| Literature DB >> 30740253 |
Sobia Nisar1, Ghulam Dastgeer2, Muhammad Shafiq3, Muhammad Usman4.
Abstract
Laser-induced breakdown spectroscopy (LIBS) is a sensitive optical technique that is capable of rapid multi-elemental analysis. The development of this technique for elemental analysis of pharmaceutical products may eventually revolutionize the field of human health. Under normal circumstances, the elemental analysis of pharmaceutical products based on chemical methods is time-consuming and complicated. In this investigation, the principal aim is to develop an LIBS-based methodology for elemental analysis of pharmaceutical products. This LIBS technique was utilized for qualitative as well as quantitative analysis of the elements present in Ca-based tablets. All the elements present in the tablets were detected and their percentage compositions were verified in a single shot, using the proposed instrument. These elements (e.g., Ca, Mg, Fe, Zn, and others) were identified by the wavelengths of their spectral lines, which were verified using the NIST database. The approximate amount of each element was determined based on their observed peaks and the result was in exact agreement with the content specification. The determination of the composition of prescription drug for patients is highly important in numerous circumstances. For example, the exploitation of LIBS may facilitate elemental decomposition of medicines to determine the accuracy of the stated composition information. Moreover, the approach can provide element-specific, meaningful, and accurate information related to pharmaceutical products.Entities:
Keywords: Elements identification; Health-care pharmaceutics; Laser-induced breakdown spectroscopy; Qualitative analysis; Quantitative analysis
Year: 2018 PMID: 30740253 PMCID: PMC6355465 DOI: 10.1016/j.jpha.2018.10.003
Source DB: PubMed Journal: J Pharm Anal ISSN: 2214-0883
Fig. 1(A) Schematic diagram demonstrating the analysis of tablet samples using an Nd: YAG laser where the wavelengths of the elements associated with the resulting plasma are detected by a spectrometer connected to a computer. (B) The SEM image of tablet sample indicates the region where the laser is incident on the sample to collect elemental analysis data.
Fig. 2The LIBS data obtained for OMC-D tablet is plotted in the range of 300–700 nm wavelength. (A) The elements observed in the range of 300–700 nm wavelength. (B) The elements observed in the range of 385–425 nm wavelength. (C) The elements observed in the range of 580–600 nm wavelength. (D) The elements observed in the range of 600–630 nm wavelength. (E) The elements observed in the range of 635–675 nm wavelength.
The elements traced by their spectral lines present in each sample of OMC-D tablets using 1064 nm Nd:YAG laser.
| Sr. No | Wavelength (nm) | Traced elements | Transitions | |
|---|---|---|---|---|
| Lower energy | Upper energy | |||
| 1 | 393.33 | Ca II | 3p64s2S1/2 | 3p64p 2P° 3/2 |
| 2 | 396.80 | Ca II | 3p64s 2S 1/2 | 3p64p 2P° 1/2 |
| 3 | 422.88 | Fe II | 3 | 3 |
| 4 | 585.69 | Cu I | 3 | 3 |
| 6 | 588.97 | Fe I | 3p64s4f | 3d7(4F)4d |
| 7 | 589.18 | Fe I | 3d72f4s | 3 |
| 8 | 610.27 | Ca I | 3 | 3 |
| 9 | 612.73 | Mg III | 2 | 2 |
| 10 | 616.21 | Ca I | 3p64s4p 3P° | 3p64s5s3S |
| 11 | 617.68 | Ni I | 3 | 3 |
| 8 | 643.63 | P I | – | – |
| 9 | 644.76 | Cu II | 3 | 3 |
| 10 | 646.25 | Ca I | 3 | 3 |
| 14 | 647.91 | Zn I | – | – |
| 15 | 649.44 | Ca I | 3p63d4s | 3p64s4f |
| 16 | 649.96 | Fe I | 3 | 3 |
| 17 | 671.83 | Ni I | 3s23p2(3P)4p | 3s23p2(3P)5d |
The elements traced by their spectral lines present in each sample of Osnate-d tablets using 1064 nm Nd:YAG laser.
| Sr. No | Wavelength (nm) | Traced elements | Transitions | |
|---|---|---|---|---|
| Lower energy | Upper energy | |||
| 1 | 317.22 | Zn II | – | – |
| 2 | 319.63 | Zn II | ||
| 3 | 393.33 | Ca II | 3p64s2S1/2 | 3p64p 2P° 3/2 |
| 4 | 396.80 | Ca II | 3p64s 2S 1/2 | 3p64p 2P° 1/2 |
| 6 | 422.88 | Fe II | 3 | 3 |
| 7 | 430.77 | Ca I | 3 | 3 |
| 8 | 440.62 | Ca III | 3 | 3 |
| 9 | 442.31 | Mg III | 2 | 2 |
| 10 | 453.07 | Cu I | 2s22p5(2P°1/2)3d | 2s22p5(2P°1/2)4f |
| 11 | 487.80 | Ca I | 3p63d4s | 3p64s4f |
| 8 | 516.71 | Mg I | 3 | 3 |
| 9 | 519.13 | P II | 3 | 3 |
| 10 | 527.09 | Ca I | 3p63d4s | 3p64s4f |
| 14 | 551.72 | P I | 3d6(5D)4s | 3d5(6S)4s4p(1P°) |
| 15 | 588.97 | Fe I | 3p64s4f | 3d7(4F)4d |
| 16 | 625.72 | Ca I | 2s24p2P° | 2s25d |
| 17 | 671.83 | Ni I | 3s23p2(3P)4p | 3s23p2(3P)5d |
The elements traced by their spectral lines present in each sample of Hectoral tablets using 1064 nm Nd:YAG laser.
| Sr. No | Wavelength (nm) | Traced elements | Transitions | |
|---|---|---|---|---|
| Lower energy | Upper energy | |||
| 1 | 305.56 | Fe I | 3 | 3 |
| 2 | 319.63 | Zn II | – | – |
| 3 | 334.89 | Ni II | 5p5 (2P°) 6s | 5p64p 2P° 3/2 |
| 4 | 370.39 | Mg III | 2 | 2 |
| 6 | 393.33 | Ca II | 3p64s2S1/2 | 3p64p 2P° 3/2 |
| 7 | 396.80 | Ca II | 3p64s 2S 1/2 | 3p64p 2P° 1/2 |
| 8 | 430.77 | Ca I | 3 | 3 |
| 9 | 453.07 | Cu I | 2s22p5(2P°1/2)3d | 2s22p5(2P°1/2)4f |
| 10 | 498.16 | Fe I | 3d7(4F)4p | 3d7(4F)4d |
| 11 | 500.73 | Mg III | 2 | 2 |
| 8 | 502.14 | Ca II | 3 | 3 |
| 9 | 518.88 | Ca I | 3 | 3 |
| 10 | 551.72 | P I | 3d6(5D)4s | 3d5(6S)4s4p(1P°) |
| 14 | 558.92 | Ca I | 3p64s2S1/2 | 3p63d4p3D° |
| 15 | 588.97 | Fe I | 3p64s4f | 3d7(4F)4d |
| 16 | 625.72 | Ca I | 2s24p2P° | 2s25d |
| 17 | 671.83 | Ni I | 3s23p2(3P)4p | 3s23p2(3P)5d |
Fig. 3The LIBS data obtained for Osnate-d tablet is plotted in the range of 300–700 nm wavelength. The small arrows indicate the identified peaks of the elements.
Fig. 4The LIBS data obtained for Hectoral tablet is plotted in the range of 300–700 nm wavelength. The small arrows indicate the identified peaks of the elements.