Analysis of Human Tooth Pulp Chamber Temperature After 670 nm Laser Irradiation: In Vitro Study

2017 ◽  
Vol 35 (10) ◽  
pp. 515-519 ◽  
Author(s):  
Cleide Regina Alves Carrara de Oliveira ◽  
Fátima Zanin ◽  
Alessandra Cassoni ◽  
José Augusto Rodrigues ◽  
Landulfo Silveira ◽  
...  
2008 ◽  
Vol 16 (5) ◽  
pp. 355-359 ◽  
Author(s):  
Thaise Graciele Carrasco ◽  
Laise Daniela Carrasco-Guerisoli ◽  
Izabel Cristina Fröner

2021 ◽  
Vol 37 (2) ◽  
pp. 157-164
Author(s):  
Aysegul Ayhan Bani ◽  
Burcu Balos Tuncer ◽  
Cumhur Tuncer

Laser Physics ◽  
2021 ◽  
Vol 31 (5) ◽  
pp. 055601
Author(s):  
Sogol Saberi ◽  
Sima Shahabi ◽  
Saba Tohidkhah ◽  
Shiva Jafarnia ◽  
Parham Pedram

2020 ◽  
Vol 8 (03) ◽  
pp. 080-083
Author(s):  
Aditya Bansal ◽  
Yogesh Kumar ◽  
Neetu Jindal ◽  
Renu Aggarwal ◽  
Somya Jain

Abstract Introduction The aim of the study was to evaluate rise in pulp chamber temperature after activation with different curing lights on bleached teeth in an in vitro study. The present study is an in vitro study with a sample size of 100. A total of 100 human extracted maxillary central and lateral incisors were collected and then randomly assigned into one control group and four experimental groups (n = 20). Material and Methods As many as 100 freshly extracted noncarious human maxillary central and lateral incisor teeth were used in this study. The access opening of all 100 samples were done to facilitate access to the pulp chambers for measuring the temperature. The samples were embedded into the additional silicone model, and uniform distance of 5 mm from tooth surface was taken for gel activation using different curing lights (LED, QTH, plasma arc, diode laser). The temperature inside the pulp chamber was measured using digital infrared thermometer. Infrared light of infrared thermometer was put on pulp chamber before the bleaching gel application (T0) 1 minute after bleaching gel application (T1). Later, there was changing of color of bleaching gel from dark red into green color when activated with different curing lights (T2). Statistical Analysis The temperature data obtained were analyzed statistically by one-way ANOVA and posthoc Tukey’s tests. Significance level was set at 5% for all analyses. Results The mean and standard deviation (SD) values of rise in pulp chamber temperature after activation with different light sources were Group II (LED) 0.5 ± 0.466, Group III (QTH) 0.775 ± 0.229, Group IV (plasma arc) 1.26 ± 0.690, and Group V (diode laser) 1.355 ± 0.452. Conclusion Compared with other light-curing units, LED group induced lowest rise in pulp chamber temperature. Whereas, bleaching without light activation does not induce rise in pulp chamber temperature.


2010 ◽  
Vol 26 (2) ◽  
pp. 143-147 ◽  
Author(s):  
Márcio de Alencar Mollo ◽  
Lucio Frigo ◽  
Giovani Marino Favero ◽  
Rodrigo Álvaro Brandão Lopes-Martins ◽  
Aldo Brugnera Junior

2010 ◽  
Vol 38 (2) ◽  
pp. 76-79 ◽  
Author(s):  
Bağdagül Helvacıoğlu Kivanç ◽  
Hacer Deniz Arisu ◽  
Özgür İlke Atasoy Ulusoy ◽  
Baran Can Sağlam ◽  
Güliz Görgül

2021 ◽  
Vol 37 (2) ◽  
pp. 157-164
Author(s):  
Aysegul Ayhan Bani ◽  
Burcu Balos Tuncer ◽  
Cumhur Tuncer

Author(s):  
Katharina Kuhn ◽  
Carmen U. Schmid ◽  
Ralph G. Luthardt ◽  
Heike Rudolph ◽  
Rolf Diebolder

AbstractInadvertent Er:YAG laser irradiation occurs in dentistry and may harm restorative materials in teeth. The aim of this in vitro study was to quantify Er:YAG laser-induced damage to a nanohybrid composite in simulated clinical scenarios for inadvertent direct and indirect (reflection) laser irradiation. The simulation was performed by varying the output energy (OE;direct˃indirect) reaching the specimen and the operating distance (OD;direct˂indirect). Composite specimens were irradiated by an Er:YAG laser. The ablation threshold was determined and clinically relevant parameters were applied (n = 6 for each OE/OD combination) for direct (OE: 570 mJ/OD: 10 mm, OE: 190 mJ/OD: 10 mm) and indirect irradiation (OE: 466 mJ/OD: 15 mm, OE: 57 mJ/OD: 15 mm, OE: 155 mJ/OD: 15 mm, OE: 19 mJ/OD: 15 mm). The extent of damage in the form of craters was evaluated using a laser scanning microscope (LSM) and a conventional light microscope (LM). The ablation threshold was determined to be 2.6 J/cm2. The crater diameter showed the highest value (LM: 1075 ± 18 µm/LSM: 1082 ± 17 µm) for indirect irradiation (reflectant:dental mirror) (OE: 466 mJ/OD: 15 mm). The crater depth showed the highest and comparable value for direct (OE: 570 mJ/OD: 10 mm; LSM: 89 ± 2 µm) and indirect irradiation (OE: 466 mJ/OD: 15 mm; LSM: 90 ± 4 µm). For each OD, the crater diameter, depth, and volume increased with higher laser fluence. However, the OD—and thus the laser spot diameter—also had an enlarging effect. Thus, indirect irradiation (reflectant:dental mirror) with only 47% of the laser fluence of direct irradiation led to a larger diameter and a comparable depth. The three-dimensional extent of the crater was large enough to cause roughening, which may lead to plaque accumulation and encourage caries, gingivitis, and periodontitis under clinical conditions. Clinicians should be aware that reflected irradiation can still create such craters.


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