<abstract xmlns="http://www.w3.org/1999/xhtml"><p>TlBr single crystals grown using the vertical Bridgman-Stockbarger method were characterized for semiconductor based radiation detector applications. It has been shown that the vertical Bridgman-Stockbarger method is effective to grow high-quality single crystalline ingots of TlBr. The TlBr single crystalline sample, which was located 6 cm from the tip of the ingot, exhibited lower impurity concentration, higher crystalline quality, high enough bandgap (>2.7 eV), and higher resistivity (2.5 × 10<sup>11</sup> Ω·cm) which enables using the fabricated samples from the middle part of the TlBr ingot for fabricating high performance semiconductor radiation detectors.</p></abstract>

TlBr single crystals grown using the vertical Bridgman-Stockbarger method were characterized for semiconductor based radiation detector applications. It has been shown that the vertical Bridgman-Stockbarger method is effective to grow high-quality single crystalline ingots of TlBr. The TlBr single crystalline sample, which was located 6 cm from the tip of the ingot, exhibited lower impurity concentration, higher crystalline quality, high enough bandgap (>2.7 eV), and higher resistivity (2.5 × 1011 Ω·cm) which enables using the fabricated samples from the middle part of the TlBr ingot for fabricating high performance semiconductor radiation detectors.


<div xmlns="http://www.w3.org/1999/xhtml"><sec id="j_msp-2016-0034_s_001_w2aab2b8d168b1b7b1ab1aAa"><label>1</label><div>Introduction</div><p>Semiconductor radiation detectors are of considerable technological importance due to their increasing use in medical imaging, and industrial and transportation security applications <a ref-type="bibr" href="#j_msp-2016-0034_ref_01_w2aab2b8d168b1b7b1ab2b1b1Aa">[1</a>, <a ref-type="bibr" href="#j_msp-2016-0034_ref_02_w2aab2b8d168b1b7b1ab2b1b2Aa">2]</a>. To fabricate such a high-quality semiconductor-based radiation detector, high-quality and high-purity semiconductor single crystals are needed. In addition, materials consisting of high atomic number elements are needed due to the higher probability of an incoming radiation beam interaction with valence electrons <a ref-type="bibr" href="#j_msp-2016-0034_ref_03_w2aab2b8d168b1b7b1ab2b1b3Aa">[3]</a>. In this regard, a TlBr (atomic numbers: Tl-81, Br-35) compound semiconductor with a bandgap of ~2.7 eV is considered as one of the promising candidates for various applications, and was intensively researched by various research groups <a ref-type="bibr" href="#j_msp-2016-0034_ref_04_w2aab2b8d168b1b7b1ab2b1b4Aa">[4</a>–<a ref-type="bibr" href="#j_msp-2016-0034_ref_06_w2aab2b8d168b1b7b1ab2b1b6Aa">6]</a>. Among the various bulk crystal growth methods from the melt, zonemelting <a ref-type="bibr" href="#j_msp-2016-0034_ref_07_w2aab2b8d168b1b7b1ab2b1b7Aa">[7]</a> and Bridgman-Stockbarger <a ref-type="bibr" href="#j_msp-2016-0034_ref_04_w2aab2b8d168b1b7b1ab2b1b4Aa">[4</a>, <a ref-type="bibr" href="#j_msp-2016-0034_ref_06_w2aab2b8d168b1b7b1ab2b1b6Aa">6</a>, <a ref-type="bibr" href="#j_msp-2016-0034_ref_08_w2aab2b8d168b1b7b1ab2b1b8Aa">8]</a> methods were used. In particular, the vertical Bridgman-Stockbarger method was shown to be superior due to the fact that it is the only method by which the large diameter Tl halide ingots can be produced <a ref-type="bibr" href="#j_msp-2016-0034_ref_09_w2aab2b8d168b1b7b1ab2b1b9Aa">[9]</a>.</p><p>Thus, in this paper, we report the fabrication and characterization of TlBr single crystals grown using the vertical Bridgman-Stockbarger method for use in radiation detector applications. In particular, the diced and polished samples were selected from the top, middle, and end parts of the ingot, and these samples were compared in terms of the structural, chemical, electrical, and optical properties.</p></sec><sec id="j_msp-2016-0034_s_002_w2aab2b8d168b1b7b1ab1b1Aa"><label>2</label><div>Experimental</div><sec id="j_msp-2016-0034_s_002_s_001_w2aab2b8d168b1b7b1ab1b1b2Aa"><label>2.1</label><div>Sample preparation</div><p>TlBr raw powders of 99.998 % purity were purchased from Alfa Aesar Co. and were used as-received. These TlBr powders were loaded into a precleaned quartz ampoule with a 1-inch into a precleaned quartz ampoule with a 1-inch diameter and vacuum sealed. This quartz ampoule was loaded into a homemade vertical Bridgman-Stockbarger furnace. This Bridgman-Stockbarger furnace consisted of a top zone, a sandwiched growth zone, and a bottom zone. After complete melting of the materials, the heater unit moved upward at a speed of 1 mm/h, and the temperature gradient at the growth zone was about 10 °C/cm. After the growth zone completely scanned the entire part of the ampoule, the grown ingot was then cooled down to room temperature for a cooling period of 10 hours, finally resulting in a 1-inch single crystalline TlBr ingot with a length of about 95 mm, as shown in <a ref-type="fig" href="#j_msp-2016-0034_fig_001_w2aab2b8d168b1b7b1ab1b1b2b3Aa">Fig. 1a</a>. This TlBr ingot was diced with a diamond wire saw to make the samples, as shown in <a ref-type="fig" href="#j_msp-2016-0034_fig_001_w2aab2b8d168b1b7b1ab1b1b2b3Aa">Fig. 1b</a>, and these samples were then mechanically polished with 800-, 2400-, 4000-grit SiC papers followed by chemical polishing/etching with an etching solution of mixed HBr and methanol (1:5). The samples, which were located about 3 cm, 6 cm, 8 cm from the tip of the ingot, are herein referred to as the ‘top’, ‘middle’, and ‘bottom’ samples, respectively.</p><figure id="j_msp-2016-0034_fig_001_w2aab2b8d168b1b7b1ab1b1b2b3Aa" position="float" fig-type="figure"><h2>Fig. 1</h2><figCaption><p>(a) Single crystalline 1-inch TlBr ingot used in the study, (b) a diced and polished TlBr sample.</p></figCaption><img xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_msp-2016-0034_fig_001.jpg" src="https://sciendo-parsed.s3.eu-central-1.amazonaws.com/64724ff9215d2f6c89dc3d9a/j_msp-2016-0034_fig_001.jpg?X-Amz-Algorithm=AWS4-HMAC-SHA256&amp;X-Amz-Date=20240609T072031Z&amp;X-Amz-SignedHeaders=host&amp;X-Amz-Expires=18000&amp;X-Amz-Credential=AKIA6AP2G7AKP25APDM2%2F20240609%2Feu-central-1%2Fs3%2Faws4_request&amp;X-Amz-Signature=29bd745748da33bfd1ad9c8914dd0f93f6d75b3d0aef325dec0cbba94ae90d2d" class="mw-100"/></figure></sec></sec><sec id="j_msp-2016-0034_s_003_w2aab2b8d168b1b7b1ab1b2Aa"><label>3</label><div>Characterizations</div><p>An impurity analysis was performed using an ICP-MS (inductively coupled plasma mass spectrometry) system (Nexion 300X, Perkin Elmer). Microstructural perfection of the samples was investigated using an XRD (X-ray diffraction) system (D/Max 4200, Rigaku) within the 2 theta range of 20 to 65 degrees. Optical transmittance results were obtained using a UV-Vis spectrophotometer (Cary 300, Agilent Technologies, Co.) equipped with an integrating sphere within the wavelength range of 200 nm to 800 nm. The current-voltage (I-V) characteristics of the samples were measured with a parameter analyzer (4200SCS, Keithley). Before measuring the I-V data, 300 Å thick gold-contacts were evaporated on both sides of the samples.</p></sec><sec id="j_msp-2016-0034_s_004_w2aab2b8d168b1b7b1ab1b3Aa"><label>4</label><div>Results</div><p><a ref-type="fig" href="#j_msp-2016-0034_fig_002_w2aab2b8d168b1b7b1ab1b3b3Aa">Fig. 2</a> and <a ref-type="table" href="#j_msp-2016-0034_tab_001_w2aab2b8d168b1b7b1ab1b3b4Ab2">Table 1</a> show the ICP-MS results for the raw material used, and the top, middle, and bottom samples of TlBr. It should be noted that the concentrations of the major impurity elements observed in the raw material were significantly reduced for the top and middle samples investigated in this study. More notably, some of the elements were not detected in the top, middle and bottom samples, possibly due to the detection limit (resolution) of the equipment used. In addition, the impurity (Mg, Fe, Al) concentrations were higher in the bottom sample compared to those of the top and middle samples. For example, the concentrations of Al were 0.12 ppm, 0.09 ppm, and 0.47 ppm for the top, middle, and bottom samples, respectively. Similar purification effects using the Bridgman-Stockbarger technique were also reported by Dos Santos et al. <a ref-type="bibr" href="#j_msp-2016-0034_ref_010_w2aab2b8d168b1b7b1ab2b1c10Aa">[10]</a>.</p><figure id="j_msp-2016-0034_fig_002_w2aab2b8d168b1b7b1ab1b3b3Aa" position="float" fig-type="figure"><h2>Fig. 2</h2><figCaption><p>ICP-MS results of the raw material, and top and bottom samples of TlBr.</p></figCaption><img xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_msp-2016-0034_fig_002.jpg" src="https://sciendo-parsed.s3.eu-central-1.amazonaws.com/64724ff9215d2f6c89dc3d9a/j_msp-2016-0034_fig_002.jpg?X-Amz-Algorithm=AWS4-HMAC-SHA256&amp;X-Amz-Date=20240609T072031Z&amp;X-Amz-SignedHeaders=host&amp;X-Amz-Expires=18000&amp;X-Amz-Credential=AKIA6AP2G7AKP25APDM2%2F20240609%2Feu-central-1%2Fs3%2Faws4_request&amp;X-Amz-Signature=1b17b31ae4f1428d5ce33207482aa48fcc697d01326d226ff7852bfcdb8be0f6" class="mw-100"/></figure><table-wrap position="float" orientation="portrait" id="j_msp-2016-0034_tab_001_w2aab2b8d168b1b7b1ab1b3b4Ab2"><label>Table 1</label><caption><p>Summary of the major impurities observed in the raw material and in the three samples, which were measured using an ICP-MS.</p></caption><table frame="hsides" rules="groups"><thead><tr><th align="center">Unit [ppm]</th><th align="center">Na</th><th align="center">Ca</th><th align="center">Mg</th><th align="center">Fe</th><th align="center">Al</th><th align="center">Si</th><th align="center">Ga</th><th align="center">K</th><th align="center">In</th></tr></thead><tbody><tr><td align="center">Raw material</td><td align="center">2.00</td><td align="center">5.00</td><td align="center">0.20</td><td align="center">3.00</td><td align="center">0.50</td><td align="center">2.00</td><td align="center">0.20</td><td align="center">0.10</td><td align="center">0.10</td></tr><tr><td align="center">Top</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.01</td><td align="center">0.15</td><td align="center">0.12</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.00</td></tr><tr><td align="center">Middle</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.04</td><td align="center">0.09</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.00</td></tr><tr><td align="center">Bottom</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.04</td><td align="center">0.22</td><td align="center">0.47</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.00</td><td align="center">0.00</td></tr></tbody></table></table-wrap><p><a ref-type="fig" href="#j_msp-2016-0034_fig_003_w2aab2b8d168b1b7b1ab1b3b6Aa">Fig. 3</a> shows the XRD measurement results for the top, middle, and bottom samples investigated in this study. It should be noted that the middle sample (<a ref-type="fig" href="#j_msp-2016-0034_fig_003_w2aab2b8d168b1b7b1ab1b3b6Aa">Fig. 3b</a>) exhibits only a (1 1 0) peak without any additional noticeable peaks within the measured range. However, the top sample additionally exhibits weak peaks corresponding to (1 0 0), (2 0 0), and (2 1 0) (<a ref-type="fig" href="#j_msp-2016-0034_fig_003_w2aab2b8d168b1b7b1ab1b3b6Aa">Fig. 3a</a>). More notably, the bottom sample shows a poorer crystalline quality compared to the other two samples (<a ref-type="fig" href="#j_msp-2016-0034_fig_003_w2aab2b8d168b1b7b1ab1b3b6Aa">Fig. 3c</a>).</p><figure id="j_msp-2016-0034_fig_003_w2aab2b8d168b1b7b1ab1b3b6Aa" position="float" fig-type="figure"><h2>Fig. 3</h2><figCaption><p>XRD patterns for the top, middle, and bottom samples of TlBr.</p></figCaption><img xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_msp-2016-0034_fig_003.jpg" src="https://sciendo-parsed.s3.eu-central-1.amazonaws.com/64724ff9215d2f6c89dc3d9a/j_msp-2016-0034_fig_003.jpg?X-Amz-Algorithm=AWS4-HMAC-SHA256&amp;X-Amz-Date=20240609T072031Z&amp;X-Amz-SignedHeaders=host&amp;X-Amz-Expires=17999&amp;X-Amz-Credential=AKIA6AP2G7AKP25APDM2%2F20240609%2Feu-central-1%2Fs3%2Faws4_request&amp;X-Amz-Signature=6dbf3ab2636c8a34d6dcbe545d5b243451c9cf776a06a10558a3056e043bdacb" class="mw-100"/></figure><p><a ref-type="fig" href="#j_msp-2016-0034_fig_004_w2aab2b8d168b1b7b1ab1b3b9Aa">Fig. 4a</a> shows the transmittance curves for the three samples. It was shown that all the three samples exhibit similar absorption edges. From the transmittance data, optical bandgaps can be extracted. Park et al. explained <a ref-type="bibr" href="#j_msp-2016-0034_ref_011_w2aab2b8d168b1b7b1ab2b1c11Aa">[11]</a> that the absorption coefficient (α) can be defined as:</p><disp-formula id="j_msp-2016-0034_eq_1_w2aab2b8d168b1b7b1ab1b3b8Aa"><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_msp-2016-0034_eq1.png"></graphic><math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="block"><mrow><mi>I</mi><mo>=</mo><msub><mi>I</mi><mn>0</mn></msub><mo>×</mo><mi>exp</mi><mo stretchy="false">(</mo><mo>−</mo><mi>α</mi><mi>t</mi><mo stretchy="false">)</mo></mrow></math><tex-math>$$I = {I_0} \times \exp ( - \alpha t)$$</tex-math></alternatives><label>(1)</label></disp-formula><figure id="j_msp-2016-0034_fig_004_w2aab2b8d168b1b7b1ab1b3b9Aa" position="float" fig-type="figure"><h2>Fig. 4</h2><figCaption><p>(a) Transmittance and (b) α<sup>2</sup> vs. hν curves for the top, middle, and bottom samples of TlBr.</p></figCaption><img xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_msp-2016-0034_fig_004.jpg" src="https://sciendo-parsed.s3.eu-central-1.amazonaws.com/64724ff9215d2f6c89dc3d9a/j_msp-2016-0034_fig_004.jpg?X-Amz-Algorithm=AWS4-HMAC-SHA256&amp;X-Amz-Date=20240609T072031Z&amp;X-Amz-SignedHeaders=host&amp;X-Amz-Expires=18000&amp;X-Amz-Credential=AKIA6AP2G7AKP25APDM2%2F20240609%2Feu-central-1%2Fs3%2Faws4_request&amp;X-Amz-Signature=055cadcd2359a73bf862838ef07e174099d63e42227801089037dfd6fcf6e325" class="mw-100"/></figure><p>where I is intensity of the transmitted light, I<sub>0</sub> – intensity of the incident light, t – thickness of a sample. In the direct transition semiconductor, <italic>α</italic> and optical energy bandgap (E<sub>g</sub>) can also be related by:</p><disp-formula id="j_msp-2016-0034_eq_2_w2aab2b8d168b1b7b1ab1b3c11Aa"><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_msp-2016-0034_eq2.png"></graphic><math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="block"><mrow><mi>α</mi><mo>=</mo><msup><mrow><mo stretchy="false">(</mo><mi>h</mi><mi>ν</mi><mo>−</mo><msub><mi>E</mi><mi>g</mi></msub><mo stretchy="false">)</mo></mrow><mrow><mn>1</mn><mo>/</mo><mn>2</mn></mrow></msup></mrow></math><tex-math>$$\alpha  = {(h\nu  - {E_g})^{1/2}}$$</tex-math></alternatives><label>(2)</label></disp-formula><p>where h is Planck’s constant, and hν the photon energy of the incident light. Thus, after plotting <italic>α</italic><sup>2</sup> vs. hν curves, we can obtain optical bandgaps by extrapolating the linear part of the drawn curves to the α = 0 (x-axis), as can be seen in <a ref-type="fig" href="#j_msp-2016-0034_fig_004_w2aab2b8d168b1b7b1ab1b3b9Aa">Fig. 4b</a>. The optical bandgaps of 2.79 eV (top), 2.76 eV (middle), and 2.78 eV (bottom) were obtained, which are all very similar to the reported value <a ref-type="bibr" href="#j_msp-2016-0034_ref_04_w2aab2b8d168b1b7b1ab2b1b4Aa">[4]</a>.</p><p><a ref-type="fig" href="#j_msp-2016-0034_fig_005_w2aab2b8d168b1b7b1ab1b3c14Aa">Fig. 5</a> shows I-V characteristics of the three samples with Au electrodes on both sides. All samples show very similar linear I-V characteristics, meaning that the Au electrode and TlBr formed ohmic contacts. It was calculated that the resistivities of the samples are 2.2 × 10<sup>11</sup> Ω·cm (top), 2.5 × 10<sup>11</sup> Ω·cm (middle), and 2.2 × 10<sup>11</sup> Ω·cm (bottom), respectively.</p><figure id="j_msp-2016-0034_fig_005_w2aab2b8d168b1b7b1ab1b3c14Aa" position="float" fig-type="figure"><h2>Fig. 5</h2><figCaption><p>I-V characteristics and resistivities of the top, middle, and bottom samples of TlBr.</p></figCaption><img xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/j_msp-2016-0034_fig_005.jpg" src="https://sciendo-parsed.s3.eu-central-1.amazonaws.com/64724ff9215d2f6c89dc3d9a/j_msp-2016-0034_fig_005.jpg?X-Amz-Algorithm=AWS4-HMAC-SHA256&amp;X-Amz-Date=20240609T072031Z&amp;X-Amz-SignedHeaders=host&amp;X-Amz-Expires=18000&amp;X-Amz-Credential=AKIA6AP2G7AKP25APDM2%2F20240609%2Feu-central-1%2Fs3%2Faws4_request&amp;X-Amz-Signature=51666b265a0b6af107665c6c874272ff0e2411a7a13f1992e5e4f78f001b6990" class="mw-100"/></figure></sec><sec id="j_msp-2016-0034_s_005_w2aab2b8d168b1b7b1ab1b4Aa"><label>5</label><div>Discussion</div><p>For any semiconductor material to be used in radiation detector applications that can be operable at room temperature, the material should have possibly low impurity concentration <a ref-type="bibr" href="#j_msp-2016-0034_ref_012_w2aab2b8d168b1b7b1ab2b1c12Aa">[12]</a>, the highest possible crystalline quality <a ref-type="bibr" href="#j_msp-2016-0034_ref_013_w2aab2b8d168b1b7b1ab2b1c13Aa">[13]</a>, a large bandgap, and a high resistivity <a ref-type="bibr" href="#j_msp-2016-0034_ref_03_w2aab2b8d168b1b7b1ab2b1b3Aa">[3]</a> at the same time. In this regard, the data of <a ref-type="fig" href="#j_msp-2016-0034_fig_002_w2aab2b8d168b1b7b1ab1b3b3Aa">Fig. 2</a> to <a ref-type="fig" href="#j_msp-2016-0034_fig_005_w2aab2b8d168b1b7b1ab1b3c14Aa">Fig. 5</a>, which are also summarized in <a ref-type="table" href="#j_msp-2016-0034_tab_002_w2aab2b8d168b1b7b1ab1b4b3Ab2">Table 2</a>, can be interpreted as follows. Defects including extrinsic point defects (impurities) and other crystalline defects can act as parasitic shunt paths for the charge carriers <a ref-type="bibr" href="#j_msp-2016-0034_ref_014_w2aab2b8d168b1b7b1ab2b1c14Aa">[14]</a>, leading to the higher leakage current and lower resistivities in the samples. Additionally, a higher amount of impurities in the bottom sample might be responsible for the deteriorated crystalline quality of the sample. In this connection, the middle sample can be judged to be more appropriate to make semiconductor radiation detectors due to the lower defect concentrations (<a ref-type="fig" href="#j_msp-2016-0034_fig_002_w2aab2b8d168b1b7b1ab1b3b3Aa">Fig. 2</a>), lower FWHM (full width at half-maximum) values with a higher crystalline quality (<a ref-type="fig" href="#j_msp-2016-0034_fig_003_w2aab2b8d168b1b7b1ab1b3b6Aa">Fig. 3</a>), high enough bandgap (>2.7 eV, <a ref-type="fig" href="#j_msp-2016-0034_fig_004_w2aab2b8d168b1b7b1ab1b3b9Aa">Fig. 4</a>), and higher resistivity (<a ref-type="fig" href="#j_msp-2016-0034_fig_005_w2aab2b8d168b1b7b1ab1b3c14Aa">Fig. 5</a>). Thus, TlBr samples from the middle part of the ingot in this study can be regarded as one of the most promising materials for the next-generation radiation detectors.</p><table-wrap position="float" orientation="portrait" id="j_msp-2016-0034_tab_002_w2aab2b8d168b1b7b1ab1b4b3Ab2"><label>Table 2</label><caption><p>Summary of the Al impurity concentrations, FWHM (full width at half-maximum) values from the main peaks in the XRD graphs, optical bandgaps, and resistivities of the three samples used in this study.</p></caption><table frame="hsides" rules="groups"><thead><tr><th></th><th align="center">Top</th><th align="center" colspan="2">Middle Bottom</th></tr></thead><tbody><tr><td align="left">Al impurity conc. [ppm]</td><td align="center">0.12</td><td align="center">0.09</td><td align="center">0.47</td></tr><tr><td align="left">FWHM [radian]</td><td align="center">0.215</td><td align="center">0.156</td><td align="center">0.223</td></tr><tr><td align="left">Optical bandgap [eV]</td><td align="center">2.79</td><td align="center">2.76</td><td align="center">2.78</td></tr><tr><td align="left">Resistivity [×10<sup>11</sup> Ω·cm]</td><td align="center">2.2</td><td align="center">2.5</td><td align="center">2.2</td></tr></tbody></table></table-wrap></sec><sec id="j_msp-2016-0034_s_006_w2aab2b8d168b1b7b1ab1b5Aa"><label>6</label><div>Conclusions</div><p>TlBr single crystalline samples for use in semiconductor radiation detection applications were fabricated using the vertical Bridgman-Stockbarger method. Based on the results of ICP-MS, XRD, optical bandgap, and I-V measurements, it can be seen that the middle sample has lower impurity concentrations, lower FWHM (full width at half-maximum) values for a higher crystalline quality, high enough bandgap (>2.7 eV), and higher resistivity (2.5 × 10<sup>11</sup> Ω·cm), which are all eligible properties for enhanced radiation detection properties. Therefore, TlBr single crystals can be regarded as one of the most promising materials for the next-generation semiconductor radiation detection device.</p></sec></div>

Characteristics of TlBr single crystals grown using the vertical Bridgman-Stockbarger method for semiconductor-based radiation detector applications

Korea Atomic Energy Research Institute, 29 Geumgu-gil, Jeong-eup, Republic of Korea 580-185

WCU Department of Energy Science, Sungkyunkwan University, Suwon, Republic of Korea, 440-746

Materials Science-Poland

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.

TlBr single crystals grown using the vertical Bridgman-Stockbarger method were characterized for semiconductor based radiation detector applications. It has...

Characteristics of TlBr single crystals grown using the vertical Bridgman-Stockbarger method for semiconductor-based radiation detector applications

Article Category: Research Article

Publicado en línea: 18 jun 2016

Páginas: 297 - 301

Recibido: 10 jun 2015

Aceptado: 13 ene 2016

DOI: https://doi.org/10.1515/msp-2016-0034

Palabras clave
semiconductor single crystal, TlBr, radiation detection, crystalline quality, impurity, resistivity, optical bandgap

© Wroclaw University of Technology

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.

Characteristics of TlBr single crystals grown using the vertical Bridgman-Stockbarger method for semiconductor-based radiation detector applications

Article Category: Research Article

Publicado en línea: 18 jun 2016

Páginas: 297 - 301

Recibido: 10 jun 2015

Aceptado: 13 ene 2016

DOI: https://doi.org/10.1515/msp-2016-0034

Palabras clavesemiconductor single crystal, TlBr, radiation detection, crystalline quality, impurity, resistivity, optical bandgap

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Palabras clave
semiconductor single crystal, TlBr, radiation detection, crystalline quality, impurity, resistivity, optical bandgap