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Dive into the research topics where B.C. Bhatt is active.

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Featured researches published by B.C. Bhatt.


Radiation Measurements | 2002

The E1′-centre and its role in TL sensitization in quartz

P.G Benny; T.K. Gundu Rao; B.C. Bhatt

Abstract The effect of UV (253.7 nm ) bleaching and subsequent thermal annealing treatment in the range 400–500°C, were studied in order to investigate the role of E1′-centre on sensitization of 110°C and 220°C peaks in quartz. The decay of E1′-centre in thermal annealed samples and observation of E1′-centres after UV bleach, accompanied by desensitization of TL in the quartz sample, appears to lend support to the role of competing traps and E1′-centres in the sensitization process.


Radiation Measurements | 1997

Sensitization of 220°C TL peak in quartz separated from sand

P.G Benny; B.C. Bhatt

In the present paper we have investigated sensitization of the 220°C TL peak in quartz, separated from sand, as a function of pre-gamma dose and post-irradiation annealing treatment at a test gamma dose of 50 Gy. A pre-gamma dose of 2.50 kGy followed by 400°C post-irradiation annealing treatment yielded the maximum sensitization factor of 35. The sensitization decreases for pre-doses higher than 2.50 kGy as well as for post-irradiation annealing temperatures higher than 400°C. The sensitization of the peak in quartz due to accrued geological dose of 72 Gy and thermal annealing treatment was estimated to be 2.36. The position and shape of the TL glow curve in sensitized and unsensitized samples was nearly the same.


Geochronometria | 2013

Thermally assisted OSL: A potent tool for improvement in minimum detectable dose and extension of dose range of Al2O3:C

Anuj Soni; D.R. Mishra; B.C. Bhatt; Shiv K. Gupta; Narendra S. Rawat; M.S. Kulkarni; Devanand N. Sharma

The influence of electron-phonon interaction on the shape of the optically stimulated luminescence decay curve of Al2O3:C has been studied using thermally assisted optically stimulated luminescence (TA-OSL). The minimum detectable dose (MDD) of a phosphor depends on the standard deviation of the background signal which affects the signal-to-noise ratio. The standard deviation of the background signal reduces at lower stimulation light intensity while the readout time increases. Further, measurement at higher temperature enhances the OSL signal with faster decay due to the temperature dependence of photo-ionization cross-section. To achieve the same decay constant and more signal, the temperature of measurement was raised. As a result of lowering the stimulation in-tensity at higher temperature (85°C) the overall MDD of α-Al2O3:C was found to improve by 1.8 times. For extension of dose linearity in higher range, deeper traps were studied by simultaneous application of CW-OSL and thermal stimulation up to 400°C, using a linear heating rate of 4K/s. By using this method, two well defined peaks at 121°C and 232°C were observed. These TA-OSL peaks have been correlated with two deeper defects which can be thermally bleached at 650°C and 900°C respectively. These deeper defects are stable up to 500°C, so they can store absorbed dose information even if the sample is inadvertently exposed to light or heat. The dose vs. TA-OSL response from deep traps of α-Al2O3:C was found to be linear up to 10 kGy, thus extending its application for high dose dosimetry.


Radiation Protection Dosimetry | 2015

Na2SiF6:Cu,P: a new OSL phosphor for the radiation dosimetric applications.

R. A. Barve; R.R. Patil; S.V. Moharil; N.P. Gaikwad; B.C. Bhatt; Ratna Pradeep; D.R. Mishra; M.S. Kulkarni

A new Cu,P-doped, sodium fluorosilicate-based optically stimulated luminescence (OSL) phosphor is developed. This phosphor shows good OSL properties, and the sensitivity is comparable with that of the commercial Al(2)O(3):C (Landauer, Inc.) phosphor. For the luminescence averaged over initial 1 s, blue-stimulated luminescence and green-stimulated luminescence sensitivities were found to be 0.76 and 3.8 times, respectively, of Al(2)O(3):C (Landauer, Inc.) with 28 % of post-irradiation fading in 3 days and nil thereafter. The simple preparation procedure, fast decay, very good sensitivity and moderate fading will make this phosphor suitable for radiation dosimetry, using OSL.


Radiation Protection Dosimetry | 2016

A new highly sensitive low-Z LiF-based OSL phosphor for radiation dosimetry

R.R. Patil; S. U. Gaikwad; Y. K. More; M.S. Kulkarni; B.C. Bhatt; S.V. Moharil

A new low-Z lithium fluoride-based optical stimulated luminescent (OSL) phosphor is developed. The phosphor shows good OSL properties, and its sensitivity is comparable with that of the commercial Al2O3:C (Landauer, Inc.) phosphor. For the luminescence averaged over initial 3 s, blue stimulated luminescence (BSL) and green stimulated luminescence (GSL) sensitivities were found to be 0.27 and 4 times, respectively, than that of Al2O3:C (Landauer, Inc.). The BSL decay is fast, and the whole signal decays within 3 s; the GSL decay is relatively slow, and the signal decays in 25 s. The fast decay, good sensitivity, good linearity and its near tissue equivalence (Zeff ∼8.14) will make this phosphor suitable for radiation dosimetry particularly in personnel as well as in medical dosimetry.


Phase Transitions | 2016

Thermoluminescence and optically stimulated luminescence in various phases of doped Na2SO4

S.U. Gaikwad; R.R. Patil; M.S. Kulkarni; B.C. Bhatt; S.V. Moharil

The dependence of optically stimulated luminescence (OSL) and thermoluminescence (TL) response due to crystal phase in Cu and Cu,Mg-doped Na2SO4 was studied. Study shows that the slowly cooled samples which crystallize in phase V show good OSL sensitivity whereas the quenched samples of Na2SO4 which crystallize in phase III irrespective of doping show no OSL sensitivity. However, during storage when phase III samples get converted to phase V, samples show OSL sensitivity comparable to freshly prepared samples in phase V. Hence, it is observed that TL–OSL properties of doped Na2SO4 are phase dependent .This study will be helpful in developing OSL phosphors in which phase plays an important role in deciding the desired properties.


Applied Radiation and Isotopes | 2016

Optically stimulated luminescence in doped NaF

S.U. Gaikwad; R.R. Patil; M.S. Kulkarni; B.C. Bhatt; S.V. Moharil

OSL in doped NaF is studied. Study shows that NaF:Mg,Cu,P phosphor possess good OSL properties having sensitivity comparable to that of commercially available Al2O3:C (Landauer Inc.). For the luminescence averaged over 3s the obtained OSL is 37% of that commercial available Al2O3:C. Of the several phosphors investigated, phosphor with impurities concentration Mg(0.01mol%), Cu(0.2mol%), P(1mol%) shows good OSL sensitivity good linearity in the 10mGy to 1Gy dose range and negligible fading. This sample shows a intense single TL peak around 350°C which gets depleted by 14% after the OSL readout. This imply that maximum OSL is coming from deep traps giving stability to the signal. The ease of preparation along with other good OSL properties will make this phosphor suitable for radiation dosimetry applications using OSL.


Applied Radiation and Isotopes | 2016

Effect of Al3+ co-doping on the luminescence properties of Cu doped Na2SiF6

R.A. Barve; R.R. Patil; S.V. Moharil; B.C. Bhatt; M.S. Kulkarni

Studies were carried out to assess the correlation between thermoluminescence (TL) and optically stimulated luminescence (OSL) of this phosphor. It was observed that the OSL and TL glow curve consists of a wide distribution of traps having different photo-ionization cross-sections, trap depths and frequency factors. In case of Al doped sample, some of the traps up to 200°C are assumed to act as a source traps for the observance of OSL due to thermal transfer of charge carriers into the deep traps beyond 480°C. This suggests that Al impurities play an important role in the thermal transfer OSL process. As most of the work on this phenomenon is done on natural materials (mainly quartz) in which aluminum is a natural impurity, this study will explain the role of Al in this phenomenon.


Applied Radiation and Isotopes | 2015

Optically stimulated luminescence studies in combustion synthesized Al2O3:C,Cu,P

R.A. Barve; R.R. Patil; S.V. Moharil; B.C. Bhatt; M.S. Kulkarni

A new Al2O3:C,Cu,P phosphor is developed by the combustion synthesis technique which exhibits entirely different OSL properties as compared to that of the commercial alumina. No thermoluminescence (TL) is observed in this phosphor which also differentiates the present phosphor from the commercially available Al2O3:C (Landauer). The phosphor shows good optically stimulated luminescence (OSL) sensitivity for ionizing radiation with a fast OSL decay as compared to the commercial Al2O3:C. The phosphor heated in air followed by heating under the reactive atmosphere exhibits maximum sensitivity amongst several other phosphors. On the basis of area integration method; integrated over initial 3s, the sensitivity of this phosphor is about 67% of that of commercial Al2O3:C.


ADVANCED MATERIALS AND RADIATION PHYSICS (AMRP-2015): 4th National Conference on Advanced Materials and Radiation Physics | 2015

Optically stimulated luminescence in K2SO4:AEu (A=Ca,Na,Al)

Y. K. More; R.R. Patil; S. P. Wankhede; M.S. Kulkarni; Munish Kumar; B.C. Bhatt; S.V. Moharil

Optically stimulated luminescence in doped K2SO4 is reported. K2SO4 was prepared by simple melt quenched process using readymade potassium sulphate. Samples were doped with Eu and AEu (A=Ca, Na and Al). Out of these samples K2SO4:Eu and K2SO4:Ca,Eu shows good OSL response to 470 nm optical stimulation. K2SO4:Eu and K2SO4:Ca,Eu have the sensitivities comparable with that of commercial phosphor Al2O3:C (Landauer).

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M.S. Kulkarni

Bhabha Atomic Research Centre

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S.V. Moharil

Rashtrasant Tukadoji Maharaj Nagpur University

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D.R. Mishra

Bhabha Atomic Research Centre

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R.R. Patil

Bhabha Atomic Research Centre

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N.S. Rawat

Bhabha Atomic Research Centre

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Anuj Soni

Bhabha Atomic Research Centre

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D.N. Sharma

Bhabha Atomic Research Centre

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Bhushan Dhabekar

Bhabha Atomic Research Centre

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K.P. Muthe

Bhabha Atomic Research Centre

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N.P. Gaikwad

Bhabha Atomic Research Centre

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