ved with the implementation of a near real-time ion-range verification sys
 tem. Such monitoring would make it possible to minimize safety margins and
  better exploit the full potential of the treatment by mitigating sources 
 of systematic uncertainty.\nTwo of the most promising methodologies for in
 -room\, real-time monitoring are positron emission tomography (PET) and pr
 ompt-gamma imaging (PGI). The PGI technique is particularly well-suited fo
 r real-time monitoring because of the prompt nature of the emitted radiati
 on. In contrast\, PET imaging offers tomographic and functional informatio
 n\, making it valuable for studying physiological processes and tumor resp
 onse. A PGI-PET hybrid imaging system could help to address some of the li
 mitations inherent to each technique. This expectation arises from the com
 plementary strengths of the two techniques: prompt-gamma emission is more 
 suitable for real-time monitoring\, while PET imaging provides tomographic
  and functional information valuable for studying physiological processes 
 and tumor response.\nIn this contribution I will summarize the status of h
 ybrid PGI-PET technique explored at three different types of ion-therapy m
 achines: the large synchrotron at HIT\, the Proteus Plus iso-cyclotron and
  the Proteus One synchro-cyclotron from IBA. The main experimental results
  will be presented\, together with a discussion on the present experimenta
 l limitations and future steps to further develop this promising technique
  towards the clinical environment.\n\nhttps://indico.ific.uv.es/event/8181
 /contributions/28535/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28535/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Live cell spectroscopy analysis for personalised particle radiatio
 n therapy of metastatic bone cancer
DTSTART;VALUE=DATE-TIME:20251028T114500Z
DTEND;VALUE=DATE-TIME:20251028T120000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28546@indico.ific.uv.es
DESCRIPTION:Speakers: Eva Montbarbon (1.	Instituto de Instrumentación par
 a Imagen Molecular (I3M)\, CSIC-Universitat Politècnica de València)\nMe
 tastatic bone cancer contributes to approximately 2 to 3 million cancer-re
 lated deaths worldwide annually. Between 5% and 10% of new cancer patients
  will develop bone metastases. A major challenge in treating this disease 
 is the inability to perform imaging during particle radiation therapy (PRT
 )\, due to high radiation doses from frequent scans\, patient pain\, and m
 obility constraints. Consequently\, tumour imaging is typically limited to
  pre  and post treatment assessments—often several months apart\, which 
 hinder timely treatment adjustments and personalized care.\nThe BoneOscopy
  project\, funded by the European Innovation Council under Horizon Europe\
 , seeks to transform metastatic bone cancer treatment by enabling daily\, 
 real time monitoring of tumour regression and calcium content without addi
 tional radiation exposure\, using a novel prompt-gamma spectroscopy (PGS) 
 approach. The system utilizes specific detectors\, custom nanosecond elect
 ronics\, and a robotic arm to perform precise spectroscopic measurements f
 ocused on calcium concentration in the bone tissue\, which is the indicato
 r of tumour regression and bone health status.\nBoneOscopy’s research in
 tegrates a broad spectrum of technical and scientific expertise\, as it br
 ings together skills in bioengineering (DKFZ\, Germany)\, the institute le
 ader of the project\, molecular imaging and robotics (CSIC\, specifically 
 i3M in Valencia\, Spain)\, high-speed electronics (LIP\, Portugal)\, clini
 cal PRT experience and Monte Carlo simulation modeling (THM\, Germany)\, m
 edical device software\, and hardware integration and mechanical design (C
 osylab\, Slovenia). \nIn its first six months\, the BoneOscopy project has
  established the clinical contexts in which the detection system must oper
 ate. Monte Carlo simulations (via Geant4) using proton beams\, modeled fro
 m the ones delivered in centres like HIT and MIT in Germany\, have allowed
  the project team to estimate prompt gamma–ray generation under realisti
 c clinical conditions. In parallel\, simulation work has been carried out 
 to optimize the detector’s crystal design supporting decisions on sensor
  types\, geometric layout\, and mechanical integration. With this groundwo
 rk completed\, the project is ready to transition into the implementation 
 phase.\nThe presentation will offer an overview of the BoneOscopy initiati
 ve\, detailing the clinical environment requirements—including beam para
 meters\, patient positioning mechanics\, and expected variations in calciu
 m concentration. It will then present comprehensive results from the simul
 ation studies achieved with Geant4 focused on prompt-gamma generation and 
 detection. Finally\, it will include an in-depth analysis of critical dete
 ctor components\, particularly the crystal materials and configurations us
 ed in the primary detection system.\n\nhttps://indico.ific.uv.es/event/818
 1/contributions/28546/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28546/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Escáner PET basado en BGO para la verificación de dosis en proto
 nterapia
DTSTART;VALUE=DATE-TIME:20251028T104500Z
DTEND;VALUE=DATE-TIME:20251028T110000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28519@indico.ific.uv.es
DESCRIPTION:Speakers: Óscar Pietrzyk (I3M)\nLa terapia con protones es un
 a forma de radioterapia más precisa\, eficaz y segura que la radioterapia
  convencional en muchos casos de cáncer. Se trata de una técnica innovad
 ora que está experimentando un notable crecimiento e interés. Actualment
 e\, en España existen dos centros de protonterapia en funcionamiento\, y 
 está prevista la instalación de diez nuevos centros en distintas regione
 s del país en los próximos años.\nEsta terapia permite una deposición 
 muy precisa y concentrada de la dosis en la zona que se trata. No obstante
 \, la administración de radiación más precisa y concentrada sobre el tu
 mor puede convertirse en una desventaja si\, por mala posición del pacien
 te o por el movimiento de los órganos internos\, el haz de protones no se
  dirige a la masa tumoral afectando las zonas sanas colindantes.\nLa verif
 icación de la dosis en la terapia con protones administrada al paciente i
 nmediatamente después de cada sesión juega un papel decisivo en la valid
 ación del tratamiento\, seguridad del procedimiento y el objetivo clínic
 o. Actualmente no se aplica ningún método de forma rutinaria en la clín
 ica para la verificación de dosis. Por ello\, existe la necesidad de desa
 rrollar técnicas de verificación precisas y aplicables en la práctica c
 línica.\nPara abordar esta necesidad\, proponemos el desarrollo de un pro
 totipo PET\, llamado INSPIRE\, dedicado a verificar la dosis administrada 
 tras una terapia con protones en el cerebro del paciente. La propuesta se 
 centra en la detección de $^{18}$F\, uno de los radioisótopos emisores d
 e positrones que se producen cuando el haz de protones interacciona con el
  tejido. Esto supone un desafío debido a la baja concentración de $^{18}
 $F que se genera (~0.1 Bq/ml con 3 Gy). Nuestra propuesta se basa en el us
 o de detectores PET basado en cristales semi-monolíticos de BGO. El uso d
 e este material para nuestro diseño se debe a tres razones principales: r
 educción del coste de fabricación (3 veces menor al del LYSO)\, alta den
 sidad (más fotones de aniquilación capturados a mismo volumen) y ausenci
 a de radioactividad natural de Lu-176.\nPresentaremos resultados de medida
 s de $^{18}$F-FDG a muy baja actividad\, realizadas con un prototipo PET b
 asado en LYSO (DeepBreast) y con un escáner PET comercial basado en BGO (
 GE Omni Legend). Además\, mostraremos los resultados de las primeras simu
 laciones del equipo completo INSPIRE y de una evaluación experimental de 
 los detectores del equipo.\n\nhttps://indico.ific.uv.es/event/8181/contrib
 utions/28519/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28519/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Mitigating Radiodermatitis in Ultra-Hypofractionated Breast Radiot
 herapy: Objective Assessment of a Dermoprotective Bra by Laser Doppler Ima
 ging
DTSTART;VALUE=DATE-TIME:20251028T090000Z
DTEND;VALUE=DATE-TIME:20251028T091500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28542@indico.ific.uv.es
DESCRIPTION:Speakers: Carlos Galindo González (Universidad de Valencia)\n
 Objective:\nTo evaluate the effect of a dermoprotective bra on the progres
 sion of acute radiodermatitis induced by radiotherapy\, using as an object
 ive biomarker a quantitative skin perfusion index obtained by Laser Dopple
 r imaging.\nMaterials and methods:\nForty-seven patients with breast cance
 r treated with ultra-hypofractionated radiotherapy (total dose 26 Gy deliv
 ered in five fractions of 5.2 Gy) were included. According to the bra worn
  during RT\, patients were assigned to two groups: dermoprotective bra\, s
 eamless and made of viscose/chitin fiber with ionic silver (n = 21)\, and 
 conventional bra (n = 26). Skin toxicity was assessed clinically with the 
 CTCAE scale and objectively by skin perfusion measured with Laser Doppler 
 Imaging.\nThe upper-outer region of the irradiated breast and the contrala
 teral breast (internal control) were scanned to obtain mean perfusion. A M
 icrocirculation Index (MCI) was defined as the relative difference in mean
  perfusion between the treated and contralateral breast. Measurements were
  performed at four time points: pre-RT\, mid-treatment\, at RT completion 
 and at one month. Receipt of chemotherapy was also recorded.\nStatistical 
 analysis was performed using a general linear model for repeated measures\
 , including main effects of time\, bra type and chemotherapy\, and their i
 nteractions. Post-hoc comparisons were adjusted by the Bonferroni method.\
 nResults:\nBy CTCAE scale\, at RT completion 90.5% of the dermoprotective-
 bra group remained Grade 0 and 9.5% had mild erythema (Grade 1). In the co
 nventional-bra group\, 65.4% were Grade 0 and 34.6% Grade 1.\nObjective an
 alysis using the MCI showed significant differences: at the end of RT the 
 conventional-bra group exhibited a significantly higher MCI than the dermo
 protective-bra group (p = 0.037). At 30 days\, the dermoprotective-bra gro
 up showed a trend toward lower MCI\, close to statistical significance (p 
 = 0.065)\, suggesting faster microvascular recovery. Analysis of chemother
 apy effect indicated that\, among patients who did not receive chemotherap
 y\, those who did not use the dermoprotective bra had a significantly grea
 ter increase in MCI at RT completion (p = 0.017).\nConclusion:\nUse of the
  dermoprotective bra during breast radiotherapy reduces the incidence and 
 severity of acute radiodermatitis and moderates the acute increase in skin
  perfusion at treatment completion (p = 0.037)\, with a tendency to accele
 rate microvascular recovery at one month (p = 0.065). Furthermore\, it att
 enuates the adverse vascular effect observed in patients receiving RT alon
 e (p = 0.017). These findings support the relevance of the dermoprotective
  bra’s design and composition and warrant consideration of its clinical 
 implementation.\n\nhttps://indico.ific.uv.es/event/8181/contributions/2854
 2/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28542/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Development and Initial Testing of a Silicon-Based Compton Camera 
 Prototype for Radiotracer Imaging
DTSTART;VALUE=DATE-TIME:20251028T091500Z
DTEND;VALUE=DATE-TIME:20251028T093000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28543@indico.ific.uv.es
DESCRIPTION:Speakers: Luis Barrientos Mauriz ()\nCompton cameras (CCs) are
  promising imaging devices for nuclear medicine applications\, as they can
  produce 3D images over a broad range of gamma-ray energies. Their flexibl
 e geometry suits compact and unconventional imaging setups. High energy re
 solution also improves background rejection and supports multi-isotope ima
 ging\, crucial in clinical contexts. Silicon detectors\, due to their supe
 rior energy resolution are well-suited as scatterers in Compton camera sys
 tems.\n\nThe IRIS group at IFIC (Valencia)\, after developing several scin
 tillator-based CCs under the MACACO project\, is now working on a new prot
 otype using silicon detectors\, with the aim of improving the performance 
 for radionuclides emitting photons with energies below 300 keV such as ¹
 ⁷⁷Lu. The system combines a silicon pad detector as the scatterer and 
 a scintillator crystal coupled to a SiPM array as the absorber. This desig
 n aims to enhance spatial resolution over previous setups\, while preservi
 ng compactness and high detection efficiency. To evaluate its performance\
 , experimental tests at the laboratory have been conducted using a ¹³³B
 a source\, focusing on the 356 keV gamma-ray line.\n\nThe dimensions of th
 e silicon detector are 46.4 x 11.6 x 0.5 mm³ and 1 mm x 1 mm pads manufac
 tured by SINTEF for the MADEIRA project. The second detector of the CC con
 sists of a Lanthanum (III) Bromide scintillator crystal from Saint Gobain 
 of size 25.8 x 25.8 x 5 mm³ coupled to a SiPM array S13360-3025CS with a 
 pixel size of 3 mm². Data acquisition is handled by two time-synchronized
  AliVATA readout boards\, each tailored to operate the ASIC for its respec
 tive detector: the VATA64HDR16 collects charge from the SiPM signals\, whi
 le the VATAGP7.2 interfaces with the silicon detector\, both developed by 
 IDEAS.\n\nFunctional verification was performed by acquiring data in singl
 es and coincidence mode using a point-like source of ¹³³Ba with an acti
 vity of 683 kBq. Energy spectra from both detectors were analyzed\, and co
 rrelations between energy deposits are being evaluated to identify valid C
 ompton events. System optimization is ongoing.\n\nTo complement the experi
 mental work\, Monte Carlo simulations using GATE v8.2 were performed\, rep
 licating the physical system. Two radionuclides (¹³³Ba and ¹³¹I) wer
 e studied using a point-like source and a simplified Derenzo-like phantom 
 to assess the spatial resolution. Simulations indicate that the silicon–
 scintillator configuration achieves superior performance at low energies r
 elative to earlier MACACO prototypes.\n\nCurrent efforts focus on comprehe
 nsive characterization of the silicon detector\, expanded simulations for 
 radionuclides emitting photons near 200 keV\, and ongoing imaging experime
 nts.\n\nhttps://indico.ific.uv.es/event/8181/contributions/28543/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28543/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Imaging therapeutic radiopharmaceuticals in mice using the MACACO 
 III+ Compton camera.
DTSTART;VALUE=DATE-TIME:20251028T084500Z
DTEND;VALUE=DATE-TIME:20251028T090000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28537@indico.ific.uv.es
DESCRIPTION:Speakers: Karol Brzezinski (IFIC/CSIC)\nIntroduction\nCompton 
 cameras are a promising tool in radiopharmaceutical therapy (RPT) treatmen
 t assessment and dosimetry\, where gamma cameras perform sub-optimally due
  to the high energies of the emitted photons and low activities. The IRIS 
 group is developing MACACO\, a LaBr3-based Compton camera\, for this appli
 cation. The prototype MACACO III has been successfully used to visualize I
 -131 and Ac-225 [1\,2] in phantoms. The latest prototype\, MACACO III+\, w
 as tested at CIC biomaGUNE using a mouse phantom with several organs fille
 d with I-131 and live mice injected with [I-131]NaI. The images were compa
 red with those obtained using a commercial pre-clinical SPECT system. Simu
 lations of a mouse with a realistic biodistribution of [Ac-225]Ac-DOTA wer
 e performed to test the viability of using MACACO III+ for imaging Ac-225 
 in small animals.\n\nMethods\nMACACO III+ features two detector planes\, t
 he first one composed of a single detector with 25.8 mm x 25.5 mm x 5 mm c
 rystal size\, and the second plane comprising four such detectors. The sys
 tem was tested at CIC biomaGUNE with a mouse phantom\, filling different c
 ombinations of the brain\, heart\, kidney and bladder in 45 minute acquisi
 tions. Two living mice injected with 1.20 MBq and 2.16 MBq of [I-131]NaI w
 ere imaged during 30 minutes. The mouse phantom and the living mice were a
 lso imaged in a γ-CUBE SPECT system from Molecubes for 3 hours in a tomog
 raphic acquisition. \nSimulations were performed using GATE and a digital 
 3D mouse phantom containing 25 kBq of Ac-225\, with activity per organ bas
 ed on data from biodistributions in mice injected with [Ac-225]Ac-DOTA [3]
 \, including a tumor of realistic size and uptake located in the brain.\n\
 nResults/Discussion\nMeasurements of the mouse phantom filled with I-131 r
 esulted in images comparable to those obtained using the γ-CUBE. When fou
 r organs were filled\, the brain\, heart\, bladder and individual kidneys 
 were clearly distinguishable. Images of the two live mice acquired using M
 ACACO III+ are also similar to those obtained with the γ-CUBE\, as can be
  seen in the attached figure. Here\, I-131 uptake can be clearly identifie
 d in the thyroid gland as well as in the bladder and stomach. Form the sim
 ulation studies\, Ac-225 accumulation can be clearly visualized in the tum
 or and the individual kidneys.    \nConclusion\nThe MACACO Compton camera 
 developed by the IRIS group successfully imaged I-131 distributions in a m
 ouse phantom and living mice for the first time and shows great promise fo
 r imaging Ac-225\, as shown by realistic simulations. Images of I-131 dist
 ributions were obtained with lower acquisition times and of similar qualit
 y compared to those obtained using a commercial pre-clinical SPECT. Future
  studies will be aimed at imaging other isotopes in live animals\, in part
 icular Ac-225.\n\nReferences\n[1] J Roser et  al. 2024 Phys Medica 132:104
 928\n[2] K. Brzezinski et al\, Talk at 2024 IEEE NSS MIC\, Tampa\, USA\, 2
 6 Oct - 2 Nov 2024.\n[3] M. Rodak et al. 2022 Mol Cancer Ther. 21(12) 1835
 –1845\n\nhttps://indico.ific.uv.es/event/8181/contributions/28537/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28537/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Hybrid PET-MRI-FUS: Performance Validation\, Trimodal Imaging\, an
 d 9.4T Positron Range Confinement
DTSTART;VALUE=DATE-TIME:20251027T154500Z
DTEND;VALUE=DATE-TIME:20251027T160000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28520@indico.ific.uv.es
DESCRIPTION:Speakers: Fernando Lopez-Berenguer (Institute for Instrumentat
 ion in Molecular Imaging)\nHybrid imaging systems integrating Positron Emi
 ssion Tomography (PET)\, Magnetic Resonance Imaging (MRI)\, and Focused Ul
 trasound (FUS) are increasingly demanded in preclinical and translational 
 research\, yet no trimodal commercial solution currently exists. We have d
 esigned\, assembled\, and validated a dedicated PET insert based on monoli
 thic LYSO crystals (33×25.4×8 mm³) with 67 mm of axial FOV\, capable of
  simultaneous operation with high-field MRI and commercial FUS devices. We
  evaluated the system inspired on NEMA NU-4 2008 protocol. The PET insert 
 achieved a homogeneous submillimeter resolution (0.9 mm with Depth of Inte
 raction)\, a sensitivity of 3.8%\, and a Noise Equivalent Count Rate peak 
 of 80 kcps. Image quality metrics yielded recovery coefficients up to 0.89
  and spill-over ratios of 11% (air) and 22% (water)\, matching state-of-th
 e-art preclinical PET scanners.\n\nBeyond performance characterization\, t
 he PET insert was employed in various trimodal studies. In a proof-of-conc
 ept phantom experiment\, the PET was combined with a custom low-field MRI 
 and a custom FUS device. Localized sonication was used to heat up the phan
 tom and melt a gelatin compartment\, allowing the initially confined ¹⁸
 F-FDG solution to diffuse into the gel matrix. This redistribution process
  was successfully monitored in real time by PET-MRI.\n\nSubsequently\, in 
 vivo feasibility was demonstrated in murine brain studies using our PET in
 sert combined with a 9.4T MRI and a commercial RK-300 FUS system. FUS-indu
 ced BBB opening was achieved with microbubbles\, while Gd-DOTA (MRI) and 
 ⁶⁴Cu-DOTA (PET) were co-administered. PET-MRI images confirmed co-loca
 lization of contrast enhancement with sonicated regions\, validating the a
 bility of the trimodal system to perform concurrent imaging and therapy mo
 nitoring in vivo.\n\nIn parallel\, we investigated the impact of high magn
 etic fields on PET resolution through a positron range confinement study. 
 A microDerenzo phantom was sequentially filled with ¹⁸F\, ⁸⁹Zr\, an
 d ⁶⁸Ga and imaged with the PET insert inside and outside a 9.4T MRI. R
 esults confirmed that the magnetic field confines positron trajectories pe
 rpendicular to B₀\, with the most pronounced benefits for high-energy em
 itters: rods as small as 0.9 mm with ⁸⁹Zr and 1.0 mm with ⁶⁸Ga wer
 e resolved inside the MRI\, while only the 1.2 mm and 1.5 mm rods were dis
 tinguished when the PET insert was outside the MRI\, respectively.\n\nThes
 e results establish the developed PET insert as the first preclinical trim
 odal PET-MRI-FUS platform\, offering both state-of-the-art PET performance
  and unique multimodal capabilities. By enabling simultaneous imaging and 
 therapy guidance\, as well as demonstrating positron range confinement at 
 9.4T\, this system opens new avenues for molecular imaging\, BBB-targeted 
 drug delivery\, and advanced preclinical FUS research.\n\nhttps://indico.i
 fic.uv.es/event/8181/contributions/28520/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28520/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Spatial Resolution Characterization of PET Detectors Using BGO Cry
 stals and ASIC Readout
DTSTART;VALUE=DATE-TIME:20251027T153000Z
DTEND;VALUE=DATE-TIME:20251027T154500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28523@indico.ific.uv.es
DESCRIPTION:Speakers: Neus Cucarella (Instituto de Instrumentación para I
 magen Molecular\, i3M-UPV)\nPET has consolidated as one of the most used a
 nd important molecular imaging techniques. However\, there is still room f
 or improvement. Specifically\, boosting the system’s sensitivity will al
 low dose and/or time acquisition reduction without impacting the reconstru
 cted image’s quality. BGO detectors have higher density when compared wi
 th the most used lutetium-based detectors\, which translates into an incre
 ased sensitivity\,. Moreover\, the BGO crystals produce Cherenkov photons\
 , generated much faster than the scintillation ones\, that can be used and
  positively impact the timing performance of the PET detector. Furthermore
 \, DOI capability is key in PET\, for correcting parallax errors\, allowin
 g a uniform spatial resolution across the entire FOV.\nWe propose two BGO 
 PET detectors designs\, both with DOI and timing capabilities. The first i
 s a semi-monolithic block of 1×8 slab of 3×25×15 mm3 each. All faces of
  each slab are polished and covered with ESR\, except for the face coupled
  to the photosensor. The second detector proposed is a BGO crystal with th
 e so-called pseudo-slabs geometry. This crystal is composed of 1×8 pseudo
 -slabs of 3×25×15 mm3 each\, covered in BaSO4. Each pseudo-slab consists
  of 8 pixels of 3×3×15 mm3 with the four lateral faces unpolished and gl
 ued together. The entrance face of the block has an ESR film. The external
  dimensions of both crystal blocks is 25.8×25.8×15 mm3 and for all the s
 tudies these were coupled to a Silicon SiPM matrix. The TOFPET2 ASIC from 
 PETsys Electronics was used as the readout electronics. Experimental data 
 was acquired to study the spatial capabilities of the proposed detectors. 
 \nA uniform measurement was performed and the floodmap for each detector w
 as generated. The x-monolithic and the y-pixelated direction were estimate
 d using the RTP2 and CoG algorithms\, respectively.\nThe monolithic spatia
 l resolution of the semi-monolithic block and the DOI resolution of both c
 rystals were studied. In each case a NN based on a MLP was used. For the t
 raining and testing along the monolithic direction\, a slit collimator was
  moved in 1 mm steps between the detector under study and a single BGO pix
 el. For the DOI evaluation\, the slit was displaced in 2 mm steps along th
 e 25.8×15 mm2 face. In all cases the data was split into training\, evalu
 ation and testing datasets. The testing dataset was used for predicting th
 e monolithic/DOI positions and the FWHM and MAE of the error profiles are 
 reported. The mean monolithic spatial resolution of the semi-monolithic bl
 ock was 3.4±1.1 mm. For the pseudo-slabs crystal\, all pixels are well re
 solved. The mean DOI spatial resolution values was 3.8± 0.9 mm and 4.3±0
 .5 mm for the semi-monolithic and pseudo-slabs crystal\, respectively. \nT
 he results obtained indicate that both crystals are suitable for a clinica
 l PET system. We are currently working on the timing capabilities for thes
 e BGO blocks using ASICs.\n\nhttps://indico.ific.uv.es/event/8181/contribu
 tions/28523/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28523/
END:VEVENT
BEGIN:VEVENT
SUMMARY:IMAS: a Total-Body PET system with TOF and DOI capabilities
DTSTART;VALUE=DATE-TIME:20251027T151500Z
DTEND;VALUE=DATE-TIME:20251027T153000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28525@indico.ific.uv.es
DESCRIPTION:Speakers: Álvaro Anreus (i3M\, grupo DMIL)\nTotal-Body Positr
 on Emission Tomography (TB-PET) systems have become very popular in the re
 cent times\, due to their increased sensitivity with respect to Whole-Body
  (WB) PET systems. This is mainly attributed to their extended axial Field
  of View (FOV) and\, in a few cases\, the capability of Time of Flight (TO
 F) information. This combination enables the simultaneous visualization of
  the biomarker distribution across multiple organs.\nThe DMIL group from i
 3M has recently developed and built\, with the collaboration of other rese
 arch groups and companies\, a new TB-PET scanner\, named IMAS\, already in
 stalled at Hospital La Fe in Valencia\, \nThe IMAS scanner features five r
 ings with an inner diameter of 82 cm and an axial length of around 10 cm e
 ach\, separated by 5 cm gaps between rings. This gives a total axial cover
 age of 70 cm. The IMAS scanner is based on semi-monolithic scintillator cr
 ystal with a total of 15\,260 LYSO slabs\, grouped into mini-modules (MM).
  Each MM contains an array of 1x8 LYSO slabs of 25×3×20 mm3\, wrapped wi
 th Enhanced Specular Reflector (ESR) and coupled to an array of 8×8 Silic
 on Photomultipliers (SiPM) from Hamamatsu Photonics\, model S13361-3075AE-
 08. Our design also uses novel multiplexed read-out electronics that reduc
 e the number of signals from N2 to N. The x-(pixelated) coordinates are di
 rectly inferred from the triggered pixel\, while y-(monolithic) and DOI (z
 ) coordinates were estimated using two different Multilayer Perceptron’s
  (MLPs). Images were reconstructed using iterative methods.  For the entir
 e NEMA protocol\, we used the Maximum-Likelihood Expectation-Maximization 
 (MLEM) algorithm. We also carried out the first studies with patients. The
 se images were reconstructed using the Ordered Subset Expectation Maximiza
 tion (OSEM) algorithm.\nA preliminary experimental evaluation of the IMAS 
 system was performed . A system spatial resolution of 3.37 mm was obtained
  at the center of the scanner. This value remains almost constant along th
 e radial direction due to the DOI capabilities of the system. The system h
 as a peak sensitivity of 7.6% at the center of the scanner. \nA significan
 t step forward has been accomplished by acquiring the first patient images
  with the system. Clinically\, image quality of our IMAS system seems to b
 e superior to the conventional WB-PET/CT.\n\nhttps://indico.ific.uv.es/eve
 nt/8181/contributions/28525/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28525/
END:VEVENT
BEGIN:VEVENT
SUMMARY:PET Image Quality impact with CT Dosage Optimization
DTSTART;VALUE=DATE-TIME:20251027T150000Z
DTEND;VALUE=DATE-TIME:20251027T151500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28528@indico.ific.uv.es
DESCRIPTION:Speakers: Edwing Yair Ulin Briseño (Instituto de Instrumentac
 ión de imagen Molecular (I3M)\, CSIC-UPV\, Valencia)\nPositron Emission T
 omography (PET) relies on CT-based attenuation maps for accurate image rec
 onstruction. The quality of these attenuation maps depends on CT acquisiti
 on parameters\, particularly tube voltage and current. Higher tube current
 s improve image quality by reducing noise\, but at the cost of higher radi
 ation exposure. Conversely\, reducing the current lowers the radiation dos
 e but introduces more noise\, which may affect PET quantification. Optimiz
 ing this balance is especially relevant in new long axial field-of-view PE
 T systems\, where higher sensitivity enables lower CT doses. This study ev
 aluates how different CT dose levels affect PET image reliability\, using 
 the IMAS Total-Body PET system installed at La Fe Hospital in Valencia.\nT
 he experimental setup included the IMAS PET system\, a GE Brightspeed CT s
 canner\, and the NEMA IEC Body Phantom. The IMAS system employs semi-monol
 ithic crystals\, provides a 71.4 cm axial field of view\, includes time-of
 -flight capabilities\, and delivers spatial resolution below 4 mm uniforml
 y across the field of view. CT scans were acquired at 80\, 100\, and 120 k
 V\, with tube currents ranging from 10 to 120 mA in steps 10\, producing 4
 8 CT datasets. PET images were reconstructed with the OSEM algorithm using
  20 iterations. Quantitative analysis of the CT images was performed with 
 two regions of interest (ROIs): one covering the phantom background\, excl
 uding the lung insert\, and one inside the lung insert. The mean and stand
 ard deviation of voxel values were extracted for each ROI. Additionally\, 
 representative CT dose levels were selected\, and the corresponding PET im
 ages were evaluated according to the NEMA NU 2-2018 image quality protocol
 .\nROI analysis of the CT confirmed stable mean attenuation across tube cu
 rrents and voltages\, even at low doses. Noise increased in the background
  at low currents\, especially at 80 kV\, while the lung insert remained mo
 re stable\, indicating that noise propagation affects uniform regions.\nTh
 e analysis based of the PET images using the NEMA protocol\, compared low\
 , mid\, and high CT dose levels. Contrast recovery improved with increasin
 g sphere diameter\, and was higher for mid and high dose acquisitions\, wh
 ile low-dose conditions consistently showed lower recovery values. Backgro
 und variability decreased with sphere size but was always higher in the lo
 w-dose group than in the mid and high doses. Importantly\, differences bet
 ween mid and high dose conditions were minimal\, suggesting that intermedi
 ate CT dose levels are sufficient to ensure robust PET image quality while
  avoiding unnecessary exposure.\nIn conclusion\, the reliability of PET im
 ages in the IMAS system remains consistent across most CT dose levels\, wi
 th mean attenuation preserved even at low doses. Still\, very low currents
 \, particularly at 80 kV\, increase noise and reduce contrast recovery. NE
 MA analysis shows that mid-level doses perform similarly to high doses\, o
 ffering the best balance between safety and diagnostic quality. The study 
 confirms the feasibility of optimized low-dose PET/CT protocols.\n\nhttps:
 //indico.ific.uv.es/event/8181/contributions/28528/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28528/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Deep Learning-Based Super-Resolution of Cardiac PET Images Guided 
 by Ultrafast Ultrasound
DTSTART;VALUE=DATE-TIME:20251027T144500Z
DTEND;VALUE=DATE-TIME:20251027T150000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28540@indico.ific.uv.es
DESCRIPTION:Speakers: Eva Zabala Sanz De Galdeano (Complutense University 
 of Madrid\, Spain)\nCardiac Positron Emission Tomography (PET) is a powerf
 ul molecular imaging technique\, but its use is severely limited by poor s
 patial resolution. This limitation is particularly critical in preclinical
  studies with rodents\, where small anatomical structures\, high respirato
 ry and heart rates exacerbate image blurring\, partial volume effects\, an
 d quantitative errors [1]. These degradations arise from fundamental physi
 cal factors—positron range (PR)\, finite detector size\, acollinearity\,
  photon scatter—and are further amplified by physiological cardiac and r
 espiratory motion [2]. To address this\, we developed a novel deep learnin
 g-based super-resolution framework that integrates high-resolution ultrafa
 st ultrasound (UUS) images as a priori anatomical and motion information t
 o guide cardiac PET resolution recovery. Unlike previous approaches relyin
 g only on low-resolution PET data\, this method leverages UUS images acqui
 red simultaneously and co-registered with PET on the hybrid system PETRUS 
 (PET/CT combined with UUS) [3]\, capturing fine structural boundaries and 
 cardiac motion patterns.\nRealistic PET data were generated using 50 digit
 al mouse phantoms with the MOBY numerical phantom [4] to model diverse ana
 tomies\,  cardiac and respiratory cycles. Physical and instrumental degrad
 ation factors -such as PR effects (simulated with PENEASY [5])\, point spr
 ead function (PSF) blurring\, and statistical noise - were applied to FDG 
 activity maps\, using experimentally measured parameters from the PETRUS s
 canner [6]. In parallel\, corresponding UUS images were simulated for the 
 same anatomical models using MUST simulations [7]. Two U-Net [8] convoluti
 onal neural networks were trained: one using only PET images\, and another
  combining PET with co-registered UUS guidance.\nThe UUS-guided model clea
 rly outperformed the PET-only model\, achieving superior recovery of fine 
 myocardial structures\, higher SUV accuracy\, and enhanced contrast in hig
 h-uptake regions (Fig.1). When applied to experimental datasets acquired w
 ith PETRUS\, it produced sharper images with reduced noise and partial vol
 ume effects. These results show that incorporating anatomical and motion p
 riors from UUS can overcome intrinsic resolution limits of cardiac PET\, e
 nabling more reliable quantification in cardiovascular diseases.\n[1] J.J.
  Vaquero\, P. Kinahan\, Positron Emission Tomography: Current Challenges a
 nd Opportunities for Technological Advances in Clinical and Preclinical Im
 aging Systems\, Annu. Rev. Biomed. Eng. 17\, 385 (2015).\n[2] M. Perez-Liv
 a et al.\, Ultrafast Ultrasound Imaging for Super-Resolution Preclinical C
 ardiac PET\, Mol. Imaging Biol. 22\, 1342 (2020).\n[3] J. Provost et al.\,
  Simultaneous positron emission tomography and ultrafast ultrasound for hy
 brid molecular\, anatomical and functional imaging\, Nat. Biomed. Eng. 2\,
  85–94 (2018).\n[4] W.P. Segars et al.\, Development of a 4-D digital mo
 use phantom for molecular imaging research. Mol. Imaging Biol. 6\, 149–1
 59 (2004). \n[5] J. Sempau et al.\, A PENELOPE‐based system for the auto
 mated Monte Carlo simulation of clinacs and voxelized geometries—applica
 tion to far‐from‐axis fields. Med. Phys.\, 38(11)\, 5887-5895 (2011).\
 n[6 ] M. Perez-Liva et al.\, Performance evaluation of the PET component o
 f a hybrid PET/CT-ultrafast ultrasound imaging instrument\, Phys. Med. Bio
 l. 63\, 19NT01 (2018). \n[7] D. Garcia\, Make the Most of MUST: An Open-So
 urce Matlab Ultrasound Toolbox\, IEEE IUS (2021).\n [8] G. Du et al.\, Med
 ical Image Segmentation Based on U-Net: A Review\, J. Imaging Sci. Technol
 . 64(2) (2020).\n\nhttps://indico.ific.uv.es/event/8181/contributions/2854
 0/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28540/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Technological developments and evaluation of the radiosensitizing 
 potential of gold nanoparticles (AuNPs) for hadron therapy.
DTSTART;VALUE=DATE-TIME:20251027T113000Z
DTEND;VALUE=DATE-TIME:20251027T114500Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28530@indico.ific.uv.es
DESCRIPTION:Speakers: Nuria Fuster Martínez (Instituto de Física Corpusc
 ular\, IFIC (CSIC-UV))\nApproximately half of newly diagnosed cancer patie
 nts undergo radiotherapy\, most\ncommonly with X-rays. Proton therapy has 
 emerged as an advanced alternative\,\noffering highly localized energy dep
 osition at the Bragg peak\, which reduces\nirradiation of healthy tissues 
 and associated toxicity. Technological advances have\nenhanced its availab
 ility in clinical routine\, which has redirected research efforts\ntoward 
 maximizing the therapeutic potential of proton therapy and improving\npati
 ents’ long-term quality of life.\n\nWithin this framework\, a promising 
 strategy is the combination of proton therapy\nwith radiosensitizers. Amon
 g them\, gold nanoparticles (AuNPs) stand out because of\ntheir high atomi
 c number\, biocompatibility\, low toxicity\, and natural tendency to\naccu
 mulate in tumors\, which makes them especially attractive for improving\nt
 herapeutic outcomes. Their use has demonstrated radiation enhancement effe
 cts in\nboth in vitro and in vivo studies. However\, the underlying mechan
 isms responsible\nfor the observed increase in effectiveness under proton 
 irradiation remain poorly\nunderstood\, underscoring the need for further 
 research to enable an efficient.\n\nThis work is being conducted by a mult
 idisciplinary collaboration involving physicists\nfrom the Universidad de 
 Sevilla (US) and the Instituto de Física Corpuscular (IFIC)\,\nbiochemist
 s from the Universitat de València (UV)\, and biologists from the Centro\
 nAndaluz de Biología Molecular y Regenerativa (CABIMER). Irradiations of 
 cell samples\nwere carried out at the Centro Nacional de Aceleradores (Sev
 ille\, Spain) using a\nCyclone 18/9 cyclotron (Ion Beam Applications\, IBA
 \, Belgium)\, which can accelerate\nprotons and deuterons to 18 and 9 MeV\
 , respectively. Significant efforts have been\ndevoted to improving experi
 mental conditions through the development and\nimplementation of new techn
 ologies\, such as a robotic arm for remote sample\nhandling\, which facili
 tate data acquisition and enable a greater number of\nirradiations per exp
 erimental campaign. The study investigates the radiosensitizing\neffects o
 f 50 nm diameter gold nanoparticles (AuNPs) in HeLa cells irradiated with\
 nprotons. A comprehensive set of assays\, including clonogenic survival as
 says and\nimmunofluorescence analyses with Hela cells\, was performed to a
 ssess cell survival\nand DNA damage response in the presence and absence o
 f AuNPs. Preliminary\nfindings support the potential of AuNPs as effective
  radiosensitizers in proton\ntherapy.\n\nhttps://indico.ific.uv.es/event/8
 181/contributions/28530/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28530/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Radiation field characterization of a nuclear reactor as a thermal
  neutron source for  BNCT in-vitro studies
DTSTART;VALUE=DATE-TIME:20251027T111500Z
DTEND;VALUE=DATE-TIME:20251027T113000Z
DTSTAMP;VALUE=DATE-TIME:20260815T015023Z
UID:indico-contribution-8181-28531@indico.ific.uv.es
DESCRIPTION:Speakers: JOAN FLORS MARTI (i3M (CSIC-UPV))\nBoron Neutron Cap
 ture Therapy (BNCT) is a neutron-based treatment designed to eliminate tum
 ors\, mainly head and neck tumors or Glioblastoma Multiforme (GBM)\, using
  1 or 2 sessions\, which is an advantage over conventional therapies that 
 could use more than 20 individual sessions. It is a two-step strategy: fir
 st\, the administration of a boron-containing compound to selectively enri
 ch tumor cells with boron-10 nuclei\; and second\, irradiation with therma
 l neutrons. The aim is to induce reactions between thermal neutrons and bo
 ron-10 nuclei\, releasing high-LET alpha particles with an average range s
 horter than the cell size. This feature gives BNCT a highly selective and 
 destructive character\, maximizing the dose contrast between tumor and hea
 lthy tissue. \n\nThe uptake of boron-rich nanoparticles and the response t
 o BNCT can be studied in-vitro with cell cultures. This requires access to
  a source of thermal neutrons at very high flux. In this work\, a nanopart
 icle-based boron compound was tested through a series of experiments carri
 ed out at the TRIGA nuclear reactor in Mainz. The objectives focused on th
 e one hand\, on characterizing the background dose generated by the reacto
 r. For this purpose\, pre-calibrated radiochromic films (RCF) were used un
 der different reactor power and irradiation time configurations. In some e
 xperiments\, parts of the RCF were covered with cadmium or lead to attenua
 te this background dose. These results allow for estimating the dose absor
 bed by a cell population exposed to the reactor in the absence of alpha pa
 rticle production. It is worth noting that this dose originates both from 
 the photon background and from fast\, unmoderated neutrons emitted from th
 e reactor core. \n\nOn the other hand\, aqueous solutions of the boron-con
 taining compound were prepared at different concentrations and irradiated 
 under variable power and time conditions in wells of Petri plates. The wel
 l openings were covered with PADC (CR-39) detectors to register alpha-part
 icle tracks generated by the interaction between boron-10 nuclei and therm
 al neutrons. After etching\, holes associated with alpha particles were ob
 served\, superimposed on a rough background attributed to secondary proton
 s produced by fast neutrons. These observations qualitatively confirm alph
 a production. \n\nAs a future perspective\, we plan to use cell lines incu
 bated with these boron-based nanoparticles to evaluate both the absorbed d
 ose and the cell survival fraction under nuclear reactor irradiation.\n\nh
 ttps://indico.ific.uv.es/event/8181/contributions/28531/
LOCATION:Jardín Botánico de la Universitat de València
URL:https://indico.ific.uv.es/event/8181/contributions/28531/
END:VEVENT
END:VCALENDAR
