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0802.1098
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 68529, "num_imgs": 0, "llama3_tokens_count": 20363 }
[]
# Model dynamics on a multigrid across multiple length and time scales A. J. Roberts Computational Engineering and Sciences Research Centre, Dept Maths and Computing, University of Southern Queensland, Toowoomba, Queensland 4350, Australia. ###### Abstract Most methods for modelling dynamics posit just two time sca...
0911.3721
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 59632, "num_imgs": 0, "llama3_tokens_count": 20963 }
[]
# Optimal Paths on the Space–Time SINR Random Graph ###### Abstract We analyze a class of Signal-to-Interference-and-Noise-Ratio (SINR) random graphs. These random graphs arise in the modeling packet transmissions in wireless networks. In contrast to previous studies on the SINR graphs, we consider both a space and a...
1304.2618
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 18829, "num_imgs": 0, "llama3_tokens_count": 5818 }
[]
# Lexicographic identifying codes Maximilien Gadouleau School of Engineering and Computing Sciences Durham University m.r.gadouleau@durham.ac.uk ###### Abstract An identifying code in a graph is a set of vertices which intersects all the symmetric differences between pairs of neighbourhoods of vertices. Not all g...
1311.6600
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 32960, "num_imgs": 1, "llama3_tokens_count": 10209 }
[ "content_image/1311.6600/x1.png" ]
# Optimal condition for measurement observable via error-propagation Wei Zhong\({}^{1}\), Xiao-Ming Lu\({}^{2}\), Xiao-Xing Jing\({}^{1}\) and Xiaoguang Wang\({}^{1}\) \({}^{1}\) Zhejiang Institute of Modern Physics, Department of Physics, Zhejiang University, Hangzhou 310027, China. \({}^{2}\) Centre for Quantum Tec...
1510.07423
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 86158, "num_imgs": 1, "llama3_tokens_count": 35723 }
[ "content_image/1510.07423/x1.png" ]
"# Anisotropic scaling of random grain model\n\nwith application to network traffic\n\nVytautė Pili(...TRUNCATED)
1812.06383
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 46015, "num_imgs": 0, "llama3_tokens_count": 19408 }
[]
"# Exact normalized eigenfunctions for general deformed Hulthén potentials\n\nRichard L. Hall\n\nDe(...TRUNCATED)
1902.06526
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 23519, "num_imgs": 2, "llama3_tokens_count": 6742 }
[ "content_image/1902.06526/x1.png", "content_image/1902.06526/x2.png" ]
"# Exact results for the entanglement in 1D Hubbard models with spatial constraints\n\nIoannis Kleft(...TRUNCATED)
1602.00825
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 54956, "num_imgs": 21, "llama3_tokens_count": 20136 }
["content_image/1602.00825/x1.png","content_image/1602.00825/x2.png","content_image/1602.00825/x8.pn(...TRUNCATED)
"# Nonclassical Particle Transport in 1-D Random Periodic Media\n\n**R. Vasques \\({}^{\\dagger,}\\)(...TRUNCATED)
1009.0666
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 17134, "num_imgs": 9, "llama3_tokens_count": 3996 }
["content_image/1009.0666/x1.png","content_image/1009.0666/x2.png","content_image/1009.0666/x3.png",(...TRUNCATED)
"# The First Station of the Long Wavelength Array\n\nUniversity of New Mexico\n\nE-mail:\n\nSteven W(...TRUNCATED)
1912.09110
{ "language": "en", "source": "Arxiv", "date_download": "2024-12-03T00:00:00" }
{ "doc_length": 21698, "num_imgs": 1, "llama3_tokens_count": 7023 }
[ "content_image/1912.09110/x1.png" ]
"# Mixed QCD-EW two-loop corrections to Drell-Yan production\n\nPRISMA\\({}^{+}\\) Cluster of Excell(...TRUNCATED)
End of preview. Expand in Data Studio

📥 IN-Scientific

IN-Scientific: An Open Multimodal Interleaved Dataset for Scientific Knowledge Representation

This project is a subproject of the 📌PIN project, focusing on the development of the largest scientific document multimodal dataset, which integrates both text and images.

📑: https://arxiv.org/abs/2406.13923

🤗: https://huggingface.co/datasets/m-a-p/PIN-14M

Dataset statistics

Source Content Images (#) Content Images (Size GB) Documents (#) Documents (Size GB) Llama3 Tokens (#)
IN-Arxiv 3.947 M 507.99 0.715 M 37.38 11.752 B
IN-PMC 19.711 M 2154.95 5.677 M 219.00 57.500 B
Total 23.658 M 2662.94 6.392 M 256.38 69.252 B

Examples

IN-Arxiv

{
    "id": "1407.4558",
    "meta": {
        "language": "en",
        "source": "Arxiv",
        "date_download": "2024-12-03"
    },
    "quality_signals": {
        "doc_length": 55245,
        "num_imgs": 1,
        "llama3_tokens_count": 22007
    },
    "content_image": [
        "content_image/1407.4558/x1.png"
    ],
    "md": "# Div First-Order System LL* (FOSLL*) for Second-Order Elliptic Partial Differential Equations \u2020\n[FOOTNOTE:\u2020][ENDFOOTNOTE]\n\nZhiqiang Cai\n\n Department of Mathematics ..."
}

IN-PMC

{
    "id": "PMC3231073",
    "meta": {
        "date_download": "2024-12-14",
        "language": "en",
        "source": "PMC"
    },
    "quality_signals": {
        "doc_length": 20785,
        "llama3_tokens_count": 4364,
        "num_imgs": 7
    },
    "content_image": [
        "content_image/PMC3231073/sensors-10-10663-v2f1.jpg",
        "content_image/PMC3231073/sensors-10-10663-v2f2.jpg",
        "content_image/PMC3231073/sensors-10-10663-v2f3.jpg",
        "content_image/PMC3231073/sensors-10-10663-v2f4.jpg",
        "content_image/PMC3231073/sensors-10-10663-v2f5.jpg",
        "content_image/PMC3231073/sensors-10-10663-v2f6.jpg",
        "content_image/PMC3231073/sensors-10-10663-v2f7.jpg"
    ],
    "md": "# The Use of Helmholtz Resonance for Measuring the Volume of Liquids and Solids\n\n## Abstract\n\nAn experimental investigation was undertaken to ascertain the potential of using Helmholtz resonance for volume determination and the factors that may influence accuracy. The uses for a rapid non-interference volume measurement system range from agricultural produce and mineral sampling through to liquid fill measurements. By weighing the sample the density can also measured indirectly..."
}
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