Vol. 10, 2025

Radon and Thoron

THE RADON EYE MONITOR: A REVIEW OF BENEFITS AND PROBLEMS

Peter Bossew

Pages: 1-5

DOI: 10.37392/RapProc.2025.01

The RadonEye is an active radon gas monitor that has become increasingly popular for some years. Among consumer grade active radon monitors it is the most sensitive one. It is sold for a fair price and it is easy to operate via a Smartphone app through Bluetooth connection. This makes it useful for individual radon monitoring and for research in the framework of Citizen Science, for example in the context identifying radon priority areas, recording radon time series or measuring radon exhalation. If limitations are considered, it can be used in scientific research. In this paper its benefits and problems are reviewed and examples of its usage given.
  1. P. Bossew, E. Benà, S. Chambers, M. Janik, “Analysis of outdoor and indoor radon concentration time series recorded with RadonEye monitors,”Atmosphere, vol. 15, no. 12, 1468, Dec. 2024.
    DOI: 10.3390/atmos15121468
  2. P. Bossew, “Performance of the RadonEye Monitor,” Atmosphere, vol. 16, no. 5, 525, May 2025.
    DOI: 10.3390/atmos16050525
  3. P. Bossew, “The RadonEye monitor - Benefits and problems,” presented at Int. Conf. Radiat. Appl. (RAP 2025), Crete, Greece, May 2025.
    Retrieved from: https://www.rap-conference.org/25/index.php?page=presentations
    Retrieved on: Jun. 22, 2025
  4. P. Bossew, M. Janik, “Radon time series” in Book of Abstr. 17th Int. workshop on the Geological Aspects of Radon Risk Mapping (GARRM 2025), Prague, Czech Republic, 2025.
  5. FTLAB Corp., Ansan, South Korea, 2001.
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  6. P. Warkentin, E. Curry, O. Michael, B. Bjorndal, “A comparison of consumer-grade electronic radon monitors,” J. Radiol. Prot., vol. 40, no. 4, pp. 1258 – 1272, Dec. 2020.
    DOI: 10.1088/1361-6498/ab96d6
  7. K. Mitev et al., “Recent work with electronic radon detectors for continuous Radon-222 monitoring,” JERA, vol. 3, 8844, Dec. 2022.
    DOI: 10.35815/radon.v3.8844
  8. J. P. Sá, P. T. B. S. Branco, M. C. M. Alvim-Ferraz, F. G. Martins, S. I. V. Sousa, “Radon in Indoor Air: Towards Continuous Monitoring,” Sustainability, vol. 14, no. 3, 1529, Feb. 2022.
    DOI: 10.3390/su14031529
  9. T. Turtiainen, K. Mitev, R. Dehqanzada, O. Holmgren, S. Georgiev, “Testing of thoron cross-interference of continuous radon measuring instruments,” JERA, vol. 3, 7694, Mar. 2022.
    DOI: 10.35815/radon.v3.7694
  10. I. Dimitrova et al., “Study of the performance and time response of the RadonEye Plus2 continuous radon monitor,” Measurement, vol. 207, 112409, Feb. 2023.
    DOI: 10.1016/j.measurement.2022.112409
  11. A. Bahadori, B. Hanson, “Evaluation of consumer digital radon measurement devices: a comparative analysis,” J. Radiol. Prot., vol. 44, no. 2, 021514, Jun. 2024.
    DOI: 10.1088/1361-6498/ad4bf1
  12. T. R. Beck, E. Foerster, M. Biel, S. Feige, “Measurement Performance of Electronic Radon Monitors,” Atmosphere, vol. 15, no. 10, 1180, Oct. 2024.
    DOI: 10.3390/atmos15101180
  13. D. Rábago et al., “Investigation of the Performance of Various Low-Cost Radon Monitors under Variable Environmental Conditions,” Sensors, vol. 24, no. 6, 1836, Mar. 2024.
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  14. J. F. Rey, N. Meisser, D. Licina, J. Goyette Pernot, “Performance evaluation of radon active sensors and passive dosimeters at low and high radon concentrations,” Build. Environ., vol. 250, 111154, Feb. 2024.
    DOI: 10.1016/j.buildenv.2023.111154
  15. J. F. Rey, N. Meisser, D. Licina, J. Goyette Pernot, “Evaluating the impact of indoor aerosols on the performance of real-time radon sensors,” Front. Built Environ. vol. 10, 1407499, May 2024.
    DOI: 10.3389/fbuil.2024.1407499
  16. S. D. Chambers et al., “Portable two-filter dual-flow-loop 222Rn detector: stand-alone monitor and calibration transfer device,” ADGEO, vol. 57, pp. 63 – 80, May 2022.
    DOI: 10.5194/adgeo-57-63-2022
  17. P. Bossew, J. Vaupotič, Approximate secondary calibration of RadonEye monitors. In preparation.
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  19. D. E. Tchorz-Trzeciakiewicz, M. Rysiukiewicz, “Ambient gamma dose rate as an indicator of geogenic radon potential,” Sci. Total. Environ., vol. 755, part 1, 142771, Feb. 2021.
    DOI: 10.1016/j.scitotenv.2020.142771

Biotechnology

STUDY OF CHARACTERISTICS OF PRIMULA VULGARIS USING RAMAN SPECTROSCOPY

Evi Llaka, Arjana Ylli, Ramadan Firanj, Eugena Dedushaj

Pages: 6-10

DOI: 10.37392/RapProc.2025.02

Primrose, or Primula vulgaris, is a perennial herb that has long been prized for its therapeutic qualities. The entire plant is used for its expectorant, anti-inflammatory, analgesic, antispasmodic, and healing-promoting properties. P. vulgaris is effective in treating rheumatic disorders, gout, insomnia, anxiety, respiratory tract infections, and bronchitis. This study examines the ecological variation of Primula vulgaris from two locations: Dajti Mountain, which is 1023 meters above sea level, and the Tirana Hills, 217 meters above sea level. These locations provide different environmental conditions, making it possible to investigate how these ecological variations might affect the traits of plants. Leaf dimensions (length and width), chlorophyll content were measured, and statistical analysis were performed using Mann-Whitney U test. The findings showed that there was a statistically significant variation in leaf size, with Dajti Mountain plants having shorter leaves. For this study, Raman spectroscopy measurements were performed using a B&W Tek i-Raman Ex Raman spectrometer. We have encountered the presence of Rutin and Tangerine essential oil, from the characteristic peaks present in the Raman spectra. These findings provide insights into how altitude and light exposure shape the morphological, physiological, and chemical traits of Primula vulgaris, revealing that plants in sunnier, low-altitude habitats develop broader leaves and higher concentrations of bioactive compounds, while those at higher elevations exhibit greater chlorophyll content and enhanced photosynthetic efficiency.
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Radon and Thoron

INDOOR RADON SURVEY IN TIRANA CITY, ALBANIA

Blerim Rrakaqi, Gerti Xhixha, Kozeta Tushe, Merita Xhixha (Kaçeli), Njomza Elezaj, Ylli Kaçiu, Nazim Gashi

Pages: 11-15

DOI: 10.37392/RapProc.2025.03

Indoor radon concentration is investigated in the urban area of Tirana city, the capital of Albania. CR-39 Solid State Nuclear Track Detectors (SSNTDs) are used to survey 147 dwellings and 78 workplaces during 3-month measurements. In dwellings, the arithmetic mean and geometric mean value of radon concentration are found to be 97 and 71 Bq/m3, while in workplaces 131 and 98 Bq/m3, respectively. Radon concentration on the ground floor in dwellings is higher than that of other floors, while for workplaces no significant difference is found among floors. Radon concentrations in dwellings and workplaces are found to be higher than the reference level of 300 Bq/m3 for approximately 6% and 9% of cases, respectively. The results are spatially distributed using a grid of 1×1 km2 realizing the indoor radon map showing the number of measurements and the arithmetic mean values. This information is used to assess the radiation health risk due to residential exposure to radon indoors.
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Radiation Measurements

OPTIMAL GEOMETRIC DESIGN OF THE DIAPHRAGM OF A FREE-AIR IONIZATION CHAMBER FOR LOW-ENERGY X-RAYS

Jessica Gschweng, Stefan Pojtinger

Pages: 16-20

DOI: 10.37392/RapProc.2025.04

For reliable and comparable measurements of the dose quantity air kerma, dosimeter measurements must be traceable to a primary standard. Primary standard laboratories use free-air ionization chambers (FACs) for the primary realization of the unit of the air kerma free-in-air. Correction factors must be applied to convert measured charge to air kerma. One such correction factor is the correction factor for diaphragm effects (kdia). This study investigated the impact of the geometry of the diaphragm on kdia, as established FACs from different metrology institutes use different diaphragm geometries. The aim was to find the optimal diaphragm thickness and aperture shape to minimize the required diaphragm correction for the new PTB primary standard. Monte Carlo simulations were performed to determine kdia for various diaphragm geometries of a low-energy x-ray FAC. The influence of the diaphragm thickness and the aperture shape were investigated. The results showed that the diaphragm needs to be sufficiently thick to prevent transmission yet as thin as possible to reduce scattering at the inner surface of the aperture. The optimal diaphragm thickness, which depends on the air path length of the FAC, ranges from 0.8 mm to 1 mm. Using a diaphragm geometry with a more complex geometry than a simple 1 mm thick diaphragm with a cylindrical aperture is not advantageous.
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Medical Physics

EXAMINING LESION VISIBILITY OF THICK COMPRESSED BREASTS UNDER DIFFERENT IONIZING RADIATION EXPOSURE CONDITIONS BY USING A MAMMOGRAPHIC MATHEMATICAL PHANTOM

Spyridoula Katsanevaki, Nektarios Kalyvas, Christos Michail, Ioannis Valais, George Fountos, Ioannis Kandarakis

Pages: 21-27

DOI: 10.37392/RapProc.2025.05

Mammography is an X-ray imaging application used for breast diagnosis. Its high importance is denoted by the routinely mammographic examinations suggested for women above a certain age. In the era of digital mammography, various dedicated detector designs have been considered for possible use in a mammographic system. Despite, the detector characteristics the image of thick or dense breasts is a challenge since the amount of radiation transmitted through the breast and incident at the detector surface is a function of the ionizing radiation energy and exposure. In addition, possible breast lesions may be visible or not depending upon their size and composition. In general, a large size and high atomic number lesion has higher visibility than a small size and low atomic number one. A simple mathematical breast phantom was designed which was comprised from breast tissue as a background material and areas corresponding to a) blood for low atomic number material and b) Ca for a high atomic number material like microcalcifications. The phantom dimensions were 1000×1000 pixels, while the lesions were constructed as squares ranging from 2x2 pixels up to 50×50 pixels and lines. The breast thicknesses considered were 5.2 cm and 6 cm for the phantom. For the Ca the thicknesses ranged from 0.0008 cm up to 0.01 cm and for the blood lesions from 0.08 cm up to 0.5 cm. Simulations of the irradiated with 22 keV and 28 keV X-ray photons for different photon fluences, which after transmission from the phantom they have been assumed to impinge a Dexela mammographic detector, have been performed. It was found that at 22 keV and 6 cm breast thickness the 0.003 cm, 10×10 Ca lesion could be observed as well as the 20×20 blood lesion of 0.2 cm thickness. The increase of photon fluence improved the derived image due to the decrease of the image noise levels. The 5.2 cm thickness irradiation conditions produced less noisy images due to the higher number of photons impinging on the detector surface.
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