Salih Mustafa Karabıdak
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Salih Mustafa Karabıdak has a total of 11 co-authors. Here are the top co-authors by number of shared publications:
- Selim Kaya
Faculty of Engineering and Natural Sciences, Department of Physics Engineering, Gümüşhane University, Gümüşhane, Türkiye
6 shared publications U. Cevik
Karadeniz Technical University
2 shared publicationsU. Çevik
Karadeniz Technical University
2 shared publicationsA. Kaya
Department of Physics Engineering, Faculty of Engineering and Natural Sciences, Gümüşhane University, Gümüşhane, Turkey
1 shared publicationA. Çelik
Giresun University
1 shared publicationAhmet Celik
Giresun University
1 shared publication
Latest Publications
- 1 September 2020
- Published by Canadian Science Publishing in Canadian Journal of Physics
- Vol. 98 (9) , 877-882
PUC Program: the pulse pile up correction for X-ray and gamma ray spectrometry
Pile up and dead time are two important corrections in the analysis of X-ray and gamma ray spectra. The most important of these is pile up correction because these peaks do not really exist in the spectra; they only seem to exist. For this reason, these peaks affect both the qualitative and quantitative accuracy of the analysis. In addition, the pile up pulses forming the pile up peaks increase the background count in the spectrum. Companies that produce X-ray or gamma ray detector systems design pile up reject circuits and integrate them into detector systems to prevent these pulses. These circuits have time limitations because they are made up of electronic devices. For this reason, the pile up problem cannot be solved completely in these circuits. Therefore, mathematical models based on a statistical approach are needed. Such a model was developed in this study. A computer program based on this model was developed. This developed program has been applied to X-ray and gamma ray spectra. It has been shown that this model provides about 2% correction in the main peak regions and significantly reduces background counts.
- 1 September 2020
- Published by Canadian Science Publishing in Canadian Journal of Physics
- Vol. 98 (9) , 877-882
PUC Program: the pulse pile up correction for X-ray and gamma ray spectrometry
Pile up and dead time are two important corrections in the analysis of X-ray and gamma ray spectra. The most important of these is pile up correction because these peaks do not really exist in the spectra; they only seem to exist. For this reason, these peaks affect both the qualitative and quantitative accuracy of the analysis. In addition, the pile up pulses forming the pile up peaks increase the background count in the spectrum. Companies that produce X-ray or gamma ray detector systems design pile up reject circuits and integrate them into detector systems to prevent these pulses. These circuits have time limitations because they are made up of electronic devices. For this reason, the pile up problem cannot be solved completely in these circuits. Therefore, mathematical models based on a statistical approach are needed. Such a model was developed in this study. A computer program based on this model was developed. This developed program has been applied to X-ray and gamma ray spectra. It has been shown that this model provides about 2% correction in the main peak regions and significantly reduces background counts.
- 1 August 2019
- Published by Springer Nature in Sustainable Water Resources Management
- Vol. 5 (4) , 1939-1949
Cancer risk analysis of some drinking water resources in Gümüşhane, Turkey
- 1 August 2019
- Published by Springer Nature in Sustainable Water Resources Management
- Vol. 5 (4) , 1939-1949
Cancer risk analysis of some drinking water resources in Gümüşhane, Turkey
- Open Access
- 24 May 2017
- Published by IntechOpen
Dead Time in the Gamma‐Ray Spectrometry
Dead Time in the Gamma‐Ray Spectrometry | InTechOpen, Published on: 2017-05-24. Authors: Salih Mustafa Karabıdak
- 24 May 2017
- Published by IntechOpen
Open AccessDead Time in the Gamma‐Ray Spectrometry
Dead Time in the Gamma‐Ray Spectrometry | InTechOpen, Published on: 2017-05-24. Authors: Salih Mustafa Karabıdak
- 1 January 2017
- Published by AIP Publishing in AIP Conference Proceedings
- Vol. 1815, 060012
The determination of the pulse pile-up reject (PUR) counting for X and gamma ray spectrometry
The collection the charged particles produced by the incident radiation on a detector requires a time interval. If this time interval is not sufficiently short compared with the peaking time of the amplifier, a loss in the recovered signal amplitude occurs. Another major constraint on the throughput of modern x or gamma-ray spectrometers is the time required for the subsequent the pulse processing by the electronics. Two above-mentioned limitations are cause of counting losses resulting from the dead time and the pile-up. The pulse pile-up is a common problem in x and gamma ray radiation detection systems. The pulses pile-up in spectroscopic analysis can cause significant errors. Therefore, inhibition of these pulses is a vital step. A way to reduce errors due to the pulse pile-up is a pile-up inspection circuitry (PUR). Such a circuit rejects some of the pulse pile-up. Therefore, this circuit leads to counting losses. Determination of these counting losses is an important problem. In this work, a new method is suggested for the determination of the pulse pile-up reject.
- 1 January 2017
- Published by AIP Publishing in AIP Conference Proceedings
- Vol. 1815, 060012
The determination of the pulse pile-up reject (PUR) counting for X and gamma ray spectrometry
The collection the charged particles produced by the incident radiation on a detector requires a time interval. If this time interval is not sufficiently short compared with the peaking time of the amplifier, a loss in the recovered signal amplitude occurs. Another major constraint on the throughput of modern x or gamma-ray spectrometers is the time required for the subsequent the pulse processing by the electronics. Two above-mentioned limitations are cause of counting losses resulting from the dead time and the pile-up. The pulse pile-up is a common problem in x and gamma ray radiation detection systems. The pulses pile-up in spectroscopic analysis can cause significant errors. Therefore, inhibition of these pulses is a vital step. A way to reduce errors due to the pulse pile-up is a pile-up inspection circuitry (PUR). Such a circuit rejects some of the pulse pile-up. Therefore, this circuit leads to counting losses. Determination of these counting losses is an important problem. In this work, a new method is suggested for the determination of the pulse pile-up reject.
- 1 November 2013
- Published by Elsevier in Radiation Measurements
- Vol. 58, 18-23
Decaying source model: Alternative approach to determination of true counting rates at X and gamma ray counting systems
- 1 November 2013
- Published by Elsevier in Radiation Measurements
- Vol. 58, 18-23
Decaying source model: Alternative approach to determination of true counting rates at X and gamma ray counting systems
- 1 April 2011
- Published by Elsevier in Radiation Measurements
- Vol. 46 (4) , 446-450
Determination of proper peaking time for Ultra-LEGe detector
- 1 April 2011
- Published by Elsevier in Radiation Measurements
- Vol. 46 (4) , 446-450
Determination of proper peaking time for Ultra-LEGe detector
- 24 April 2010
- Published by Springer Nature in Water, Air, & Soil Pollution
- Vol. 214 (1-4) , 461-469
Radon Survey and Exposure Assessment in Karaca and Çal Caves, Turkey
- 24 April 2010
- Published by Springer Nature in Water, Air, & Soil Pollution
- Vol. 214 (1-4) , 461-469
Radon Survey and Exposure Assessment in Karaca and Çal Caves, Turkey
- 1 September 2007
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
- Vol. 262 (2) , 165-170
K-shell X-ray fluorescence cross-sections and intensity ratios for some pure metals at 59.5 and 123.6keV
- 1 September 2007
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
- Vol. 262 (2) , 165-170
K-shell X-ray fluorescence cross-sections and intensity ratios for some pure metals at 59.5 and 123.6keV