| Literature DB >> 30735548 |
Hyunuk Kim1,2,3, Inho Hong4, Woo-Sung Jung1,4,5.
Abstract
In the era of big science, countries allocate big research and development budgets to large scientific facilities that boost collaboration and research capability. A nuclear fusion device called the "tokamak" is a source of great interest for many countries because it ideally generates sustainable energy expected to solve the energy crisis in the future. Here, to explore the scientific effects of tokamaks, we map a country's research capability in nuclear fusion research with normalized revealed comparative advantage on five topical clusters-material, plasma, device, diagnostics, and simulation-detected through a dynamic topic model. Our approach captures not only the growth of China, India, and the Republic of Korea but also the decline of Canada, Japan, Sweden, and the Netherlands. Time points of their rise and fall are related to tokamak operation, highlighting the importance of large facilities in big science. The gravity model points out that two countries collaborate less in device, diagnostics, and plasma research if they have comparative advantages in different topics. This relation is a unique feature of nuclear fusion compared to other science fields. Our results can be used and extended when building national policies for big science.Entities:
Mesh:
Year: 2019 PMID: 30735548 PMCID: PMC6368312 DOI: 10.1371/journal.pone.0211963
Source DB: PubMed Journal: PLoS One ISSN: 1932-6203 Impact factor: 3.240
Summary statistics of 14 leading countries in nuclear fusion research.
All values are real numbers as we count the number of papers by the fractional counting method. Ratio is the proportion of collaborative papers to total papers.
| Country | Collaborative Papers | Total Papers | Ratio |
|---|---|---|---|
| United States | 978.4 | 7646.4 | 0.13 |
| Japan | 411.7 | 3025.7 | 0.14 |
| China | 335.7 | 2777.7 | 0.12 |
| Germany | 738.1 | 2147.1 | 0.34 |
| United Kingdom | 522.5 | 1775.5 | 0.29 |
| Russia | 299.5 | 1392.5 | 0.22 |
| France | 403.6 | 1135.6 | 0.36 |
| Italy | 325.1 | 964.1 | 0.34 |
| Republic of Korea | 115.8 | 424.8 | 0.27 |
| Switzerland | 153.5 | 409.5 | 0.37 |
| India | 49.8 | 400.8 | 0.12 |
| Sweden | 135.0 | 326.0 | 0.41 |
| Canada | 73.6 | 292.6 | 0.25 |
| Netherlands | 102.4 | 276.4 | 0.37 |
Fig 1Schematics of the fractional counting method for publication and collaboration counts.
Two matrices, the fractional publication counts by countries A and the topic distributions of papers B, were extracted from the document set of year t. (1) represents the fractional publication counts by topics at year t. For further analysis, based on the hierarchical tree of clusters in Fig 2, the fractional publications by 41 topics are grouped into five topical clusters: material, plasma, device, diagnostics, and simulation. R is the aggregated matrix and is transposed in the figure to match with the hierarchical tree of 41 clusters. (2) The country profile of a paper is transformed into a collaboration matrix W1, which was distributed over the five topical clusters by weights. For each year, by aggregating the collaboration matrices of all published papers, we had five fractional collaboration matrices.
Fig 2Hierarchical tree of 41 topics detected from the dynamic topic model.
Topics were agglomerated by the ward.D method [50]. The distance between topics was measured by the Jensen-Shannon distance [51], a square root of the Jensen-Shannon divergence. Five topical clusters—material, plasma, device, diagnostics, and simulation—are revealed. The branches are colored by the corresponding topical clusters.
Fig 3Ranks of normalized revealed comparative advantages for the top 14 countries.
Rank series of the countries are smoothed with LOESS (locally estimated scatterplot smoothing) and colored by the topical clusters.
Gravity model OLS regression results.
| Variables | Material | Plasma | Device | Diagnostics | Simulation |
|---|---|---|---|---|---|
| 0.497 | 0.508 | 0.411 | 0.438 | 0.488 | |
| 0.497 | 0.508 | 0.411 | 0.438 | 0.488 | |
| -0.495 | -0.451 | -0.464 | -0.546 | -0.485 | |
| -0.133 | -0.911 | -0.949 | -0.690 | -0.027 | |
| Observations | 3518 | 3518 | 3518 | 3518 | 3518 |
| 0.113 | 0.123 | 0.101 | 0.094 | 0.107 |
Standard error is in parenthesis.
Fixed time effects are included.
* p-value < 0.1,
** p-value < 0.05,
*** p-value < 0.01